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Energy levels, radiative rates, and electron impact excitation rates for transitions in Li-like ions with 21≤Z≤28
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Energy levels, radiative rates, and electron impact excitation rates for transitions in Li-like ions with 21 ≤ Z ≤ 28 Kanti M. Aggarwal ∗ , Francis P. Keenan Astrophysics Research Centre, School of Mathematics and Physics, Queen’s University Belfast, Belfast BT7 1NN, Northern Ireland, UK
article
info
Article history: Received 15 March 2011 Received in revised form 13 May 2011 Accepted 27 May 2011 Available online xxxx
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abstract We report calculations of energy levels, radiative rates, and electron impact excitation rates for transitions in Li-like ions with 21 ≤ Z ≤ 28. The General-Purpose Relativistic Atomic Structure Package is adopted for calculating energy levels and radiative rates, while for determining the collision strengths and subsequently the excitation rates, the Dirac Atomic R-matrix Code is used. Oscillator strengths, radiative rates, and line strengths are listed for all E1, E2, M1, and M2 transitions among the lowest 24 levels of the Li-like ions considered. Collision strengths have been averaged over a Maxwellian velocity distribution, and the effective collision strengths obtained are given over a wide temperature range up to 107.8 K. Additionally, lifetimes are listed for all calculated levels of these ions. Finally, extensive comparisons are made with results available in the literature, as well as with our analogous calculations for all parameters with the Flexible Atomic Code, in order to assess the accuracy of the results. © 2012 Elsevier Inc. All rights reserved.
Corresponding author. Tel.: +44 28 9097 3239; fax: +44 28 9097 3110. E-mail address: [email protected] (K.M. Aggarwal).
0092-640X/$ – see front matter © 2012 Elsevier Inc. All rights reserved. doi:10.1016/j.adt.2011.05.002
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Contents 1. 2. 3. 4. 5. 6. 7.
Introduction........................................................................................................................................................................................................................ Energy levels....................................................................................................................................................................................................................... Radiative rates .................................................................................................................................................................................................................... Lifetimes ............................................................................................................................................................................................................................. Collision strengths ............................................................................................................................................................................................................. Effective collision strengths .............................................................................................................................................................................................. Conclusions......................................................................................................................................................................................................................... Acknowledgment ............................................................................................................................................................................................................... Appendix. Supplementary data.................................................................................................................................................................................... References........................................................................................................................................................................................................................... Explanation of Tables ......................................................................................................................................................................................................... Table 1. Energy levels of Sc XIX, their threshold energies (in Ryd), and lifetimes (in s). ........................................................................................ Table 2. Energy levels of Ti XX, their threshold energies (in Ryd), and lifetimes (in s)........................................................................................... Table 3. Energy levels of V XXI, their threshold energies (in Ryd), and lifetimes (in s). ......................................................................................... Table 4. Energy levels of Cr XXII, their threshold energies (in Ryd), and lifetimes (in s). ....................................................................................... Table 5. Energy levels of Mn XXIII, their threshold energies (in Ryd), and lifetimes (in s). .................................................................................... Table 6. Energy levels of Fe XXIV, their threshold energies (in Ryd), and lifetimes (in s)....................................................................................... Table 7. Energy levels of Co XXV, their threshold energies (in Ryd), and lifetimes (in s). ...................................................................................... Table 8. Energy levels of Ni XXVI, their threshold energies (in Ryd), and lifetimes (in s)....................................................................................... Table 9. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Sc XIX. ................................................................................................................................................................................................................. Table 10. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ti XX. ............................................................................................................................................................................................... Table 11. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in V XXI. ............................................................................................................................................................................................... Table 12. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Cr XXII.............................................................................................................................................................................................. Table 13. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Mn XXIII........................................................................................................................................................................................... Table 14. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Fe XXIV. ........................................................................................................................................................................................... Table 15. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Co XXV. ............................................................................................................................................................................................ Table 16. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ni XXVI. ........................................................................................................................................................................................... Table 17. Collision strengths for resonance transitions in Sc XIX............................................................................................................................. Table 18. Collision strengths for resonance transitions in Ti XX. ............................................................................................................................. Table 19. Collision strengths for resonance transitions in V XXI. ............................................................................................................................. Table 20. Collision strengths for resonance transitions in Cr XXII............................................................................................................................ Table 21. Collision strengths for resonance transitions in Mn XXIII. ....................................................................................................................... Table 22. Collision strengths for resonance transitions in Fe XXIV. ......................................................................................................................... Table 23. Collision strengths for resonance transitions in Co XXV........................................................................................................................... Table 24. Collision strengths for resonance transitions in Ni XXVI. ......................................................................................................................... Table 25. Effective collision strengths for transitions in Sc XIX................................................................................................................................ Table 26. Effective collision strengths for transitions in Ti XX. ................................................................................................................................ Table 27. Effective collision strengths for transitions in V XXI. ................................................................................................................................ Table 28. Effective collision strengths for transitions in Cr XXII............................................................................................................................... Table 29. Effective collision strengths for transitions in Mn XXIII. .......................................................................................................................... Table 30. Effective collision strengths for transitions in Fe XXIV. ............................................................................................................................ Table 31. Effective collision strengths for transitions in Co XXV. ............................................................................................................................. Table 32. Effective collision strengths for transitions in Ni XXVI. ............................................................................................................................
1. Introduction
Emission lines of Li-like ions have been observed in the spectra of a variety of astrophysical [1,2] and laboratory plasmas [3,4]. Transitions of many Li-like ions are useful for temperature and density diagnostics of solar plasmas [2] as well as for the determination of chemical abundances [5]. However to analyse
2 3 3 5 6 8 11 11 11 11 12 12 12 12 12 12 12 12 12
12
12
12
12
12
12
12
13 13 13 13 13 13 13 13 13 13 13 13 13 13 13 13 13
observations, atomic data are required for a variety of parameters, such as energy levels, radiative rates (A-values), and excitation rates or equivalently the effective collision strengths (Υ ), which are obtained from the electron impact collision strengths (Ω ). These data are also required for the modelling of fusion plasmas, as many elements are present in the plasmas because of sputtering from the reactor walls. Similarly, data are required for diagnostics of laboratory plasmas [6]. With this in view we have already
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
reported calculations for Li-like ions with Z ≤ 20 [7–10] and in this paper we provide similar results for ions with 21 ≤ Z ≤ 28. Experimentally, there have been some measurements of energy levels for Li-like ions, which have been compiled by the National Institute of Standards and Technology (NIST) and are available at their website www.nist.gov/pml/data/asd.cfm. Theoretically, energy levels and A-values have been calculated by Nahar [11] for transitions in 15 Li-like ions with 6 ≤ Z ≤ 28. However, collisional atomic data are limited to transitions among the lowest three levels of Li-like ions with 8 ≤ Z ≤ 92, and from these levels to the higher excited levels of the n ≤ 5 configurations [12]. The calculations of Zhang et al. [12] are based on the relativistic distortedwave (DW) method, and collision strengths are reported only at six energies above thresholds. Since resonances in the threshold region have not been resolved, the subsequent results for effective collision strengths are significantly underestimated over a wide temperature range for a large number of transitions (in particular forbidden transitions), as already demonstrated in our earlier papers for ions with Z ≤ 20 [7–10]. In this paper we report a complete set of results (namely, energy levels, radiative rates, and effective collision strengths) for all transitions among the lowest 24 levels of Li-like ions with 21 ≤ Z ≤ 28. Additionally, we provide the A-values for four types of transitions, namely electric dipole (E1), electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions, because these are also required for plasma modelling. For our calculations of wavefunctions we employ the fully relativistic General-Purpose Relativistic Atomic Structure Package (grasp), originally developed by Grant et al. [13] and revised by P.H. Norrington. It is a fully relativistic code, and is based on the jj coupling scheme. Further relativistic corrections arising from the Breit interaction and QED effects (vacuum polarization and Lamb shift) have also been included. In calculating energy levels, we have kept the 1s shell frozen and have used the option of extended average level, in which a weighted (proportional to 2j+1) trace of the Hamiltonian matrix is minimized. This produces a compromise set of orbitals describing closely lying states with moderate accuracy. Similarly, for our calculations of Ω , we have adopted the Dirac Atomic R-matrix Code (darc) of P.H. Norrington and I.P. Grant (web.am.qub.ac.uk/DARC/). Finally, to make comparisons and to assess the accuracy of our results, we have performed analogous calculations from the Flexible Atomic Code (fac) of Gu [14], available from the website sprg.ssl.berkeley.edu/~mfgu/fac/. This is also a fully relativistic code that provides a variety of atomic parameters, and yields results comparable to grasp and darc — see, for example, Ref. [15] and references therein. Generally, there is no major discrepancy in the determination of energy levels and radiative rates between results of grasp and fac, but the former code allows more flexibility in terms of optimizations. Furthermore, in cases of strong mixing, the identification of different J levels belonging to a particular configuration is a greater problem in fac than in grasp, although it should not apply to simple Li-like ions. On the other hand, differences in collision strengths can sometimes be larger, particularly for the forbidden transitions, as discussed and demonstrated in some of our earlier papers [7–10]. Similarly, results for Υ can be significantly underestimated by fac, particularly for forbidden transitions and at lower temperatures, due to the neglect of the contribution of resonances. Nevertheless, results from fac will be helpful in assessing the accuracy of our energy levels, radiative rates, and collision strengths, and in estimating the contribution of resonances for the determination of Υ .
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2. Energy levels The 1s2 nℓ (2 ≤ n ≤ 5) configurations of Li-like ions give rise to the lowest 24 energy levels listed in Tables 1–8. Included in these tables are the level energies from grasp, obtained without and with the inclusion of Breit and QED effects, plus the experimental energies compiled by NIST. Also listed in these tables are the theoretical energies obtained from our analogous calculations from fac and those by Nahar [11] from the Breit–Pauli R-matrix (BPRM) code of Berrington et al. [16]. The inclusion of the Breit and QED corrections decreases the energy levels (except for level 2, i.e., 2p 2 Po1/2 ) by a maximum of ∼0.1 Ryd, depending on the ion. As the ion nuclear charge Z increases, so does the effect of the Breit and QED corrections. For example, energy levels of Sc XIX decrease by ∼0.04 Ryd, but for Ni XXVI by ∼0.1 Ryd. Clearly, the importance of relativistic effects increases with increasing Z . Our Breit and QED corrected energies from grasp agree closely (generally within 0.02 Ryd) with those of NIST and the orderings are also nearly the same, although there is a noticeable difference for the 3s 2 S1/2 level of Sc XIX for which the NIST energy appears to be higher by ∼0.1 Ryd. Furthermore, the NIST energies for some levels are the same — see, for example, the 4f 2 Fo5/2,7/2 and 5p 2 Po1/2,3/2 levels of Sc XIX. Similarly, NIST energies are not available for some levels — see, for example, the 5f 2 Fo5/2,7/2 and 5g 2 G7/2,9/2 levels of all Li-like ions under consideration. The energies obtained from fac are generally comparable with the experimental compilations of NIST and/or our calculations from grasp. However, the orderings of some of the levels are slightly different from fac than from the experimental and other theoretical energies. As examples, see the 13–14 and 22–23 levels of Sc XIX and Ni XXVI. Nevertheless, the energy differences among these levels are very small. Finally, the BPRM energies of Nahar [11] have the same orderings as NIST and our calculations from grasp, but are higher for most of the levels by about 0.06 Ryd for Ti XX and 0.2 Ryd for Ni XXVI. Clearly, this is due to the neglect of the two-body relativistic effects in the BPRM calculations. Overall, we may state that there is no (major) discrepancy between theory and experiment for the energy levels of Li-like ions. 3. Radiative rates The absorption oscillator strength fij and radiative rate Aji (in s−1 ) for a transition i–j are related by the following expression: fij =
mc 8π 2 e2
λ2ji
ωj Aji = 1.49 × 10−16 λ2ji (ωj /ωi )Aji ωi
(1)
where m and e are the electron mass and charge, respectively, c is the velocity of light, λji is the transition wavelength in Å, and ωi and ωj are the statistical weights of the lower (i) and upper (j) levels, respectively. Similarly, the oscillator strength fij (dimensionless) and the line strength S (in atomic units, 1 a.u. = 6.460 × 10−36 cm2 esu2 ) are related by the following standard equations: for the electric dipole transitions Aji =
2.0261 × 1018
ωλ
3 j ji
S E1
and fij =
303.75
λji ωi
S E1 ,
(2)
for the magnetic dipole transitions Aji =
2.6974 × 1013
ωλ
3 j ji
S M1
and
fij =
4.044 × 10−3
λji ωi
S M1 ,
(3)
for the electric quadrupole transitions Aji =
1.1199 × 1018
ωj λ5ji
S E2
and fij =
167.89
λ3ji ωi
S E2 ,
(4)
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table A Comparison of radiative rates (A-values, s−1 ) for some transitions in Sc XIX. (a ± b ≡ a × 10±b ).
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Table B Comparison of radiative rates (A-values, s−1 ) for some transitions in Ti XX. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 6 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.4088+09 2.2436+09 2.9037+12 2.8418+12 1.2853+12 1.2661+12 6.6475+11 6.5628+11 7.2211+12 2.3558+12 1.0869+12 8.5877+12 2.7892+12 1.2837+12 2.9760+08 3.7765+11 3.6813+11 2.0806+11 2.0405+11 7.5949+11 3.7414+11 9.1135+11 4.4674+11 5.1265+09 1.6828+12 2.2009+09 5.5580+11 1.1980+11 1.7984+12 3.9440+10 5.9323+11 8.8555+10 8.6131+10 1.5739+11 1.8974+11 2.7380+09 3.1477+11 2.2480+10 3.3695+11 5.3544+11
1.4170+09 2.2490+09 2.9520+12 2.8950+12 1.3450+12 1.3280+12 7.4680+11 7.3940+11 7.2530+12 2.3980+12 1.1650+12 8.6360+12 2.8420+12 1.3730+12 2.9670+08 3.8310+11 3.7380+11 2.2220+11 2.1810+11 7.6540+11 3.8740+11 9.1850+11 4.6190+11 5.2060+09 1.6820+12 2.4010+09 5.5650+11 1.1960+11 1.7980+12 3.9420+10 5.9440+11 9.1090+10 8.8640+10 1.6070+11 1.9360+11 2.7950+09 3.1380+11 2.2400+10 3.3600+11 5.3550+11
2.2257−02 5.2315−02 1.2380−01 2.4111−01 3.0979−02 6.0936−02 1.2900−02 2.5452−02 6.7380−01 1.2235−01 4.5196−02 6.1083−01 1.1005−01 4.0508−02 8.8766−02 1.3575−01 2.6303−01 3.5963−02 7.0385−02 5.8296−01 1.3622−01 5.3159−01 1.2319−01 2.0927−03 1.0135+00 4.1604−04 1.5669−01 4.8336−02 9.6650−01 7.4375−03 1.4911−01 1.5091−01 2.9156−01 5.6643−01 5.1813−01 5.2232−03 8.8440−01 4.2296−02 8.4432−01 1.3437+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
1.4907+09 2.5447+09 3.5749+12 3.4911+12 1.5800+12 1.5542+12 8.1676+11 8.0541+11 8.8657+12 2.8917+12 1.3340+12 1.0533+13 3.4188+12 1.5731+12 1.9328+08 3.3925+08 4.6591+11 4.5300+11 2.5631+11 2.5088+11 2.4095+07 9.3273+11 4.5946+11 1.2640+07 1.1192+12 5.4834+11 6.2633+09 2.0665+12 2.6896+09 6.8262+11 1.4706+11 2.2079+12 4.8404+10 7.2830+11 4.5265+07 8.0239+07 1.0936+11 1.0607+11 7.4663+06 1.9329+11 3.8843+06 2.3314+11 1.6307+04 3.3472+09 3.8650+11 1.4472+01 4.0837+03 2.7602+10 4.1369+11 6.5745+11 1.4704+07 2.6185+07 2.6949+06 1.3974+06 8.3660+03 9.2274+00 2.1866+03 2.7721+02
1.4990+09 2.5500+09 3.6310+12 3.5540+12 1.6500+12 1.6270+12 9.1200+11 9.0220+11 8.9040+12 2.9410+12 1.4250+12 1.0590+13 3.4810+12 1.6780+12
1.4030+09 2.5930+09 3.6770+12 3.5830+12 1.3880+12 1.3630+12 7.4220+11 7.3070+11 8.8800+12 2.8480+12 1.3250+12 1.0540+13 3.3630+12 1.5610+12 1.6820+08 3.2530+08 4.3630+11 4.2210+11 2.4470+11 2.3870+11 2.6690+07 9.2720+11 4.6000+11 1.2510+07 1.1130+12 5.4910+11 1.7550+12 2.0740+12 1.2150+06 6.8420+11 1.4750+11 2.2150+12 4.8480+10 7.2960+11 2.9160+08 4.2270+08 1.0170+11 9.7840+10 2.0560+07 1.9160+11 1.2340+07 2.3150+11 1.8750+04 1.8630+11 3.8590+11 7.7210+00 3.9990+03 2.7560+10 4.1310+11 6.5660+11 8.2050+07 1.2070+08 5.7560+06 3.2770+06 9.5790+03 5.0810+00 2.1250+03 3.0120+02
2.1176−02 5.0977−02 1.2474−01 2.4228−01 3.1126−02 6.1127−02 1.2949−02 2.5518−02 6.7361−01 1.2229−01 4.5170−02 6.1113−01 1.0998−01 4.0469−02 3.5750−02 8.6622−02 1.3690−01 2.6440−01 3.6170−02 7.0638−02 2.6693−02 5.8285−01 1.3620−01 1.8246−02 5.3223−01 1.2323−01 2.0804−03 1.0132+00 4.1388−04 1.5669−01 4.8328−02 9.6633−01 7.4344−03 1.4908−01 4.9417−02 1.1998−01 1.5227−01 2.9315−01 4.7484−02 5.6630−01 3.2363−02 5.1892−01 3.6407−03 5.1952−03 8.8399−01 4.0115−05 2.1363−03 4.2296−02 8.4414−01 1.3435+00 6.2748−02 1.5249−01 6.6087−02 4.4991−02 6.8101−03 8.0693−05 4.0532−03 1.3874−03
GRASP: Present results from grasp. FAC: Present results from fac.
and for the magnetic quadrupole transitions Aji =
1.4910 × 1013
ωj λ5ji
S M2
and fij =
2.236 × 10−3
λ3ji ωi
S M2 .
(5)
In Tables 9–16 we present transition wavelengths, radiative rates, oscillator strengths, and line strengths, in length form only, for all 92 electric dipole transitions among the 24 levels of Lilike ions with 21 ≤ Z ≤ 28. The indices used to represent the lower and upper levels of a transition have already been defined in Tables 1–8. Similarly, there are 100 electric quadrupole, 79 magnetic dipole, and 108 magnetic quadrupole transitions among the 24 levels. However, for these transitions only the A-values are listed in Tables 9–16, and the corresponding results for f - or Svalues may be easily obtained using Eqs. (1)–(5). In Tables A–H we compare our A-values from grasp and fac for some of the common E1 transitions with those of Nahar [11] from the BPRM code of Berrington et al. [16]. Also included in these tables are the f -values from our grasp calculations. In general, the A-values from grasp and fac agree satisfactorily (within ∼10%) for a majority of transitions for all ions. However, there are significant differences with the Nahar calculations, of up to two orders of magnitude, particularly for the comparatively weaker (f ≤ 0.01) transitions, such as 7–11, 7–18, and 12–18. Similar large differences have also been noted for transitions of other
4.7240+11 4.5970+11 2.7290+11 2.6730+11 9.3960+11 4.7490+11 1.1280+12 5.6610+11 6.3600+09 2.0650+12 2.9250+09 6.8360+11 1.4680+11 2.2080+12 4.8380+10 7.2980+11
1.1230+11 1.0900+11 1.9710+11 2.3760+11 3.4160+09 3.8550+11
2.7510+10 4.1270+11 6.5750+11
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
Li-like ions with Z ≤ 20 [8–10]. The A-values for such weak transitions from the BPRM code are likely to be less accurate, as discussed by Hibbert [17] and Aggarwal et al. [18]. In addition, several transitions are missing from the Nahar calculations, and examples include 2p 2 Po1/2 –3s 2 S1/2 (2–4), 2p 2 Po3/2 –3s 2 S1/2 (3–4), and 2p 2 Po3/2 –3d 2 D3/2 (3–7). Finally, there are significantly large differences (of over an order of magnitude) between the BPRM A-values of Nahar and our calculations from grasp for several transitions among levels 16 and higher. For all such transitions, the
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables ( Table C Comparison of radiative rates (A-values, s−1 ) for some transitions in V XXI. (a ± b ≡ a × 10±b ).
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Table D Comparison of radiative rates (A-values, s−1 ) for some transitions in Cr XXII. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.5739+09 2.8950+09 4.3570+12 4.2452+12 1.9230+12 1.8887+12 9.9358+11 9.7857+11 1.0778+13 3.5149+12 1.6215+12 1.2792+13 4.1493+12 1.9088+12 5.6888+11 5.5162+11 3.1253+11 3.0531+11 1.1340+12 5.5866+11 1.3607+12 6.6637+11 7.5793+09 2.5125+12 3.2555+09 8.3005+11 1.7873+11 2.6836+12 5.8814+10 8.8520+11 1.3364+11 1.2923+11 2.3498+11 2.8357+11 4.0527+09 4.6984+11 3.3554+10 5.0285+11 7.9923+11
1.5830+09 2.9010+09 4.4220+12 4.3200+12 2.0030+12 1.9740+12 1.1030+12 1.0910+12 1.0820+13 3.5730+12 1.7270+12 1.2870+13 4.2230+12 2.0300+12 5.7650+11 5.5950+11 3.3170+11 3.2440+11 1.1420+12 5.7660+11 1.3710+12 6.8690+11 7.6950+09 2.5110+12 3.5310+09 8.3120+11 1.7840+11 2.6840+12 5.8770+10 8.8710+11 1.3710+11 1.3270+11 2.3940+11 2.8870+11 4.1350+09 4.6870+11 3.3450+10 5.0180+11 7.9940+11
2.0198−02 4.9883−02 1.2559−01 2.4323−01 3.1258−02 6.1281−02 1.2993−02 2.5571−02 6.7331−01 1.2222−01 4.5146−02 6.1136−01 1.0992−01 4.0432−02 1.3794−01 2.6550−01 3.6356−02 7.0841−02 5.8258−01 1.3616−01 5.3277−01 1.2326−01 2.0692−03 1.0128+00 4.1191−04 1.5668−01 4.8320−02 9.6614−01 7.4312−03 1.4906−01 1.5351−01 2.9442−01 5.6599−01 5.1959−01 5.1697−03 8.8355−01 4.2295−02 8.4395−01 1.3433+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
1.6584+09 3.3042+09 5.2619+12 5.1146+12 2.3192+12 2.2743+12 1.1978+12 1.1782+12 1.2985+13 4.2346+12 1.9535+12 1.5395+13 4.9910+12 2.2955+12 2.1571+08 4.4502+08 6.8816+11 6.6537+11 3.7759+11 3.6809+11 3.7274+07 1.3663+12 6.7317+11 1.6271+07 1.6394+12 8.0251+11 9.0925+09 3.0271+12 3.9065+09 1.0002+12 2.1525+11 3.2322+12 7.0816+10 1.0662+12 5.0559+07 1.0560+08 1.6177+11 1.5596+11 1.1585+07 2.8304+11 5.0104+06 3.4177+11 3.5887+04 4.8642+09 5.6600+11 1.6902+01 8.0438+03 4.0420+10 6.0570+11 9.6280+11 1.6430+07 3.4515+07 4.1868+06 1.8042+06 1.8175+04 1.0772+01 4.2329+03 7.1401+02
1.6680+09 3.3100+09 5.3370+12 5.2020+12 2.4110+12 2.3730+12 1.3240+12 1.3070+12 1.3040+13 4.3020+12 2.0760+12 1.5480+13 5.0770+12 2.4350+12
1.5480+09 3.3930+09 5.4330+12 5.2700+12 1.9700+12 1.9270+12 1.0580+12 1.0390+12 1.3010+13 4.1670+12 1.9440+12 1.5410+13 4.9040+12 2.2810+12 1.8410+08 4.2800+08 6.3280+11 6.0820+11 3.5550+11 3.4520+11 4.2150+07 1.3580+12 6.7520+11 1.6270+07 1.6300+12 8.0490+11 2.5660+12 3.0400+12 1.3600+06 1.0030+12 2.1610+11 3.2450+12 7.0950+10 1.0690+12 5.5190+08 8.2890+08 1.4640+11 1.3960+11 3.4530+07 2.8070+11 1.8440+07 3.3960+11 4.0690+04 2.7310+11 5.6500+11 7.0400+00 7.6720+03 4.0350+10 6.0460+11 9.6120+11 1.5970+08 2.4260+08 8.7510+06 4.2630+06 2.0560+04 4.7010+00 4.0070+03 7.6510+02
1.9307−02 4.9008−02 1.2637−01 2.4400−01 3.1376−02 6.1403−02 1.3033−02 2.5613−02 6.7293−01 1.2216−01 4.5124−02 6.1154−01 1.0986−01 4.0396−02 3.2636−02 8.3532−02 1.3889−01 2.6637−01 3.6524−02 7.1002−02 2.7168−02 5.8217−01 1.3611−01 1.7470−02 5.3322−01 1.2329−01 2.0589−03 1.0125+00 4.1011−04 1.5667−01 4.8312−02 9.6594−01 7.4278−03 1.4904−01 4.5132−02 1.1582−01 1.5463−01 2.9541−01 4.8385−02 5.6550−01 3.1012−02 5.2014−01 4.1696−03 5.1462−03 8.8308−01 3.7188−05 2.3579−03 4.2295−02 8.4375−01 1.3430+00 5.7320−02 1.4726−01 6.7376−02 4.3129−02 7.7661−03 7.4800−05 4.4480−03 1.6746−03
GRASP: Present results from grasp. FAC: Present results from fac.
energy differences (∆Eij ) are very small and hence small changes in these affect the A-values significantly. One of the general criteria to assess the accuracy of radiative rates is to compare the length and velocity forms of the f - or Avalues. However, such comparisons are only desirable, and are not a fully sufficient test to assess accuracy, as different calculations (or combinations of configurations) may give comparable f -values in the two forms, but entirely different results in magnitude. Generally, there is good agreement between the length and velocity forms of the f -values for strong transitions, but differences between the two forms can sometimes be substantial even for some very strong transitions, as demonstrated by Aggarwal et al. [19]. However, for transitions of Li-like ions, there is no discrepancy between the two forms, and this is irrespective of the magnitude of a transition. Furthermore, to assess the importance of configuration interaction (CI), we have performed another calculation including the levels of the n = 6 configurations. Only for two transitions, namely 2–16 (2p 2 Po1/2 –5s 2 S1/2 ) and 3–16 (2p 2 Po3/2 –5s 2 S1/2 ), have the A-values decreased by 20% for Sc XIX and by 15% for Ni XXVI. For the remaining transitions the effect of additional CI is much less noticeable. Based on this and other comparisons discussed above, we may state that the A-values listed in Tables 9–16 from our grasp calculations are accurate to better than 20% for all transitions and all ions, and hence should be the best currently available.
6.9700+11 6.7460+11 3.9970+11 3.9010+11 1.3760+12 6.9390+11 1.6510+12 8.2620+11 9.2300+09 3.0260+12 4.2260+09 1.0020+12 2.1480+11 3.2330+12 7.0750+10 1.0690+12
1.6580+11 1.5990+11 2.8810+11 3.4760+11 4.9610+09 5.6480+11
4.0310+10 6.0470+11 9.6300+11
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
4. Lifetimes The lifetime τ for a level j is defined as follows: 1
τj =
Aji
.
(6)
i
Since this is a measurable parameter, it provides a check on the accuracy of the calculations. Therefore, in Tables 1–8 we have also listed our calculated lifetimes from grasp, which include
6
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table E Comparison of radiative rates (A-values, s−1 ) for some transitions in Mn XXIII. (a ± b ≡ a × 10±b ).
)
–
Table F Comparison of radiative rates (A-values, s−1 ) for some transitions in Fe XXIV. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.7445+09 3.7834+09 6.3020+12 6.1102+12 2.7742+12 2.7159+12 1.4322+12 1.4069+12 1.5516+13 5.0604+12 2.3345+12 1.8376+13 5.9545+12 2.7381+12 8.2540+11 7.9568+11 4.5238+11 4.4003+11 1.6324+12 8.0451+11 1.9588+12 9.5852+11 1.0822+10 3.6171+12 4.6506+09 1.1954+12 2.5710+11 3.8610+12 8.4564+10 1.2736+12 1.9416+11 1.8658+11 3.3810+11 4.0849+11 5.7920+09 6.7621+11 4.8291+10 7.2357+11 1.1503+12
1.7540+09 3.7890+09 6.3880+12 6.2120+12 2.8790+12 2.8290+12 1.5760+12 1.5550+12 1.5580+13 5.1380+12 2.4750+12 1.8480+13 6.0550+12 2.8980+12 8.3560+11 8.0640+11 4.7770+11 4.6530+11 1.6430+12 8.2830+11 1.9720+12 9.8560+11 1.0980+10 3.6160+12 5.0190+09 1.1970+12 2.5660+11 3.8630+12 8.4470+10 1.2770+12 1.9880+11 1.9120+11 3.4380+11 4.1510+11 5.9060+09 6.7500+11 4.8170+10 7.2250+11 1.1510+12
1.8494−02 4.8329−02 1.2707−01 2.4459−01 3.1482−02 6.1496−02 1.3068−02 2.5645−02 6.7245−01 1.2210−01 4.5105−02 6.1166−01 1.0980−01 4.0362−02 1.3976−01 2.6702−01 3.6677−02 7.1123−02 5.8162−01 1.3604−01 5.3359−01 1.2331−01 2.0495−03 1.0121+00 4.0846−04 1.5666−01 4.8302−02 9.6573−01 7.4243−03 1.4901−01 1.5566−01 2.9616−01 5.6484−01 5.2060−01 5.1247−03 8.8258−01 4.2294−02 8.4353−01 1.3428+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.8321+09 4.3461+09 7.4905+12 7.2436+12 3.2936+12 3.2188+12 1.6997+12 1.6673+12 1.8404+13 6.0027+12 2.7694+12 2.1770+13 7.0510+12 3.2417+12 9.8236+11 9.4404+11 5.3784+11 5.2195+11 1.9357+12 9.5426+11 2.3227+12 1.1363+12 1.2787+10 4.2896+12 5.4965+09 1.4179+12 3.0476+11 4.5773+12 1.0022+11 1.5099+12 2.3121+11 2.2143+11 4.0078+11 4.8453+11 6.8467+09 8.0181+11 5.7259+10 8.5786+11 1.3640+12
1.8420+09 4.3510+09 7.5880+12 7.3630+12 3.4130+12 3.3490+12 1.8630+12 1.8360+12 1.8480+13 6.0910+12 2.9300+12 2.1900+13 7.1670+12 3.4250+12 9.9410+11 9.5650+11 5.6670+11 5.5070+11 1.9480+12 9.8150+11 2.3380+12 1.1670+12 1.2980+10 4.2890+12 5.9190+09 1.4200+12 3.0420+11 4.5810+12 1.0010+11 1.5140+12 2.3650+11 2.2670+11 4.0730+11 4.9190+11 6.9800+09 8.0060+11 5.7120+10 8.5690+11 1.3640+12
1.7748−02 4.7827−02 1.2772−01 2.4502−01 3.1578−02 6.1563−02 1.3099−02 2.5668−02 6.7190−01 1.2204−01 4.5087−02 6.1173−01 1.0973−01 4.0328−02 1.4055−01 2.6748−01 3.6817−02 7.1209−02 5.8094−01 1.3596−01 5.3388−01 1.2332−01 2.0408−03 1.0117+00 4.0695−04 1.5664−01 4.8293−02 9.6551−01 7.4207−03 1.4899−01 1.5660−01 2.9667−01 5.6403−01 5.2096−01 5.1047−03 8.8205−01 4.2292−02 8.4330−01 1.3425+00
GRASP: Present results from grasp. FAC: Present results from fac.
GRASP: Present results from grasp. FAC: Present results from fac.
the contributions from four types of transitions (i.e., E1, E2, M1, and M2). To our knowledge, no measurements are available for lifetimes in most of the Li-like ions with 21 ≤ Z ≤ 28. However, Grandin et al. [20] have measured the lifetime for the 2p 2 Po3/2 level of Cr XXII to be 307 ± 20 ps, which agrees very well with our result and the other [21] calculated value of 303 ps. Froese-Fischer has calculated lifetimes for all the Li-like ions under discussion here and has posted results for some levels up to 4s 2 S1/2 on the website www.vuse.vanderbilt.edu/~cff/mchf_collection/. For all levels and ions the discrepancies between the Froese-Fischer results and our calculations are generally less than ∼10%. However, discrepancies between the two independent calculations for the 2p 2 Po1/2 level are significantly larger, up to a factor of two depending on the ion. In Table I we compare our calculations using grasp with her work using the mchf code for the 2p 2 Po1/2 level of Li-like ions with 11 ≤ Z ≤ 28. For ions up to Z = 22 (Ti XX), the two sets of lifetimes agree within 10%, but for heavier ions the discrepancy increases with increasing nuclear charge. As Z increases, the lifetimes in our calculations from grasp decrease for all ions. However, this is also the case in the mchf calculations, but only up to Z = 23. After that the mchf lifetimes increase with increasing Z and thus widen the discrepancy with our calculations from grasp. We have confidence in our calculations and hope the present results for all levels will be useful for future comparisons, and may also encourage experimentalists to measure lifetimes for the Li-like ions.
5. Collision strengths For the computation of collision strengths we have employed darc, which includes the relativistic effects in a systematic way, in both the target description and the scattering model. It is based on the jj coupling scheme, and uses the Dirac–Coulomb Hamiltonian in the R-matrix approach. The R-matrix radii adopted for Li-like ions with 21 ≤ Z ≤ 28 are 4.80, 4.48, 4.16, 4.00, 3.84, 3.68, 3.52, and 3.36 atomic units, respectively. For all eight ions, 56 continuum orbitals have been included for each channel angular momentum for the expansion of the wavefunction. This allows us to compute Ω up to an energy of 700, 800, 920, 1000, 1070, 1160, 1280, and 1400 Ryd, for 21 ≤ Z ≤ 28, respectively. Furthermore, these energy ranges are sufficient to calculate values of Υ up to Te = 107.8 K, (i.e., well above the temperature of maximum abundance of these ions in ionization equilibrium — see Bryans et al. [22]). The maximum number of channels for a partial wave is 108, and the corresponding size of the Hamiltonian matrix is 6086. To obtain convergence of Ω for all transitions and at all energies, we have included all partial waves with angular momentum J ≤ 60, although a larger number would have been preferable for the convergence of some allowed transitions, especially at higher energies. However, to account for the neglected higher partial waves, we have included a ‘‘top-up’’, based on the Coulomb–Bethe [23] approximation for allowed transitions and geometric series for others.
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables ( Table G Comparison of radiative rates (A-values, s−1 ) for some transitions in Co XXV. (a ± b ≡ a × 10±b ).
)
–
7
Table H Comparison of radiative rates (A-values, s−1 ) for some transitions in Ni XXVI. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.9213+09 5.0082+09 8.8414+12 8.5266+12 3.8833+12 3.7882+12 2.0032+12 1.9622+12 2.1679+13 7.0723+12 3.2630+12 2.5613+13 8.2923+12 3.8118+12 1.1609+12 1.1120+12 6.3497+11 6.1473+11 2.2794+12 1.1241+12 2.7350+12 1.3377+12 1.5009+10 5.0520+12 6.4531+09 1.6702+12 3.5876+11 5.3889+12 1.1795+11 1.7777+12 2.7337+11 2.6088+11 4.7176+11 5.7070+11 8.0395+09 9.4415+11 6.7423+10 1.0100+12 1.6061+12
1.9320+09 5.0130+09 8.9520+12 8.6650+12 4.0180+12 3.9370+12 2.1870+12 2.1540+12 2.1770+13 7.1730+12 3.4460+12 2.5770+13 8.4270+12 4.0200+12 1.1740+12 1.1260+12 6.6760+11 6.4740+11 2.2940+12 1.1550+12 2.7530+12 1.3730+12 1.5230+10 5.0520+12 6.9300+09 1.6730+12 3.5810+11 5.3940+12 1.1780+11 1.7820+12 2.7940+11 2.6680+11 4.7910+11 5.7900+11 8.1930+09 9.4290+11 6.7270+10 1.0090+12 1.6070+12
1.7061−02 4.7486−02 1.2831−01 2.4532−01 3.1664−02 6.1606−02 1.3126−02 2.5682−02 6.7127−01 1.2197−01 4.5070−02 6.1176−01 1.0967−01 4.0295−02 1.4128−01 2.6777−01 3.6944−02 7.1263−02 5.8014−01 1.3587−01 5.3411−01 1.2332−01 2.0327−03 1.0113+00 4.0555−04 1.5663−01 4.8282−02 9.6527−01 7.4170−03 1.4896−01 1.5746−01 2.9697−01 5.6308−01 5.2124−01 5.0862−03 8.8150−01 4.2291−02 8.4305−01 1.3422+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
2.0122+09 5.7889+09 1.0369+13 9.9716+12 4.5496+12 4.4298+12 2.3460+12 2.2945+12 2.5376+13 8.2804+12 3.8207+12 2.9943+13 9.6906+12 4.4538+12 2.6303+08 7.9566+08 1.3630+12 1.3011+12 7.4481+11 7.1927+11 9.1748+07 2.6669+12 1.3158+12 2.7488+07 3.2000+12 1.5647+12 1.7510+10 5.9119+12 7.5298+09 1.9549+12 4.1963+11 6.3040+12 1.3792+11 2.0796+12 6.1708+07 1.9002+08 3.2108+11 3.0528+11 2.8687+07 5.5170+11 8.5089+06 6.6787+11 1.5389+05 9.3819+09 1.1047+12 2.1655+01 2.9248+04 7.8884+10 1.1816+12 1.8792+12 2.0060+07 6.2283+07 1.0393+07 3.0712+06 7.6541+04 1.3801+01 1.4987+04 3.7657+03
2.0230+09 5.7940+09 1.0490+13 1.0130+13 4.7010+12 4.6000+12 2.5530+12 2.5110+12 2.5480+13 8.3950+12 4.0280+12 3.0130+13 9.8450+12 4.6900+12
1.9590+09 6.3140+09 1.0810+13 1.0380+13 4.1760+12 4.0690+12 1.8090+12 1.7710+12 2.5470+13 8.1070+12 3.8080+12 3.0000+13 9.4740+12 4.4300+12 2.4260+08 8.4070+08 1.2850+12 1.2190+12 6.3580+11 6.1100+11 1.0570+08 2.6390+12 1.3210+12 2.7010+07 3.1710+12 1.5710+12 4.9960+12 5.9380+12 1.5460+06 1.9600+12 4.2120+11 6.3290+12 1.3810+11 2.0840+12 6.7760+08 1.2810+09 2.6400+11 2.4650+11 1.0700+08 5.4630+11 4.6560+07 6.6310+11 1.7420+05 5.3220+11 1.1020+12 6.2430+00 2.8090+04 7.8700+10 1.1790+12 1.8750+12 1.2070+09 1.7500+09 2.3810+07 8.7950+06 8.6850+04 4.4410+00 1.4400+04 3.9950+03
1.6427−02 4.7293−02 1.2886−01 2.4548−01 3.1743−02 6.1628−02 1.3151−02 2.5689−02 6.7056−01 1.2191−01 4.5055−02 6.1175−01 1.0961−01 4.0262−02 2.7840−02 8.1123−02 1.4196−01 2.6789−01 3.7061−02 7.1287−02 2.9316−02 5.7923−01 1.3577−01 1.6634−02 5.3427−01 1.2332−01 2.0253−03 1.0108+00 4.0425−04 1.5662−01 4.8272−02 9.6503−01 7.4130−03 1.4893−01 3.8532−02 1.1271−01 1.5826−01 2.9709−01 5.2329−02 5.6198−01 2.9586−02 5.2144−01 5.4191−03 5.0691−03 8.8092−01 3.2295−05 2.9008−03 4.2289−02 8.4279−01 1.3419+00 4.8958−02 1.4344−01 7.2938−02 4.1184−02 1.0033−02 6.4969−05 5.4239−03 2.3324−03
GRASP: Present results from grasp. FAC: Present results from fac.
For illustration, in Figs. 1–3 we show the variation of Ω with angular momentum J for three transitions in Fe XXIV, namely 1–3 (2s 2 S1/2 –2p 2 Po3/2 ), 1–8 (2s 2 S1/2 –3d 2 D5/2 ), and 1–10 (2s 2 S1/2 –4p
2 o P1/2 ), respectively, and at five energies, 200, 400, 600, 800, and 1000 Ryd. Values of Ω have fully converged for all forbidden (such as 1–8) and most of the allowed (such as 1–10) transitions. However, for some allowed transitions, such as 1–3 shown in Fig. 1, our adopted range of partial waves (J ≤ 60) is not sufficient for the convergence of Ω at most of the energies, particularly above thresholds. For such transitions the top-up has been included as mentioned above, and has been found to be appreciable. A similar conclusion applies to the transitions in other Li-like ions. In Tables 17–24 we list our values of Ω for resonance transitions in Li-like ions with 21 ≤ Z ≤ 28 at energies above thresholds. The indices used to represent the levels of a transition have already been defined in Tables 1–8. Very limited data are available for comparison, as already stated in Section 1. Therefore, to make an accuracy assessment of the values of Ω , we have performed another calculation using fac. This code is also fully relativistic, and is based on the well-known and widely-used DW method. Furthermore, the same CI is included in fac as in the calculations from darc. Therefore, also included in Tables 17–24 for comparison purposes are the Ω values from fac at a single excited energy Ej , which corresponds to ∼ 500, 560, 600, 660, 750, 820, 900, and 980 Ryd for 21 ≤ Z ≤ 28, respectively. Generally, the two sets of Ω from darc and fac agree to within 20% for a majority of transitions. However, for ∼15% of the tran-
1.3780+12 1.3180+12 7.8170+11 7.5620+11 2.6830+12 1.3510+12 3.2200+12 1.6040+12 1.7770+10 5.9130+12 8.0710+09 1.9580+12 4.1880+11 6.3110+12 1.3770+11 2.0850+12
3.2800+11 3.1200+11 5.5990+11 6.7720+11 9.5590+09 1.1030+12
7.8720+10 1.1810+12 1.8800+12
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
sitions there are differences of over 20%, and for ∼5% the discrepancies between the two independent calculations are up to a factor of two. Most of the transitions for which the discrepancies are large are forbidden, and one of the main reasons is the anomalous behaviour of Ω in the calculations from fac. To illustrate this, in Fig. 4 we compare the two sets of Ω from darc and fac for three allowed transitions in Fe XXIV, namely 4–6 (3s 2 S1/2 –3p 2 Po3/2 ), 6–8 (3p 2 Po3/2 –3d 2 D5/2 ), and 10–12 (4p 2 o P1/2 –4d 2 D3/2 ).
For these three and many other allowed transitions there are no major discrepancies between the two sets of
8
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table I Comparison of lifetimes (τ , s) for the 2p 2 Po1/2 level of Li-like ions with 11 ≤ Z ≤ 28. (a ± b ≡ a × 10±b ). Ion
GRASP
MCHF
Na IX Mg X Al XI Si XII P XIII S XIV Cl XV Ar XVI K XVII Ca XVIII Sc XIX Ti XX V XXI Cr XXII Mn XXIII Fe XXIV Co XXV Ni XXVI
1.552−09 1.394−09 1.264−09 1.155−09 1.063−09 9.840−10 9.151−10 8.546−10 8.009−10 7.530−10 7.098−10 6.708−10 6.354−10 6.030−10 5.732−10 5.458−10 5.208−10 4.970−10
1.603−09 1.437−09 1.301−09 1.189−09 1.094−09 1.014−09 9.452−10 8.863−10 8.363−10 7.943−10 7.601−10 7.341−10 7.180−10 7.136−10 7.255−10 7.629−10 8.444−10 1.018−09
GRASP: Present results from grasp. MCHF: Earlier results from mchf.
Fig. 1. Partial collision strengths for the 2s 2 S1/2 –2p 2 Po3/2 (1–3) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
Fig. 3. Partial collision strengths for the 2s 2 S1/2 –4p 2 Po1/2 (1–10) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
(and some other) transitions are generally within 50%, but are up to a factor of two for a few, such as 12–16, 13–16, 16–18, 19–21, and 20–22. For some transitions, such as 6–11, there are differences over the entire energy range, while for others such as 8–13, the discrepancies are mainly at the lower end of the energy range, and completely disappear at large energies. In some cases, such as 10–13, the differences between the two sets of Ω are mainly at the higher end of the energy range due to a sudden anomaly in Ω from fac. Such anomalies are larger, up to an order of magnitude in the case of Ni XXVI, and common for all ions particularly for the 9–21, 9–22, and 21–24 transitions. Discrepancies in the values of Ω for some transitions from darc and fac are partly due to the differences in the methodology, that is, the R-matrix and DW methods, respectively, but mainly because fac is designed to generate a large amount of atomic data in a comparatively very short period of time, and without too much loss of accuracy. This aim is achieved by employing various interpolation and extrapolation techniques, which result in significant differences in the values of Ω for some transitions and at some energies, as noted above. Overall, we may state that for transitions for which there is no anomaly in the calculations of Ω from fac, the differences between the darc and fac calculations of collision strengths are generally lower than 20%. However, the discrepancies are significant for those transitions for which values of Ω from fac are anomalous. A similar conclusion applies to transitions in other Li-like ions. Finally, based on the comparisons made above as well as for other Li-like ions [7– 10], we estimate our results for Ω to be accurate to better than 20% for a majority of the transitions of all eight Li-like ions. 6. Effective collision strengths
Fig. 2. Partial collision strengths for the 2s 2 S1/2 –3d 2 D5/2 (1–8) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
Excitation rates, along with energy levels and radiative rates, are required for plasma modelling, and are determined from the collision strengths. Since the threshold energy region is dominated by numerous closed-channel (Feshbach) resonances, values of Ω need to be calculated using a fine energy mesh in order to accurately account for their contribution. Furthermore, in a hot plasma electrons have a wide distribution of velocities, and therefore values of Ω are generally weighted over a Maxwellian distribution as follows:
Ω , although there is a fall in magnitude in ΩFAC for these (and
Υ (Te ) =
some other) transitions at the lower end of the energy range for all ions. In Fig. 5 we show similar comparisons for three forbidden transitions, namely 6–11 (3p 2 Po3/2 –4p 2 Po3/2 ), 8–13 (3d 2 D5/2 –4d 2
D5/2 ), and 10–13 (4p 2 Po1/2 –4d 2 D5/2 ). Differences for these three
∞
Ω (Ej ) exp(−Ej /kTe )d(Ej /kTe ),
(7)
0
where k (= 6.334 × 10−6 Ryd/K) is Boltzmann constant, Te is electron temperature in K, and Ej is the electron energy (in Ryd) with respect to the final (excited) state. Once the value of Υ is
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Fig. 4. Comparison of collision strengths from our calculations using darc (continuous curves) and fac (broken curves) for the 4–6 (circles: 3s 2 S1/2 –3p 2 Po3/2 ), 6–8 (triangles: 3p 2 Po3/2 –3d2 D5/2 ), and 10–12 (stars: 4p 2 Po1/2 –4d 2 D3/2 ) allowed transitions in Fe XXIV.
Fig. 7. Collision strengths for the 2s 2 S1/2 –2p 2 Po3/2 (1–3) transition in Fe XXIV.
Fig. 5. Comparison of collision strengths from our calculations using darc (continuous curves) and fac (broken curves) for the 6–11 (triangles: 3p 2 Po3/2 –4p 2 o P3/2 ), 8–13 (stars: 3d 2 D5/2 –4d 2 D5/2 ), and 10–13 (circles: 4p 2 Po1/2 –4d 2 D5/2 ) forbidden transitions in Fe XXIV.
Fig. 8. Collision strengths for the 2p 2 Po1/2 –2p 2 Po3/2 (2–3) transition in Fe XXIV.
Fig. 9. Collision strengths for the 3d 2 D3/2 –3d 2 D5/2 (7–8) transition in Fe XXIV. 2
Fig. 6. Collision strengths for the 2s S1/2 –2p
2 o P1/2
(1–2) transition in Fe XXIV.
and
known the corresponding results for the excitation rate q(i, j) and de-excitation rate q(j, i) can be easily obtained from the following equations: q(i, j) =
8.63 × 10−6 1/2
ωi Te
Υ exp(−Eij /kTe ) cm s
3 −1
(8)
q(j, i) =
8.63 × 10−6 1/2
ωj Te
Υ cm3 s−1 ,
(9)
where, as above, ωi and ωj are the statistical weights of the lower (i) and upper (j) levels, respectively, and Eij is the transition energy. The contribution of resonances may enhance the values of Υ
10
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Fig. 10. Comparison of effective collision strengths for the 7–8 (circles: 3d 2 D3/2 –3d D5/2 ), 12–13 (triangles: 4d 2 D3/2 –4d 2 D5/2 ), and 14–15 (stars: 4f 2 Fo5/2 –4f 2 Fo7/2 ) transitions in Fe XXIV. Continuous and broken curves are from the present darc and earlier BPRM calculations [25], respectively. 2
over those of the background values of collision strengths (ΩB ), especially for the forbidden transitions, by up to a factor of ten (or even more) depending on the transition and/or the temperature. Similarly, values of Ω need to be calculated over a wide energy range (above thresholds) in order to obtain convergence of the integral in Eq. (7), as demonstrated in Fig. 7 of Ref. [24]. To delineate resonances, we have performed our calculations of Ω in the threshold region at over 73 000 energies, depending on the ion. Close to thresholds (∼0.1 Ryd above a threshold) the energy mesh is 0.001 Ryd, and away from thresholds is 0.002 Ryd. Thus, care has been taken to include as many resonances as possible, and with as fine a resolution as is computationally feasible. The density and importance of resonances can be appreciated from Figs. 6–8, where we show Ω in the threshold region for three transitions in Fe XXIV, namely 1–2 (2s 2 S1/2 –2p 2 Po1/2 ), 1–3
(2s 2 S1/2 –2p 2 Po3/2 ), and 2–3 (2p 2 Po1/2 –2p 2 Po3/2 ). Similar resonances are observed for transitions in other Li-like ions. These resonances affect the values of Υ particularly towards the lower end of the temperature range. Our calculated values of Υ are listed in Tables 25–32 over a wide temperature range up to 107.8 K, suitable for applications to astrophysical and laboratory plasmas. As stated in Section 1, there are no similar results available for comparison purposes for most of the ions. Therefore, as for collision strengths we have also calculated values of Υ from our non-resonant Ω data from fac, which are included in Tables 25–32 at the lowest and the highest calculated temperatures for each ion. This provides a comparison between the two independent calculations, and also gives an estimate of the importance of resonances. For example, at Te = 106.1 K, our resonance-resolved values of Υ differ by over 20% for 76 transitions (∼28%) in Sc XIX, and in some instances by up to a factor of five, see, for example, 2–4, 3–4, and 7–9. Many of these are resonance transitions, such as 1–5/6/7/8/10/11, and our results from darc are invariably higher due to the inclusion of resonances. However, at Te = 107.5 K, only 9 transitions differ by over 20%, with a maximum discrepancy of 30%. For the 21–24 (5f 2 Fo5/2 –5g 2 G9/2 ) transition, values of Υ from fac are higher by a factor of 5 because of a sudden rise in the corresponding values of Ω , as shown for the 10–13 transition in Fe XXIV in Fig. 5. Overall we may state that the contribution of resonances is more dominant and appreciable at lower temperatures. Similar conclusions apply for transitions in other Li-like ions. The only Li-like ion considered here for which results for Υ are available in the literature is Fe XXIV. Whiteford et al. [25] have reported values of Υ for all transitions among the lowest 24 levels
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over a wide range of electron temperature. They have adopted the standard R-matrix code of Berrington et al. [16] and have included one-body relativistic operators in the calculations, which may be nearly sufficient for a moderately heavy ion such as Fe XXIV. Furthermore, they included a comparable large range of partial waves with angular momentum J ≤ 58, but resolved resonances in the threshold region in a comparatively coarser energy mesh of ∼0.005 Ryd. Therefore, some differences are expected between their results for Υ and our calculations from the fully relativistic darc. A comparison between the two independent sets of Υ shows that, at the lowest common temperature of 105.6 K, for about 40% transitions the differences are over 20%. For most of these transitions the differences are within a factor of two, but in some instances are over an order of magnitude, such as 7–8, 12–13, 14–15, 19–20, 21–22, and 23–24. All of these transitions are forbidden, there is no (major) discrepancy between the Ω values from darc and fac, and there is no large variation of their Ω values with increasing energy (i.e., ΩB is quite stable). Therefore, the differences in the values of Υ should not be due to the corresponding differences in the values of Ω , but because of the contribution of resonances. However, all of these transitions belong to the same n and therefore their ∆Eij are very small, but resonances in the collision strengths are neither too dense nor too high in magnitude. In fact, 7–8 (3d 2 D3/2 –3d 2 D5/2 ) is the only transition for which both the thresholds range and resonances are appreciable, as shown in Fig. 9. In Fig. 10 we compare values of Υ from the BPRM calculations of Whiteford et al. [25] with our own from darc for three transitions, namely 7–8 (3d 2 D3/2 –3d 2 D5/2 ), 12–13 (4d 2 D3/2 –4d 2 D5/2 ), and 14–15 (4f 2 Fo5/2 –4f 2 Fo7/2 ). At the lowest common temperature of
105.6 K, values of Υ from the BPRM calculations are higher, by up to a factor of ∼70, for these three and some other transitions, as noted above. As the electron temperature increases the discrepancy between the two calculations decreases significantly, and towards the higher end of the temperature range the two independent calculations become comparable. In fact, for only 5 transitions (7–8, 12–13, 14–15, 21–22, and 23–24) do the values of Υ differ at the highest common temperature of 107.46 K by over 20%, and by up to a factor of 5. The resonances for the 7–8 transition are neither too high in magnitude nor dense (see Fig. 9), and hence cannot make a large contribution to the determination of Υ as shown by our calculations from darc. Clearly, the BPRM calculations of Υ have overestimated the contribution of resonances for these seven transitions. The main reason for such a large discrepancy between the two R-matrix calculations for a few transitions, particularly those between the degenerate levels of a state, is the limitation of the BPRM method, as recently discussed and demonstrated by Bautista et al. [26]. The jj coupling method adopted in darc includes fine-structure in the definition of channel coupling and hence gives a better representation of resonances, particularly for transitions within the degenerate levels of a state. These near-threshold resonances affect the subsequent results for Υ , especially at lower temperatures as shown in Fig. 10. We discuss this further below. Another source of higher values of Υ from the BPRM calculations of Whiteford et al. [25], for some transitions and at lower temperatures, could be their inclusion of higher levels of the 1snℓn′ ℓ′ configurations. These additional levels in the 486–580 Ryd energy range, well above the highest threshold of our calculations (i.e., ∼127 Ryd) may give rise to some resonances that may affect the values of Υ . However, although this may be true for the calculations of Υ at very high temperatures, such as Te = 107.4 K (equivalent to ∼163 Ryd), resonances will not contribute to Υ values at lower temperatures, such as Te = 105.6 K (equivalent to ∼2.52 Ryd) unless there are very high spurious resonances. Therefore, we are confident in our results listed in Tables 25–32, which are assessed to be accurate to better than ∼20% for a majority of transitions and
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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11
over a wide range of temperatures. However, the contribution of higher neglected resonances, from the 1s2 nℓ (n ≥ 6) and 1snℓn′ ℓ′ configurations, may affect these results towards the higher end of the temperature range, as discussed above, and particularly for transitions involving the levels of the n = 5 configurations. Finally, we note that differences in values of Υ between our calculations from darc and those of Whiteford et al. [25] for transitions in Fe XXIV are similar to those observed earlier for transitions in Ar XVI [10]. However, differences in the case of Fe XXIV are comparatively larger in magnitude apart from affecting a larger number of transitions. This may be due to two reasons. First, relativistic effects are comparatively more important for Fe XXIV than for Ar XVI. Second, Whiteford et al. adopted a coarser mesh of 0.005 Ryd to resolve resonances for transitions in Fe XXIV in comparison to 0.002 Ryd for Ar XVI, whereas our energy mesh for these two (and other) ions is better than 0.002 Ryd.
but there is no evidence of a similar (significant) effect for the transitions considered in this paper. We believe the present set of complete results for radiative and excitation rates for eight Li-like ions are probably the best currently available and will be highly useful for the modelling of a variety of plasmas.
7. Conclusions
References
In this paper we have presented results for energy levels and radiative rates for four types of transitions (E1, E2, M1, and M2) among the lowest 24 levels belonging to the n ≤ 5 configurations of Li-like ions with 21 ≤ Z ≤ 28. Additionally, lifetimes of all the levels have been reported, although measurements or other theoretical results are not available for comparison for most of the ions/levels. However, based on a variety of comparisons among various calculations from grasp and fac, our energy levels are assessed to be accurate to better than 1%, and the results for radiative rates, oscillator strengths, line strengths, and lifetimes are assessed to be accurate to better than 20% for a majority of strong transitions (levels). Similarly, the accuracy of our results for collision strengths and effective collision strengths is estimated to be better than 20% for a majority of the transitions. This accuracy estimate is based on the comparison made between two independent calculations performed with darc and fac, as well as with other results available in the literature, particularly for Fe XXIV. Additionally, we have considered a large range of partial waves to achieve convergence of Ω at all energies, included a wide energy range to accurately calculate the values of Υ up to Te = 107.8 K, and resolved resonances on a fine energy mesh to account for their contributions. Hence we see no obvious deficiency in our calculated results. However, the present results for effective collision strengths for transitions involving the levels of the n = 5 configurations may (perhaps) be improved by the inclusion of the levels of the n = 6 configurations, as has been noted for the A-values. Finally, we would like to note that inclusion of radiation and Auger damping may reduce the contribution of resonances, particularly at lower temperatures, for some of the transitions. However, it is certainly true for transitions involving the inner-shell, as demonstrated by Whiteford et al. [25],
[1] K.P. Dere, E. Landi, P.R. Young, G. Del Zanna, Astrophys. J. Suppl. Ser. 134 (2001) 331. [2] G.A. Doschek, U. Feldman, J. Phys. B 43 (2010) 232001. [3] F.B. Rosmej, D. Reiter, V.S Lisitsa, M. Bitter, O. Herzog, G. Bertschinger, H.J. Kunze, Plasma Phys. Contr. Fusion 41 (1999) 191. [4] S. Fujioka, H. Takabe, Y. Yamamoto, D. Salzman, F. Wang, H. Nishimura, Y. Li, Q. Dong, S. Wang, Y. Zhang, Y.J. Rhee, Y.W. Lee, J.M. Han, M. Tanabe, T. Fujiwara, Y. Nakabayashi, G. Zhao, J. Zhang, K. Mima, Nature Phys. 5 (2009) 821. [5] J.R. Lemen, J. Sylwester, R.D. Bentley, Advances Space Res. 6 (1986) 245. [6] N.J. Peacock, R. Barnsley, I.H. Coffey, R. Giannella, N.C. Hawkes, K.D. Lawson, I.M. Melnick, M.G. O’Mullane, M.A. Singleton, A. Patel, Fusion Eng. Design 3435 (1997) 171. [7] K.M. Aggarwal, F.P. Keenan, Phys. Scr. 70 (2004) 222. [8] K.M. Aggarwal, F.P. Keenan, R.F. Heeter, Phys. Scr. 81 (2010) 015303. [9] K.M. Aggarwal, F.P. Keenan, Phys. Scr. 82 (2010) 065302. [10] K.M. Aggarwal, F.P. Keenan, At. Data Nucl. Data Tables xx, 2012, in press, (http://dx.doi.org/10.1016/j.adt.2012.03.001). [11] S.N. Nahar, Astron. Astrophys. 389 (2002) 716. [12] H.L. Zhang, D.H. Sampson, C.J. Fontes, At. Data Nucl. Data Tables 44 (1990) 31. [13] I.P. Grant, B.J. McKenzie, P.H. Norrington, D.F. Mayers, N.C. Pyper, Comput. Phys. Commun. 21 (1980) 207. [14] M.F. Gu, Can. J. Phys. 86 (2008) 675. [15] K.M. Aggarwal, K. Hamada, A. Igarashi, V. Jonauskas, F.P. Keenan, S. Nakazaki, Astron. Astrophys. 484 (2008) 879. [16] K.A. Berrington, W.B. Eissner, P.H. Norrington, Comput. Phys. Commun. 92 (1995) 290. [17] A. Hibbert, J. Phys. B 36 (2003) 4703. [18] K.M. Aggarwal, F.P. Keenan, R. Kisielius, Astron. Astrophys. 420 (2004) 783. [19] K.M. Aggarwal, V. Tayal, G.P. Gupta, F.P. Keenan, At. Data Nucl. Data Tables 93 (2007) 615. [20] J.P. Grandin, M. Huet, X. Husson, D. Lecler, D. Touvet, J.P. Buchet, M.C. BuchetPoulizac, A. Denis, J. Desesquelles, M. Druetta, J. Physique 45 (1984) 1423. [21] K.T. Cheng, Y.K. Kim, J.P. Desclaux, At. Data Nucl. Data Tables 24 (1979) 95. [22] P. Bryans, E. Landi, D.W. Savin, Astrophys. J. 691 (2009) 1540. [23] A. Burgess, V.B. Sheorey, J. Phys. B 7 (1974) 2403. [24] K.M. Aggarwal, F.P. Keenan, Eur. Phys. J. D 46 (2008) 205. [25] A.D. Whiteford, N.R. Badnell, C.P. Ballance, S.D. Loch, M.G. O’Mullane, H.P. Summers, J. Phys. B 35 (2002) 3729. [26] M.A. Bautista, C.P. Ballance, P. Quinet, Astrophys. J. Lett. 718 (2010) L189.
Acknowledgment FPK is grateful to AWE Aldermaston for the award of a William Penney Fellowship. Appendix. Supplementary data Supplementary material related to this article can be found online at http://dx.doi.org/10.1016/j.adt.2011.05.002.
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Explanation of Tables
Table 1
Table 2
Table 3 Table 4 Table 5 Table 6 Table 7 Table 8 Table 9
Table 10
Table 11
Table 12
Table 13
Table 14
Table 15
Energy levels of Sc XIX, their threshold energies (in Ryd), and lifetimes (in s). Index Level Index Configuration The configuration to which the level belongs NIST Experimentally compiled energies from NIST (www.nist.gov/pml/data/asd.cfm) GRASP1 Present energies from grasp without Breit and QED corrections GRASP2 Present energies from grasp with Breit and QED corrections FAC Present energies from fac τ (s) Lifetime of the level in s Energy levels of Ti XX, their threshold energies (in Ryd), and lifetimes (in s). Index Level Index Configuration The configuration to which the level belongs NIST Experimentally compiled energies from NIST (www.nist.gov/pml/data/asd.cfm) GRASP1 Present energies from grasp without Breit and QED corrections GRASP2 Present energies from grasp with Breit and QED corrections FAC Present energies from fac BPRM Energies of Nahar [11] from the BPRM code [16] τ (s) Lifetime of the level in s Energy levels of V XXI, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Cr XXII, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 2. Energy levels of Mn XXIII, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Fe XXIV, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Co XXV, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Ni XXVI, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 2. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Sc XIX. i and j The lower (i) and upper (j) levels of a transition as defined in Table 1.
λij
Transition wavelength (in Å)
AE1 ji
Radiative transition probability (in s−1 ) for the E1 transitions
fijE1 E1
Absorption oscillator strength (dimensionless) for the E1 transitions
S
Line strength in atomic unit (a.u.), 1 a.u. = 6.460 × 10−36 cm2 esu2 for the E1 transitions
AE2 ji AjiM1 AjiM2
Radiative transition probability (in s−1 ) for the E2 transitions Radiative transition probability (in s−1 ) for the M1 transitions
Radiative transition probability (in s−1 ) for the M2 transitions a±b ≡ a × 10±b Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ti XX. Same as for Table 9 for transitions as defined in Table 2. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in V XXI. Same as for Table 9 for transitions as defined in Table 3. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Cr XXII. Same as for Table 9 for transitions as defined in Table 4. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Mn XXIII. Same as for Table 9 for transitions as defined in Table 5. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Fe XXIV. Same as for Table 9 for transitions as defined in Table 6. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Co XXV. Same as for Table 9 for transitions as defined in Table 7.
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table 16
Table 17
Table 18 Table 19 Table 20 Table 21 Table 22 Table 23 Table 24 Table 25
Table 26 Table 27 Table 28 Table 29 Table 30 Table 31 Table 32
)
–
Transition wavelengths (λij in Å), radiative rates (Aji in s ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ni XXVI. Same as for Table 9 for transitions as defined in Table 8. Collision strengths for resonance transitions in Sc XIX. Transition The lower (i) and upper (j) levels are defined in Table 1. Energy Energy (in Ryd) at which collision strengths obtained from the darc code are listed. FAC Collision strengths obtained from fac at a single excited energy of ∼500 Ryd. a±b ≡ a × 10±b Collision strengths for resonance transitions in Ti XX. Same as for Table 17 for levels defined in Table 2. Results from the FAC are at ∼560 Ryd. Collision strengths for resonance transitions in V XXI. Same as for Table 17 for levels defined in Table 3. Results from the FAC are at ∼600 Ryd. Collision strengths for resonance transitions in Cr XXII. Same as for Table 17 for levels defined in Table 4. Results from the FAC are at ∼660 Ryd. Collision strengths for resonance transitions in Mn XXIII. Same as for Table 17 for levels defined in Table 5. Results from the FAC are at ∼750 Ryd. Collision strengths for resonance transitions in Fe XXIV. Same as for Table 17 for levels defined in Table 6. Results from the FAC are at ∼820 Ryd. Collision strengths for resonance transitions in Co XXV. Same as for Table 17 for levels defined in Table 7. Results from the FAC are at ∼900 Ryd. Collision strengths for resonance transitions in Ni XXVI. Same as for Table 17 for levels defined in Table 8. Results from the FAC are at ∼980 Ryd. Effective collision strengths for transitions in Sc XIX. Transition The lower (i) and upper (j) levels are defined in Table 1. Temperature Temperatures (in log K) at which effective collision strengths from darc are listed. FAC Effective collision strengths from fac at the lowest (LHS) and the highest (RHS) temperature. a±b ≡ a × 10±b Effective collision strengths for transitions in Ti XX. Same as for Table 25 for levels defined in Table 2. Effective collision strengths for transitions in V XXI. Same as for Table 25 for levels defined in Table 3. Effective collision strengths for transitions in Cr XXII. Same as for Table 25 for levels defined in Table 4. Effective collision strengths for transitions in Mn XXIII. Same as for Table 25 for levels defined in Table 5. Effective collision strengths for transitions in Fe XXIV. Same as for Table 25 for levels defined in Table 6. Effective collision strengths for transitions in Co XXV. Same as for Table 25 for levels defined in Table 7. Effective collision strengths for transitions in Ni XXVI. Same as for Table 25 for levels defined in Table 8. −1
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Table 1 Experimental and theoretical energy levels (in Ryd) for Sc XIX and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.000 2.795 3.257 53.360 54.050 54.180 54.480 54.510
0.00000 2.80532 3.28673 53.28735 54.06380 54.20600 54.50117 54.54433 71.58356 71.90314 71.96299 72.08550 72.10374 72.11010 72.11915 79.97088 80.13250 80.16309 80.22533 80.23467 80.23825 80.24289 80.24296 80.24574
0.00000 2.80715 3.26772 53.25951 54.03701 54.17315 54.46362 54.50651 71.54981 71.86980 71.92713 72.04777 72.06586 72.07214 72.08119 79.93505 80.09689 80.12620 80.18750 80.19676 80.20030 80.20493 80.20500 80.20778
0.00000 2.81952 3.27812 53.26471 54.04351 54.17891 54.46530 54.50798 71.54525 71.86118 71.91811 72.05228 72.07013 72.06516 72.07420 79.92707 80.08757 80.11649 80.18900 80.19736 80.19810 80.19767 80.19305 80.20014
71.900 72.070 72.100 72.100 72.100 80.100 80.100 80.200 80.200
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 7.098−10 4.457−10 8.863−13 3.442−13 3.517−13 1.155−13 1.164−13 1.310−12 5.822−13 5.928−13 2.680−13 2.702−13 5.538−13 5.551−13 2.068−12 9.866−13 1.003−12 5.142−13 5.189−13 1.070−12 1.073−12 1.799−12 1.801−12
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 2 Experimental and theoretical energy levels (in Ryd) for Ti XX and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 2.94814 3.51495 58.92244 59.73921 59.90706 60.21762 60.27047 79.16195 79.50504 70.57585 79.70671 79.72894 79.73587 79.74498 88.44913 88.62437 88.66054 88.72752 88.73891
0.00000 2.95843 3.54785 58.94397 59.76326 59.93739 60.24985 60.30285 79.19708 79.53436 79.60766 79.73733 79.75972 79.76650 79.77762 88.48424 88.65482 88.69228 88.75816 88.76962 88.77345 88.77914 88.77921 88.78262
0.00000 2.96034 3.52549 58.91143 59.73184 59.89893 60.20592 60.25860 79.15763 79.49532 79.56569 79.69318 79.71540 79.72211 79.73322 88.44234 88.61314 88.64912 88.71390 88.72527 88.72904 88.73473 88.73480 88.73821
0.00000 2.97295 3.53597 58.91679 59.73847 59.90476 60.20768 60.26015 79.15313 79.48676 79.55669 79.69778 79.71973 79.71511 79.72622 88.43439 88.60387 88.63941 88.71542 88.72663 88.72179 88.72747 88.72717 88.73058
0.00000 2.90900 3.55600 58.96600 59.75200 59.94280 60.24240 60.30120 78.84310 79.47540 79.55750 79.75280 79.77760 79.78310 79.79539 88.33580 88.63940 88.68069 88.76910 88.78180 88.78500 88.79120 88.79090 88.79460
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 6.708−10 3.930−10 7.279−13 2.796−13 2.863−13 9.412−14 9.490−14 1.074−12 4.732−13 4.827−13 2.183−13 2.203−13 4.509−13 4.520−13 1.695−12 8.021−13 8.169−13 4.190−13 4.232−13 8.712−13 8.736−13 1.465−12 1.467−12
16
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 3 Experimental and theoretical energy levels (in Ryd) for V XXI and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.10227 3.79028 64.86700 65.72669 65.93063 66.25768 66.32192 87.16324 87.52438 87.61040 87.74818 87.77525
0.00000 3.11270 3.82747 64.89302 65.75546 65.96665 66.29641 66.36085 87.20456 87.55965 87.64854 87.78538 87.81261 87.81982 87.83333 97.43819 97.61780 97.66324 97.73275 97.74670 97.75075 97.75767 97.75774 97.76189
0.00000 3.11464 3.80137 64.85526 65.71887 65.92195 66.24540 66.30946 87.15875 87.51426 87.59979 87.73412 87.76114 87.76825 87.78176 97.38955 97.56937 97.61310 97.68135 97.69518 97.69919 97.70611 97.70618 97.71033
0.00000 3.12752 3.81195 64.86079 65.72564 65.92786 66.24724 66.31107 87.15432 87.50578 87.59082 87.73879 87.76553 87.76127 87.77477 97.38163 97.56014 97.60340 97.68291 97.69656 97.69194 97.69885 97.69854 97.70268
97.39659 97.58103 97.62495
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 6.354−10 3.454−10 6.030−13 2.294−13 2.354−13 7.743−14 7.814−14 8.889−13 3.885−13 3.970−13 1.796−13 1.814−13 3.708−13 3.718−13 1.402−12 6.588−13 6.720−13 3.447−13 3.485−13 7.164−13 7.186−13 1.205−12 1.207−12
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 4 Experimental and theoretical energy levels (in Ryd) for Cr XXII and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 3.25756 4.08607 71.10243 72.00541 72.25090 72.59445 72.67172 95.55729 95.93956 95.04008 96.18478 96.21741
0.00000 3.26819 4.12747 71.13598 72.04188 72.29581 72.64289 72.72052 95.60789 95.98091 96.08781 96.23182 96.26462 96.27225 96.28853 106.83485 107.02353 107.07817 107.15131 107.16812 107.17242 107.18076 107.18083 107.18583
0.00000 3.27012 4.09721 71.09246 71.99957 72.24420 72.58404 72.66124 95.55507 95.92852 96.03155 96.17268 96.20525 96.21277 96.22904 106.77873 106.96764 107.02031 107.09203 107.10870 107.11293 107.12126 107.12135 107.12634
0.00000 3.28326 4.10787 71.09813 72.00645 72.25014 72.58591 72.66286 95.55066 95.92004 96.02255 96.17736 96.20962 96.20573 96.22200 106.77079 106.95840 107.01057 107.09356 107.11003 107.10562 107.11395 107.11364 107.11864
0.00000 3.20500 4.14301 71.16300 72.02690 72.30380 72.63580 72.72100 95.07121 95.90580 96.02520 96.25730 96.29340 96.29900 96.31680 106.60690 107.01100 107.07090 107.17000 107.18851 107.19170 107.20090 107.20040 107.20580
106.78355 106.97719 107.03014 107.10413 107.12090
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 6.030−10 3.026−10 5.034−13 1.899−13 1.954−13 6.428−14 6.493−14 7.416−13 3.219−13 3.296−13 1.491−13 1.508−13 3.077−13 3.087−13 1.169−12 5.459−13 5.579−13 2.862−13 2.896−13 5.944−13 5.964−13 1.000−12 1.002−12
18
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 5 Experimental and theoretical energy levels (in Ryd) for Mn XXIII and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.41410 4.40374 77.63449 78.58111 78.87426 79.23412 79.32662 104.35010 104.74778 104.87135 105.02289 105.06198
0.00000 3.42497 4.44982 77.67440 78.62411 78.92703 79.29143 79.38419 104.40911 104.80020 104.92772 105.07890 105.11810 105.12616 105.14561 116.67639 116.87422 116.93939 117.01619 117.03627 117.04080 117.05077 117.05085 117.05682
0.00000 3.42684 4.41495 77.62454 78.57549 78.86780 79.22395 79.31622 104.34856 104.74007 104.86319 105.01109 105.05003 105.05795 105.07740 116.61206 116.81010 116.87304 116.94820 116.96812 116.97259 116.98255 116.98263 116.98860
0.00000 3.44029 4.42575 77.63040 78.58252 78.87383 79.22588 79.31790 104.34423 104.73168 104.85423 105.01585 105.05443 105.05092 105.07035 116.60416 116.80093 116.86331 116.94976 116.96948 116.96529 116.97523 116.97492 116.98089
116.61630 116.81924 116.88257 116.96003 116.98008
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.732−10 2.643−10 4.234−13 1.586−13 1.635−13 5.380−14 5.439−14 6.232−13 2.689−13 2.759−13 1.248−13 1.263−13 2.574−13 2.583−13 9.816−13 4.562−13 4.671−13 2.396−13 2.427−13 4.973−13 4.991−13 8.371−13 8.383−13
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 6 Experimental and theoretical energy levels (in Ryd) for Fe XXIV and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.57201 4.74549 84.49724 85.46045 85.81493 86.19675 86.32068 113.58397 113.98948 114.13529 114.26560 114.32027 114.34214 114.37860 126.89804 127.06161 127.13633 127.21744 127.26118
0.00000 3.58311 4.79661 84.50994 85.50381 85.86255 86.24429 86.35430 113.61034 114.01965 114.17065 114.32903 114.37552 114.38400 114.40707 126.96514 127.17218 127.24937 127.32980 127.35362 127.35839 127.37021 127.37029 127.37737
0.00000 3.58487 4.75665 84.45313 85.44825 85.79495 86.16734 86.27679 113.54131 113.95103 114.09705 114.25170 114.29788 114.30622 114.32928 126.89179 127.09904 127.17369 127.25228 127.27592 127.28061 127.29242 127.29250 127.29958
0.00000 3.59862 4.76759 84.45915 85.45541 85.80104 86.16928 86.27847 113.53700 113.94265 114.08807 114.25646 114.30227 114.29912 114.32217 126.88386 127.08985 127.16391 127.25381 127.27722 127.27324 127.28504 127.28473 127.29179
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.458−10 2.301−10 3.585−13 1.334−13 1.380−13 4.537−14 4.591−14 5.273−13 2.264−13 2.328−13 1.053−13 1.067−13 2.170−13 2.179−13 8.301−13 3.841−13 3.940−13 2.020−13 2.049−13 4.192−13 4.209−13 7.058−13 7.070−13
20
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 7 Experimental and theoretical energy levels (in Ryd) for Co XXV and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.73114 5.11313 91.59291 92.62747 93.03681 93.42911 93.55833 123.13879 123.57319 123.74578 123.91100 123.96558
0.00000 3.74268 5.17001 91.64433 92.68274 93.10475 93.50383 93.63341 123.21382 123.64148 123.81913 123.98470 124.03945 124.04836 124.07552 137.70354 137.91985 138.01065 138.09474 138.12279 138.12781 138.14171 138.14180 138.15015
0.00000 3.74427 5.12446 91.57992 92.61957 93.02801 93.41653 93.54547 123.13553 123.56358 123.73560 123.89697 123.95138 123.96011 123.98727 137.62033 137.83684 137.92479 138.00679 138.03464 138.03955 138.05347 138.05356 138.06189
0.00000 3.75836 5.13557 91.58613 92.62685 93.03418 93.41850 93.54715 123.13127 123.55524 123.72662 123.90176 123.95576 123.95298 123.98013 137.61240 137.82768 137.91498 138.00832 138.03590 138.03215 138.04604 138.04572 138.05406
137.62638 137.84810 137.93631 138.02078 138.04876
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.205−10 1.997−10 3.053−13 1.130−13 1.172−13 3.852−14 3.902−14 4.489−13 1.919−13 1.977−13 8.939−14 9.066−14 1.843−13 1.850−13 7.064−13 3.256−13 3.347−13 1.715−13 1.742−13 3.559−13 3.574−13 5.993−13 6.004−13
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 8 Experimental and theoretical energy levels (in Ryd) for Ni XXVI and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 3.89178 5.50927 99.02019 100.09931 100.57828 100.98671 101.13798 133.13657 133.58956 133.79150 133.96346 134.02734
0.00000 3.90376 5.57232 99.07935 100.16271 100.65613 101.07256 101.22420 133.22189 133.66806 133.87576 134.04854 134.11261 134.12195 134.15372 148.89410 149.11978 149.22594 149.31369 149.34651 149.35176 149.36804 149.36813 149.37788
0.00000 3.90511 5.52065 99.00668 100.09123 100.56940 100.97398 101.12491 133.13351 133.58003 133.78142 133.94948 134.01317 134.02229 134.05408 148.80017 149.02602 149.12897 149.21437 149.24698 149.25212 149.26840 149.26849 149.27824
0.00000 3.91952 5.53194 99.01307 100.09864 100.57562 100.97593 101.12655 133.12926 133.57172 133.77240 133.95422 134.01749 134.01509 134.04684 148.79221 149.01685 149.11909 149.21584 149.24818 149.24463 149.26088 149.26057 149.27032
0.00000 3.88501 5.70100 99.15861 100.21990 100.75800 101.14600 101.31030 132.58530 133.58981 133.82431 134.16301 134.23280 134.23880 134.27321 148.27220 149.16661 149.28311 149.41470 149.45050 149.45401 149.47160 149.47070 149.48120
148.80599 149.03718 149.14052 149.22836 149.26108
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 4.970−10 1.727−10 2.615−13 9.637−14 1.002−13 3.291−14 3.338−14 3.843−13 1.637−13 1.691−13 7.638−14 7.755−14 1.574−13 1.581−13 6.046−13 2.778−13 2.862−13 1.466−13 1.490−13 3.040−13 3.054−13 5.122−13 5.132−13
22
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 9 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Sc XIX. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
3.246+02 2.789+02 1.711+01 1.686+01 1.682+01 1.673+01 1.672+01 1.274+01 1.268+01 1.267+01 1.265+01 1.265+01 1.264+01 1.140+01 1.138+01 1.137+01 1.136+01 1.136+01 1.136+01 1.979+03 1.806+01 1.779+01 1.774+01 1.764+01 1.763+01 1.326+01 1.319+01 1.318+01 1.316+01 1.316+01 1.316+01 1.181+01 1.179+01 1.179+01 1.178+01 1.177+01 1.177+01 1.823+01 1.795+01 1.790+01 1.780+01 1.778+01 1.335+01 1.328+01 1.327+01 1.325+01 1.325+01 1.324+01 1.324+01 1.189+01 1.186+01 1.186+01 1.185+01 1.185+01 1.185+01 1.184+01 1.184+01 1.172+03 9.974+02 7.568+02 7.308+02 4.982+01 4.897+01 4.881+01 4.850+01 4.846+01 4.844+01 3.416+01 3.396+01 3.392+01 3.384+01 3.383+01 3.383+01
1.409+09 2.244+09 0.000+00 2.904+12 2.842+12 0.000+00 0.000+00 0.000+00 1.285+12 1.266+12 0.000+00 0.000+00 0.000+00 0.000+00 6.647+11 6.563+11 0.000+00 0.000+00 0.000+00 0.000+00 3.680+11 0.000+00 0.000+00 7.221+12 0.000+00 1.470+11 0.000+00 0.000+00 2.356+12 0.000+00 0.000+00 7.359+10 0.000+00 0.000+00 1.087+12 0.000+00 0.000+00 7.602+11 0.000+00 0.000+00 1.431+12 8.588+12 3.021+11 0.000+00 0.000+00 4.632+11 2.789+12 0.000+00 0.000+00 1.501+11 0.000+00 0.000+00 2.129+11 1.284+12 0.000+00 0.000+00 0.000+00 1.823+08 2.976+08 0.000+00 0.000+00 0.000+00 3.776+11 3.681+11 0.000+00 0.000+00 0.000+00 0.000+00 2.081+11 2.041+11 0.000+00 0.000+00 0.000+00
2.226−02 5.232−02 0.000+00 1.238−01 2.411−01 0.000+00 0.000+00 0.000+00 3.098−02 6.094−02 0.000+00 0.000+00 0.000+00 0.000+00 1.290−02 2.545−02 0.000+00 0.000+00 0.000+00 0.000+00 1.800−02 0.000+00 0.000+00 6.738−01 0.000+00 3.872−03 0.000+00 0.000+00 1.223−01 0.000+00 0.000+00 1.540−03 0.000+00 0.000+00 4.520−02 0.000+00 0.000+00 1.894−02 0.000+00 0.000+00 6.796−02 6.108−01 4.033−03 0.000+00 0.000+00 1.219−02 1.101−01 0.000+00 0.000+00 1.590−03 0.000+00 0.000+00 4.480−03 4.051−02 0.000+00 0.000+00 0.000+00 3.755−02 8.877−02 0.000+00 0.000+00 0.000+00 1.357−01 2.630−01 0.000+00 0.000+00 0.000+00 0.000+00 3.596−02 7.039−02 0.000+00 0.000+00 0.000+00
4.757−02 9.606−02 0.000+00 1.375−02 2.670−02 0.000+00 0.000+00 0.000+00 2.586−03 5.083−03 0.000+00 0.000+00 0.000+00 0.000+00 9.663−04 1.906−03 0.000+00 0.000+00 0.000+00 0.000+00 2.141−03 0.000+00 0.000+00 7.826−02 0.000+00 3.379−04 0.000+00 0.000+00 1.060−02 0.000+00 0.000+00 1.198−04 0.000+00 0.000+00 3.504−03 0.000+00 0.000+00 4.545−03 0.000+00 0.000+00 1.593−02 1.431−01 7.088−04 0.000+00 0.000+00 2.127−03 1.919−02 0.000+00 0.000+00 2.488−04 0.000+00 0.000+00 6.990−04 6.319−03 0.000+00 0.000+00 0.000+00 2.898−01 5.829−01 0.000+00 0.000+00 0.000+00 4.377−02 8.454−02 0.000+00 0.000+00 0.000+00 0.000+00 8.040−03 1.572−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.006+09 3.014+09 0.000+00 0.000+00 0.000+00 4.168+08 4.227+08 0.000+00 0.000+00 0.000+00 0.000+00 1.090+08 1.116+08 0.000+00 4.734−02 0.000+00 0.000+00 5.849+08 0.000+00 0.000+00 0.000+00 0.000+00 2.535+08 0.000+00 0.000+00 2.261+09 0.000+00 0.000+00 1.354+08 0.000+00 0.000+00 1.515+09 0.000+00 1.163+09 5.790+08 0.000+00 0.000+00 0.000+00 4.949+08 2.485+08 0.000+00 0.000+00 6.454+08 2.897+09 0.000+00 2.566+08 1.293+08 0.000+00 0.000+00 4.328+08 1.944+09 0.000+00 0.000+00 0.000+00 1.373+02 1.643+02 0.000+00 0.000+00 0.000+00 2.048+08 2.051+08 0.000+00 0.000+00 0.000+00 0.000+00 6.974+07 7.026+07 0.000+00
0.000+00 0.000+00 1.511+04 0.000+00 0.000+00 8.459+02 0.000+00 1.273+04 0.000+00 0.000+00 4.970+02 0.000+00 0.000+00 8.339+03 0.000+00 0.000+00 2.794+02 0.000+00 0.000+00 1.158+03 0.000+00 3.429+03 2.373+04 0.000+00 0.000+00 0.000+00 2.689+03 1.213+04 0.000+00 0.000+00 0.000+00 0.000+00 1.736+03 6.692+03 0.000+00 0.000+00 0.000+00 0.000+00 8.956+04 2.444+04 0.000+00 0.000+00 0.000+00 5.221+04 1.918+04 0.000+00 0.000+00 2.757+02 0.000+00 0.000+00 3.012+04 1.222+04 0.000+00 0.000+00 2.424+02 0.000+00 0.000+00 0.000+00 0.000+00 7.621−04 0.000+00 1.514+02 0.000+00 0.000+00 3.541+00 0.000+00 0.000+00 1.887+02 0.000+00 0.000+00 4.714+00 0.000+00 0.000+00
0.000+00 3.181+00 0.000+00 0.000+00 1.109+06 0.000+00 0.000+00 0.000+00 0.000+00 8.704+05 0.000+00 0.000+00 2.199−01 0.000+00 0.000+00 5.597+05 0.000+00 0.000+00 1.960−01 0.000+00 0.000+00 0.000+00 0.000+00 1.020+05 7.287+05 0.000+00 0.000+00 0.000+00 5.968+04 4.273+05 0.000+00 0.000+00 0.000+00 0.000+00 3.437+04 2.463+05 0.000+00 2.534+05 0.000+00 0.000+00 0.000+00 3.880+06 1.879+05 0.000+00 0.000+00 0.000+00 2.268+06 0.000+00 0.000+00 1.177+05 0.000+00 0.000+00 0.000+00 1.305+06 0.000+00 0.000+00 2.772−02 0.000+00 3.301−02 0.000+00 0.000+00 0.000+00 0.000+00 1.706+04 0.000+00 0.000+00 1.206−03 0.000+00 0.000+00 1.958+04 0.000+00 0.000+00 3.393−04
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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23
Table 9 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
6.693+03 2.136+03 1.941+03 5.203+01 5.110+01 5.094+01 5.060+01 5.054+01 5.053+01 3.519+01 3.497+01 3.493+01 3.485+01 3.483+01 3.483+01 3.137+03 2.734+03 5.244+01 5.149+01 5.133+01 5.098+01 5.093+01 5.091+01 5.089+01 3.537+01 3.515+01 3.511+01 3.503+01 3.502+01 3.501+01 3.501+01 3.501+01 2.125+04 5.333+01 5.235+01 5.218+01 5.182+01 5.177+01 5.175+01 5.172+01 3.578+01 3.555+01 3.551+01 3.542+01 3.541+01 3.541+01 3.540+01 3.540+01 5.347+01 5.248+01 5.231+01 5.195+01 5.190+01 5.188+01 5.185+01 3.584+01 3.561+01 3.557+01 3.548+01 3.547+01 3.547+01 3.546+01 3.546+01 3.546+01 2.848+03 2.415+03 1.830+03 1.766+03 1.745+03 1.087+02 1.066+02 1.062+02 1.055+02 1.054+02 1.053+02
0.000+00 1.946+07 0.000+00 1.027+11 0.000+00 0.000+00 7.595+11 0.000+00 0.000+00 4.976+10 0.000+00 0.000+00 3.741+11 0.000+00 0.000+00 1.226+06 1.116+07 2.118+11 0.000+00 0.000+00 1.524+11 9.113+11 0.000+00 0.000+00 1.020+11 0.000+00 0.000+00 7.451+10 4.467+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.404+10 5.126+09 0.000+00 0.000+00 1.683+12 0.000+00 0.000+00 2.318+10 2.201+09 0.000+00 0.000+00 5.558+11 0.000+00 0.000+00 0.000+00 0.000+00 4.683+10 0.000+00 0.000+00 1.198+11 1.798+12 0.000+00 0.000+00 2.009+10 0.000+00 0.000+00 3.944+10 5.932+11 0.000+00 0.000+00 4.268+07 7.027+07 0.000+00 0.000+00 0.000+00 0.000+00 8.856+10 8.613+10 0.000+00 0.000+00 0.000+00
0.000+00 2.663−02 0.000+00 4.170−02 0.000+00 0.000+00 5.830−01 0.000+00 0.000+00 9.236−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.809−03 1.875−02 4.366−02 0.000+00 0.000+00 5.938−02 5.316−01 0.000+00 0.000+00 9.570−03 0.000+00 0.000+00 1.371−02 1.232−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.110−02 2.093−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.196−03 4.160−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.281−02 0.000+00 0.000+00 4.834−02 9.665−01 0.000+00 0.000+00 2.540−03 0.000+00 0.000+00 7.438−03 1.491−01 0.000+00 0.000+00 5.189−02 1.229−01 0.000+00 0.000+00 0.000+00 0.000+00 1.509−01 2.916−01 0.000+00 0.000+00 0.000+00
0.000+00 3.745−01 0.000+00 1.429−02 0.000+00 0.000+00 1.942−01 0.000+00 0.000+00 2.140−03 0.000+00 0.000+00 3.125−02 0.000+00 0.000+00 7.474−02 6.748−01 3.015−02 0.000+00 0.000+00 3.987−02 3.565−01 0.000+00 0.000+00 4.458−03 0.000+00 0.000+00 6.322−03 5.680−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.654−03 1.438−03 0.000+00 0.000+00 6.907−01 0.000+00 0.000+00 1.028−03 1.945−04 0.000+00 0.000+00 7.306−02 0.000+00 0.000+00 0.000+00 0.000+00 1.323−02 0.000+00 0.000+00 4.953−02 9.899−01 0.000+00 0.000+00 1.785−03 0.000+00 0.000+00 5.210−03 1.044−01 0.000+00 0.000+00 9.731−01 1.954+00 0.000+00 0.000+00 0.000+00 0.000+00 1.059−01 2.040−01 0.000+00 0.000+00 0.000+00
3.953−03 0.000+00 0.000+00 0.000+00 0.000+00 6.192+07 0.000+00 0.000+00 2.310+08 0.000+00 0.000+00 3.509+07 0.000+00 0.000+00 2.516+06 0.000+00 0.000+00 0.000+00 1.235+08 6.152+07 0.000+00 0.000+00 6.437+07 2.903+08 0.000+00 6.864+07 3.446+07 0.000+00 0.000+00 5.617+05 2.635+06 0.000+00 1.784−06 2.170+07 0.000+00 0.000+00 3.929+07 1.122+07 0.000+00 0.000+00 1.316+07 0.000+00 0.000+00 1.890+07 5.415+06 0.000+00 0.000+00 4.916+08 3.258+07 0.000+00 0.000+00 1.679+07 4.477+07 0.000+00 0.000+00 1.972+07 0.000+00 0.000+00 8.051+06 2.153+07 0.000+00 0.000+00 5.458+07 5.454+08 0.000+00 0.000+00 2.371+01 2.842+01 0.000+00 0.000+00 0.000+00 0.000+00 2.827+07 2.829+07 0.000+00
2.995+01 0.000+00 0.000+00 0.000+00 4.325+01 1.342+03 0.000+00 0.000+00 0.000+00 0.000+00 5.189+01 9.408+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.694+03 3.080+02 0.000+00 0.000+00 9.553+00 0.000+00 0.000+00 2.851+03 3.691+02 0.000+00 0.000+00 4.609+00 0.000+00 0.000+00 1.124+00 4.766−02 0.000+00 0.000+00 1.132+02 8.779+01 0.000+00 0.000+00 2.881−02 0.000+00 0.000+00 1.168+02 5.238+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.339+02 3.744+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.491+02 3.863+02 0.000+00 0.000+00 8.520+00 0.000+00 0.000+00 0.000+00 3.250−05 0.000+00 0.000+00 5.214+00 0.000+00 0.000+00 5.131−02 0.000+00 0.000+00
0.000+00 1.879−05 2.168−04 0.000+00 0.000+00 0.000+00 1.308+03 9.299+03 0.000+00 0.000+00 0.000+00 0.000+00 1.357+03 9.663+03 0.000+00 0.000+00 2.135−04 8.512+03 0.000+00 0.000+00 0.000+00 5.026+04 0.000+00 0.000+00 9.015+03 0.000+00 0.000+00 0.000+00 5.209+04 0.000+00 0.000+00 3.910−03 0.000+00 0.000+00 8.722+01 0.000+00 0.000+00 0.000+00 1.649+04 2.116+04 0.000+00 8.119+01 0.000+00 0.000+00 0.000+00 1.162+04 1.493+04 0.000+00 0.000+00 9.393+02 2.454+03 0.000+00 0.000+00 0.000+00 1.446+05 0.000+00 8.748+02 2.277+03 0.000+00 0.000+00 0.000+00 1.019+05 0.000+00 0.000+00 0.000+00 1.329−03 0.000+00 0.000+00 4.403−12 0.000+00 0.000+00 8.425+02 0.000+00 0.000+00 1.820−05
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24
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 9 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.589+04 5.120+03 4.648+03 4.503+03 1.130+02 1.108+02 1.104+02 1.096+02 1.094+02 1.094+02 7.554+03 6.569+03 6.284+03 5.915+03 1.138+02 1.115+02 1.111+02 1.103+02 1.102+02 1.102+02 1.101+02 1.101+02 5.038+04 3.738+04 2.726+04 1.155+02 1.132+02 1.128+02 1.119+02 1.118+02 1.118+02 1.117+02 1.117+02 1.449+05 5.941+04 1.158+02 1.135+02 1.131+02 1.122+02 1.121+02 1.120+02 1.120+02 1.120+02 1.119+02 1.007+05 1.159+02 1.136+02 1.131+02 1.123+02 1.122+02 1.121+02 1.121+02 1.121+02 1.120+02 1.133+02 1.124+02 1.123+02 1.122+02 1.122+02 1.122+02 1.121+02 5.631+03 4.767+03 3.610+03 3.482+03 3.436+03 3.109+04 1.006+04 9.124+03 8.812+03 1.486+04 1.292+04 1.230+04 1.157+04 1.156+04
0.000+00 6.023+06 0.000+00 0.000+00 3.531+10 0.000+00 0.000+00 1.574+11 0.000+00 0.000+00 3.746+05 3.425+06 0.000+00 0.000+00 7.268+10 0.000+00 0.000+00 3.178+10 1.897+11 0.000+00 0.000+00 0.000+00 0.000+00 1.082+04 0.000+00 0.000+00 2.870+10 2.738+09 0.000+00 0.000+00 3.148+11 0.000+00 0.000+00 1.326+01 2.889+03 0.000+00 0.000+00 2.497+10 0.000+00 0.000+00 2.248+10 3.370+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.774+09 3.164+08 0.000+00 0.000+00 5.354+11 0.000+00 0.000+00 0.000+00 6.385+09 0.000+00 0.000+00 1.980+10 5.547+11 1.386+07 2.291+07 0.000+00 0.000+00 0.000+00 0.000+00 2.172+06 0.000+00 0.000+00 1.344+05 1.232+06 0.000+00 0.000+00 0.000+00
0.000+00 4.734−02 0.000+00 0.000+00 6.759−02 0.000+00 0.000+00 5.664−01 0.000+00 0.000+00 3.205−03 3.324−02 0.000+00 0.000+00 7.055−02 0.000+00 0.000+00 5.799−02 5.181−01 0.000+00 0.000+00 0.000+00 0.000+00 3.401−03 0.000+00 0.000+00 2.757−02 5.223−03 0.000+00 0.000+00 8.844−01 0.000+00 0.000+00 4.173−05 2.038−03 0.000+00 0.000+00 3.190−02 0.000+00 0.000+00 4.230−02 8.443−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.537−03 5.968−04 0.000+00 0.000+00 1.344+00 0.000+00 0.000+00 0.000+00 9.052−03 0.000+00 0.000+00 3.734−02 1.307+00 6.589−02 1.561−01 0.000+00 0.000+00 0.000+00 0.000+00 6.587−02 0.000+00 0.000+00 4.452−03 4.620−02 0.000+00 0.000+00 0.000+00
0.000+00 1.596+00 0.000+00 0.000+00 5.028−02 0.000+00 0.000+00 4.086−01 0.000+00 0.000+00 3.188−01 2.875+00 0.000+00 0.000+00 1.057−01 0.000+00 0.000+00 8.424−02 7.519−01 0.000+00 0.000+00 0.000+00 0.000+00 1.674+00 0.000+00 0.000+00 4.111−02 7.759−03 0.000+00 0.000+00 1.302+00 0.000+00 0.000+00 1.194−01 2.392+00 0.000+00 0.000+00 7.125−02 0.000+00 0.000+00 9.359−02 1.867+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.894−02 1.322−03 0.000+00 0.000+00 2.974+00 0.000+00 0.000+00 0.000+00 2.677−02 0.000+00 0.000+00 1.103−01 3.860+00 2.443+00 4.902+00 0.000+00 0.000+00 0.000+00 0.000+00 4.362+00 0.000+00 0.000+00 8.715−01 7.857+00 0.000+00 0.000+00 0.000+00
5.889−04 0.000+00 0.000+00 1.252−01 0.000+00 0.000+00 1.098+07 0.000+00 0.000+00 3.667+07 0.000+00 0.000+00 6.746−03 4.118−02 0.000+00 2.190+07 1.092+07 0.000+00 0.000+00 1.028+07 4.636+07 0.000+00 3.815−07 0.000+00 0.000+00 6.680+06 0.000+00 0.000+00 8.786+06 2.509+06 0.000+00 0.000+00 4.290+07 0.000+00 0.000+00 1.002+07 0.000+00 0.000+00 3.758+06 1.002+07 0.000+00 0.000+00 4.728+06 4.736+07 3.060−09 0.000+00 2.352+06 3.307+05 0.000+00 0.000+00 6.172+06 7.716+05 0.000+00 0.000+00 1.988+06 0.000+00 0.000+00 1.027+06 6.421+06 0.000+00 0.000+00 0.000+00 0.000+00 5.439+00 6.527+00 0.000+00 1.294−04 0.000+00 0.000+00 4.256−02 0.000+00 0.000+00 2.294−03 1.400−02 0.000+00
2.238+00 0.000+00 0.000+00 0.000+00 0.000+00 1.621+00 1.458+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.033−07 0.000+00 0.000+00 3.527+02 1.154+01 0.000+00 0.000+00 2.372−01 0.000+00 0.000+00 8.432−02 0.000+00 0.000+00 5.150−03 0.000+00 0.000+00 5.417+00 1.288+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.456+01 1.792+01 0.000+00 0.000+00 3.308−01 0.000+00 1.131−02 0.000+00 0.000+00 2.837−04 0.000+00 0.000+00 7.881+00 1.849+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.333+00 1.854+01 0.000+00 0.000+00 0.000+00 0.000+00 2.413−06 0.000+00 0.000+00 2.991−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.479−08 0.000+00 0.000+00
0.000+00 1.013−06 1.173−05 0.000+00 0.000+00 0.000+00 0.000+00 5.786+01 4.105+02 0.000+00 0.000+00 1.136−05 0.000+00 0.000+00 6.200+02 0.000+00 0.000+00 0.000+00 2.236+03 0.000+00 0.000+00 2.408−05 0.000+00 2.034−10 1.264−09 0.000+00 9.896+00 0.000+00 0.000+00 0.000+00 6.618+02 8.475+02 0.000+00 0.000+00 1.770−10 0.000+00 1.065+02 2.799+02 0.000+00 0.000+00 0.000+00 5.814+03 0.000+00 0.000+00 0.000+00 1.335−08 0.000+00 0.000+00 1.414+01 0.000+00 0.000+00 0.000+00 2.846+03 1.489+03 0.000+00 2.429+01 1.097+02 0.000+00 0.000+00 0.000+00 1.376+04 0.000+00 1.113−04 0.000+00 0.000+00 2.809−13 0.000+00 9.478−08 1.099−06 0.000+00 0.000+00 1.057−06 0.000+00 0.000+00 2.086−16
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)
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25
Table 9 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
9.843+04 7.120+04 5.227+04 5.208+04 2.573+05 1.115+05 1.106+05 8.271+04 1.967+05 1.940+05 1.219+05 1.416+07 3.206+05 3.280+05
0.000+00 5.595+03 0.000+00 0.000+00 8.456+00 1.562+03 0.000+00 0.000+00 0.000+00 1.668+02 0.000+00 1.586−05 3.831+01 0.000+00
0.000+00 6.378−03 0.000+00 0.000+00 8.394−05 3.880−03 0.000+00 0.000+00 0.000+00 1.254−03 0.000+00 4.768−07 7.378−04 0.000+00
0.000+00 5.979+00 0.000+00 0.000+00 4.266−01 8.543+00 0.000+00 0.000+00 0.000+00 4.805+00 0.000+00 1.778−01 6.229+00 0.000+00
9.627−08 0.000+00 0.000+00 3.245−06 0.000+00 0.000+00 8.335−09 3.568−07 1.053−09 0.000+00 0.000+00 0.000+00 0.000+00 2.662−11
1.131−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.877−12 0.000+00 1.519−03 0.000+00 0.000+00 0.000+00 0.000+00 3.396−04
0.000+00 2.900−11 1.742−10 0.000+00 0.000+00 2.719−11 0.000+00 0.000+00 0.000+00 2.958−13 1.579−12 0.000+00 1.164−13 0.000+00
26
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 10 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Ti XX. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
3.078+02 2.585+02 1.547+01 1.526+01 1.521+01 1.514+01 1.512+01 1.151+01 1.146+01 1.145+01 1.144+01 1.143+01 1.143+01 1.030+01 1.028+01 1.028+01 1.027+01 1.027+01 1.027+01 1.612+03 1.629+01 1.605+01 1.600+01 1.592+01 1.590+01 1.196+01 1.191+01 1.190+01 1.188+01 1.187+01 1.187+01 1.066+01 1.064+01 1.064+01 1.063+01 1.062+01 1.062+01 1.645+01 1.621+01 1.617+01 1.608+01 1.606+01 1.205+01 1.199+01 1.198+01 1.196+01 1.196+01 1.196+01 1.196+01 1.073+01 1.071+01 1.070+01 1.070+01 1.070+01 1.069+01 1.069+01 1.069+01 1.111+03 9.228+02 7.040+02 6.764+02 4.501+01 4.427+01 4.412+01 4.385+01 4.380+01 4.379+01 3.086+01 3.068+01 3.064+01 3.058+01 3.057+01 3.056+01
1.491+09 2.545+09 0.000+00 3.575+12 3.491+12 0.000+00 0.000+00 0.000+00 1.580+12 1.554+12 0.000+00 0.000+00 0.000+00 0.000+00 8.168+11 8.054+11 0.000+00 0.000+00 0.000+00 0.000+00 4.470+11 0.000+00 0.000+00 8.866+12 0.000+00 1.788+11 0.000+00 0.000+00 2.892+12 0.000+00 0.000+00 8.960+10 0.000+00 0.000+00 1.334+12 0.000+00 0.000+00 9.269+11 0.000+00 0.000+00 1.755+12 1.053+13 3.687+11 0.000+00 0.000+00 5.676+11 3.419+12 0.000+00 0.000+00 1.833+11 0.000+00 0.000+00 2.608+11 1.573+12 0.000+00 0.000+00 0.000+00 1.933+08 3.392+08 0.000+00 0.000+00 0.000+00 4.659+11 4.530+11 0.000+00 0.000+00 0.000+00 0.000+00 2.563+11 2.509+11 0.000+00 0.000+00 0.000+00
2.118−02 5.098−02 0.000+00 1.247−01 2.423−01 0.000+00 0.000+00 0.000+00 3.113−02 6.113−02 0.000+00 0.000+00 0.000+00 0.000+00 1.295−02 2.552−02 0.000+00 0.000+00 0.000+00 0.000+00 1.778−02 0.000+00 0.000+00 6.736−01 0.000+00 3.833−03 0.000+00 0.000+00 1.223−01 0.000+00 0.000+00 1.527−03 0.000+00 0.000+00 4.517−02 0.000+00 0.000+00 1.881−02 0.000+00 0.000+00 6.801−02 6.111−01 4.012−03 0.000+00 0.000+00 1.218−02 1.100−01 0.000+00 0.000+00 1.582−03 0.000+00 0.000+00 4.474−03 4.047−02 0.000+00 0.000+00 0.000+00 3.575−02 8.662−02 0.000+00 0.000+00 0.000+00 1.369−01 2.644−01 0.000+00 0.000+00 0.000+00 0.000+00 3.617−02 7.064−02 0.000+00 0.000+00 0.000+00
4.292−02 8.676−02 0.000+00 1.253−02 2.427−02 0.000+00 0.000+00 0.000+00 2.349−03 4.610−03 0.000+00 0.000+00 0.000+00 0.000+00 8.768−04 1.727−03 0.000+00 0.000+00 0.000+00 0.000+00 1.906−03 0.000+00 0.000+00 7.060−02 0.000+00 3.018−04 0.000+00 0.000+00 9.562−03 0.000+00 0.000+00 1.072−04 0.000+00 0.000+00 3.160−03 0.000+00 0.000+00 4.075−03 0.000+00 0.000+00 1.440−02 1.293−01 6.365−04 0.000+00 0.000+00 1.919−03 1.732−02 0.000+00 0.000+00 2.236−04 0.000+00 0.000+00 6.302−04 5.700−03 0.000+00 0.000+00 0.000+00 2.614−01 5.263−01 0.000+00 0.000+00 0.000+00 3.990−02 7.681−02 0.000+00 0.000+00 0.000+00 0.000+00 7.307−03 1.425−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.060+09 4.073+09 0.000+00 0.000+00 0.000+00 5.578+08 5.666+08 0.000+00 0.000+00 0.000+00 0.000+00 1.448+08 1.487+08 0.000+00 1.073−01 0.000+00 0.000+00 7.954+08 0.000+00 0.000+00 0.000+00 0.000+00 3.451+08 0.000+00 0.000+00 3.075+09 0.000+00 0.000+00 1.847+08 0.000+00 0.000+00 2.060+09 0.000+00 1.580+09 7.866+08 0.000+00 0.000+00 0.000+00 6.719+08 3.376+08 0.000+00 0.000+00 8.778+08 3.940+09 0.000+00 3.486+08 1.758+08 0.000+00 0.000+00 5.884+08 2.642+09 0.000+00 0.000+00 0.000+00 1.606+02 1.969+02 0.000+00 0.000+00 0.000+00 2.776+08 2.780+08 0.000+00 0.000+00 0.000+00 0.000+00 9.408+07 9.486+07 0.000+00
0.000+00 0.000+00 2.504+04 0.000+00 0.000+00 1.402+03 0.000+00 2.111+04 0.000+00 0.000+00 8.230+02 0.000+00 0.000+00 1.383+04 0.000+00 0.000+00 4.622+02 0.000+00 0.000+00 2.139+03 0.000+00 5.723+03 3.963+04 0.000+00 0.000+00 0.000+00 4.487+03 2.026+04 0.000+00 0.000+00 0.000+00 0.000+00 2.898+03 1.118+04 0.000+00 0.000+00 0.000+00 0.000+00 1.492+05 4.062+04 0.000+00 0.000+00 0.000+00 8.698+04 3.188+04 0.000+00 0.000+00 4.603+02 0.000+00 0.000+00 5.017+04 2.031+04 0.000+00 0.000+00 4.046+02 0.000+00 0.000+00 0.000+00 0.000+00 1.154−03 0.000+00 2.517+02 0.000+00 0.000+00 5.912+00 0.000+00 0.000+00 3.139+02 0.000+00 0.000+00 7.862+00 0.000+00 0.000+00
0.000+00 4.199+00 0.000+00 0.000+00 1.666+06 0.000+00 0.000+00 0.000+00 0.000+00 1.307+06 0.000+00 0.000+00 4.049−01 0.000+00 0.000+00 8.407+05 0.000+00 0.000+00 3.614−01 0.000+00 0.000+00 0.000+00 0.000+00 1.537+05 1.099+06 0.000+00 0.000+00 0.000+00 8.990+04 6.442+05 0.000+00 0.000+00 0.000+00 0.000+00 5.177+04 3.713+05 0.000+00 3.793+05 0.000+00 0.000+00 0.000+00 5.833+06 2.814+05 0.000+00 0.000+00 0.000+00 3.409+06 0.000+00 0.000+00 1.764+05 0.000+00 0.000+00 0.000+00 1.960+06 0.000+00 0.000+00 5.121−02 0.000+00 4.395−02 0.000+00 0.000+00 0.000+00 0.000+00 2.570+04 0.000+00 0.000+00 2.214−03 0.000+00 0.000+00 2.950+04 0.000+00 0.000+00 6.181−04
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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27
Table 10 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
5.454+03 1.922+03 1.730+03 4.691+01 4.611+01 4.594+01 4.565+01 4.560+01 4.559+01 3.174+01 3.155+01 3.151+01 3.144+01 3.143+01 3.143+01 2.968+03 2.534+03 4.732+01 4.650+01 4.633+01 4.604+01 4.599+01 4.597+01 4.594+01 3.193+01 3.174+01 3.170+01 3.162+01 3.161+01 3.161+01 3.160+01 3.160+01 1.730+04 4.808+01 4.724+01 4.707+01 4.676+01 4.671+01 4.669+01 4.667+01 3.227+01 3.208+01 3.204+01 3.197+01 3.195+01 3.195+01 3.194+01 3.194+01 4.822+01 4.737+01 4.720+01 4.689+01 4.683+01 4.682+01 4.679+01 3.233+01 3.214+01 3.210+01 3.203+01 3.201+01 3.201+01 3.200+01 3.200+01 3.200+01 2.698+03 2.233+03 1.702+03 1.634+03 1.614+03 9.815+01 9.637+01 9.601+01 9.536+01 9.525+01 9.521+01
0.000+00 2.410+07 0.000+00 1.250+11 0.000+00 0.000+00 9.327+11 0.000+00 0.000+00 6.059+10 0.000+00 0.000+00 4.595+11 0.000+00 0.000+00 1.305+06 1.264+07 2.585+11 0.000+00 0.000+00 1.872+11 1.119+12 0.000+00 0.000+00 1.246+11 0.000+00 0.000+00 9.146+10 5.483+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.640+10 6.263+09 0.000+00 0.000+00 2.067+12 0.000+00 0.000+00 2.848+10 2.690+09 0.000+00 0.000+00 6.826+11 0.000+00 0.000+00 0.000+00 0.000+00 5.731+10 0.000+00 0.000+00 1.471+11 2.208+12 0.000+00 0.000+00 2.459+10 0.000+00 0.000+00 4.840+10 7.283+11 0.000+00 0.000+00 4.526+07 8.024+07 0.000+00 0.000+00 0.000+00 0.000+00 1.094+11 1.061+11 0.000+00 0.000+00 0.000+00
0.000+00 2.669−02 0.000+00 4.123−02 0.000+00 0.000+00 5.828−01 0.000+00 0.000+00 9.152−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.724−03 1.825−02 4.338−02 0.000+00 0.000+00 5.949−02 5.322−01 0.000+00 0.000+00 9.523−03 0.000+00 0.000+00 1.371−02 1.232−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.111−02 2.080−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.197−03 4.139−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.276−02 0.000+00 0.000+00 4.833−02 9.663−01 0.000+00 0.000+00 2.532−03 0.000+00 0.000+00 7.434−03 1.491−01 0.000+00 0.000+00 4.942−02 1.200−01 0.000+00 0.000+00 0.000+00 0.000+00 1.523−01 2.932−01 0.000+00 0.000+00 0.000+00
0.000+00 3.378−01 0.000+00 1.273−02 0.000+00 0.000+00 1.752−01 0.000+00 0.000+00 1.913−03 0.000+00 0.000+00 2.820−02 0.000+00 0.000+00 6.741−02 6.088−01 2.703−02 0.000+00 0.000+00 3.606−02 3.223−01 0.000+00 0.000+00 4.004−03 0.000+00 0.000+00 5.711−03 5.130−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.911−03 1.290−03 0.000+00 0.000+00 6.230−01 0.000+00 0.000+00 9.281−04 1.746−04 0.000+00 0.000+00 6.592−02 0.000+00 0.000+00 0.000+00 0.000+00 1.190−02 0.000+00 0.000+00 4.470−02 8.932−01 0.000+00 0.000+00 1.605−03 0.000+00 0.000+00 4.700−03 9.424−02 0.000+00 0.000+00 8.780−01 1.764+00 0.000+00 0.000+00 0.000+00 0.000+00 9.662−02 1.853−01 0.000+00 0.000+00 0.000+00
8.965−03 0.000+00 0.000+00 0.000+00 0.000+00 8.424+07 0.000+00 0.000+00 3.144+08 0.000+00 0.000+00 4.778+07 0.000+00 0.000+00 3.442+06 0.000+00 0.000+00 0.000+00 1.679+08 8.363+07 0.000+00 0.000+00 8.740+07 3.943+08 0.000+00 9.328+07 4.685+07 0.000+00 0.000+00 7.479+05 3.526+06 0.000+00 4.060−06 2.946+07 0.000+00 0.000+00 5.347+07 1.527+07 0.000+00 0.000+00 1.787+07 0.000+00 0.000+00 2.571+07 7.368+06 0.000+00 0.000+00 6.688+08 4.422+07 0.000+00 0.000+00 2.284+07 6.090+07 0.000+00 0.000+00 2.679+07 0.000+00 0.000+00 1.095+07 2.928+07 0.000+00 0.000+00 7.424+07 7.418+08 0.000+00 0.000+00 2.777+01 3.415+01 0.000+00 0.000+00 0.000+00 0.000+00 3.836+07 3.840+07 0.000+00
5.536+01 0.000+00 0.000+00 0.000+00 7.225+01 2.241+03 0.000+00 0.000+00 0.000+00 0.000+00 8.668+01 1.571+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.160+03 5.131+02 0.000+00 0.000+00 1.593+01 0.000+00 0.000+00 4.755+03 6.148+02 0.000+00 0.000+00 7.676+00 0.000+00 0.000+00 2.082+00 7.941−02 0.000+00 0.000+00 1.892+02 1.469+02 0.000+00 0.000+00 4.774−02 0.000+00 0.000+00 1.951+02 8.762+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.580+02 6.252+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.163+02 6.450+02 0.000+00 0.000+00 1.423+01 0.000+00 0.000+00 0.000+00 4.937−05 0.000+00 0.000+00 8.683+00 0.000+00 0.000+00 8.620−02 0.000+00 0.000+00
0.000+00 2.873−05 3.478−04 0.000+00 0.000+00 0.000+00 1.973+03 1.402+04 0.000+00 0.000+00 0.000+00 0.000+00 2.047+03 1.457+04 0.000+00 0.000+00 2.816−04 1.276+04 0.000+00 0.000+00 0.000+00 7.572+04 0.000+00 0.000+00 1.352+04 0.000+00 0.000+00 0.000+00 7.844+04 0.000+00 0.000+00 7.229−03 0.000+00 0.000+00 1.316+02 0.000+00 0.000+00 0.000+00 2.487+04 3.192+04 0.000+00 1.226+02 0.000+00 0.000+00 0.000+00 1.753+04 2.252+04 0.000+00 0.000+00 1.419+03 3.689+03 0.000+00 0.000+00 0.000+00 2.180+05 0.000+00 1.322+03 3.424+03 0.000+00 0.000+00 0.000+00 1.536+05 0.000+00 0.000+00 0.000+00 1.776−03 0.000+00 0.000+00 7.162−12 0.000+00 0.000+00 1.271+03 0.000+00 0.000+00 3.350−05
(continued on next page)
28
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 10 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.295+04 4.606+03 4.141+03 4.018+03 1.018+02 9.994+01 9.955+01 9.885+01 9.873+01 9.869+01 7.148+03 6.087+03 5.826+03 5.440+03 1.027+02 1.007+02 1.003+02 9.961+01 9.949+01 9.945+01 9.939+01 9.938+01 4.101+04 3.151+04 2.276+04 1.042+02 1.022+02 1.018+02 1.010+02 1.009+02 1.008+02 1.008+02 1.008+02 1.360+05 5.116+04 1.044+02 1.024+02 1.020+02 1.013+02 1.011+02 1.011+02 1.010+02 1.010+02 1.010+02 8.201+04 1.045+02 1.025+02 1.021+02 1.013+02 1.012+02 1.012+02 1.011+02 1.011+02 1.011+02 1.022+02 1.015+02 1.013+02 1.013+02 1.012+02 1.012+02 1.012+02 5.335+03 4.407+03 3.356+03 3.221+03 3.178+03 2.533+04 9.044+03 8.126+03 7.862+03 1.407+04 1.196+04 1.140+04 1.064+04 1.063+04
0.000+00 7.466+06 0.000+00 0.000+00 4.299+10 0.000+00 0.000+00 1.933+11 0.000+00 0.000+00 3.988+05 3.884+06 0.000+00 0.000+00 8.877+10 0.000+00 0.000+00 3.907+10 2.331+11 0.000+00 0.000+00 0.000+00 0.000+00 1.631+04 0.000+00 0.000+00 3.526+10 3.347+09 0.000+00 0.000+00 3.865+11 0.000+00 0.000+00 1.447+01 4.084+03 0.000+00 0.000+00 3.058+10 0.000+00 0.000+00 2.760+10 4.137+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.334+09 3.885+08 0.000+00 0.000+00 6.575+11 0.000+00 0.000+00 0.000+00 7.846+09 0.000+00 0.000+00 2.430+10 6.810+11 1.470+07 2.618+07 0.000+00 0.000+00 0.000+00 0.000+00 2.695+06 0.000+00 0.000+00 1.431+05 1.397+06 0.000+00 0.000+00 0.000+00
0.000+00 4.748−02 0.000+00 0.000+00 6.686−02 0.000+00 0.000+00 5.663−01 0.000+00 0.000+00 3.055−03 3.236−02 0.000+00 0.000+00 7.012−02 0.000+00 0.000+00 5.812−02 5.189−01 0.000+00 0.000+00 0.000+00 0.000+00 3.641−03 0.000+00 0.000+00 2.759−02 5.195−03 0.000+00 0.000+00 8.840−01 0.000+00 0.000+00 4.011−05 2.136−03 0.000+00 0.000+00 3.180−02 0.000+00 0.000+00 4.230−02 8.441−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.555−03 5.966−04 0.000+00 0.000+00 1.344+00 0.000+00 0.000+00 0.000+00 9.060−03 0.000+00 0.000+00 3.734−02 1.307+00 6.275−02 1.525−01 0.000+00 0.000+00 0.000+00 0.000+00 6.609−02 0.000+00 0.000+00 4.244−03 4.499−02 0.000+00 0.000+00 0.000+00
0.000+00 1.440+00 0.000+00 0.000+00 4.484−02 0.000+00 0.000+00 3.686−01 0.000+00 0.000+00 2.875−01 2.594+00 0.000+00 0.000+00 9.480−02 0.000+00 0.000+00 7.624−02 6.798−01 0.000+00 0.000+00 0.000+00 0.000+00 1.511+00 0.000+00 0.000+00 3.711−02 6.961−03 0.000+00 0.000+00 1.174+00 0.000+00 0.000+00 1.077−01 2.159+00 0.000+00 0.000+00 6.406−02 0.000+00 0.000+00 8.446−02 1.685+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.712−02 1.193−03 0.000+00 0.000+00 2.683+00 0.000+00 0.000+00 0.000+00 2.418−02 0.000+00 0.000+00 9.955−02 3.483+00 2.204+00 4.425+00 0.000+00 0.000+00 0.000+00 0.000+00 3.935+00 0.000+00 0.000+00 7.862−01 7.089+00 0.000+00 0.000+00 0.000+00
1.336−03 0.000+00 0.000+00 1.802−01 0.000+00 0.000+00 1.494+07 0.000+00 0.000+00 4.993+07 0.000+00 0.000+00 8.017−03 5.097−02 0.000+00 2.979+07 1.485+07 0.000+00 0.000+00 1.397+07 6.300+07 0.000+00 8.687−07 0.000+00 0.000+00 9.073+06 0.000+00 0.000+00 1.196+07 3.414+06 0.000+00 0.000+00 5.842+07 0.000+00 0.000+00 1.361+07 0.000+00 0.000+00 5.112+06 1.363+07 0.000+00 0.000+00 6.433+06 6.445+07 6.956−09 0.000+00 3.202+06 4.494+05 0.000+00 0.000+00 8.396+06 1.050+06 0.000+00 0.000+00 2.702+06 0.000+00 0.000+00 1.397+06 8.734+06 0.000+00 0.000+00 0.000+00 0.000+00 6.379+00 7.851+00 0.000+00 2.934−04 0.000+00 0.000+00 6.129−02 0.000+00 0.000+00 2.726−03 1.734−02 0.000+00
4.138+00 0.000+00 0.000+00 0.000+00 0.000+00 2.708+00 2.435+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.125−07 0.000+00 0.000+00 5.884+02 1.924+01 0.000+00 0.000+00 3.959−01 0.000+00 0.000+00 1.563−01 0.000+00 0.000+00 8.594−03 0.000+00 0.000+00 9.053+00 2.154+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.778+01 2.994+01 0.000+00 0.000+00 5.527−01 0.000+00 2.094−02 0.000+00 0.000+00 4.722−04 0.000+00 0.000+00 1.317+01 3.089+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.225+01 3.097+01 0.000+00 0.000+00 0.000+00 0.000+00 3.669−06 0.000+00 0.000+00 5.531−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.812−08 0.000+00 0.000+00
0.000+00 1.552−06 1.886−05 0.000+00 0.000+00 0.000+00 0.000+00 8.728+01 6.191+02 0.000+00 0.000+00 1.500−05 0.000+00 0.000+00 9.305+02 0.000+00 0.000+00 0.000+00 3.370+03 0.000+00 0.000+00 4.447−05 0.000+00 4.314−10 2.812−09 0.000+00 1.493+01 0.000+00 0.000+00 0.000+00 9.981+02 1.278+03 0.000+00 0.000+00 3.375−10 0.000+00 1.608+02 4.210+02 0.000+00 0.000+00 0.000+00 8.765+03 0.000+00 0.000+00 0.000+00 2.495−08 0.000+00 0.000+00 2.136+01 0.000+00 0.000+00 0.000+00 4.291+03 2.245+03 0.000+00 3.672+01 1.655+02 0.000+00 0.000+00 0.000+00 2.075+04 0.000+00 1.488−04 0.000+00 0.000+00 4.576−13 0.000+00 1.454−07 1.769−06 0.000+00 0.000+00 1.396−06 0.000+00 0.000+00 3.510−16
(continued on next page)
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29
Table 10 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
8.012+04 6.016+04 4.374+04 4.359+04 2.415+05 9.630+04 9.560+04 7.040+04 1.602+05 1.582+05 9.937+04 1.320+07 2.618+05 2.671+05
0.000+00 8.366+03 0.000+00 0.000+00 9.227+00 2.187+03 0.000+00 0.000+00 0.000+00 2.772+02 0.000+00 1.767−05 6.346+01 0.000+00
0.000+00 6.810−03 0.000+00 0.000+00 8.069−05 4.053−03 0.000+00 0.000+00 0.000+00 1.387−03 0.000+00 4.616−07 8.152−04 0.000+00
0.000+00 5.396+00 0.000+00 0.000+00 3.850−01 7.710+00 0.000+00 0.000+00 0.000+00 4.336+00 0.000+00 1.604−01 5.622+00 0.000+00
2.193−07 0.000+00 0.000+00 6.433−06 0.000+00 0.000+00 1.407−08 6.503−07 2.394−09 0.000+00 0.000+00 0.000+00 0.000+00 6.049−11
2.097−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.688−11 0.000+00 2.813−03 0.000+00 0.000+00 0.000+00 0.000+00 6.287−04
0.000+00 6.071−11 3.835−10 0.000+00 0.000+00 5.100−11 0.000+00 0.000+00 0.000+00 7.390−13 3.958−12 0.000+00 2.890−13 0.000+00
30
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 11 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in V XXI. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.926+02 2.397+02 1.405+01 1.387+01 1.382+01 1.376+01 1.374+01 1.045+01 1.041+01 1.040+01 1.039+01 1.038+01 1.038+01 9.357+00 9.340+00 9.335+00 9.329+00 9.328+00 9.327+00 1.327+03 1.476+01 1.456+01 1.451+01 1.444+01 1.442+01 1.084+01 1.080+01 1.079+01 1.077+01 1.077+01 1.077+01 9.666+00 9.648+00 9.643+00 9.636+00 9.635+00 9.634+00 1.493+01 1.472+01 1.467+01 1.459+01 1.458+01 1.093+01 1.089+01 1.088+01 1.086+01 1.085+01 1.085+01 1.085+01 9.737+00 9.718+00 9.714+00 9.707+00 9.705+00 9.705+00 9.704+00 9.704+00 1.055+03 8.543+02 6.555+02 6.267+02 4.086+01 4.022+01 4.006+01 3.983+01 3.978+01 3.977+01 2.801+01 2.785+01 2.782+01 2.776+01 2.775+01 2.775+01
1.574+09 2.895+09 0.000+00 4.357+12 4.245+12 0.000+00 0.000+00 0.000+00 1.923+12 1.889+12 0.000+00 0.000+00 0.000+00 0.000+00 9.936+11 9.786+11 0.000+00 0.000+00 0.000+00 0.000+00 5.382+11 0.000+00 0.000+00 1.078+13 0.000+00 2.155+11 0.000+00 0.000+00 3.515+12 0.000+00 0.000+00 1.081+11 0.000+00 0.000+00 1.621+12 0.000+00 0.000+00 1.120+12 0.000+00 0.000+00 2.131+12 1.279+13 4.460+11 0.000+00 0.000+00 6.886+11 4.149+12 0.000+00 0.000+00 2.219+11 0.000+00 0.000+00 3.163+11 1.909+12 0.000+00 0.000+00 0.000+00 2.044+08 3.879+08 0.000+00 0.000+00 0.000+00 5.689+11 5.516+11 0.000+00 0.000+00 0.000+00 0.000+00 3.125+11 3.053+11 0.000+00 0.000+00 0.000+00
2.020−02 4.988−02 0.000+00 1.256−01 2.432−01 0.000+00 0.000+00 0.000+00 3.126−02 6.128−02 0.000+00 0.000+00 0.000+00 0.000+00 1.299−02 2.557−02 0.000+00 0.000+00 0.000+00 0.000+00 1.758−02 0.000+00 0.000+00 6.733−01 0.000+00 3.798−03 0.000+00 0.000+00 1.222−01 0.000+00 0.000+00 1.514−03 0.000+00 0.000+00 4.515−02 0.000+00 0.000+00 1.871−02 0.000+00 0.000+00 6.804−02 6.114−01 3.995−03 0.000+00 0.000+00 1.217−02 1.099−01 0.000+00 0.000+00 1.577−03 0.000+00 0.000+00 4.467−03 4.043−02 0.000+00 0.000+00 0.000+00 3.412−02 8.489−02 0.000+00 0.000+00 0.000+00 1.379−01 2.655−01 0.000+00 0.000+00 0.000+00 0.000+00 3.636−02 7.084−02 0.000+00 0.000+00 0.000+00
3.891−02 7.874−02 0.000+00 1.147−02 2.214−02 0.000+00 0.000+00 0.000+00 2.143−03 4.197−03 0.000+00 0.000+00 0.000+00 0.000+00 7.990−04 1.572−03 0.000+00 0.000+00 0.000+00 0.000+00 1.708−03 0.000+00 0.000+00 6.399−02 0.000+00 2.711−04 0.000+00 0.000+00 8.666−03 0.000+00 0.000+00 9.638−05 0.000+00 0.000+00 2.864−03 0.000+00 0.000+00 3.677−03 0.000+00 0.000+00 1.308−02 1.174−01 5.752−04 0.000+00 0.000+00 1.740−03 1.571−02 0.000+00 0.000+00 2.022−04 0.000+00 0.000+00 5.710−04 5.167−03 0.000+00 0.000+00 0.000+00 2.370−01 4.775−01 0.000+00 0.000+00 0.000+00 3.653−02 7.004−02 0.000+00 0.000+00 0.000+00 0.000+00 6.668−03 1.297−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.409+09 5.427+09 0.000+00 0.000+00 0.000+00 7.368+08 7.498+08 0.000+00 0.000+00 0.000+00 0.000+00 1.901+08 1.958+08 0.000+00 2.338−01 0.000+00 0.000+00 1.066+09 0.000+00 0.000+00 0.000+00 0.000+00 4.627+08 0.000+00 0.000+00 4.121+09 0.000+00 0.000+00 2.482+08 0.000+00 0.000+00 2.760+09 0.000+00 2.115+09 1.053+09 0.000+00 0.000+00 0.000+00 8.987+08 4.518+08 0.000+00 0.000+00 1.176+09 5.277+09 0.000+00 4.664+08 2.354+08 0.000+00 0.000+00 7.880+08 3.538+09 0.000+00 0.000+00 0.000+00 1.885+02 2.374+02 0.000+00 0.000+00 0.000+00 3.708+08 3.715+08 0.000+00 0.000+00 0.000+00 0.000+00 1.252+08 1.263+08 0.000+00
0.000+00 0.000+00 4.052+04 0.000+00 0.000+00 2.269+03 0.000+00 3.418+04 0.000+00 0.000+00 1.331+03 0.000+00 0.000+00 2.239+04 0.000+00 0.000+00 7.468+02 0.000+00 0.000+00 3.836+03 0.000+00 9.320+03 6.458+04 0.000+00 0.000+00 0.000+00 7.306+03 3.302+04 0.000+00 0.000+00 0.000+00 0.000+00 4.720+03 1.823+04 0.000+00 0.000+00 0.000+00 0.000+00 2.425+05 6.588+04 0.000+00 0.000+00 0.000+00 1.414+05 5.169+04 0.000+00 0.000+00 7.494+02 0.000+00 0.000+00 8.154+04 3.292+04 0.000+00 0.000+00 6.588+02 0.000+00 0.000+00 0.000+00 0.000+00 1.728−03 0.000+00 4.086+02 0.000+00 0.000+00 9.630+00 0.000+00 0.000+00 5.096+02 0.000+00 0.000+00 1.279+01 0.000+00 0.000+00
0.000+00 5.554+00 0.000+00 0.000+00 2.454+06 0.000+00 0.000+00 0.000+00 0.000+00 1.926+06 0.000+00 0.000+00 7.243−01 0.000+00 0.000+00 1.238+06 0.000+00 0.000+00 6.469−01 0.000+00 0.000+00 0.000+00 0.000+00 2.272+05 1.624+06 0.000+00 0.000+00 0.000+00 1.328+05 9.524+05 0.000+00 0.000+00 0.000+00 0.000+00 7.646+04 5.489+05 0.000+00 5.573+05 0.000+00 0.000+00 0.000+00 8.598+06 4.137+05 0.000+00 0.000+00 0.000+00 5.023+06 0.000+00 0.000+00 2.595+05 0.000+00 0.000+00 0.000+00 2.888+06 0.000+00 0.000+00 9.182−02 0.000+00 5.864−02 0.000+00 0.000+00 0.000+00 0.000+00 3.796+04 0.000+00 0.000+00 3.949−03 0.000+00 0.000+00 4.356+04 0.000+00 0.000+00 1.095−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 11 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
4.487+03 1.731+03 1.543+03 4.250+01 4.181+01 4.165+01 4.139+01 4.134+01 4.133+01 2.877+01 2.861+01 2.857+01 2.851+01 2.850+01 2.850+01 2.817+03 2.352+03 4.291+01 4.220+01 4.204+01 4.178+01 4.173+01 4.171+01 4.169+01 2.896+01 2.879+01 2.875+01 2.869+01 2.868+01 2.868+01 2.867+01 2.867+01 1.422+04 4.357+01 4.285+01 4.267+01 4.241+01 4.235+01 4.234+01 4.231+01 2.926+01 2.909+01 2.905+01 2.899+01 2.898+01 2.897+01 2.897+01 2.897+01 4.371+01 4.297+01 4.280+01 4.253+01 4.248+01 4.247+01 4.244+01 2.932+01 2.915+01 2.911+01 2.905+01 2.903+01 2.903+01 2.902+01 2.902+01 2.902+01 2.563+03 2.066+03 1.584+03 1.513+03 1.495+03 8.907+01 8.753+01 8.717+01 8.660+01 8.649+01 8.645+01
0.000+00 2.992+07 0.000+00 1.506+11 0.000+00 0.000+00 1.134+12 0.000+00 0.000+00 7.312+10 0.000+00 0.000+00 5.587+11 0.000+00 0.000+00 1.384+06 1.433+07 3.128+11 0.000+00 0.000+00 2.277+11 1.361+12 0.000+00 0.000+00 1.509+11 0.000+00 0.000+00 1.111+11 6.664+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.084+10 7.579+09 0.000+00 0.000+00 2.513+12 0.000+00 0.000+00 3.468+10 3.256+09 0.000+00 0.000+00 8.301+11 0.000+00 0.000+00 0.000+00 0.000+00 6.947+10 0.000+00 0.000+00 1.787+11 2.684+12 0.000+00 0.000+00 2.981+10 0.000+00 0.000+00 5.881+10 8.852+11 0.000+00 0.000+00 4.789+07 9.191+07 0.000+00 0.000+00 0.000+00 0.000+00 1.336+11 1.292+11 0.000+00 0.000+00 0.000+00
0.000+00 2.688−02 0.000+00 4.079−02 0.000+00 0.000+00 5.826−01 0.000+00 0.000+00 9.076−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.647−03 1.782−02 4.317−02 0.000+00 0.000+00 5.959−02 5.328−01 0.000+00 0.000+00 9.485−03 0.000+00 0.000+00 1.372−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.112−02 2.069−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.200−03 4.119−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.272−02 0.000+00 0.000+00 4.832−02 9.661−01 0.000+00 0.000+00 2.525−03 0.000+00 0.000+00 7.431−03 1.491−01 0.000+00 0.000+00 4.717−02 1.176−01 0.000+00 0.000+00 0.000+00 0.000+00 1.535−01 2.944−01 0.000+00 0.000+00 0.000+00
0.000+00 3.063−01 0.000+00 1.142−02 0.000+00 0.000+00 1.588−01 0.000+00 0.000+00 1.719−03 0.000+00 0.000+00 2.556−02 0.000+00 0.000+00 6.109−02 5.519−01 2.439−02 0.000+00 0.000+00 3.278−02 2.927−01 0.000+00 0.000+00 3.617−03 0.000+00 0.000+00 5.183−03 4.655−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.276−03 1.163−03 0.000+00 0.000+00 5.647−01 0.000+00 0.000+00 8.428−04 1.576−04 0.000+00 0.000+00 5.977−02 0.000+00 0.000+00 0.000+00 0.000+00 1.075−02 0.000+00 0.000+00 4.053−02 8.099−01 0.000+00 0.000+00 1.452−03 0.000+00 0.000+00 4.261−03 8.546−02 0.000+00 0.000+00 7.962−01 1.600+00 0.000+00 0.000+00 0.000+00 0.000+00 8.847−02 1.690−01 0.000+00 0.000+00 0.000+00
1.955−02 0.000+00 0.000+00 0.000+00 0.000+00 1.129+08 0.000+00 0.000+00 4.218+08 0.000+00 0.000+00 6.411+07 0.000+00 0.000+00 4.654+06 0.000+00 0.000+00 0.000+00 2.249+08 1.120+08 0.000+00 0.000+00 1.169+08 5.277+08 0.000+00 1.249+08 6.275+07 0.000+00 0.000+00 9.831+05 4.659+06 0.000+00 8.876−06 3.939+07 0.000+00 0.000+00 7.166+07 2.047+07 0.000+00 0.000+00 2.391+07 0.000+00 0.000+00 3.445+07 9.878+06 0.000+00 0.000+00 8.962+08 5.914+07 0.000+00 0.000+00 3.060+07 8.160+07 0.000+00 0.000+00 3.585+07 0.000+00 0.000+00 1.466+07 3.923+07 0.000+00 0.000+00 9.948+07 9.939+08 0.000+00 0.000+00 3.269+01 4.126+01 0.000+00 0.000+00 0.000+00 0.000+00 5.131+07 5.136+07 0.000+00
9.936+01 0.000+00 0.000+00 0.000+00 1.178+02 3.652+03 0.000+00 0.000+00 0.000+00 0.000+00 1.412+02 2.560+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.002+04 8.339+02 0.000+00 0.000+00 2.590+01 0.000+00 0.000+00 7.737+03 9.990+02 0.000+00 0.000+00 1.247+01 0.000+00 0.000+00 3.744+00 1.291−01 0.000+00 0.000+00 3.084+02 2.396+02 0.000+00 0.000+00 7.727−02 0.000+00 0.000+00 3.181+02 1.430+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.096+02 1.018+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.786+02 1.051+03 0.000+00 0.000+00 2.318+01 0.000+00 0.000+00 0.000+00 7.407−05 0.000+00 0.000+00 1.411+01 0.000+00 0.000+00 1.411−01 0.000+00 0.000+00
0.000+00 4.399−05 5.588−04 0.000+00 0.000+00 0.000+00 2.917+03 2.074+04 0.000+00 0.000+00 0.000+00 0.000+00 3.026+03 2.155+04 0.000+00 0.000+00 3.706−04 1.878+04 0.000+00 0.000+00 0.000+00 1.118+05 0.000+00 0.000+00 1.990+04 0.000+00 0.000+00 0.000+00 1.158+05 0.000+00 0.000+00 1.297−02 0.000+00 0.000+00 1.949+02 0.000+00 0.000+00 0.000+00 3.677+04 4.720+04 0.000+00 1.815+02 0.000+00 0.000+00 0.000+00 2.591+04 3.331+04 0.000+00 0.000+00 2.103+03 5.439+03 0.000+00 0.000+00 0.000+00 3.220+05 0.000+00 1.960+03 5.048+03 0.000+00 0.000+00 0.000+00 2.268+05 0.000+00 0.000+00 0.000+00 2.376−03 0.000+00 0.000+00 1.155−11 0.000+00 0.000+00 1.878+03 0.000+00 0.000+00 5.992−05
(continued on next page)
32
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 11 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.065+04 4.145+03 3.691+03 3.588+03 9.228+01 9.063+01 9.024+01 8.963+01 8.951+01 8.947+01 6.784+03 5.648+03 5.409+03 5.008+03 9.308+01 9.140+01 9.101+01 9.039+01 9.027+01 9.023+01 9.017+01 9.017+01 3.372+04 2.670+04 1.913+04 9.438+01 9.265+01 9.224+01 9.161+01 9.148+01 9.145+01 9.138+01 9.138+01 1.281+05 4.419+04 9.464+01 9.291+01 9.250+01 9.186+01 9.173+01 9.169+01 9.163+01 9.163+01 9.159+01 6.746+04 9.471+01 9.298+01 9.256+01 9.193+01 9.180+01 9.176+01 9.170+01 9.170+01 9.166+01 9.269+01 9.205+01 9.192+01 9.189+01 9.182+01 9.182+01 9.178+01 5.068+03 4.076+03 3.123+03 2.982+03 2.943+03 2.084+04 8.138+03 7.243+03 7.020+03 1.335+04 1.110+04 1.058+04 9.798+03 9.790+03
0.000+00 9.286+06 0.000+00 0.000+00 5.185+10 0.000+00 0.000+00 2.350+11 0.000+00 0.000+00 4.228+05 4.409+06 0.000+00 0.000+00 1.074+11 0.000+00 0.000+00 4.755+10 2.836+11 0.000+00 0.000+00 0.000+00 0.000+00 2.432+04 0.000+00 0.000+00 4.293+10 4.053+09 0.000+00 0.000+00 4.698+11 0.000+00 0.000+00 1.569+01 5.746+03 0.000+00 0.000+00 3.708+10 0.000+00 0.000+00 3.355+10 5.028+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.015+10 4.722+08 0.000+00 0.000+00 7.992+11 0.000+00 0.000+00 0.000+00 9.546+09 0.000+00 0.000+00 2.954+10 8.277+11 1.556+07 3.002+07 0.000+00 0.000+00 0.000+00 0.000+00 3.354+06 0.000+00 0.000+00 1.517+05 1.587+06 0.000+00 0.000+00 0.000+00
0.000+00 4.784−02 0.000+00 0.000+00 6.620−02 0.000+00 0.000+00 5.660−01 0.000+00 0.000+00 2.917−03 3.163−02 0.000+00 0.000+00 6.979−02 0.000+00 0.000+00 5.824−02 5.196−01 0.000+00 0.000+00 0.000+00 0.000+00 3.897−03 0.000+00 0.000+00 2.762−02 5.170−03 0.000+00 0.000+00 8.835−01 0.000+00 0.000+00 3.861−05 2.243−03 0.000+00 0.000+00 3.170−02 0.000+00 0.000+00 4.230−02 8.439−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.574−03 5.965−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.069−03 0.000+00 0.000+00 3.733−02 1.307+00 5.991−02 1.496−01 0.000+00 0.000+00 0.000+00 0.000+00 6.659−02 0.000+00 0.000+00 4.054−03 4.397−02 0.000+00 0.000+00 0.000+00
0.000+00 1.306+00 0.000+00 0.000+00 4.022−02 0.000+00 0.000+00 3.340−01 0.000+00 0.000+00 2.606−01 2.352+00 0.000+00 0.000+00 8.555−02 0.000+00 0.000+00 6.933−02 6.176−01 0.000+00 0.000+00 0.000+00 0.000+00 1.370+00 0.000+00 0.000+00 3.370−02 6.280−03 0.000+00 0.000+00 1.064+00 0.000+00 0.000+00 9.770−02 1.958+00 0.000+00 0.000+00 5.793−02 0.000+00 0.000+00 7.661−02 1.528+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.557−02 1.082−03 0.000+00 0.000+00 2.433+00 0.000+00 0.000+00 0.000+00 2.196−02 0.000+00 0.000+00 9.028−02 3.159+00 1.999+00 4.014+00 0.000+00 0.000+00 0.000+00 0.000+00 3.568+00 0.000+00 0.000+00 7.127−01 6.428+00 0.000+00 0.000+00 0.000+00
2.912−03 0.000+00 0.000+00 2.612−01 0.000+00 0.000+00 2.002+07 0.000+00 0.000+00 6.698+07 0.000+00 0.000+00 9.552−03 6.338−02 0.000+00 3.992+07 1.989+07 0.000+00 0.000+00 1.871+07 8.435+07 0.000+00 1.901−06 0.000+00 0.000+00 1.214+07 0.000+00 0.000+00 1.603+07 4.577+06 0.000+00 0.000+00 7.838+07 0.000+00 0.000+00 1.822+07 0.000+00 0.000+00 6.852+06 1.826+07 0.000+00 0.000+00 8.622+06 8.640+07 1.519−08 0.000+00 4.295+06 6.018+05 0.000+00 0.000+00 1.125+07 1.407+06 0.000+00 0.000+00 3.618+06 0.000+00 0.000+00 1.872+06 1.170+07 0.000+00 0.000+00 0.000+00 0.000+00 7.515+00 9.500+00 0.000+00 6.399−04 0.000+00 0.000+00 8.884−02 0.000+00 0.000+00 3.250−03 2.157−02 0.000+00
7.428+00 0.000+00 0.000+00 0.000+00 0.000+00 4.414+00 3.968+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.737−07 0.000+00 0.000+00 9.575+02 3.130+01 0.000+00 0.000+00 6.446−01 0.000+00 0.000+00 2.811−01 0.000+00 0.000+00 1.399−02 0.000+00 0.000+00 1.476+01 3.515+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.419+01 4.878+01 0.000+00 0.000+00 9.006−01 0.000+00 3.763−02 0.000+00 0.000+00 7.669−04 0.000+00 0.000+00 2.145+01 5.034+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.996+01 5.046+01 0.000+00 0.000+00 0.000+00 0.000+00 5.510−06 0.000+00 0.000+00 9.928−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.779−08 0.000+00 0.000+00
0.000+00 2.383−06 3.037−05 0.000+00 0.000+00 0.000+00 0.000+00 1.291+02 9.151+02 0.000+00 0.000+00 1.977−05 0.000+00 0.000+00 1.370+03 0.000+00 0.000+00 0.000+00 4.980+03 0.000+00 0.000+00 7.974−05 0.000+00 8.960−10 6.090−09 0.000+00 2.210+01 0.000+00 0.000+00 0.000+00 1.476+03 1.890+03 0.000+00 0.000+00 6.363−10 0.000+00 2.382+02 6.209+02 0.000+00 0.000+00 0.000+00 1.295+04 0.000+00 0.000+00 0.000+00 4.515−08 0.000+00 0.000+00 3.162+01 0.000+00 0.000+00 0.000+00 6.341+03 3.319+03 0.000+00 5.441+01 2.448+02 0.000+00 0.000+00 0.000+00 3.066+04 0.000+00 1.994−04 0.000+00 0.000+00 7.390−13 0.000+00 2.234−07 2.852−06 0.000+00 0.000+00 1.842−06 0.000+00 0.000+00 5.847−16
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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33
Table 11 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
6.588+04 5.109+04 3.681+04 3.670+04 2.276+05 8.344+04 8.288+04 6.018+04 1.317+05 1.303+05 8.181+04 1.236+07 2.159+05 2.197+05
0.000+00 1.239+04 0.000+00 0.000+00 1.000+01 3.049+03 0.000+00 0.000+00 0.000+00 4.498+02 0.000+00 1.951−05 1.027+02 0.000+00
0.000+00 7.273−03 0.000+00 0.000+00 7.765−05 4.243−03 0.000+00 0.000+00 0.000+00 1.527−03 0.000+00 4.470−07 8.967−04 0.000+00
0.000+00 4.893+00 0.000+00 0.000+00 3.491−01 6.992+00 0.000+00 0.000+00 0.000+00 3.933+00 0.000+00 1.455−01 5.099+00 0.000+00
4.798−07 0.000+00 0.000+00 1.250−05 0.000+00 0.000+00 2.363−08 1.172−06 5.229−09 0.000+00 0.000+00 0.000+00 0.000+00 1.321−10
3.771−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.150−11 0.000+00 5.055−03 0.000+00 0.000+00 0.000+00 0.000+00 1.129−03
0.000+00 1.247−10 8.233−10 0.000+00 0.000+00 9.472−11 0.000+00 0.000+00 0.000+00 1.767−12 9.490−12 0.000+00 6.874−13 0.000+00
34
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 12 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Cr XXII. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.787+02 2.224+02 1.282+01 1.266+01 1.261+01 1.256+01 1.254+01 9.537+00 9.499+00 9.489+00 9.475+00 9.472+00 9.471+00 8.534+00 8.519+00 8.515+00 8.509+00 8.508+00 8.507+00 1.102+03 1.344+01 1.326+01 1.321+01 1.315+01 1.313+01 9.875+00 9.835+00 9.824+00 9.809+00 9.805+00 9.805+00 8.804+00 8.788+00 8.783+00 8.777+00 8.776+00 8.775+00 1.360+01 1.342+01 1.337+01 1.331+01 1.329+01 9.964+00 9.923+00 9.912+00 9.897+00 9.894+00 9.893+00 9.891+00 8.875+00 8.858+00 8.854+00 8.848+00 8.846+00 8.846+00 8.845+00 8.845+00 1.005+03 7.912+02 6.109+02 5.809+02 3.725+01 3.669+01 3.654+01 3.633+01 3.629+01 3.628+01 2.554+01 2.540+01 2.536+01 2.531+01 2.530+01 2.530+01
1.658+09 3.304+09 0.000+00 5.262+12 5.115+12 0.000+00 0.000+00 0.000+00 2.319+12 2.274+12 0.000+00 0.000+00 0.000+00 0.000+00 1.198+12 1.178+12 0.000+00 0.000+00 0.000+00 0.000+00 6.427+11 0.000+00 0.000+00 1.299+13 0.000+00 2.576+11 0.000+00 0.000+00 4.235+12 0.000+00 0.000+00 1.294+11 0.000+00 0.000+00 1.953+12 0.000+00 0.000+00 1.344+12 0.000+00 0.000+00 2.565+12 1.539+13 5.353+11 0.000+00 0.000+00 8.279+11 4.991+12 0.000+00 0.000+00 2.664+11 0.000+00 0.000+00 3.801+11 2.296+12 0.000+00 0.000+00 0.000+00 2.157+08 4.450+08 0.000+00 0.000+00 0.000+00 6.882+11 6.654+11 0.000+00 0.000+00 0.000+00 0.000+00 3.776+11 3.681+11 0.000+00 0.000+00 0.000+00
1.931−02 4.901−02 0.000+00 1.264−01 2.440−01 0.000+00 0.000+00 0.000+00 3.138−02 6.140−02 0.000+00 0.000+00 0.000+00 0.000+00 1.303−02 2.561−02 0.000+00 0.000+00 0.000+00 0.000+00 1.740−02 0.000+00 0.000+00 6.729−01 0.000+00 3.766−03 0.000+00 0.000+00 1.222−01 0.000+00 0.000+00 1.504−03 0.000+00 0.000+00 4.512−02 0.000+00 0.000+00 1.863−02 0.000+00 0.000+00 6.807−02 6.115−01 3.983−03 0.000+00 0.000+00 1.216−02 1.099−01 0.000+00 0.000+00 1.573−03 0.000+00 0.000+00 4.461−03 4.040−02 0.000+00 0.000+00 0.000+00 3.264−02 8.353−02 0.000+00 0.000+00 0.000+00 1.389−01 2.664−01 0.000+00 0.000+00 0.000+00 0.000+00 3.652−02 7.100−02 0.000+00 0.000+00 0.000+00
3.542−02 7.177−02 0.000+00 1.053−02 2.026−02 0.000+00 0.000+00 0.000+00 1.962−03 3.836−03 0.000+00 0.000+00 0.000+00 0.000+00 7.310−04 1.436−03 0.000+00 0.000+00 0.000+00 0.000+00 1.539−03 0.000+00 0.000+00 5.825−02 0.000+00 2.449−04 0.000+00 0.000+00 7.890−03 0.000+00 0.000+00 8.715−05 0.000+00 0.000+00 2.608−03 0.000+00 0.000+00 3.337−03 0.000+00 0.000+00 1.193−02 1.070−01 5.226−04 0.000+00 0.000+00 1.584−03 1.431−02 0.000+00 0.000+00 1.838−04 0.000+00 0.000+00 5.197−04 4.706−03 0.000+00 0.000+00 0.000+00 2.159−01 4.352−01 0.000+00 0.000+00 0.000+00 3.355−02 6.408−02 0.000+00 0.000+00 0.000+00 0.000+00 6.109−03 1.186−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.113+09 7.140+09 0.000+00 0.000+00 0.000+00 9.618+08 9.806+08 0.000+00 0.000+00 0.000+00 0.000+00 2.467+08 2.549+08 0.000+00 4.917−01 0.000+00 0.000+00 1.408+09 0.000+00 0.000+00 0.000+00 0.000+00 6.122+08 0.000+00 0.000+00 5.446+09 0.000+00 0.000+00 3.291+08 0.000+00 0.000+00 3.647+09 0.000+00 2.794+09 1.390+09 0.000+00 0.000+00 0.000+00 1.186+09 5.965+08 0.000+00 0.000+00 1.554+09 6.972+09 0.000+00 6.155+08 3.110+08 0.000+00 0.000+00 1.041+09 4.673+09 0.000+00 0.000+00 0.000+00 2.224+02 2.879+02 0.000+00 0.000+00 0.000+00 4.890+08 4.899+08 0.000+00 0.000+00 0.000+00 0.000+00 1.645+08 1.662+08 0.000+00
0.000+00 0.000+00 6.418+04 0.000+00 0.000+00 3.594+03 0.000+00 5.416+04 0.000+00 0.000+00 2.106+03 0.000+00 0.000+00 3.546+04 0.000+00 0.000+00 1.181+03 0.000+00 0.000+00 6.699+03 0.000+00 1.484+04 1.029+05 0.000+00 0.000+00 0.000+00 1.164+04 5.263+04 0.000+00 0.000+00 0.000+00 0.000+00 7.519+03 2.906+04 0.000+00 0.000+00 0.000+00 0.000+00 3.855+05 1.045+05 0.000+00 0.000+00 0.000+00 2.248+05 8.197+04 0.000+00 0.000+00 1.193+03 0.000+00 0.000+00 1.296+05 5.218+04 0.000+00 0.000+00 1.049+03 0.000+00 0.000+00 0.000+00 0.000+00 2.558−03 0.000+00 6.488+02 0.000+00 0.000+00 1.534+01 0.000+00 0.000+00 8.093+02 0.000+00 0.000+00 2.036+01 0.000+00 0.000+00
0.000+00 7.363+00 0.000+00 0.000+00 3.551+06 0.000+00 0.000+00 0.000+00 0.000+00 2.787+06 0.000+00 0.000+00 1.262+00 0.000+00 0.000+00 1.792+06 0.000+00 0.000+00 1.128+00 0.000+00 0.000+00 0.000+00 0.000+00 3.297+05 2.359+06 0.000+00 0.000+00 0.000+00 1.927+05 1.383+06 0.000+00 0.000+00 0.000+00 0.000+00 1.109+05 7.971+05 0.000+00 8.051+05 0.000+00 0.000+00 0.000+00 1.245+07 5.979+05 0.000+00 0.000+00 0.000+00 7.269+06 0.000+00 0.000+00 3.752+05 0.000+00 0.000+00 0.000+00 4.178+06 0.000+00 0.000+00 1.602−01 0.000+00 7.842−02 0.000+00 0.000+00 0.000+00 0.000+00 5.505+04 0.000+00 0.000+00 6.864−03 0.000+00 0.000+00 6.317+04 0.000+00 0.000+00 1.894−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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35
Table 12 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
3.725+03 1.559+03 1.377+03 3.869+01 3.808+01 3.792+01 3.770+01 3.765+01 3.763+01 2.620+01 2.606+01 2.602+01 2.597+01 2.595+01 2.595+01 2.682+03 2.185+03 3.909+01 3.848+01 3.831+01 3.808+01 3.803+01 3.802+01 3.799+01 2.639+01 2.624+01 2.620+01 2.615+01 2.614+01 2.613+01 2.613+01 2.613+01 1.180+04 3.967+01 3.904+01 3.886+01 3.863+01 3.858+01 3.857+01 3.854+01 2.665+01 2.650+01 2.646+01 2.641+01 2.640+01 2.639+01 2.639+01 2.639+01 3.980+01 3.917+01 3.899+01 3.876+01 3.871+01 3.869+01 3.867+01 2.671+01 2.656+01 2.652+01 2.647+01 2.645+01 2.645+01 2.644+01 2.644+01 2.644+01 2.440+03 1.912+03 1.476+03 1.402+03 1.386+03 8.119+01 7.985+01 7.948+01 7.899+01 7.887+01 7.884+01
0.000+00 3.727+07 0.000+00 1.801+11 0.000+00 0.000+00 1.366+12 0.000+00 0.000+00 8.751+10 0.000+00 0.000+00 6.732+11 0.000+00 0.000+00 1.461+06 1.627+07 3.754+11 0.000+00 0.000+00 2.745+11 1.639+12 0.000+00 0.000+00 1.812+11 0.000+00 0.000+00 1.339+11 8.025+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.759+10 9.093+09 0.000+00 0.000+00 3.027+12 0.000+00 0.000+00 4.187+10 3.907+09 0.000+00 0.000+00 1.000+12 0.000+00 0.000+00 0.000+00 0.000+00 8.349+10 0.000+00 0.000+00 2.152+11 3.232+12 0.000+00 0.000+00 3.584+10 0.000+00 0.000+00 7.082+10 1.066+12 0.000+00 0.000+00 5.056+07 1.056+08 0.000+00 0.000+00 0.000+00 0.000+00 1.618+11 1.560+11 0.000+00 0.000+00 0.000+00
0.000+00 2.717−02 0.000+00 4.041−02 0.000+00 0.000+00 5.822−01 0.000+00 0.000+00 9.007−03 0.000+00 0.000+00 1.361−01 0.000+00 0.000+00 1.575−03 1.747−02 4.300−02 0.000+00 0.000+00 5.967−02 5.332−01 0.000+00 0.000+00 9.457−03 0.000+00 0.000+00 1.372−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.115−02 2.059−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.205−03 4.101−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.269−02 0.000+00 0.000+00 4.831−02 9.659−01 0.000+00 0.000+00 2.519−03 0.000+00 0.000+00 7.428−03 1.490−01 0.000+00 0.000+00 4.513−02 1.158−01 0.000+00 0.000+00 0.000+00 0.000+00 1.546−01 2.954−01 0.000+00 0.000+00 0.000+00
0.000+00 2.789−01 0.000+00 1.029−02 0.000+00 0.000+00 1.445−01 0.000+00 0.000+00 1.554−03 0.000+00 0.000+00 2.327−02 0.000+00 0.000+00 5.562−02 5.027−01 2.214−02 0.000+00 0.000+00 2.993−02 2.670−01 0.000+00 0.000+00 3.286−03 0.000+00 0.000+00 4.726−03 4.244−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.730−03 1.054−03 0.000+00 0.000+00 5.142−01 0.000+00 0.000+00 7.694−04 1.429−04 0.000+00 0.000+00 5.445−02 0.000+00 0.000+00 0.000+00 0.000+00 9.772−03 0.000+00 0.000+00 3.692−02 7.377−01 0.000+00 0.000+00 1.320−03 0.000+00 0.000+00 3.881−03 7.785−02 0.000+00 0.000+00 7.251−01 1.458+00 0.000+00 0.000+00 0.000+00 0.000+00 8.129−02 1.546−01 0.000+00 0.000+00 0.000+00
4.114−02 0.000+00 0.000+00 0.000+00 0.000+00 1.493+08 0.000+00 0.000+00 5.585+08 0.000+00 0.000+00 8.486+07 0.000+00 0.000+00 6.227+06 0.000+00 0.000+00 0.000+00 2.973+08 1.480+08 0.000+00 0.000+00 1.544+08 6.968+08 0.000+00 1.649+08 8.292+07 0.000+00 0.000+00 1.277+06 6.087+06 0.000+00 1.872−05 5.199+07 0.000+00 0.000+00 9.476+07 2.707+07 0.000+00 0.000+00 3.158+07 0.000+00 0.000+00 4.554+07 1.306+07 0.000+00 0.000+00 1.185+09 7.806+07 0.000+00 0.000+00 4.045+07 1.078+08 0.000+00 0.000+00 4.733+07 0.000+00 0.000+00 1.936+07 5.184+07 0.000+00 0.000+00 1.315+08 1.314+09 0.000+00 0.000+00 3.865+01 5.017+01 0.000+00 0.000+00 0.000+00 0.000+00 6.772+07 6.779+07 0.000+00
1.737+02 0.000+00 0.000+00 0.000+00 1.877+02 5.820+03 0.000+00 0.000+00 0.000+00 0.000+00 2.251+02 4.079+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.595+04 1.325+03 0.000+00 0.000+00 4.119+01 0.000+00 0.000+00 1.231+04 1.587+03 0.000+00 0.000+00 1.981+01 0.000+00 0.000+00 6.552+00 2.052−01 0.000+00 0.000+00 4.915+02 3.821+02 0.000+00 0.000+00 1.224−01 0.000+00 0.000+00 5.068+02 2.280+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.449+03 1.622+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.081+03 1.673+03 0.000+00 0.000+00 3.692+01 0.000+00 0.000+00 0.000+00 1.099−04 0.000+00 0.000+00 2.243+01 0.000+00 0.000+00 2.257−01 0.000+00 0.000+00
0.000+00 6.750−05 8.985−04 0.000+00 0.000+00 0.000+00 4.237+03 3.012+04 0.000+00 0.000+00 0.000+00 0.000+00 4.394+03 3.130+04 0.000+00 0.000+00 4.873−04 2.716+04 0.000+00 0.000+00 0.000+00 1.621+05 0.000+00 0.000+00 2.878+04 0.000+00 0.000+00 0.000+00 1.679+05 0.000+00 0.000+00 2.266−02 0.000+00 0.000+00 2.835+02 0.000+00 0.000+00 0.000+00 5.339+04 6.854+04 0.000+00 2.641+02 0.000+00 0.000+00 0.000+00 3.762+04 4.838+04 0.000+00 0.000+00 3.063+03 7.878+03 0.000+00 0.000+00 0.000+00 4.672+05 0.000+00 2.856+03 7.313+03 0.000+00 0.000+00 0.000+00 3.291+05 0.000+00 0.000+00 0.000+00 3.186−03 0.000+00 0.000+00 1.850−11 0.000+00 0.000+00 2.727+03 0.000+00 0.000+00 1.044−04
(continued on next page)
36
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 12 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
8.845+03 3.732+03 3.293+03 3.206+03 8.399+01 8.255+01 8.216+01 8.163+01 8.151+01 8.148+01 6.457+03 5.246+03 5.028+03 4.614+03 8.479+01 8.333+01 8.293+01 8.239+01 8.227+01 8.223+01 8.217+01 8.217+01 2.798+04 2.273+04 1.617+04 8.592+01 8.442+01 8.401+01 8.345+01 8.333+01 8.329+01 8.323+01 8.323+01 1.212+05 3.830+04 8.618+01 8.467+01 8.426+01 8.370+01 8.358+01 8.354+01 8.348+01 8.348+01 8.344+01 5.600+04 8.625+01 8.473+01 8.432+01 8.376+01 8.363+01 8.360+01 8.354+01 8.354+01 8.350+01 8.444+01 8.389+01 8.376+01 8.373+01 8.366+01 8.366+01 8.362+01 4.824+03 3.772+03 2.909+03 2.762+03 2.727+03 1.730+04 7.326+03 6.460+03 6.272+03 1.271+04 1.031+04 9.839+03 9.027+03 9.020+03
0.000+00 1.158+07 0.000+00 0.000+00 6.203+10 0.000+00 0.000+00 2.830+11 0.000+00 0.000+00 4.466+05 5.010+06 0.000+00 0.000+00 1.290+11 0.000+00 0.000+00 5.734+10 3.418+11 0.000+00 0.000+00 0.000+00 0.000+00 3.589+04 0.000+00 0.000+00 5.181+10 4.864+09 0.000+00 0.000+00 5.660+11 0.000+00 0.000+00 1.690+01 8.044+03 0.000+00 0.000+00 4.458+10 0.000+00 0.000+00 4.042+10 6.057+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.225+10 5.687+08 0.000+00 0.000+00 9.628+11 0.000+00 0.000+00 0.000+00 1.151+10 0.000+00 0.000+00 3.557+10 9.970+11 1.643+07 3.452+07 0.000+00 0.000+00 0.000+00 0.000+00 4.187+06 0.000+00 0.000+00 1.602+05 1.804+06 0.000+00 0.000+00 0.000+00
0.000+00 4.839−02 0.000+00 0.000+00 6.560−02 0.000+00 0.000+00 5.655−01 0.000+00 0.000+00 2.791−03 3.101−02 0.000+00 0.000+00 6.953−02 0.000+00 0.000+00 5.835−02 5.201−01 0.000+00 0.000+00 0.000+00 0.000+00 4.170−03 0.000+00 0.000+00 2.768−02 5.146−03 0.000+00 0.000+00 8.831−01 0.000+00 0.000+00 3.719−05 2.358−03 0.000+00 0.000+00 3.163−02 0.000+00 0.000+00 4.230−02 8.438−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.594−03 5.964−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.079−03 0.000+00 0.000+00 3.733−02 1.306+00 5.732−02 1.473−01 0.000+00 0.000+00 0.000+00 0.000+00 6.738−02 0.000+00 0.000+00 3.879−03 4.313−02 0.000+00 0.000+00 0.000+00
0.000+00 1.189+00 0.000+00 0.000+00 3.627−02 0.000+00 0.000+00 3.039−01 0.000+00 0.000+00 2.373−01 2.142+00 0.000+00 0.000+00 7.763−02 0.000+00 0.000+00 6.331−02 5.635−01 0.000+00 0.000+00 0.000+00 0.000+00 1.248+00 0.000+00 0.000+00 3.077−02 5.693−03 0.000+00 0.000+00 9.686−01 0.000+00 0.000+00 8.899−02 1.784+00 0.000+00 0.000+00 5.265−02 0.000+00 0.000+00 6.979−02 1.391+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.422−02 9.852−04 0.000+00 0.000+00 2.216+00 0.000+00 0.000+00 0.000+00 2.003−02 0.000+00 0.000+00 8.225−02 2.877+00 1.821+00 3.657+00 0.000+00 0.000+00 0.000+00 0.000+00 3.250+00 0.000+00 0.000+00 6.491−01 5.856+00 0.000+00 0.000+00 0.000+00
6.130−03 0.000+00 0.000+00 3.805−01 0.000+00 0.000+00 2.647+07 0.000+00 0.000+00 8.867+07 0.000+00 0.000+00 1.142−02 7.921−02 0.000+00 5.278+07 2.629+07 0.000+00 0.000+00 2.471+07 1.114+08 0.000+00 4.010−06 0.000+00 0.000+00 1.604+07 0.000+00 0.000+00 2.120+07 6.052+06 0.000+00 0.000+00 1.037+08 0.000+00 0.000+00 2.406+07 0.000+00 0.000+00 9.059+06 2.414+07 0.000+00 0.000+00 1.140+07 1.143+08 3.199−08 0.000+00 5.684+06 7.950+05 0.000+00 0.000+00 1.488+07 1.860+06 0.000+00 0.000+00 4.780+06 0.000+00 0.000+00 2.475+06 1.547+07 0.000+00 0.000+00 0.000+00 0.000+00 8.896+00 1.156+01 0.000+00 1.347−03 0.000+00 0.000+00 1.295−01 0.000+00 0.000+00 3.886−03 2.696−02 0.000+00
1.298+01 0.000+00 0.000+00 0.000+00 0.000+00 7.036+00 6.324+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.092−07 0.000+00 0.000+00 1.524+03 4.978+01 0.000+00 0.000+00 1.026+00 0.000+00 0.000+00 4.921−01 0.000+00 0.000+00 2.227−02 0.000+00 0.000+00 2.351+01 5.606+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.501+02 7.770+01 0.000+00 0.000+00 1.435+00 0.000+00 6.579−02 0.000+00 0.000+00 1.218−03 0.000+00 0.000+00 3.417+01 8.021+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.178+01 8.035+01 0.000+00 0.000+00 0.000+00 0.000+00 8.185−06 0.000+00 0.000+00 1.735+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.653−08 0.000+00 0.000+00
0.000+00 3.666−06 4.897−05 0.000+00 0.000+00 0.000+00 0.000+00 1.874+02 1.328+03 0.000+00 0.000+00 2.604−05 0.000+00 0.000+00 1.983+03 0.000+00 0.000+00 0.000+00 7.226+03 0.000+00 0.000+00 1.392−04 0.000+00 1.824−09 1.286−08 0.000+00 3.214+01 0.000+00 0.000+00 0.000+00 2.142+03 2.744+03 0.000+00 0.000+00 1.186−09 0.000+00 3.468+02 8.997+02 0.000+00 0.000+00 0.000+00 1.880+04 0.000+00 0.000+00 0.000+00 7.934−08 0.000+00 0.000+00 4.599+01 0.000+00 0.000+00 0.000+00 9.204+03 4.818+03 0.000+00 7.919+01 3.556+02 0.000+00 0.000+00 0.000+00 4.448+04 0.000+00 2.677−04 0.000+00 0.000+00 1.185−12 0.000+00 3.441−07 4.603−06 0.000+00 0.000+00 2.428−06 0.000+00 0.000+00 9.657−16
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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37
Table 12 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
5.466+04 4.359+04 3.117+04 3.108+04 2.152+05 7.250+04 7.206+04 5.165+04 1.093+05 1.083+05 6.796+04 1.162+07 1.796+05 1.824+05
0.000+00 1.818+04 0.000+00 0.000+00 1.077+01 4.233+03 0.000+00 0.000+00 0.000+00 7.140+02 0.000+00 2.137−05 1.625+02 0.000+00
0.000+00 7.766−03 0.000+00 0.000+00 7.480−05 4.448−03 0.000+00 0.000+00 0.000+00 1.675−03 0.000+00 4.330−07 9.821−04 0.000+00
0.000+00 4.458+00 0.000+00 0.000+00 3.180−01 6.370+00 0.000+00 0.000+00 0.000+00 3.583+00 0.000+00 1.326−01 4.646+00 0.000+00
1.012−06 0.000+00 0.000+00 2.383−05 0.000+00 0.000+00 3.948−08 2.089−06 1.101−08 0.000+00 0.000+00 0.000+00 0.000+00 2.781−10
6.602−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.776−11 0.000+00 8.839−03 0.000+00 0.000+00 0.000+00 0.000+00 1.974−03
0.000+00 2.512−10 1.725−09 0.000+00 0.000+00 1.742−10 0.000+00 0.000+00 0.000+00 4.061−12 2.186−11 0.000+00 1.573−12 0.000+00
38
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 13 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Mn XXIII. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.659+02 2.064+02 1.174+01 1.160+01 1.155+01 1.150+01 1.149+01 8.733+00 8.700+00 8.690+00 8.678+00 8.675+00 8.674+00 7.814+00 7.801+00 7.797+00 7.792+00 7.791+00 7.790+00 9.222+02 1.228+01 1.213+01 1.208+01 1.202+01 1.201+01 9.029+00 8.995+00 8.984+00 8.971+00 8.967+00 8.966+00 8.051+00 8.037+00 8.033+00 8.027+00 8.026+00 8.026+00 1.245+01 1.229+01 1.224+01 1.218+01 1.217+01 9.119+00 9.083+00 9.072+00 9.059+00 9.055+00 9.054+00 9.053+00 8.122+00 8.108+00 8.103+00 8.098+00 8.096+00 8.096+00 8.095+00 8.095+00 9.583+02 7.330+02 5.698+02 5.387+02 3.410+01 3.361+01 3.346+01 3.327+01 3.323+01 3.322+01 2.337+01 2.325+01 2.322+01 2.317+01 2.316+01 2.316+01
1.744+09 3.783+09 0.000+00 6.302+12 6.110+12 0.000+00 0.000+00 0.000+00 2.774+12 2.716+12 0.000+00 0.000+00 0.000+00 0.000+00 1.432+12 1.407+12 0.000+00 0.000+00 0.000+00 0.000+00 7.619+11 0.000+00 0.000+00 1.552+13 0.000+00 3.058+11 0.000+00 0.000+00 5.060+12 0.000+00 0.000+00 1.537+11 0.000+00 0.000+00 2.335+12 0.000+00 0.000+00 1.600+12 0.000+00 0.000+00 3.061+12 1.838+13 6.377+11 0.000+00 0.000+00 9.873+11 5.954+12 0.000+00 0.000+00 3.176+11 0.000+00 0.000+00 4.531+11 2.738+12 0.000+00 0.000+00 0.000+00 2.272+08 5.122+08 0.000+00 0.000+00 0.000+00 8.254+11 7.957+11 0.000+00 0.000+00 0.000+00 0.000+00 4.524+11 4.400+11 0.000+00 0.000+00 0.000+00
1.849−02 4.833−02 0.000+00 1.271−01 2.446−01 0.000+00 0.000+00 0.000+00 3.148−02 6.150−02 0.000+00 0.000+00 0.000+00 0.000+00 1.307−02 2.565−02 0.000+00 0.000+00 0.000+00 0.000+00 1.723−02 0.000+00 0.000+00 6.725−01 0.000+00 3.737−03 0.000+00 0.000+00 1.221−01 0.000+00 0.000+00 1.493−03 0.000+00 0.000+00 4.510−02 0.000+00 0.000+00 1.858−02 0.000+00 0.000+00 6.810−02 6.117−01 3.975−03 0.000+00 0.000+00 1.214−02 1.098−01 0.000+00 0.000+00 1.570−03 0.000+00 0.000+00 4.454−03 4.036−02 0.000+00 0.000+00 0.000+00 3.128−02 8.250−02 0.000+00 0.000+00 0.000+00 1.398−01 2.670−01 0.000+00 0.000+00 0.000+00 0.000+00 3.668−02 7.112−02 0.000+00 0.000+00 0.000+00
3.238−02 6.568−02 0.000+00 9.703−03 1.861−02 0.000+00 0.000+00 0.000+00 1.803−03 3.519−03 0.000+00 0.000+00 0.000+00 0.000+00 6.712−04 1.317−03 0.000+00 0.000+00 0.000+00 0.000+00 1.393−03 0.000+00 0.000+00 5.323−02 0.000+00 2.222−04 0.000+00 0.000+00 7.212−03 0.000+00 0.000+00 7.917−05 0.000+00 0.000+00 2.384−03 0.000+00 0.000+00 3.046−03 0.000+00 0.000+00 1.092−02 9.799−02 4.773−04 0.000+00 0.000+00 1.449−03 1.309−02 0.000+00 0.000+00 1.679−04 0.000+00 0.000+00 4.750−04 4.303−03 0.000+00 0.000+00 0.000+00 1.974−01 3.982−01 0.000+00 0.000+00 0.000+00 3.093−02 5.882−02 0.000+00 0.000+00 0.000+00 0.000+00 5.616−03 1.087−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.246+09 9.284+09 0.000+00 0.000+00 0.000+00 1.242+09 1.269+09 0.000+00 0.000+00 0.000+00 0.000+00 3.171+08 3.286+08 0.000+00 1.001+00 0.000+00 0.000+00 1.839+09 0.000+00 0.000+00 0.000+00 0.000+00 8.000+08 0.000+00 0.000+00 7.110+09 0.000+00 0.000+00 4.309+08 0.000+00 0.000+00 4.760+09 0.000+00 3.645+09 1.813+09 0.000+00 0.000+00 0.000+00 1.545+09 7.779+08 0.000+00 0.000+00 2.029+09 9.097+09 0.000+00 8.023+08 4.058+08 0.000+00 0.000+00 1.358+09 6.097+09 0.000+00 0.000+00 0.000+00 2.637+02 3.512+02 0.000+00 0.000+00 0.000+00 6.371+08 6.384+08 0.000+00 0.000+00 0.000+00 0.000+00 2.137+08 2.161+08 0.000+00
0.000+00 0.000+00 9.965+04 0.000+00 0.000+00 5.581+03 0.000+00 8.412+04 0.000+00 0.000+00 3.268+03 0.000+00 0.000+00 5.508+04 0.000+00 0.000+00 1.831+03 0.000+00 0.000+00 1.142+04 0.000+00 2.317+04 1.608+05 0.000+00 0.000+00 0.000+00 1.816+04 8.220+04 0.000+00 0.000+00 0.000+00 0.000+00 1.174+04 4.540+04 0.000+00 0.000+00 0.000+00 0.000+00 6.005+05 1.624+05 0.000+00 0.000+00 0.000+00 3.501+05 1.274+05 0.000+00 0.000+00 1.860+03 0.000+00 0.000+00 2.019+05 8.105+04 0.000+00 0.000+00 1.635+03 0.000+00 0.000+00 0.000+00 0.000+00 3.752−03 0.000+00 1.010+03 0.000+00 0.000+00 2.393+01 0.000+00 0.000+00 1.260+03 0.000+00 0.000+00 3.174+01 0.000+00 0.000+00
0.000+00 9.787+00 0.000+00 0.000+00 5.056+06 0.000+00 0.000+00 0.000+00 0.000+00 3.968+06 0.000+00 0.000+00 2.145+00 0.000+00 0.000+00 2.552+06 0.000+00 0.000+00 1.919+00 0.000+00 0.000+00 0.000+00 0.000+00 4.709+05 3.372+06 0.000+00 0.000+00 0.000+00 2.751+05 1.976+06 0.000+00 0.000+00 0.000+00 0.000+00 1.584+05 1.139+06 0.000+00 1.145+06 0.000+00 0.000+00 0.000+00 1.773+07 8.509+05 0.000+00 0.000+00 0.000+00 1.035+07 0.000+00 0.000+00 5.342+05 0.000+00 0.000+00 0.000+00 5.947+06 0.000+00 0.000+00 2.727−01 0.000+00 1.052−01 0.000+00 0.000+00 0.000+00 0.000+00 7.853+04 0.000+00 0.000+00 1.165−02 0.000+00 0.000+00 9.012+04 0.000+00 0.000+00 3.200−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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39
Table 13 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
3.118+03 1.405+03 1.230+03 3.536+01 3.483+01 3.467+01 3.447+01 3.442+01 3.441+01 2.396+01 2.383+01 2.379+01 2.375+01 2.374+01 2.373+01 2.559+03 2.032+03 3.576+01 3.522+01 3.506+01 3.486+01 3.481+01 3.479+01 3.477+01 2.414+01 2.402+01 2.398+01 2.393+01 2.392+01 2.392+01 2.391+01 2.391+01 9.875+03 3.627+01 3.571+01 3.554+01 3.534+01 3.528+01 3.527+01 3.525+01 2.437+01 2.425+01 2.420+01 2.416+01 2.414+01 2.414+01 2.413+01 2.413+01 3.640+01 3.584+01 3.567+01 3.547+01 3.541+01 3.540+01 3.537+01 2.443+01 2.430+01 2.426+01 2.422+01 2.420+01 2.420+01 2.419+01 2.419+01 2.419+01 2.328+03 1.771+03 1.375+03 1.299+03 1.285+03 7.431+01 7.313+01 7.276+01 7.232+01 7.221+01 7.218+01
0.000+00 4.655+07 0.000+00 2.137+11 0.000+00 0.000+00 1.632+12 0.000+00 0.000+00 1.039+11 0.000+00 0.000+00 8.045+11 0.000+00 0.000+00 1.538+06 1.850+07 4.472+11 0.000+00 0.000+00 3.281+11 1.959+12 0.000+00 0.000+00 2.160+11 0.000+00 0.000+00 1.599+11 9.585+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.169+11 1.082+10 0.000+00 0.000+00 3.617+12 0.000+00 0.000+00 5.017+10 4.651+09 0.000+00 0.000+00 1.195+12 0.000+00 0.000+00 0.000+00 0.000+00 9.956+10 0.000+00 0.000+00 2.571+11 3.861+12 0.000+00 0.000+00 4.274+10 0.000+00 0.000+00 8.456+10 1.274+12 0.000+00 0.000+00 5.327+07 1.217+08 0.000+00 0.000+00 0.000+00 0.000+00 1.942+11 1.866+11 0.000+00 0.000+00 0.000+00
0.000+00 2.756−02 0.000+00 4.005−02 0.000+00 0.000+00 5.816−01 0.000+00 0.000+00 8.944−03 0.000+00 0.000+00 1.360−01 0.000+00 0.000+00 1.509−03 1.718−02 4.288−02 0.000+00 0.000+00 5.975−02 5.336−01 0.000+00 0.000+00 9.437−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.118−02 2.049−03 0.000+00 0.000+00 1.012+00 0.000+00 0.000+00 2.210−03 4.085−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.266−02 0.000+00 0.000+00 4.830−02 9.657−01 0.000+00 0.000+00 2.515−03 0.000+00 0.000+00 7.424−03 1.490−01 0.000+00 0.000+00 4.327−02 1.145−01 0.000+00 0.000+00 0.000+00 0.000+00 1.557−01 2.962−01 0.000+00 0.000+00 0.000+00
0.000+00 2.550−01 0.000+00 9.324−03 0.000+00 0.000+00 1.320−01 0.000+00 0.000+00 1.411−03 0.000+00 0.000+00 2.127−02 0.000+00 0.000+00 5.085−02 4.597−01 2.019−02 0.000+00 0.000+00 2.743−02 2.446−01 0.000+00 0.000+00 3.000−03 0.000+00 0.000+00 4.326−03 3.884−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.257−03 9.592−04 0.000+00 0.000+00 4.701−01 0.000+00 0.000+00 7.057−04 1.302−04 0.000+00 0.000+00 4.980−02 0.000+00 0.000+00 0.000+00 0.000+00 8.921−03 0.000+00 0.000+00 3.378−02 6.748−01 0.000+00 0.000+00 1.205−03 0.000+00 0.000+00 3.549−03 7.121−02 0.000+00 0.000+00 6.631−01 1.334+00 0.000+00 0.000+00 0.000+00 0.000+00 7.495−02 1.419−01 0.000+00 0.000+00 0.000+00
8.383−02 0.000+00 0.000+00 0.000+00 0.000+00 1.950+08 0.000+00 0.000+00 7.305+08 0.000+00 0.000+00 1.110+08 0.000+00 0.000+00 8.253+06 0.000+00 0.000+00 0.000+00 3.882+08 1.931+08 0.000+00 0.000+00 2.013+08 9.089+08 0.000+00 2.151+08 1.082+08 0.000+00 0.000+00 1.642+06 7.871+06 0.000+00 3.818−05 6.779+07 0.000+00 0.000+00 1.238+08 3.535+07 0.000+00 0.000+00 4.119+07 0.000+00 0.000+00 5.947+07 1.706+07 0.000+00 0.000+00 1.547+09 1.018+08 0.000+00 0.000+00 5.281+07 1.408+08 0.000+00 0.000+00 6.174+07 0.000+00 0.000+00 2.527+07 6.767+07 0.000+00 0.000+00 1.717+08 1.715+09 0.000+00 0.000+00 4.593+01 6.137+01 0.000+00 0.000+00 0.000+00 0.000+00 8.831+07 8.842+07 0.000+00
2.962+02 0.000+00 0.000+00 0.000+00 2.931+02 9.090+03 0.000+00 0.000+00 0.000+00 0.000+00 3.515+02 6.369+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.486+04 2.063+03 0.000+00 0.000+00 6.418+01 0.000+00 0.000+00 1.920+04 2.471+03 0.000+00 0.000+00 3.084+01 0.000+00 0.000+00 1.119+01 3.198−01 0.000+00 0.000+00 7.672+02 5.969+02 0.000+00 0.000+00 1.901−01 0.000+00 0.000+00 7.910+02 3.562+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.262+03 2.529+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.688+03 2.609+03 0.000+00 0.000+00 5.758+01 0.000+00 0.000+00 0.000+00 1.616−04 0.000+00 0.000+00 3.494+01 0.000+00 0.000+00 3.535−01 0.000+00 0.000+00
0.000+00 1.037−04 1.445−03 0.000+00 0.000+00 0.000+00 6.053+03 4.302+04 0.000+00 0.000+00 0.000+00 0.000+00 6.278+03 4.472+04 0.000+00 0.000+00 6.405−04 3.868+04 0.000+00 0.000+00 0.000+00 2.313+05 0.000+00 0.000+00 4.099+04 0.000+00 0.000+00 0.000+00 2.395+05 0.000+00 0.000+00 3.861−02 0.000+00 0.000+00 4.059+02 0.000+00 0.000+00 0.000+00 7.625+04 9.791+04 0.000+00 3.783+02 0.000+00 0.000+00 0.000+00 5.372+04 6.911+04 0.000+00 0.000+00 4.390+03 1.123+04 0.000+00 0.000+00 0.000+00 6.668+05 0.000+00 4.095+03 1.042+04 0.000+00 0.000+00 0.000+00 4.696+05 0.000+00 0.000+00 0.000+00 4.284−03 0.000+00 0.000+00 2.945−11 0.000+00 0.000+00 3.892+03 0.000+00 0.000+00 1.775−04
(continued on next page)
40
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 13 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
7.402+03 3.362+03 2.940+03 2.867+03 7.676+01 7.550+01 7.511+01 7.464+01 7.452+01 7.450+01 6.161+03 4.877+03 4.679+03 4.254+03 7.756+01 7.628+01 7.588+01 7.540+01 7.528+01 7.525+01 7.519+01 7.519+01 2.341+04 1.945+04 1.374+04 7.855+01 7.723+01 7.682+01 7.634+01 7.621+01 7.618+01 7.612+01 7.612+01 1.149+05 3.329+04 7.882+01 7.749+01 7.708+01 7.659+01 7.646+01 7.643+01 7.637+01 7.637+01 7.633+01 4.686+04 7.887+01 7.754+01 7.713+01 7.664+01 7.651+01 7.648+01 7.642+01 7.642+01 7.638+01 7.725+01 7.676+01 7.664+01 7.661+01 7.654+01 7.654+01 7.650+01 4.601+03 3.492+03 2.711+03 2.559+03 2.528+03 1.448+04 6.599+03 5.767+03 5.608+03 1.212+04 9.584+03 9.154+03 8.322+03 8.315+03
0.000+00 1.449+07 0.000+00 0.000+00 7.365+10 0.000+00 0.000+00 3.381+11 0.000+00 0.000+00 4.700+05 5.703+06 0.000+00 0.000+00 1.538+11 0.000+00 0.000+00 6.858+10 4.085+11 0.000+00 0.000+00 0.000+00 0.000+00 5.242+04 0.000+00 0.000+00 6.206+10 5.792+09 0.000+00 0.000+00 6.762+11 0.000+00 0.000+00 1.811+01 1.120+04 0.000+00 0.000+00 5.317+10 0.000+00 0.000+00 4.829+10 7.236+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.468+10 6.794+08 0.000+00 0.000+00 1.150+12 0.000+00 0.000+00 0.000+00 1.377+10 0.000+00 0.000+00 4.249+10 1.191+12 1.731+07 3.982+07 0.000+00 0.000+00 0.000+00 0.000+00 5.240+06 0.000+00 0.000+00 1.687+05 2.055+06 0.000+00 0.000+00 0.000+00
0.000+00 4.912−02 0.000+00 0.000+00 6.505−02 0.000+00 0.000+00 5.648−01 0.000+00 0.000+00 2.675−03 3.051−02 0.000+00 0.000+00 6.934−02 0.000+00 0.000+00 5.846−02 5.206−01 0.000+00 0.000+00 0.000+00 0.000+00 4.458−03 0.000+00 0.000+00 2.775−02 5.125−03 0.000+00 0.000+00 8.826−01 0.000+00 0.000+00 3.585−05 2.481−03 0.000+00 0.000+00 3.157−02 0.000+00 0.000+00 4.229−02 8.435−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.615−03 5.962−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.090−03 0.000+00 0.000+00 3.732−02 1.306+00 5.496−02 1.455−01 0.000+00 0.000+00 0.000+00 0.000+00 6.841−02 0.000+00 0.000+00 3.718−03 4.244−02 0.000+00 0.000+00 0.000+00
0.000+00 1.087+00 0.000+00 0.000+00 3.288−02 0.000+00 0.000+00 2.776−01 0.000+00 0.000+00 2.170−01 1.960+00 0.000+00 0.000+00 7.083−02 0.000+00 0.000+00 5.805−02 5.161−01 0.000+00 0.000+00 0.000+00 0.000+00 1.142+00 0.000+00 0.000+00 2.822−02 5.184−03 0.000+00 0.000+00 8.854−01 0.000+00 0.000+00 8.139−02 1.632+00 0.000+00 0.000+00 4.806−02 0.000+00 0.000+00 6.385−02 1.273+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.304−02 9.011−04 0.000+00 0.000+00 2.027+00 0.000+00 0.000+00 0.000+00 1.835−02 0.000+00 0.000+00 7.524−02 2.632+00 1.665+00 3.346+00 0.000+00 0.000+00 0.000+00 0.000+00 2.972+00 0.000+00 0.000+00 5.936−01 5.356+00 0.000+00 0.000+00 0.000+00
1.249−02 0.000+00 0.000+00 5.569−01 0.000+00 0.000+00 3.458+07 0.000+00 0.000+00 1.160+08 0.000+00 0.000+00 1.370−02 9.950−02 0.000+00 6.893+07 3.432+07 0.000+00 0.000+00 3.224+07 1.454+08 0.000+00 8.184−06 0.000+00 0.000+00 2.092+07 0.000+00 0.000+00 2.768+07 7.904+06 0.000+00 0.000+00 1.356+08 0.000+00 0.000+00 3.140+07 0.000+00 0.000+00 1.183+07 3.152+07 0.000+00 0.000+00 1.489+07 1.493+08 6.518−08 0.000+00 7.432+06 1.037+06 0.000+00 0.000+00 1.942+07 2.428+06 0.000+00 0.000+00 6.239+06 0.000+00 0.000+00 3.230+06 2.020+07 0.000+00 0.000+00 0.000+00 0.000+00 1.058+01 1.416+01 0.000+00 2.744−03 0.000+00 0.000+00 1.895−01 0.000+00 0.000+00 4.664−03 3.389−02 0.000+00
2.215+01 0.000+00 0.000+00 0.000+00 0.000+00 1.099+01 9.876+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.050−06 0.000+00 0.000+00 2.376+03 7.756+01 0.000+00 0.000+00 1.600+00 0.000+00 0.000+00 8.404−01 0.000+00 0.000+00 3.472−02 0.000+00 0.000+00 3.671+01 8.757+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.344+02 1.212+02 0.000+00 0.000+00 2.239+00 0.000+00 1.122−01 0.000+00 0.000+00 1.897−03 0.000+00 0.000+00 5.332+01 1.252+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.958+01 1.253+02 0.000+00 0.000+00 0.000+00 0.000+00 1.204−05 0.000+00 0.000+00 2.960+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.282−07 0.000+00 0.000+00
0.000+00 5.649−06 7.896−05 0.000+00 0.000+00 0.000+00 0.000+00 2.677+02 1.897+03 0.000+00 0.000+00 3.429−05 0.000+00 0.000+00 2.824+03 0.000+00 0.000+00 0.000+00 1.031+04 0.000+00 0.000+00 2.371−04 0.000+00 3.639−09 2.650−08 0.000+00 4.600+01 0.000+00 0.000+00 0.000+00 3.060+03 3.920+03 0.000+00 0.000+00 2.186−09 0.000+00 4.969+02 1.283+03 0.000+00 0.000+00 0.000+00 2.683+04 0.000+00 0.000+00 0.000+00 1.358−07 0.000+00 0.000+00 6.579+01 0.000+00 0.000+00 0.000+00 1.314+04 6.879+03 0.000+00 1.134+02 5.081+02 0.000+00 0.000+00 0.000+00 6.348+04 0.000+00 3.604−04 0.000+00 0.000+00 1.888−12 0.000+00 5.308−07 7.430−06 0.000+00 0.000+00 3.200−06 0.000+00 0.000+00 1.584−15
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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41
Table 13 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
4.573+04 3.736+04 2.653+04 2.647+04 2.042+05 6.319+04 6.283+04 4.451+04 9.151+04 9.075+04 5.692+04 1.097+07 1.506+05 1.527+05
0.000+00 2.640+04 0.000+00 0.000+00 1.154+01 5.850+03 0.000+00 0.000+00 0.000+00 1.111+03 0.000+00 2.324−05 2.522+02 0.000+00
0.000+00 8.289−03 0.000+00 0.000+00 7.212−05 4.669−03 0.000+00 0.000+00 0.000+00 1.829−03 0.000+00 4.196−07 1.072−03 0.000+00
0.000+00 4.078+00 0.000+00 0.000+00 2.909−01 5.828+00 0.000+00 0.000+00 0.000+00 3.278+00 0.000+00 1.213−01 4.250+00 0.000+00
2.067−06 0.000+00 0.000+00 4.457−05 0.000+00 0.000+00 6.556−08 3.680−06 2.245−08 0.000+00 0.000+00 0.000+00 0.000+00 5.665−10
1.128−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.042−10 0.000+00 1.508−02 0.000+00 0.000+00 0.000+00 0.000+00 3.366−03
0.000+00 4.968−10 3.531−09 0.000+00 0.000+00 3.169−10 0.000+00 0.000+00 0.000+00 9.001−12 4.854−11 0.000+00 3.471−12 0.000+00
42
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 14 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Fe XXIV. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.542+02 1.916+02 1.079+01 1.066+01 1.062+01 1.058+01 1.056+01 8.026+00 7.997+00 7.987+00 7.976+00 7.973+00 7.972+00 7.181+00 7.170+00 7.166+00 7.161+00 7.160+00 7.160+00 7.777+02 1.127+01 1.113+01 1.109+01 1.103+01 1.102+01 8.288+00 8.257+00 8.246+00 8.234+00 8.231+00 8.230+00 7.390+00 7.378+00 7.373+00 7.369+00 7.367+00 7.367+00 1.143+01 1.129+01 1.124+01 1.119+01 1.118+01 8.377+00 8.345+00 8.334+00 8.322+00 8.319+00 8.318+00 8.317+00 7.461+00 7.449+00 7.444+00 7.439+00 7.438+00 7.438+00 7.437+00 7.437+00 9.157+02 6.791+02 5.316+02 4.997+02 3.133+01 3.089+01 3.074+01 3.058+01 3.053+01 3.052+01 2.147+01 2.137+01 2.133+01 2.129+01 2.128+01 2.128+01
1.832+09 4.346+09 0.000+00 7.491+12 7.244+12 0.000+00 0.000+00 0.000+00 3.294+12 3.219+12 0.000+00 0.000+00 0.000+00 0.000+00 1.700+12 1.667+12 0.000+00 0.000+00 0.000+00 0.000+00 8.972+11 0.000+00 0.000+00 1.840+13 0.000+00 3.604+11 0.000+00 0.000+00 6.003+12 0.000+00 0.000+00 1.813+11 0.000+00 0.000+00 2.769+12 0.000+00 0.000+00 1.892+12 0.000+00 0.000+00 3.626+12 2.177+13 7.548+11 0.000+00 0.000+00 1.169+12 7.051+12 0.000+00 0.000+00 3.760+11 0.000+00 0.000+00 5.361+11 3.242+12 0.000+00 0.000+00 0.000+00 2.389+08 5.913+08 0.000+00 0.000+00 0.000+00 9.824+11 9.440+11 0.000+00 0.000+00 0.000+00 0.000+00 5.378+11 5.220+11 0.000+00 0.000+00 0.000+00
1.775−02 4.783−02 0.000+00 1.277−01 2.450−01 0.000+00 0.000+00 0.000+00 3.158−02 6.156−02 0.000+00 0.000+00 0.000+00 0.000+00 1.310−02 2.567−02 0.000+00 0.000+00 0.000+00 0.000+00 1.708−02 0.000+00 0.000+00 6.719−01 0.000+00 3.711−03 0.000+00 0.000+00 1.220−01 0.000+00 0.000+00 1.485−03 0.000+00 0.000+00 4.509−02 0.000+00 0.000+00 1.855−02 0.000+00 0.000+00 6.812−02 6.117−01 3.970−03 0.000+00 0.000+00 1.213−02 1.097−01 0.000+00 0.000+00 1.569−03 0.000+00 0.000+00 4.448−03 4.033−02 0.000+00 0.000+00 0.000+00 3.004−02 8.178−02 0.000+00 0.000+00 0.000+00 1.406−01 2.675−01 0.000+00 0.000+00 0.000+00 0.000+00 3.682−02 7.121−02 0.000+00 0.000+00 0.000+00
2.970−02 6.033−02 0.000+00 8.968−03 1.714−02 0.000+00 0.000+00 0.000+00 1.663−03 3.237−03 0.000+00 0.000+00 0.000+00 0.000+00 6.183−04 1.211−03 0.000+00 0.000+00 0.000+00 0.000+00 1.267−03 0.000+00 0.000+00 4.882−02 0.000+00 2.025−04 0.000+00 0.000+00 6.617−03 0.000+00 0.000+00 7.224−05 0.000+00 0.000+00 2.188−03 0.000+00 0.000+00 2.792−03 0.000+00 0.000+00 1.004−02 9.005−02 4.379−04 0.000+00 0.000+00 1.330−03 1.202−02 0.000+00 0.000+00 1.541−04 0.000+00 0.000+00 4.357−04 3.950−03 0.000+00 0.000+00 0.000+00 1.811−01 3.657−01 0.000+00 0.000+00 0.000+00 2.859−02 5.414−02 0.000+00 0.000+00 0.000+00 0.000+00 5.180−03 1.000−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.189+10 1.194+10 0.000+00 0.000+00 0.000+00 1.589+09 1.626+09 0.000+00 0.000+00 0.000+00 0.000+00 4.037+08 4.200+08 0.000+00 1.979+00 0.000+00 0.000+00 2.375+09 0.000+00 0.000+00 0.000+00 0.000+00 1.034+09 0.000+00 0.000+00 9.177+09 0.000+00 0.000+00 5.580+08 0.000+00 0.000+00 6.143+09 0.000+00 4.703+09 2.337+09 0.000+00 0.000+00 0.000+00 1.991+09 1.003+09 0.000+00 0.000+00 2.618+09 1.174+10 0.000+00 1.034+09 5.236+08 0.000+00 0.000+00 1.753+09 7.864+09 0.000+00 0.000+00 0.000+00 3.143+02 4.311+02 0.000+00 0.000+00 0.000+00 8.210+08 8.229+08 0.000+00 0.000+00 0.000+00 0.000+00 2.747+08 2.781+08 0.000+00
0.000+00 0.000+00 1.520+05 0.000+00 0.000+00 8.511+03 0.000+00 1.283+05 0.000+00 0.000+00 4.981+03 0.000+00 0.000+00 8.399+04 0.000+00 0.000+00 2.789+03 0.000+00 0.000+00 1.904+04 0.000+00 3.550+04 2.465+05 0.000+00 0.000+00 0.000+00 2.782+04 1.260+05 0.000+00 0.000+00 0.000+00 0.000+00 1.798+04 6.962+04 0.000+00 0.000+00 0.000+00 0.000+00 9.181+05 2.476+05 0.000+00 0.000+00 0.000+00 5.353+05 1.942+05 0.000+00 0.000+00 2.846+03 0.000+00 0.000+00 3.086+05 1.236+05 0.000+00 0.000+00 2.502+03 0.000+00 0.000+00 0.000+00 0.000+00 5.458−03 0.000+00 1.543+03 0.000+00 0.000+00 3.664+01 0.000+00 0.000+00 1.925+03 0.000+00 0.000+00 4.856+01 0.000+00 0.000+00
0.000+00 1.305+01 0.000+00 0.000+00 7.093+06 0.000+00 0.000+00 0.000+00 0.000+00 5.567+06 0.000+00 0.000+00 3.566+00 0.000+00 0.000+00 3.580+06 0.000+00 0.000+00 3.194+00 0.000+00 0.000+00 0.000+00 0.000+00 6.626+05 4.747+06 0.000+00 0.000+00 0.000+00 3.870+05 2.782+06 0.000+00 0.000+00 0.000+00 0.000+00 2.228+05 1.604+06 0.000+00 1.606+06 0.000+00 0.000+00 0.000+00 2.487+07 1.194+06 0.000+00 0.000+00 0.000+00 1.451+07 0.000+00 0.000+00 7.498+05 0.000+00 0.000+00 0.000+00 8.339+06 0.000+00 0.000+00 4.538−01 0.000+00 1.414−01 0.000+00 0.000+00 0.000+00 0.000+00 1.104+05 0.000+00 0.000+00 1.936−02 0.000+00 0.000+00 1.266+05 0.000+00 0.000+00 5.296−03 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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43
Table 14 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
2.628+03 1.267+03 1.100+03 3.244+01 3.197+01 3.181+01 3.164+01 3.159+01 3.158+01 2.199+01 2.188+01 2.184+01 2.180+01 2.179+01 2.178+01 2.447+03 1.891+03 3.284+01 3.237+01 3.220+01 3.202+01 3.197+01 3.196+01 3.194+01 2.217+01 2.206+01 2.202+01 2.198+01 2.197+01 2.197+01 2.196+01 2.196+01 8.325+03 3.329+01 3.280+01 3.263+01 3.245+01 3.239+01 3.238+01 3.236+01 2.238+01 2.226+01 2.222+01 2.218+01 2.217+01 2.217+01 2.216+01 2.216+01 3.342+01 3.293+01 3.276+01 3.257+01 3.252+01 3.251+01 3.248+01 2.244+01 2.232+01 2.228+01 2.224+01 2.223+01 2.222+01 2.222+01 2.222+01 2.221+01 2.224+03 1.640+03 1.283+03 1.204+03 1.191+03 6.826+01 6.721+01 6.685+01 6.646+01 6.635+01 6.633+01
0.000+00 5.827+07 0.000+00 2.518+11 0.000+00 0.000+00 1.936+12 0.000+00 0.000+00 1.226+11 0.000+00 0.000+00 9.543+11 0.000+00 0.000+00 1.613+06 2.107+07 5.293+11 0.000+00 0.000+00 3.892+11 2.323+12 0.000+00 0.000+00 2.557+11 0.000+00 0.000+00 1.896+11 1.136+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.391+11 1.279+10 0.000+00 0.000+00 4.290+12 0.000+00 0.000+00 5.969+10 5.497+09 0.000+00 0.000+00 1.418+12 0.000+00 0.000+00 0.000+00 0.000+00 1.179+11 0.000+00 0.000+00 3.048+11 4.577+12 0.000+00 0.000+00 5.061+10 0.000+00 0.000+00 1.002+11 1.510+12 0.000+00 0.000+00 5.603+07 1.408+08 0.000+00 0.000+00 0.000+00 0.000+00 2.312+11 2.214+11 0.000+00 0.000+00 0.000+00
0.000+00 2.806−02 0.000+00 3.972−02 0.000+00 0.000+00 5.809−01 0.000+00 0.000+00 8.886−03 0.000+00 0.000+00 1.360−01 0.000+00 0.000+00 1.448−03 1.695−02 4.280−02 0.000+00 0.000+00 5.983−02 5.339−01 0.000+00 0.000+00 9.424−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.122−02 2.041−03 0.000+00 0.000+00 1.012+00 0.000+00 0.000+00 2.218−03 4.070−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.264−02 0.000+00 0.000+00 4.829−02 9.655−01 0.000+00 0.000+00 2.511−03 0.000+00 0.000+00 7.421−03 1.490−01 0.000+00 0.000+00 4.156−02 1.135−01 0.000+00 0.000+00 0.000+00 0.000+00 1.566−01 2.967−01 0.000+00 0.000+00 0.000+00
0.000+00 2.341−01 0.000+00 8.484−03 0.000+00 0.000+00 1.210−01 0.000+00 0.000+00 1.287−03 0.000+00 0.000+00 1.951−02 0.000+00 0.000+00 4.666−02 4.221−01 1.851−02 0.000+00 0.000+00 2.523−02 2.248−01 0.000+00 0.000+00 2.752−03 0.000+00 0.000+00 3.975−03 3.567−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.845−03 8.768−04 0.000+00 0.000+00 4.314−01 0.000+00 0.000+00 6.502−04 1.191−04 0.000+00 0.000+00 4.572−02 0.000+00 0.000+00 0.000+00 0.000+00 8.179−03 0.000+00 0.000+00 3.101−02 6.195−01 0.000+00 0.000+00 1.105−03 0.000+00 0.000+00 3.258−03 6.538−02 0.000+00 0.000+00 6.086−01 1.225+00 0.000+00 0.000+00 0.000+00 0.000+00 6.930−02 1.306−01 0.000+00 0.000+00 0.000+00
1.658−01 0.000+00 0.000+00 0.000+00 0.000+00 2.518+08 0.000+00 0.000+00 9.451+08 0.000+00 0.000+00 1.435+08 0.000+00 0.000+00 1.084+07 0.000+00 0.000+00 0.000+00 5.011+08 2.492+08 0.000+00 0.000+00 2.596+08 1.172+09 0.000+00 2.774+08 1.397+08 0.000+00 0.000+00 2.091+06 1.008+07 0.000+00 7.555−05 8.742+07 0.000+00 0.000+00 1.598+08 4.564+07 0.000+00 0.000+00 5.314+07 0.000+00 0.000+00 7.677+07 2.204+07 0.000+00 0.000+00 1.997+09 1.313+08 0.000+00 0.000+00 6.817+07 1.817+08 0.000+00 0.000+00 7.965+07 0.000+00 0.000+00 3.259+07 8.732+07 0.000+00 0.000+00 2.216+08 2.213+09 0.000+00 0.000+00 5.486+01 7.553+01 0.000+00 0.000+00 0.000+00 0.000+00 1.139+08 1.140+08 0.000+00
4.942+02 0.000+00 0.000+00 0.000+00 4.492+02 1.394+04 0.000+00 0.000+00 0.000+00 0.000+00 5.388+02 9.762+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.805+04 3.153+03 0.000+00 0.000+00 9.815+01 0.000+00 0.000+00 2.938+04 3.776+03 0.000+00 0.000+00 4.713+01 0.000+00 0.000+00 1.867+01 4.890−01 0.000+00 0.000+00 1.175+03 9.150+02 0.000+00 0.000+00 2.901−01 0.000+00 0.000+00 1.212+03 5.460+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.464+03 3.871+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.585+03 3.993+03 0.000+00 0.000+00 8.814+01 0.000+00 0.000+00 0.000+00 2.356−04 0.000+00 0.000+00 5.344+01 0.000+00 0.000+00 5.429−01 0.000+00 0.000+00
0.000+00 1.596−04 2.324−03 0.000+00 0.000+00 0.000+00 8.520+03 6.055+04 0.000+00 0.000+00 0.000+00 0.000+00 8.835+03 6.294+04 0.000+00 0.000+00 8.422−04 5.429+04 0.000+00 0.000+00 0.000+00 3.250+05 0.000+00 0.000+00 5.754+04 0.000+00 0.000+00 0.000+00 3.364+05 0.000+00 0.000+00 6.432−02 0.000+00 0.000+00 5.727+02 0.000+00 0.000+00 0.000+00 1.073+05 1.378+05 0.000+00 5.340+02 0.000+00 0.000+00 0.000+00 7.556+04 9.725+04 0.000+00 0.000+00 6.202+03 1.577+04 0.000+00 0.000+00 0.000+00 9.372+05 0.000+00 5.788+03 1.464+04 0.000+00 0.000+00 0.000+00 6.599+05 0.000+00 0.000+00 0.000+00 5.777−03 0.000+00 0.000+00 4.666−11 0.000+00 0.000+00 5.473+03 0.000+00 0.000+00 2.953−04 (continued on next page)
44
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 14 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
6.241+03 3.031+03 2.627+03 2.566+03 7.042+01 6.931+01 6.892+01 6.851+01 6.839+01 6.836+01 5.892+03 4.537+03 4.356+03 3.924+03 7.122+01 7.009+01 6.969+01 6.927+01 6.915+01 6.912+01 6.906+01 6.906+01 1.973+04 1.672+04 1.175+04 7.209+01 7.093+01 7.052+01 7.009+01 6.997+01 6.994+01 6.988+01 6.988+01 1.093+05 2.903+04 7.236+01 7.119+01 7.077+01 7.034+01 7.022+01 7.019+01 7.013+01 7.013+01 7.009+01 3.952+04 7.241+01 7.123+01 7.082+01 7.039+01 7.026+01 7.024+01 7.017+01 7.017+01 7.013+01 7.095+01 7.051+01 7.039+01 7.036+01 7.030+01 7.030+01 7.026+01 4.397+03 3.233+03 2.528+03 2.372+03 2.344+03 1.221+04 5.947+03 5.152+03 5.019+03 1.160+04 8.914+03 8.523+03 7.675+03 7.669+03
0.000+00 1.816+07 0.000+00 0.000+00 8.684+10 0.000+00 0.000+00 4.008+11 0.000+00 0.000+00 4.932+05 6.504+06 0.000+00 0.000+00 1.820+11 0.000+00 0.000+00 8.140+10 4.845+11 0.000+00 0.000+00 0.000+00 0.000+00 7.580+04 0.000+00 0.000+00 7.381+10 6.847+09 0.000+00 0.000+00 8.018+11 0.000+00 0.000+00 1.931+01 1.551+04 0.000+00 0.000+00 6.297+10 0.000+00 0.000+00 5.726+10 8.579+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.744+10 8.055+08 0.000+00 0.000+00 1.364+12 0.000+00 0.000+00 0.000+00 1.634+10 0.000+00 0.000+00 5.037+10 1.412+12 1.821+07 4.608+07 0.000+00 0.000+00 0.000+00 0.000+00 6.573+06 0.000+00 0.000+00 1.770+05 2.345+06 0.000+00 0.000+00 0.000+00
0.000+00 5.003−02 0.000+00 0.000+00 6.456−02 0.000+00 0.000+00 5.640−01 0.000+00 0.000+00 2.567−03 3.011−02 0.000+00 0.000+00 6.922−02 0.000+00 0.000+00 5.855−02 5.210−01 0.000+00 0.000+00 0.000+00 0.000+00 4.763−03 0.000+00 0.000+00 2.784−02 5.105−03 0.000+00 0.000+00 8.820−01 0.000+00 0.000+00 3.460−05 2.613−03 0.000+00 0.000+00 3.152−02 0.000+00 0.000+00 4.229−02 8.433−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.638−03 5.961−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.102−03 0.000+00 0.000+00 3.732−02 1.306+00 5.279−02 1.444−01 0.000+00 0.000+00 0.000+00 0.000+00 6.970−02 0.000+00 0.000+00 3.569−03 4.189−02 0.000+00 0.000+00 0.000+00
0.000+00 9.983−01 0.000+00 0.000+00 2.993−02 0.000+00 0.000+00 2.544−01 0.000+00 0.000+00 1.992−01 1.799+00 0.000+00 0.000+00 6.492−02 0.000+00 0.000+00 5.341−02 4.744−01 0.000+00 0.000+00 0.000+00 0.000+00 1.048+00 0.000+00 0.000+00 2.600−02 4.740−03 0.000+00 0.000+00 8.124−01 0.000+00 0.000+00 7.473−02 1.498+00 0.000+00 0.000+00 4.407−02 0.000+00 0.000+00 5.864−02 1.168+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.201−02 8.274−04 0.000+00 0.000+00 1.861+00 0.000+00 0.000+00 0.000+00 1.687−02 0.000+00 0.000+00 6.909−02 2.417+00 1.528+00 3.073+00 0.000+00 0.000+00 0.000+00 0.000+00 2.729+00 0.000+00 0.000+00 5.449−01 4.918+00 0.000+00 0.000+00 0.000+00
2.471−02 0.000+00 0.000+00 8.179−01 0.000+00 0.000+00 4.466+07 0.000+00 0.000+00 1.500+08 0.000+00 0.000+00 1.650−02 1.256−01 0.000+00 8.900+07 4.430+07 0.000+00 0.000+00 4.160+07 1.877+08 0.000+00 1.621−05 0.000+00 0.000+00 2.699+07 0.000+00 0.000+00 3.575+07 1.021+07 0.000+00 0.000+00 1.753+08 0.000+00 0.000+00 4.051+07 0.000+00 0.000+00 1.527+07 4.070+07 0.000+00 0.000+00 1.923+07 1.928+08 1.289−07 0.000+00 9.610+06 1.339+06 0.000+00 0.000+00 2.507+07 3.135+06 0.000+00 0.000+00 8.053+06 0.000+00 0.000+00 4.170+06 2.607+07 0.000+00 0.000+00 0.000+00 0.000+00 1.265+01 1.745+01 0.000+00 5.428−03 0.000+00 0.000+00 2.784−01 0.000+00 0.000+00 5.619−03 4.281−02 0.000+00
3.695+01 0.000+00 0.000+00 0.000+00 0.000+00 1.684+01 1.514+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.541−06 0.000+00 0.000+00 3.638+03 1.186+02 0.000+00 0.000+00 2.449+00 0.000+00 0.000+00 1.403+00 0.000+00 0.000+00 5.314−02 0.000+00 0.000+00 5.623+01 1.342+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.590+02 1.856+02 0.000+00 0.000+00 3.428+00 0.000+00 1.871−01 0.000+00 0.000+00 2.898−03 0.000+00 0.000+00 8.164+01 1.917+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.591+01 1.918+02 0.000+00 0.000+00 0.000+00 0.000+00 1.757−05 0.000+00 0.000+00 4.939+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.881−07 0.000+00 0.000+00
0.000+00 8.715−06 1.272−04 0.000+00 0.000+00 0.000+00 0.000+00 3.767+02 2.668+03 0.000+00 0.000+00 4.518−05 0.000+00 0.000+00 3.966+03 0.000+00 0.000+00 0.000+00 1.450+04 0.000+00 0.000+00 3.949−04 0.000+00 7.121−09 5.336−08 0.000+00 6.487+01 0.000+00 0.000+00 0.000+00 4.304+03 5.514+03 0.000+00 0.000+00 3.981−09 0.000+00 7.014+02 1.802+03 0.000+00 0.000+00 0.000+00 3.772+04 0.000+00 0.000+00 0.000+00 2.267−07 0.000+00 0.000+00 9.272+01 0.000+00 0.000+00 0.000+00 1.848+04 9.675+03 0.000+00 1.599+02 7.151+02 0.000+00 0.000+00 0.000+00 8.923+04 0.000+00 4.866−04 0.000+00 0.000+00 2.995−12 0.000+00 8.197−07 1.199−05 0.000+00 0.000+00 4.221−06 0.000+00 0.000+00 2.582−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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45
Table 14 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
3.855+04 3.216+04 2.270+04 2.265+04 1.943+05 5.523+04 5.494+04 3.851+04 7.716+04 7.660+04 4.803+04 1.039+07 1.272+05 1.288+05
0.000+00 3.800+04 0.000+00 0.000+00 1.230+01 8.046+03 0.000+00 0.000+00 0.000+00 1.696+03 0.000+00 2.511−05 3.843+02 0.000+00
0.000+00 8.841−03 0.000+00 0.000+00 6.960−05 4.906−03 0.000+00 0.000+00 0.000+00 1.990−03 0.000+00 4.067−07 1.165−03 0.000+00
0.000+00 3.745+00 0.000+00 0.000+00 2.670−01 5.352+00 0.000+00 0.000+00 0.000+00 3.010+00 0.000+00 1.113−01 3.903+00 0.000+00
4.094−06 0.000+00 0.000+00 8.183−05 0.000+00 0.000+00 1.082−07 6.405−06 4.439−08 0.000+00 0.000+00 0.000+00 0.000+00 1.120−09
1.882−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.848−10 0.000+00 2.514−02 0.000+00 0.000+00 0.000+00 0.000+00 5.611−03
0.000+00 9.646−10 7.067−09 0.000+00 0.000+00 5.706−10 0.000+00 0.000+00 0.000+00 1.930−11 1.042−10 0.000+00 7.415−12 0.000+00
46
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 15 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Co XXV. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.434+02 1.778+02 9.950+00 9.839+00 9.796+00 9.755+00 9.741+00 7.400+00 7.375+00 7.365+00 7.355+00 7.352+00 7.351+00 6.622+00 6.611+00 6.607+00 6.603+00 6.602+00 6.602+00 6.602+02 1.038+01 1.025+01 1.021+01 1.016+01 1.015+01 7.633+00 7.605+00 7.594+00 7.584+00 7.581+00 7.580+00 6.807+00 6.796+00 6.791+00 6.787+00 6.786+00 6.786+00 1.054+01 1.041+01 1.037+01 1.032+01 1.031+01 7.722+00 7.694+00 7.683+00 7.672+00 7.669+00 7.668+00 7.667+00 6.878+00 6.866+00 6.862+00 6.858+00 6.856+00 6.856+00 6.855+00 6.855+00 8.765+02 6.293+02 4.962+02 4.636+02 2.888+01 2.849+01 2.834+01 2.820+01 2.815+01 2.814+01 1.979+01 1.970+01 1.966+01 1.963+01 1.962+01 1.961+01
1.921+09 5.008+09 0.000+00 8.841+12 8.527+12 0.000+00 0.000+00 0.000+00 3.883+12 3.788+12 0.000+00 0.000+00 0.000+00 0.000+00 2.003+12 1.962+12 0.000+00 0.000+00 0.000+00 0.000+00 1.050+12 0.000+00 0.000+00 2.168+13 0.000+00 4.222+11 0.000+00 0.000+00 7.072+12 0.000+00 0.000+00 2.125+11 0.000+00 0.000+00 3.263+12 0.000+00 0.000+00 2.225+12 0.000+00 0.000+00 4.266+12 2.561+13 8.879+11 0.000+00 0.000+00 1.373+12 8.292+12 0.000+00 0.000+00 4.424+11 0.000+00 0.000+00 6.299+11 3.812+12 0.000+00 0.000+00 0.000+00 2.509+08 6.849+08 0.000+00 0.000+00 0.000+00 1.161+12 1.112+12 0.000+00 0.000+00 0.000+00 0.000+00 6.350+11 6.147+11 0.000+00 0.000+00 0.000+00
1.706−02 4.749−02 0.000+00 1.283−01 2.453−01 0.000+00 0.000+00 0.000+00 3.166−02 6.161−02 0.000+00 0.000+00 0.000+00 0.000+00 1.313−02 2.568−02 0.000+00 0.000+00 0.000+00 0.000+00 1.694−02 0.000+00 0.000+00 6.713−01 0.000+00 3.687−03 0.000+00 0.000+00 1.220−01 0.000+00 0.000+00 1.476−03 0.000+00 0.000+00 4.507−02 0.000+00 0.000+00 1.853−02 0.000+00 0.000+00 6.813−02 6.118−01 3.969−03 0.000+00 0.000+00 1.212−02 1.097−01 0.000+00 0.000+00 1.569−03 0.000+00 0.000+00 4.441−03 4.030−02 0.000+00 0.000+00 0.000+00 2.889−02 8.132−02 0.000+00 0.000+00 0.000+00 1.413−01 2.678−01 0.000+00 0.000+00 0.000+00 0.000+00 3.694−02 7.126−02 0.000+00 0.000+00 0.000+00
2.734−02 5.560−02 0.000+00 8.312−03 1.582−02 0.000+00 0.000+00 0.000+00 1.538−03 2.987−03 0.000+00 0.000+00 0.000+00 0.000+00 5.714−04 1.117−03 0.000+00 0.000+00 0.000+00 0.000+00 1.157−03 0.000+00 0.000+00 4.492−02 0.000+00 1.853−04 0.000+00 0.000+00 6.091−03 0.000+00 0.000+00 6.616−05 0.000+00 0.000+00 2.014−03 0.000+00 0.000+00 2.572−03 0.000+00 0.000+00 9.260−03 8.303−02 4.035−04 0.000+00 0.000+00 1.225−03 1.108−02 0.000+00 0.000+00 1.421−04 0.000+00 0.000+00 4.011−04 3.638−03 0.000+00 0.000+00 0.000+00 1.668−01 3.370−01 0.000+00 0.000+00 0.000+00 2.650−02 4.996−02 0.000+00 0.000+00 0.000+00 0.000+00 4.792−03 9.226−03 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.514+10 1.522+10 0.000+00 0.000+00 0.000+00 2.013+09 2.065+09 0.000+00 0.000+00 0.000+00 0.000+00 5.098+08 5.322+08 0.000+00 3.805+00 0.000+00 0.000+00 3.034+09 0.000+00 0.000+00 0.000+00 0.000+00 1.322+09 0.000+00 0.000+00 1.172+10 0.000+00 0.000+00 7.152+08 0.000+00 0.000+00 7.846+09 0.000+00 6.005+09 2.983+09 0.000+00 0.000+00 0.000+00 2.539+09 1.280+09 0.000+00 0.000+00 3.344+09 1.498+10 0.000+00 1.318+09 6.685+08 0.000+00 0.000+00 2.238+09 1.004+10 0.000+00 0.000+00 0.000+00 3.765+02 5.324+02 0.000+00 0.000+00 0.000+00 1.048+09 1.050+09 0.000+00 0.000+00 0.000+00 0.000+00 3.498+08 3.544+08 0.000+00
0.000+00 0.000+00 2.279+05 0.000+00 0.000+00 1.277+04 0.000+00 1.925+05 0.000+00 0.000+00 7.466+03 0.000+00 0.000+00 1.260+05 0.000+00 0.000+00 4.178+03 0.000+00 0.000+00 3.110+04 0.000+00 5.349+04 3.716+05 0.000+00 0.000+00 0.000+00 4.191+04 1.900+05 0.000+00 0.000+00 0.000+00 0.000+00 2.709+04 1.050+05 0.000+00 0.000+00 0.000+00 0.000+00 1.380+06 3.714+05 0.000+00 0.000+00 0.000+00 8.046+05 2.913+05 0.000+00 0.000+00 4.279+03 0.000+00 0.000+00 4.638+05 1.852+05 0.000+00 0.000+00 3.763+03 0.000+00 0.000+00 0.000+00 0.000+00 7.884−03 0.000+00 2.319+03 0.000+00 0.000+00 5.515+01 0.000+00 0.000+00 2.893+03 0.000+00 0.000+00 7.305+01 0.000+00 0.000+00
0.000+00 1.745+01 0.000+00 0.000+00 9.818+06 0.000+00 0.000+00 0.000+00 0.000+00 7.705+06 0.000+00 0.000+00 5.811+00 0.000+00 0.000+00 4.956+06 0.000+00 0.000+00 5.208+00 0.000+00 0.000+00 0.000+00 0.000+00 9.198+05 6.593+06 0.000+00 0.000+00 0.000+00 5.370+05 3.865+06 0.000+00 0.000+00 0.000+00 0.000+00 3.091+05 2.228+06 0.000+00 2.223+06 0.000+00 0.000+00 0.000+00 3.442+07 1.654+06 0.000+00 0.000+00 0.000+00 2.008+07 0.000+00 0.000+00 1.039+06 0.000+00 0.000+00 0.000+00 1.153+07 0.000+00 0.000+00 7.397−01 0.000+00 1.908−01 0.000+00 0.000+00 0.000+00 0.000+00 1.530+05 0.000+00 0.000+00 3.152−02 0.000+00 0.000+00 1.755+05 0.000+00 0.000+00 8.599−03 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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47
Table 15 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
2.231+03 1.143+03 9.842+02 2.986+01 2.945+01 2.929+01 2.914+01 2.908+01 2.908+01 2.025+01 2.015+01 2.011+01 2.008+01 2.007+01 2.006+01 2.345+03 1.761+03 3.027+01 2.984+01 2.968+01 2.952+01 2.947+01 2.946+01 2.943+01 2.044+01 2.034+01 2.030+01 2.026+01 2.025+01 2.025+01 2.024+01 2.024+01 7.067+03 3.066+01 3.023+01 3.006+01 2.990+01 2.984+01 2.983+01 2.981+01 2.061+01 2.051+01 2.047+01 2.044+01 2.042+01 2.042+01 2.042+01 2.042+01 3.080+01 3.036+01 3.018+01 3.002+01 2.997+01 2.996+01 2.993+01 2.067+01 2.057+01 2.053+01 2.050+01 2.048+01 2.048+01 2.047+01 2.047+01 2.047+01 2.129+03 1.519+03 1.197+03 1.117+03 1.105+03 6.291+01 6.199+01 6.162+01 6.128+01 6.116+01 6.114+01
0.000+00 7.306+07 0.000+00 2.949+11 0.000+00 0.000+00 2.279+12 0.000+00 0.000+00 1.437+11 0.000+00 0.000+00 1.124+12 0.000+00 0.000+00 1.687+06 2.404+07 6.226+11 0.000+00 0.000+00 4.585+11 2.735+12 0.000+00 0.000+00 3.009+11 0.000+00 0.000+00 2.232+11 1.338+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.645+11 1.501+10 0.000+00 0.000+00 5.052+12 0.000+00 0.000+00 7.057+10 6.453+09 0.000+00 0.000+00 1.670+12 0.000+00 0.000+00 0.000+00 0.000+00 1.386+11 0.000+00 0.000+00 3.588+11 5.389+12 0.000+00 0.000+00 5.954+10 0.000+00 0.000+00 1.179+11 1.778+12 0.000+00 0.000+00 5.884+07 1.633+08 0.000+00 0.000+00 0.000+00 0.000+00 2.734+11 2.609+11 0.000+00 0.000+00 0.000+00
0.000+00 2.864−02 0.000+00 3.943−02 0.000+00 0.000+00 5.801−01 0.000+00 0.000+00 8.833−03 0.000+00 0.000+00 1.359−01 0.000+00 0.000+00 1.391−03 1.677−02 4.276−02 0.000+00 0.000+00 5.990−02 5.341−01 0.000+00 0.000+00 9.418−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.126−02 2.033−03 0.000+00 0.000+00 1.011+00 0.000+00 0.000+00 2.226−03 4.056−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.263−02 0.000+00 0.000+00 4.828−02 9.653−01 0.000+00 0.000+00 2.509−03 0.000+00 0.000+00 7.417−03 1.490−01 0.000+00 0.000+00 3.998−02 1.129−01 0.000+00 0.000+00 0.000+00 0.000+00 1.575−01 2.970−01 0.000+00 0.000+00 0.000+00
0.000+00 2.156−01 0.000+00 7.752−03 0.000+00 0.000+00 1.113−01 0.000+00 0.000+00 1.178−03 0.000+00 0.000+00 1.796−02 0.000+00 0.000+00 4.297−02 3.888−01 1.704−02 0.000+00 0.000+00 2.328−02 2.073−01 0.000+00 0.000+00 2.535−03 0.000+00 0.000+00 3.664−03 3.288−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.484−03 8.045−04 0.000+00 0.000+00 3.973−01 0.000+00 0.000+00 6.014−04 1.093−04 0.000+00 0.000+00 4.212−02 0.000+00 0.000+00 0.000+00 0.000+00 7.527−03 0.000+00 0.000+00 2.857−02 5.708−01 0.000+00 0.000+00 1.018−03 0.000+00 0.000+00 3.000−03 6.024−02 0.000+00 0.000+00 5.605−01 1.129+00 0.000+00 0.000+00 0.000+00 0.000+00 6.427−02 1.205−01 0.000+00 0.000+00 0.000+00
3.192−01 0.000+00 0.000+00 0.000+00 0.000+00 3.219+08 0.000+00 0.000+00 1.210+09 0.000+00 0.000+00 1.836+08 0.000+00 0.000+00 1.413+07 0.000+00 0.000+00 0.000+00 6.402+08 3.183+08 0.000+00 0.000+00 3.313+08 1.497+09 0.000+00 3.541+08 1.784+08 0.000+00 0.000+00 2.639+06 1.280+07 0.000+00 1.454−04 1.116+08 0.000+00 0.000+00 2.042+08 5.832+07 0.000+00 0.000+00 6.785+07 0.000+00 0.000+00 9.808+07 2.816+07 0.000+00 0.000+00 2.551+09 1.676+08 0.000+00 0.000+00 8.708+07 2.321+08 0.000+00 0.000+00 1.017+08 0.000+00 0.000+00 4.161+07 1.115+08 0.000+00 0.000+00 2.830+08 2.826+09 0.000+00 0.000+00 6.587+01 9.349+01 0.000+00 0.000+00 0.000+00 0.000+00 1.454+08 1.456+08 0.000+00
8.078+02 0.000+00 0.000+00 0.000+00 6.770+02 2.101+04 0.000+00 0.000+00 0.000+00 0.000+00 8.118+02 1.471+04 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.724+04 4.737+03 0.000+00 0.000+00 1.475+02 0.000+00 0.000+00 4.421+04 5.671+03 0.000+00 0.000+00 7.079+01 0.000+00 0.000+00 3.051+01 7.352−01 0.000+00 0.000+00 1.769+03 1.379+03 0.000+00 0.000+00 4.354−01 0.000+00 0.000+00 1.824+03 8.227+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.214+03 5.823+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.890+03 6.006+03 0.000+00 0.000+00 1.326+02 0.000+00 0.000+00 0.000+00 3.409−04 0.000+00 0.000+00 8.035+01 0.000+00 0.000+00 8.190−01 0.000+00 0.000+00
0.000+00 2.458−04 3.731−03 0.000+00 0.000+00 0.000+00 1.183+04 8.405+04 0.000+00 0.000+00 0.000+00 0.000+00 1.226+04 8.738+04 0.000+00 0.000+00 1.108−03 7.520+04 0.000+00 0.000+00 0.000+00 4.505+05 0.000+00 0.000+00 7.973+04 0.000+00 0.000+00 0.000+00 4.662+05 0.000+00 0.000+00 1.050−01 0.000+00 0.000+00 7.974+02 0.000+00 0.000+00 0.000+00 1.488+05 1.912+05 0.000+00 7.438+02 0.000+00 0.000+00 0.000+00 1.048+05 1.350+05 0.000+00 0.000+00 8.645+03 2.185+04 0.000+00 0.000+00 0.000+00 1.299+06 0.000+00 8.072+03 2.029+04 0.000+00 0.000+00 0.000+00 9.147+05 0.000+00 0.000+00 0.000+00 7.813−03 0.000+00 0.000+00 7.362−11 0.000+00 0.000+00 7.590+03 0.000+00 0.000+00 4.815−04 (continued on next page)
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 15 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
5.297+03 2.733+03 2.350+03 2.298+03 6.483+01 6.384+01 6.345+01 6.309+01 6.297+01 6.295+01 5.647+03 4.223+03 4.059+03 3.621+03 6.563+01 6.462+01 6.422+01 6.385+01 6.373+01 6.371+01 6.365+01 6.365+01 1.675+04 1.443+04 1.009+04 6.640+01 6.537+01 6.496+01 6.458+01 6.446+01 6.443+01 6.437+01 6.437+01 1.043+05 2.539+04 6.667+01 6.563+01 6.521+01 6.483+01 6.471+01 6.468+01 6.462+01 6.462+01 6.458+01 3.356+04 6.671+01 6.567+01 6.525+01 6.487+01 6.475+01 6.472+01 6.466+01 6.466+01 6.462+01 6.538+01 6.500+01 6.487+01 6.485+01 6.478+01 6.478+01 6.475+01 4.209+03 2.993+03 2.358+03 2.200+03 2.174+03 1.036+04 5.362+03 4.607+03 4.495+03 1.111+04 8.295+03 7.940+03 7.082+03 7.076+03
0.000+00 2.281+07 0.000+00 0.000+00 1.017+11 0.000+00 0.000+00 4.718+11 0.000+00 0.000+00 5.161+05 7.432+06 0.000+00 0.000+00 2.142+11 0.000+00 0.000+00 9.594+10 5.707+11 0.000+00 0.000+00 0.000+00 0.000+00 1.085+05 0.000+00 0.000+00 8.722+10 8.039+09 0.000+00 0.000+00 9.442+11 0.000+00 0.000+00 2.049+01 2.136+04 0.000+00 0.000+00 7.408+10 0.000+00 0.000+00 6.742+10 1.010+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.059+10 9.484+08 0.000+00 0.000+00 1.606+12 0.000+00 0.000+00 0.000+00 1.926+10 0.000+00 0.000+00 5.930+10 1.662+12 1.913+07 5.349+07 0.000+00 0.000+00 0.000+00 0.000+00 8.260+06 0.000+00 0.000+00 1.853+05 2.681+06 0.000+00 0.000+00 0.000+00
0.000+00 5.110−02 0.000+00 0.000+00 6.410−02 0.000+00 0.000+00 5.631−01 0.000+00 0.000+00 2.467−03 2.981−02 0.000+00 0.000+00 6.915−02 0.000+00 0.000+00 5.864−02 5.212−01 0.000+00 0.000+00 0.000+00 0.000+00 5.083−03 0.000+00 0.000+00 2.794−02 5.086−03 0.000+00 0.000+00 8.815−01 0.000+00 0.000+00 3.341−05 2.753−03 0.000+00 0.000+00 3.149−02 0.000+00 0.000+00 4.229−02 8.431−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.662−03 5.960−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.114−03 0.000+00 0.000+00 3.731−02 1.306+00 5.080−02 1.437−01 0.000+00 0.000+00 0.000+00 0.000+00 7.121−02 0.000+00 0.000+00 3.430−03 4.148−02 0.000+00 0.000+00 0.000+00
0.000+00 9.196−01 0.000+00 0.000+00 2.736−02 0.000+00 0.000+00 2.339−01 0.000+00 0.000+00 1.834−01 1.658+00 0.000+00 0.000+00 5.976−02 0.000+00 0.000+00 4.931−02 4.374−01 0.000+00 0.000+00 0.000+00 0.000+00 9.660−01 0.000+00 0.000+00 2.405−02 4.351−03 0.000+00 0.000+00 7.480−01 0.000+00 0.000+00 6.884−02 1.381+00 0.000+00 0.000+00 4.056−02 0.000+00 0.000+00 5.403−02 1.076+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.110−02 7.623−04 0.000+00 0.000+00 1.714+00 0.000+00 0.000+00 0.000+00 1.557−02 0.000+00 0.000+00 6.366−02 2.227+00 1.408+00 2.832+00 0.000+00 0.000+00 0.000+00 0.000+00 2.514+00 0.000+00 0.000+00 5.019−01 4.531+00 0.000+00 0.000+00 0.000+00
4.757−02 0.000+00 0.000+00 1.204+00 0.000+00 0.000+00 5.709+07 0.000+00 0.000+00 1.920+08 0.000+00 0.000+00 1.995−02 1.595−01 0.000+00 1.137+08 5.659+07 0.000+00 0.000+00 5.312+07 2.397+08 0.000+00 3.121−05 0.000+00 0.000+00 3.447+07 0.000+00 0.000+00 4.569+07 1.304+07 0.000+00 0.000+00 2.242+08 0.000+00 0.000+00 5.174+07 0.000+00 0.000+00 1.951+07 5.200+07 0.000+00 0.000+00 2.457+07 2.464+08 2.477−07 0.000+00 1.230+07 1.710+06 0.000+00 0.000+00 3.203+07 4.006+06 0.000+00 0.000+00 1.029+07 0.000+00 0.000+00 5.326+06 3.330+07 0.000+00 0.000+00 0.000+00 0.000+00 1.521+01 2.162+01 0.000+00 1.045−02 0.000+00 0.000+00 4.100−01 0.000+00 0.000+00 6.799−03 5.436−02 0.000+00
6.040+01 0.000+00 0.000+00 0.000+00 0.000+00 2.538+01 2.282+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.242−06 0.000+00 0.000+00 5.474+03 1.783+02 0.000+00 0.000+00 3.683+00 0.000+00 0.000+00 2.294+00 0.000+00 0.000+00 7.994−02 0.000+00 0.000+00 8.466+01 2.023+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.405+02 2.792+02 0.000+00 0.000+00 5.159+00 0.000+00 3.055−01 0.000+00 0.000+00 4.355−03 0.000+00 0.000+00 1.228+02 2.885+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.142+02 2.886+02 0.000+00 0.000+00 0.000+00 0.000+00 2.544−05 0.000+00 0.000+00 8.073+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.737−07 0.000+00 0.000+00
0.000+00 1.345−05 2.048−04 0.000+00 0.000+00 0.000+00 0.000+00 5.227+02 3.702+03 0.000+00 0.000+00 5.959−05 0.000+00 0.000+00 5.495+03 0.000+00 0.000+00 0.000+00 2.011+04 0.000+00 0.000+00 6.443−04 0.000+00 1.368−08 1.051−07 0.000+00 9.027+01 0.000+00 0.000+00 0.000+00 5.971+03 7.650+03 0.000+00 0.000+00 7.166−09 0.000+00 9.771+02 2.497+03 0.000+00 0.000+00 0.000+00 5.231+04 0.000+00 0.000+00 0.000+00 3.701−07 0.000+00 0.000+00 1.289+02 0.000+00 0.000+00 0.000+00 2.562+04 1.342+04 0.000+00 2.225+02 9.926+02 0.000+00 0.000+00 0.000+00 1.237+05 0.000+00 6.589−04 0.000+00 0.000+00 4.730−12 0.000+00 1.267−06 1.932−05 0.000+00 0.000+00 5.573−06 0.000+00 0.000+00 4.189−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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49
Table 15 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
3.272+04 2.781+04 1.952+04 1.948+04 1.853+05 4.841+04 4.817+04 3.344+04 6.552+04 6.509+04 4.080+04 9.876+06 1.082+05 1.094+05
0.000+00 5.418+04 0.000+00 0.000+00 1.306+01 1.101+04 0.000+00 0.000+00 0.000+00 2.548+03 0.000+00 2.697−05 5.760+02 0.000+00
0.000+00 9.423−03 0.000+00 0.000+00 6.722−05 5.157−03 0.000+00 0.000+00 0.000+00 2.158−03 0.000+00 3.944−07 1.263−03 0.000+00
0.000+00 3.451+00 0.000+00 0.000+00 2.460−01 4.931+00 0.000+00 0.000+00 0.000+00 2.774+00 0.000+00 1.026−01 3.597+00 0.000+00
7.886−06 0.000+00 0.000+00 1.476−04 0.000+00 0.000+00 1.771−07 1.101−05 8.536−08 0.000+00 0.000+00 0.000+00 0.000+00 2.152−09
3.078−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.229−10 0.000+00 4.106−02 0.000+00 0.000+00 0.000+00 0.000+00 9.161−03
0.000+00 1.840−09 1.384−08 0.000+00 0.000+00 1.016−09 0.000+00 0.000+00 0.000+00 4.012−11 2.170−10 0.000+00 1.537−11 0.000+00
50
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 16 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Ni XXVI. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.334+02 1.651+02 9.204+00 9.104+00 9.061+00 9.025+00 9.011+00 6.845+00 6.822+00 6.812+00 6.803+00 6.800+00 6.799+00 6.124+00 6.115+00 6.111+00 6.107+00 6.106+00 6.106+00 5.641+02 9.582+00 9.474+00 9.427+00 9.388+00 9.373+00 7.052+00 7.027+00 7.016+00 7.007+00 7.004+00 7.003+00 6.289+00 6.279+00 6.275+00 6.271+00 6.270+00 6.270+00 9.748+00 9.636+00 9.587+00 9.547+00 9.532+00 7.141+00 7.116+00 7.105+00 7.095+00 7.092+00 7.091+00 7.090+00 6.360+00 6.350+00 6.345+00 6.342+00 6.340+00 6.340+00 6.339+00 6.339+00 8.402+02 5.831+02 4.632+02 4.302+02 2.670+01 2.636+01 2.620+01 2.608+01 2.603+01 2.602+01 1.830+01 1.822+01 1.818+01 1.815+01 1.814+01 1.814+01
2.012+09 5.789+09 0.000+00 1.037+13 9.972+12 0.000+00 0.000+00 0.000+00 4.550+12 4.430+12 0.000+00 0.000+00 0.000+00 0.000+00 2.346+12 2.295+12 0.000+00 0.000+00 0.000+00 0.000+00 1.222+12 0.000+00 0.000+00 2.538+13 0.000+00 4.916+11 0.000+00 0.000+00 8.280+12 0.000+00 0.000+00 2.477+11 0.000+00 0.000+00 3.821+12 0.000+00 0.000+00 2.602+12 0.000+00 0.000+00 4.987+12 2.994+13 1.039+12 0.000+00 0.000+00 1.604+12 9.691+12 0.000+00 0.000+00 5.177+11 0.000+00 0.000+00 7.355+11 4.454+12 0.000+00 0.000+00 0.000+00 2.630+08 7.957+08 0.000+00 0.000+00 0.000+00 1.363+12 1.301+12 0.000+00 0.000+00 0.000+00 0.000+00 7.448+11 7.193+11 0.000+00 0.000+00 0.000+00
1.643−02 4.729−02 0.000+00 1.289−01 2.455−01 0.000+00 0.000+00 0.000+00 3.174−02 6.163−02 0.000+00 0.000+00 0.000+00 0.000+00 1.315−02 2.569−02 0.000+00 0.000+00 0.000+00 0.000+00 1.681−02 0.000+00 0.000+00 6.706−01 0.000+00 3.665−03 0.000+00 0.000+00 1.219−01 0.000+00 0.000+00 1.469−03 0.000+00 0.000+00 4.505−02 0.000+00 0.000+00 1.853−02 0.000+00 0.000+00 6.814−02 6.118−01 3.970−03 0.000+00 0.000+00 1.211−02 1.096−01 0.000+00 0.000+00 1.570−03 0.000+00 0.000+00 4.435−03 4.026−02 0.000+00 0.000+00 0.000+00 2.784−02 8.112−02 0.000+00 0.000+00 0.000+00 1.420−01 2.679−01 0.000+00 0.000+00 0.000+00 0.000+00 3.706−02 7.129−02 0.000+00 0.000+00 0.000+00
2.524−02 5.140−02 0.000+00 7.724−03 1.464−02 0.000+00 0.000+00 0.000+00 1.426−03 2.764−03 0.000+00 0.000+00 0.000+00 0.000+00 5.295−04 1.034−03 0.000+00 0.000+00 0.000+00 0.000+00 1.061−03 0.000+00 0.000+00 4.145−02 0.000+00 1.702−04 0.000+00 0.000+00 5.625−03 0.000+00 0.000+00 6.082−05 0.000+00 0.000+00 1.860−03 0.000+00 0.000+00 2.379−03 0.000+00 0.000+00 8.567−03 7.678−02 3.733−04 0.000+00 0.000+00 1.131−03 1.024−02 0.000+00 0.000+00 1.315−04 0.000+00 0.000+00 3.703−04 3.362−03 0.000+00 0.000+00 0.000+00 1.540−01 3.115−01 0.000+00 0.000+00 0.000+00 2.464−02 4.622−02 0.000+00 0.000+00 0.000+00 0.000+00 4.446−03 8.534−03 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.911+10 1.921+10 0.000+00 0.000+00 0.000+00 2.531+09 2.601+09 0.000+00 0.000+00 0.000+00 0.000+00 6.388+08 6.693+08 0.000+00 7.137+00 0.000+00 0.000+00 3.841+09 0.000+00 0.000+00 0.000+00 0.000+00 1.676+09 0.000+00 0.000+00 1.483+10 0.000+00 0.000+00 9.080+08 0.000+00 0.000+00 9.925+09 0.000+00 7.594+09 3.771+09 0.000+00 0.000+00 0.000+00 3.206+09 1.618+09 0.000+00 0.000+00 4.229+09 1.895+10 0.000+00 1.665+09 8.454+08 0.000+00 0.000+00 2.830+09 1.269+10 0.000+00 0.000+00 0.000+00 4.533+02 6.611+02 0.000+00 0.000+00 0.000+00 1.324+09 1.328+09 0.000+00 0.000+00 0.000+00 0.000+00 4.414+08 4.478+08 0.000+00
0.000+00 0.000+00 3.367+05 0.000+00 0.000+00 1.886+04 0.000+00 2.844+05 0.000+00 0.000+00 1.102+04 0.000+00 0.000+00 1.860+05 0.000+00 0.000+00 6.165+03 0.000+00 0.000+00 4.985+04 0.000+00 7.933+04 5.516+05 0.000+00 0.000+00 0.000+00 6.214+04 2.819+05 0.000+00 0.000+00 0.000+00 0.000+00 4.018+04 1.558+05 0.000+00 0.000+00 0.000+00 0.000+00 2.042+06 5.482+05 0.000+00 0.000+00 0.000+00 1.191+06 4.299+05 0.000+00 0.000+00 6.332+03 0.000+00 0.000+00 6.862+05 2.733+05 0.000+00 0.000+00 5.570+03 0.000+00 0.000+00 0.000+00 0.000+00 1.131−02 0.000+00 3.431+03 0.000+00 0.000+00 8.170+01 0.000+00 0.000+00 4.280+03 0.000+00 0.000+00 1.082+02 0.000+00 0.000+00
0.000+00 2.341+01 0.000+00 0.000+00 1.342+07 0.000+00 0.000+00 0.000+00 0.000+00 1.053+07 0.000+00 0.000+00 9.293+00 0.000+00 0.000+00 6.774+06 0.000+00 0.000+00 8.336+00 0.000+00 0.000+00 0.000+00 0.000+00 1.261+06 9.044+06 0.000+00 0.000+00 0.000+00 7.358+05 5.301+06 0.000+00 0.000+00 0.000+00 0.000+00 4.235+05 3.056+06 0.000+00 3.041+06 0.000+00 0.000+00 0.000+00 4.704+07 2.263+06 0.000+00 0.000+00 0.000+00 2.742+07 0.000+00 0.000+00 1.422+06 0.000+00 0.000+00 0.000+00 1.575+07 0.000+00 0.000+00 1.183+00 0.000+00 2.581−01 0.000+00 0.000+00 0.000+00 0.000+00 2.093+05 0.000+00 0.000+00 5.041−02 0.000+00 0.000+00 2.402+05 0.000+00 0.000+00 1.372−02 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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51
Table 16 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
1.906+03 1.032+03 8.816+02 2.758+01 2.721+01 2.705+01 2.691+01 2.686+01 2.686+01 1.871+01 1.862+01 1.858+01 1.855+01 1.854+01 1.854+01 2.252+03 1.640+03 2.798+01 2.760+01 2.744+01 2.730+01 2.725+01 2.724+01 2.721+01 1.889+01 1.881+01 1.877+01 1.873+01 1.872+01 1.872+01 1.871+01 1.871+01 6.038+03 2.834+01 2.795+01 2.778+01 2.764+01 2.758+01 2.757+01 2.755+01 1.905+01 1.896+01 1.892+01 1.889+01 1.888+01 1.888+01 1.887+01 1.887+01 2.847+01 2.808+01 2.791+01 2.776+01 2.771+01 2.770+01 2.767+01 1.911+01 1.902+01 1.898+01 1.895+01 1.894+01 1.893+01 1.893+01 1.893+01 1.892+01 2.041+03 1.406+03 1.117+03 1.036+03 1.025+03 5.817+01 5.734+01 5.697+01 5.667+01 5.655+01 5.653+01
0.000+00 9.175+07 0.000+00 3.434+11 0.000+00 0.000+00 2.667+12 0.000+00 0.000+00 1.674+11 0.000+00 0.000+00 1.316+12 0.000+00 0.000+00 1.760+06 2.749+07 7.283+11 0.000+00 0.000+00 5.366+11 3.200+12 0.000+00 0.000+00 3.520+11 0.000+00 0.000+00 2.611+11 1.565+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.933+11 1.751+10 0.000+00 0.000+00 5.912+12 0.000+00 0.000+00 8.294+10 7.530+09 0.000+00 0.000+00 1.955+12 0.000+00 0.000+00 0.000+00 0.000+00 1.621+11 0.000+00 0.000+00 4.196+11 6.304+12 0.000+00 0.000+00 6.962+10 0.000+00 0.000+00 1.379+11 2.080+12 0.000+00 0.000+00 6.171+07 1.900+08 0.000+00 0.000+00 0.000+00 0.000+00 3.211+11 3.053+11 0.000+00 0.000+00 0.000+00
0.000+00 2.932−02 0.000+00 3.915−02 0.000+00 0.000+00 5.792−01 0.000+00 0.000+00 8.785−03 0.000+00 0.000+00 1.358−01 0.000+00 0.000+00 1.338−03 1.663−02 4.275−02 0.000+00 0.000+00 5.996−02 5.343−01 0.000+00 0.000+00 9.419−03 0.000+00 0.000+00 1.374−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.132−02 2.025−03 0.000+00 0.000+00 1.011+00 0.000+00 0.000+00 2.236−03 4.042−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.261−02 0.000+00 0.000+00 4.827−02 9.650−01 0.000+00 0.000+00 2.507−03 0.000+00 0.000+00 7.413−03 1.489−01 0.000+00 0.000+00 3.853−02 1.127−01 0.000+00 0.000+00 0.000+00 0.000+00 1.583−01 2.971−01 0.000+00 0.000+00 0.000+00
0.000+00 1.993−01 0.000+00 7.110−03 0.000+00 0.000+00 1.027−01 0.000+00 0.000+00 1.082−03 0.000+00 0.000+00 1.658−02 0.000+00 0.000+00 3.969−02 3.593−01 1.575−02 0.000+00 0.000+00 2.156−02 1.917−01 0.000+00 0.000+00 2.343−03 0.000+00 0.000+00 3.388−03 3.040−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.165−03 7.408−04 0.000+00 0.000+00 3.670−01 0.000+00 0.000+00 5.584−04 1.007−04 0.000+00 0.000+00 3.893−02 0.000+00 0.000+00 0.000+00 0.000+00 6.953−03 0.000+00 0.000+00 2.641−02 5.275−01 0.000+00 0.000+00 9.402−04 0.000+00 0.000+00 2.773−03 5.568−02 0.000+00 0.000+00 5.178−01 1.044+00 0.000+00 0.000+00 0.000+00 0.000+00 5.975−02 1.114−01 0.000+00 0.000+00 0.000+00
5.993−01 0.000+00 0.000+00 0.000+00 0.000+00 4.075+08 0.000+00 0.000+00 1.536+09 0.000+00 0.000+00 2.328+08 0.000+00 0.000+00 1.829+07 0.000+00 0.000+00 0.000+00 8.103+08 4.027+08 0.000+00 0.000+00 4.189+08 1.893+09 0.000+00 4.476+08 2.256+08 0.000+00 0.000+00 3.304+06 1.613+07 0.000+00 2.729−04 1.411+08 0.000+00 0.000+00 2.584+08 7.381+07 0.000+00 0.000+00 8.582+07 0.000+00 0.000+00 1.241+08 3.565+07 0.000+00 0.000+00 3.227+09 2.120+08 0.000+00 0.000+00 1.102+08 2.937+08 0.000+00 0.000+00 1.287+08 0.000+00 0.000+00 5.260+07 1.410+08 0.000+00 0.000+00 3.581+08 3.575+09 0.000+00 0.000+00 7.950+01 1.164+02 0.000+00 0.000+00 0.000+00 0.000+00 1.839+08 1.842+08 0.000+00
1.296+03 0.000+00 0.000+00 0.000+00 1.004+03 3.118+04 0.000+00 0.000+00 0.000+00 0.000+00 1.204+03 2.183+04 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.477+04 7.004+03 0.000+00 0.000+00 2.183+02 0.000+00 0.000+00 6.548+04 8.385+03 0.000+00 0.000+00 1.047+02 0.000+00 0.000+00 4.892+01 1.088+00 0.000+00 0.000+00 2.622+03 2.044+03 0.000+00 0.000+00 6.436−01 0.000+00 0.000+00 2.702+03 1.220+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.724+03 8.619+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.762+03 8.890+03 0.000+00 0.000+00 1.963+02 0.000+00 0.000+00 0.000+00 4.901−04 0.000+00 0.000+00 1.189+02 0.000+00 0.000+00 1.216+00 0.000+00 0.000+00
0.000+00 3.786−04 5.982−03 0.000+00 0.000+00 0.000+00 1.621+04 1.152+05 0.000+00 0.000+00 0.000+00 0.000+00 1.681+04 1.198+05 0.000+00 0.000+00 1.460−03 1.029+05 0.000+00 0.000+00 0.000+00 6.165+05 0.000+00 0.000+00 1.091+05 0.000+00 0.000+00 0.000+00 6.378+05 0.000+00 0.000+00 1.680−01 0.000+00 0.000+00 1.096+03 0.000+00 0.000+00 0.000+00 2.038+05 2.620+05 0.000+00 1.023+03 0.000+00 0.000+00 0.000+00 1.436+05 1.850+05 0.000+00 0.000+00 1.190+04 2.990+04 0.000+00 0.000+00 0.000+00 1.778+06 0.000+00 1.112+04 2.777+04 0.000+00 0.000+00 0.000+00 1.252+06 0.000+00 0.000+00 0.000+00 1.060−02 0.000+00 0.000+00 1.158−10 0.000+00 0.000+00 1.039+04 0.000+00 0.000+00 7.707−04 (continued on next page)
52
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 16 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
4.525+03 2.466+03 2.104+03 2.060+03 5.987+01 5.900+01 5.861+01 5.829+01 5.817+01 5.815+01 5.422+03 3.932+03 3.783+03 3.342+03 6.067+01 5.978+01 5.938+01 5.905+01 5.892+01 5.890+01 5.884+01 5.884+01 1.431+04 1.251+04 8.712+03 6.136+01 6.044+01 6.003+01 5.970+01 5.957+01 5.955+01 5.949+01 5.949+01 9.974+04 2.228+04 6.163+01 6.070+01 6.029+01 5.995+01 5.982+01 5.980+01 5.974+01 5.973+01 5.970+01 2.868+04 6.166+01 6.074+01 6.032+01 5.998+01 5.985+01 5.983+01 5.977+01 5.977+01 5.973+01 6.045+01 6.011+01 5.998+01 5.996+01 5.990+01 5.990+01 5.986+01 4.035+03 2.772+03 2.200+03 2.040+03 2.016+03 8.852+03 4.838+03 4.124+03 4.030+03 1.067+04 7.722+03 7.400+03 6.536+03 6.531+03
0.000+00 2.869+07 0.000+00 0.000+00 1.185+11 0.000+00 0.000+00 5.517+11 0.000+00 0.000+00 5.386+05 8.509+06 0.000+00 0.000+00 2.505+11 0.000+00 0.000+00 1.124+11 6.679+11 0.000+00 0.000+00 0.000+00 0.000+00 1.539+05 0.000+00 0.000+00 1.025+11 9.382+09 0.000+00 0.000+00 1.105+12 0.000+00 0.000+00 2.166+01 2.925+04 0.000+00 0.000+00 8.662+10 0.000+00 0.000+00 7.888+10 1.182+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.416+10 1.110+09 0.000+00 0.000+00 1.879+12 0.000+00 0.000+00 0.000+00 2.256+10 0.000+00 0.000+00 6.937+10 1.945+12 2.006+07 6.228+07 0.000+00 0.000+00 0.000+00 0.000+00 1.039+07 0.000+00 0.000+00 1.934+05 3.071+06 0.000+00 0.000+00 0.000+00
0.000+00 5.233−02 0.000+00 0.000+00 6.368−02 0.000+00 0.000+00 5.620−01 0.000+00 0.000+00 2.374−03 2.959−02 0.000+00 0.000+00 6.914−02 0.000+00 0.000+00 5.872−02 5.214−01 0.000+00 0.000+00 0.000+00 0.000+00 5.419−03 0.000+00 0.000+00 2.806−02 5.069−03 0.000+00 0.000+00 8.809−01 0.000+00 0.000+00 3.229−05 2.901−03 0.000+00 0.000+00 3.146−02 0.000+00 0.000+00 4.229−02 8.428−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.687−03 5.960−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.127−03 0.000+00 0.000+00 3.731−02 1.306+00 4.896−02 1.434−01 0.000+00 0.000+00 0.000+00 0.000+00 7.294−02 0.000+00 0.000+00 3.301−03 4.118−02 0.000+00 0.000+00 0.000+00
0.000+00 8.498−01 0.000+00 0.000+00 2.510−02 0.000+00 0.000+00 2.157−01 0.000+00 0.000+00 1.695−01 1.532+00 0.000+00 0.000+00 5.524−02 0.000+00 0.000+00 4.566−02 4.046−01 0.000+00 0.000+00 0.000+00 0.000+00 8.930−01 0.000+00 0.000+00 2.234−02 4.007−03 0.000+00 0.000+00 6.908−01 0.000+00 0.000+00 6.363−02 1.276+00 0.000+00 0.000+00 3.747−02 0.000+00 0.000+00 4.995−02 9.944−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.029−02 7.046−04 0.000+00 0.000+00 1.584+00 0.000+00 0.000+00 0.000+00 1.442−02 0.000+00 0.000+00 5.885−02 2.058+00 1.301+00 2.618+00 0.000+00 0.000+00 0.000+00 0.000+00 2.323+00 0.000+00 0.000+00 4.638−01 4.188+00 0.000+00 0.000+00 0.000+00
8.933−02 0.000+00 0.000+00 1.776+00 0.000+00 0.000+00 7.228+07 0.000+00 0.000+00 2.435+08 0.000+00 0.000+00 2.423−02 2.034−01 0.000+00 1.440+08 7.161+07 0.000+00 0.000+00 6.720+07 3.033+08 0.000+00 5.859−05 0.000+00 0.000+00 4.362+07 0.000+00 0.000+00 5.784+07 1.651+07 0.000+00 0.000+00 2.842+08 0.000+00 0.000+00 6.547+07 0.000+00 0.000+00 2.469+07 6.580+07 0.000+00 0.000+00 3.110+07 3.120+08 4.643−07 0.000+00 1.559+07 2.163+06 0.000+00 0.000+00 4.054+07 5.069+06 0.000+00 0.000+00 1.302+07 0.000+00 0.000+00 6.738+06 4.213+07 0.000+00 0.000+00 0.000+00 0.000+00 1.837+01 2.695+01 0.000+00 1.962−02 0.000+00 0.000+00 6.048−01 0.000+00 0.000+00 8.261−03 6.936−02 0.000+00
9.691+01 0.000+00 0.000+00 0.000+00 0.000+00 3.764+01 3.386+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.237−06 0.000+00 0.000+00 8.108+03 2.638+02 0.000+00 0.000+00 5.453+00 0.000+00 0.000+00 3.679+00 0.000+00 0.000+00 1.184−01 0.000+00 0.000+00 1.254+02 3.000+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.008+02 4.134+02 0.000+00 0.000+00 7.641+00 0.000+00 4.895−01 0.000+00 0.000+00 6.441−03 0.000+00 0.000+00 1.819+02 4.274+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.691+02 4.272+02 0.000+00 0.000+00 0.000+00 0.000+00 3.660−05 0.000+00 0.000+00 1.295+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.953−07 0.000+00 0.000+00
0.000+00 2.077−05 3.291−04 0.000+00 0.000+00 0.000+00 0.000+00 7.162+02 5.070+03 0.000+00 0.000+00 7.870−05 0.000+00 0.000+00 7.522+03 0.000+00 0.000+00 0.000+00 2.753+04 0.000+00 0.000+00 1.032−03 0.000+00 2.579−08 2.026−07 0.000+00 1.241+02 0.000+00 0.000+00 0.000+00 8.179+03 1.048+04 0.000+00 0.000+00 1.274−08 0.000+00 1.344+03 3.417+03 0.000+00 0.000+00 0.000+00 7.161+04 0.000+00 0.000+00 0.000+00 5.919−07 0.000+00 0.000+00 1.769+02 0.000+00 0.000+00 0.000+00 3.508+04 1.838+04 0.000+00 3.056+02 1.360+03 0.000+00 0.000+00 0.000+00 1.693+05 0.000+00 8.948−04 0.000+00 0.000+00 7.444−12 0.000+00 1.958−06 3.106−05 0.000+00 0.000+00 7.367−06 0.000+00 0.000+00 6.763−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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53
Table 16 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
2.795+04 2.414+04 1.687+04 1.684+04 1.772+05 4.255+04 4.236+04 2.915+04 5.600+04 5.566+04 3.489+04 9.410+06 9.255+04 9.346+04
0.000+00 7.654+04 0.000+00 0.000+00 1.380+01 1.499+04 0.000+00 0.000+00 0.000+00 3.766+03 0.000+00 2.882−05 8.500+02 0.000+00
0.000+00 1.003−02 0.000+00 0.000+00 6.497−05 5.424−03 0.000+00 0.000+00 0.000+00 2.332−03 0.000+00 3.826−07 1.364−03 0.000+00
0.000+00 3.190+00 0.000+00 0.000+00 2.274−01 4.559+00 0.000+00 0.000+00 0.000+00 2.565+00 0.000+00 9.483−02 3.325+00 0.000+00
1.481−05 0.000+00 0.000+00 2.617−04 0.000+00 0.000+00 2.880−07 1.871−05 1.600−07 0.000+00 0.000+00 0.000+00 0.000+00 4.031−09
4.937−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.559−10 0.000+00 6.579−02 0.000+00 0.000+00 0.000+00 0.000+00 1.467−02
0.000+00 3.448−09 2.658−08 0.000+00 0.000+00 1.790−09 0.000+00 0.000+00 0.000+00 8.110−11 4.391−10 0.000+00 3.097−11 0.000+00
54
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 17 Collision strengths for transitions in Sc XIX. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
200
300
400
500
600
700
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.955−1 7.600−1 2.289−2 9.468−3 1.809−2 1.930−2 2.893−2 4.307−3 1.971−3 3.814−3 3.217−3 4.836−3 1.771−3 2.357−3 1.670−3 8.296−4 1.614−3 1.270−3 1.910−3 9.794−4 1.304−3 1.100−4 1.369−4
4.541−1 8.765−1 2.508−2 1.667−2 3.200−2 2.434−2 3.650−2 4.774−3 3.283−3 6.379−3 3.564−3 5.365−3 1.816−3 2.420−3 1.822−3 1.275−3 2.487−3 1.243−3 1.874−3 8.964−4 1.196−3 6.776−5 8.462−5
4.892−1 9.461−1 2.604−2 2.213−2 4.259−2 2.712−2 4.068−2 4.986−3 4.336−3 8.445−3 3.891−3 5.860−3 1.907−3 2.542−3 1.899−3 1.667−3 3.261−3 1.330−3 2.006−3 9.313−4 1.243−3 6.803−5 8.504−5
5.140−1 9.960−1 2.660−2 2.647−2 5.100−2 2.883−2 4.324−2 5.117−3 5.172−3 1.009−2 4.113−3 6.196−3 1.959−3 2.612−3 1.946−3 1.981−3 3.880−3 1.398−3 2.109−3 9.556−4 1.275−3 7.027−5 8.786−5
5.332−1 1.035+0 2.701−2 3.008−2 5.799−2 2.999−2 4.498−2 5.210−3 5.864−3 1.145−2 4.269−3 6.431−3 1.993−3 2.657−3 1.981−3 2.241−3 4.393−3 1.448−3 2.185−3 9.726−4 1.298−3 7.238−5 9.050−5
5.488−1 1.066+0 2.732−2 3.318−2 6.397−2 3.084−2 4.624−2 5.280−3 6.458−3 1.261−2 4.384−3 6.605−3 2.019−3 2.692−3 2.007−3 2.463−3 4.832−3 1.485−3 2.241−3 9.857−4 1.316−3 7.417−5 9.274−5
5.618−1 1.092+0 2.758−2 3.592−2 6.924−2 3.147−2 4.723−2 5.340−3 6.979−3 1.363−2 4.475−3 6.743−3 2.039−3 2.720−3 2.029−3 2.658−3 5.215−3 1.516−3 2.288−3 9.965−4 1.330−3 7.567−5 9.464−5
5.588−1 1.091+0 2.780−2 3.697−2 7.132−2 3.167−2 4.742−2 5.567−3 7.368−3 1.436−2 4.463−3 6.712−3 2.090−3 2.780−3 2.173−3 2.838−3 5.539−3 1.500−3 2.259−3 1.031−3 1.373−3 7.533−5 9.394−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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55
Table 18 Collision strengths for transitions in Ti XX. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
200
300
400
500
600
700
800
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.546−1 6.781−1 2.042−2 7.955−3 1.512−2 1.692−2 2.535−2 3.839−3 1.680−3 3.239−3 2.901−3 4.361−3 1.642−3 2.184−3 1.501−3 7.271−4 1.410−3 1.181−3 1.775−3 9.378−4 1.248−3 1.177−4 1.465−4
4.073−1 7.822−1 2.252−2 1.414−2 2.702−2 2.142−2 3.212−2 4.278−3 2.779−3 5.381−3 3.151−3 4.745−3 1.628−3 2.170−3 1.634−3 1.080−3 2.102−3 1.107−3 1.669−3 8.079−4 1.077−3 6.256−5 7.808−5
4.389−1 8.447−1 2.345−2 1.895−2 3.630−2 2.402−2 3.603−2 4.485−3 3.701−3 7.186−3 3.443−3 5.186−3 1.714−3 2.286−3 1.708−3 1.422−3 2.774−3 1.179−3 1.778−3 8.373−4 1.117−3 6.140−5 7.673−5
4.618−1 8.903−1 2.399−2 2.280−2 4.374−2 2.566−2 3.848−2 4.610−3 4.442−3 8.639−3 3.651−3 5.502−3 1.766−3 2.355−3 1.753−3 1.700−3 3.322−3 1.241−3 1.872−3 8.608−4 1.149−3 6.317−5 7.898−5
4.793−1 9.255−1 2.439−2 2.602−2 4.996−2 2.678−2 4.017−2 4.698−3 5.060−3 9.849−3 3.800−3 5.727−3 1.800−3 2.401−3 1.787−3 1.932−3 3.778−3 1.288−3 1.944−3 8.775−4 1.171−3 6.505−5 8.134−5
4.934−1 9.541−1 2.468−2 2.879−2 5.530−2 2.761−2 4.140−2 4.765−3 5.590−3 1.089−2 3.911−3 5.895−3 1.826−3 2.434−3 1.812−3 2.131−3 4.170−3 1.324−3 1.999−3 8.901−4 1.188−3 6.671−5 8.343−5
5.053−1 9.781−1 2.493−2 3.124−2 6.001−2 2.823−2 4.237−2 4.821−3 6.056−3 1.180−2 3.999−3 6.028−3 1.846−3 2.462−3 1.832−3 2.305−3 4.514−3 1.353−3 2.043−3 9.006−4 1.202−3 6.813−5 8.521−5
5.156−1 9.990−1 2.515−2 3.344−2 6.422−2 2.876−2 4.312−2 4.871−3 6.474−3 1.262−2 4.071−3 6.137−3 1.864−3 2.485−3 1.851−3 2.461−3 4.821−3 1.377−3 2.079−3 9.098−4 1.214−3 6.936−5 8.674−5
4.775−1 9.272−1 2.482−2 2.805−2 5.383−2 2.732−2 4.089−2 4.945−3 5.623−3 1.091−2 3.840−3 5.777−3 1.859−3 2.472−3 1.921−3 2.171−3 4.222−3 1.288−3 1.940−3 9.105−4 1.212−3 6.764−5 8.434−5
56
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 19 Collision strengths for transitions in V XXI. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
300
500
700
900
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.133−1 5.971−1 1.836−2 6.738−3 1.273−2 1.492−2 2.235−2 3.453−3 1.453−3 2.791−3 2.641−3 3.970−3 1.541−3 2.049−3 1.363−3 6.565−4 1.270−3 1.102−3 1.657−3 9.107−4 1.212−3 1.300−4 1.618−4
3.959−1 7.577−1 2.121−2 1.630−2 3.108−2 2.136−2 3.203−2 4.052−3 3.176−3 6.144−3 3.062−3 4.614−3 1.547−3 2.062−3 1.543−3 1.220−3 2.372−3 1.050−3 1.585−3 7.559−4 1.009−3 5.579−5 6.970−5
4.327−1 8.315−1 2.211−2 2.261−2 4.323−2 2.400−2 3.600−2 4.256−3 4.386−3 8.513−3 3.397−3 5.122−3 1.632−3 2.176−3 1.618−3 1.674−3 3.265−3 1.151−3 1.737−3 7.947−4 1.061−3 5.870−5 7.340−5
4.567−1 8.798−1 2.263−2 2.730−2 5.224−2 2.543−2 3.812−2 4.374−3 5.281−3 1.026−2 3.589−3 5.412−3 1.677−3 2.236−3 1.662−3 2.009−3 3.924−3 1.213−3 1.832−3 8.171−4 1.091−3 6.156−5 7.698−5
4.745−1 9.158−1 2.302−2 3.108−2 5.947−2 2.634−2 3.953−2 4.459−3 5.998−3 1.166−2 3.718−3 5.606−3 1.709−3 2.279−3 1.695−3 2.277−3 4.452−3 1.256−3 1.897−3 8.337−4 1.113−3 6.374−5 7.973−5
4.395−1 8.496−1 2.260−2 2.583−2 4.937−2 2.496−2 3.735−2 4.496−3 5.160−3 9.985−3 3.498−3 5.263−3 1.700−3 2.261−3 1.745−3 1.989−3 3.859−3 1.172−3 1.766−3 8.324−4 1.108−3 6.206−5 7.737−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 20 Collision strengths for transitions in Cr XXII. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.325−1 6.312−1 1.841−2 1.035−2 1.955−2 1.682−2 2.522−2 3.488−3 2.028−3 3.895−3 2.515−3 3.788−3 1.330−3 1.772−3 1.332−3 7.926−4 1.531−3 9.008−4 1.358−3 6.706−4 8.939−4 5.566−5 6.936−5
3.777−1 7.201−1 1.978−2 1.715−2 3.260−2 2.055−2 3.081−2 3.790−3 3.325−3 6.422−3 2.914−3 4.395−3 1.451−3 1.934−3 1.442−3 1.271−3 2.469−3 9.915−4 1.498−3 7.063−4 9.427−4 5.181−5 6.476−5
4.045−1 7.739−1 2.041−2 2.197−2 4.185−2 2.236−2 3.354−2 3.933−3 4.247−3 8.224−3 3.151−3 4.754−3 1.509−3 2.012−3 1.494−3 1.617−3 3.148−3 1.065−3 1.610−3 7.343−4 9.802−4 5.456−5 6.823−5
4.233−1 8.119−1 2.083−2 2.575−2 4.907−2 2.346−2 3.519−2 4.029−3 4.964−3 9.624−3 3.301−3 4.981−3 1.545−3 2.061−3 1.531−3 1.885−3 3.676−3 1.114−3 1.684−3 7.524−4 1.005−3 5.689−5 7.116−5
4.377−1 8.412−1 2.117−2 2.888−2 5.504−2 2.421−2 3.634−2 4.102−3 5.557−3 1.078−2 3.407−3 5.141−3 1.573−3 2.098−3 1.559−3 2.107−3 4.110−3 1.150−3 1.738−3 7.666−4 1.024−3 5.874−5 7.348−5
4.052−1 7.798−1 2.065−2 2.391−2 4.553−2 2.290−2 3.427−2 4.096−3 4.756−3 9.176−3 3.200−3 4.817−3 1.561−3 2.075−3 1.596−3 1.830−3 3.541−3 1.071−3 1.615−3 7.640−4 1.017−3 5.715−5 7.123−5
58
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 21 Collision strengths for transitions in Mn XXIII. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.015−1 5.687−1 1.675−2 8.915−3 1.675−2 1.500−2 2.248−2 3.168−3 1.748−3 3.342−3 2.269−3 3.418−3 1.213−3 1.615−3 1.212−3 6.863−4 1.321−3 8.229−4 1.241−3 6.184−4 8.239−4 5.375−5 6.692−5
3.437−1 6.512−1 1.806−2 1.497−2 2.830−2 1.848−2 2.771−2 3.456−3 2.895−3 5.570−3 2.620−3 3.953−3 1.320−3 1.760−3 1.315−3 1.106−3 2.141−3 8.926−4 1.349−3 6.430−4 8.582−4 4.728−5 5.907−5
3.684−1 7.008−1 1.867−2 1.931−2 3.661−2 2.022−2 3.033−2 3.595−3 3.726−3 7.190−3 2.845−3 4.294−3 1.378−3 1.838−3 1.366−3 1.418−3 2.752−3 9.615−4 1.454−3 6.701−4 8.948−4 4.961−5 6.203−5
3.858−1 7.359−1 1.906−2 2.273−2 4.313−2 2.128−2 3.193−2 3.683−3 4.374−3 8.454−3 2.989−3 4.512−3 1.413−3 1.885−3 1.400−3 1.660−3 3.229−3 1.008−3 1.525−3 6.876−4 9.181−4 5.176−5 6.474−5
3.993−1 7.631−1 1.938−2 2.557−2 4.853−2 2.204−2 3.303−2 3.753−3 4.912−3 9.501−3 3.090−3 4.666−3 1.440−3 1.920−3 1.426−3 1.861−3 3.623−3 1.042−3 1.577−3 7.012−4 9.362−4 5.352−5 6.694−5
3.759−1 7.194−1 1.893−2 2.219−2 4.207−2 2.109−2 3.155−2 3.760−3 4.398−3 8.460−3 2.940−3 4.427−3 1.439−3 1.912−3 1.462−3 1.691−3 3.262−3 9.832−4 1.483−3 7.040−4 9.365−4 5.281−5 6.580−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 22 Collision strengths for transitions in Fe XXIV. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.753−1 5.151−1 1.528−2 7.714−3 1.440−2 1.344−2 2.013−2 2.886−3 1.516−3 2.884−3 2.061−3 3.105−3 1.113−3 1.481−3 1.105−3 5.983−4 1.147−3 7.583−4 1.144−3 5.753−4 7.661−4 5.276−5 6.563−5
3.143−1 5.916−1 1.654−2 1.311−2 2.465−2 1.666−2 2.498−2 3.164−3 2.530−3 4.849−3 2.364−3 3.569−3 1.205−3 1.606−3 1.204−3 9.663−4 1.864−3 8.070−4 1.220−3 5.871−4 7.837−4 4.335−5 5.416−5
3.371−1 6.372−1 1.713−2 1.704−2 3.214−2 1.834−2 2.750−2 3.296−3 3.280−3 6.307−3 2.577−3 3.891−3 1.262−3 1.683−3 1.252−3 1.247−3 2.414−3 8.705−4 1.317−3 6.133−4 8.189−4 4.525−5 5.658−5
3.531−1 6.696−1 1.751−2 2.014−2 3.803−2 1.937−2 2.906−2 3.382−3 3.869−3 7.453−3 2.714−3 4.100−3 1.297−3 1.729−3 1.284−3 1.468−3 2.846−3 9.151−4 1.385−3 6.304−4 8.418−4 4.723−5 5.907−5
3.655−1 6.948−1 1.781−2 2.272−2 4.294−2 2.009−2 3.014−2 3.449−3 4.358−3 8.404−3 2.814−3 4.250−3 1.322−3 1.763−3 1.310−3 1.651−3 3.204−3 9.478−4 1.435−3 6.434−4 8.592−4 4.888−5 6.114−5
3.496−1 6.656−1 1.743−2 2.065−2 3.896−2 1.950−2 2.916−2 3.464−3 4.078−3 7.818−3 2.711−3 4.083−3 1.331−3 1.768−3 1.345−3 1.568−3 3.017−3 9.063−4 1.368−3 6.514−4 8.664−4 4.899−5 6.103−5
60
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 23 Collision strengths for transitions in Co XXV. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
1200
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.525−1 4.696−1 1.399−2 6.707−3 1.243−2 1.208−2 1.810−2 2.639−3 1.322−3 2.502−3 1.883−3 2.838−3 1.028−3 1.368−3 1.012−3 5.256−4 1.003−3 7.042−4 1.062−3 5.398−4 7.185−4 5.263−5 6.539−5
2.876−1 5.377−1 1.520−2 1.152−2 2.154−2 1.507−2 2.259−2 2.904−3 2.219−3 4.235−3 2.142−3 3.234−3 1.102−3 1.469−3 1.105−3 8.474−4 1.629−3 7.328−4 1.109−3 5.378−4 7.178−4 3.997−5 4.991−5
3.088−1 5.800−1 1.577−2 1.508−2 2.829−2 1.667−2 2.500−2 3.031−3 2.898−3 5.550−3 2.340−3 3.535−3 1.159−3 1.545−3 1.151−3 1.101−3 2.124−3 7.909−4 1.197−3 5.627−4 7.514−4 4.142−5 5.179−5
3.238−1 6.102−1 1.614−2 1.790−2 3.364−2 1.768−2 2.651−2 3.114−3 3.434−3 6.591−3 2.473−3 3.738−3 1.193−3 1.590−3 1.183−3 1.302−3 2.517−3 8.336−4 1.263−3 5.794−4 7.738−4 4.321−5 5.405−5
3.354−1 6.335−1 1.642−2 2.026−2 3.810−2 1.838−2 2.756−2 3.176−3 3.880−3 7.457−3 2.569−3 3.884−3 1.217−3 1.623−3 1.207−3 1.469−3 2.844−3 8.650−4 1.310−3 5.919−4 7.906−4 4.476−5 5.599−5
3.448−1 6.527−1 1.667−2 2.231−2 4.196−2 1.892−2 2.838−2 3.231−3 4.266−3 8.204−3 2.644−3 3.996−3 1.238−3 1.651−3 1.227−3 1.613−3 3.125−3 8.897−4 1.348−3 6.024−4 8.046−4 4.606−5 5.763−5
3.268−1 6.378−1 1.611−2 1.928−2 3.620−2 1.806−2 2.701−2 3.205−3 3.797−3 7.254−3 2.507−3 3.778−3 1.237−3 1.642−3 1.241−3 1.457−3 2.795−3 8.378−4 1.265−3 6.042−4 8.035−4 4.558−5 5.676−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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61
Table 24 Collision strengths for transitions in Ni XXVI. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
1200
1400
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.314−1 4.266−1 1.286−2 5.855−3 1.077−2 1.090−2 1.633−2 2.426−3 1.160−3 2.184−3 1.732−3 2.609−3 9.564−4 1.272−3 9.321−4 4.657−4 8.849−4 6.597−4 9.947−4 5.117−4 6.807−4 5.333−5 6.617−5
2.643−1 4.908−1 1.402−2 1.016−2 1.888−2 1.366−2 2.048−2 2.676−3 1.953−3 3.711−3 1.947−3 2.941−3 1.011−3 1.347−3 1.017−3 7.459−4 1.428−3 6.683−4 1.011−3 4.941−4 6.593−4 3.706−5 4.626−5
2.841−1 5.299−1 1.456−2 1.339−2 2.498−2 1.520−2 2.278−2 2.795−3 2.568−3 4.899−3 2.132−3 3.222−3 1.066−3 1.421−3 1.062−3 9.756−4 1.875−3 7.211−4 1.092−3 5.176−4 6.912−4 3.804−5 4.756−5
2.982−1 5.581−1 1.491−2 1.596−2 2.984−2 1.616−2 2.424−2 2.876−3 3.057−3 5.846−3 2.259−3 3.416−3 1.099−3 1.466−3 1.092−3 1.159−3 2.233−3 7.612−4 1.154−3 5.338−4 7.130−4 3.964−5 4.958−5
3.089−1 5.799−1 1.519−2 1.812−2 3.391−2 1.685−2 2.528−2 2.936−3 3.465−3 6.636−3 2.352−3 3.557−3 1.124−3 1.499−3 1.115−3 1.311−3 2.531−3 7.918−4 1.200−3 5.460−4 7.292−4 4.108−5 5.139−5
3.178−1 5.978−1 1.542−2 1.999−2 3.743−2 1.737−2 2.606−2 2.988−3 3.818−3 7.319−3 2.424−3 3.667−3 1.143−3 1.525−3 1.135−3 1.443−3 2.788−3 8.154−4 1.236−3 5.561−4 7.428−4 4.231−5 5.294−5
3.253−1 6.130−1 1.564−2 2.166−2 4.057−2 1.781−2 2.669−2 3.033−3 4.131−3 7.925−3 2.485−3 3.759−3 1.161−3 1.548−3 1.152−3 1.560−3 3.017−3 8.361−4 1.268−3 5.651−4 7.547−4 4.338−5 5.428−5
3.059−1 5.926−1 1.496−2 1.798−2 3.358−2 1.679−2 2.510−2 2.971−3 3.545−3 6.749−3 2.328−3 3.509−3 1.150−3 1.527−3 1.152−3 1.358−3 2.597−3 7.776−4 1.175−3 5.635−4 7.497−4 4.252−5 5.294−5
62
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 25 Effective collision strengths for transitions in Sc XIX. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.573−1 5.045−1 2.305−2 6.441−3 1.223−2 1.755−2 2.625−2 4.622−3 1.624−3 3.124−3 3.188−3 4.781−3 1.882−3 2.503−3 1.805−3 6.944−4 1.337−3 1.231−3 1.847−3 9.951−4 1.323−3 1.285−4 1.603−4 4.563−2 1.639−3 2.521−2 6.600−3 8.495−2 1.216−2 5.175−4 5.239−3 2.156−3 1.558−2 3.780−3 2.623−3 1.578−3 2.450−4 2.102−3 1.036−3 5.849−3 1.766−3 1.389−3 9.530−4 1.290−4 1.268−4 3.315−3 6.743−3 5.736−2 3.222−2 1.657−1 1.032−3 2.174−3 1.266−2 7.725−3 3.146−2 2.844−3 5.749−3 4.871−4 1.042−3 5.238−3 3.313−3 1.206−2 1.654−3 3.118−3 2.178−4 3.071−4 1.684+0 3.297+0 1.225−1 1.840−1 1.082−1 1.762−2 3.317−2
2.639−1 5.138−1 2.483−2 8.036−3 1.558−2 1.886−2 2.864−2 4.934−3 2.257−3 4.457−3 3.749−3 5.664−3 2.496−3 3.336−3 1.704−3 8.260−4 1.592−3 1.322−3 1.986−3 1.061−3 1.414−3 1.408−4 1.753−4 6.651−2 7.258−3 2.562−2 1.090−2 8.571−2 1.916−2 1.601−3 5.583−3 3.405−3 1.671−2 5.192−3 4.078−3 2.969−3 4.710−4 1.915−3 1.131−3 6.140−3 1.886−3 1.559−3 9.975−4 1.519−4 1.285−4 1.633−2 1.126−2 6.389−2 4.087−2 1.736−1 3.118−3 3.470−3 1.443−2 9.782−3 3.455−2 5.191−3 9.270−3 9.377−4 1.150−3 4.975−3 3.532−3 1.270−2 1.775−3 3.468−3 2.298−4 3.483−4 1.678+0 3.282+0 1.600−1 2.437−1 1.096−1 2.140−2 4.547−2
2.759−1 5.376−1 2.431−2 8.231−3 1.596−2 1.909−2 2.896−2 4.755−3 2.182−3 4.293−3 3.623−3 5.465−3 2.322−3 3.094−3 1.693−3 8.322−4 1.610−3 1.307−3 1.963−3 1.036−3 1.381−3 1.314−4 1.636−4 7.323−2 5.885−3 2.548−2 1.024−2 8.896−2 1.808−2 1.314−3 5.337−3 2.991−3 1.693−2 4.644−3 3.800−3 2.508−3 4.207−4 1.889−3 1.062−3 6.271−3 1.764−3 1.558−3 9.214−4 1.447−4 1.161−4 1.297−2 1.051−2 6.247−2 4.016−2 1.786−1 2.577−3 3.044−3 1.357−2 9.144−3 3.453−2 4.489−3 8.462−3 8.406−4 1.077−3 4.856−3 3.409−3 1.284−2 1.674−3 3.410−3 2.103−4 3.278−4 1.784+0 3.477+0 1.564−1 2.379−1 1.086−1 2.279−2 4.731−2
2.901−1 5.653−1 2.392−2 8.541−3 1.652−2 1.925−2 2.913−2 4.631−3 2.160−3 4.233−3 3.516−3 5.298−3 2.163−3 2.879−3 1.693−3 8.531−4 1.654−3 1.289−3 1.937−3 1.008−3 1.344−3 1.208−4 1.504−4 7.505−2 4.793−3 2.517−2 9.220−3 9.332−2 1.620−2 1.085−3 5.127−3 2.598−3 1.738−2 4.069−3 3.598−3 2.071−3 3.773−4 1.865−3 9.811−4 6.468−3 1.609−3 1.573−3 8.295−4 1.380−4 1.020−4 1.039−2 9.442−3 6.053−2 3.875−2 1.850−1 2.143−3 2.642−3 1.280−2 8.516−3 3.492−2 3.837−3 7.807−3 7.563−4 9.945−4 4.730−3 3.259−3 1.308−2 1.557−3 3.371−3 1.885−4 3.069−4 1.922+0 3.734+0 1.491−1 2.264−1 1.085−1 2.561−2 5.167−2
3.072−1 5.982−1 2.372−2 9.157−3 1.766−2 1.957−2 2.954−2 4.570−3 2.221−3 4.338−3 3.450−3 5.194−3 2.038−3 2.712−3 1.705−3 8.959−4 1.740−3 1.272−3 1.913−3 9.808−4 1.307−3 1.097−4 1.366−4 7.135−2 3.973−3 2.489−2 8.117−3 9.976−2 1.402−2 9.127−4 4.973−3 2.247−3 1.818−2 3.500−3 3.521−3 1.685−3 3.398−4 1.844−3 8.921−4 6.764−3 1.427−3 1.617−3 7.272−4 1.326−4 8.709−5 8.512−3 8.318−3 5.866−2 3.743−2 1.950−1 1.815−3 2.285−3 1.218−2 7.968−3 3.594−2 3.293−3 7.406−3 6.831−4 9.040−4 4.600−3 3.096−3 1.347−2 1.434−3 3.374−3 1.660−4 2.879−4 2.094+0 4.052+0 1.408−1 2.134−1 1.093−1 3.033−2 5.978−2
3.284−1 6.387−1 2.375−2 1.027−2 1.977−2 2.021−2 3.045−2 4.569−3 2.390−3 4.658−3 3.436−3 5.171−3 1.953−3 2.599−3 1.726−3 9.704−4 1.888−3 1.262−3 1.899−3 9.578−4 1.276−3 9.929−5 1.237−4 6.384−2 3.436−3 2.473−2 7.122−3 1.093−1 1.192−2 7.915−4 4.877−3 1.946−3 1.944−2 2.959−3 3.586−3 1.361−3 3.092−4 1.828−3 7.999−4 7.198−3 1.231−3 1.701−3 6.226−4 1.297−4 7.250−5 7.301−3 7.318−3 5.724−2 3.684−2 2.108−1 1.586−3 1.981−3 1.172−2 7.550−3 3.784−2 2.874−3 7.299−3 6.237−4 8.109−4 4.478−3 2.944−3 1.410−2 1.321−3 3.446−3 1.449−4 2.731−4 2.289+0 4.419+0 1.333−1 2.017−1 1.108−1 3.732−2 7.248−2
3.542−1 6.878−1 2.401−2 1.202−2 2.312−2 2.124−2 3.194−2 4.617−3 2.689−3 5.234−3 3.477−3 5.233−3 1.906−3 2.537−3 1.756−3 1.086−3 2.117−3 1.264−3 1.903−3 9.423−4 1.256−3 9.042−5 1.127−4 5.509−2 3.176−3 2.475−2 6.325−3 1.226−1 1.009−2 7.178−4 4.829−3 1.697−3 2.125−2 2.468−3 3.793−3 1.099−3 2.877−4 1.818−3 7.114−4 7.805−3 1.036−3 1.831−3 5.247−4 1.294−4 5.935−5 6.719−3 6.527−3 5.641−2 3.736−2 2.339−1 1.450−3 1.730−3 1.139−2 7.309−3 4.077−2 2.583−3 7.484−3 5.829−4 7.220−4 4.372−3 2.829−3 1.505−2 1.229−3 3.604−3 1.267−4 2.640−4 2.499+0 4.817+0 1.273−1 1.922−1 1.126−1 4.685−2 9.022−2
3.822−1 7.411−1 2.430−2 1.436−2 2.762−2 2.245−2 3.373−2 4.672−3 3.095−3 6.026−3 3.548−3 5.340−3 1.879−3 2.503−3 1.781−3 1.237−3 2.415−3 1.271−3 1.915−3 9.303−4 1.240−3 8.327−5 1.039−4 4.692−2 3.152−3 2.478−2 5.725−3 1.391−1 8.584−3 6.838−4 4.794−3 1.494−3 2.346−2 2.042−3 4.089−3 8.955−4 2.756−4 1.806−3 6.309−4 8.527−3 8.582−4 1.989−3 4.398−4 1.308−4 4.827−5 6.662−3 5.937−3 5.584−2 3.890−2 2.630−1 1.392−3 1.527−3 1.114−2 7.229−3 4.446−2 2.396−3 7.863−3 5.611−4 6.416−4 4.269−3 2.756−3 1.622−2 1.163−3 3.821−3 1.118−4 2.589−4 2.697+0 5.199+0 1.221−1 1.842−1 1.139−1 5.824−2 1.117−1
4.004−1 7.758−1 2.397−2 1.647−2 3.170−2 2.305−2 3.461−2 4.596−3 3.442−3 6.703−3 3.532−3 5.318−3 1.818−3 2.422−3 1.751−3 1.359−3 2.655−3 1.248−3 1.880−3 8.972−4 1.197−3 7.616−5 9.505−5 3.972−2 3.206−3 2.420−2 5.194−3 1.523−1 7.299−3 6.618−4 4.643−3 1.311−3 2.503−2 1.673−3 4.282−3 7.328−4 2.647−4 1.745−3 5.527−4 9.001−3 6.987−4 2.086−3 3.658−4 1.291−4 3.900−5 6.778−3 5.411−3 5.412−2 4.003−2 2.861−1 1.357−3 1.343−3 1.066−2 7.091−3 4.702−2 2.234−3 8.090−3 5.414−4 5.632−4 4.070−3 2.657−3 1.695−2 1.094−3 3.938−3 9.848−5 2.499−4 2.792+0 5.386+0 1.152−1 1.736−1 1.116−1 6.775−2 1.296−1
4.165−1 8.099−1 2.581−2 1.844−2 3.542−2 2.446−2 3.662−2 5.123−3 3.830−3 7.429−3 3.644−3 5.476−3 1.883−3 2.504−3 1.986−3 1.508−3 2.929−3 1.268−3 1.907−3 9.353−4 1.245−3 7.776−5 9.694−5 3.012−2 3.132−3 2.640−2 5.102−3 1.666−1 6.573−3 6.377−4 5.329−3 1.311−3 2.685−2 1.547−3 4.578−3 6.701−4 2.472−4 2.099−3 5.685−4 9.510−3 6.697−4 2.285−3 3.755−4 1.363−4 4.090−5 6.574−3 5.330−3 5.838−2 4.212−2 3.111−1 1.312−3 1.342−3 1.202−2 7.304−3 5.018−2 2.228−3 8.539−3 5.062−4 5.799−4 4.777−3 2.727−3 1.784−2 1.161−3 4.276−3 1.073−4 2.810−4 2.952+0 5.725+0 1.156−1 1.740−1 1.214−1 7.670−2 1.468−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
63
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
4.487−2 6.690−2 4.562−2 6.080−2 2.040−2 4.049−3 7.739−3 9.440−3 1.412−2 5.278−3 7.049−3 8.138−3 1.016−2 2.019−1 2.467+0 3.102−2 7.211−3 1.156−1 1.630−2 1.438−1 2.087−2 1.515−1 2.210−2 1.708−3 2.255−2 4.476−3 2.990−2 5.917−3 1.603−2 5.069−3 1.947−2 6.332−3 5.652−1 4.672+0 1.488−2 1.706−2 2.488−1 5.559−2 2.838−1 7.244−2 2.785−1 3.416−3 4.600−3 4.972−2 1.334−2 5.981−2 1.110−2 3.105−2 1.517−2 3.727−2 1.455−1 6.195−3 1.161−2 1.186−2 2.227−1 2.817−2 9.829−1 4.972−2 2.008−3 3.616−3 4.547−3 4.273−2 1.029−2 1.548−1 1.651−2 4.241−2 9.552−3 9.335−3 8.043−3 2.735−2 2.827−2 3.486−1 1.241−1 1.431+0
4.625−2 7.435−2 5.405−2 7.443−2 1.894−2 4.691−3 8.964−3 9.712−3 1.454−2 6.397−3 8.547−3 8.698−3 1.087−2 2.417−1 2.491+0 1.032−1 1.758−2 1.092−1 2.294−2 1.440−1 3.056−2 1.518−1 3.519−2 2.778−3 1.950−2 4.396−3 3.197−2 6.417−3 1.717−2 5.789−3 2.011−2 6.712−3 6.446−1 4.710+0 3.687−2 2.331−2 2.504−1 6.613−2 3.037−1 8.995−2 2.956−1 5.664−3 4.551−3 4.347−2 1.438−2 6.400−2 1.238−2 3.361−2 1.592−2 3.865−2 4.077−1 1.852−2 2.561−2 2.960−2 2.310−1 5.361−2 9.753−1 8.885−2 3.175−3 5.073−3 5.692−3 4.149−2 1.126−2 1.583−1 1.773−2 4.427−2 9.620−3 2.732−2 2.030−2 6.301−2 5.282−2 3.868−1 1.661−1 1.442+0
4.744−2 7.503−2 5.235−2 7.164−2 1.911−2 5.061−3 9.691−3 9.960−3 1.492−2 6.092−3 8.139−3 8.501−3 1.063−2 2.345−1 2.628+0 9.553−2 1.509−2 1.091−1 2.121−2 1.555−1 2.762−2 1.564−1 3.091−2 2.599−3 1.971−2 4.309−3 3.406−2 6.044−3 1.732−2 5.269−3 2.060−2 6.219−3 6.649−1 4.956+0 3.185−2 2.146−2 2.474−1 6.521−2 3.204−1 8.564−2 2.989−1 5.302−3 4.454−3 4.383−2 1.434−2 6.754−2 1.174−2 3.347−2 1.542−2 3.915−2 3.747−1 1.473−2 2.222−2 2.451−2 2.273−1 4.507−2 1.023+0 7.452−2 2.750−3 4.700−3 5.098−3 4.108−2 1.012−2 1.639−1 1.571−2 4.602−2 8.527−3 2.185−2 1.654−2 5.385−2 4.443−2 3.743−1 1.540−1 1.503+0
4.947−2 7.695−2 5.090−2 6.918−2 1.939−2 5.658−3 1.085−2 1.031−2 1.546−2 5.769−3 7.707−3 8.337−3 1.042−2 2.234−1 2.831+0 8.201−2 1.390−2 1.096−1 1.990−2 1.735−1 2.495−2 1.633−1 2.703−2 2.543−3 1.999−2 4.250−3 3.710−2 5.641−3 1.757−2 4.711−3 2.125−2 5.700−3 6.961−1 5.349+0 2.941−2 2.024−2 2.455−1 6.594−2 3.489−1 8.253−2 3.067−1 5.200−3 4.392−3 4.436−2 1.447−2 7.280−2 1.109−2 3.347−2 1.493−2 3.991−2 3.182−1 1.188−2 1.968−2 2.001−2 2.244−1 3.711−2 1.095+0 6.105−2 2.405−3 4.384−3 4.502−3 4.073−2 8.887−3 1.719−1 1.351−2 4.869−2 7.391−3 1.770−2 1.325−2 4.645−2 3.666−2 3.632−1 1.446−1 1.600+0
5.250−2 8.053−2 4.986−2 6.740−2 1.977−2 6.556−3 1.260−2 1.078−2 1.617−2 5.461−3 7.295−3 8.242−3 1.030−2 2.115−1 3.095+0 6.751−2 1.398−2 1.107−1 1.922−2 1.997−1 2.281−2 1.730−1 2.390−2 2.616−3 2.032−2 4.232−3 4.138−2 5.243−3 1.796−2 4.166−3 2.203−2 5.201−3 7.411−1 5.869+0 2.957−2 1.974−2 2.456−1 6.900−2 3.938−1 8.118−2 3.199−1 5.367−3 4.375−3 4.504−2 1.485−2 8.032−2 1.048−2 3.372−2 1.453−2 4.091−2 2.573−1 9.838−3 1.815−2 1.644−2 2.229−1 3.044−2 1.200+0 4.954−2 2.126−3 4.148−3 3.940−3 4.046−2 7.653−3 1.832−1 1.132−2 5.246−2 6.313−3 1.472−2 1.060−2 4.136−2 3.016−2 3.554−1 1.397−1 1.745+0
5.640−2 8.565−2 4.926−2 6.630−2 2.019−2 7.831−3 1.508−2 1.136−2 1.704−2 5.198−3 6.944−3 8.242−3 1.030−2 2.009−1 3.397+0 5.503−2 1.527−2 1.123−1 1.917−2 2.360−1 2.122−2 1.849−1 2.160−2 2.828−3 2.068−2 4.265−3 4.717−2 4.882−3 1.847−2 3.681−3 2.289−2 4.763−3 7.963−1 6.463+0 3.230−2 1.988−2 2.477−1 7.475−2 4.580−1 8.159−2 3.381−1 5.826−3 4.413−3 4.583−2 1.559−2 9.062−2 9.998−3 3.423−2 1.422−2 4.207−2 2.035−1 8.464−3 1.766−2 1.384−2 2.228−1 2.523−2 1.342+0 4.034−2 1.909−3 4.016−3 3.450−3 4.032−2 6.522−3 1.983−1 9.322−3 5.732−2 5.378−3 1.270−2 8.586−3 3.866−2 2.509−2 3.509−1 1.399−1 1.945+0
6.088−2 9.184−2 4.902−2 6.577−2 2.063−2 9.537−3 1.840−2 1.202−2 1.803−2 5.000−3 6.680−3 8.340−3 1.042−2 1.924−1 3.715+0 4.561−2 1.772−2 1.141−1 1.962−2 2.831−1 2.012−2 1.982−1 2.007−2 3.190−3 2.105−2 4.349−3 5.465−2 4.581−3 1.909−2 3.286−3 2.373−2 4.408−3 8.569−1 7.079+0 3.753−2 2.050−2 2.511−1 8.331−2 5.433−1 8.339−2 3.593−1 6.596−3 4.504−3 4.668−2 1.675−2 1.041−1 9.657−3 3.498−2 1.403−2 4.325−2 1.613−1 7.598−3 1.817−2 1.210−2 2.237−1 2.138−2 1.526+0 3.337−2 1.751−3 4.006−3 3.060−3 4.029−2 5.567−3 2.178−1 7.630−3 6.304−2 4.635−3 1.143−2 7.113−3 3.818−2 2.135−2 3.491−1 1.457−1 2.206+0
6.509−2 9.780−2 4.877−2 6.531−2 2.093−2 1.155−2 2.232−2 1.262−2 1.893−2 4.846−3 6.474−3 8.464−3 1.058−2 1.849−1 4.007+0 3.899−2 2.103−2 1.153−1 2.026−2 3.376−1 1.929−2 2.103−1 1.905−2 3.659−3 2.127−2 4.447−3 6.319−2 4.329−3 1.962−2 2.979−3 2.432−2 4.124−3 9.133−1 7.639+0 4.458−2 2.128−2 2.537−1 9.373−2 6.427−1 8.551−2 3.790−1 7.592−3 4.608−3 4.723−2 1.819−2 1.195−1 9.405−3 3.564−2 1.384−2 4.406−2 1.299−1 7.064−3 1.938−2 1.100−2 2.238−1 1.862−2 1.735+0 2.824−2 1.637−3 4.089−3 2.765−3 4.013−2 4.800−3 2.395−1 6.282−3 6.870−2 4.073−3 1.065−2 6.055−3 3.933−2 1.866−2 3.471−1 1.553−1 2.504+0
6.665−2 9.993−2 4.727−2 6.321−2 2.052−2 1.317−2 2.546−2 1.274−2 1.911−2 4.610−3 6.160−3 8.348−3 1.043−2 1.744−1 4.141+0 3.393−2 2.383−2 1.129−1 2.032−2 3.805−1 1.822−2 2.139−1 1.795−2 4.032−3 2.078−2 4.414−3 6.950−2 4.029−3 1.947−2 2.692−3 2.400−2 3.813−3 9.361−1 7.891+0 5.060−2 2.143−2 2.485−1 1.014−1 7.207−1 8.508−2 3.842−1 8.385−3 4.577−3 4.623−2 1.912−2 1.308−1 8.987−3 3.516−2 1.331−2 4.329−2 1.061−1 6.581−3 2.034−2 1.013−2 2.174−1 1.636−2 1.885+0 2.415−2 1.521−3 4.111−3 2.500−3 3.882−2 4.140−3 2.530−1 5.187−3 7.147−2 3.594−3 9.929−3 5.212−3 4.025−2 1.644−2 3.359−1 1.619−1 2.718+0
7.191−2 1.073−1 4.901−2 6.534−2 2.305−2 1.499−2 2.899−2 1.341−2 2.008−2 4.528−3 6.050−3 8.836−3 1.103−2 1.788−1 4.460+0 2.667−2 2.689−2 1.254−1 2.235−2 4.252−1 1.895−2 2.292−1 1.797−2 4.594−3 2.455−2 5.006−3 7.561−2 4.145−3 1.993−2 2.695−3 2.544−2 3.998−3 1.005+0 8.531+0 5.662−2 2.358−2 2.750−1 1.112−1 8.001−1 8.950−2 4.098−1 9.508−3 5.178−3 5.422−2 2.048−2 1.418−1 9.126−3 3.595−2 1.405−2 4.579−2 7.924−2 6.258−3 2.098−2 9.623−3 2.295−1 1.547−2 2.061+0 2.259−2 1.547−3 4.365−3 2.570−3 4.192−2 4.173−3 2.726−1 5.210−3 7.675−2 3.834−3 9.460−3 4.719−3 4.078−2 1.564−2 3.526−1 1.723−1 2.966+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
64
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
3.017−3 3.208−3 9.073−3 1.029−2 6.928−2 2.880−2 2.288−1 1.539−2 6.294−2 5.977+0 1.159+1 5.491−1 8.238−1 5.027−2 6.718−2 3.263−1 4.542−2 8.579−2 9.662−2 1.438−1 1.058−1 1.408−1 5.457−2 6.816−2 7.085−1 1.096+1 9.048−2 4.314−1 4.129−2 2.573−2 3.474−1 4.446−2 2.569−1 4.695−2 3.227−1 3.775−2 1.920−1 3.637−2 2.359+0 2.003+1 1.764−1 7.706−1 5.339−2 4.682−2 7.418−1 1.119−1 5.174−1 1.430−1 5.893−1 1.131−1 3.464−1 3.547−1 1.230+1 8.231−2 2.167−2 3.876−2 2.988−2 7.115−1 4.546−2 1.375+0 6.506−2 8.800−1 6.537−2 9.501−1 1.753+1 3.272−2 1.887−2 8.471−2 4.587−2 1.091+0 1.693−1 2.004+0 1.708−1 1.250+0
4.725−3 3.967−3 1.221−2 1.131−2 6.775−2 3.040−2 2.344−1 1.574−2 6.561−2 6.165+0 1.208+1 5.867−1 1.056+0 1.327−1 1.691−1 3.027−1 4.769−2 8.765−2 9.421−2 1.408−1 1.071−1 1.428−1 5.749−2 7.187−2 7.699−1 1.130+1 1.927−1 5.403−1 1.497−1 3.470−2 3.061−1 3.992−2 2.563−1 4.376−2 3.135−1 3.965−2 1.988−1 3.980−2 2.651+0 2.291+1 3.926−1 1.065+0 7.147−2 4.382−2 6.493−1 1.078−1 5.143−1 1.429−1 5.756−1 1.197−1 3.595−1 6.200−1 1.497+1 3.757−1 2.929−2 5.183−2 3.176−2 6.538−1 4.496−2 1.345+0 6.356−2 8.558−1 6.516−2 1.664+0 2.655+1 4.446−2 1.968−2 1.028−1 4.551−2 1.004+0 1.655−1 1.958+0 1.678−1 1.218+0
4.105−3 3.519−3 1.121−2 1.016−2 6.664−2 2.861−2 2.415−1 1.470−2 6.763−2 6.696+0 1.303+1 5.710−1 9.999−1 1.139−1 1.449−1 3.086−1 5.591−2 1.042−1 1.008−1 1.506−1 1.080−1 1.439−1 5.774−2 7.218−2 7.359−1 1.239+1 1.716−1 5.062−1 1.201−1 3.615−2 3.119−1 4.214−2 2.953−1 4.397−2 3.340−1 3.932−2 1.996−1 3.763−2 2.883+0 2.479+1 3.363−1 9.774−1 7.506−2 4.555−2 6.650−1 1.162−1 5.871−1 1.484−1 6.110−1 1.171−1 3.595−1 5.432−1 1.753+1 2.945−1 2.704−2 5.176−2 3.111−2 6.659−1 4.386−2 1.485+0 5.992−2 9.023−1 6.055−2 1.830+0 2.992+1 4.106−2 1.868−2 1.037−1 4.440−2 1.022+0 1.716−1 2.157+0 1.678−1 1.281+0
3.599−3 3.063−3 1.030−2 8.915−3 6.555−2 2.682−2 2.521−1 1.373−2 7.092−2 7.306+0 1.414+1 5.555−1 9.398−1 9.691−2 1.239−1 3.155−1 6.859−2 1.289−1 1.091−1 1.630−1 1.087−1 1.449−1 5.840−2 7.300−2 7.041−1 1.361+1 1.528−1 4.744−1 9.409−2 4.050−2 3.190−1 4.514−2 3.514−1 4.416−2 3.591−1 3.921−2 2.004−1 3.559−2 3.144+0 2.690+1 2.839−1 8.963−1 8.467−2 4.837−2 6.834−1 1.282−1 6.914−1 1.556−1 6.544−1 1.146−1 3.593−1 4.723−1 2.011+1 2.236−1 2.603−2 5.424−2 3.106−2 6.799−1 4.309−2 1.681+0 5.639−2 9.589−1 5.633−2 1.991+0 3.317+1 3.953−2 1.796−2 1.086−1 4.362−2 1.043+0 1.820−1 2.438+0 1.694−1 1.357+0
3.188−3 2.626−3 9.534−3 7.676−3 6.457−2 2.526−2 2.672−1 1.294−2 7.576−2 7.971+0 1.536+1 5.415−1 8.872−1 8.382−2 1.080−1 3.229−1 8.667−2 1.637−1 1.188−1 1.774−1 1.093−1 1.456−1 5.949−2 7.436−2 6.767−1 1.491+1 1.389−1 4.479−1 7.381−2 4.799−2 3.264−1 4.883−2 4.281−1 4.432−2 3.876−1 3.935−2 2.010−1 3.384−2 3.418+0 2.915+1 2.416−1 8.296−1 1.009−1 5.205−2 7.031−1 1.444−1 8.339−1 1.640−1 7.040−1 1.125−1 3.592−1 4.151−1 2.251+1 1.686−1 2.589−2 5.951−2 3.165−2 6.945−1 4.276−2 1.945+0 5.325−2 1.023+0 5.285−2 2.143+0 3.621+1 3.931−2 1.745−2 1.180−1 4.330−2 1.065+0 1.978−1 2.818+0 1.727−1 1.445+0
2.868−3 2.235−3 8.985−3 6.543−3 6.381−2 2.419−2 2.880−1 1.243−2 8.219−2 8.670+0 1.669+1 5.293−1 8.450−1 7.474−2 9.708−2 3.300−1 1.110−1 2.102−1 1.292−1 1.930−1 1.097−1 1.461−1 6.090−2 7.613−2 6.537−1 1.624+1 1.300−1 4.269−1 5.911−2 5.885−2 3.337−1 5.294−2 5.282−1 4.446−2 4.176−1 3.972−2 2.017−1 3.251−2 3.696+0 3.148+1 2.101−1 7.775−1 1.242−1 5.625−2 7.227−1 1.655−1 1.020+0 1.732−1 7.564−1 1.110−1 3.593−1 3.721−1 2.468+1 1.292−1 2.633−2 6.782−2 3.293−2 7.088−1 4.289−2 2.286+0 5.070−2 1.090+0 5.030−2 2.283+0 3.900+1 3.997−2 1.710−2 1.327−1 4.344−2 1.087+0 2.199−1 3.309+0 1.773−1 1.537+0
2.633−3 1.909−3 8.700−3 5.586−3 6.330−2 2.376−2 3.152−1 1.224−2 8.990−2 9.385+0 1.806+1 5.186−1 8.120−1 6.897−2 9.029−2 3.364−1 1.417−1 2.688−1 1.395−1 2.085−1 1.100−1 1.466−1 6.247−2 7.810−2 6.337−1 1.755+1 1.251−1 4.104−1 4.897−2 7.307−2 3.402−1 5.708−2 6.523−1 4.459−2 4.465−1 4.024−2 2.024−1 3.160−2 3.969+0 3.381+1 1.874−1 7.372−1 1.546−1 6.050−2 7.406−1 1.917−1 1.250+0 1.822−1 8.067−1 1.100−1 3.599−1 3.408−1 2.661+1 1.024−1 2.704−2 7.920−2 3.485−2 7.214−1 4.333−2 2.706+0 4.879−2 1.154+0 4.864−2 2.410+0 4.154+1 4.107−2 1.689−2 1.528−1 4.389−2 1.106+0 2.487−1 3.914+0 1.826−1 1.625+0
2.464−3 1.649−3 8.632−3 4.819−3 6.268−2 2.386−2 3.457−1 1.224−2 9.758−2 1.003+1 1.931+1 5.064−1 7.824−1 6.527−2 8.598−2 3.397−1 1.763−1 3.346−1 1.477−1 2.210−1 1.097−1 1.462−1 6.363−2 7.955−2 6.126−1 1.869+1 1.224−1 3.953−1 4.203−2 8.928−2 3.436−1 6.045−2 7.893−1 4.450−2 4.685−1 4.057−2 2.021−1 3.091−2 4.204+0 3.584+1 1.707−1 7.020−1 1.893−1 6.392−2 7.512−1 2.201−1 1.505+0 1.889−1 8.445−1 1.090−1 3.590−1 3.169−1 2.815+1 8.466−2 2.765−2 9.236−2 3.697−2 7.273−1 4.362−2 3.163+0 4.723−2 1.202+0 4.742−2 2.510+0 4.357+1 4.203−2 1.670−2 1.759−1 4.419−2 1.115+0 2.807−1 4.575+0 1.864−1 1.690+0
2.291−3 1.424−3 8.482−3 4.158−3 6.039−2 2.366−2 3.647−1 1.201−2 1.012−1 1.026+1 1.979+1 4.816−1 7.376−1 6.138−2 8.120−2 3.313−1 2.035−1 3.860−1 1.490−1 2.231−1 1.062−1 1.415−1 6.258−2 7.824−2 5.773−1 1.907+1 1.178−1 3.726−1 3.658−2 1.019−1 3.351−1 6.106−2 8.928−1 4.308−2 4.693−1 3.960−2 1.959−1 2.960−2 4.269+0 3.644+1 1.547−1 6.551−1 2.163−1 6.444−2 7.352−1 2.397−1 1.696+0 1.876−1 8.443−1 1.051−1 3.476−1 2.914−1 2.848+1 7.173−2 2.731−2 1.021−1 3.785−2 7.084−1 4.250−2 3.490+0 4.481−2 1.197+0 4.531−2 2.512+0 4.385+1 4.151−2 1.608−2 1.926−1 4.306−2 1.086+0 3.024−1 5.049+0 1.835−1 1.682+0
2.331−3 1.443−3 8.926−3 4.193−3 6.503−2 2.508−2 3.924−1 1.287−2 1.087−1 1.083+1 2.086+1 5.081−1 7.637−1 6.015−2 8.039−2 3.607−1 2.256−1 4.307−1 1.597−1 2.379−1 1.236−1 1.647−1 6.755−2 8.445−2 6.183−1 2.029+1 1.174−1 3.878−1 3.156−2 1.168−1 3.740−1 6.918−2 9.895−1 4.934−2 4.907−1 4.236−2 2.118−1 3.156−2 4.346+0 3.712+1 1.505−1 6.844−1 2.459−1 7.305−2 8.205−1 2.662−1 1.872+0 1.976−1 8.836−1 1.131−1 3.755−1 2.952−1 3.209+1 5.706−2 2.719−2 1.120−1 4.264−2 7.575−1 5.518−2 3.820+0 4.980−2 1.270+0 4.842−2 2.608+0 5.229+1 4.111−2 1.803−2 2.105−1 5.389−2 1.165+0 3.287−1 5.508+0 1.953−1 1.786+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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65
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
3.129−1 7.948−3 1.627−2 1.667−2 6.269−2 3.109−2 8.961−1 6.437−2 4.907+0 1.164−1 1.062−2 9.465−3 3.438−2 2.490−2 1.003−1 6.445−2 1.217+0 3.029−1 6.405+0 1.525+1 2.961+1 1.549+0 2.323+0 1.793−1 2.395−1 4.967−2 6.226−2 1.816+0 2.952+1 2.451−1 1.684+0 1.171−1 1.072−1 3.347−2 6.403+0 5.469+1 6.320−1 2.978+0 7.996−2 1.993−1 9.221−1 4.154+1 1.702−1 1.393+0 8.320−2 3.106+0 7.092+1 2.478−1 1.967+0 5.986−1 3.378+1 1.569−1 1.695+0 4.576+1 5.566−1
1.046+0 1.519−2 1.984−2 1.929−2 7.600−2 3.248−2 8.569−1 6.312−2 4.816+0 1.120−1 1.820−2 1.132−2 3.961−2 2.545−2 1.178−1 6.327−2 1.164+0 2.953−1 6.282+0 1.713+1 3.287+1 1.523+0 2.294+0 2.010−1 2.675−1 5.262−2 6.579−2 1.727+0 3.514+1 2.769−1 1.638+0 1.215−1 1.213−1 3.334−2 8.048+0 6.745+1 6.233−1 2.898+0 8.439−2 2.229−1 8.881−1 7.272+1 1.821−1 1.353+0 8.046−2 6.696+0 1.131+2 2.395−1 1.911+0 5.731−1 7.075+1 1.442−1 4.720+0 9.960+1 4.943−1
8.308−1 1.220−2 1.836−2 1.707−2 7.376−2 2.892−2 8.619−1 5.604−2 5.162+0 9.878−2 1.498−2 9.697−3 3.672−2 2.222−2 1.139−1 5.616−2 1.168+0 2.944−1 6.729+0 1.861+1 3.563+1 1.505+0 2.266+0 2.025−1 2.696−1 5.050−2 6.314−2 1.696+0 3.817+1 2.811−1 1.609+0 1.192−1 1.204−1 3.079−2 8.727+0 7.333+1 6.114−1 2.843+0 8.067−2 2.196−1 8.706−1 7.889+1 1.796−1 1.323+0 7.332−2 7.182+0 1.224+2 2.281−1 1.865+0 5.495−1 7.620+1 1.305−1 4.935+0 1.069+2 4.470−1
6.389−1 1.007−2 1.732−2 1.510−2 7.267−2 2.554−2 8.684−1 4.923−2 5.643+0 8.598−2 1.262−2 8.252−3 3.441−2 1.910−2 1.113−1 4.935−2 1.175+0 2.989−1 7.351+0 2.022+1 3.870+1 1.484+0 2.232+0 2.046−1 2.727−1 4.863−2 6.081−2 1.663+0 4.140+1 2.864−1 1.576+0 1.170−1 1.200−1 2.857−2 9.436+0 7.951+1 5.990−1 2.783+0 7.756−2 2.175−1 8.523−1 8.494+1 1.781−1 1.291+0 6.694−2 7.649+0 1.313+2 2.175−1 1.819+0 5.267−1 8.144+1 1.184−1 5.135+0 1.139+2 4.033−1
4.869−1 8.559−3 1.664−2 1.346−2 7.313−2 2.260−2 8.758−1 4.323−2 6.285+0 7.457−2 1.091−2 7.032−3 3.269−2 1.632−2 1.110−1 4.334−2 1.183+0 3.110−1 8.184+0 2.192+1 4.198+1 1.459+0 2.194+0 2.075−1 2.766−1 4.709−2 5.888−2 1.627+0 4.476+1 2.924−1 1.541+0 1.152−1 1.201−1 2.680−2 1.016+1 8.585+1 5.861−1 2.718+0 7.524−2 2.165−1 8.334−1 9.079+1 1.778−1 1.259+0 6.163−2 8.093+0 1.399+2 2.080−1 1.771+0 5.057−1 8.643+1 1.088−1 5.323+0 1.205+2 3.653−1
3.747−1 7.501−3 1.627−2 1.219−2 7.544−2 2.030−2 8.834−1 3.837−2 7.109+0 6.520−2 9.689−3 6.063−3 3.156−2 1.401−2 1.135−1 3.849−2 1.191+0 3.323−1 9.255+0 2.367+1 4.540+1 1.431+0 2.151+0 2.109−1 2.812−1 4.591−2 5.741−2 1.586+0 4.816+1 2.988−1 1.501+0 1.138−1 1.208−1 2.553−2 1.088+1 9.220+1 5.728−1 2.648+0 7.373−2 2.166−1 8.138−1 9.640+1 1.787−1 1.225+0 5.752−2 8.512+0 1.481+2 1.997−1 1.722+0 4.866−1 9.114+1 1.017−1 5.499+0 1.267+2 3.339−1
2.955−1 6.787−3 1.612−2 1.126−2 7.968−2 1.869−2 8.899−1 3.471−2 8.117+0 5.806−2 8.858−3 5.341−3 3.092−2 1.223−2 1.189−1 3.483−2 1.199+0 3.632−1 1.057+1 2.544+1 4.888+1 1.401+0 2.105+0 2.147−1 2.864−1 4.505−2 5.635−2 1.539+0 5.153+1 3.051−1 1.457+0 1.126−1 1.216−1 2.470−2 1.158+1 9.843+1 5.585−1 2.570+0 7.289−2 2.175−1 7.929−1 1.017+2 1.803−1 1.190+0 5.448−2 8.903+0 1.558+2 1.922−1 1.671+0 4.692−1 9.553+1 9.692−2 5.662+0 1.324+2 3.089−1
2.403−1 6.295−3 1.602−2 1.058−2 8.496−2 1.760−2 8.899−1 3.193−2 9.204+0 5.275−2 8.278−3 4.813−3 3.045−2 1.090−2 1.261−1 3.207−2 1.198+0 3.995−1 1.199+1 2.699+1 5.195+1 1.365+0 2.049+0 2.175−1 2.902−1 4.424−2 5.534−2 1.480+0 5.440+1 3.086−1 1.400+0 1.109−1 1.217−1 2.407−2 1.216+1 1.037+2 5.402−1 2.473+0 7.204−2 2.171−1 7.662−1 1.059+2 1.811−1 1.145+0 5.205−2 9.202+0 1.619+2 1.845−1 1.609+0 4.506−1 9.893+1 9.342−2 5.775+0 1.368+2 2.877−1
1.990−1 5.815−3 1.551−2 9.835−3 8.776−2 1.648−2 8.615−1 2.918−2 9.930+0 4.783−2 7.685−3 4.339−3 2.928−2 9.722−3 1.297−1 2.931−2 1.159+0 4.226−1 1.294+1 2.742+1 5.288+1 1.296+0 1.945+0 2.135−1 2.849−1 4.236−2 5.299−2 1.383+0 5.506+1 3.011−1 1.307+0 1.060−1 1.178−1 2.296−2 1.226+1 1.048+2 5.071−1 2.310+0 6.925−2 2.099−1 7.188−1 1.060+2 1.760−1 1.070+0 4.884−2 9.151+0 1.616+2 1.724−1 1.503+0 4.213−1 9.854+1 8.846−2 5.683+0 1.360+2 2.637−1
1.637−1 6.003−3 1.600−2 1.054−2 8.587−2 1.749−2 9.063−1 3.122−2 1.077+1 5.220−2 8.024−3 4.731−3 3.051−2 1.069−2 1.269−1 3.136−2 1.220+0 4.540−1 1.400+1 2.475+1 4.823+1 1.285+0 1.930+0 2.460−1 3.295−1 4.586−2 5.746−2 1.426+0 5.011+1 3.890−1 1.369+0 1.228−1 1.463−1 2.625−2 1.145+1 9.612+1 5.413−1 2.425+0 8.086−2 2.522−1 7.594−1 1.132+2 1.930−1 1.137+0 5.394−2 8.007+0 2.079+2 1.859−1 1.599+0 4.524−1 9.516+1 4.487−1 4.931+0 1.354+2 2.950−1
66
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 26 Effective collision strengths for transitions in Ti XX. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.325−1 4.546−1 2.080−2 5.840−3 1.103−2 1.587−2 2.372−2 4.168−3 1.472−3 2.820−3 2.884−3 4.325−3 1.713−3 2.277−3 1.628−3 6.287−4 1.205−3 1.114−3 1.672−3 9.061−4 1.205−3 1.180−4 1.471−4 4.146−2 1.475−3 2.270−2 5.985−3 7.619−2 1.108−2 4.696−4 4.714−3 1.960−3 1.401−2 3.453−3 2.353−3 1.441−3 2.226−4 1.890−3 9.415−4 5.260−3 1.614−3 1.250−3 8.714−4 1.168−4 1.162−4 2.984−3 6.127−3 5.173−2 2.918−2 1.491−1 9.357−4 1.978−3 1.142−2 7.018−3 2.836−2 2.592−3 5.191−3 4.421−4 9.473−4 4.720−3 3.013−3 1.088−2 1.509−3 2.821−3 1.997−4 2.797−4 1.518+0 2.943+0 1.109−1 1.666−1 9.751−2 1.571−2 2.937−2
2.391−1 4.626−1 2.251−2 7.611−3 1.411−2 1.709−2 2.596−2 4.581−3 2.082−3 4.059−3 3.432−3 5.171−3 2.285−3 3.093−3 1.554−3 7.390−4 1.429−3 1.195−3 1.798−3 9.651−4 1.285−3 1.292−4 1.609−4 5.880−2 6.931−3 2.418−2 1.019−2 7.701−2 1.733−2 1.526−3 5.069−3 3.145−3 1.507−2 4.781−3 3.699−3 2.762−3 4.517−4 1.732−3 1.026−3 5.518−3 1.721−3 1.400−3 9.113−4 1.372−4 1.181−4 1.550−2 1.100−2 5.774−2 3.711−2 1.565−1 3.072−3 3.170−3 1.343−2 8.955−3 3.139−2 4.782−3 8.565−3 9.555−4 1.044−3 4.518−3 3.209−3 1.146−2 1.619−3 3.129−3 2.112−4 3.179−4 1.508+0 2.947+0 1.449−1 2.208−1 9.816−2 1.960−2 3.847−2
2.493−1 4.835−1 2.213−2 7.690−3 1.446−2 1.730−2 2.629−2 4.391−3 2.000−3 3.896−3 3.314−3 4.984−3 2.129−3 2.868−3 1.540−3 7.450−4 1.442−3 1.181−3 1.777−3 9.435−4 1.256−3 1.209−4 1.505−4 6.558−2 5.603−3 2.375−2 9.588−3 7.976−2 1.652−2 1.244−3 4.850−3 2.764−3 1.523−2 4.297−3 3.444−3 2.348−3 3.964−4 1.710−3 9.667−4 5.624−3 1.617−3 1.397−3 8.462−4 1.307−4 1.074−4 1.228−2 1.015−2 5.672−2 3.665−2 1.610−1 2.502−3 2.793−3 1.258−2 8.384−3 3.130−2 4.154−3 7.813−3 8.277−4 9.816−4 4.413−3 3.103−3 1.157−2 1.531−3 3.077−3 1.940−4 2.993−4 1.600+0 3.115+0 1.426−1 2.169−1 9.753−2 2.059−2 4.018−2
2.617−1 5.079−1 2.180−2 7.871−3 1.491−2 1.742−2 2.643−2 4.253−3 1.964−3 3.819−3 3.208−3 4.821−3 1.982−3 2.661−3 1.537−3 7.625−4 1.478−3 1.165−3 1.753−3 9.187−4 1.223−3 1.114−4 1.388−4 6.831−2 4.542−3 2.327−2 8.649−3 8.336−2 1.494−2 1.020−3 4.659−3 2.403−3 1.558−2 3.780−3 3.248−3 1.945−3 3.513−4 1.690−3 8.972−4 5.786−3 1.483−3 1.407−3 7.664−4 1.245−4 9.487−5 9.799−3 9.065−3 5.510−2 3.542−2 1.663−1 2.053−3 2.432−3 1.182−2 7.808−3 3.152−2 3.557−3 7.173−3 7.266−4 9.100−4 4.301−3 2.972−3 1.175−2 1.429−3 3.038−3 1.746−4 2.801−4 1.721+0 3.334+0 1.364−1 2.070−1 9.759−2 2.282−2 4.411−2
2.765−1 5.367−1 2.159−2 8.314−3 1.581−2 1.766−2 2.672−2 4.176−3 2.001−3 3.883−3 3.135−3 4.711−3 1.864−3 2.496−3 1.545−3 7.980−4 1.548−3 1.150−3 1.730−3 8.934−4 1.190−3 1.015−4 1.263−4 6.597−2 3.732−3 2.286−2 7.609−3 8.866−2 1.301−2 8.511−4 4.516−3 2.080−3 1.622−2 3.264−3 3.158−3 1.587−3 3.136−4 1.671−3 8.191−4 6.031−3 1.323−3 1.441−3 6.757−4 1.194−4 8.145−5 7.964−3 7.935−3 5.341−2 3.413−2 1.745−1 1.716−3 2.109−3 1.120−2 7.293−3 3.228−2 3.051−3 6.753−3 6.448−4 8.306−4 4.186−3 2.826−3 1.207−2 1.318−3 3.033−3 1.542−4 2.623−4 1.872+0 3.612+0 1.289−1 1.951−1 9.839−2 2.670−2 5.121−2
2.950−1 5.719−1 2.158−2 9.189−3 1.751−2 1.818−2 2.743−2 4.159−3 2.132−3 4.134−3 3.109−3 4.673−3 1.781−3 2.381−3 1.562−3 8.601−4 1.670−3 1.139−3 1.714−3 8.716−4 1.161−3 9.185−5 1.144−4 5.970−2 3.180−3 2.259−2 6.653−3 9.657−2 1.110−2 7.306−4 4.423−3 1.802−3 1.725−2 2.769−3 3.194−3 1.284−3 2.832−4 1.657−3 7.368−4 6.392−3 1.148−3 1.509−3 5.813−4 1.164−4 6.813−5 6.740−3 6.929−3 5.206−2 3.340−2 1.874−1 1.478−3 1.831−3 1.073−2 6.887−3 3.379−2 2.655−3 6.596−3 5.803−4 7.474−4 4.075−3 2.684−3 1.259−2 1.213−3 3.085−3 1.347−4 2.482−4 2.047+0 3.937+0 1.218−1 1.841−1 9.977−2 3.261−2 6.223−2
3.177−1 6.149−1 2.177−2 1.064−2 2.031−2 1.904−2 2.866−2 4.190−3 2.379−3 4.611−3 3.134−3 4.713−3 1.734−3 2.315−3 1.588−3 9.583−4 1.863−3 1.138−3 1.714−3 8.564−4 1.141−3 8.351−5 1.041−4 5.179−2 2.884−3 2.252−2 5.875−3 1.079−1 9.397−3 6.545−4 4.376−3 1.570−3 1.878−2 2.315−3 3.360−3 1.036−3 2.613−4 1.648−3 6.564−4 6.906−3 9.711−4 1.619−3 4.913−4 1.158−4 5.593−5 6.096−3 6.126−3 5.122−2 3.362−2 2.068−1 1.331−3 1.599−3 1.040−2 6.633−3 3.622−2 2.373−3 6.710−3 5.352−4 6.667−4 3.977−3 2.572−3 1.338−2 1.126−3 3.215−3 1.177−4 2.391−4 2.238+0 4.295+0 1.160−1 1.751−1 1.015−1 4.081−2 7.770−2
3.437−1 6.640−1 2.207−2 1.271−2 2.429−2 2.017−2 3.032−2 4.247−3 2.742−3 5.317−3 3.200−3 4.815−3 1.712−3 2.284−3 1.616−3 1.095−3 2.131−3 1.147−3 1.728−3 8.473−4 1.129−3 7.689−5 9.588−5 4.415−2 2.821−3 2.255−2 5.293−3 1.226−1 7.995−3 6.178−4 4.355−3 1.382−3 2.078−2 1.920−3 3.628−3 8.432−4 2.489−4 1.642−3 5.832−4 7.566−3 8.071−4 1.764−3 4.123−4 1.173−4 4.555−5 5.966−3 5.535−3 5.078−2 3.492−2 2.327−1 1.264−3 1.412−3 1.017−2 6.547−3 3.955−2 2.194−3 7.044−3 5.106−4 5.936−4 3.893−3 2.504−3 1.445−2 1.064−3 3.414−3 1.038−4 2.347−4 2.428+0 4.658+0 1.113−1 1.679−1 1.031−1 5.113−2 9.722−2
3.653−1 7.051−1 2.206−2 1.490−2 2.853−2 2.103−2 3.159−2 4.236−3 3.116−3 6.049−3 3.231−3 4.864−3 1.678−3 2.238−3 1.613−3 1.230−3 2.397−3 1.142−3 1.721−3 8.283−4 1.105−3 7.100−5 8.858−5 3.749−2 2.886−3 2.228−2 4.825−3 1.368−1 6.835−3 6.023−4 4.275−3 1.221−3 2.260−2 1.582−3 3.871−3 6.923−4 2.412−4 1.609−3 5.152−4 8.143−3 6.614−4 1.887−3 3.450−4 1.176−4 3.697−5 6.116−3 5.064−3 4.981−2 3.641−2 2.580−1 1.240−3 1.252−3 9.854−3 6.497−3 4.260−2 2.063−3 7.363−3 4.963−4 5.256−4 3.760−3 2.441−3 1.538−2 1.011−3 3.582−3 9.203−5 2.295−4 2.558+0 4.911+0 1.061−1 1.599−1 1.025−1 6.115−2 1.162−1
3.736−1 7.238−1 2.324−2 1.607−2 3.071−2 2.185−2 3.270−2 4.603−3 3.339−3 6.454−3 3.261−3 4.900−3 1.703−3 2.264−3 1.783−3 1.315−3 2.546−3 1.137−3 1.710−3 8.463−4 1.126−3 7.140−5 8.899−5 2.758−2 2.676−3 2.375−2 4.607−3 1.454−1 6.051−3 5.540−4 4.785−3 1.197−3 2.354−2 1.447−3 4.028−3 6.215−4 2.173−4 1.883−3 5.217−4 8.358−3 6.302−4 2.011−3 3.502−4 1.260−4 3.839−5 5.640−3 4.832−3 5.258−2 3.722−2 2.723−1 1.142−3 1.228−3 1.082−2 6.522−3 4.413−2 2.008−3 7.557−3 4.453−4 5.328−4 4.298−3 2.449−3 1.573−2 1.050−3 3.786−3 9.405−5 2.318−4 2.657+0 5.211+0 1.044−1 1.572−1 1.087−1 6.679−2 1.272−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
67
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
4.040−2 6.019−2 4.123−2 5.494−2 1.836−2 3.621−3 6.884−3 8.507−3 1.273−2 4.789−3 6.398−3 7.383−3 9.217−3 1.827−1 2.184+0 2.819−2 6.324−3 1.040−1 1.461−2 1.275−1 1.888−2 1.357−1 2.010−2 1.526−3 2.024−2 4.036−3 2.665−2 5.387−3 1.444−2 4.639−3 1.745−2 5.772−3 5.039−1 4.149+0 1.307−2 1.536−2 2.239−1 4.991−2 2.527−1 6.534−2 2.498−1 3.047−3 4.158−3 4.467−2 1.206−2 5.352−2 1.009−2 2.802−2 1.375−2 3.354−2 1.329−1 5.591−3 1.044−2 1.079−2 2.008−1 2.576−2 8.778−1 4.554−2 1.822−3 3.269−3 4.147−3 3.858−2 9.427−3 1.388−1 1.517−2 3.786−2 8.760−3 8.427−3 7.341−3 2.468−2 2.585−2 3.146−1 1.121−1 1.279+0
4.172−2 6.699−2 4.881−2 6.972−2 1.708−2 4.238−3 8.047−3 8.712−3 1.307−2 5.770−3 7.710−3 7.866−3 9.833−3 2.247−1 2.227+0 9.440−2 1.421−2 9.922−2 2.012−2 1.285−1 2.775−2 1.368−1 3.294−2 2.474−3 1.769−2 3.988−3 2.854−2 5.845−3 1.539−2 5.276−3 1.798−2 6.119−3 5.813−1 4.227+0 3.064−2 2.136−2 2.227−1 6.009−2 2.753−1 8.206−2 2.746−1 5.630−3 4.200−3 3.951−2 1.298−2 5.735−2 1.121−2 3.021−2 1.442−2 3.472−2 3.723−1 1.819−2 2.466−2 2.755−2 2.096−1 4.978−2 8.756−1 8.273−2 3.255−3 4.583−3 5.185−3 3.744−2 1.034−2 1.418−1 1.622−2 3.957−2 8.878−3 2.652−2 1.924−2 6.424−2 4.943−2 3.647−1 1.523−1 1.317+0
4.268−2 6.762−2 4.731−2 6.690−2 1.723−2 4.524−3 8.612−3 8.925−3 1.339−2 5.505−3 7.355−3 7.688−3 9.610−3 2.175−1 2.338+0 8.895−2 1.244−2 9.903−2 1.861−2 1.380−1 2.517−2 1.404−1 2.900−2 2.304−3 1.784−2 3.903−3 3.024−2 5.515−3 1.552−2 4.822−3 1.840−2 5.683−3 5.985−1 4.424+0 2.673−2 1.961−2 2.207−1 5.905−2 2.886−1 7.800−2 2.758−1 5.075−3 4.083−3 3.974−2 1.292−2 6.021−2 1.065−2 3.007−2 1.397−2 3.513−2 3.482−1 1.428−2 2.112−2 2.279−2 2.063−1 4.212−2 9.144−1 6.983−2 2.735−3 4.241−3 4.659−3 3.711−2 9.333−3 1.464−1 1.446−2 4.097−2 7.897−3 2.104−2 1.569−2 5.387−2 4.178−2 3.519−1 1.411−1 1.364+0
4.438−2 6.918−2 4.599−2 6.418−2 1.749−2 5.008−3 9.555−3 9.228−3 1.384−2 5.218−3 6.973−3 7.535−3 9.419−3 2.067−1 2.507+0 7.727−2 1.162−2 9.931−2 1.750−2 1.527−1 2.276−2 1.461−1 2.529−2 2.241−3 1.807−2 3.841−3 3.275−2 5.154−3 1.573−2 4.327−3 1.896−2 5.216−3 6.241−1 4.750+0 2.487−2 1.842−2 2.196−1 5.936−2 3.114−1 7.490−2 2.804−1 4.821−3 4.004−3 4.015−2 1.300−2 6.454−2 1.007−2 3.006−2 1.353−2 3.578−2 2.995−1 1.137−2 1.843−2 1.858−2 2.035−1 3.478−2 9.741−1 5.740−2 2.338−3 3.950−3 4.127−3 3.681−2 8.227−3 1.531−1 1.252−2 4.318−2 6.866−3 1.687−2 1.256−2 4.549−2 3.453−2 3.389−1 1.319−1 1.439+0
4.696−2 7.217−2 4.504−2 6.207−2 1.782−2 5.756−3 1.101−2 9.635−3 1.445−2 4.940−3 6.601−3 7.440−3 9.299−3 1.950−1 2.734+0 6.392−2 1.176−2 1.001−1 1.695−2 1.746−1 2.079−2 1.543−1 2.224−2 2.288−3 1.835−2 3.814−3 3.634−2 4.792−3 1.607−2 3.834−3 1.966−2 4.762−3 6.627−1 5.202+0 2.510−2 1.787−2 2.202−1 6.166−2 3.480−1 7.335−2 2.898−1 4.849−3 3.970−3 4.071−2 1.330−2 7.084−2 9.518−3 3.025−2 1.315−2 3.666−2 2.438−1 9.293−3 1.672−2 1.522−2 2.018−1 2.852−2 1.061+0 4.662−2 2.030−3 3.729−3 3.618−3 3.658−2 7.107−3 1.626−1 1.055−2 4.637−2 5.874−3 1.387−2 1.003−2 3.957−2 2.837−2 3.288−1 1.265−1 1.555+0
5.037−2 7.659−2 4.447−2 6.067−2 1.820−2 6.837−3 1.311−2 1.014−2 1.522−2 4.699−3 6.279−3 7.427−3 9.283−3 1.846−1 3.000+0 5.203−2 1.289−2 1.014−1 1.693−2 2.052−1 1.931−2 1.646−1 1.995−2 2.456−3 1.867−2 3.833−3 4.125−2 4.459−3 1.652−2 3.387−3 2.044−2 4.356−3 7.117−1 5.732+0 2.746−2 1.790−2 2.224−1 6.634−2 4.017−1 7.343−2 3.042−1 5.164−3 3.988−3 4.138−2 1.389−2 7.958−2 9.063−3 3.068−2 1.286−2 3.770−2 1.933−1 7.890−3 1.602−2 1.275−2 2.015−1 2.357−2 1.182+0 3.790−2 1.795−3 3.597−3 3.168−3 3.644−2 6.065−3 1.755−1 8.718−3 5.056−2 5.000−3 1.183−2 8.084−3 3.611−2 2.351−2 3.222−1 1.258−1 1.721+0
5.438−2 8.209−2 4.424−2 5.990−2 1.860−2 8.308−3 1.596−2 1.073−2 1.610−2 4.514−3 6.032−3 7.505−3 9.381−3 1.760−1 3.285+0 4.285−2 1.500−2 1.030−1 1.736−2 2.457−1 1.827−2 1.764−1 1.840−2 2.757−3 1.900−2 3.900−3 4.768−2 4.179−3 1.708−2 3.018−3 2.122−2 4.024−3 7.665−1 6.292+0 3.195−2 1.840−2 2.257−1 7.357−2 4.744−1 7.486−2 3.222−1 5.774−3 4.058−3 4.213−2 1.487−2 9.115−2 8.737−3 3.134−2 1.268−2 3.880−2 1.528−1 6.998−3 1.625−2 1.107−2 2.021−1 1.988−2 1.340+0 3.123−2 1.626−3 3.574−3 2.804−3 3.641−2 5.172−3 1.923−1 7.142−3 5.563−2 4.295−3 1.053−2 6.659−3 3.492−2 1.990−2 3.187−1 1.299−1 1.943+0
5.846−2 8.786−2 4.416−2 5.949−2 1.895−2 1.014−2 1.952−2 1.133−2 1.699−2 4.382−3 5.856−3 7.641−3 9.550−3 1.691−1 3.564+0 3.638−2 1.797−2 1.045−1 1.803−2 2.949−1 1.754−2 1.882−1 1.741−2 3.176−3 1.926−2 3.997−3 5.545−2 3.952−3 1.763−2 2.733−3 2.187−2 3.765−3 8.212−1 6.832+0 3.831−2 1.915−2 2.291−1 8.301−2 5.642−1 7.698−2 3.408−1 6.647−3 4.161−3 4.278−2 1.618−2 1.052−1 8.521−3 3.206−2 1.255−2 3.973−2 1.226−1 6.460−3 1.727−2 1.002−2 2.028−1 1.724−2 1.530+0 2.633−2 1.509−3 3.652−3 2.531−3 3.639−2 4.454−3 2.124−1 5.878−3 6.101−2 3.764−3 9.739−3 5.642−3 3.556−2 1.731−2 3.167−1 1.384−1 2.212+0
6.096−2 9.140−2 4.341−2 5.827−2 1.887−2 1.188−2 2.289−2 1.164−2 1.746−2 4.224−3 5.644−3 7.655−3 9.567−3 1.611−1 3.749+0 3.172−2 2.096−2 1.037−1 1.841−2 3.407−1 1.676−2 1.948−1 1.655−2 3.584−3 1.910−2 4.029−3 6.245−2 3.719−3 1.779−2 2.491−3 2.194−2 3.518−3 8.560−1 7.184+0 4.473−2 1.959−2 2.279−1 9.170−2 6.480−1 7.778−2 3.510−1 7.504−3 4.195−3 4.251−2 1.733−2 1.178−1 8.248−3 3.213−2 1.223−2 3.967−2 1.002−1 6.057−3 1.841−2 9.304−3 1.998−1 1.523−2 1.698+0 2.260−2 1.411−3 3.731−3 2.308−3 3.570−2 3.865−3 2.289−1 4.876−3 6.475−2 3.342−3 9.146−3 4.876−3 3.673−2 1.533−2 3.100−1 1.467−1 2.452+0
6.442−2 9.605−2 4.418−2 5.890−2 2.071−2 1.300−2 2.505−2 1.198−2 1.794−2 4.076−3 5.448−3 7.944−3 9.920−3 1.619−1 3.945+0 2.400−2 2.285−2 1.125−1 1.988−2 3.684−1 1.711−2 2.045−1 1.620−2 3.923−3 2.201−2 4.460−3 6.573−2 3.764−3 1.785−2 2.458−3 2.280−2 3.633−3 9.005−1 7.600+0 4.839−2 2.110−2 2.466−1 9.757−2 6.959−1 8.016−2 3.661−1 8.149−3 4.630−3 4.861−2 1.805−2 1.237−1 8.230−3 3.223−2 1.268−2 4.115−2 7.258−2 5.590−3 1.834−2 8.606−3 2.069−1 1.411−2 1.803+0 2.076−2 1.391−3 3.847−3 2.330−3 3.781−2 3.854−3 2.398−1 4.873−3 6.799−2 3.531−3 8.458−3 4.303−3 3.574−2 1.428−2 3.181−1 1.519−1 2.595+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
68
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.739−3 2.932−3 8.229−3 9.429−3 6.262−2 2.621−2 2.053−1 1.401−2 5.630−2 5.347+0 1.033+1 4.966−1 7.450−1 4.520−2 6.042−2 2.938−1 3.991−2 7.486−2 8.666−2 1.289−1 9.553−2 1.271−1 4.913−2 6.137−2 6.408−1 9.699+0 8.128−2 3.902−1 3.759−2 2.217−2 3.124−1 3.953−2 2.248−1 4.226−2 2.878−1 3.401−2 1.731−1 3.304−2 2.091+0 1.772+1 1.599−1 6.974−1 4.610−2 4.187−2 6.670−1 9.986−2 4.556−1 1.282−1 5.267−1 1.023−1 3.125−1 3.215−1 1.086+1 7.515−2 1.935−2 3.432−2 2.683−2 6.409−1 4.110−2 1.217+0 5.916−2 7.868−1 5.955−2 8.251−1 1.471+1 2.922−2 1.706−2 7.530−2 4.150−2 9.831−1 1.517−1 1.775+0 1.540−1 1.119+0
4.766−3 3.691−3 1.108−2 1.037−2 6.148−2 2.759−2 2.101−1 1.438−2 5.881−2 5.482+0 1.118+1 5.476−1 8.914−1 1.184−1 1.690−1 2.740−1 4.223−2 7.733−2 8.452−2 1.263−1 9.668−2 1.288−1 5.168−2 6.460−2 7.537−1 9.988+0 1.651−1 4.854−1 1.472−1 2.943−2 2.757−1 3.587−2 2.245−1 3.951−2 2.801−1 3.567−2 1.789−1 3.612−2 2.436+0 2.034+1 3.384−1 1.013+0 6.665−2 3.949−2 5.858−1 9.630−2 4.537−1 1.281−1 5.151−1 1.082−1 3.241−1 5.360−1 1.295+1 3.763−1 2.744−2 4.468−2 2.842−2 5.885−1 4.067−2 1.189+0 5.786−2 7.660−1 5.926−2 1.553+0 2.579+1 4.366−2 1.757−2 9.281−2 4.115−2 9.051−1 1.483−1 1.733+0 1.513−1 1.090+0
4.034−3 3.270−3 1.017−2 9.357−3 6.047−2 2.602−2 2.159−1 1.344−2 6.038−2 5.958+0 1.196+1 5.320−1 8.534−1 1.022−1 1.446−1 2.788−1 4.912−2 9.109−2 9.018−2 1.347−1 9.746−2 1.299−1 5.182−2 6.477−2 7.148−1 1.092+1 1.477−1 4.563−1 1.188−1 3.072−2 2.810−1 3.763−2 2.574−1 3.967−2 2.975−1 3.533−2 1.797−1 3.413−2 2.633+0 2.203+1 2.921−1 9.269−1 6.769−2 4.085−2 5.993−1 1.034−1 5.152−1 1.327−1 5.452−1 1.058−1 3.239−1 4.732−1 1.517+1 2.984−1 2.491−2 4.489−2 2.781−2 5.995−1 3.961−2 1.307+0 5.453−2 8.056−1 5.503−2 1.693+0 2.872+1 3.911−2 1.674−2 9.275−2 4.009−2 9.211−1 1.532−1 1.902+0 1.510−1 1.144+0
3.468−3 2.848−3 9.336−3 8.247−3 5.946−2 2.441−2 2.248−1 1.253−2 6.307−2 6.512+0 1.286+1 5.149−1 8.129−1 8.724−2 1.222−1 2.847−1 5.983−2 1.119−1 9.737−2 1.454−1 9.812−2 1.308−1 5.233−2 6.541−2 6.749−1 1.201+1 1.324−1 4.286−1 9.297−2 3.436−2 2.873−1 4.014−2 3.047−1 3.981−2 3.191−1 3.518−2 1.804−1 3.225−2 2.853+0 2.393+1 2.486−1 8.437−1 7.443−2 4.322−2 6.154−1 1.134−1 6.032−1 1.389−1 5.827−1 1.035−1 3.237−1 4.148−1 1.747+1 2.271−1 2.366−2 4.710−2 2.770−2 6.120−1 3.883−2 1.473+0 5.128−2 8.546−1 5.113−2 1.826+0 3.121+1 3.676−2 1.613−2 9.618−2 3.932−2 9.395−1 1.616−1 2.140+0 1.521−1 1.210+0
3.024−3 2.444−3 8.628−3 7.125−3 5.854−2 2.297−2 2.375−1 1.177−2 6.713−2 7.119+0 1.388+1 4.989−1 7.769−1 7.550−2 1.047−1 2.911−1 7.526−2 1.414−1 1.059−1 1.581−1 9.861−2 1.314−1 5.326−2 6.657−2 6.396−1 1.317+1 1.213−1 4.051−1 7.240−2 4.064−2 2.940−1 4.331−2 3.697−1 3.993−2 3.441−1 3.528−2 1.809−1 3.062−2 3.088+0 2.596+1 2.132−1 7.741−1 8.722−2 4.640−2 6.330−1 1.272−1 7.243−1 1.463−1 6.263−1 1.015−1 3.235−1 3.673−1 1.964+1 1.705−1 2.331−2 5.164−2 2.814−2 6.252−1 3.845−2 1.698+0 4.836−2 9.109−1 4.788−2 1.951+0 3.343+1 3.593−2 1.568−2 1.037−1 3.896−2 9.592−1 1.748−1 2.462+0 1.548−1 1.287+0
2.685−3 2.080−3 8.105−3 6.082−3 5.781−2 2.191−2 2.552−1 1.126−2 7.266−2 7.759+0 1.501+1 4.851−1 7.473−1 6.727−2 9.236−2 2.975−1 9.621−2 1.813−1 1.153−1 1.720−1 9.898−2 1.319−1 5.452−2 6.815−2 6.104−1 1.436+1 1.142−1 3.864−1 5.732−2 4.980−2 3.007−1 4.692−2 4.553−1 4.002−2 3.710−1 3.560−2 1.815−1 2.937−2 3.330+0 2.807+1 1.866−1 7.197−1 1.065−1 5.013−2 6.507−1 1.453−1 8.837−1 1.545−1 6.733−1 1.000−1 3.236−1 3.314−1 2.162+1 1.291−1 2.356−2 5.879−2 2.919−2 6.382−1 3.850−2 1.990+0 4.597−2 9.710−1 4.547−2 2.068+0 3.552+1 3.612−2 1.538−2 1.159−1 3.903−2 9.787−1 1.935−1 2.883+0 1.587−1 1.370+0
2.438−3 1.774−3 7.815−3 5.189−3 5.732−2 2.142−2 2.786−1 1.103−2 7.946−2 8.415+0 1.621+1 4.735−1 7.237−1 6.200−2 8.444−2 3.034−1 1.231−1 2.323−1 1.247−1 1.863−1 9.931−2 1.323−1 5.597−2 6.997−2 5.865−1 1.555+1 1.106−1 3.716−1 4.684−2 6.196−2 3.067−1 5.066−2 5.628−1 4.013−2 3.974−1 3.608−2 1.822−1 2.851−2 3.573+0 3.020+1 1.674−1 6.781−1 1.324−1 5.402−2 6.672−1 1.681−1 1.084+0 1.628−1 7.194−1 9.912−2 3.241−1 3.052−1 2.340+1 1.007−1 2.416−2 6.868−2 3.083−2 6.500−1 3.888−2 2.354+0 4.417−2 1.030+0 4.389−2 2.177+0 3.750+1 3.693−2 1.519−2 1.330−1 3.943−2 9.966−1 2.183−1 3.408+0 1.635−1 1.451+0
2.268−3 1.530−3 7.752−3 4.472−3 5.692−2 2.149−2 3.068−1 1.104−2 8.676−2 9.042+0 1.739+1 4.625−1 7.030−1 5.881−2 7.960−2 3.076−1 1.548−1 2.923−1 1.329−1 1.988−1 9.945−2 1.325−1 5.729−2 7.163−2 5.649−1 1.667+1 1.091−1 3.591−1 3.975−2 7.652−2 3.110−1 5.402−2 6.875−1 4.019−2 4.197−1 3.653−2 1.826−1 2.796−2 3.799+0 3.219+1 1.535−1 6.445−1 1.635−1 5.750−2 6.797−1 1.943−1 1.316+0 1.698−1 7.579−1 9.852−2 3.244−1 2.855−1 2.492+1 8.188−2 2.482−2 8.075−2 3.285−2 6.582−1 3.930−2 2.772+0 4.283−2 1.079+0 4.289−2 2.273+0 3.927+1 3.787−2 1.508−2 1.540−1 3.987−2 1.009+0 2.477−1 4.012+0 1.678−1 1.518+0
2.122−3 1.329−3 7.724−3 3.883−3 5.559−2 2.161−2 3.302−1 1.098−2 9.181−2 9.423+0 1.812+1 4.446−1 6.734−1 5.604−2 7.551−2 3.046−1 1.839−1 3.472−1 1.366−1 2.045−1 9.766−2 1.301−1 5.727−2 7.160−2 5.365−1 1.731+1 1.069−1 3.427−1 3.458−2 8.983−2 3.079−1 5.562−2 7.988−1 3.948−2 4.280−1 3.622−2 1.795−1 2.714−2 3.921+0 3.330+1 1.411−1 6.069−1 1.921−1 5.910−2 6.754−1 2.165−1 1.523+0 1.715−1 7.711−1 9.639−2 3.187−1 2.664−1 2.567+1 6.891−2 2.494−2 9.159−2 3.424−2 6.508−1 3.887−2 3.135+0 4.115−2 1.093+0 4.154−2 2.309+0 4.002+1 3.802−2 1.474−2 1.727−1 3.945−2 9.977−1 2.727−1 4.536+0 1.678−1 1.537+0
2.097−3 1.328−3 7.911−3 3.873−3 5.870−2 2.238−2 3.454−1 1.156−2 9.638−2 9.730+0 1.864+1 4.599−1 6.914−1 5.384−2 7.196−2 3.236−1 1.974−1 3.751−1 1.437−1 2.140−1 1.113−1 1.484−1 6.053−2 7.568−2 5.605−1 1.805+1 1.052−1 3.512−1 2.858−2 9.956−2 3.349−1 6.155−2 8.577−1 4.457−2 4.408−1 3.801−2 1.902−1 2.837−2 3.906+0 3.329+1 1.362−1 6.198−1 2.108−1 6.537−2 7.351−1 2.339−1 1.629+0 1.778−1 7.951−1 1.017−1 3.375−1 2.674−1 2.785+1 5.159−2 2.450−2 9.748−2 3.770−2 6.828−1 4.217−2 3.330+0 4.506−2 1.139+0 4.380−2 2.372+0 4.466+1 3.707−2 1.629−2 1.832−1 4.286−2 1.047+0 2.886−1 4.804+0 1.756−1 1.603+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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69
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.863−1 7.219−3 1.471−2 1.521−2 5.643−2 2.848−2 8.084−1 5.900−2 4.371+0 1.068−1 9.644−3 8.678−3 3.115−2 2.288−2 9.052−2 5.908−2 1.098+0 2.731−1 5.707+0 1.354+1 2.675+1 1.402+0 2.102+0 1.604−1 2.144−1 4.497−2 5.638−2 1.644+0 2.599+1 2.196−1 1.524+0 1.059−1 9.634−2 3.051−2 5.652+0 4.823+1 5.719−1 2.696+0 7.240−2 1.793−1 8.347−1 3.486+1 1.534−1 1.262+0 7.603−2 2.683+0 5.763+1 2.243−1 1.781+0 5.436−1 2.870+1 1.435−1 1.456+0 3.882+1 5.095−1
1.012+0 1.388−2 1.810−2 1.799−2 6.745−2 2.979−2 7.735−1 5.774−2 4.289+0 1.032−1 1.835−2 1.103−2 3.682−2 2.354−2 1.071−1 5.790−2 1.050+0 2.664−1 5.601+0 1.532+1 2.924+1 1.392+0 2.093+0 1.793−1 2.388−1 4.757−2 5.947−2 1.579+0 3.100+1 2.469−1 1.495+0 1.094−1 1.088−1 3.040−2 7.162+0 5.982+1 5.672−1 2.639+0 7.628−2 2.002−1 8.094−1 6.287+1 1.641−1 1.234+0 7.362−2 5.906+0 9.828+1 2.189−1 1.742+0 5.228−1 6.093+1 1.330−1 4.190+0 8.598+1 4.569−1
8.127−1 1.114−2 1.668−2 1.583−2 6.561−2 2.654−2 7.776−1 5.134−2 4.583+0 9.110−2 1.476−2 9.318−3 3.382−2 2.056−2 1.030−1 5.147−2 1.054+0 2.647−1 5.978+0 1.666+1 3.171+1 1.372+0 2.063+0 1.805−1 2.405−1 4.558−2 5.699−2 1.547+0 3.371+1 2.506−1 1.465+0 1.072−1 1.079−1 2.801−2 7.784+0 6.516+1 5.554−1 2.585+0 7.276−2 1.970−1 7.919−1 6.860+1 1.614−1 1.204+0 6.694−2 6.367+0 1.069+2 2.080−1 1.697+0 5.005−1 6.605+1 1.198−1 4.396+0 9.286+1 4.122−1
6.275−1 9.184−3 1.568−2 1.394−2 6.463−2 2.342−2 7.833−1 4.513−2 4.990+0 7.929−2 1.220−2 7.846−3 3.147−2 1.767−2 1.002−1 4.525−2 1.059+0 2.676−1 6.505+0 1.812+1 3.446+1 1.349+0 2.029+0 1.824−1 2.432−1 4.381−2 5.479−2 1.514+0 3.662+1 2.553−1 1.434+0 1.053−1 1.074−1 2.591−2 8.434+0 7.079+1 5.433−1 2.527+0 6.981−2 1.948−1 7.740−1 7.424+1 1.598−1 1.174+0 6.095−2 6.811+0 1.154+2 1.979−1 1.653+0 4.789−1 7.098+1 1.082−1 4.589+0 9.944+1 3.708−1
4.773−1 7.786−3 1.502−2 1.237−2 6.494−2 2.069−2 7.899−1 3.960−2 5.537+0 6.870−2 1.036−2 6.627−3 2.973−2 1.508−2 9.940−2 3.972−2 1.067+0 2.770−1 7.213+0 1.966+1 3.742+1 1.325+0 1.992+0 1.849−1 2.466−1 4.237−2 5.299−2 1.479+0 3.965+1 2.606−1 1.400+0 1.036−1 1.075−1 2.424−2 9.094+0 7.656+1 5.311−1 2.467+0 6.760−2 1.937−1 7.561−1 7.967+1 1.593−1 1.143+0 5.598−2 7.229+0 1.234+2 1.889−1 1.608+0 4.592−1 7.565+1 9.895−2 4.767+0 1.056+2 3.348−1
3.649−1 6.805−3 1.465−2 1.115−2 6.686−2 1.853−2 7.967−1 3.509−2 6.244+0 5.993−2 9.064−3 5.666−3 2.858−2 1.292−2 1.011−1 3.520−2 1.074+0 2.945−1 8.131+0 2.125+1 4.052+1 1.299+0 1.952+0 1.880−1 2.508−1 4.127−2 5.163−2 1.441+0 4.272+1 2.665−1 1.363+0 1.023−1 1.080−1 2.304−2 9.751+0 8.234+1 5.189−1 2.403+0 6.616−2 1.938−1 7.380−1 8.485+1 1.600−1 1.112+0 5.212−2 7.622+0 1.310+2 1.812−1 1.563+0 4.416−1 8.004+1 9.214−2 4.933+0 1.114+2 3.053−1
2.850−1 6.140−3 1.451−2 1.026−2 7.052−2 1.698−2 8.030−1 3.165−2 7.120+0 5.319−2 8.187−3 4.952−3 2.792−2 1.125−2 1.056−1 3.178−2 1.082+0 3.208−1 9.272+0 2.287+1 4.368+1 1.272+0 1.911+0 1.916−1 2.556−1 4.050−2 5.067−2 1.400+0 4.578+1 2.725−1 1.324+0 1.013−1 1.089−1 2.226−2 1.040+1 8.804+1 5.061−1 2.333+0 6.538−2 1.946−1 7.190−1 8.974+1 1.615−1 1.080+0 4.930−2 7.987+0 1.381+2 1.744−1 1.517+0 4.258−1 8.413+1 8.756−2 5.086+0 1.168+2 2.818−1
2.296−1 5.699−3 1.448−2 9.636−3 7.552−2 1.598−2 8.062−1 2.913−2 8.120+0 4.827−2 7.604−3 4.442−3 2.755−2 1.001−2 1.123−1 2.926−2 1.085+0 3.540−1 1.058+1 2.438+1 4.668+1 1.245+0 1.872+0 1.952−1 2.602−1 3.991−2 4.993−2 1.352+0 4.862+1 2.771−1 1.278+0 1.002−1 1.094−1 2.175−2 1.098+1 9.326+1 4.911−1 2.252+0 6.486−2 1.952−1 6.970−1 9.404+1 1.629−1 1.043+0 4.719−2 8.300+0 1.443+2 1.678−1 1.465+0 4.101−1 8.766+1 8.452−2 5.213+0 1.214+2 2.628−1
1.897−1 5.328−3 1.424−2 9.055−3 7.951−2 1.513−2 7.919−1 2.688−2 8.955+0 4.417−2 7.112−3 4.031−3 2.687−2 8.997−3 1.176−1 2.703−2 1.065+0 3.820−1 1.167+1 2.522+1 4.838+1 1.203+0 1.813+0 1.950−1 2.599−1 3.879−2 4.853−2 1.281+0 5.010+1 2.749−1 1.210+0 9.719−2 1.076−1 2.103−2 1.126+1 9.588+1 4.667−1 2.130+0 6.325−2 1.915−1 6.618−1 9.575+1 1.608−1 9.869−1 4.484−2 8.392+0 1.466+2 1.588−1 1.386+0 3.882−1 8.883+1 8.106−2 5.212+0 1.228+2 2.434−1
1.499−1 5.418−3 1.450−2 9.580−3 7.677−2 1.570−2 8.185−1 2.864−2 9.442+0 4.784−2 7.244−3 4.322−3 2.764−2 9.829−3 1.130−1 2.878−2 1.102+0 4.002−1 1.227+1 2.274+1 4.964+1 1.176+0 1.767+0 2.236−1 2.998−1 4.176−2 5.235−2 1.307+0 4.493+1 3.575−1 1.253+0 1.124−1 1.337−1 2.398−2 1.043+1 8.690+1 4.943−1 2.219+0 7.350−2 2.294−1 6.956−1 9.707+1 1.770−1 1.038+0 4.908−2 7.361+0 1.736+2 1.695−1 1.459+0 4.123−1 8.355+1 8.950−2 4.430+0 1.211+2 2.689−1
70
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 27 Effective collision strengths for transitions in V XXI. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.148−1 4.183−1 1.893−2 5.452−3 1.024−2 1.451−2 2.169−2 3.788−3 1.362−3 2.599−3 2.619−3 3.929−3 1.558−3 2.070−3 1.477−3 5.793−4 1.107−3 1.009−3 1.514−3 8.223−4 1.093−3 1.063−4 1.325−4 3.731−2 1.339−3 2.057−2 5.387−3 6.972−2 9.939−3 4.246−4 4.262−3 1.760−3 1.279−2 3.089−3 2.147−3 1.287−3 2.008−4 1.706−3 8.436−4 4.797−3 1.443−3 1.139−3 7.778−4 1.054−4 1.034−4 2.712−3 5.530−3 4.687−2 2.651−2 1.365−1 8.459−4 1.778−3 1.032−2 6.340−3 2.588−2 2.334−3 4.728−3 3.986−4 8.494−4 4.255−3 2.716−3 9.910−3 1.357−3 2.564−3 1.787−4 2.521−4 1.408+0 2.720+0 1.005−1 1.509−1 8.873−2 1.500−2 2.788−2
2.194−1 4.271−1 2.107−2 7.020−3 1.333−2 1.581−2 2.383−2 4.225−3 1.897−3 3.673−3 3.101−3 4.700−3 2.043−3 2.739−3 1.398−3 6.773−4 1.303−3 1.079−3 1.622−3 8.705−4 1.158−3 1.154−4 1.436−4 5.584−2 6.510−3 2.158−2 9.306−3 7.104−2 1.571−2 1.349−3 4.604−3 2.736−3 1.378−2 4.245−3 3.298−3 2.384−3 3.529−4 1.577−3 9.180−4 5.031−3 1.529−3 1.261−3 8.080−4 1.218−4 1.046−4 1.318−2 9.801−3 5.538−2 3.399−2 1.437−1 2.550−3 2.837−3 1.185−2 8.038−3 2.866−2 4.237−3 7.573−3 7.192−4 9.340−4 4.086−3 2.883−3 1.042−2 1.445−3 2.817−3 1.879−4 2.831−4 1.399+0 2.726+0 1.314−1 2.004−1 9.375−2 1.845−2 3.484−2
2.301−1 4.472−1 2.051−2 7.139−3 1.360−2 1.596−2 2.403−2 4.045−3 1.831−3 3.541−3 2.991−3 4.522−3 1.899−3 2.539−3 1.394−3 6.857−4 1.322−3 1.065−3 1.602−3 8.499−4 1.131−3 1.076−4 1.339−4 6.110−2 5.164−3 2.135−2 8.596−3 7.371−2 1.471−2 1.091−3 4.393−3 2.403−3 1.396−2 3.784−3 3.072−3 2.008−3 3.205−4 1.555−3 8.606−4 5.139−3 1.427−3 1.263−3 7.452−4 1.163−4 9.448−5 1.046−2 8.999−3 5.330−2 3.327−2 1.477−1 2.095−3 2.478−3 1.115−2 7.500−3 2.862−2 3.654−3 6.907−3 6.512−4 8.742−4 3.989−3 2.778−3 1.054−2 1.362−3 2.774−3 1.718−4 2.665−4 1.489+0 2.887+0 1.280−1 1.947−1 9.253−2 1.967−2 3.706−2
2.424−1 4.704−1 2.009−2 7.374−3 1.405−2 1.606−2 2.416−2 3.915−3 1.813−3 3.502−3 2.898−3 4.375−3 1.771−3 2.364−3 1.398−3 7.057−4 1.363−3 1.050−3 1.580−3 8.272−4 1.101−3 9.884−5 1.230−4 6.216−2 4.127−3 2.101−2 7.657−3 7.731−2 1.311−2 8.908−4 4.220−3 2.089−3 1.433−2 3.306−3 2.916−3 1.656−3 2.909−4 1.535−3 7.943−4 5.304−3 1.298−3 1.278−3 6.698−4 1.110−4 8.286−5 8.377−3 7.995−3 5.111−2 3.202−2 1.532−1 1.734−3 2.146−3 1.053−2 6.978−3 2.892−2 3.120−3 6.379−3 5.902−4 8.063−4 3.885−3 2.654−3 1.074−2 1.266−3 2.748−3 1.538−4 2.495−4 1.607+0 3.099+0 1.218−1 1.848−1 9.183−2 2.208−2 4.156−2
2.569−1 4.979−1 1.985−2 7.883−3 1.501−2 1.631−2 2.451−2 3.843−3 1.867−3 3.603−3 2.841−3 4.284−3 1.672−3 2.231−3 1.409−3 7.438−4 1.438−3 1.037−3 1.561−3 8.053−4 1.072−3 8.977−5 1.117−4 5.874−2 3.368−3 2.070−2 6.694−3 8.267−2 1.132−2 7.435−4 4.097−3 1.809−3 1.500−2 2.835−3 2.864−3 1.347−3 2.642−4 1.518−3 7.214−4 5.552−3 1.149−3 1.318−3 5.862−4 1.069−4 7.057−5 6.865−3 6.987−3 4.918−2 3.091−2 1.617−1 1.465−3 1.856−3 1.003−2 6.525−3 2.976−2 2.678−3 6.066−3 5.362−4 7.323−4 3.780−3 2.520−3 1.107−2 1.167−3 2.758−3 1.353−4 2.341−4 1.753+0 3.364+0 1.149−1 1.740−1 9.188−2 2.611−2 4.914−2
2.751−1 5.320−1 1.983−2 8.821−3 1.679−2 1.684−2 2.529−2 3.828−3 2.014−3 3.885−3 2.828−3 4.262−3 1.607−3 2.142−3 1.428−3 8.087−4 1.566−3 1.030−3 1.551−3 7.874−4 1.049−3 8.130−5 1.012−4 5.232−2 2.874−3 2.053−2 5.849−3 9.059−2 9.614−3 6.419−4 4.020−3 1.569−3 1.605−2 2.392−3 2.929−3 1.088−3 2.423−4 1.506−3 6.463−4 5.916−3 9.892−4 1.391−3 5.014−4 1.048−4 5.863−5 5.901−3 6.111−3 4.776−2 3.043−2 1.751−1 1.279−3 1.609−3 9.653−3 6.186−3 3.133−2 2.342−3 5.998−3 4.925−4 6.566−4 3.681−3 2.398−3 1.161−2 1.076−3 2.826−3 1.180−4 2.225−4 1.919+0 3.670+0 1.088−1 1.644−1 9.261−2 3.208−2 6.045−2
2.973−1 5.733−1 2.001−2 1.032−2 1.964−2 1.770−2 2.655−2 3.858−3 2.270−3 4.384−3 2.863−3 4.314−3 1.573−3 2.096−3 1.454−3 9.091−4 1.763−3 1.032−3 1.556−3 7.763−4 1.034−3 7.419−5 9.244−5 4.502−2 2.631−3 2.051−2 5.183−3 1.018−1 8.140−3 5.813−4 3.985−3 1.371−3 1.757−2 1.992−3 3.111−3 8.806−4 2.272−4 1.499−3 5.747−4 6.428−3 8.324−4 1.502−3 4.226−4 1.050−4 4.794−5 5.453−3 5.430−3 4.692−2 3.091−2 1.946−1 1.172−3 1.407−3 9.397−3 5.997−3 3.379−2 2.110−3 6.171−3 4.635−4 5.850−4 3.598−3 2.308−3 1.241−2 1.004−3 2.967−3 1.032−4 2.157−4 2.097+0 4.005+0 1.039−1 1.568−1 9.377−2 4.021−2 7.587−2
3.215−1 6.188−1 2.026−2 1.235−2 2.353−2 1.874−2 2.811−2 3.903−3 2.627−3 5.078−3 2.928−3 4.412−3 1.557−3 2.076−3 1.479−3 1.042−3 2.024−3 1.042−3 1.571−3 7.692−4 1.025−3 6.862−5 8.556−5 3.831−2 2.599−3 2.053−2 4.691−3 1.157−1 6.941−3 5.553−4 3.964−3 1.211−3 1.946−2 1.649−3 3.371−3 7.196−4 2.199−4 1.492−3 5.106−4 7.053−3 6.897−4 1.640−3 3.548−4 1.066−4 3.900−5 5.442−3 4.934−3 4.641−2 3.230−2 2.195−1 1.133−3 1.245−3 9.206−3 5.955−3 3.697−2 1.967−3 6.516−3 4.505−4 5.210−4 3.521−3 2.259−3 1.344−2 9.541−4 3.162−3 9.137−5 2.125−4 2.268+0 4.331+0 9.984−2 1.506−1 9.472−2 5.006−2 9.454−2
3.387−1 6.511−1 2.007−2 1.428−2 2.724−2 1.935−2 2.902−2 3.856−3 2.950−3 5.712−3 2.934−3 4.422−3 1.517−3 2.023−3 1.463−3 1.158−3 2.252−3 1.031−3 1.554−3 7.473−4 9.965−4 6.328−5 7.895−5 3.251−2 2.652−3 2.013−2 4.274−3 1.277−1 5.935−3 5.424−4 3.861−3 1.069−3 2.094−2 1.356−3 3.562−3 5.925−4 2.141−4 1.451−3 4.498−4 7.515−3 5.635−4 1.736−3 2.967−4 1.062−4 3.162−5 5.600−3 4.513−3 4.514−2 3.352−2 2.408−1 1.117−3 1.103−3 8.864−3 5.892−3 3.944−2 1.850−3 6.763−3 4.409−4 4.602−4 3.379−3 2.197−3 1.417−2 9.050−4 3.290−3 8.097−5 2.068−4 2.362+0 4.513+0 9.463−2 1.427−1 9.313−2 5.870−2 1.109−1
3.518−1 6.786−1 2.126−2 1.574−2 2.998−2 2.035−2 3.045−2 4.208−3 3.242−3 6.250−3 3.007−3 4.521−3 1.566−3 2.082−3 1.629−3 1.271−3 2.455−3 1.043−3 1.570−3 7.767−4 1.033−3 6.473−5 8.066−5 2.466−2 2.546−3 2.159−2 4.160−3 1.381−1 5.364−3 5.208−4 4.341−3 1.066−3 2.224−2 1.258−3 3.780−3 5.451−4 2.023−4 1.705−3 4.614−4 7.873−3 5.444−4 1.886−3 3.931−4 1.085−4 3.303−5 5.402−3 4.390−3 4.783−2 3.497−2 2.589−1 1.079−3 1.098−3 9.805−3 6.034−3 4.165−2 1.840−3 7.084−3 4.164−4 4.727−4 3.884−3 2.250−3 1.479−2 9.556−4 3.542−3 8.313−5 2.111−4 2.494+0 4.866+0 9.473−2 1.426−1 9.930−2 6.536−2 1.239−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
71
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.724−2 5.545−2 3.749−2 4.996−2 1.670−2 3.407−3 6.447−3 7.790−3 1.165−2 4.314−3 5.763−3 6.704−3 8.368−3 1.650−1 2.012+0 2.540−2 5.854−3 9.431−2 1.329−2 1.182−1 1.705−2 1.242−1 1.808−2 1.400−3 1.833−2 3.649−3 2.459−2 4.840−3 1.315−2 4.145−3 1.592−2 5.169−3 4.670−1 3.841+0 1.215−2 1.405−2 2.033−1 4.589−2 2.346−1 5.947−2 2.288−1 2.798−3 3.772−3 4.047−2 1.099−2 4.940−2 9.087−3 2.545−2 1.244−2 3.060−2 1.189−1 5.043−3 9.513−3 9.687−3 1.822−1 2.302−2 8.064−1 4.061−2 1.635−3 2.950−3 3.702−3 3.493−2 8.397−3 1.270−1 1.348−2 3.478−2 7.789−3 7.606−3 6.578−3 2.239−2 2.312−2 2.853−1 1.017−1 1.175+0
3.935−2 6.600−2 4.517−2 7.107−2 1.562−2 3.950−3 7.457−3 7.967−3 1.194−2 5.137−3 6.867−3 7.115−3 8.892−3 1.997−1 2.041+0 8.517−2 1.366−2 9.051−2 1.752−2 1.189−1 2.519−2 1.256−1 3.193−2 2.146−3 1.617−2 3.597−3 2.635−2 5.220−3 1.396−2 4.679−3 1.637−2 5.466−3 5.335−1 3.882+0 2.775−2 1.986−2 2.023−1 5.760−2 2.720−1 7.712−2 3.017−1 4.430−3 3.768−3 3.599−2 1.181−2 5.291−2 1.003−2 2.732−2 1.301−2 3.161−2 3.361−1 1.400−2 2.140−2 2.316−2 1.897−1 4.364−2 8.044−1 7.315−2 2.371−3 4.028−3 4.573−3 3.411−2 9.158−3 1.299−1 1.435−2 3.608−2 7.930−3 2.234−2 1.664−2 5.633−2 4.416−2 3.580−1 1.431−1 1.313+0
4.020−2 6.572−2 4.359−2 6.667−2 1.579−2 4.269−3 8.086−3 8.180−3 1.226−2 4.894−3 6.542−3 6.963−3 8.702−3 1.928−1 2.153+0 7.790−2 1.179−2 9.039−2 1.633−2 1.287−1 2.271−2 1.292−1 2.775−2 2.040−3 1.633−2 3.524−3 2.809−2 4.916−3 1.409−2 4.258−3 1.679−2 5.064−3 5.499−1 4.087+0 2.438−2 1.832−2 2.005−1 5.634−2 2.822−1 7.288−2 2.928−1 4.201−3 3.680−3 3.628−2 1.179−2 5.588−2 9.520−3 2.723−2 1.261−2 3.205−2 3.052−1 1.122−2 1.837−2 1.911−2 1.868−1 3.657−2 8.445−1 6.112−2 2.096−3 3.748−3 4.103−3 3.378−2 8.224−3 1.346−1 1.271−2 3.757−2 7.032−3 1.795−2 1.351−2 4.767−2 3.703−2 3.395−1 1.319−1 1.341+0
4.176−2 6.648−2 4.222−2 6.251−2 1.604−2 4.777−3 9.074−3 8.481−3 1.271−2 4.637−3 6.198−3 6.836−3 8.543−3 1.831−1 2.319+0 6.636−2 1.097−2 9.073−2 1.554−2 1.438−1 2.048−2 1.349−1 2.388−2 2.019−3 1.654−2 3.475−3 3.062−2 4.587−3 1.432−2 3.806−3 1.735−2 4.638−3 5.765−1 4.417+0 2.296−2 1.723−2 1.999−1 5.643−2 3.023−1 6.967−2 2.871−1 4.162−3 3.623−3 3.670−2 1.191−2 6.027−2 8.992−3 2.727−2 1.222−2 3.270−2 2.571−1 9.127−3 1.617−2 1.562−2 1.845−1 3.005−2 9.054−1 4.991−2 1.861−3 3.509−3 3.624−3 3.349−2 7.208−3 1.413−1 1.092−2 3.983−2 6.087−3 1.455−2 1.079−2 4.056−2 3.043−2 3.218−1 1.228−1 1.397+0
4.416−2 6.877−2 4.124−2 5.928−2 1.634−2 5.540−3 1.055−2 8.877−3 1.331−2 4.393−3 5.872−3 6.766−3 8.456−3 1.732−1 2.535+0 5.441−2 1.114−2 9.156−2 1.522−2 1.658−1 1.870−2 1.428−1 2.075−2 2.094−3 1.680−2 3.460−3 3.417−2 4.262−3 1.466−2 3.364−3 1.801−2 4.228−3 6.151−1 4.854+0 2.351−2 1.672−2 2.009−1 5.854−2 3.366−1 6.803−2 2.878−1 4.329−3 3.607−3 3.723−2 1.224−2 6.655−2 8.510−3 2.750−2 1.189−2 3.355−2 2.069−1 7.639−3 1.488−2 1.290−2 1.833−1 2.462−2 9.930−1 4.039−2 1.664−3 3.331−3 3.172−3 3.327−2 6.196−3 1.507−1 9.137−3 4.299−2 5.186−3 1.209−2 8.624−3 3.558−2 2.493−2 3.083−1 1.177−1 1.496+0
4.731−2 7.251−2 4.065−2 5.708−2 1.669−2 6.623−3 1.265−2 9.365−3 1.404−2 4.189−3 5.599−3 6.775−3 8.467−3 1.646−1 2.783+0 4.432−2 1.227−2 9.278−2 1.537−2 1.961−1 1.739−2 1.526−1 1.846−2 2.279−3 1.709−2 3.488−3 3.899−2 3.970−3 1.511−2 2.973−3 1.872−2 3.870−3 6.622−1 5.351+0 2.606−2 1.674−2 2.032−1 6.302−2 3.880−1 6.799−2 2.950−1 4.731−3 3.639−3 3.786−2 1.286−2 7.517−2 8.124−3 2.796−2 1.164−2 3.452−2 1.634−1 6.642−3 1.450−2 1.093−2 1.832−1 2.041−2 1.112+0 3.283−2 1.508−3 3.240−3 2.779−3 3.315−2 5.273−3 1.634−1 7.513−3 4.706−2 4.407−3 1.041−2 6.980−3 3.280−2 2.067−2 2.993−1 1.172−1 1.646+0
5.097−2 7.730−2 4.040−2 5.575−2 1.705−2 8.073−3 1.546−2 9.917−3 1.487−2 4.040−3 5.400−3 6.866−3 8.580−3 1.577−1 3.043+0 3.679−2 1.433−2 9.422−2 1.587−2 2.354−1 1.648−2 1.635−1 1.693−2 2.584−3 1.738−2 3.560−3 4.523−2 3.729−3 1.563−2 2.658−3 1.942−2 3.584−3 7.136−1 5.866+0 3.057−2 1.719−2 2.064−1 6.996−2 4.577−1 6.922−2 3.071−1 5.386−3 3.716−3 3.854−2 1.385−2 8.643−2 7.860−3 2.860−2 1.149−2 3.551−2 1.295−1 6.021−3 1.495−2 9.630−3 1.840−1 1.733−2 1.265+0 2.714−2 1.395−3 3.249−3 2.469−3 3.314−2 4.500−3 1.797−1 6.148−3 5.184−2 3.792−3 9.357−3 5.785−3 3.206−2 1.755−2 2.942−1 1.215−1 1.852+0
5.451−2 8.212−2 4.023−2 5.487−2 1.732−2 9.813−3 1.883−2 1.044−2 1.566−2 3.932−3 5.255−3 6.989−3 8.735−3 1.520−1 3.289+0 3.158−2 1.710−2 9.528−2 1.651−2 2.815−1 1.583−2 1.736−1 1.595−2 2.983−3 1.757−2 3.648−3 5.249−2 3.533−3 1.612−2 2.418−3 1.994−2 3.361−3 7.624−1 6.341+0 3.661−2 1.781−2 2.091−1 7.871−2 5.411−1 7.090−2 3.200−1 6.241−3 3.811−3 3.905−2 1.510−2 9.961−2 7.680−3 2.923−2 1.137−2 3.625−2 1.046−1 5.649−3 1.602−2 8.841−3 1.843−1 1.514−2 1.442+0 2.300−2 1.315−3 3.341−3 2.240−3 3.306−2 3.889−3 1.983−1 5.071−3 5.664−2 3.334−3 8.712−3 4.935−3 3.286−2 1.534−2 2.905−1 1.294−1 2.097+0
5.609−2 8.419−2 3.919−2 5.304−2 1.707−2 1.129−2 2.169−2 1.060−2 1.591−2 3.771−3 5.040−3 6.942−3 8.676−3 1.443−1 3.418+0 2.769−2 1.959−2 9.369−2 1.671−2 3.199−1 1.502−2 1.775−1 1.500−2 3.323−3 1.726−2 3.644−3 5.826−2 3.309−3 1.610−2 2.201−3 1.979−2 3.127−3 7.859−1 6.587+0 4.203−2 1.798−2 2.061−1 8.573−2 6.108−1 7.082−2 3.235−1 6.972−3 3.809−3 3.843−2 1.601−2 1.100−1 7.390−3 2.902−2 1.100−2 3.583−2 8.593−2 5.318−3 1.698−2 8.239−3 1.800−1 1.338−2 1.579+0 1.977−2 1.235−3 3.398−3 2.041−3 3.216−2 3.373−3 2.113−1 4.209−3 5.932−2 2.955−3 8.157−3 4.272−3 3.374−2 1.357−2 2.811−1 1.357−1 2.289+0
5.988−2 8.924−2 4.039−2 5.384−2 1.887−2 1.268−2 2.435−2 1.110−2 1.661−2 3.717−3 4.969−3 7.316−3 9.135−3 1.468−1 3.648+0 2.193−2 2.180−2 1.023−1 1.828−2 3.526−1 1.552−2 1.886−1 1.475−2 3.749−3 1.997−2 4.090−3 6.274−2 3.400−3 1.641−2 2.208−3 2.088−2 3.274−3 8.381−1 7.057+0 4.645−2 1.951−2 2.248−1 9.264−2 6.671−1 7.377−2 3.379−1 7.824−3 4.263−3 4.417−2 1.703−2 1.181−1 7.500−3 2.957−2 1.156−2 3.771−2 6.485−2 5.099−3 1.739−2 7.879−3 1.882−1 1.266−2 1.706+0 1.847−2 1.263−3 3.598−3 2.099−3 3.434−2 3.405−3 2.255−1 4.246−3 6.323−2 3.133−3 7.722−3 3.859−3 3.362−2 1.283−2 2.892−1 1.425−1 2.456+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
72
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.458−3 2.614−3 7.401−3 8.399−3 5.665−2 2.356−2 1.878−1 1.259−2 5.165−2 4.982+0 9.586+0 4.500−1 6.752−1 4.108−2 5.492−2 2.672−1 3.866−2 7.209−2 8.035−2 1.194−1 8.712−2 1.159−1 4.479−2 5.594−2 5.788−1 8.924+0 7.421−2 3.529−1 3.383−2 2.086−2 2.834−1 3.617−2 2.118−1 3.832−2 2.645−1 3.087−2 1.572−1 2.976−2 1.949+0 1.648+1 1.443−1 6.306−1 4.360−2 3.854−2 6.056−1 9.258−2 4.294−1 1.175−1 4.845−1 9.264−2 2.839−1 2.900−1 1.032+1 6.738−2 1.762−2 3.186−2 2.441−2 5.821−1 3.718−2 1.130+0 5.317−2 7.215−1 5.347−2 7.965−1 1.433+1 2.664−2 1.546−2 6.952−2 3.759−2 8.930−1 1.391−1 1.648+0 1.400−1 1.026+0
3.644−3 3.249−3 9.861−3 9.205−3 5.571−2 2.473−2 1.923−1 1.294−2 5.356−2 5.254+0 9.998+0 4.860−1 8.106−1 1.088−1 1.515−1 2.505−1 4.173−2 7.702−2 7.862−2 1.173−1 8.753−2 1.167−1 4.724−2 5.904−2 6.259−1 9.257+0 1.610−1 4.624−1 1.255−1 2.797−2 2.517−1 3.292−2 2.176−1 3.576−2 2.583−1 3.252−2 1.618−1 3.284−2 2.212+0 1.966+1 3.001−1 1.008+0 5.958−2 3.642−2 5.376−1 9.076−2 4.396−1 1.178−1 4.756−1 9.811−2 2.932−1 4.994−1 1.225+1 3.136−1 2.307−2 4.225−2 2.588−2 5.385−1 3.714−2 1.128+0 5.266−2 7.061−1 5.423−2 1.564+0 2.526+1 3.504−2 1.583−2 8.695−2 3.782−2 8.275−1 1.389−1 1.653+0 1.391−1 1.005+0
3.204−3 2.872−3 9.052−3 8.259−3 5.481−2 2.330−2 1.983−1 1.210−2 5.529−2 5.686+0 1.078+1 4.723−1 7.724−1 9.310−2 1.285−1 2.550−1 4.943−2 9.178−2 8.414−2 1.255−1 8.816−2 1.175−1 4.749−2 5.936−2 6.005−1 1.012+1 1.423−1 4.306−1 1.002−1 2.976−2 2.569−1 3.476−2 2.520−1 3.587−2 2.750−1 3.228−2 1.624−1 3.109−2 2.404+0 2.110+1 2.569−1 9.039−1 6.332−2 3.795−2 5.501−1 9.806−2 5.040−1 1.224−1 5.046−1 9.597−2 2.930−1 4.368−1 1.422+1 2.444−1 2.155−2 4.280−2 2.545−2 5.486−1 3.626−2 1.250+0 4.968−2 7.442−1 5.054−2 1.661+0 2.717+1 3.277−2 1.511−2 8.761−2 3.688−2 8.425−1 1.445−1 1.829+0 1.393−1 1.057+0
2.834−3 2.493−3 8.313−3 7.234−3 5.390−2 2.185−2 2.072−1 1.129−2 5.808−2 6.180+0 1.170+1 4.583−1 7.340−1 7.910−2 1.083−1 2.605−1 6.054−2 1.129−1 9.102−2 1.357−1 8.873−2 1.182−1 4.803−2 6.004−2 5.756−1 1.112+1 1.260−1 4.002−1 7.816−2 3.357−2 2.628−1 3.721−2 2.992−1 3.597−2 2.954−1 3.217−2 1.629−1 2.937−2 2.620+0 2.270+1 2.183−1 8.072−1 7.148−2 4.031−2 5.648−1 1.081−1 5.922−1 1.283−1 5.401−1 9.386−2 2.927−1 3.802−1 1.622+1 1.847−1 2.091−2 4.517−2 2.544−2 5.600−1 3.557−2 1.415+0 4.667−2 7.903−1 4.696−2 1.754+0 2.897+1 3.181−2 1.457−2 9.134−2 3.616−2 8.595−1 1.531−1 2.064+0 1.404−1 1.120+0
2.527−3 2.132−3 7.698−3 6.218−3 5.308−2 2.060−2 2.199−1 1.063−2 6.216−2 6.725+0 1.273+1 4.456−1 7.010−1 6.835−2 9.297−2 2.664−1 7.592−2 1.421−1 9.901−2 1.475−1 8.919−2 1.189−1 4.889−2 6.111−2 5.536−1 1.218+1 1.142−1 3.748−1 6.108−2 3.968−2 2.689−1 4.021−2 3.624−1 3.606−2 3.187−1 3.225−2 1.635−1 2.786−2 2.849+0 2.444+1 1.876−1 7.286−1 8.463−2 4.336−2 5.807−1 1.214−1 7.101−1 1.352−1 5.806−1 9.203−2 2.926−1 3.350−1 1.811+1 1.389−1 2.090−2 4.965−2 2.591−2 5.719−1 3.523−2 1.633+0 4.393−2 8.424−1 4.391−2 1.845+0 3.075+1 3.179−2 1.417−2 9.875−2 3.581−2 8.773−1 1.658−1 2.374+0 1.428−1 1.191+0
2.287−3 1.811−3 7.267−3 5.293−3 5.245−2 1.975−2 2.374−1 1.021−2 6.755−2 7.302+0 1.384+1 4.347−1 6.743−1 6.093−2 8.244−2 2.721−1 9.636−2 1.807−1 1.076−1 1.603−1 8.957−2 1.193−1 5.002−2 6.253−2 5.348−1 1.327+1 1.066−1 3.549−1 4.877−2 4.839−2 2.749−1 4.356−2 4.443−1 3.614−2 3.433−1 3.252−2 1.641−1 2.670−2 3.081+0 2.627+1 1.649−1 6.688−1 1.034−1 4.685−2 5.964−1 1.388−1 8.630−1 1.427−1 6.236−1 9.068−2 2.928−1 3.011−1 1.983+1 1.062−1 2.133−2 5.655−2 2.694−2 5.833−1 3.526−2 1.911+0 4.168−2 8.970−1 4.162−2 1.936+0 3.252+1 3.242−2 1.390−2 1.105−1 3.584−2 8.946−1 1.836−1 2.773+0 1.463−1 1.265+0
2.112−3 1.546−3 7.059−3 4.519−3 5.204−2 1.945−2 2.601−1 1.005−2 7.400−2 7.895+0 1.499+1 4.252−1 6.529−1 5.624−2 7.578−2 2.773−1 1.222−1 2.296−1 1.160−1 1.728−1 8.992−2 1.198−1 5.130−2 6.413−2 5.186−1 1.435+1 1.026−1 3.395−1 4.031−2 5.980−2 2.801−1 4.694−2 5.460−1 3.625−2 3.671−1 3.292−2 1.648−1 2.592−2 3.309+0 2.814+1 1.487−1 6.241−1 1.281−1 5.040−2 6.107−1 1.604−1 1.053+0 1.501−1 6.650−1 8.989−2 2.935−1 2.767−1 2.139+1 8.409−2 2.199−2 6.597−2 2.850−2 5.935−1 3.559−2 2.255+0 4.002−2 9.491−1 4.010−2 2.025+0 3.426+1 3.339−2 1.374−2 1.267−1 3.618−2 9.100−1 2.070−1 3.267+0 1.504−1 1.337+0
1.989−3 1.338−3 7.044−3 3.907−3 5.162−2 1.962−2 2.864−1 1.008−2 8.054−2 8.440+0 1.606+1 4.151−1 6.329−1 5.332−2 7.164−2 2.803−1 1.518−1 2.851−1 1.229−1 1.830−1 8.993−2 1.198−1 5.233−2 6.542−2 5.019−1 1.532+1 1.005−1 3.264−1 3.457−2 7.302−2 2.832−1 4.975−2 6.601−1 3.623−2 3.857−1 3.323−2 1.650−1 2.537−2 3.511+0 2.983+1 1.367−1 5.882−1 1.567−1 5.333−2 6.201−1 1.844−1 1.266+0 1.558−1 6.971−1 8.924−2 2.935−1 2.582−1 2.267+1 6.952−2 2.260−2 7.706−2 3.030−2 5.992−1 3.586−2 2.636+0 3.874−2 9.890−1 3.906−2 2.100+0 3.574+1 3.428−2 1.362−2 1.459−1 3.645−2 9.186−1 2.337−1 3.818+0 1.536−1 1.391+0
1.867−3 1.162−3 6.992−3 3.392−3 5.001−2 1.963−2 3.047−1 9.948−3 8.412−2 8.682+0 1.656+1 3.960−1 6.012−1 5.042−2 6.761−2 2.749−1 1.761−1 3.309−1 1.246−1 1.855−1 8.760−2 1.167−1 5.175−2 6.471−2 4.749−1 1.573+1 9.724−2 3.083−1 3.019−2 8.385−2 2.776−1 5.054−2 7.512−1 3.529−2 3.884−1 3.262−2 1.610−1 2.442−2 3.585+0 3.046+1 1.252−1 5.471−1 1.802−1 5.409−2 6.100−1 2.021−1 1.436+0 1.555−1 7.006−1 8.660−2 2.860−1 2.389−1 2.308+1 5.911−2 2.253−2 8.585−2 3.123−2 5.867−1 3.511−2 2.928+0 3.693−2 9.898−1 3.747−2 2.106+0 3.603+1 3.416−2 1.321−2 1.609−1 3.569−2 8.995−1 2.533−1 4.240+0 1.519−1 1.392+0
1.905−3 1.177−3 7.336−3 3.425−3 5.329−2 2.068−2 3.247−1 1.059−2 8.961−2 9.078+0 1.731+1 4.160−1 6.257−1 4.956−2 6.626−2 2.950−1 1.918−1 3.625−1 1.328−1 1.975−1 1.028−1 1.370−1 5.572−2 6.966−2 5.068−1 1.660+1 9.701−2 3.180−1 2.595−2 9.440−2 3.043−1 5.628−2 8.199−1 4.116−2 4.024−1 3.474−2 1.741−1 2.595−2 3.640+0 3.093+1 1.234−1 5.611−1 2.011−1 6.017−2 6.687−1 2.226−1 1.561+0 1.626−1 7.269−1 9.306−2 3.090−1 2.421−1 2.515+1 4.693−2 2.204−2 9.289−2 3.496−2 6.209−1 3.693−2 3.163+0 4.094−2 1.043+0 3.978−2 2.231+0 4.053+1 3.337−2 1.483−2 1.734−1 3.844−2 9.513−1 2.723−1 4.565+0 1.605−1 1.468+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
73
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.558−1 6.480−3 1.333−2 1.361−2 5.140−2 2.544−2 7.336−1 5.263−2 4.030+0 9.516−2 8.658−3 7.734−3 2.812−2 2.037−2 8.220−2 5.271−2 9.963−1 2.484−1 5.261+0 1.265+1 2.476+1 1.270+0 1.905+0 1.464−1 1.956−1 4.061−2 5.091−2 1.485+0 2.415+1 2.009−1 1.377+0 9.597−2 8.784−2 2.743−2 5.298+0 4.510+1 5.173−1 2.438+0 6.544−2 1.631−1 7.541−1 3.339+1 1.394−1 1.140+0 6.811−2 2.596+0 5.186+1 2.020−1 1.609+0 4.897−1 2.742+1 1.284−1 1.408+0 3.685+1 4.552−1
8.545−1 1.052−2 1.603−2 1.626−2 6.280−2 2.715−2 7.040−1 5.278−2 4.030+0 9.460−2 1.367−2 1.027−2 3.378−2 2.144−2 9.722−2 5.286−2 9.571−1 2.481−1 5.266+0 1.406+1 2.676+1 1.263+0 1.898+0 1.613−1 2.147−1 4.338−2 5.424−2 1.432+0 2.774+1 2.222−1 1.355+0 9.907−2 9.822−2 2.825−2 6.426+0 5.351+1 5.139−1 2.390+0 6.990−2 1.812−1 7.341−1 5.518+1 1.495−1 1.119+0 6.859−2 5.299+0 8.668+1 2.006−1 1.579+0 4.773−1 5.338+1 1.247−1 3.782+0 7.549+1 4.260−1
6.753−1 8.796−3 1.495−2 1.438−2 6.105−2 2.430−2 7.086−1 4.710−2 4.334+0 8.382−2 1.151−2 8.654−3 3.103−2 1.881−2 9.422−2 4.718−2 9.614−1 2.481−1 5.657+0 1.531+1 2.907+1 1.243+0 1.869+0 1.627−1 2.167−1 4.170−2 5.215−2 1.403+0 3.026+1 2.259−1 1.328+0 9.725−2 9.764−2 2.621−2 7.009+0 5.851+1 5.034−1 2.341+0 6.698−2 1.788−1 7.184−1 6.027+1 1.475−1 1.092+0 6.285−2 5.707+0 9.435+1 1.911−1 1.539+0 4.577−1 5.787+1 1.135−1 3.960+0 8.151+1 3.870−1
5.179−1 7.493−3 1.415−2 1.268−2 6.013−2 2.145−2 7.141−1 4.138−2 4.737+0 7.291−2 9.858−3 7.255−3 2.885−2 1.616−2 9.215−2 4.147−2 9.667−1 2.517−1 6.177+0 1.671+1 3.169+1 1.222+0 1.836+0 1.646−1 2.194−1 4.008−2 5.013−2 1.372+0 3.305+1 2.304−1 1.297+0 9.548−2 9.734−2 2.427−2 7.642+0 6.399+1 4.919−1 2.285+0 6.427−2 1.769−1 7.014−1 6.561+1 1.461−1 1.064+0 5.725−2 6.127+0 1.023+2 1.816−1 1.497+0 4.375−1 6.252+1 1.026−1 4.140+0 8.771+1 3.480−1
3.943−1 6.520−3 1.362−2 1.124−2 6.043−2 1.892−2 7.200−1 3.620−2 5.261+0 6.294−2 8.615−3 6.093−3 2.722−2 1.374−2 9.177−2 3.630−2 9.729−1 2.609−1 6.856+0 1.820+1 3.451+1 1.198+0 1.800+0 1.671−1 2.228−1 3.867−2 4.837−2 1.338+0 3.599+1 2.355−1 1.265+0 9.392−2 9.742−2 2.261−2 8.295+0 6.967+1 4.802−1 2.227+0 6.208−2 1.759−1 6.840−1 7.094+1 1.456−1 1.035+0 5.231−2 6.539+0 1.102+2 1.728−1 1.454+0 4.183−1 6.710+1 9.334−2 4.315+0 9.378+1 3.125−1
3.034−1 5.818−3 1.333−2 1.012−2 6.228−2 1.690−2 7.259−1 3.196−2 5.930+0 5.467−2 7.714−3 5.181−3 2.613−2 1.173−2 9.369−2 3.208−2 9.793−1 2.775−1 7.725+0 1.972+1 3.745+1 1.173+0 1.763+0 1.700−1 2.267−1 3.756−2 4.699−2 1.301+0 3.895+1 2.410−1 1.230+0 9.265−2 9.788−2 2.137−2 8.943+0 7.533+1 4.682−1 2.166+0 6.055−2 1.758−1 6.663−1 7.604+1 1.460−1 1.005+0 4.836−2 6.929+0 1.178+2 1.650−1 1.411+0 4.009−1 7.144+1 8.621−2 4.479+0 9.951+1 2.827−1
2.395−1 5.337−3 1.323−2 9.308−3 6.577−2 1.549−2 7.312−1 2.877−2 6.753+0 4.837−2 7.095−3 4.511−3 2.550−2 1.018−2 9.815−2 2.889−2 9.853−1 3.023−1 8.798+0 2.125+1 4.042+1 1.148+0 1.725+0 1.733−1 2.312−1 3.677−2 4.601−2 1.261+0 4.186+1 2.465−1 1.192+0 9.165−2 9.859−2 2.053−2 9.565+0 8.081+1 4.557−1 2.100+0 5.965−2 1.763−1 6.480−1 8.080+1 1.471−1 9.741−1 4.543−2 7.287+0 1.247+2 1.583−1 1.368+0 3.853−1 7.543+1 8.127−2 4.628+0 1.048+2 2.589−1
1.952−1 5.010−3 1.319−2 8.726−3 7.031−2 1.456−2 7.322−1 2.640−2 7.661+0 4.377−2 6.671−3 4.033−3 2.510−2 9.033−3 1.042−1 2.653−2 9.857−1 3.324−1 9.984+0 2.260+1 4.309+1 1.122+0 1.688+0 1.762−1 2.351−1 3.612−2 4.520−2 1.215+0 4.440+1 2.501−1 1.148+0 9.040−2 9.882−2 1.993−2 1.009+1 8.554+1 4.406−1 2.021+0 5.889−2 1.763−1 6.261−1 8.471+1 1.478−1 9.377−1 4.317−2 7.571+0 1.304+2 1.516−1 1.317+0 3.695−1 7.865+1 7.777−2 4.740+0 1.089+2 2.395−1
1.624−1 4.689−3 1.288−2 8.136−3 7.317−2 1.368−2 7.125−1 2.416−2 8.317+0 3.973−2 6.252−3 3.631−3 2.425−2 8.065−3 1.080−1 2.430−2 9.587−1 3.536−1 1.085+1 2.312+1 4.416+1 1.079+0 1.630+0 1.747−1 2.332−1 3.479−2 4.355−2 1.144+0 4.530+1 2.458−1 1.078+0 8.691−2 9.621−2 1.904−2 1.025+1 8.708+1 4.150−1 1.897+0 5.680−2 1.713−1 5.895−1 8.553+1 1.444−1 8.795−1 4.053−2 7.588+0 1.313+2 1.420−1 1.235+0 3.464−1 7.905+1 7.358−2 4.698+0 1.093+2 2.192−1
1.342−1 4.904−3 1.313−2 8.644−3 7.048−2 1.411−2 7.434−1 2.558−2 8.915+0 4.281−2 6.559−3 3.897−3 2.500−2 8.585−3 1.039−1 2.572−2 1.000+0 3.754−1 1.159+1 2.077+1 4.527+1 1.049+0 1.576+0 2.108−1 2.830−1 3.847−2 4.826−2 1.166+0 4.063+1 3.416−1 1.119+0 1.046−1 1.263−1 2.220−2 9.466+0 7.863+1 4.468−1 1.984+0 6.909−2 2.176−1 6.287−1 9.469+1 1.671−1 9.302−1 4.456−2 6.791+0 1.543+2 1.525−1 1.308+0 3.707−1 7.561+1 1.265−1 4.116+0 1.050+2 2.459−1
74
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 28 Effective collision strengths for transitions in Cr XXII. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.958−1 3.801−1 1.726−2 5.029−3 9.395−3 1.314−2 1.963−2 3.445−3 1.253−3 2.382−3 2.387−3 3.580−3 1.433−3 1.903−3 1.344−3 5.290−4 1.006−3 9.216−4 1.383−3 7.549−4 1.003−3 9.837−5 1.226−4 3.420−2 1.220−3 1.870−2 4.921−3 6.331−2 9.146−3 3.908−4 3.868−3 1.612−3 1.162−2 2.849−3 1.902−3 1.183−3 1.843−4 1.548−3 7.738−4 4.357−3 1.331−3 1.029−3 7.176−4 9.600−5 9.483−5 2.469−3 5.064−3 4.267−2 2.427−2 1.243−1 7.781−4 1.630−3 9.382−3 5.815−3 2.359−2 2.130−3 4.229−3 3.654−4 7.793−4 3.871−3 2.493−3 9.027−3 1.248−3 2.331−3 1.640−4 2.306−4 1.277+0 2.460+0 9.175−2 1.378−1 8.090−2 1.356−2 2.514−2
2.002−1 3.877−1 1.928−2 6.459−3 1.213−2 1.436−2 2.184−2 3.808−3 1.725−3 3.318−3 2.844−3 4.296−3 1.893−3 2.513−3 1.280−3 6.114−4 1.170−3 9.854−4 1.480−3 7.982−4 1.061−3 1.056−4 1.318−4 4.986−2 5.389−3 2.008−2 8.413−3 6.432−2 1.449−2 1.209−3 4.276−3 2.571−3 1.256−2 3.905−3 3.034−3 2.218−3 3.263−4 1.433−3 8.297−4 4.559−3 1.407−3 1.138−3 7.437−4 1.090−4 9.593−5 1.195−2 8.844−3 4.925−2 3.114−2 1.313−1 2.483−3 2.698−3 1.106−2 7.431−3 2.617−2 3.962−3 6.948−3 6.580−4 8.560−4 3.710−3 2.645−3 9.477−3 1.328−3 2.555−3 1.720−4 2.567−4 1.272+0 2.462+0 1.204−1 1.845−1 8.374−2 1.678−2 3.462−2
2.097−1 4.056−1 1.883−2 6.548−3 1.239−2 1.452−2 2.209−2 3.662−3 1.657−3 3.191−3 2.743−3 4.138−3 1.761−3 2.336−3 1.275−3 6.175−4 1.185−3 9.731−4 1.463−3 7.801−4 1.037−3 9.888−5 1.233−4 5.519−2 4.397−3 1.981−2 7.893−3 6.661−2 1.374−2 9.843−4 4.066−3 2.255−3 1.269−2 3.498−3 2.821−3 1.879−3 2.937−4 1.415−3 7.825−4 4.649−3 1.319−3 1.138−3 6.893−4 1.042−4 8.705−5 9.579−3 8.253−3 4.804−2 3.065−2 1.349−1 2.014−3 2.345−3 1.038−2 6.941−3 2.608−2 3.430−3 6.344−3 5.927−4 8.026−4 3.631−3 2.553−3 9.572−3 1.255−3 2.517−3 1.579−4 2.420−4 1.350+0 2.605+0 1.181−1 1.804−1 8.287−2 1.768−2 3.589−2
2.206−1 4.262−1 1.846−2 6.722−3 1.276−2 1.462−2 2.219−2 3.555−3 1.634−3 3.145−3 2.655−3 4.001−3 1.640−3 2.176−3 1.277−3 6.341−4 1.219−3 9.593−4 1.443−3 7.596−4 1.010−3 9.115−5 1.136−4 5.691−2 3.591−3 1.944−2 7.103−3 6.962−2 1.236−2 8.075−4 3.894−3 1.957−3 1.297−2 3.071−3 2.664−3 1.556−3 2.655−4 1.400−3 7.267−4 4.787−3 1.207−3 1.150−3 6.229−4 9.959−5 7.680−5 7.722−3 7.412−3 4.644−2 2.956−2 1.394−1 1.649−3 2.024−3 9.766−3 6.453−3 2.627−2 2.931−3 5.845−3 5.361−4 7.427−4 3.546−3 2.442−3 9.734−3 1.170−3 2.491−3 1.420−4 2.269−4 1.454+0 2.793+0 1.127−1 1.717−1 8.255−2 1.965−2 3.892−2
2.334−1 4.505−1 1.822−2 7.126−3 1.352−2 1.482−2 2.243−2 3.496−3 1.675−3 3.222−3 2.596−3 3.911−3 1.544−3 2.050−3 1.287−3 6.667−4 1.284−3 9.465−4 1.425−3 7.393−4 9.835−4 8.304−5 1.035−4 5.446−2 2.970−3 1.910−2 6.239−3 7.410−2 1.072−2 6.750−4 3.769−3 1.694−3 1.351−2 2.646−3 2.598−3 1.270−3 2.407−4 1.386−3 6.637−4 4.997−3 1.074−3 1.183−3 5.482−4 9.603−5 6.583−5 6.333−3 6.511−3 4.487−2 2.846−2 1.463−1 1.378−3 1.746−3 9.271−3 6.022−3 2.692−2 2.511−3 5.532−3 4.870−4 6.770−4 3.457−3 2.321−3 1.001−2 1.080−3 2.496−3 1.255−4 2.131−4 1.585+0 3.029+0 1.063−1 1.615−1 8.289−2 2.305−2 4.469−2
2.494−1 4.804−1 1.817−2 7.903−3 1.499−2 1.527−2 2.303−2 3.484−3 1.798−3 3.458−3 2.577−3 3.881−3 1.479−3 1.965−3 1.303−3 7.222−4 1.393−3 9.384−4 1.413−3 7.222−4 9.613−4 7.532−5 9.387−5 4.896−2 2.548−3 1.888−2 5.453−3 8.081−2 9.114−3 5.820−4 3.689−3 1.467−3 1.439−2 2.242−3 2.638−3 1.028−3 2.203−4 1.375−3 5.972−4 5.307−3 9.297−4 1.244−3 4.709−4 9.415−5 5.499−5 5.411−3 5.701−3 4.363−2 2.786−2 1.574−1 1.190−3 1.511−3 8.898−3 5.689−3 2.821−2 2.187−3 5.438−3 4.469−4 6.090−4 3.370−3 2.206−3 1.046−2 9.949−4 2.550−3 1.097−4 2.025−4 1.736+0 3.305+0 1.004−1 1.522−1 8.377−2 2.820−2 5.389−2
2.692−1 5.170−1 1.831−2 9.177−3 1.740−2 1.600−2 2.409−2 3.513−3 2.018−3 3.884−3 2.601−3 3.918−3 1.443−3 1.919−3 1.327−3 8.088−4 1.563−3 9.390−4 1.415−3 7.110−4 9.469−4 6.869−5 8.563−5 4.232−2 2.328−3 1.880−2 4.818−3 9.037−2 7.705−3 5.248−4 3.649−3 1.279−3 1.569−2 1.873−3 2.786−3 8.318−4 2.059−4 1.369−3 5.324−4 5.747−3 7.853−4 1.341−3 3.978−4 9.429−5 4.512−5 4.945−3 5.054−3 4.287−2 2.809−2 1.739−1 1.078−3 1.318−3 8.640−3 5.488−3 3.030−2 1.958−3 5.566−3 4.195−4 5.435−4 3.296−3 2.117−3 1.115−2 9.259−4 2.669−3 9.597−5 1.960−4 1.899+0 3.607+0 9.565−2 1.447−1 8.502−2 3.531−2 6.695−2
2.916−1 5.586−1 1.854−2 1.097−2 2.082−2 1.695−2 2.548−2 3.561−3 2.335−3 4.500−3 2.659−3 4.006−3 1.428−3 1.901−3 1.351−3 9.275−4 1.796−3 9.475−4 1.429−3 7.047−4 9.391−4 6.349−5 7.918−5 3.604−2 2.293−3 1.882−2 4.345−3 1.028−1 6.551−3 4.991−4 3.631−3 1.127−3 1.737−2 1.553−3 3.016−3 6.787−4 1.985−4 1.365−3 4.737−4 6.307−3 6.523−4 1.465−3 3.341−4 9.596−5 3.676−5 4.886−3 4.580−3 4.245−2 2.923−2 1.959−1 1.031−3 1.163−3 8.460−3 5.429−3 3.313−2 1.815−3 5.869−3 4.067−4 4.846−4 3.231−3 2.066−3 1.206−2 8.777−4 2.845−3 8.489−5 1.933−4 2.060+0 3.912+0 9.183−2 1.387−1 8.619−2 4.418−2 8.344−2
3.096−1 5.925−1 1.849−2 1.284−2 2.439−2 1.765−2 2.651−2 3.547−3 2.654−3 5.122−3 2.683−3 4.044−3 1.400−3 1.864−3 1.347−3 1.042−3 2.022−3 9.433−4 1.423−3 6.893−4 9.191−4 5.879−5 7.336−5 3.062−2 2.355−3 1.856−2 3.963−3 1.146−1 5.599−3 4.892−4 3.559−3 9.975−4 1.887−2 1.281−3 3.217−3 5.590−4 1.940−4 1.337−3 4.190−4 6.785−3 5.346−4 1.568−3 2.798−4 9.647−5 2.987−5 5.037−3 4.198−3 4.157−2 3.048−2 2.169−1 1.017−3 1.032−3 8.192−3 5.393−3 3.565−2 1.710−3 6.143−3 3.999−4 4.297−4 3.121−3 2.017−3 1.284−2 8.355−4 2.988−3 7.546−5 1.895−4 2.166+0 4.115+0 8.744−2 1.320−1 8.550−2 5.264−2 9.924−2
3.189−1 6.116−1 1.930−2 1.393−2 2.640−2 1.833−2 2.742−2 3.815−3 2.865−3 5.502−3 2.717−3 4.086−3 1.430−3 1.901−3 1.478−3 1.122−3 2.159−3 9.445−4 1.422−3 7.085−4 9.423−4 5.980−5 7.450−5 2.276−2 2.220−3 1.959−2 3.787−3 1.221−1 4.972−3 4.605−4 3.930−3 9.809−4 1.973−2 1.184−3 3.354−3 5.085−4 1.801−4 1.546−3 4.267−4 6.999−3 5.139−4 1.677−3 2.857−4 9.824−5 3.122−5 4.731−3 4.014−3 4.346−2 3.128−2 2.296−1 9.564−4 1.012−3 8.900−3 5.443−3 3.706−2 1.671−3 6.323−3 3.710−4 4.377−4 3.532−3 2.037−3 1.319−2 8.718−4 3.168−3 7.780−5 1.935−4 2.261+0 4.385+0 8.640−2 1.301−1 8.979−2 5.756−2 1.085−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
75
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.380−2 5.029−2 3.389−2 4.517−2 1.432−2 3.224−3 6.169−3 7.127−3 1.065−2 3.906−3 5.218−3 6.150−3 7.675−3 1.506−1 1.803+0 2.329−2 5.185−3 8.569−2 1.204−2 1.056−1 1.553−2 1.125−1 1.660−2 1.610−3 1.589−2 3.227−3 2.124−2 4.269−3 1.235−2 4.003−3 1.420−2 4.812−3 4.205−1 3.449+0 1.078−2 1.279−2 1.848−1 4.154−2 2.106−1 5.422−2 2.076−1 3.250−3 3.345−3 3.511−2 9.559−3 4.284−2 8.679−3 2.399−2 1.138−2 2.748−2 1.095−1 4.597−3 8.628−3 8.887−3 1.660−1 2.125−2 7.271−1 3.751−2 1.466−3 3.128−3 3.530−3 3.135−2 7.796−3 1.109−1 1.219−2 3.276−2 7.215−3 6.937−3 6.058−3 2.039−2 2.135−2 2.601−1 9.275−2 1.061+0
3.536−2 6.333−2 4.076−2 6.103−2 1.428−2 3.513−3 6.602−3 7.240−3 1.086−2 4.666−3 6.232−3 6.454−3 8.062−3 1.818−1 1.840+0 7.858−2 1.242−2 8.290−2 1.762−2 1.066−1 2.521−2 1.142−1 2.723−2 1.896−3 1.471−2 3.253−3 2.362−2 4.759−3 1.271−2 4.268−3 1.473−2 4.976−3 4.849−1 3.520+0 2.706−2 1.811−2 2.084−1 5.075−2 2.526−1 6.859−2 2.600−1 4.040−3 3.499−3 3.287−2 1.071−2 4.763−2 9.146−3 2.485−2 1.181−2 2.856−2 3.105−1 1.372−2 2.100−2 2.317−2 1.746−1 4.264−2 7.280−1 6.867−2 2.267−3 3.643−3 4.151−3 3.103−2 8.372−3 1.178−1 1.316−2 3.218−2 7.209−3 2.189−2 1.577−2 4.827−2 4.054−2 3.075−1 1.253−1 1.101+0
3.614−2 6.255−2 3.942−2 5.812−2 1.440−2 3.776−3 7.117−3 7.418−3 1.113−2 4.451−3 5.945−3 6.315−3 7.889−3 1.767−1 1.935+0 7.306−2 1.070−2 8.269−2 1.624−2 1.146−1 2.264−2 1.173−1 2.390−2 1.794−3 1.486−2 3.191−3 2.507−2 4.490−3 1.282−2 3.896−3 1.510−2 4.617−3 4.992−1 3.689+0 2.353−2 1.666−2 2.029−1 4.977−2 2.597−1 6.509−2 2.553−1 3.778−3 3.393−3 3.310−2 1.067−2 5.010−2 8.688−3 2.475−2 1.144−2 2.894−2 2.868−1 1.092−2 1.770−2 1.911−2 1.717−1 3.590−2 7.608−1 5.769−2 1.976−3 3.377−3 3.729−3 3.075−2 7.545−3 1.217−1 1.170−2 3.347−2 6.402−3 1.745−2 1.280−2 4.139−2 3.419−2 2.954−1 1.160−1 1.139+0
3.754−2 6.242−2 3.826−2 5.519−2 1.461−2 4.211−3 7.958−3 7.674−3 1.152−2 4.222−3 5.640−3 6.200−3 7.745−3 1.684−1 2.076+0 6.290−2 9.856−3 8.288−2 1.514−2 1.272−1 2.016−2 1.220−1 2.081−2 1.770−3 1.505−2 3.148−3 2.721−2 4.199−3 1.300−2 3.493−3 1.559−2 4.237−3 5.219−1 3.970+0 2.166−2 1.563−2 1.973−1 4.997−2 2.747−1 6.244−2 2.527−1 3.704−3 3.324−3 3.346−2 1.075−2 5.383−2 8.212−3 2.475−2 1.110−2 2.951−2 2.445−1 8.808−3 1.531−2 1.552−2 1.692−1 2.945−2 8.117−1 4.722−2 1.738−3 3.157−3 3.304−3 3.050−2 6.642−3 1.274−1 1.011−2 3.545−2 5.559−3 1.401−2 1.022−2 3.556−2 2.821−2 2.836−1 1.087−1 1.202+0
3.968−2 6.370−2 3.742−2 5.285−2 1.488−2 4.872−3 9.234−3 8.018−3 1.203−2 4.002−3 5.348−3 6.135−3 7.665−3 1.594−1 2.265+0 5.179−2 9.874−3 8.353−2 1.450−2 1.460−1 1.812−2 1.288−1 1.828−2 1.832−3 1.529−2 3.132−3 3.026−2 3.907−3 1.328−2 3.096−3 1.619−2 3.869−3 5.559−1 4.355+0 2.158−2 1.513−2 1.937−1 5.191−2 3.022−1 6.112−2 2.551−1 3.825−3 3.297−3 3.393−2 1.102−2 5.922−2 7.772−3 2.493−2 1.080−2 3.029−2 1.980−1 7.287−3 1.384−2 1.266−2 1.678−1 2.399−2 8.862−1 3.823−2 1.545−3 2.995−3 2.900−3 3.031−2 5.734−3 1.354−1 8.505−3 3.824−2 4.754−3 1.151−2 8.151−3 3.138−2 2.316−2 2.744−1 1.045−1 1.301+0
4.252−2 6.646−2 3.692−2 5.124−2 1.519−2 5.817−3 1.106−2 8.448−3 1.267−2 3.815−3 5.099−3 6.140−3 7.672−3 1.514−1 2.486+0 4.212−2 1.075−2 8.457−2 1.435−2 1.720−1 1.658−2 1.374−1 1.640−2 1.989−3 1.555−2 3.154−3 3.443−2 3.641−3 1.367−2 2.739−3 1.685−2 3.544−3 5.985−1 4.803+0 2.337−2 1.513−2 1.922−1 5.588−2 3.450−1 6.117−2 2.629−1 4.158−3 3.314−3 3.449−2 1.155−2 6.667−2 7.414−3 2.532−2 1.058−2 3.119−2 1.566−1 6.258−3 1.327−2 1.057−2 1.675−1 1.971−2 9.887−1 3.102−2 1.393−3 2.910−3 2.546−3 3.021−2 4.894−3 1.463−1 7.021−3 4.186−2 4.050−3 9.798−3 6.576−3 2.902−2 1.920−2 2.685−1 1.042−1 1.442+0
4.586−2 7.038−2 3.672−2 5.029−2 1.553−2 7.093−3 1.352−2 8.945−3 1.342−2 3.676−3 4.914−3 6.220−3 7.773−3 1.449−1 2.721+0 3.476−2 1.246−2 8.584−2 1.460−2 2.062−1 1.551−2 1.471−1 1.514−2 2.252−3 1.582−2 3.215−3 3.988−2 3.419−3 1.414−2 2.447−3 1.752−2 3.281−3 6.455−1 5.274+0 2.700−2 1.552−2 1.927−1 6.202−2 4.048−1 6.235−2 2.749−1 4.720−3 3.377−3 3.510−2 1.240−2 7.652−2 7.164−3 2.589−2 1.045−2 3.214−2 1.238−1 5.607−3 1.350−2 9.159−3 1.679−1 1.655−2 1.122+0 2.554−2 1.282−3 2.913−3 2.262−3 3.020−2 4.179−3 1.605−1 5.754−3 4.617−2 3.486−3 8.707−3 5.426−3 2.840−2 1.627−2 2.653−1 1.081−1 1.629+0
4.924−2 7.467−2 3.665−2 4.974−2 1.581−2 8.665−3 1.655−2 9.443−3 1.416−2 3.580−3 4.786−3 6.344−3 7.928−3 1.396−1 2.950+0 2.962−2 1.488−2 8.695−2 1.508−2 2.476−1 1.476−2 1.567−1 1.434−2 2.608−3 1.603−2 3.300−3 4.642−2 3.240−3 1.461−2 2.225−3 1.806−2 3.078−3 6.917−1 5.723+0 3.221−2 1.613−2 1.938−1 6.999−2 4.792−1 6.408−2 2.882−1 5.484−3 3.466−3 3.563−2 1.352−2 8.840−2 7.003−3 2.651−2 1.036−2 3.293−2 9.954−2 5.221−3 1.440−2 8.289−3 1.684−1 1.431−2 1.281+0 2.155−2 1.206−3 2.999−3 2.051−3 3.019−2 3.609−3 1.774−1 4.745−3 5.069−2 3.064−3 8.046−3 4.610−3 2.918−2 1.419−2 2.634−1 1.154−1 1.855+0
5.122−2 7.711−2 3.598−2 4.855−2 1.571−2 1.013−2 1.938−2 9.690−3 1.453−2 3.457−3 4.621−3 6.357−3 7.944−3 1.333−1 3.096+0 2.591−2 1.727−2 8.616−2 1.531−2 2.853−1 1.400−2 1.618−1 1.364−2 2.946−3 1.587−2 3.326−3 5.219−2 3.052−3 1.473−2 2.033−3 1.810−2 2.879−3 7.198−1 6.005+0 3.740−2 1.646−2 1.914−1 7.715−2 5.476−1 6.462−2 2.948−1 6.210−3 3.492−3 3.535−2 1.448−2 9.884−2 6.783−3 2.655−2 1.010−2 3.285−2 8.155−2 4.924−3 1.536−2 7.685−3 1.657−1 1.261−2 1.419+0 1.851−2 1.137−3 3.077−3 1.878−3 2.959−2 3.140−3 1.910−1 3.946−3 5.373−2 2.727−3 7.539−3 3.993−3 3.028−2 1.259−2 2.574−1 1.223−1 2.052+0
5.410−2 8.056−2 3.670−2 4.892−2 1.722−2 1.080−2 2.065−2 1.006−2 1.505−2 3.393−3 4.538−3 6.749−3 8.426−3 1.340−1 3.264+0 1.993−2 1.882−2 9.272−2 1.643−2 3.092−1 1.413−2 1.700−1 1.342−2 3.202−3 1.820−2 3.667−3 5.409−2 3.082−3 1.495−2 2.028−3 1.863−2 2.975−3 7.580−1 6.353+0 4.034−2 1.765−2 2.038−1 8.222−2 5.873−1 6.675−2 3.051−1 6.696−3 3.839−3 4.023−2 1.490−2 1.022−1 6.845−3 2.694−2 1.041−2 3.375−2 5.988−2 4.607−3 1.539−2 7.118−3 1.714−1 1.165−2 1.510+0 1.711−2 1.136−3 3.236−3 2.082−3 3.171−2 3.179−3 1.992−1 3.974−3 5.679−2 2.938−3 6.983−3 3.564−3 2.982−2 1.181−2 2.635−1 1.271−1 2.176+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.203−3 2.445−3 7.598−3 7.799−3 5.095−2 2.109−2 1.641−1 1.174−2 4.863−2 4.498+0 8.628+0 4.109−1 6.164−1 3.732−2 4.991−2 2.429−1 3.427−2 6.340−2 7.268−2 1.079−1 7.939−2 1.056−1 4.067−2 5.080−2 5.282−1 7.954+0 6.733−2 3.221−1 3.107−2 1.822−2 2.573−1 3.249−2 1.873−1 3.481−2 2.381−1 2.805−2 1.430−1 2.730−2 1.761+0 1.485+1 1.320−1 5.760−1 3.820−2 3.484−2 5.498−1 8.345−2 3.823−1 1.063−1 4.373−1 8.463−2 2.586−1 2.652−1 9.235+0 6.204−2 1.591−2 2.849−2 2.213−2 5.294−1 3.393−2 1.010+0 4.881−2 6.516−1 4.916−2 7.100−1 1.235+1 2.406−2 1.412−2 6.244−2 3.434−2 8.124−1 1.259−1 1.476+0 1.274−1 9.269−1
3.361−3 2.953−3 8.755−3 8.427−3 5.079−2 2.259−2 1.745−1 1.171−2 4.795−2 4.676+0 1.117+1 4.974−1 7.436−1 9.661−2 1.347−1 2.285−1 3.646−2 6.712−2 7.123−2 1.060−1 7.999−2 1.066−1 4.233−2 5.291−2 6.789−1 8.281+0 1.394−1 4.086−1 1.194−1 2.517−2 2.305−1 2.992−2 1.921−1 3.263−2 2.327−1 2.918−2 1.473−1 2.929−2 2.328+0 1.825+1 2.720−1 8.561−1 5.308−2 3.319−2 4.928−1 8.196−2 3.893−1 1.063−1 4.294−1 8.858−2 2.668−1 4.464−1 1.077+1 2.986−1 2.188−2 3.583−2 2.312−2 4.933−1 3.335−2 1.008+0 4.716−2 6.371−1 4.808−2 1.339+0 1.918+1 3.323−2 1.503−2 7.519−2 3.403−2 7.583−1 1.240−1 1.469+0 1.246−1 9.074−1
2.943−3 2.617−3 8.067−3 7.584−3 4.998−2 2.130−2 1.794−1 1.095−2 4.942−2 5.084+0 1.153+1 4.754−1 7.089−1 8.309−2 1.150−1 2.325−1 4.286−2 7.916−2 7.598−2 1.131−1 8.063−2 1.075−1 4.251−2 5.314−2 6.415−1 9.055+0 1.243−1 3.823−1 9.586−2 2.603−2 2.349−1 3.137−2 2.202−1 3.274−2 2.472−1 2.893−2 1.480−1 2.770−2 2.447+0 1.955+1 2.337−1 7.798−1 5.518−2 3.441−2 5.032−1 8.791−2 4.423−1 1.102−1 4.546−1 8.665−2 2.667−1 3.928−1 1.252+1 2.344−1 2.002−2 3.650−2 2.269−2 5.018−1 3.250−2 1.109+0 4.446−2 6.702−1 4.468−2 1.450+0 2.162+1 3.046−2 1.414−2 7.576−2 3.311−2 7.708−1 1.283−1 1.613+0 1.245−1 9.520−1
2.599−3 2.280−3 7.437−3 6.671−3 4.917−2 1.998−2 1.869−1 1.022−2 5.185−2 5.552+0 1.192+1 4.514−1 6.732−1 7.087−2 9.733−2 2.374−1 5.246−2 9.724−2 8.200−2 1.221−1 8.116−2 1.082−1 4.303−2 5.379−2 5.974−1 9.947+0 1.110−1 3.574−1 7.482−2 2.894−2 2.400−1 3.342−2 2.603−1 3.283−2 2.651−1 2.884−2 1.485−1 2.621−2 2.577+0 2.091+1 1.991−1 7.068−1 6.166−2 3.642−2 5.157−1 9.640−2 5.176−1 1.153−1 4.858−1 8.483−2 2.665−1 3.435−1 1.434+1 1.777−1 1.915−2 3.879−2 2.268−2 5.113−1 3.189−2 1.249+0 4.184−2 7.109−1 4.157−2 1.553+0 2.398+1 2.915−2 1.350−2 7.920−2 3.246−2 7.850−1 1.356−1 1.815+0 1.256−1 1.007+0
2.316−3 1.959−3 6.909−3 5.757−3 4.844−2 1.883−2 1.977−1 9.626−3 5.543−2 6.064+0 1.245+1 4.299−1 6.423−1 6.142−2 8.378−2 2.426−1 6.596−2 1.227−1 8.915−2 1.327−1 8.157−2 1.087−1 4.387−2 5.485−2 5.571−1 1.090+1 1.013−1 3.367−1 5.828−2 3.405−2 2.453−1 3.602−2 3.149−1 3.290−2 2.858−1 2.896−2 1.490−1 2.494−2 2.726+0 2.238+1 1.713−1 6.463−1 7.286−2 3.909−2 5.293−1 1.080−1 6.202−1 1.216−1 5.221−1 8.330−2 2.664−1 3.037−1 1.606+1 1.334−1 1.898−2 4.293−2 2.311−2 5.215−1 3.162−2 1.438+0 3.951−2 7.577−1 3.902−2 1.650+0 2.619+1 2.888−2 1.306−2 8.595−2 3.218−2 8.001−1 1.468−1 2.086+0 1.279−1 1.071+0
2.093−3 1.670−3 6.533−3 4.915−3 4.787−2 1.801−2 2.127−1 9.239−3 6.022−2 6.602+0 1.314+1 4.125−1 6.173−1 5.486−2 7.441−2 2.478−1 8.403−2 1.567−1 9.699−2 1.444−1 8.190−2 1.091−1 4.499−2 5.624−2 5.239−1 1.189+1 9.515−2 3.204−1 4.625−2 4.153−2 2.505−1 3.899−2 3.864−1 3.297−2 3.081−1 2.926−2 1.495−1 2.399−2 2.891+0 2.395+1 1.507−1 5.997−1 8.919−2 4.220−2 5.431−1 1.232−1 7.542−1 1.285−1 5.610−1 8.219−2 2.666−1 2.738−1 1.764+1 1.014−1 1.927−2 4.919−2 2.404−2 5.315−1 3.170−2 1.682+0 3.762−2 8.074−1 3.716−2 1.742+0 2.824+1 2.931−2 1.276−2 9.647−2 3.228−2 8.152−1 1.625−1 2.438+0 1.314−1 1.140+0
1.930−3 1.428−3 6.345−3 4.199−3 4.750−2 1.766−2 2.326−1 9.086−3 6.603−2 7.152+0 1.396+1 3.987−1 5.977−1 5.073−2 6.849−2 2.525−1 1.071−1 1.999−1 1.049−1 1.562−1 8.221−2 1.095−1 4.626−2 5.783−2 4.976−1 1.287+1 9.195−2 3.078−1 3.793−2 5.146−2 2.552−1 4.208−2 4.759−1 3.306−2 3.299−1 2.969−2 1.501−1 2.335−2 3.067+0 2.558+1 1.359−1 5.651−1 1.109−1 4.543−2 5.561−1 1.423−1 9.222−1 1.354−1 5.992−1 8.157−2 2.673−1 2.520−1 1.907+1 7.967−2 1.982−2 5.768−2 2.544−2 5.406−1 3.205−2 1.984+0 3.621−2 8.561−1 3.597−2 1.829+0 3.013+1 3.015−2 1.259−2 1.110−1 3.265−2 8.290−1 1.833−1 2.876+0 1.354−1 1.207+0
1.817−3 1.237−3 6.337−3 3.628−3 4.719−2 1.777−2 2.563−1 9.116−3 7.220−2 7.673+0 1.481+1 3.868−1 5.807−1 4.826−2 6.492−2 2.558−1 1.340−1 2.504−1 1.116−1 1.664−1 8.236−2 1.097−1 4.739−2 5.925−2 4.753−1 1.378+1 9.058−2 2.973−1 3.233−2 6.330−2 2.584−1 4.483−2 5.791−1 3.310−2 3.481−1 3.009−2 1.506−1 2.296−2 3.236+0 2.712+1 1.251−1 5.381−1 1.367−1 4.825−2 5.657−1 1.641−1 1.116+0 1.411−1 6.306−1 8.118−2 2.677−1 2.359−1 2.028+1 6.535−2 2.039−2 6.788−2 2.713−2 5.468−1 3.241−2 2.331+0 3.518−2 8.961−1 3.523−2 1.905+0 3.176+1 3.104−2 1.248−2 1.286−1 3.303−2 8.384−1 2.078−1 3.377+0 1.389−1 1.262+0
1.714−3 1.079−3 6.342−3 3.158−3 4.606−2 1.789−2 2.755−1 9.075−3 7.635−2 7.971+0 1.531+1 3.698−1 5.560−1 4.603−2 6.178−2 2.529−1 1.582−1 2.957−1 1.143−1 1.706−1 8.083−2 1.077−1 4.734−2 5.920−2 4.485−1 1.428+1 8.859−2 2.835−1 2.822−2 7.391−2 2.554−1 4.604−2 6.695−1 3.247−2 3.542−1 2.982−2 1.480−1 2.230−2 3.319+0 2.792+1 1.154−1 5.081−1 1.599−1 4.938−2 5.610−1 1.822−1 1.285+0 1.424−1 6.402−1 7.943−2 2.629−1 2.199−1 2.085+1 5.543−2 2.046−2 7.683−2 2.824−2 5.395−1 3.204−2 2.624+0 3.382−2 9.064−1 3.415−2 1.929+0 3.245+1 3.118−2 1.218−2 1.438−1 3.267−2 8.273−1 2.280−1 3.802+0 1.388−1 1.276+0
1.714−3 1.090−3 6.699−3 3.199−3 4.923−2 1.853−2 2.870−1 9.659−3 8.059−2 8.238+0 1.562+1 3.804−1 5.721−1 4.468−2 5.975−2 2.669−1 1.696−1 3.188−1 1.205−1 1.791−1 9.458−2 1.261−1 5.046−2 6.309−2 4.637−1 1.486+1 8.785−2 2.909−1 2.371−2 8.173−2 2.764−1 5.061−2 7.192−1 3.754−2 3.652−1 3.166−2 1.581−1 2.355−2 3.306+0 2.799+1 1.128−1 5.132−1 1.752−1 5.446−2 6.091−1 1.979−1 1.375+0 1.481−1 6.610−1 8.387−2 2.774−1 2.214−1 2.223+1 4.282−2 2.008−2 8.196−2 3.130−2 5.650−1 3.462−2 2.792+0 3.750−2 9.458−1 3.633−2 2.064+0 3.536+1 3.043−2 1.353−2 1.530−1 3.526−2 8.663−1 2.421−1 4.032+0 1.459−1 1.331+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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77
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.361−1 5.945−3 1.218−2 1.254−2 4.670−2 2.351−2 6.682−1 4.868−2 3.628+0 8.812−2 7.944−3 7.156−3 2.572−2 1.889−2 7.485−2 4.876−2 9.079−1 2.262−1 4.739+0 1.145+1 2.220+1 1.161+0 1.740+0 1.324−1 1.769−1 3.712−2 4.654−2 1.357+0 2.170+1 1.818−1 1.258+0 8.760−2 7.978−2 2.522−2 4.771+0 4.061+1 4.724−1 2.227+0 5.980−2 1.482−1 6.891−1 2.904+1 1.269−1 1.041+0 6.278−2 2.277+0 4.339+1 1.852−1 1.471+0 4.487−1 2.390+1 1.185−1 1.225+0 3.172+1 4.202−1
8.013−1 1.045−2 1.554−2 1.507−2 5.575−2 2.395−2 6.436−1 4.668−2 3.628+0 8.343−2 1.303−2 8.685−3 3.007−2 1.906−2 8.544−2 4.682−2 8.743−1 2.216−1 4.729+0 1.306+1 2.465+1 1.129+0 1.697+0 1.451−1 1.934−1 3.837−2 4.799−2 1.283+0 2.570+1 2.013−1 1.209+0 8.895−2 8.811−2 2.448−2 6.032+0 5.011+1 4.594−1 2.139+0 6.145−2 1.618−1 6.576−1 5.055+1 1.331−1 9.990−1 5.943−2 4.899+0 7.942+1 1.770−1 1.412+0 4.238−1 4.848+1 1.072−1 3.456+0 6.842+1 3.688−1
6.372−1 8.502−3 1.410−2 1.311−2 5.395−2 2.134−2 6.470−1 4.148−2 3.875+0 7.359−2 1.077−2 7.368−3 2.758−2 1.661−2 8.271−2 4.160−2 8.771−1 2.205−1 5.049+0 1.420+1 2.671+1 1.114+0 1.676+0 1.464−1 1.954−1 3.684−2 4.607−2 1.260+0 2.793+1 2.046−1 1.188+0 8.729−2 8.758−2 2.258−2 6.567+0 5.462+1 4.507−1 2.099+0 5.874−2 1.596−1 6.442−1 5.536+1 1.313−1 9.769−1 5.408−2 5.300+0 8.679+1 1.685−1 1.378+0 4.062−1 5.282+1 9.670−2 3.636+0 7.431+1 3.328−1
4.901−1 7.099−3 1.313−2 1.147−2 5.311−2 1.885−2 6.513−1 3.647−2 4.217+0 6.406−2 9.115−3 6.231−3 2.567−2 1.426−2 8.105−2 3.659−2 8.812−1 2.232−1 5.492+0 1.542+1 2.899+1 1.099+0 1.652+0 1.484−1 1.980−1 3.550−2 4.440−2 1.235+0 3.032+1 2.087−1 1.166+0 8.585−2 8.745−2 2.094−2 7.117+0 5.933+1 4.420−1 2.057+0 5.651−2 1.582−1 6.310−1 6.005+1 1.302−1 9.550−1 4.933−2 5.680+0 9.390+1 1.607−1 1.345+0 3.896−1 5.697+1 8.752−2 3.803+0 7.989+1 2.999−1
3.730−1 6.092−3 1.251−2 1.014−2 5.348−2 1.670−2 6.562−1 3.205−2 4.673+0 5.557−2 7.908−3 5.288−3 2.430−2 1.217−2 8.101−2 3.217−2 8.864−1 2.314−1 6.085+0 1.672+1 3.144+1 1.082+0 1.627+0 1.508−1 2.013−1 3.442−2 4.305−2 1.210+0 3.281+1 2.134−1 1.142+0 8.468−2 8.774−2 1.966−2 7.673+0 6.414+1 4.333−1 2.013+0 5.490−2 1.578−1 6.178−1 6.455+1 1.302−1 9.331−1 4.542−2 6.036+0 1.006+2 1.539−1 1.312+0 3.745−1 6.087+1 8.024−2 3.957+0 8.510+1 2.716−1
2.864−1 5.385−3 1.217−2 9.134−3 5.525−2 1.501−2 6.614−1 2.847−2 5.261+0 4.859−2 7.051−3 4.546−3 2.342−2 1.045−2 8.300−2 2.859−2 8.921−1 2.463−1 6.851+0 1.805+1 3.401+1 1.064+0 1.599+0 1.537−1 2.051−1 3.362−2 4.206−2 1.181+0 3.534+1 2.186−1 1.116+0 8.379−2 8.840−2 1.876−2 8.224+0 6.895+1 4.244−1 1.966+0 5.391−2 1.582−1 6.043−1 6.884+1 1.311−1 9.107−1 4.242−2 6.366+0 1.070+2 1.480−1 1.279+0 3.611−1 6.453+1 7.497−2 4.098+0 8.994+1 2.484−1
2.251−1 4.910−3 1.204−2 8.414−3 5.848−2 1.383−2 6.663−1 2.577−2 5.989+0 4.326−2 6.470−3 3.996−3 2.294−2 9.121−3 8.720−2 2.590−2 8.977−1 2.684−1 7.801+0 1.940+1 3.664+1 1.045+0 1.570+0 1.570−1 2.094−1 3.308−2 4.139−2 1.150+0 3.786+1 2.238−1 1.087+0 8.312−2 8.930−2 1.820−2 8.761+0 7.368+1 4.150−1 1.914+0 5.345−2 1.593−1 5.900−1 7.289+1 1.326−1 8.868−1 4.026−2 6.673+0 1.129+2 1.428−1 1.245+0 3.490−1 6.793+1 7.151−2 4.227+0 9.443+1 2.300−1
1.828−1 4.596−3 1.200−2 7.913−3 6.280−2 1.307−2 6.685−1 2.379−2 6.817+0 3.940−2 6.084−3 3.606−3 2.269−2 8.145−3 9.306−2 2.393−2 9.000−1 2.962−1 8.884+0 2.066+1 3.911+1 1.025+0 1.537+0 1.602−1 2.136−1 3.267−2 4.087−2 1.110+0 4.018+1 2.278−1 1.050+0 8.234−2 8.992−2 1.784−2 9.243+0 7.797+1 4.038−1 1.852+0 5.316−2 1.601−1 5.730−1 7.641+1 1.339−1 8.583−1 3.866−2 6.931+0 1.180+2 1.377−1 1.205+0 3.368−1 7.083+1 6.924−2 4.332+0 9.822+1 2.151−1
1.522−1 4.320−3 1.178−2 7.441−3 6.613−2 1.241−2 6.557−1 2.200−2 7.491+0 3.613−2 5.734−3 3.286−3 2.214−2 7.345−3 9.757−2 2.215−2 8.822−1 3.189−1 9.769+0 2.131+1 4.044+1 9.886−1 1.479+0 1.599−1 2.133−1 3.176−2 3.973−2 1.050+0 4.131+1 2.258−1 9.917−1 7.987−2 8.839−2 1.728−2 9.451+0 7.997+1 3.845−1 1.754+0 5.190−2 1.572−1 5.449−1 7.771+1 1.323−1 8.129−1 3.679−2 6.994+0 1.197+2 1.303−1 1.140+0 3.190−1 7.171+1 6.650−2 4.324+0 9.924+1 1.996−1
1.239−1 4.471−3 1.201−2 7.931−3 6.365−2 1.285−2 6.778−1 2.367−2 7.909+0 3.955−2 5.982−3 3.592−3 2.285−2 7.921−3 9.378−2 2.381−2 9.124−1 3.348−1 1.028+1 1.917+1 4.036+1 9.685−1 1.456+0 1.935−1 2.600−1 3.535−2 4.434−2 1.078+0 3.700+1 3.127−1 1.033+0 9.527−2 1.146−1 2.028−2 8.668+0 7.178+1 4.115−1 1.831+0 6.325−2 1.990−1 5.845−1 7.896+1 1.560−1 8.572−1 4.098−2 6.502+0 1.329+2 1.391−1 1.202+0 3.410−1 7.122+1 1.479−1 3.736+0 9.432+1 2.261−1
78
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 29 Effective collision strengths for transitions in Mn XXIII. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.825−1 3.526−1 1.584−2 4.742−3 8.808−3 1.210−2 1.807−2 3.157−3 1.170−3 2.215−3 2.185−3 3.278−3 1.313−3 1.743−3 1.231−3 4.915−4 9.310−4 8.415−4 1.263−3 6.900−4 9.166−4 8.921−5 1.111−4 3.101−2 1.118−3 1.709−2 4.461−3 5.849−2 8.264−3 3.565−4 3.528−3 1.458−3 1.071−2 2.568−3 1.745−3 1.063−3 1.676−4 1.410−3 6.988−4 4.009−3 1.199−3 9.454−4 6.449−4 8.725−5 8.480−5 2.267−3 4.605−3 3.900−2 2.225−2 1.150−1 7.101−4 1.476−3 8.550−3 5.295−3 2.173−2 1.930−3 3.874−3 3.322−4 7.042−4 3.521−3 2.264−3 8.296−3 1.131−3 2.135−3 1.476−4 2.093−4 1.196+0 2.291+0 8.382−2 1.259−1 7.250−2 1.382−2 2.558−2
1.879−1 3.609−1 1.777−2 6.020−3 1.108−2 1.330−2 2.018−2 3.656−3 1.594−3 2.998−3 2.598−3 3.902−3 1.710−3 2.289−3 1.172−3 5.604−4 1.072−3 8.957−4 1.346−3 7.256−4 9.649−4 9.483−5 1.179−4 4.766−2 4.718−3 1.852−2 7.421−3 5.957−2 1.300−2 1.036−3 3.855−3 2.249−3 1.153−2 3.486−3 2.682−3 1.929−3 2.754−4 1.314−3 7.470−4 4.186−3 1.261−3 1.032−3 6.637−4 9.732−5 8.491−5 1.088−2 8.220−3 4.412−2 2.850−2 1.214−1 2.105−3 2.362−3 1.018−2 6.712−3 2.399−2 3.476−3 6.183−3 5.600−4 7.624−4 3.395−3 2.393−3 8.688−3 1.194−3 2.320−3 1.532−4 2.286−4 1.190+0 2.298+0 1.101−1 1.682−1 7.612−2 1.568−2 2.898−2
1.968−1 3.781−1 1.728−2 6.111−3 1.135−2 1.340−2 2.031−2 3.492−3 1.537−3 2.904−3 2.503−3 3.757−3 1.587−3 2.121−3 1.170−3 5.689−4 1.090−3 8.842−4 1.330−3 7.083−4 9.421−4 8.836−5 1.098−4 5.163−2 3.821−3 1.818−2 6.890−3 6.179−2 1.208−2 8.450−4 3.677−3 1.968−3 1.167−2 3.100−3 2.501−3 1.620−3 2.507−4 1.297−3 7.004−4 4.281−3 1.174−3 1.036−3 6.107−4 9.302−5 7.645−5 8.588−3 7.488−3 4.319−2 2.782−2 1.248−1 1.723−3 2.057−3 9.562−3 6.246−3 2.395−2 2.988−3 5.646−3 5.089−4 7.134−4 3.314−3 2.303−3 8.791−3 1.124−3 2.288−3 1.399−4 2.153−4 1.270+0 2.441+0 1.068−1 1.626−1 7.545−2 1.677−2 3.112−2
2.071−1 3.981−1 1.693−2 6.319−3 1.180−2 1.349−2 2.041−2 3.365−3 1.527−3 2.895−3 2.424−3 3.640−3 1.480−3 1.976−3 1.175−3 5.885−4 1.129−3 8.719−4 1.312−3 6.895−4 9.174−4 8.114−5 1.008−4 5.196−2 3.109−3 1.781−2 6.159−3 6.488−2 1.071−2 6.960−4 3.535−3 1.708−3 1.199−2 2.702−3 2.385−3 1.334−3 2.284−4 1.282−3 6.465−4 4.425−3 1.065−3 1.053−3 5.475−4 8.916−5 6.689−5 6.853−3 6.621−3 4.188−2 2.675−2 1.294−1 1.423−3 1.777−3 8.991−3 5.801−3 2.423−2 2.551−3 5.238−3 4.635−4 6.581−4 3.231−3 2.198−3 8.968−3 1.044−3 2.273−3 1.251−4 2.021−4 1.375+0 2.627+0 1.013−1 1.538−1 7.543−2 1.898−2 3.528−2
2.197−1 4.219−1 1.674−2 6.783−3 1.270−2 1.373−2 2.072−2 3.290−3 1.582−3 3.008−3 2.377−3 3.572−3 1.399−3 1.866−3 1.186−3 6.247−4 1.200−3 8.614−4 1.297−3 6.717−4 8.941−4 7.378−5 9.174−5 4.864−2 2.582−3 1.750−2 5.405−3 6.953−2 9.224−3 5.861−4 3.434−3 1.479−3 1.257−2 2.313−3 2.359−3 1.086−3 2.088−4 1.269−3 5.873−4 4.643−3 9.399−4 1.091−3 4.781−4 8.643−5 5.688−5 5.617−3 5.775−3 4.063−2 2.585−2 1.368−1 1.201−3 1.534−3 8.526−3 5.424−3 2.498−2 2.194−3 5.014−3 4.240−4 5.979−4 3.148−3 2.088−3 9.266−3 9.626−4 2.291−3 1.101−4 1.906−4 1.503+0 2.856+0 9.548−2 1.446−1 7.601−2 2.262−2 4.208−2
2.356−1 4.512−1 1.674−2 7.631−3 1.433−2 1.421−2 2.140−2 3.265−3 1.718−3 3.277−3 2.368−3 3.562−3 1.347−3 1.796−3 1.204−3 6.844−4 1.317−3 8.564−4 1.290−3 6.579−4 8.761−4 6.699−5 8.334−5 4.306−2 2.245−3 1.732−2 4.744−3 7.641−2 7.829−3 5.111−4 3.373−3 1.284−3 1.349−2 1.948−3 2.432−3 8.781−4 1.929−4 1.261−3 5.266−4 4.962−3 8.070−4 1.158−3 4.082−4 8.538−5 4.722−5 4.848−3 5.057−3 3.970−2 2.551−2 1.485−1 1.050−3 1.330−3 8.179−3 5.148−3 2.638−2 1.926−3 4.994−3 3.929−4 5.366−4 3.071−3 1.988−3 9.742−3 8.889−4 2.360−3 9.619−5 1.823−4 1.648+0 3.118+0 9.038−2 1.367−1 7.704−2 2.793−2 5.206−2
2.548−1 4.867−1 1.690−2 8.962−3 1.687−2 1.496−2 2.249−2 3.282−3 1.948−3 3.727−3 2.400−3 3.613−3 1.321−3 1.761−3 1.227−3 7.744−4 1.493−3 8.599−4 1.297−3 6.498−4 8.658−4 6.136−5 7.640−5 3.695−2 2.095−3 1.728−2 4.225−3 8.602−2 6.636−3 4.681−4 3.346−3 1.123−3 1.480−2 1.621−3 2.598−3 7.118−4 1.826−4 1.256−3 4.689−4 5.404−3 6.777−4 1.257−3 3.440−4 8.615−5 3.863−5 4.511−3 4.505−3 3.917−2 2.600−2 1.653−1 9.665−4 1.163−3 7.941−3 5.003−3 2.852−2 1.744−3 5.172−3 3.738−4 4.789−4 3.007−3 1.918−3 1.045−2 8.321−4 2.490−3 8.443−5 1.779−4 1.800+0 3.400+0 8.635−2 1.304−1 7.829−2 3.507−2 6.547−2
2.752−1 5.245−1 1.709−2 1.070−2 2.019−2 1.582−2 2.376−2 3.305−3 2.252−3 4.320−3 2.450−3 3.691−3 1.307−3 1.742−3 1.245−3 8.875−4 1.715−3 8.670−4 1.308−3 6.436−4 8.579−4 5.690−5 7.091−5 3.142−2 2.098−3 1.725−2 3.839−3 9.764−2 5.666−3 4.507−4 3.322−3 9.924−4 1.637−2 1.342−3 2.816−3 5.829−4 1.779−4 1.249−3 4.169−4 5.920−3 5.607−4 1.371−3 2.888−4 8.775−5 3.146−5 4.523−3 4.102−3 3.878−2 2.719−2 1.861−1 9.366−4 1.030−3 7.750−3 4.969−3 3.117−2 1.631−3 5.469−3 3.663−4 4.271−4 2.942−3 1.877−3 1.129−2 7.921−4 2.654−3 7.494−5 1.760−4 1.940+0 3.662+0 8.292−2 1.252−1 7.908−2 4.342−2 8.115−2
2.873−1 5.469−1 1.678−2 1.220−2 2.304−2 1.618−2 2.428−2 3.231−3 2.495−3 4.797−3 2.433−3 3.667−3 1.264−3 1.685−3 1.221−3 9.736−4 1.884−3 8.501−4 1.283−3 6.206−4 8.276−4 5.226−5 6.518−5 2.660−2 2.138−3 1.677−2 3.487−3 1.064−1 4.833−3 4.389−4 3.209−3 8.726−4 1.740−2 1.100−3 2.947−3 4.793−4 1.727−4 1.205−3 3.658−4 6.235−3 4.564−4 1.437−3 2.407−4 8.687−5 2.546−5 4.621−3 3.737−3 3.748−2 2.795−2 2.017−1 9.174−4 9.077−4 7.392−3 4.877−3 3.286−2 1.527−3 5.626−3 3.577−4 3.759−4 2.803−3 1.812−3 1.178−2 7.470−4 2.735−3 6.623−5 1.704−4 1.997+0 3.773+0 7.807−2 1.178−1 7.717−2 5.005−2 9.360−2
3.031−1 5.783−1 1.781−2 1.381−2 2.606−2 1.724−2 2.578−2 3.520−3 2.814−3 5.389−3 2.531−3 3.807−3 1.327−3 1.763−3 1.363−3 1.097−3 2.106−3 8.755−4 1.319−3 6.559−4 8.721−4 5.461−5 6.802−5 2.051−2 2.145−3 1.797−2 3.451−3 1.174−1 4.442−3 4.387−4 3.602−3 8.815−4 1.886−2 1.035−3 3.182−3 4.492−4 1.698−4 1.415−3 3.804−4 6.670−3 4.458−4 1.590−3 2.508−4 1.102−4 2.707−5 4.605−3 3.685−3 3.990−2 2.973−2 2.209−1 9.162−4 9.135−4 8.147−3 5.091−3 3.539−2 1.546−3 5.994−3 3.517−4 3.917−4 3.226−3 1.890−3 1.255−2 8.025−4 2.998−3 6.962−5 1.779−4 2.141+0 4.105+0 7.910−2 1.192−1 8.237−2 5.665−2 1.063−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
79
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.151−2 4.685−2 3.074−2 4.097−2 1.308−2 3.030−3 5.777−3 6.601−3 9.863−3 3.551−3 4.745−3 5.649−3 7.054−3 1.372−1 1.675+0 2.116−2 5.027−3 7.746−2 1.096−2 9.955−2 1.395−2 1.045−1 1.485−2 1.510−3 1.449−2 2.938−3 1.959−2 3.841−3 1.139−2 3.617−3 1.300−2 4.342−3 3.943−1 3.225+0 1.029−2 1.174−2 1.676−1 3.836−2 1.983−1 4.966−2 1.927−1 3.055−3 3.057−3 3.202−2 8.717−3 3.952−2 7.908−3 2.207−2 1.036−2 2.517−2 9.873−2 4.137−3 7.981−3 7.922−3 1.508−1 1.862−2 6.720−1 3.252−2 1.322−3 2.885−3 3.186−3 2.866−2 7.005−3 1.020−1 1.088−2 3.059−2 6.467−3 6.247−3 5.350−3 1.867−2 1.873−2 2.362−1 8.346−2 9.800−1
3.272−2 5.038−2 3.768−2 5.190−2 1.312−2 3.277−3 6.155−3 6.658−3 9.982−3 4.174−3 5.580−3 5.855−3 7.317−3 1.653−1 1.704+0 7.089−2 1.084−2 7.680−2 1.457−2 1.008−1 2.005−2 1.055−1 2.319−2 1.698−3 1.357−2 2.969−3 2.184−2 4.258−3 1.158−2 3.783−3 1.356−2 4.435−3 4.494−1 3.264+0 2.278−2 1.694−2 1.792−1 4.679−2 2.117−1 6.132−2 2.064−1 3.434−3 3.116−3 3.032−2 9.757−3 4.403−2 8.203−3 2.257−2 1.070−2 2.623−2 2.799−1 1.147−2 1.821−2 1.899−2 1.602−1 3.559−2 6.763−1 5.796−2 1.947−3 3.264−3 3.679−3 2.831−2 7.402−3 1.083−1 1.159−2 2.980−2 6.348−3 1.863−2 1.339−2 4.302−2 3.551−2 2.655−1 1.116−1 1.004+0
3.358−2 5.124−2 3.632−2 4.967−2 1.326−2 3.568−3 6.711−3 6.845−3 1.026−2 3.975−3 5.314−3 5.735−3 7.166−3 1.596−1 1.801+0 6.400−2 9.435−3 7.647−2 1.355−2 1.092−1 1.812−2 1.086−1 2.029−2 1.620−3 1.371−2 2.910−3 2.336−2 4.007−3 1.171−2 3.434−3 1.393−2 4.100−3 4.640−1 3.447+0 2.006−2 1.559−2 1.767−1 4.612−2 2.246−1 5.834−2 2.085−1 3.299−3 3.051−3 3.053−2 9.756−3 4.664−2 7.778−3 2.252−2 1.036−2 2.663−2 2.509−1 9.170−3 1.549−2 1.561−2 1.574−1 2.967−2 7.109−1 4.823−2 1.708−3 3.019−3 3.282−3 2.807−2 6.622−3 1.124−1 1.022−2 3.114−2 5.599−3 1.485−2 1.080−2 3.657−2 2.966−2 2.566−1 1.036−1 1.048+0
3.507−2 5.310−2 3.518−2 4.778−2 1.348−2 4.031−3 7.597−3 7.107−3 1.066−2 3.771−3 5.041−3 5.644−3 7.053−3 1.516−1 1.944+0 5.407−2 8.874−3 7.660−2 1.290−2 1.221−1 1.645−2 1.135−1 1.775−2 1.618−3 1.389−2 2.873−3 2.557−2 3.742−3 1.191−2 3.067−3 1.441−2 3.755−3 4.883−1 3.738+0 1.901−2 1.465−2 1.745−1 4.667−2 2.463−1 5.635−2 2.139−1 3.319−3 3.012−3 3.087−2 9.882−3 5.051−2 7.353−3 2.259−2 1.006−2 2.722−2 2.096−1 7.458−3 1.357−2 1.274−2 1.552−1 2.433−2 7.635−1 3.938−2 1.511−3 2.825−3 2.894−3 2.787−2 5.792−3 1.183−1 8.755−3 3.316−2 4.836−3 1.199−2 8.612−3 3.146−2 2.438−2 2.492−1 9.770−2 1.119+0
3.724−2 5.606−2 3.438−2 4.643−2 1.374−2 4.719−3 8.916−3 7.450−3 1.117−2 3.581−3 4.788−3 5.605−3 7.005−3 1.435−1 2.126+0 4.419−2 9.119−3 7.718−2 1.267−2 1.410−1 1.514−2 1.202−1 1.577−2 1.697−3 1.411−2 2.866−3 2.867−2 3.484−3 1.222−2 2.715−3 1.498−2 3.430−3 5.227−1 4.115+0 1.962−2 1.420−2 1.736−1 4.891−2 2.796−1 5.563−2 2.231−1 3.511−3 3.008−3 3.131−2 1.020−2 5.604−2 6.975−3 2.283−2 9.810−3 2.797−2 1.680−1 6.251−3 1.247−2 1.053−2 1.541−1 1.995−2 8.389−1 3.198−2 1.351−3 2.696−3 2.537−3 2.773−2 4.978−3 1.265−1 7.317−3 3.594−2 4.127−3 9.949−3 6.894−3 2.802−2 2.003−2 2.441−1 9.505−2 1.223+0
4.001−2 5.999−2 3.392−2 4.563−2 1.404−2 5.683−3 1.077−2 7.868−3 1.180−2 3.427−3 4.582−3 5.634−3 7.041−3 1.365−1 2.332+0 3.601−2 1.015−2 7.811−2 1.282−2 1.668−1 1.419−2 1.284−1 1.434−2 1.869−3 1.435−2 2.896−3 3.285−2 3.254−3 1.261−2 2.407−3 1.559−2 3.151−3 5.637−1 4.536+0 2.191−2 1.422−2 1.741−1 5.307−2 3.265−1 5.610−2 2.356−1 3.895−3 3.044−3 3.183−2 1.078−2 6.356−2 6.682−3 2.325−2 9.638−3 2.882−2 1.326−1 5.451−3 1.217−2 8.944−3 1.539−1 1.658−2 9.411−1 2.613−2 1.228−3 2.643−3 2.232−3 2.767−2 4.246−3 1.374−1 6.020−3 3.946−2 3.523−3 8.581−3 5.605−3 2.630−2 1.668−2 2.413−1 9.603−2 1.367+0
4.316−2 6.454−2 3.373−2 4.525−2 1.434−2 6.956−3 1.322−2 8.337−3 1.250−2 3.318−3 4.436−3 5.729−3 7.159−3 1.310−1 2.547+0 3.000−2 1.192−2 7.922−2 1.326−2 2.002−1 1.353−2 1.375−1 1.342−2 2.138−3 1.459−2 2.962−3 3.821−2 3.067−3 1.307−2 2.163−3 1.618−2 2.930−3 6.077−1 4.969+0 2.583−2 1.459−2 1.757−1 5.923−2 3.880−1 5.748−2 2.501−1 4.485−3 3.116−3 3.239−2 1.165−2 7.328−2 6.488−3 2.383−2 9.538−3 2.968−2 1.052−1 4.958−3 1.259−2 7.913−3 1.543−1 1.413−2 1.072+0 2.175−2 1.141−3 2.674−3 1.995−3 2.768−2 3.637−3 1.514−1 4.939−3 4.353−2 3.051−3 7.727−3 4.676−3 2.613−2 1.425−2 2.403−1 1.007−1 1.552+0
4.608−2 6.873−2 3.355−2 4.492−2 1.453−2 8.426−3 1.604−2 8.755−3 1.313−2 3.234−3 4.325−3 5.832−3 7.289−3 1.262−1 2.742+0 2.585−2 1.420−2 7.985−2 1.377−2 2.381−1 1.303−2 1.454−1 1.282−2 2.471−3 1.471−2 3.032−3 4.421−2 2.909−3 1.344−2 1.975−3 1.658−2 2.754−3 6.472−1 5.350+0 3.084−2 1.506−2 1.767−1 6.658−2 4.582−1 5.897−2 2.631−1 5.211−3 3.192−3 3.273−2 1.269−2 8.421−2 6.346−3 2.432−2 9.435−3 3.024−2 8.521−2 4.655−3 1.349−2 7.282−3 1.542−1 1.238−2 1.217+0 1.855−2 1.078−3 2.764−3 1.820−3 2.758−2 3.153−3 1.667−1 4.087−3 4.743−2 2.698−3 7.196−3 4.012−3 2.705−2 1.252−2 2.388−1 1.078−1 1.760+0
4.699−2 6.995−2 3.243−2 4.336−2 1.419−2 9.548−3 1.820−2 8.808−3 1.321−2 3.084−3 4.124−3 5.748−3 7.183−3 1.191−1 2.818+0 2.263−2 1.602−2 7.777−2 1.383−2 2.664−1 1.230−2 1.471−1 1.210−2 2.720−3 1.431−2 3.003−3 4.839−2 2.711−3 1.331−2 1.792−3 1.631−2 2.551−3 6.601−1 5.496+0 3.488−2 1.504−2 1.721−1 7.164−2 5.102−1 5.849−2 2.651−1 5.756−3 3.161−3 3.191−2 1.331−2 9.175−2 6.068−3 2.395−2 9.064−3 2.963−2 6.990−2 4.354−3 1.415−2 6.751−3 1.493−1 1.092−2 1.315+0 1.596−2 1.007−3 2.795−3 1.656−3 2.661−2 2.731−3 1.755−1 3.391−3 4.910−2 2.390−3 6.693−3 3.472−3 2.766−2 1.106−2 2.304−1 1.122−1 1.900+0
5.070−2 7.545−2 3.376−2 4.501−2 1.591−2 1.061−2 2.023−2 9.407−3 1.408−2 3.127−3 4.184−3 6.274−3 7.833−3 1.226−1 3.049+0 1.839−2 1.825−2 8.471−2 1.520−2 2.981−1 1.287−2 1.585−1 1.235−2 3.082−3 1.678−2 3.399−3 5.220−2 2.808−3 1.388−2 1.837−3 1.723−2 2.703−3 7.130−1 5.959+0 3.938−2 1.645−2 1.865−1 7.867−2 5.677−1 6.206−2 2.845−1 6.476−3 3.574−3 3.712−2 1.420−2 9.861−2 6.291−3 2.496−2 9.582−3 3.125−2 5.396−2 4.242−3 1.481−2 6.590−3 1.574−1 1.050−2 1.443+0 1.526−2 1.043−3 3.052−3 1.748−3 2.916−2 2.834−3 1.895−1 3.490−3 5.336−2 2.630−3 6.437−3 3.224−3 2.845−2 1.067−2 2.419−1 1.204−1 2.081+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
80
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.987−3 2.198−3 6.965−3 7.009−3 4.652−2 1.906−2 1.508−1 1.067−2 4.535−2 4.234+0 8.070+0 3.753−1 5.632−1 3.424−2 4.580−2 2.233−1 3.349−2 6.145−2 6.794−2 1.007−1 7.308−2 9.723−2 3.719−2 4.643−2 4.810−1 7.429+0 6.203−2 2.938−1 2.819−2 1.733−2 2.353−1 3.007−2 1.790−1 3.185−2 2.205−1 2.558−2 1.318−1 2.499−2 1.663+0 1.430+1 1.202−1 5.252−1 3.664−2 3.243−2 5.036−1 7.830−2 3.654−1 9.818−2 4.054−1 7.776−2 2.380−1 2.412−1 8.907+0 5.606−2 1.464−2 2.667−2 2.036−2 4.852−1 3.108−2 9.508−1 4.451−2 6.025−1 4.480−2 6.993−1 1.202+1 2.217−2 1.295−2 5.808−2 3.150−2 7.446−1 1.170−1 1.389+0 1.171−1 8.572−1
2.978−3 2.592−3 7.968−3 7.434−3 4.628−2 2.028−2 1.603−1 1.048−2 4.424−2 4.729+0 8.811+0 4.153−1 6.918−1 8.584−2 1.227−1 2.114−1 3.433−2 6.340−2 6.658−2 9.922−2 7.351−2 9.795−2 3.868−2 4.835−2 5.408−1 8.591+0 1.303−1 3.674−1 1.047−1 2.136−2 2.126−1 2.778−2 1.779−1 2.986−2 2.168−1 2.650−2 1.348−1 2.620−2 2.047+0 1.645+1 2.488−1 8.239−1 4.630−2 3.017−2 4.555−1 7.559−2 3.628−1 9.830−2 4.003−1 8.027−2 2.438−1 3.995−1 1.032+1 2.578−1 1.969−2 3.369−2 2.153−2 4.539−1 3.016−2 9.329−1 4.225−2 5.928−1 4.284−2 1.175+0 1.762+1 3.030−2 1.317−2 7.133−2 3.087−2 6.980−1 1.134−1 1.362+0 1.138−1 8.433−1
2.602−3 2.285−3 7.273−3 6.647−3 4.553−2 1.907−2 1.655−1 9.789−3 4.583−2 5.076+0 9.441+0 4.022−1 6.586−1 7.328−2 1.040−1 2.150−1 4.119−2 7.610−2 7.136−2 1.063−1 7.406−2 9.869−2 3.895−2 4.868−2 5.159−1 9.203+0 1.158−1 3.440−1 8.307−2 2.316−2 2.168−1 2.926−2 2.075−1 2.996−2 2.311−1 2.632−2 1.354−1 2.478−2 2.189+0 1.773+1 2.120−1 7.420−1 5.000−2 3.175−2 4.654−1 8.194−2 4.185−1 1.023−1 4.252−1 7.855−2 2.437−1 3.489−1 1.192+1 1.996−1 1.818−2 3.430−2 2.102−2 4.621−1 2.946−2 1.038+0 3.980−2 6.252−1 3.981−2 1.289+0 1.985+1 2.791−2 1.254−2 7.141−2 3.009−2 7.099−1 1.183−1 1.512+0 1.141−1 8.873−1
2.296−3 1.982−3 6.676−3 5.812−3 4.481−2 1.790−2 1.733−1 9.156−3 4.836−2 5.462+0 1.016+1 3.883−1 6.235−1 6.252−2 8.791−2 2.194−1 5.126−2 9.484−2 7.727−2 1.151−1 7.451−2 9.928−2 3.952−2 4.940−2 4.911−1 9.867+0 1.032−1 3.223−1 6.455−2 2.673−2 2.215−1 3.128−2 2.489−1 3.004−2 2.484−1 2.631−2 1.359−1 2.349−2 2.343+0 1.914+1 1.798−1 6.654−1 5.769−2 3.396−2 4.770−1 9.079−2 4.963−1 1.073−1 4.554−1 7.699−2 2.436−1 3.049−1 1.352+1 1.504−1 1.752−2 3.667−2 2.099−2 4.711−1 2.901−2 1.182+0 3.750−2 6.643−1 3.713−2 1.400+0 2.205+1 2.684−2 1.210−2 7.475−2 2.960−2 7.233−1 1.262−1 1.719+0 1.154−1 9.406−1
2.050−3 1.698−3 6.208−3 4.997−3 4.419−2 1.693−2 1.845−1 8.669−3 5.198−2 5.887+0 1.097+1 3.757−1 5.927−1 5.450−2 7.580−2 2.241−1 6.515−2 1.208−1 8.408−2 1.251−1 7.486−2 9.973−2 4.039−2 5.049−2 4.692−1 1.059+1 9.402−2 3.044−1 5.036−2 3.225−2 2.263−1 3.374−2 3.041−1 3.010−2 2.678−1 2.648−2 1.363−1 2.243−2 2.508+0 2.064+1 1.546−1 6.030−1 6.971−2 3.664−2 4.895−1 1.026−1 6.002−1 1.133−1 4.895−1 7.573−2 2.437−1 2.704−1 1.502+1 1.130−1 1.745−2 4.095−2 2.144−2 4.805−1 2.888−2 1.372+0 3.551−2 7.080−1 3.501−2 1.504+0 2.411+1 2.669−2 1.178−2 8.157−2 2.946−2 7.373−1 1.378−1 1.992+0 1.179−1 1.001+0
1.861−3 1.448−3 5.902−3 4.263−3 4.373−2 1.630−2 1.997−1 8.383−3 5.668−2 6.344+0 1.185+1 3.650−1 5.676−1 4.909−2 6.758−2 2.287−1 8.340−2 1.548−1 9.131−2 1.359−1 7.514−2 1.001−1 4.148−2 5.186−2 4.510−1 1.137+1 8.824−2 2.903−1 4.021−2 3.988−2 2.309−1 3.645−2 3.751−1 3.016−2 2.881−1 2.681−2 1.368−1 2.167−2 2.681+0 2.220+1 1.361−1 5.555−1 8.640−2 3.959−2 5.018−1 1.178−1 7.335−1 1.196−1 5.253−1 7.489−2 2.440−1 2.449−1 1.640+1 8.651−2 1.777−2 4.728−2 2.238−2 4.895−1 2.905−2 1.613+0 3.393−2 7.535−1 3.352−2 1.599+0 2.601+1 2.714−2 1.158−2 9.213−2 2.964−2 7.509−1 1.538−1 2.341+0 1.213−1 1.063+0
1.727−3 1.243−3 5.782−3 3.654−3 4.345−2 1.614−2 2.193−1 8.307−3 6.220−2 6.818+0 1.277+1 3.558−1 5.475−1 4.575−2 6.244−2 2.327−1 1.061−1 1.972−1 9.826−2 1.464−1 7.541−2 1.005−1 4.266−2 5.334−2 4.355−1 1.217+1 8.518−2 2.792−1 3.328−2 4.963−2 2.350−1 3.910−2 4.620−1 3.024−2 3.074−1 2.723−2 1.375−1 2.119−2 2.855+0 2.377+1 1.229−1 5.206−1 1.078−1 4.248−2 5.130−1 1.364−1 8.971−1 1.258−1 5.596−1 7.448−2 2.448−1 2.265−1 1.764+1 6.872−2 1.827−2 5.565−2 2.375−2 4.974−1 2.943−2 1.907+0 3.279−2 7.965−1 3.262−2 1.686+0 2.773+1 2.789−2 1.147−2 1.064−1 3.003−2 7.629−1 1.742−1 2.765+0 1.251−1 1.123+0
1.632−3 1.081−3 5.799−3 3.171−3 4.304−2 1.631−2 2.408−1 8.346−3 6.754−2 7.234+0 1.360+1 3.458−1 5.281−1 4.364−2 5.915−2 2.345−1 1.311−1 2.437−1 1.035−1 1.543−1 7.523−2 1.002−1 4.350−2 5.438−2 4.195−1 1.286+1 8.347−2 2.689−1 2.856−2 6.045−2 2.367−1 4.112−2 5.562−1 3.014−2 3.215−1 2.749−2 1.374−1 2.082−2 3.001+0 2.510+1 1.130−1 4.922−1 1.315−1 4.468−2 5.189−1 1.562−1 1.074+0 1.303−1 5.848−1 7.397−2 2.445−1 2.122−1 1.861+1 5.699−2 1.867−2 6.501−2 2.521−2 5.005−1 2.968−2 2.221+0 3.185−2 8.274−1 3.195−2 1.751+0 2.907+1 2.849−2 1.136−2 1.224−1 3.029−2 7.676−1 1.964−1 3.220+0 1.277−1 1.165+0
1.525−3 9.390−4 5.728−3 2.749−3 4.137−2 1.620−2 2.532−1 8.187−3 6.979−2 7.341+0 1.384+1 3.268−1 4.965−1 4.114−2 5.553−2 2.278−1 1.496−1 2.782−1 1.035−1 1.545−1 7.261−2 9.673−2 4.268−2 5.337−2 3.933−1 1.302+1 8.021−2 2.525−1 2.483−2 6.839−2 2.298−1 4.116−2 6.232−1 2.907−2 3.201−1 2.678−2 1.328−1 1.995−2 3.022+0 2.536+1 1.030−1 4.571−1 1.490−1 4.473−2 5.055−1 1.689−1 1.199+0 1.289−1 5.821−1 7.130−2 2.363−1 1.958−1 1.874+1 4.835−2 1.836−2 7.153−2 2.570−2 4.855−1 2.890−2 2.431+0 3.023−2 8.203−1 3.055−2 1.744+0 2.915+1 2.801−2 1.093−2 1.332−1 2.949−2 7.445−1 2.103−1 3.526+0 1.253−1 1.154+0
1.575−3 9.746−4 6.206−3 2.855−3 4.523−2 1.732−2 2.730−1 8.936−3 7.571−2 7.754+0 1.462+1 3.470−1 5.222−1 4.166−2 5.573−2 2.464−1 1.526−1 2.824−1 1.063−1 1.576−1 2.427−1 3.310−1 4.998−2 6.252−2 4.227−1 1.380+1 8.192−2 2.657−1 2.177−2 7.564−2 2.555−1 4.470−2 6.684−1 3.455−2 3.357−1 3.050−2 1.505−1 2.295−2 3.108+0 2.695+1 1.031−1 4.686−1 1.658−1 4.916−2 5.588−1 1.853−1 1.290+0 1.380−1 6.096−1 8.068−2 2.660−1 2.023−1 2.041+1 3.935−2 1.823−2 7.713−2 3.348−2 5.172−1 3.833−2 2.656+0 3.503−2 8.737−1 3.367−2 1.966+0 3.233+1 2.765−2 1.459−2 1.457−1 3.768−2 7.964−1 2.299−1 3.842+0 1.348−1 1.230+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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81
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.125−1 5.413−3 1.116−2 1.139−2 4.288−2 2.136−2 6.116−1 4.420−2 3.382+0 8.005−2 7.234−3 6.484−3 2.351−2 1.713−2 6.869−2 4.428−2 8.309−1 2.087−1 4.418+0 1.095+1 2.087+1 1.060+0 1.589+0 1.219−1 1.630−1 3.381−2 4.240−2 1.235+0 2.042+1 1.679−1 1.147+0 8.008−2 7.342−2 2.285−2 4.509+0 3.839+1 4.309−1 2.031+0 5.451−2 1.360−1 6.277−1 2.828+1 1.164−1 9.488−1 5.668−2 2.234+0 4.137+1 1.682−1 1.340+0 4.074−1 2.313+1 1.068−1 1.201+0 3.065+1 3.782−1
6.859−1 8.749−3 1.304−2 1.325−2 4.871−2 2.098−2 5.889−1 4.099−2 3.338+0 7.309−2 1.161−2 7.428−3 2.864−2 1.663−2 7.700−2 4.141−2 7.996−1 2.000−1 4.359+0 1.236+1 2.313+1 1.043+0 1.571+0 1.327−1 1.769−1 3.444−2 4.306−2 1.183+0 2.397+1 1.843−1 1.117+0 8.057−2 8.002−2 2.167−2 5.705+0 4.717+1 4.217−1 1.970+0 5.507−2 1.464−1 6.035−1 4.712+1 1.205−1 9.185−1 5.241−2 4.633+0 7.435+1 1.602−1 1.296+0 3.848−1 4.505+1 9.417−2 3.230+0 6.365+1 3.268−1
5.375−1 7.201−3 1.213−2 1.152−2 4.781−2 1.865−2 5.925−1 3.630−2 3.596+0 6.420−2 9.573−3 6.314−3 2.581−2 1.442−2 7.465−2 3.661−2 8.029−1 2.003−1 4.693+0 1.344+1 2.511+1 1.028+0 1.547+0 1.342−1 1.789−1 3.312−2 4.142−2 1.159+0 2.607+1 1.877−1 1.095+0 7.918−2 7.975−2 2.004−2 6.206+0 5.139+1 4.132−1 1.930+0 5.278−2 1.448−1 5.905−1 5.143+1 1.192−1 8.970−1 4.775−2 4.992+0 8.094+1 1.525−1 1.263+0 3.686−1 4.891+1 8.502−2 3.390+0 6.886+1 2.948−1
4.108−1 6.084−3 1.151−2 1.009−2 4.772−2 1.649−2 5.970−1 3.190−2 3.949+0 5.581−2 8.100−3 5.356−3 2.377−2 1.236−2 7.356−2 3.214−2 8.074−1 2.047−1 5.148+0 1.460+1 2.726+1 1.010+0 1.521+0 1.362−1 1.816−1 3.201−2 4.003−2 1.133+0 2.830+1 1.919−1 1.071+0 7.799−2 7.985−2 1.867−2 6.716+0 5.577+1 4.045−1 1.887+0 5.097−2 1.440−1 5.774−1 5.563+1 1.186−1 8.751−1 4.370−2 5.331+0 8.726+1 1.455−1 1.231+0 3.534−1 5.259+1 7.730−2 3.537+0 7.379+1 2.659−1
3.128−1 5.284−3 1.114−2 8.960−3 4.870−2 1.467−2 6.019−1 2.812−2 4.409+0 4.851−2 7.045−3 4.569−3 2.238−2 1.056−2 7.413−2 2.831−2 8.126−1 2.143−1 5.746+0 1.581+1 2.956+1 9.919−1 1.493+0 1.386−1 1.849−1 3.113−2 3.894−2 1.107+0 3.058+1 1.965−1 1.046+0 7.706−2 8.031−2 1.763−2 7.227+0 6.019+1 3.958−1 1.841+0 4.973−2 1.440−1 5.642−1 5.965+1 1.190−1 8.532−1 4.045−2 5.647+0 9.325+1 1.394−1 1.199+0 3.397−1 5.605+1 7.135−2 3.673+0 7.839+1 2.414−1
2.416−1 4.729−3 1.097−2 8.119−3 5.093−2 1.329−2 6.068−1 2.512−2 4.992+0 4.265−2 6.311−3 3.960−3 2.153−2 9.113−3 7.666−2 2.529−2 8.182−1 2.303−1 6.504+0 1.705+1 3.194+1 9.722−1 1.463+0 1.414−1 1.887−1 3.050−2 3.816−2 1.078+0 3.290+1 2.014−1 1.019+0 7.637−2 8.108−2 1.693−2 7.730+0 6.458+1 3.870−1 1.793+0 4.903−2 1.448−1 5.511−1 6.348+1 1.201−1 8.308−1 3.801−2 5.941+0 9.889+1 1.341−1 1.166+0 3.275−1 5.929+1 6.718−2 3.797+0 8.267+1 2.216−1
1.919−1 4.360−3 1.094−2 7.533−3 5.442−2 1.236−2 6.111−1 2.291−2 5.700+0 3.827−2 5.824−3 3.517−3 2.109−2 8.018−3 8.117−2 2.307−2 8.232−1 2.527−1 7.428+0 1.828+1 3.433+1 9.516−1 1.431+0 1.445−1 1.928−1 3.009−2 3.765−2 1.046+0 3.518+1 2.062−1 9.888−1 7.584−2 8.198−2 1.651−2 8.215+0 6.885+1 3.776−1 1.741+0 4.875−2 1.459−1 5.372−1 6.706+1 1.216−1 8.069−1 3.627−2 6.211+0 1.041+2 1.295−1 1.133+0 3.164−1 6.229+1 6.452−2 3.911+0 8.661+1 2.060−1
1.574−1 4.106−3 1.092−2 7.107−3 5.845−2 1.175−2 6.105−1 2.125−2 6.447+0 3.504−2 5.487−3 3.196−3 2.078−2 7.204−3 8.659−2 2.139−2 8.217−1 2.781−1 8.406+0 1.932+1 3.638+1 9.266−1 1.392+0 1.468−1 1.957−1 2.966−2 3.710−2 1.005+0 3.708+1 2.088−1 9.498−1 7.487−2 8.220−2 1.618−2 8.603+0 7.234+1 3.652−1 1.674+0 4.837−2 1.461−1 5.192−1 6.984+1 1.224−1 7.766−1 3.485−2 6.408+0 1.081+2 1.245−1 1.090+0 3.041−1 6.454+1 6.256−2 3.984+0 8.952+1 1.926−1
1.311−1 3.826−3 1.057−2 6.617−3 6.039−2 1.105−2 5.889−1 1.948−2 6.909+0 3.191−2 5.115−3 2.897−3 1.995−2 6.459−3 8.907−2 1.962−2 7.923−1 2.929−1 9.013+0 1.950+1 3.682+1 8.783−1 1.317+0 1.441−1 1.920−1 2.842−2 3.554−2 9.367−1 3.734+1 2.034−1 8.836−1 7.153−2 7.947−2 1.546−2 8.617+0 7.267+1 3.422−1 1.561+0 4.649−2 1.411−1 4.862−1 6.964+1 1.189−1 7.241−1 3.277−2 6.341+0 1.075+2 1.162−1 1.016+0 2.839−1 6.409+1 5.936−2 3.904+0 8.872+1 1.767−1
1.118−1 4.089−3 1.098−2 7.251−3 5.954−2 1.196−2 6.208−1 2.143−2 7.536+0 3.589−2 5.472−3 3.291−3 2.087−2 7.290−3 8.785−2 2.156−2 8.357−1 3.172−1 9.802+0 2.054+1 3.708+1 8.698−1 1.308+0 1.867−1 2.513−1 3.314−2 4.161−2 9.680−1 3.365+1 3.025−1 9.291−1 8.904−2 1.088−1 1.884−2 8.078+0 6.582+1 3.751−1 1.649+0 6.052−2 1.927−1 5.316−1 7.082+1 1.476−1 7.735−1 3.769−2 6.022+0 1.094+2 1.275−1 1.085+0 3.091−1 6.571+1 1.634−1 3.505+0 8.486+1 2.062−1
82
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 30 Effective collision strengths for transitions in Fe XXIV. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.674−1 3.225−1 1.453−2 4.372−3 8.069−3 1.108−2 1.655−2 2.899−3 1.070−3 2.014−3 2.013−3 3.020−3 1.210−3 1.606−3 1.129−3 4.510−4 8.506−4 7.734−4 1.161−3 6.351−4 8.435−4 8.207−5 1.022−4 2.864−2 1.028−3 1.566−2 4.110−3 5.342−2 7.652−3 3.285−4 3.235−3 1.350−3 9.783−3 2.382−3 1.611−3 9.886−4 1.542−4 1.293−3 6.456−4 3.661−3 1.107−3 8.748−4 5.948−4 8.051−5 7.939−5 2.083−3 4.253−3 3.579−2 2.050−2 1.054−1 6.537−4 1.367−3 7.854−3 4.889−3 1.991−2 1.795−3 3.587−3 3.056−4 6.526−4 3.237−3 2.093−3 7.602−3 1.054−3 1.995−3 1.404−4 1.971−4 1.089+0 2.086+0 7.711−2 1.158−1 6.651−2 1.248−2 2.292−2
1.716−1 3.298−1 1.597−2 5.709−3 1.078−2 1.234−2 1.861−2 3.248−3 1.462−3 2.821−3 2.407−3 3.605−3 1.584−3 2.109−3 1.087−3 5.100−4 9.769−4 8.240−4 1.237−3 6.688−4 8.893−4 8.789−5 1.092−4 4.313−2 4.088−3 1.717−2 7.223−3 5.452−2 1.206−2 9.586−4 3.616−3 2.130−3 1.061−2 3.260−3 2.492−3 1.812−3 2.723−4 1.202−3 6.860−4 3.827−3 1.168−3 9.413−4 6.148−4 8.895−5 7.882−5 1.045−2 7.897−3 4.267−2 2.659−2 1.115−1 1.939−3 2.213−3 9.382−3 6.237−3 2.206−2 3.309−3 5.807−3 5.329−4 7.018−4 3.119−3 2.211−3 7.965−3 1.105−3 2.128−3 1.424−4 2.105−4 1.086+0 2.093+0 1.015−1 1.549−1 6.985−2 1.417−2 2.661−2
1.799−1 3.453−1 1.569−2 5.750−3 1.079−2 1.244−2 1.876−2 3.116−3 1.407−3 2.716−3 2.316−3 3.469−3 1.473−3 1.957−3 1.082−3 5.181−4 9.923−4 8.134−4 1.223−3 6.536−4 8.692−4 8.217−5 1.020−4 4.726−2 3.370−3 1.686−2 6.652−3 5.644−2 1.130−2 7.827−4 3.438−3 1.864−3 1.072−2 2.909−3 2.320−3 1.529−3 2.427−4 1.190−3 6.462−4 3.908−3 1.092−3 9.440−4 5.684−4 8.514−5 7.137−5 8.221−3 7.172−3 4.115−2 2.594−2 1.145−1 1.584−3 1.927−3 8.798−3 5.810−3 2.199−2 2.855−3 5.294−3 4.795−4 6.596−4 3.052−3 2.132−3 8.052−3 1.044−3 2.099−3 1.306−4 1.988−4 1.157+0 2.218+0 9.884−2 1.506−1 6.928−2 1.509−2 2.827−2
1.893−1 3.632−1 1.545−2 5.888−3 1.101−2 1.250−2 1.883−2 3.023−3 1.393−3 2.682−3 2.239−3 3.357−3 1.373−3 1.824−3 1.084−3 5.353−4 1.025−3 8.019−4 1.206−3 6.367−4 8.469−4 7.568−5 9.401−5 4.813−2 2.776−3 1.650−2 5.916−3 5.905−2 1.009−2 6.448−4 3.293−3 1.617−3 1.097−2 2.543−3 2.201−3 1.263−3 2.179−4 1.178−3 5.994−4 4.031−3 9.956−4 9.576−4 5.123−4 8.162−5 6.282−5 6.531−3 6.331−3 3.951−2 2.490−2 1.184−1 1.307−3 1.666−3 8.274−3 5.395−3 2.218−2 2.436−3 4.885−3 4.339−4 6.111−4 2.980−3 2.037−3 8.201−3 9.722−4 2.083−3 1.173−4 1.868−4 1.251+0 2.383+0 9.397−2 1.428−1 6.925−2 1.699−2 3.168−2
2.006−1 3.842−1 1.532−2 6.243−3 1.166−2 1.266−2 1.905−2 2.974−3 1.436−3 2.757−3 2.189−3 3.286−3 1.296−3 1.722−3 1.093−3 5.664−4 1.086−3 7.917−4 1.192−3 6.202−4 8.253−4 6.895−5 8.567−5 4.553−2 2.321−3 1.618−2 5.165−3 6.299−2 8.722−3 5.421−4 3.188−3 1.398−3 1.144−2 2.184−3 2.161−3 1.030−3 1.971−4 1.168−3 5.467−4 4.217−3 8.832−4 9.893−4 4.496−4 7.901−5 5.371−5 5.311−3 5.508−3 3.804−2 2.396−2 1.246−1 1.102−3 1.439−3 7.850−3 5.036−3 2.279−2 2.088−3 4.642−3 3.951−4 5.574−4 2.907−3 1.935−3 8.453−3 8.973−4 2.095−3 1.035−4 1.761−4 1.368+0 2.588+0 8.855−2 1.343−1 6.976−2 2.015−2 3.745−2
2.147−1 4.103−1 1.534−2 6.940−3 1.297−2 1.304−2 1.960−2 2.966−3 1.550−3 2.971−3 2.174−3 3.268−3 1.245−3 1.655−3 1.108−3 6.178−4 1.185−3 7.860−4 1.184−3 6.069−4 8.080−4 6.261−5 7.785−5 4.059−2 2.020−3 1.599−2 4.506−3 6.887−2 7.411−3 4.709−4 3.122−3 1.211−3 1.222−2 1.844−3 2.211−3 8.339−4 1.804−4 1.160−3 4.916−4 4.492−3 7.621−4 1.046−3 3.854−4 7.786−5 4.478−5 4.530−3 4.802−3 3.696−2 2.352−2 1.345−1 9.615−4 1.247−3 7.534−3 4.765−3 2.396−2 1.821−3 4.587−3 3.643−4 5.018−4 2.837−3 1.841−3 8.859−3 8.280−4 2.151−3 9.054−5 1.681−4 1.500+0 2.825+0 8.371−2 1.267−1 7.068−2 2.482−2 4.608−2
2.322−1 4.420−1 1.551−2 8.077−3 1.512−2 1.368−2 2.054−2 2.992−3 1.750−3 3.352−3 2.198−3 3.307−3 1.218−3 1.620−3 1.128−3 6.961−4 1.338−3 7.879−4 1.188−3 5.988−4 7.977−4 5.727−5 7.126−5 3.494−2 1.878−3 1.593−2 3.985−3 7.721−2 6.277−3 4.285−4 3.090−3 1.057−3 1.335−2 1.538−3 2.349−3 6.757−4 1.692−4 1.157−3 4.384−4 4.878−3 6.424−4 1.132−3 3.253−4 7.838−5 3.671−5 4.155−3 4.254−3 3.632−2 2.381−2 1.491−1 8.810−4 1.091−3 7.317−3 4.611−3 2.582−2 1.637−3 4.719−3 3.443−4 4.485−4 2.778−3 1.771−3 9.469−3 7.729−4 2.262−3 7.937−5 1.637−4 1.641+0 3.082+0 7.984−2 1.207−1 7.185−2 3.115−2 5.788−2
2.515−1 4.772−1 1.571−2 9.637−3 1.808−2 1.447−2 2.171−2 3.029−3 2.025−3 3.882−3 2.245−3 3.381−3 1.206−3 1.606−3 1.148−3 7.991−4 1.539−3 7.951−4 1.200−3 5.939−4 7.916−4 5.306−5 6.609−5 2.971−2 1.876−3 1.592−2 3.600−3 8.772−2 5.351−3 4.107−4 3.071−3 9.321−4 1.478−2 1.274−3 2.547−3 5.525−4 1.637−4 1.153−3 3.902−4 5.352−3 5.328−4 1.239−3 2.733−4 7.996−5 2.991−5 4.122−3 3.856−3 3.593−2 2.482−2 1.679−1 8.515−4 9.652−4 7.156−3 4.569−3 2.823−2 1.522−3 4.985−3 3.360−4 4.004−4 2.723−3 1.731−3 1.025−2 7.345−4 2.414−3 7.036−5 1.619−4 1.776+0 3.333+0 7.667−2 1.158−1 7.277−2 3.882−2 7.218−2
2.652−1 5.023−1 1.557−2 1.112−2 2.091−2 1.493−2 2.240−2 2.994−3 2.275−3 4.365−3 2.248−3 3.389−3 1.176−3 1.566−3 1.136−3 8.883−4 1.714−3 7.862−4 1.188−3 5.774−4 7.700−4 4.898−5 6.106−5 2.519−2 1.927−3 1.559−2 3.272−3 9.671−2 4.572−3 4.018−4 2.989−3 8.218−4 1.589−2 1.047−3 2.694−3 4.549−4 1.594−4 1.121−3 3.439−4 5.700−3 4.354−4 1.313−3 2.284−4 7.992−5 2.427−5 4.225−3 3.519−3 3.495−2 2.570−2 1.840−1 8.397−4 8.543−4 6.882−3 4.511−3 3.009−2 1.429−3 5.176−3 3.297−4 3.541−4 2.615−3 1.681−3 1.080−2 6.963−4 2.515−3 6.240−5 1.580−4 1.849+0 3.472+0 7.263−2 1.096−1 7.167−2 4.552−2 8.468−2
2.769−1 5.251−1 1.631−2 1.230−2 2.310−2 1.567−2 2.342−2 3.224−3 2.504−3 4.775−3 2.307−3 3.471−3 1.218−3 1.617−3 1.246−3 9.776−4 1.870−3 7.991−4 1.204−3 6.023−4 8.007−4 5.064−5 6.306−5 1.905−2 1.889−3 1.645−2 3.166−3 1.047−1 4.141−3 3.899−4 3.297−3 8.171−4 1.688−2 9.788−4 2.861−3 4.216−4 1.523−4 1.294−3 3.542−4 5.988−3 4.234−4 1.431−3 2.359−4 8.312−5 2.556−5 4.078−3 3.396−3 3.656−2 2.682−2 1.978−1 8.163−4 8.486−4 7.473−3 4.629−3 3.179−2 1.419−3 5.419−3 3.157−4 3.654−4 2.958−3 1.727−3 1.130−2 7.384−4 2.715−3 6.465−5 1.634−4 1.986+0 3.722+0 7.271−2 1.096−1 7.547−2 5.044−2 9.411−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
83
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.879−2 4.278−2 2.826−2 3.766−2 1.208−2 2.716−3 5.145−3 6.054−3 9.043−3 3.286−3 4.392−3 5.201−3 6.493−3 1.261−1 1.514+0 1.955−2 4.514−3 7.097−2 9.996−3 8.975−2 1.282−2 9.523−2 1.372−2 1.344−3 1.334−2 2.705−3 1.778−2 3.560−3 1.043−2 3.351−3 1.187−2 4.029−3 3.581−1 2.919+0 9.241−3 1.077−2 1.537−1 3.505−2 1.797−1 4.556−2 1.759−1 2.718−3 2.823−3 2.949−2 8.029−3 3.602−2 7.292−3 2.023−2 9.562−3 2.307−2 9.162−2 3.804−3 7.296−3 7.325−3 1.385−1 1.730−2 6.115−1 3.028−2 1.223−3 2.616−3 2.945−3 2.643−2 6.535−3 9.343−2 1.019−2 2.776−2 6.030−3 5.747−3 4.967−3 1.714−2 1.741−2 2.170−1 7.673−2 8.924−1
3.010−2 4.726−2 3.391−2 4.801−2 1.209−2 2.985−3 5.557−3 6.113−3 9.131−3 3.835−3 5.129−3 5.387−3 6.731−3 1.543−1 1.547+0 6.549−2 9.421−3 7.055−2 1.365−2 9.130−2 1.930−2 9.636−2 2.212−2 1.597−3 1.249−2 2.726−3 1.981−2 3.934−3 1.060−2 3.510−3 1.236−2 4.107−3 4.112−1 2.978+0 2.092−2 1.487−2 1.585−1 4.271−2 1.949−1 5.684−2 1.939−1 3.377−3 2.877−3 2.787−2 8.991−3 4.008−2 7.567−3 2.069−2 9.861−3 2.400−2 2.604−1 1.107−2 1.685−2 1.819−2 1.566−1 3.362−2 6.180−1 5.513−2 1.858−3 2.946−3 3.358−3 2.611−2 6.886−3 9.889−2 1.082−2 2.707−2 5.930−3 1.763−2 1.299−2 4.080−2 3.312−2 2.505−1 1.044−1 9.239−1
3.081−2 4.776−2 3.283−2 4.594−2 1.220−2 3.231−3 6.029−3 6.265−3 9.374−3 3.659−3 4.893−3 5.276−3 6.592−3 1.487−1 1.630+0 5.993−2 8.272−3 7.026−2 1.268−2 9.839−2 1.746−2 9.901−2 1.938−2 1.501−3 1.261−2 2.672−3 2.110−2 3.710−3 1.070−2 3.198−3 1.268−2 3.806−3 4.235−1 3.131+0 1.821−2 1.370−2 1.568−1 4.204−2 2.052−1 5.401−2 1.945−1 3.150−3 2.814−3 2.806−2 8.966−3 4.231−2 7.186−3 2.063−2 9.558−3 2.434−2 2.367−1 8.823−3 1.436−2 1.493−2 1.530−1 2.816−2 6.471−1 4.609−2 1.618−3 2.739−3 3.020−3 2.588−2 6.190−3 1.024−1 9.592−3 2.822−2 5.255−3 1.395−2 1.051−2 3.455−2 2.778−2 2.419−1 9.675−2 9.599−1
3.206−2 4.910−2 3.193−2 4.413−2 1.239−2 3.626−3 6.787−3 6.488−3 9.716−3 3.474−3 4.645−3 5.188−3 6.483−3 1.410−1 1.754+0 5.110−2 7.801−3 7.036−2 1.200−2 1.094−1 1.576−2 1.032−1 1.691−2 1.479−3 1.277−2 2.635−3 2.300−2 3.470−3 1.088−2 2.865−3 1.310−2 3.491−3 4.443−1 3.382+0 1.706−2 1.295−2 1.559−1 4.241−2 2.232−1 5.201−2 1.980−1 3.095−3 2.774−3 2.836−2 9.052−3 4.565−2 6.797−3 2.068−2 9.272−3 2.486−2 1.997−1 7.136−3 1.254−2 1.214−2 1.491−1 2.314−2 6.919−1 3.770−2 1.423−3 2.572−3 2.679−3 2.568−2 5.437−3 1.075−1 8.260−3 2.997−2 4.556−3 1.120−2 8.382−3 2.953−2 2.289−2 2.338−1 9.085−2 1.018+0
3.394−2 5.148−2 3.130−2 4.281−2 1.262−2 4.221−3 7.926−3 6.787−3 1.017−2 3.299−3 4.412−3 5.145−3 6.429−3 1.333−1 1.914+0 4.191−2 8.006−3 7.086−2 1.170−2 1.256−1 1.438−2 1.091−1 1.492−2 1.533−3 1.296−2 2.624−3 2.569−2 3.232−3 1.115−2 2.539−3 1.362−2 3.189−3 4.751−1 3.718+0 1.746−2 1.265−2 1.562−1 4.427−2 2.515−1 5.114−2 2.051−1 3.212−3 2.765−3 2.875−2 9.308−3 5.043−2 6.443−3 2.087−2 9.035−3 2.553−2 1.608−1 5.933−3 1.145−2 9.978−3 1.462−1 1.895−2 7.569−1 3.059−2 1.267−3 2.455−3 2.356−3 2.553−2 4.687−3 1.146−1 6.932−3 3.240−2 3.894−3 9.248−3 6.687−3 2.609−2 1.882−2 2.278−1 8.776−2 1.107+0
3.639−2 5.483−2 3.095−2 4.200−2 1.289−2 5.063−3 9.540−3 7.159−3 1.073−2 3.153−3 4.218−3 5.162−3 6.451−3 1.266−1 2.099+0 3.413−2 8.887−3 7.169−2 1.175−2 1.481−1 1.336−2 1.164−1 1.347−2 1.672−3 1.318−2 2.646−3 2.933−2 3.017−3 1.150−2 2.249−3 1.418−2 2.926−3 5.127−1 4.102+0 1.938−2 1.275−2 1.576−1 4.786−2 2.920−1 5.140−2 2.156−1 3.515−3 2.792−3 2.923−2 9.791−3 5.700−2 6.162−3 2.124−2 8.868−3 2.631−2 1.270−1 5.126−3 1.109−2 8.420−3 1.445−1 1.570−2 8.459−1 2.492−2 1.146−3 2.404−3 2.075−3 2.546−2 4.001−3 1.242−1 5.716−3 3.554−2 3.321−3 7.940−3 5.405−3 2.424−2 1.566−2 2.241−1 8.798−2 1.231+0
3.923−2 5.886−2 3.085−2 4.161−2 1.317−2 6.190−3 1.170−2 7.585−3 1.137−2 3.049−3 4.078−3 5.242−3 6.551−3 1.212−1 2.295+0 2.830−2 1.043−2 7.272−2 1.208−2 1.775−1 1.264−2 1.247−1 1.251−2 1.900−3 1.340−2 2.701−3 3.406−2 2.839−3 1.192−2 2.016−3 1.473−2 2.716−3 5.536−1 4.502+0 2.278−2 1.316−2 1.598−1 5.328−2 3.461−1 5.255−2 2.284−1 4.013−3 2.854−3 2.974−2 1.055−2 6.559−2 5.972−3 2.176−2 8.770−3 2.712−2 1.006−1 4.622−3 1.140−2 7.390−3 1.439−1 1.331−2 9.613−1 2.065−2 1.059−3 2.427−3 1.853−3 2.547−2 3.423−3 1.366−1 4.688−3 3.923−2 2.867−3 7.122−3 4.475−3 2.386−2 1.334−2 2.223−1 9.164−2 1.395+0
4.198−2 6.284−2 3.079−2 4.137−2 1.338−2 7.539−3 1.429−2 7.993−3 1.198−2 2.975−3 3.979−3 5.348−3 6.683−3 1.168−1 2.480+0 2.426−2 1.249−2 7.348−2 1.254−2 2.122−1 1.213−2 1.325−1 1.190−2 2.200−3 1.354−2 2.770−3 3.957−2 2.694−3 1.230−2 1.838−3 1.516−2 2.551−3 5.921−1 4.870+0 2.733−2 1.369−2 1.617−1 6.004−2 4.103−1 5.401−2 2.409−1 4.664−3 2.930−3 3.013−2 1.150−2 7.564−2 5.845−3 2.228−2 8.691−3 2.774−2 8.112−2 4.320−3 1.221−2 6.761−3 1.434−1 1.161−2 1.095+0 1.753−2 9.990−4 2.511−3 1.688−3 2.543−2 2.963−3 1.507−1 3.873−3 4.297−2 2.527−3 6.630−3 3.815−3 2.460−2 1.169−2 2.210−1 9.795−2 1.585+0
4.323−2 6.461−2 3.004−2 4.026−2 1.319−2 8.685−3 1.649−2 8.129−3 1.219−2 2.859−3 3.824−3 5.320−3 6.648−3 1.109−1 2.578+0 2.125−2 1.433−2 7.221−2 1.267−2 2.409−1 1.150−2 1.355−1 1.128−2 2.454−3 1.330−2 2.769−3 4.394−2 2.526−3 1.231−2 1.675−3 1.507−2 2.377−3 6.105−1 5.059+0 3.141−2 1.387−2 1.592−1 6.542−2 4.636−1 5.406−2 2.453−1 5.221−3 2.931−3 2.965−2 1.220−2 8.356−2 5.631−3 2.215−2 8.420−3 2.746−2 6.651−2 4.058−3 1.293−2 6.283−3 1.395−1 1.026−2 1.198+0 1.509−2 9.386−4 2.565−3 1.543−3 2.475−2 2.573−3 1.606−1 3.218−3 4.508−2 2.244−3 6.208−3 3.300−3 2.534−2 1.036−2 2.147−1 1.029−1 1.733+0
4.620−2 6.871−2 3.096−2 4.127−2 1.456−2 9.436−3 1.791−2 8.565−3 1.282−2 2.866−3 3.835−3 5.731−3 7.154−3 1.128−1 2.751+0 1.685−2 1.598−2 7.760−2 1.378−2 2.643−1 1.180−2 1.441−1 1.132−2 2.710−3 1.532−2 3.090−3 4.644−2 2.587−3 1.267−2 1.701−3 1.571−2 2.496−3 6.496−1 5.400+0 3.470−2 1.503−2 1.708−1 7.054−2 5.054−1 5.663−2 2.591−1 5.719−3 3.264−3 3.391−2 1.278−2 8.802−2 5.774−3 2.280−2 8.798−3 2.857−2 5.015−2 3.868−3 1.326−2 6.002−3 1.444−1 9.724−3 1.291+0 1.421−2 9.561−4 2.744−3 1.609−3 2.674−2 2.652−3 1.704−1 3.301−3 4.830−2 2.453−3 5.877−3 2.985−3 2.552−2 9.894−3 2.221−1 1.084−1 1.863+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
84
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.838−3 2.042−3 6.358−3 6.539−3 4.294−2 1.771−2 1.383−1 9.873−3 4.124−2 3.856+0 7.321+0 3.453−1 5.182−1 3.137−2 4.197−2 2.045−1 2.997−2 5.453−2 6.188−2 9.168−2 6.706−2 8.919−2 3.406−2 4.253−2 4.423−1 6.690+0 5.674−2 2.703−1 2.609−2 1.532−2 2.154−1 2.724−2 1.596−1 2.915−2 2.001−1 2.343−2 1.208−1 2.307−2 1.511+0 1.293+1 1.108−1 4.835−1 3.250−2 2.957−2 4.609−1 7.114−2 3.281−1 8.959−2 3.690−1 7.156−2 2.185−1 2.223−1 8.251+0 5.200−2 1.335−2 2.406−2 1.862−2 4.448−1 2.858−2 8.576−1 4.115−2 5.487−1 4.149−2 6.223−1 1.065+1 2.022−2 1.193−2 5.266−2 2.900−2 6.827−1 1.067−1 1.254+0 1.075−1 7.811−1
2.762−3 2.386−3 7.203−3 6.949−3 4.266−2 1.876−2 1.465−1 9.718−3 4.027−2 3.989+0 7.674+0 3.655−1 5.567−1 7.836−2 1.123−1 1.937−1 3.095−2 5.601−2 6.072−2 9.045−2 6.744−2 8.985−2 3.541−2 4.425−2 4.851−1 7.386+0 1.108−1 3.301−1 9.364−2 1.970−2 1.955−1 2.507−2 1.593−1 2.738−2 1.970−1 2.430−2 1.235−1 2.417−2 1.674+0 1.448+1 2.244−1 6.867−1 4.389−2 2.763−2 4.170−1 6.889−2 3.270−1 8.978−2 3.646−1 7.381−2 2.236−1 3.566−1 9.107+0 2.373−1 1.791−2 2.973−2 1.913−2 4.171−1 2.779−2 8.442−1 3.909−2 5.403−1 3.969−2 1.057+0 1.730+1 2.748−2 1.218−2 6.302−2 2.872−2 6.418−1 1.037−1 1.234+0 1.045−1 7.691−1
2.415−3 2.118−3 6.620−3 6.234−3 4.198−2 1.768−2 1.510−1 9.085−3 4.162−2 4.360+0 8.289+0 3.559−1 5.406−1 6.708−2 9.515−2 1.970−1 3.690−2 6.718−2 6.490−2 9.662−2 6.796−2 9.053−2 3.562−2 4.452−2 4.646−1 8.002+0 9.926−2 3.101−1 7.450−2 2.091−2 1.991−1 2.639−2 1.846−1 2.747−2 2.094−1 2.411−2 1.240−1 2.288−2 1.837+0 1.570+1 1.926−1 6.262−1 4.599−2 2.898−2 4.262−1 7.433−2 3.748−1 9.321−2 3.863−1 7.225−2 2.236−1 3.142−1 1.053+1 1.845−1 1.652−2 3.044−2 1.884−2 4.242−1 2.712−2 9.341−1 3.687−2 5.687−1 3.692−2 1.163+0 1.910+1 2.532−2 1.159−2 6.349−2 2.788−2 6.521−1 1.077−1 1.363+0 1.046−1 8.075−1
2.132−3 1.848−3 6.103−3 5.470−3 4.132−2 1.659−2 1.577−1 8.492−3 4.380−2 4.780+0 9.005+0 3.465−1 5.250−1 5.731−2 8.036−2 2.011−1 4.567−2 8.356−2 7.013−2 1.044−1 6.839−2 9.111−2 3.611−2 4.513−2 4.444−1 8.675+0 8.950−2 2.919−1 5.810−2 2.375−2 2.033−1 2.819−2 2.202−1 2.754−2 2.247−1 2.407−2 1.245−1 2.169−2 2.018+0 1.707+1 1.643−1 5.711−1 5.193−2 3.091−2 4.368−1 8.198−2 4.421−1 9.766−2 4.130−1 7.081−2 2.235−1 2.765−1 1.199+1 1.394−1 1.590−2 3.261−2 1.890−2 4.323−1 2.665−2 1.059+0 3.474−2 6.033−1 3.441−2 1.268+0 2.079+1 2.434−2 1.116−2 6.661−2 2.732−2 6.639−1 1.144−1 1.542+0 1.057−1 8.547−1
1.902−3 1.589−3 5.683−3 4.713−3 4.073−2 1.566−2 1.673−1 8.019−3 4.696−2 5.231+0 9.800+0 3.381−1 5.112−1 4.995−2 6.926−2 2.054−1 5.784−2 1.062−1 7.625−2 1.134−1 6.874−2 9.156−2 3.688−2 4.609−2 4.266−1 9.396+0 8.254−2 2.769−1 4.549−2 2.837−2 2.076−1 3.040−2 2.683−1 2.760−2 2.421−1 2.420−2 1.249−1 2.069−2 2.205+0 1.852+1 1.418−1 5.263−1 6.192−2 3.332−2 4.483−1 9.228−2 5.328−1 1.030−1 4.437−1 6.962−2 2.236−1 2.464−1 1.338+1 1.048−1 1.583−2 3.641−2 1.934−2 4.407−1 2.647−2 1.224+0 3.286−2 6.427−1 3.238−2 1.367+0 2.239+1 2.421−2 1.087−2 7.266−2 2.710−2 6.765−1 1.244−1 1.780+0 1.078−1 9.087−1
1.724−3 1.358−3 5.398−3 4.023−3 4.029−2 1.503−2 1.806−1 7.724−3 5.113−2 5.698+0 1.065+1 3.307−1 4.993−1 4.497−2 6.172−2 2.096−1 7.391−2 1.361−1 8.289−2 1.232−1 6.904−2 9.193−2 3.786−2 4.733−2 4.115−1 1.015+1 7.834−2 2.650−1 3.646−2 3.490−2 2.118−1 3.288−2 3.304−1 2.767−2 2.606−1 2.449−2 1.255−1 1.994−2 2.391+0 2.002+1 1.251−1 4.921−1 7.623−2 3.605−2 4.597−1 1.056−1 6.499−1 1.088−1 4.762−1 6.880−2 2.239−1 2.239−1 1.466+1 8.021−2 1.613−2 4.200−2 2.019−2 4.490−1 2.658−2 1.436+0 3.135−2 6.841−1 3.092−2 1.457+0 2.391+1 2.465−2 1.067−2 8.194−2 2.721−2 6.888−1 1.383−1 2.086+0 1.107−1 9.659−1
1.596−3 1.166−3 5.275−3 3.443−3 4.001−2 1.481−2 1.979−1 7.625−3 5.614−2 6.169+0 1.153+1 3.241−1 4.890−1 4.189−2 5.703−2 2.135−1 9.414−2 1.737−1 8.952−2 1.328−1 6.936−2 9.232−2 3.896−2 4.871−2 3.986−1 1.092+1 7.634−2 2.558−1 3.027−2 4.339−2 2.156−1 3.542−2 4.073−1 2.777−2 2.786−1 2.488−2 1.261−1 1.947−2 2.572+0 2.152+1 1.133−1 4.666−1 9.493−2 3.885−2 4.703−1 1.222−1 7.950−1 1.145−1 5.077−1 6.839−2 2.246−1 2.076−1 1.582+1 6.361−2 1.664−2 4.945−2 2.142−2 4.564−1 2.689−2 1.696+0 3.024−2 7.239−1 3.002−2 1.539+0 2.534+1 2.540−2 1.057−2 9.456−2 2.755−2 7.002−1 1.563−1 2.462+0 1.141−1 1.021+0
1.507−3 1.013−3 5.291−3 2.983−3 3.972−2 1.494−2 2.179−1 7.659−3 6.125−2 6.597+0 1.235+1 3.171−1 4.781−1 4.004−2 5.417−2 2.158−1 1.172−1 2.163−1 9.504−2 1.408−1 6.942−2 9.237−2 3.987−2 4.984−2 3.857−1 1.162+1 7.553−2 2.476−1 2.609−2 5.318−2 2.178−1 3.759−2 4.935−1 2.778−2 2.929−1 2.520−2 1.264−1 1.916−2 2.729+0 2.285+1 1.047−1 4.459−1 1.165−1 4.121−2 4.773−1 1.405−1 9.577−1 1.189−1 5.326−1 6.805−2 2.248−1 1.950−1 1.678+1 5.271−2 1.713−2 5.812−2 2.282−2 4.606−1 2.716−2 1.986+0 2.939−2 7.548−1 2.943−2 1.605+0 2.655+1 2.611−2 1.049−2 1.093−1 2.783−2 7.065−1 1.768−1 2.881+0 1.169−1 1.064+0
1.417−3 8.833−4 5.270−3 2.592−3 3.850−2 1.494−2 2.318−1 7.575−3 6.410−2 6.783+0 1.273+1 3.029−1 4.568−1 3.808−2 5.131−2 2.116−1 1.361−1 2.514−1 9.654−2 1.428−1 6.764−2 9.000−2 3.952−2 4.941−2 3.649−1 1.190+1 7.358−2 2.350−1 2.289−2 6.120−2 2.135−1 3.826−2 5.622−1 2.706−2 2.951−1 2.479−2 1.233−1 1.851−2 2.786+0 2.336+1 9.642−2 4.196−1 1.343−1 4.186−2 4.694−1 1.540−1 1.087+0 1.189−1 5.357−1 6.615−2 2.192−1 1.813−1 1.709+1 4.492−2 1.710−2 6.496−2 2.354−2 4.510−1 2.665−2 2.206+0 2.809−2 7.561−1 2.836−2 1.615+0 2.682+1 2.602−2 1.018−2 1.208−1 2.731−2 6.916−1 1.917−1 3.201+0 1.157−1 1.066+0
1.444−3 9.096−4 5.604−3 2.672−3 4.151−2 1.575−2 2.456−1 8.177−3 6.861−2 7.088+0 1.329+1 3.197−1 4.812−1 3.781−2 5.056−2 2.259−1 1.380−1 2.539−1 9.798−2 1.452−1 1.807−1 2.460−1 4.476−2 5.598−2 3.898−1 1.246+1 7.487−2 2.449−1 2.003−2 6.659−2 2.347−1 4.074−2 5.957−1 3.313−2 3.074−1 2.746−2 1.366−1 2.072−2 2.848+0 2.451+1 9.492−2 4.318−1 1.469−1 4.510−2 5.134−1 1.668−1 1.154+0 1.259−1 5.588−1 7.318−2 2.416−1 1.863−1 1.862+1 3.617−2 1.675−2 6.919−2 3.266−2 4.746−1 2.885−2 2.374+0 3.241−2 7.992−1 3.091−2 1.821+0 2.884+1 2.544−2 1.380−2 1.317−1 2.955−2 7.280−1 2.069−1 3.436+0 1.235−1 1.125+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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85
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.975−1 5.004−3 1.027−2 1.056−2 3.929−2 1.988−2 5.615−1 4.116−2 3.070+0 7.461−2 6.689−3 6.042−3 2.166−2 1.599−2 6.307−2 4.124−2 7.631−1 1.916−1 4.012+0 9.966+0 1.892+1 9.755−1 1.462+0 1.112−1 1.487−1 3.116−2 3.908−2 1.137+0 1.843+1 1.532−1 1.055+0 7.366−2 6.724−2 2.116−2 4.087+0 3.478+1 3.967−1 1.870+0 5.020−2 1.246−1 5.780−1 2.508+1 1.067−1 8.737−1 5.263−2 1.979+0 3.579+1 1.553−1 1.235+0 3.762−1 2.030+1 9.927−2 1.057+0 2.673+1 3.516−1
6.540−1 8.223−3 1.188−2 1.183−2 4.501−2 1.956−2 5.416−1 3.828−2 3.037+0 6.829−2 1.015−2 6.879−3 2.463−2 1.559−2 7.095−2 3.871−2 7.360−1 1.841−1 3.968+0 1.130+1 2.102+1 9.606−1 1.446+0 1.209−1 1.611−1 3.165−2 3.959−2 1.088+0 2.164+1 1.680−1 1.027+0 7.395−2 7.314−2 2.007−2 5.207+0 4.288+1 3.877−1 1.812+0 5.063−2 1.340−1 5.557−1 4.201+1 1.104−1 8.453−1 4.869−2 4.193+0 6.640+1 1.480−1 1.193+0 3.551−1 4.000+1 8.754−2 2.927+0 5.649+1 3.045−1
5.177−1 6.751−3 1.108−2 1.042−2 4.395−2 1.743−2 5.447−1 3.400−2 3.259+0 6.020−2 8.490−3 5.879−3 2.268−2 1.356−2 6.860−2 3.431−2 7.385−1 1.839−1 4.254+0 1.229+1 2.279+1 9.460−1 1.424+0 1.223−1 1.630−1 3.046−2 3.809−2 1.067+0 2.351+1 1.711−1 1.007+0 7.268−2 7.291−2 1.855−2 5.663+0 4.668+1 3.799−1 1.775+0 4.853−2 1.325−1 5.437−1 4.595+1 1.091−1 8.257−1 4.439−2 4.532+0 7.250+1 1.409−1 1.163+0 3.403−1 4.358+1 7.910−2 3.082+0 6.138+1 2.750−1
3.975−1 5.688−3 1.053−2 9.207−3 4.368−2 1.542−2 5.485−1 2.991−2 3.565+0 5.244−2 7.267−3 5.005−3 2.120−2 1.164−2 6.738−2 3.015−2 7.422−1 1.870−1 4.649+0 1.335+1 2.473+1 9.300−1 1.400+0 1.241−1 1.656−1 2.942−2 3.681−2 1.044+0 2.551+1 1.749−1 9.857−1 7.160−2 7.301−2 1.727−2 6.130+0 5.065+1 3.720−1 1.735+0 4.683−2 1.317−1 5.315−1 4.979+1 1.085−1 8.056−1 4.061−2 4.851+0 7.835+1 1.344−1 1.133+0 3.262−1 4.699+1 7.185−2 3.223+0 6.599+1 2.481−1
3.027−1 4.925−3 1.020−2 8.216−3 4.438−2 1.370−2 5.528−1 2.634−2 3.967+0 4.558−2 6.372−3 4.275−3 2.015−2 9.953−3 6.763−2 2.653−2 7.467−1 1.949−1 5.171+0 1.446+1 2.682+1 9.131−1 1.374+0 1.264−1 1.687−1 2.861−2 3.579−2 1.019+0 2.758+1 1.792−1 9.629−1 7.075−2 7.345−2 1.628−2 6.600+0 5.468+1 3.640−1 1.694+0 4.565−2 1.317−1 5.194−1 5.349+1 1.088−1 7.855−1 3.752−2 5.148+0 8.391+1 1.287−1 1.104+0 3.134−1 5.020+1 6.616−2 3.352+0 7.029+1 2.250−1
2.330−1 4.392−3 1.005−2 7.461−3 4.622−2 1.237−2 5.573−1 2.346−2 4.480+0 3.997−2 5.739−3 3.700−3 1.950−2 8.568−3 6.966−2 2.363−2 7.516−1 2.084−1 5.838+0 1.559+1 2.899+1 8.957−1 1.348+0 1.291−1 1.722−1 2.802−2 3.505−2 9.931−1 2.970+1 1.838−1 9.387−1 7.012−2 7.418−2 1.560−2 7.064+0 5.872+1 3.559−1 1.651+0 4.496−2 1.324−1 5.072−1 5.702+1 1.098−1 7.651−1 3.518−2 5.424+0 8.914+1 1.237−1 1.074+0 3.020−1 5.322+1 6.210−2 3.471+0 7.429+1 2.061−1
1.839−1 4.037−3 1.003−2 6.925−3 4.925−2 1.145−2 5.614−1 2.131−2 5.108+0 3.573−2 5.312−3 3.277−3 1.918−2 7.511−3 7.352−2 2.148−2 7.564−1 2.279−1 6.658+0 1.673+1 3.119+1 8.783−1 1.322+0 1.321−1 1.761−1 2.763−2 3.458−2 9.646−1 3.180+1 1.884−1 9.123−1 6.966−2 7.507−2 1.520−2 7.514+0 6.267+1 3.473−1 1.604+0 4.468−2 1.335−1 4.944−1 6.036+1 1.112−1 7.437−1 3.350−2 5.679+0 9.404+1 1.193−1 1.043+0 2.916−1 5.603+1 5.948−2 3.579+0 7.799+1 1.911−1
1.499−1 3.799−3 1.005−2 6.544−3 5.300−2 1.086−2 5.623−1 1.971−2 5.799+0 3.264−2 5.025−3 2.974−3 1.899−2 6.732−3 7.856−2 1.988−2 7.571−1 2.513−1 7.562+0 1.774+1 3.319+1 8.599−1 1.296+0 1.347−1 1.797−1 2.730−2 3.417−2 9.307−1 3.365+1 1.915−1 8.800−1 6.895−2 7.554−2 1.494−2 7.899+0 6.610+1 3.366−1 1.547+0 4.444−2 1.340−1 4.787−1 6.314+1 1.123−1 7.177−1 3.221−2 5.881+0 9.806+1 1.148−1 1.006+0 2.806−1 5.831+1 5.768−2 3.658+0 8.096+1 1.787−1
1.247−1 3.564−3 9.842−3 6.139−3 5.538−2 1.027−2 5.473−1 1.815−2 6.298+0 2.984−2 4.730−3 2.709−3 1.844−2 6.058−3 8.169−2 1.832−2 7.366−1 2.677−1 8.216+0 1.810+1 3.396+1 8.273−1 1.253+0 1.337−1 1.785−1 2.640−2 3.304−2 8.775−1 3.427+1 1.884−1 8.274−1 6.644−2 7.373−2 1.444−2 7.995+0 6.711+1 3.177−1 1.454+0 4.309−2 1.307−1 4.517−1 6.364+1 1.101−1 6.745−1 3.049−2 5.879+0 9.858+1 1.079−1 9.447−1 2.637−1 5.853+1 5.511−2 3.620+0 8.110+1 1.648−1
1.039−1 3.757−3 1.011−2 6.701−3 5.438−2 1.109−2 5.706−1 1.998−2 6.759+0 3.335−2 5.029−3 3.056−3 1.921−2 6.803−3 8.028−2 2.011−2 7.682−1 2.858−1 8.793+0 1.873+1 3.337+1 8.090−1 1.216+0 1.770−1 2.386−1 3.115−2 3.912−2 9.010−1 3.101+1 2.723−1 8.643−1 8.121−2 9.863−2 1.570−2 7.374+0 6.044+1 3.485−1 1.533+0 5.593−2 1.774−1 4.949−1 6.276+1 1.357−1 7.184−1 3.467−2 5.677+0 9.852+1 1.180−1 1.008+0 2.863−1 5.904+1 1.205−1 3.208+0 7.662+1 1.933−1
86
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 31 Effective collision strengths for transitions in Co XXV. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.540−1 2.960−1 1.338−2 4.051−3 7.426−3 1.019−2 1.521−2 2.673−3 9.738−4 1.819−3 1.863−3 2.795−3 1.111−3 1.474−3 1.039−3 4.162−4 7.812−4 7.141−4 1.072−3 5.883−4 7.811−4 7.648−5 9.518−5 2.652−2 9.508−4 1.439−2 3.796−3 4.900−2 7.106−3 3.019−4 2.982−3 1.257−3 8.946−3 2.213−3 1.546−3 9.267−4 1.432−4 1.188−3 5.988−4 3.362−3 1.030−3 8.047−4 5.540−4 7.456−5 7.411−5 1.929−3 3.937−3 3.294−2 1.896−2 9.700−2 6.001−4 1.273−3 7.254−3 4.527−3 1.826−2 1.696−3 3.425−3 2.831−4 6.040−4 2.978−3 1.934−3 6.994−3 9.751−4 1.836−3 1.299−4 1.818−4 1.034+0 1.942+0 7.112−2 1.068−1 6.137−2 1.123−2 2.044−2
1.575−1 3.023−1 1.585−2 5.377−3 9.392−3 1.133−2 1.715−2 3.009−3 1.366−3 2.584−3 2.241−3 3.341−3 1.483−3 1.976−3 1.002−3 4.814−4 9.027−4 7.596−4 1.144−3 6.194−4 8.230−4 8.176−5 1.016−4 3.903−2 4.250−3 1.586−2 6.454−3 5.011−2 1.121−2 8.507−4 3.381−3 1.972−3 9.785−3 3.042−3 2.322−3 1.713−3 2.444−4 1.153−3 6.432−4 3.517−3 1.089−3 8.636−4 5.724−4 8.171−5 7.359−5 9.890−3 7.623−3 3.866−2 2.446−2 1.027−1 1.788−3 2.095−3 8.615−3 5.838−3 2.037−2 3.108−3 5.408−3 4.946−4 6.877−4 2.919−3 2.049−3 7.347−3 1.029−3 1.963−3 1.330−4 1.951−4 9.973−1 1.915+0 9.409−2 1.437−1 6.782−2 1.343−2 2.448−2
1.652−1 3.162−1 1.524−2 5.372−3 9.628−3 1.145−2 1.732−2 2.889−3 1.312−3 2.486−3 2.155−3 3.214−3 1.378−3 1.833−3 9.990−4 4.837−4 9.128−4 7.504−4 1.130−3 6.057−4 8.050−4 7.665−5 9.526−5 4.321−2 3.440−3 1.566−2 6.100−3 5.183−2 1.061−2 7.066−4 3.212−3 1.738−3 9.863−3 2.724−3 2.158−3 1.451−3 2.197−4 1.127−3 6.056−4 3.585−3 1.021−3 8.651−4 5.313−4 7.827−5 6.695−5 7.810−3 6.932−3 3.777−2 2.407−2 1.054−1 1.468−3 1.826−3 8.109−3 5.440−3 2.028−2 2.689−3 4.929−3 4.446−4 6.371−4 2.849−3 1.979−3 7.416−3 9.738−4 1.937−3 1.224−4 1.844−4 1.059+0 2.024+0 9.230−2 1.404−1 6.673−2 1.407−2 2.573−2
1.738−1 3.322−1 1.478−2 5.457−3 9.928−3 1.150−2 1.737−2 2.801−3 1.292−3 2.449−3 2.078−3 3.106−3 1.282−3 1.705−3 1.001−3 4.955−4 9.392−4 7.399−4 1.115−3 5.901−4 7.845−4 7.079−5 8.796−5 4.452−2 2.791−3 1.536−2 5.510−3 5.407−2 9.535−3 5.882−4 3.070−3 1.514−3 1.006−2 2.390−3 2.037−3 1.202−3 1.987−4 1.107−3 5.621−4 3.690−3 9.344−4 8.757−4 4.810−4 7.501−5 5.922−5 6.213−3 6.122−3 3.653−2 2.318−2 1.087−1 1.214−3 1.578−3 7.645−3 5.047−3 2.040−2 2.297−3 4.537−3 4.023−4 5.852−4 2.778−3 1.894−3 7.540−3 9.089−4 1.920−3 1.103−4 1.734−4 1.142+0 2.168+0 8.802−2 1.335−1 6.599−2 1.558−2 2.851−2
1.838−1 3.509−1 1.449−2 5.736−3 1.053−2 1.164−2 1.754−2 2.753−3 1.322−3 2.508−3 2.026−3 3.034−3 1.207−3 1.605−3 1.009−3 5.205−4 9.898−4 7.301−4 1.100−3 5.746−4 7.643−4 6.460−5 8.029−5 4.257−2 2.294−3 1.506−2 4.848−3 5.741−2 8.272−3 4.972−4 2.966−3 1.312−3 1.046−2 2.060−3 1.986−3 9.821−4 1.805−4 1.091−3 5.135−4 3.850−3 8.325−4 9.018−4 4.240−4 7.249−5 5.087−5 5.037−3 5.314−3 3.528−2 2.229−2 1.139−1 1.023−3 1.363−3 7.265−3 4.702−3 2.090−2 1.966−3 4.290−3 3.661−4 5.313−4 2.706−3 1.800−3 7.752−3 8.398−4 1.926−3 9.763−5 1.634−4 1.248+0 2.352+0 8.291−2 1.255−1 6.579−2 1.823−2 3.342−2
1.965−1 3.740−1 1.438−2 6.320−3 1.168−2 1.196−2 1.799−2 2.742−3 1.416−3 2.689−3 2.006−3 3.010−3 1.156−3 1.537−3 1.022−3 5.636−4 1.075−3 7.240−4 1.092−3 5.618−4 7.476−4 5.868−5 7.296−5 3.826−2 1.956−3 1.485−2 4.238−3 6.246−2 7.039−3 4.324−4 2.899−3 1.138−3 1.112−2 1.746−3 2.018−3 7.958−4 1.655−4 1.080−3 4.623−4 4.088−3 7.214−4 9.501−4 3.648−4 7.124−5 4.257−5 4.260−3 4.609−3 3.428−2 2.178−2 1.224−1 8.907−4 1.180−3 6.977−3 4.435−3 2.189−2 1.710−3 4.216−3 3.370−4 4.768−4 2.638−3 1.711−3 8.098−3 7.743−4 1.970−3 8.546−5 1.556−4 1.370+0 2.566+0 7.819−2 1.182−1 6.613−2 2.226−2 4.090−2
2.123−1 4.025−1 1.445−2 7.302−3 1.355−2 1.251−2 1.880−2 2.764−3 1.587−3 3.018−3 2.021−3 3.039−3 1.128−3 1.501−3 1.041−3 6.311−4 1.207−3 7.246−4 1.094−3 5.536−4 7.372−4 5.360−5 6.669−5 3.306−2 1.776−3 1.476−2 3.741−3 6.971−2 5.957−3 3.924−4 2.864−3 9.930−4 1.211−2 1.459−3 2.132−3 6.443−4 1.551−4 1.074−3 4.124−4 4.426−3 6.101−4 1.025−3 3.085−4 7.154−5 3.497−5 3.858−3 4.056−3 3.365−2 2.192−2 1.351−1 8.119−4 1.030−3 6.776−3 4.272−3 2.349−2 1.530−3 4.315−3 3.173−4 4.251−4 2.581−3 1.642−3 8.627−3 7.209−4 2.065−3 7.484−5 1.511−4 1.501+0 2.803+0 7.437−2 1.123−1 6.686−2 2.785−2 5.129−2
2.304−1 4.353−1 1.461−2 8.707−3 1.623−2 1.325−2 1.989−2 2.803−3 1.835−3 3.498−3 2.065−3 3.109−3 1.117−3 1.487−3 1.061−3 7.244−4 1.389−3 7.319−4 1.105−3 5.497−4 7.325−4 4.962−5 6.179−5 2.815−2 1.740−3 1.476−2 3.370−3 7.921−2 5.071−3 3.751−4 2.848−3 8.754−4 1.341−2 1.211−3 2.312−3 5.260−4 1.498−4 1.071−3 3.671−4 4.861−3 5.074−4 1.124−3 2.593−4 7.307−5 2.852−5 3.787−3 3.655−3 3.332−2 2.277−2 1.522−1 7.816−4 9.105−4 6.638−3 4.223−3 2.570−2 1.418−3 4.555−3 3.089−4 3.789−4 2.532−3 1.602−3 9.341−3 6.838−4 2.205−3 6.626−5 1.494−4 1.630+0 3.041+0 7.138−2 1.077−1 6.764−2 3.486−2 6.434−2
2.455−1 4.627−1 1.459−2 1.020−2 1.907−2 1.382−2 2.074−2 2.798−3 2.092−3 3.995−3 2.088−3 3.148−3 1.098−3 1.463−3 1.061−3 8.173−4 1.571−3 7.308−4 1.105−3 5.395−4 7.194−4 4.609−5 5.745−5 2.393−2 1.785−3 1.457−2 3.074−3 8.849−2 4.343−3 3.697−4 2.796−3 7.753−4 1.461−2 9.993−4 2.476−3 4.338−4 1.471−4 1.051−3 3.251−4 5.246−3 4.165−4 1.207−3 2.175−4 7.385−5 2.320−5 3.898−3 3.341−3 3.268−2 2.378−2 1.689−1 7.763−4 8.093−4 6.442−3 4.200−3 2.773−2 1.338−3 4.785−3 3.055−4 3.364−4 2.453−3 1.568−3 9.972−3 6.524−4 2.325−3 5.902−5 1.472−4 1.718+0 3.207+0 6.807−2 1.027−1 6.715−2 4.169−2 7.704−2
2.542−1 4.809−1 1.498−2 1.102−2 2.056−2 1.429−2 2.136−2 2.968−3 2.233−3 4.239−3 2.111−3 3.177−3 1.118−3 1.484−3 1.143−3 8.757−4 1.668−3 7.323−4 1.104−3 5.552−4 7.378−4 4.717−5 5.871−5 1.775−2 1.678−3 1.510−2 2.915−3 9.387−2 3.874−3 3.465−4 3.034−3 7.611−4 1.518−2 9.286−4 2.594−3 3.977−4 1.378−4 1.185−3 3.310−4 5.399−3 4.034−4 1.291−3 2.230−4 7.573−5 2.429−5 3.642−3 3.142−3 3.360−2 2.432−2 1.779−1 7.276−4 7.921−4 6.892−3 4.230−3 2.867−2 1.311−3 4.940−3 2.860−4 3.418−4 2.718−3 1.585−3 1.022−2 6.816−4 2.465−3 5.991−5 1.501−4 1.868+0 3.427+0 6.706−2 1.011−1 6.949−2 4.505−2 8.353−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
87
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.640−2 3.918−2 2.609−2 3.477−2 1.134−2 2.397−3 4.490−3 5.580−3 8.332−3 3.065−3 4.097−3 4.805−3 5.997−3 1.164−1 1.374+0 1.811−2 4.064−3 6.534−2 9.149−3 8.113−2 1.183−2 8.709−2 1.273−2 1.148−3 1.244−2 2.516−3 1.626−2 3.327−3 9.551−3 3.093−3 1.088−2 3.751−3 3.271−1 2.659+0 8.341−3 9.916−3 1.415−1 3.213−2 1.633−1 4.196−2 1.612−1 2.320−3 2.634−3 2.752−2 7.466−3 3.309−2 6.710−3 1.854−2 8.863−3 2.123−2 8.524−2 3.513−3 6.693−3 6.799−3 1.277−1 1.615−2 5.588−1 2.831−2 1.139−3 2.321−3 2.716−3 2.457−2 6.127−3 8.644−2 9.624−3 2.517−2 5.649−3 5.311−3 4.630−3 1.579−2 1.625−2 2.002−1 7.086−2 8.163−1
2.826−2 4.331−2 3.306−2 4.482−2 1.116−2 2.715−3 5.037−3 5.603−3 8.401−3 3.542−3 4.736−3 4.968−3 6.212−3 1.432−1 1.412+0 6.133−2 9.763−3 6.551−2 1.269−2 8.245−2 1.755−2 8.897−2 2.158−2 1.427−3 1.156−2 2.512−3 1.806−2 3.659−3 9.756−3 3.266−3 1.128−2 3.817−3 3.790−1 2.731+0 2.114−2 1.431−2 1.463−1 4.183−2 1.780−1 5.314−2 1.788−1 2.921−3 2.686−3 2.575−2 8.268−3 3.675−2 7.011−3 1.908−2 9.114−3 2.205−2 2.418−1 9.547−3 1.567−2 1.684−2 1.373−1 3.197−2 5.666−1 5.293−2 1.699−3 2.891−3 3.138−3 2.407−2 6.453−3 9.093−2 1.012−2 2.460−2 5.561−3 1.661−2 1.193−2 3.687−2 3.154−2 2.278−1 1.024−1 8.678−1
2.874−2 4.374−2 3.176−2 4.284−2 1.126−2 2.929−3 5.442−3 5.739−3 8.608−3 3.383−3 4.525−3 4.865−3 6.083−3 1.386−1 1.482+0 5.704−2 8.282−3 6.515−2 1.175−2 8.836−2 1.590−2 9.111−2 1.887−2 1.347−3 1.165−2 2.462−3 1.918−2 3.455−3 9.847−3 2.986−3 1.156−2 3.544−3 3.896−1 2.857+0 1.790−2 1.318−2 1.446−1 4.062−2 1.866−1 5.040−2 1.791−1 2.766−3 2.618−3 2.591−2 8.246−3 3.867−2 6.667−3 1.902−2 8.836−3 2.234−2 2.229−1 7.762−3 1.330−2 1.395−2 1.348−1 2.691−2 5.909−1 4.446−2 1.487−3 2.637−3 2.827−3 2.388−2 5.819−3 9.393−2 9.020−3 2.559−2 4.947−3 1.318−2 9.692−3 3.132−2 2.656−2 2.203−1 9.431−2 8.938−1
2.968−2 4.487−2 3.054−2 4.105−2 1.142−2 3.275−3 6.099−3 5.936−3 8.903−3 3.214−3 4.299−3 4.781−3 5.977−3 1.318−1 1.588+0 4.914−2 7.530−3 6.512−2 1.107−2 9.779−2 1.438−2 9.460−2 1.636−2 1.328−3 1.178−2 2.426−3 2.082−2 3.233−3 9.999−3 2.682−3 1.194−2 3.255−3 4.074−1 3.071+0 1.628−2 1.235−2 1.437−1 4.027−2 2.017−1 4.834−2 1.818−1 2.743−3 2.573−3 2.616−2 8.314−3 4.155−2 6.310−3 1.904−2 8.570−3 2.279−2 1.900−1 6.365−3 1.156−2 1.139−2 1.327−1 2.214−2 6.289−1 3.642−2 1.313−3 2.440−3 2.512−3 2.370−2 5.127−3 9.831−2 7.806−3 2.712−2 4.302−3 1.057−2 7.757−3 2.682−2 2.190−2 2.135−1 8.746−2 9.390−1
3.121−2 4.694−2 2.962−2 3.971−2 1.163−2 3.798−3 7.093−3 6.201−3 9.301−3 3.052−3 4.083−3 4.736−3 5.920−3 1.244−1 1.729+0 4.046−2 7.472−3 6.547−2 1.073−2 1.119−1 1.316−2 9.965−2 1.431−2 1.375−3 1.195−2 2.412−3 2.317−2 3.012−3 1.023−2 2.381−3 1.241−2 2.974−3 4.346−1 3.371+0 1.620−2 1.193−2 1.439−1 4.134−2 2.261−1 4.731−2 1.878−1 2.859−3 2.558−3 2.651−2 8.526−3 4.572−2 5.978−3 1.919−2 8.347−3 2.339−2 1.539−1 5.342−3 1.050−2 9.367−3 1.313−1 1.811−2 6.852−1 2.951−2 1.172−3 2.303−3 2.211−3 2.357−2 4.431−3 1.045−1 6.579−3 2.929−2 3.683−3 8.696−3 6.206−3 2.370−2 1.798−2 2.086−1 8.323−2 1.012+0
3.333−2 4.993−2 2.904−2 3.887−2 1.187−2 4.540−3 8.509−3 6.535−3 9.801−3 2.915−3 3.900−3 4.745−3 5.931−3 1.179−1 1.895+0 3.288−2 8.081−3 6.616−2 1.074−2 1.316−1 1.225−2 1.061−1 1.279−2 1.493−3 1.214−2 2.426−3 2.636−2 2.809−3 1.054−2 2.109−3 1.293−2 2.726−3 4.689−1 3.722+0 1.760−2 1.191−2 1.451−1 4.408−2 2.615−1 4.734−2 1.970−1 3.131−3 2.575−3 2.693−2 8.937−3 5.147−2 5.708−3 1.950−2 8.186−3 2.411−2 1.217−1 4.644−3 1.011−2 7.883−3 1.308−1 1.495−2 7.631−1 2.396−2 1.061−3 2.233−3 1.947−3 2.350−2 3.785−3 1.129−1 5.439−3 3.210−2 3.140−3 7.428−3 5.027−3 2.199−2 1.490−2 2.056−1 8.221−2 1.117+0
3.587−2 5.360−2 2.875−2 3.844−2 1.213−2 5.540−3 1.042−2 6.924−3 1.038−2 2.814−3 3.766−3 4.813−3 6.015−3 1.127−1 2.074+0 2.710−2 9.335−3 6.706−2 1.102−2 1.577−1 1.161−2 1.136−1 1.176−2 1.693−3 1.235−2 2.473−3 3.054−2 2.639−3 1.092−2 1.886−3 1.346−2 2.525−3 5.067−1 4.091+0 2.044−2 1.220−2 1.471−1 4.860−2 3.094−1 4.828−2 2.085−1 3.575−3 2.627−3 2.741−2 9.593−3 5.907−2 5.520−3 1.997−2 8.091−3 2.487−2 9.625−2 4.203−3 1.033−2 6.884−3 1.310−1 1.261−2 8.652−1 1.975−2 9.794−4 2.236−3 1.733−3 2.351−2 3.235−3 1.239−1 4.462−3 3.546−2 2.702−3 6.627−3 4.165−3 2.159−2 1.263−2 2.043−1 8.458−2 1.260+0
3.852−2 5.746−2 2.864−2 3.826−2 1.235−2 6.779−3 1.279−2 7.322−3 1.098−2 2.748−3 3.677−3 4.919−3 6.147−3 1.086−1 2.250+0 2.307−2 1.114−2 6.790−2 1.146−2 1.895−1 1.117−2 1.211−1 1.113−2 1.965−3 1.251−2 2.540−3 3.560−2 2.505−3 1.131−2 1.717−3 1.391−2 2.371−3 5.439−1 4.446+0 2.450−2 1.268−2 1.492−1 5.465−2 3.684−1 4.968−2 2.206−1 4.176−3 2.701−3 2.784−2 1.047−2 6.831−2 5.405−3 2.048−2 8.033−3 2.553−2 7.740−2 3.947−3 1.107−2 6.275−3 1.314−1 1.095−2 9.883−1 1.668−2 9.241−4 2.307−3 1.575−3 2.352−2 2.795−3 1.370−1 3.682−3 3.903−2 2.375−3 6.151−3 3.554−3 2.229−2 1.103−2 2.037−1 8.990−2 1.434+0
4.018−2 5.987−2 2.814−2 3.757−2 1.231−2 7.960−3 1.504−2 7.540−3 1.131−2 2.664−3 3.565−3 4.947−3 6.182−3 1.039−1 2.368+0 2.019−2 1.298−2 6.738−2 1.173−2 2.192−1 1.069−2 1.254−1 1.059−2 2.230−3 1.241−2 2.567−3 4.019−2 2.365−3 1.144−2 1.573−3 1.399−2 2.224−3 5.675−1 4.677+0 2.862−2 1.297−2 1.485−1 6.030−2 4.236−1 5.026−2 2.274−1 4.761−3 2.731−3 2.768−2 1.125−2 7.667−2 5.253−3 2.059−2 7.859−3 2.556−2 6.349−2 3.750−3 1.189−2 5.860−3 1.295−1 9.698−3 1.098+0 1.436−2 8.753−4 2.378−3 1.447−3 2.311−2 2.436−3 1.480−1 3.066−3 4.156−2 2.117−3 5.796−3 3.093−3 2.325−2 9.801−3 2.000−1 9.525−2 1.591+0
4.224−2 6.277−2 2.850−2 3.799−2 1.337−2 8.468−3 1.599−2 7.827−3 1.171−2 2.637−3 3.529−3 5.226−3 6.523−3 1.042−1 2.493+0 1.550−2 1.405−2 7.137−2 1.254−2 2.353−1 1.086−2 1.315−1 1.042−2 2.397−3 1.404−2 2.825−3 4.169−2 2.401−3 1.160−2 1.573−3 1.442−2 2.320−3 5.960−1 4.928+0 3.074−2 1.378−2 1.571−1 6.355−2 4.519−1 5.187−2 2.369−1 5.078−3 2.998−3 3.109−2 1.160−2 7.927−2 5.301−3 2.087−2 8.133−3 2.630−2 4.680−2 3.544−3 1.193−2 5.495−3 1.330−1 9.047−3 1.161+0 1.331−2 8.829−4 2.473−3 1.488−3 2.457−2 2.495−3 1.541−1 3.144−3 4.387−2 2.297−3 5.389−3 2.781−3 2.299−2 9.215−3 2.047−1 9.804−2 1.675+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
88
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.712−3 1.900−3 5.718−3 6.130−3 3.995−2 1.660−2 1.281−1 9.161−3 3.748−2 3.527+0 6.670+0 3.187−1 4.782−1 2.884−2 3.860−2 1.880−1 2.704−2 4.874−2 5.654−2 8.369−2 6.166−2 8.199−2 3.136−2 3.916−2 4.080−1 6.050+0 5.210−2 2.494−1 2.421−2 1.377−2 1.978−1 2.470−2 1.435−1 2.672−2 1.818−1 2.158−2 1.111−1 2.143−2 1.365+0 1.171+1 1.024−1 4.465−1 2.939−2 2.697−2 4.231−1 6.497−2 2.971−1 8.188−2 3.358−1 6.614−2 2.013−1 2.056−1 7.420+0 4.836−2 1.219−2 2.204−2 1.712−2 4.087−1 2.639−2 7.792−1 3.820−2 5.000−1 3.868−2 5.569−1 9.540+0 1.849−2 1.102−2 4.827−2 2.679−2 6.276−1 9.793−2 1.141+0 9.893−2 7.123−1
2.546−3 2.325−3 6.670−3 6.467−3 3.966−2 1.743−2 1.348−1 9.035−3 3.673−2 3.683+0 7.067+0 3.433−1 5.557−1 7.295−2 1.111−1 1.792−1 2.833−2 5.087−2 5.562−2 8.274−2 6.199−2 8.259−2 3.252−2 4.066−2 4.458−1 6.315+0 1.053−1 3.079−1 9.076−2 1.768−2 1.808−1 2.295−2 1.452−1 2.519−2 1.798−1 2.237−2 1.135−1 2.242−2 1.542+0 1.477+1 2.154−1 6.735−1 3.966−2 2.570−2 3.854−1 6.344−2 2.995−1 8.238−2 3.336−1 6.814−2 2.058−1 3.345−1 8.210+0 2.286−1 1.649−2 2.925−2 1.745−2 3.853−1 2.578−2 7.739−1 3.636−2 4.940−1 3.704−2 1.009+0 1.342+1 2.434−2 1.136−2 5.812−2 2.641−2 5.933−1 9.565−2 1.131+0 9.643−2 7.042−1
2.232−3 2.046−3 6.134−3 5.832−3 3.898−2 1.645−2 1.387−1 8.453−3 3.788−2 4.010+0 7.593+0 3.334−1 5.337−1 6.268−2 9.380−2 1.820−1 3.351−2 6.045−2 5.934−2 8.822−2 6.249−2 8.326−2 3.268−2 4.085−2 4.267−1 6.892+0 9.430−2 2.892−1 7.263−2 1.869−2 1.839−1 2.411−2 1.669−1 2.526−2 1.908−1 2.217−2 1.140−1 2.122−2 1.686+0 1.564+1 1.852−1 6.096−1 4.147−2 2.681−2 3.934−1 6.816−2 3.406−1 8.538−2 3.527−1 6.669−2 2.058−1 2.948−1 9.452+0 1.788−1 1.517−2 2.905−2 1.720−2 3.916−1 2.512−2 8.518−1 3.430−2 5.190−1 3.443−2 1.101+0 1.542+1 2.266−2 1.078−2 5.823−2 2.568−2 6.023−1 9.903−2 1.243+0 9.631−2 7.379−1
1.976−3 1.776−3 5.655−3 5.141−3 3.832−2 1.544−2 1.444−1 7.897−3 3.977−2 4.388+0 8.222+0 3.235−1 5.109−1 5.355−2 7.854−2 1.854−1 4.101−2 7.441−2 6.411−2 9.524−2 6.293−2 8.385−2 3.309−2 4.137−2 4.085−1 7.566+0 8.458−2 2.719−1 5.667−2 2.105−2 1.875−1 2.573−2 1.970−1 2.533−2 2.045−1 2.211−2 1.145−1 2.010−2 1.849+0 1.657+1 1.574−1 5.503−1 4.644−2 2.849−2 4.028−1 7.465−2 3.977−1 8.934−2 3.764−1 6.534−2 2.058−1 2.591−1 1.076+1 1.353−1 1.458−2 3.035−2 1.724−2 3.987−1 2.464−2 9.579−1 3.230−2 5.500−1 3.203−2 1.189+0 1.740+1 2.197−2 1.036−2 6.061−2 2.518−2 6.127−1 1.045−1 1.395+0 9.709−2 7.796−1
1.765−3 1.522−3 5.260−3 4.444−3 3.774−2 1.456−2 1.528−1 7.441−3 4.256−2 4.799+0 8.934+0 3.148−1 4.907−1 4.656−2 6.690−2 1.893−1 5.148−2 9.393−2 6.977−2 1.036−1 6.328−2 8.432−2 3.377−2 4.222−2 3.927−1 8.296+0 7.746−2 2.576−1 4.420−2 2.495−2 1.913−1 2.774−2 2.379−1 2.539−2 2.204−1 2.220−2 1.149−1 1.914−2 2.021+0 1.761+1 1.351−1 5.021−1 5.493−2 3.064−2 4.130−1 8.345−2 4.753−1 9.416−2 4.041−1 6.422−2 2.058−1 2.303−1 1.203+1 1.016−1 1.449−2 3.326−2 1.760−2 4.062−1 2.442−2 1.100+0 3.052−2 5.857−1 3.007−2 1.272+0 1.927+1 2.197−2 1.007−2 6.559−2 2.496−2 6.238−1 1.129−1 1.599+0 9.887−2 8.280−1
1.600−3 1.297−3 4.982−3 3.800−3 3.729−2 1.393−2 1.644−1 7.142−3 4.630−2 5.229+0 9.707+0 3.074−1 4.742−1 4.175−2 5.887−2 1.931−1 6.560−2 1.201−1 7.595−2 1.127−1 6.357−2 8.469−2 3.467−2 4.334−2 3.795−1 9.049+0 7.301−2 2.463−1 3.517−2 3.059−2 1.951−1 3.002−2 2.919−1 2.544−2 2.376−1 2.245−2 1.154−1 1.843−2 2.193+0 1.876+1 1.185−1 4.656−1 6.739−2 3.309−2 4.234−1 9.510−2 5.777−1 9.952−2 4.341−1 6.342−2 2.061−1 2.088−1 1.320+1 7.734−2 1.475−2 3.795−2 1.833−2 4.137−1 2.449−2 1.285+0 2.906−2 6.240−1 2.864−2 1.350+0 2.099+1 2.244−2 9.871−3 7.357−2 2.503−2 6.349−1 1.248−1 1.866+0 1.015−1 8.805−1
1.479−3 1.109−3 4.850−3 3.250−3 3.700−2 1.365−2 1.797−1 7.025−3 5.084−2 5.666+0 1.052+1 3.009−1 4.607−1 3.876−2 5.380−2 1.967−1 8.375−2 1.537−1 8.214−2 1.219−1 6.385−2 8.505−2 3.569−2 4.463−2 3.683−1 9.804+0 7.075−2 2.375−1 2.895−2 3.810−2 1.986−1 3.235−2 3.603−1 2.550−2 2.546−1 2.280−2 1.160−1 1.796−2 2.361+0 1.998+1 1.067−1 4.386−1 8.403−2 3.562−2 4.332−1 1.099−1 7.072−1 1.050−1 4.642−1 6.301−2 2.068−1 1.932−1 1.428+1 6.087−2 1.519−2 4.450−2 1.943−2 4.206−1 2.478−2 1.517+0 2.799−2 6.619−1 2.774−2 1.422+0 2.254+1 2.314−2 9.759−3 8.476−2 2.533−2 6.454−1 1.408−1 2.202+0 1.047−1 9.328−1
1.396−3 9.608−4 4.859−3 2.812−3 3.679−2 1.375−2 1.982−1 7.054−3 5.571−2 6.079+0 1.130+1 2.947−1 4.487−1 3.702−2 5.076−2 1.993−1 1.052−1 1.932−1 8.751−2 1.300−1 6.403−2 8.529−2 3.664−2 4.582−2 3.577−1 1.051+1 6.989−2 2.302−1 2.478−2 4.709−2 2.012−1 3.442−2 4.400−1 2.554−2 2.692−1 2.315−2 1.165−1 1.769−2 2.514+0 2.116+1 9.829−2 4.180−1 1.040−1 3.785−2 4.408−1 1.270−1 8.583−1 1.096−1 4.899−1 6.282−2 2.075−1 1.816−1 1.521+1 5.008−2 1.566−2 5.249−2 2.076−2 4.256−1 2.510−2 1.785+0 2.722−2 6.941−1 2.720−2 1.485+0 2.388+1 2.386−2 9.697−3 9.844−2 2.567−2 6.529−1 1.599−1 2.592+0 1.077−1 9.772−1
1.323−3 8.394−4 4.885−3 2.453−3 3.599−2 1.388−2 2.137−1 7.044−3 5.915−2 6.325+0 1.178+1 2.839−1 4.309−1 3.549−2 4.825−2 1.975−1 1.248−1 2.294−1 8.989−2 1.336−1 6.301−2 8.394−2 3.675−2 4.595−2 3.418−1 1.093+1 6.863−2 2.203−1 2.174−2 5.532−2 1.992−1 3.537−2 5.114−1 2.511−2 2.749−1 2.303−2 1.149−1 1.725−2 2.597+0 2.180+1 9.094−2 3.956−1 1.223−1 3.887−2 4.380−1 1.416−1 9.930−1 1.109−1 4.996−1 6.167−2 2.044−1 1.702−1 1.568+1 4.267−2 1.578−2 5.970−2 2.168−2 4.209−1 2.490−2 2.019+0 2.624−2 7.045−1 2.645−2 1.508+0 2.451+1 2.403−2 9.498−3 1.106−1 2.548−2 6.458−1 1.762−1 2.931+0 1.080−1 9.913−1
1.334−3 8.533−4 5.075−3 2.514−3 3.818−2 1.442−2 2.223−1 7.511−3 6.239−2 6.517+0 1.214+1 2.954−1 4.447−1 3.465−2 4.635−2 2.076−1 1.220−1 2.249−1 9.023−2 1.337−1 1.512−1 2.044−1 4.074−2 5.093−2 3.604−1 1.131+1 6.857−2 2.264−1 1.853−2 5.277−2 2.146−1 3.593−2 5.172−1 3.083−2 2.818−1 2.581−2 1.274−1 1.941−2 2.616+0 2.236+1 8.772−2 3.991−1 1.151−1 3.946−2 4.681−1 1.473−1 1.001+0 1.169−1 5.140−1 6.914−2 2.276−1 1.722−1 1.669+1 3.343−2 1.547−2 5.562−2 1.166−1 4.356−1 2.597−2 2.107+0 4.246−2 7.330−1 2.892−2 1.693+0 2.585+1 2.353−2 2.345−2 1.506−1 2.658−2 6.679−1 1.983−1 3.056+0 1.140−1 1.033+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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89
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.840−1 4.655−3 9.498−3 9.863−3 3.622−2 1.865−2 5.168−1 3.859−2 2.803+0 7.012−2 6.223−3 5.672−3 2.007−2 1.504−2 5.829−2 3.867−2 7.027−1 1.770−1 3.664+0 9.081+0 1.718+1 9.009−1 1.350+0 1.019−1 1.363−1 2.880−2 3.612−2 1.050+0 1.652+1 1.403−1 9.743−1 6.798−2 6.182−2 1.965−2 3.688+0 3.133+1 3.663−1 1.728+0 4.639−2 1.146−1 5.339−1 2.249+1 9.828−2 8.071−1 4.897−2 1.763+0 3.131+1 1.439−1 1.141+0 3.484−1 1.782+1 9.245−2 9.346−1 2.362+1 3.277−1
6.116−1 6.881−3 1.126−2 1.079−2 4.085−2 1.832−2 5.008−1 3.598−2 2.798+0 6.445−2 9.377−3 6.593−3 2.274−2 1.460−2 6.571−2 3.619−2 6.805−1 1.711−1 3.651+0 1.028+1 1.906+1 8.776−1 1.320+0 1.104−1 1.473−1 2.935−2 3.672−2 9.990−1 1.943+1 1.537−1 9.411−1 6.825−2 6.723−2 1.886−2 4.687+0 3.853+1 3.557−1 1.661+0 4.703−2 1.234−1 5.108−1 3.683+1 1.018−1 7.751−1 4.602−2 3.739+0 5.825+1 1.373−1 1.096+0 3.287−1 3.493+1 8.289−2 2.638+0 4.941+1 2.875−1
4.858−1 5.796−3 1.042−2 9.581−3 4.007−2 1.635−2 5.033−1 3.201−2 2.990+0 5.692−2 7.862−3 5.619−3 2.096−2 1.275−2 6.340−2 3.218−2 6.826−1 1.703−1 3.899+0 1.121+1 2.068+1 8.649−1 1.301+0 1.117−1 1.491−1 2.821−2 3.529−2 9.792−1 2.115+1 1.566−1 9.245−1 6.706−2 6.699−2 1.740−2 5.126+0 4.214+1 3.486−1 1.627+0 4.499−2 1.219−1 4.997−1 4.060+1 1.005−1 7.572−1 4.187−2 4.073+0 6.416+1 1.305−1 1.068+0 3.148−1 3.840+1 7.472−2 2.790+0 5.416+1 2.594−1
3.738−1 4.983−3 9.837−3 8.507−3 3.983−2 1.447−2 5.066−1 2.816−2 3.249+0 4.958−2 6.736−3 4.769−3 1.959−2 1.097−2 6.203−2 2.831−2 6.856−1 1.723−1 4.234+0 1.221+1 2.247+1 8.524−1 1.283+0 1.135−1 1.515−1 2.722−2 3.405−2 9.596−1 2.301+1 1.600−1 9.085−1 6.603−2 6.707−2 1.614−2 5.577+0 4.590+1 3.418−1 1.594+0 4.332−2 1.211−1 4.890−1 4.433+1 9.984−2 7.401−1 3.816−2 4.391+0 6.990+1 1.244−1 1.042+0 3.017−1 4.175+1 6.758−2 2.932+0 5.870+1 2.334−1
2.849−1 4.382−3 9.475−3 7.609−3 4.041−2 1.283−2 5.102−1 2.476−2 3.592+0 4.304−2 5.906−3 4.060−3 1.860−2 9.383−3 6.199−2 2.490−2 6.893−1 1.783−1 4.681+0 1.324+1 2.440+1 8.396−1 1.264+0 1.156−1 1.544−1 2.642−2 3.307−2 9.395−1 2.494+1 1.640−1 8.925−1 6.522−2 6.748−2 1.516−2 6.027+0 4.972+1 3.351−1 1.561+0 4.213−2 1.210−1 4.787−1 4.790+1 9.995−2 7.236−1 3.511−2 4.686+0 7.533+1 1.191−1 1.017+0 2.900−1 4.489+1 6.192−2 3.061+0 6.293+1 2.111−1
2.191−1 3.950−3 9.295−3 6.911−3 4.200−2 1.154−2 5.141−1 2.200−2 4.039+0 3.763−2 5.314−3 3.499−3 1.798−2 8.066−3 6.357−2 2.213−2 6.936−1 1.895−1 5.263+0 1.431+1 2.641+1 8.255−1 1.242+0 1.181−1 1.577−1 2.585−2 3.235−2 9.178−1 2.690+1 1.683−1 8.758−1 6.463−2 6.819−2 1.447−2 6.468+0 5.352+1 3.284−1 1.525+0 4.143−2 1.216−1 4.684−1 5.128+1 1.008−1 7.067−1 3.279−2 4.956+0 8.040+1 1.146−1 9.924−1 2.796−1 4.781+1 5.784−2 3.177+0 6.683+1 1.929−1
1.727−1 3.657−3 9.253−3 6.409−3 4.470−2 1.064−2 5.179−1 1.992−2 4.599+0 3.351−2 4.911−3 3.083−3 1.766−2 7.051−3 6.693−2 2.006−2 6.979−1 2.066−1 5.994+0 1.537+1 2.845+1 8.099−1 1.219+0 1.207−1 1.613−1 2.547−2 3.188−2 8.934−1 2.885+1 1.729−1 8.580−1 6.426−2 6.913−2 1.405−2 6.895+0 5.723+1 3.213−1 1.486+0 4.114−2 1.227−1 4.577−1 5.446+1 1.021−1 6.888−1 3.113−2 5.203+0 8.511+1 1.107−1 9.666−1 2.704−1 5.051+1 5.518−2 3.283+0 7.040+1 1.785−1
1.406−1 3.464−3 9.279−3 6.061−3 4.826−2 1.008−2 5.200−1 1.842−2 5.243+0 3.053−2 4.647−3 2.789−3 1.752−2 6.307−3 7.165−2 1.856−2 7.002−1 2.282−1 6.838+0 1.636+1 3.039+1 7.926−1 1.193+0 1.233−1 1.648−1 2.520−2 3.155−2 8.643−1 3.065+1 1.773−1 8.385−1 6.393−2 7.011−2 1.382−2 7.277+0 6.060+1 3.128−1 1.439+0 4.101−2 1.236−1 4.451−1 5.725+1 1.035−1 6.676−1 2.993−2 5.412+0 8.919+1 1.069−1 9.366−1 2.613−1 5.284+1 5.350−2 3.369+0 7.345+1 1.670−1
1.175−1 3.290−3 9.165−3 5.734−3 5.113−2 9.594−3 5.113−1 1.709−2 5.785+0 2.806−2 4.409−3 2.551−3 1.716−2 5.703−3 7.548−2 1.722−2 6.881−1 2.466−1 7.549+0 1.690+1 3.148+1 7.643−1 1.150+0 1.235−1 1.652−1 2.458−2 3.078−2 8.196−1 3.161+1 1.782−1 8.064−1 6.255−2 6.979−2 1.347−2 7.455+0 6.229+1 2.985−1 1.366+0 4.019−2 1.219−1 4.245−1 5.844+1 1.026−1 6.340−1 2.857−2 5.476+0 9.079+1 1.015−1 8.890−1 2.481−1 5.371+1 5.156−2 3.371+0 7.450+1 1.553−1
9.698−2 3.452−3 9.370−3 6.297−3 5.078−2 1.092−2 5.260−1 1.892−2 6.050+0 3.130−2 4.624−3 2.941−3 1.783−2 7.068−3 7.498−2 1.907−2 7.085−1 2.575−1 7.872+0 1.711+1 3.046+1 7.546−1 1.135+0 1.640−1 2.212−1 2.895−2 3.638−2 8.409−1 2.867+1 1.942−1 8.061−1 6.608−2 7.643−2 1.469−2 6.813+0 5.563+1 3.261−1 1.430+0 5.272−2 1.667−1 4.638−1 5.574+1 1.237−1 6.688−1 3.142−2 5.097+0 9.408+1 1.088−1 9.390−1 2.663−1 5.124+1 6.851−2 2.943+0 7.343+1 1.728−1
90
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 32 Effective collision strengths for transitions in Ni XXVI. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.449−1 2.771−1 1.240−2 3.775−3 6.860−3 9.619−3 1.436−2 2.472−3 9.209−4 1.712−3 1.724−3 2.588−3 1.028−3 1.364−3 9.620−4 3.904−4 7.294−4 6.585−4 9.889−4 5.425−4 7.200−4 6.993−5 8.700−5 2.428−2 8.777−4 1.330−2 3.490−3 4.551−2 6.475−3 2.776−4 2.748−3 1.146−3 8.324−3 2.004−3 1.432−3 8.346−4 1.316−4 1.093−3 5.463−4 3.127−3 9.368−4 7.474−4 5.027−4 6.852−5 6.699−5 1.789−3 3.629−3 3.045−2 1.752−2 9.031−2 5.504−4 1.163−3 6.682−3 4.150−3 1.697−2 1.547−3 3.180−3 2.603−4 5.516−4 2.738−3 1.774−3 6.496−3 8.927−4 1.703−3 1.184−4 1.671−4 9.784−1 1.823+0 6.561−2 9.859−2 5.736−2 1.060−2 1.907−2
1.492−1 2.839−1 1.381−2 4.748−3 8.756−3 1.059−2 1.598−2 2.788−3 1.236−3 2.380−3 2.056−3 3.094−3 1.345−3 1.786−3 9.430−4 4.417−4 8.328−4 6.985−4 1.050−3 5.681−4 7.552−4 7.428−5 9.220−5 3.765−2 3.138−3 1.454−2 5.943−3 4.685−2 1.029−2 7.999−4 3.075−3 1.785−3 9.052−3 2.789−3 2.111−3 1.505−3 2.147−4 1.041−3 5.787−4 3.264−3 9.817−4 7.947−4 5.162−4 7.431−5 6.618−5 8.127−3 6.506−3 3.516−2 2.272−2 9.621−2 1.599−3 1.853−3 8.116−3 5.304−3 1.899−2 2.785−3 4.893−3 4.377−4 6.027−4 2.661−3 1.872−3 6.802−3 9.362−4 1.806−3 1.206−4 1.776−4 9.437−1 1.802+0 8.697−2 1.328−1 5.985−2 1.247−2 2.587−2
1.564−1 2.974−1 1.357−2 4.847−3 8.954−3 1.066−2 1.609−2 2.676−3 1.200−3 2.301−3 1.975−3 2.972−3 1.248−3 1.657−3 9.373−4 4.482−4 8.477−4 6.894−4 1.037−3 5.549−4 7.378−4 6.929−5 8.601−5 4.070−2 2.629−3 1.436−2 5.493−3 4.854−2 9.554−3 6.494−4 2.938−3 1.564−3 9.150−3 2.475−3 1.964−3 1.264−3 1.940−4 1.027−3 5.441−4 3.336−3 9.145−4 7.986−4 4.755−4 7.116−5 5.969−5 6.477−3 5.929−3 3.437−2 2.215−2 9.878−2 1.303−3 1.615−3 7.614−3 4.925−3 1.892−2 2.392−3 4.461−3 3.949−4 5.625−4 2.607−3 1.803−3 6.881−3 8.820−4 1.783−3 1.102−4 1.676−4 1.006+0 1.910+0 8.426−2 1.281−1 5.949−2 1.336−2 2.688−2
1.646−1 3.129−1 1.337−2 5.031−3 9.295−3 1.072−2 1.615−2 2.599−3 1.198−3 2.287−3 1.909−3 2.873−3 1.165−3 1.546−3 9.380−4 4.636−4 8.787−4 6.798−4 1.024−3 5.406−4 7.189−4 6.370−5 7.907−5 4.089−2 2.196−3 1.410−2 4.894−3 5.087−2 8.466−3 5.336−4 2.821−3 1.356−3 9.385−3 2.151−3 1.868−3 1.041−3 1.760−4 1.014−3 5.033−4 3.447−3 8.307−4 8.126−4 4.267−4 6.831−5 5.228−5 5.208−3 5.245−3 3.329−2 2.126−2 1.023−1 1.075−3 1.397−3 7.151−3 4.567−3 1.910−2 2.038−3 4.130−3 3.580−4 5.180−4 2.546−3 1.721−3 7.019−3 8.201−4 1.773−3 9.863−5 1.575−4 1.089+0 2.053+0 7.982−2 1.210−1 5.954−2 1.513−2 2.942−2
1.746−1 3.313−1 1.326−2 5.411−3 1.000−2 1.088−2 1.638−2 2.561−3 1.246−3 2.371−3 1.868−3 2.813−3 1.101−3 1.463−3 9.447−4 4.922−4 9.349−4 6.717−4 1.012−3 5.270−4 7.012−4 5.797−5 7.198−5 3.824−2 1.861−3 1.386−2 4.282−3 5.440−2 7.281−3 4.489−4 2.735−3 1.172−3 9.825−3 1.836−3 1.841−3 8.470−4 1.604−4 1.004−3 4.579−4 3.617−3 7.338−4 8.430−4 3.730−4 6.629−5 4.448−5 4.292−3 4.578−3 3.226−2 2.049−2 1.079−1 9.095−4 1.207−3 6.773−3 4.265−3 1.966−2 1.748−3 3.946−3 3.268−4 4.703−4 2.484−3 1.635−3 7.253−3 7.564−4 1.790−3 8.684−5 1.487−4 1.193+0 2.232+0 7.510−2 1.137−1 6.000−2 1.803−2 3.417−2
1.873−1 3.543−1 1.328−2 6.094−3 1.128−2 1.124−2 1.690−2 2.558−3 1.357−3 2.578−3 1.859−3 2.801−3 1.061−3 1.410−3 9.573−4 5.395−4 1.027−3 6.680−4 1.008−3 5.167−4 6.878−4 5.269−5 6.546−5 3.384−2 1.645−3 1.372−2 3.746−3 5.967−2 6.170−3 3.915−4 2.681−3 1.015−3 1.053−2 1.542−3 1.893−3 6.852−4 1.481−4 9.969−4 4.109−4 3.865−3 6.307−4 8.957−4 3.188−4 6.559−5 3.694−5 3.722−3 4.010−3 3.150−2 2.018−2 1.169−1 7.992−4 1.047−3 6.491−3 4.045−3 2.073−2 1.530−3 3.927−3 3.027−4 4.221−4 2.426−3 1.557−3 7.627−3 6.988−4 1.846−3 7.588−5 1.424−4 1.311+0 2.438+0 7.098−2 1.073−1 6.080−2 2.227−2 4.156−2
2.029−1 3.823−1 1.342−2 7.164−3 1.328−2 1.182−2 1.775−2 2.584−3 1.542−3 2.931−3 1.883−3 2.839−3 1.041−3 1.385−3 9.751−4 6.112−4 1.167−3 6.712−4 1.014−3 5.110−4 6.807−4 4.832−5 6.010−5 2.904−2 1.556−3 1.368−2 3.326−3 6.711−2 5.223−3 3.587−4 2.655−3 8.854−4 1.156−2 1.281−3 2.021−3 5.556−4 1.402−4 9.939−4 3.662−4 4.213−3 5.303−4 9.740−4 2.688−4 6.632−5 3.022−5 3.479−3 3.575−3 3.106−2 2.053−2 1.301−1 7.396−4 9.170−4 6.300−3 3.929−3 2.240−2 1.383−3 4.066−3 2.883−4 3.769−4 2.378−3 1.503−3 8.183−3 6.545−4 1.951−3 6.660−5 1.392−4 1.435+0 2.661+0 6.775−2 1.023−1 6.179−2 2.798−2 5.182−2
2.198−1 4.127−1 1.359−2 8.585−3 1.595−2 1.252−2 1.878−2 2.616−3 1.791−3 3.408−3 1.926−3 2.906−3 1.033−3 1.375−3 9.912−4 7.036−4 1.347−3 6.785−4 1.026−3 5.078−4 6.768−4 4.493−5 5.594−5 2.471−2 1.578−3 1.367−2 3.017−3 7.633−2 4.459−3 3.465−4 2.638−3 7.817−4 1.281−2 1.060−3 2.196−3 4.555−4 1.369−4 9.901−4 3.261−4 4.631−3 4.394−4 1.068−3 2.260−4 6.785−5 2.462−5 3.509−3 3.261−3 3.079−2 2.148−2 1.468−1 7.224−4 8.136−4 6.157−3 3.909−3 2.454−2 1.293−3 4.311−3 2.839−4 3.367−4 2.333−3 1.474−3 8.876−3 6.245−4 2.088−3 5.920−5 1.382−4 1.551+0 2.875+0 6.511−2 9.830−2 6.253−2 3.478−2 6.421−2
2.310−1 4.330−1 1.342−2 9.878−3 1.839−2 1.288−2 1.932−2 2.578−3 2.006−3 3.822−3 1.925−3 2.906−3 1.006−3 1.340−3 9.776−4 7.800−4 1.496−3 6.701−4 1.014−3 4.932−4 6.577−4 4.154−5 5.177−5 2.098−2 1.632−3 1.335−2 2.747−3 8.386−2 3.814−3 3.403−4 2.561−3 6.893−4 1.374−2 8.703−4 2.316−3 3.759−4 1.340−4 9.606−4 2.874−4 4.921−3 3.590−4 1.129−3 1.891−4 6.776−5 1.999−5 3.625−3 2.987−3 2.991−2 2.223−2 1.603−1 7.165−4 7.210−4 5.905−3 3.862−3 2.609−2 1.216−3 4.471−3 2.800−4 2.978−4 2.236−3 1.433−3 9.341−3 5.929−4 2.172−3 5.257−5 1.349−4 1.607+0 2.982+0 6.158−2 9.296−2 6.138−2 4.051−2 7.468−2
2.443−1 4.597−1 1.401−2 1.099−2 2.041−2 1.362−2 2.035−2 2.768−3 2.227−3 4.215−3 1.990−3 2.996−3 1.047−3 1.390−3 1.068−3 8.680−4 1.650−3 6.868−4 1.036−3 5.193−4 6.901−4 4.342−5 5.404−5 1.615−2 1.637−3 1.404−2 2.688−3 9.134−2 3.490−3 3.348−4 2.820−3 6.901−4 1.472−2 8.170−4 2.492−3 3.533−4 1.316−4 1.098−3 2.977−4 5.215−3 3.522−4 1.241−3 1.970−4 7.097−5 2.173−5 3.591−3 2.921−3 3.126−2 2.339−2 1.734−1 7.067−4 7.222−4 6.397−3 4.004−3 2.776−2 1.227−3 4.745−3 2.751−4 3.089−4 2.511−3 1.487−3 9.852−3 6.340−4 2.363−3 5.678−5 1.417−4 1.776+0 3.246+0 6.209−2 9.367−2 6.483−2 4.526−2 8.348−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
91
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.474−2 3.669−2 2.428−2 3.235−2 1.087−2 2.234−3 4.105−3 5.197−3 7.761−3 2.847−3 3.807−3 4.428−3 5.527−3 1.070−1 1.291+0 1.661−2 3.796−3 6.076−2 8.494−3 7.635−2 1.090−2 8.124−2 1.169−2 9.407−4 1.178−2 2.367−3 1.565−2 3.117−3 8.727−3 2.760−3 1.017−2 3.422−3 3.096−1 2.512+0 7.903−3 9.274−3 1.316−1 3.012−2 1.543−1 3.897−2 1.505−1 1.898−3 2.487−3 2.608−2 7.127−3 3.185−2 6.049−3 1.689−2 8.191−3 1.983−2 7.760−2 3.242−3 6.198−3 6.232−3 1.185−1 1.479−2 5.245−1 2.588−2 1.058−3 1.981−3 2.441−3 2.289−2 5.587−3 8.225−2 8.886−3 2.317−2 5.168−3 4.906−3 4.246−3 1.457−2 1.489−2 1.856−1 6.583−2 7.663−1
2.606−2 4.361−2 2.891−2 4.406−2 1.041−2 2.597−3 4.792−3 5.212−3 7.804−3 3.212−3 4.296−3 4.568−3 5.708−3 1.287−1 1.318+0 5.562−2 7.724−3 6.065−2 1.217−2 8.022−2 1.711−2 8.284−2 1.976−2 1.355−3 1.076−2 2.305−3 1.696−2 3.310−3 9.003−3 2.937−3 1.050−2 3.452−3 3.535−1 2.556+0 1.796−2 1.257−2 1.496−1 3.668−2 1.865−1 5.011−2 1.747−1 2.683−3 2.466−3 2.396−2 7.641−3 3.447−2 6.374−3 1.756−2 8.367−3 2.045−2 2.210−1 8.446−3 1.406−2 1.537−2 1.276−1 2.963−2 5.308−1 4.683−2 1.511−3 2.511−3 2.796−3 2.238−2 5.774−3 8.467−2 9.066−3 2.307−2 5.010−3 1.458−2 1.080−2 3.676−2 2.806−2 2.299−1 8.959−2 8.500−1
2.668−2 4.355−2 2.796−2 4.165−2 1.051−2 2.824−3 5.223−3 5.356−3 8.024−3 3.062−3 4.096−3 4.476−3 5.593−3 1.243−1 1.391+0 5.008−2 6.874−3 6.047−2 1.123−2 8.626−2 1.531−2 8.517−2 1.714−2 1.275−3 1.085−2 2.262−3 1.813−2 3.118−3 9.108−3 2.669−3 1.078−2 3.192−3 3.646−1 2.694+0 1.579−2 1.168−2 1.458−1 3.611−2 1.925−1 4.741−2 1.739−1 2.565−3 2.411−3 2.413−2 7.641−3 3.650−2 6.048−3 1.752−2 8.106−3 2.077−2 1.977−1 6.841−3 1.191−2 1.258−2 1.250−1 2.461−2 5.571−1 3.889−2 1.325−3 2.323−3 2.513−3 2.216−2 5.173−3 8.782−2 7.999−3 2.413−2 4.423−3 1.164−2 8.677−3 3.087−2 2.339−2 2.194−1 8.287−2 8.689−1
2.779−2 4.416−2 2.718−2 3.945−2 1.067−2 3.188−3 5.910−3 5.559−3 8.331−3 2.907−3 3.890−3 4.407−3 5.506−3 1.182−1 1.497+0 4.226−2 6.565−3 6.055−2 1.054−2 9.574−2 1.369−2 8.887−2 1.479−2 1.259−3 1.099−2 2.234−3 1.983−2 2.913−3 9.277−3 2.385−3 1.116−2 2.922−3 3.839−1 2.917+0 1.489−2 1.111−2 1.423−1 3.654−2 2.050−1 4.543−2 1.755−1 2.571−3 2.378−3 2.439−2 7.738−3 3.951−2 5.720−3 1.758−2 7.864−3 2.123−2 1.651−1 5.620−3 1.043−2 1.022−2 1.230−1 2.005−2 5.973−1 3.165−2 1.172−3 2.175−3 2.226−3 2.198−2 4.527−3 9.239−2 6.855−3 2.571−2 3.818−3 9.393−3 6.897−3 2.615−2 1.919−2 2.092−1 7.780−2 9.095−1
2.945−2 4.577−2 2.666−2 3.778−2 1.087−2 3.730−3 6.939−3 5.827−3 8.735−3 2.764−3 3.700−3 4.378−3 5.471−3 1.120−1 1.635+0 3.452−2 6.816−3 6.096−2 1.020−2 1.099−1 1.241−2 9.400−2 1.294−2 1.310−3 1.115−2 2.228−3 2.222−2 2.713−3 9.522−3 2.111−3 1.161−2 2.668−3 4.120−1 3.213+0 1.531−2 1.091−2 1.401−1 3.832−2 2.272−1 4.448−2 1.804−1 2.715−3 2.373−3 2.473−2 7.987−3 4.381−2 5.428−3 1.778−2 7.670−3 2.183−2 1.322−1 4.748−3 9.603−3 8.392−3 1.218−1 1.630−2 6.555−1 2.559−2 1.048−3 2.078−3 1.957−3 2.186−2 3.892−3 9.876−2 5.730−3 2.790−2 3.253−3 7.787−3 5.503−3 2.291−2 1.575−2 2.013−1 7.529−2 9.794−1
3.159−2 4.831−2 2.639−2 3.669−2 1.109−2 4.493−3 8.389−3 6.156−3 9.229−3 2.650−3 3.546−3 4.404−3 5.503−3 1.067−1 1.792+0 2.813−2 7.634−3 6.164−2 1.019−2 1.296−1 1.147−2 1.004−1 1.161−2 1.436−3 1.132−2 2.251−3 2.546−2 2.536−3 9.840−3 1.873−3 1.209−2 2.450−3 4.456−1 3.547+0 1.705−2 1.104−2 1.394−1 4.162−2 2.611−1 4.456−2 1.884−1 3.013−3 2.400−3 2.513−2 8.438−3 4.968−2 5.203−3 1.813−2 7.538−3 2.252−2 1.043−1 4.167−3 9.408−3 7.091−3 1.214−1 1.343−2 7.347−1 2.083−2 9.534−4 2.042−3 1.726−3 2.180−2 3.320−3 1.073−1 4.714−3 3.067−2 2.772−3 6.712−3 4.462−3 2.118−2 1.311−2 1.962−1 7.573−2 1.084+0
3.405−2 5.153−2 2.633−2 3.610−2 1.133−2 5.506−3 1.032−2 6.530−3 9.790−3 2.571−3 3.441−3 4.483−3 5.602−3 1.025−1 1.959+0 2.344−2 9.012−3 6.248−2 1.044−2 1.553−1 1.082−2 1.074−1 1.075−2 1.640−3 1.151−2 2.302−3 2.965−2 2.392−3 1.021−2 1.684−3 1.257−2 2.279−3 4.816−1 3.891+0 2.008−2 1.142−2 1.400−1 4.650−2 3.075−1 4.545−2 1.987−1 3.475−3 2.458−3 2.557−2 9.126−3 5.732−2 5.058−3 1.861−2 7.467−3 2.322−2 8.275−2 3.812−3 9.781−3 6.244−3 1.217−1 1.135−2 8.367−1 1.727−2 8.865−4 2.073−3 1.547−3 2.181−2 2.844−3 1.183−1 3.868−3 3.389−2 2.397−3 6.042−3 3.713−3 2.080−2 1.120−2 1.932−1 7.918−2 1.224+0
3.640−2 5.470−2 2.629−2 3.570−2 1.150−2 6.700−3 1.259−2 6.878−3 1.031−2 2.516−3 3.368−3 4.579−3 5.722−3 9.896−2 2.113+0 2.023−2 1.080−2 6.306−2 1.079−2 1.853−1 1.035−2 1.139−1 1.020−2 1.901−3 1.162−2 2.363−3 3.444−2 2.275−3 1.055−2 1.542−3 1.293−2 2.146−3 5.147−1 4.202+0 2.406−2 1.188−2 1.406−1 5.246−2 3.625−1 4.659−2 2.086−1 4.060−3 2.525−3 2.589−2 9.976−3 6.612−2 4.962−3 1.905−2 7.406−3 2.374−2 6.703−2 3.602−3 1.056−2 5.733−3 1.217−1 9.893−3 9.531−1 1.470−2 8.406−4 2.156−3 1.415−3 2.177−2 2.469−3 1.307−1 3.204−3 3.708−2 2.120−3 5.638−3 3.184−3 2.141−2 9.852−3 1.910−1 8.482−2 1.387+0
3.733−2 5.587−2 2.560−2 3.455−2 1.130−2 7.673−3 1.445−2 6.971−3 1.045−2 2.419−3 3.237−3 4.546−3 5.681−3 9.391−2 2.187+0 1.781−2 1.233−2 6.175−2 1.085−2 2.093−1 9.780−3 1.160−1 9.627−3 2.113−3 1.137−2 2.356−3 3.808−2 2.133−3 1.052−2 1.408−3 1.281−2 2.000−3 5.285−1 4.346+0 2.749−2 1.199−2 1.374−1 5.696−2 4.064−1 4.643−2 2.111−1 4.535−3 2.519−3 2.539−2 1.056−2 7.273−2 4.778−3 1.890−2 7.163−3 2.343−2 5.516−2 3.401−3 1.120−2 5.332−3 1.185−1 8.717−3 1.039+0 1.266−2 7.913−4 2.203−3 1.297−3 2.113−2 2.148−3 1.388−1 2.668−3 3.873−2 1.885−3 5.276−3 2.765−3 2.196−2 8.747−3 1.845−1 8.889−2 1.508+0
4.007−2 5.950−2 2.664−2 3.551−2 1.240−2 8.621−3 1.622−2 7.386−3 1.105−2 2.420−3 3.231−3 4.850−3 6.053−3 9.634−2 2.359+0 1.446−2 1.384−2 6.633−2 1.179−2 2.317−1 1.006−2 1.240−1 9.673−3 2.378−3 1.295−2 2.658−3 4.133−2 2.223−3 1.087−2 1.436−3 1.359−2 2.143−3 5.672−1 4.677+0 3.055−2 1.305−2 1.463−1 6.201−2 4.457−1 4.877−2 2.235−1 5.077−3 2.833−3 2.877−2 1.134−2 7.860−2 4.914−3 1.951−2 7.625−3 2.481−2 4.255−2 3.313−3 1.163−2 5.145−3 1.235−1 8.276−3 1.129+0 1.207−2 8.249−4 2.365−3 1.367−3 2.264−2 2.239−3 1.493−1 2.791−3 4.173−2 2.062−3 5.043−3 2.552−3 2.218−2 8.447−3 1.901−1 9.448−2 1.630+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
92
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.592−3 1.725−3 4.960−3 5.589−3 3.717−2 1.548−2 1.218−1 8.400−3 3.453−2 3.351+0 6.301+0 2.941−1 4.413−1 2.676−2 3.583−2 1.742−1 2.680−2 4.797−2 5.334−2 7.887−2 5.721−2 7.606−2 2.915−2 3.639−2 3.753−1 5.689+0 4.853−2 2.298−1 2.219−2 1.334−2 1.830−1 2.308−2 1.382−1 2.467−2 1.705−1 1.996−2 1.029−1 1.965−2 1.297+0 1.105+1 9.420−2 4.114−1 2.866−2 2.540−2 3.919−1 6.153−2 2.865−1 7.660−2 3.153−1 6.101−2 1.863−1 1.889−1 7.048+0 4.414−2 1.137−2 2.096−2 1.591−2 3.785−1 2.433−2 7.402−1 3.495−2 4.682−1 3.535−2 5.571−1 9.392+0 1.726−2 1.019−2 4.560−2 2.473−2 5.812−1 9.168−2 1.084+0 9.169−2 6.668−1
2.358−3 2.042−3 5.926−3 5.822−3 3.642−2 1.584−2 1.255−1 8.253−3 3.435−2 3.600+0 7.192+0 3.357−1 4.992−1 7.006−2 9.397−2 1.661−1 2.828−2 5.042−2 5.283−2 7.847−2 5.727−2 7.626−2 3.028−2 3.785−2 4.322−1 5.960+0 8.941−2 2.843−1 7.825−2 1.692−2 1.683−1 2.161−2 1.403−1 2.322−2 1.693−1 2.072−2 1.047−1 2.065−2 1.572+0 1.399+1 1.893−1 6.331−1 3.670−2 2.457−2 3.593−1 6.016−2 2.896−1 7.732−2 3.144−1 6.286−2 1.900−1 3.293−1 7.815+0 1.986−1 1.477−2 2.685−2 1.626−2 3.592−1 2.387−2 7.384−1 3.352−2 4.653−1 3.423−2 1.068+0 1.542+1 2.101−2 1.053−2 5.277−2 2.457−2 5.513−1 9.009−2 1.079+0 9.018−2 6.627−1
2.049−3 1.797−3 5.477−3 5.208−3 3.585−2 1.491−2 1.295−1 7.706−3 3.560−2 3.908+0 7.594+0 3.220−1 4.802−1 5.956−2 7.933−2 1.691−1 3.377−2 6.057−2 5.650−2 8.391−2 5.773−2 7.688−2 3.048−2 3.810−2 4.103−1 6.509+0 8.022−2 2.661−1 6.194−2 1.813−2 1.713−1 2.277−2 1.629−1 2.329−2 1.802−1 2.056−2 1.052−1 1.952−2 1.690+0 1.478+1 1.617−1 5.685−1 3.948−2 2.563−2 3.670−1 6.507−2 3.329−1 8.033−2 3.335−1 6.150−2 1.899−1 2.866−1 8.967+0 1.531−1 1.381−2 2.721−2 1.606−2 3.649−1 2.327−2 8.190−1 3.155−2 4.902−1 3.177−2 1.129+0 1.675+1 2.013−2 9.973−3 5.401−2 2.389−2 5.601−1 9.378−2 1.195+0 9.019−2 6.963−1
1.801−3 1.556−3 5.070−3 4.554−3 3.529−2 1.400−2 1.356−1 7.200−3 3.759−2 4.253+0 8.085+0 3.086−1 4.614−1 5.048−2 6.704−2 1.726−1 4.169−2 7.519−2 6.107−2 9.065−2 5.813−2 7.741−2 3.090−2 3.863−2 3.890−1 7.141+0 7.291−2 2.497−1 4.822−2 2.070−2 1.747−1 2.432−2 1.944−1 2.334−2 1.933−1 2.051−2 1.056−1 1.846−2 1.824+0 1.564+1 1.377−1 5.104−1 4.531−2 2.724−2 3.760−1 7.188−2 3.929−1 8.417−2 3.567−1 6.022−2 1.899−1 2.486−1 1.016+1 1.152−1 1.342−2 2.897−2 1.614−2 3.715−1 2.284−2 9.291−1 2.964−2 5.201−1 2.951−2 1.186+0 1.799+1 1.991−2 9.577−3 5.726−2 2.343−2 5.701−1 9.969−2 1.354+0 9.099−2 7.372−1
1.603−3 1.332−3 4.744−3 3.915−3 3.480−2 1.323−2 1.443−1 6.806−3 4.044−2 4.627+0 8.671+0 2.970−1 4.451−1 4.367−2 5.797−2 1.762−1 5.260−2 9.530−2 6.638−2 9.844−2 5.846−2 7.784−2 3.156−2 3.945−2 3.708−1 7.821+0 6.800−2 2.365−1 3.780−2 2.478−2 1.783−1 2.622−2 2.366−1 2.339−2 2.083−1 2.061−2 1.061−1 1.759−2 1.966+0 1.663+1 1.189−1 4.640−1 5.450−2 2.929−2 3.856−1 8.101−2 4.731−1 8.873−2 3.831−1 5.920−2 1.900−1 2.186−1 1.130+1 8.655−2 1.345−2 3.226−2 1.655−2 3.784−1 2.266−2 1.075+0 2.797−2 5.538−1 2.769−2 1.244+0 1.920+1 2.018−2 9.302−3 6.293−2 2.325−2 5.806−1 1.085−1 1.564+0 9.270−2 7.836−1
1.454−3 1.135−3 4.533−3 3.339−3 3.444−2 1.275−2 1.561−1 6.573−3 4.415−2 5.020+0 9.333+0 2.875−1 4.316−1 3.906−2 5.190−2 1.798−1 6.699−2 1.218−1 7.209−2 1.068−1 5.875−2 7.821−2 3.241−2 4.052−2 3.561−1 8.520+0 6.526−2 2.261−1 3.038−2 3.050−2 1.817−1 2.832−2 2.911−1 2.345−2 2.241−1 2.085−2 1.066−1 1.695−2 2.113+0 1.771+1 1.052−1 4.292−1 6.739−2 3.160−2 3.951−1 9.284−2 5.766−1 9.368−2 4.109−1 5.852−2 1.904−1 1.963−1 1.236+1 6.641−2 1.376−2 3.721−2 1.732−2 3.851−1 2.275−2 1.261+0 2.666−2 5.890−1 2.640−2 1.301+0 2.039+1 2.078−2 9.127−3 7.137−2 2.334−2 5.908−1 1.207−1 1.833+0 9.517−2 8.324−1
1.349−3 9.747−4 4.462−3 2.863−3 3.422−2 1.262−2 1.715−1 6.510−3 4.854−2 5.417+0 1.004+1 2.798−1 4.205−1 3.621−2 4.819−2 1.830−1 8.502−2 1.549−1 7.767−2 1.151−1 5.905−2 7.861−2 3.335−2 4.170−2 3.445−1 9.216+0 6.417−2 2.181−1 2.534−2 3.788−2 1.848−1 3.043−2 3.582−1 2.352−2 2.393−1 2.119−2 1.073−1 1.656−2 2.258+0 1.884+1 9.558−2 4.038−1 8.399−2 3.389−2 4.039−1 1.074−1 7.043−1 9.854−2 4.377−1 5.823−2 1.913−1 1.804−1 1.333+1 5.291−2 1.420−2 4.382−2 1.842−2 3.912−1 2.301−2 1.489+0 2.572−2 6.227−1 2.562−2 1.357+0 2.154+1 2.153−2 9.036−3 8.263−2 2.362−2 6.002−1 1.366−1 2.164+0 9.803−2 8.791−1
1.277−3 8.490−4 4.503−3 2.488−3 3.398−2 1.278−2 1.890−1 6.553−3 5.292−2 5.772+0 1.070+1 2.721−1 4.094−1 3.447−2 4.594−2 1.849−1 1.052−1 1.920−1 8.212−2 1.217−1 5.910−2 7.868−2 3.411−2 4.265−2 3.335−1 9.830+0 6.386−2 2.109−1 2.194−2 4.624−2 1.865−1 3.216−2 4.323−1 2.351−2 2.511−1 2.144−2 1.075−1 1.630−2 2.384+0 1.986+1 8.854−2 3.836−1 1.028−1 3.575−2 4.093−1 1.234−1 8.451−1 1.022−1 4.583−1 5.798−2 1.915−1 1.683−1 1.411+1 4.409−2 1.460−2 5.137−2 1.962−2 3.943−1 2.322−2 1.738+0 2.499−2 6.481−1 2.511−2 1.402+0 2.249+1 2.219−2 8.967−3 9.548−2 2.384−2 6.050−1 1.543−1 2.525+0 1.002−1 9.141−1
1.201−3 7.410−4 4.494−3 2.167−3 3.286−2 1.279−2 2.004−1 6.471−3 5.513−2 5.900+0 1.095+1 2.585−1 3.891−1 3.261−2 4.351−2 1.807−1 1.211−1 2.210−1 8.291−2 1.230−1 5.747−2 7.650−2 3.371−2 4.215−2 3.158−1 1.005+1 6.229−2 1.996−1 1.928−2 5.275−2 1.821−1 3.257−2 4.887−1 2.285−2 2.519−1 2.104−2 1.047−1 1.572−2 2.418+0 2.014+1 8.151−2 3.589−1 1.174−1 3.612−2 4.011−1 1.344−1 9.514−1 1.017−1 4.590−1 5.625−2 1.864−1 1.554−1 1.432+1 3.770−2 1.454−2 5.703−2 2.017−2 3.848−1 2.271−2 1.918+0 2.384−2 6.464−1 2.413−2 1.398+0 2.261+1 2.213−2 8.689−3 1.049−1 2.331−2 5.903−1 1.664−1 2.787+0 9.888−2 9.111−1
1.248−3 7.714−4 4.801−3 2.259−3 3.514−2 1.369−2 2.152−1 7.012−3 5.935−2 6.198+0 1.148+1 2.726−1 4.105−1 3.265−2 4.366−2 1.933−1 1.189−1 2.177−1 8.381−2 1.241−1 1.677−1 2.238−1 3.898−2 4.874−2 3.325−1 1.062+1 6.495−2 2.092−1 1.718−2 5.007−2 1.990−1 3.293−2 5.000−1 2.930−2 2.622−1 2.411−2 1.210−1 1.896−2 2.489+0 2.111+1 8.106−2 3.686−1 1.100−1 3.645−2 4.342−1 1.440−1 9.704−1 1.091−1 4.792−1 6.672−2 2.172−1 1.591−1 1.549+1 3.104−2 1.421−2 5.299−2 2.319−2 4.039−1 2.400−2 2.045+0 4.261−2 6.858−1 2.703−2 1.634+0 2.412+1 2.164−2 4.869−2 9.984−2 2.461−2 6.193−1 1.943−1 2.970+0 1.067−1 9.666−1
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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93
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.673−1 4.259−3 8.783−3 8.983−3 3.366−2 1.694−2 4.780−1 3.501−2 2.641+0 6.350−2 5.694−3 5.145−3 1.846−2 1.362−2 5.401−2 3.509−2 6.498−1 1.641−1 3.452+0 8.601+0 1.623+1 8.310−1 1.246+0 9.490−2 1.269−1 2.652−2 3.327−2 9.658−1 1.581+1 1.310−1 8.973−1 6.279−2 5.753−2 1.799−2 3.487+0 2.960+1 3.376−1 1.592+0 4.273−2 1.063−1 4.913−1 2.215+1 9.106−2 7.429−1 4.466−2 1.761+0 3.070+1 1.320−1 1.050+0 3.197−1 1.749+1 8.420−2 9.297−1 2.321+1 2.979−1
5.370−1 6.383−3 1.058−2 9.955−3 3.955−2 1.691−2 4.655−1 3.312−2 2.639+0 5.931−2 9.017−3 6.313−3 2.060−2 1.349−2 5.992−2 3.333−2 6.313−1 1.600−1 3.450+0 9.599+0 1.773+1 8.192−1 1.231+0 1.023−1 1.363−1 2.734−2 3.419−2 9.338−1 1.783+1 1.422−1 8.777−1 6.321−2 6.238−2 1.781−2 4.285+0 3.529+1 3.317−1 1.546+0 4.405−2 1.147−1 4.770−1 3.246+1 9.495−2 7.249−1 4.355−2 3.298+0 5.100+1 1.292−1 1.023+0 3.076−1 3.037+1 7.891−2 2.339+0 4.279+1 2.723−1
4.212−1 5.349−3 9.750−3 8.803−3 3.833−2 1.503−2 4.676−1 2.933−2 2.839+0 5.213−2 7.461−3 5.299−3 1.911−2 1.170−2 5.830−2 2.950−2 6.333−1 1.598−1 3.708+0 1.051+1 1.932+1 8.059−1 1.211+0 1.036−1 1.382−1 2.626−2 3.285−2 9.134−1 1.951+1 1.451−1 8.608−1 6.210−2 6.221−2 1.642−2 4.722+0 3.883+1 3.245−1 1.512+0 4.213−2 1.134−1 4.658−1 3.619+1 9.377−2 7.069−1 3.957−2 3.640+0 5.692+1 1.226−1 9.960−1 2.939−1 3.384+1 7.108−2 2.499+0 4.759+1 2.451−1
3.222−1 4.579−3 9.184−3 7.785−3 3.790−2 1.324−2 4.704−1 2.568−2 3.109+0 4.516−2 6.320−3 4.439−3 1.793−2 9.996−3 5.749−2 2.583−2 6.361−1 1.626−1 4.058+0 1.150+1 2.108+1 7.914−1 1.190+0 1.053−1 1.405−1 2.528−2 3.163−2 8.916−1 2.133+1 1.484−1 8.432−1 6.110−2 6.228−2 1.517−2 5.179+0 4.259+1 3.172−1 1.477+0 4.048−2 1.126−1 4.542−1 3.998+1 9.312−2 6.884−1 3.590−2 3.979+0 6.287+1 1.163−1 9.680−1 2.806−1 3.733+1 6.399−2 2.655+0 5.237+1 2.192−1
2.454−1 4.016−3 8.839−3 6.948−3 3.842−2 1.171−2 4.737−1 2.250−2 3.463+0 3.902−2 5.497−3 3.742−3 1.709−2 8.498−3 5.791−2 2.265−2 6.396−1 1.694−1 4.517+0 1.252+1 2.295+1 7.764−1 1.168+0 1.073−1 1.432−1 2.450−2 3.066−2 8.688−1 2.321+1 1.522−1 8.254−1 6.030−2 6.265−2 1.419−2 5.633+0 4.638+1 3.098−1 1.440+0 3.927−2 1.124−1 4.429−1 4.364+1 9.315−2 6.700−1 3.285−2 4.295+0 6.852+1 1.107−1 9.408−1 2.685−1 4.062+1 5.829−2 2.798+0 5.685+1 1.969−1
1.896−1 3.621−3 8.674−3 6.314−3 4.004−2 1.055−2 4.772−1 1.998−2 3.914+0 3.409−2 4.923−3 3.209−3 1.658−2 7.288−3 5.989−2 2.013−2 6.435−1 1.813−1 5.104+0 1.355+1 2.488+1 7.609−1 1.145+0 1.096−1 1.464−1 2.393−2 2.995−2 8.450−1 2.510+1 1.564−1 8.076−1 5.974−2 6.331−2 1.352−2 6.070+0 5.009+1 3.025−1 1.402+0 3.855−2 1.129−1 4.317−1 4.705+1 9.387−2 6.516−1 3.055−2 4.580+0 7.372+1 1.060−1 9.140−1 2.579−1 4.363+1 5.419−2 2.925+0 6.091+1 1.788−1
1.505−1 3.359−3 8.637−3 5.869−3 4.272−2 9.769−3 4.805−1 1.813−2 4.464+0 3.042−2 4.544−3 2.825−3 1.633−2 6.380−3 6.345−2 1.828−2 6.474−1 1.984−1 5.822+0 1.456+1 2.681+1 7.454−1 1.122+0 1.122−1 1.499−1 2.357−2 2.951−2 8.194−1 2.694+1 1.608−1 7.901−1 5.941−2 6.424−2 1.311−2 6.484+0 5.365+1 2.950−1 1.361+0 3.822−2 1.138−1 4.203−1 5.017+1 9.505−2 6.325−1 2.891−2 4.832+0 7.841+1 1.020−1 8.867−1 2.485−1 4.633+1 5.153−2 3.036+0 6.453+1 1.647−1
1.236−1 3.184−3 8.639−3 5.553−3 4.599−2 9.273−3 4.808−1 1.677−2 5.060+0 2.777−2 4.293−3 2.554−3 1.619−2 5.717−3 6.791−2 1.691−2 6.474−1 2.186−1 6.602+0 1.543+1 2.851+1 7.304−1 1.100+0 1.146−1 1.531−1 2.327−2 2.914−2 7.898−1 2.853+1 1.649−1 7.717−1 5.901−2 6.506−2 1.285−2 6.823+0 5.664+1 2.856−1 1.311+0 3.794−2 1.142−1 4.065−1 5.267+1 9.585−2 6.094−1 2.767−2 5.023+0 8.210+1 9.788−2 8.542−1 2.388−1 4.844+1 4.970−2 3.114+0 6.731+1 1.532−1
1.033−1 2.997−3 8.440−3 5.205−3 4.789−2 8.758−3 4.666−1 1.541−2 5.464+0 2.535−2 4.031−3 2.318−3 1.570−2 5.138−3 7.043−2 1.555−2 6.280−1 2.318−1 7.132+0 1.568+1 2.905+1 7.050−1 1.065+0 1.138−1 1.520−1 2.246−2 2.813−2 7.447−1 2.896+1 1.645−1 7.396−1 5.715−2 6.410−2 1.238−2 6.886+0 5.733+1 2.688−1 1.230+0 3.664−2 1.110−1 3.824−1 5.304+1 9.362−2 5.708−1 2.606−2 5.017+0 8.249+1 9.166−2 8.003−1 2.237−1 4.860+1 4.719−2 3.078+0 6.741+1 1.406−1
8.832−2 3.240−3 8.651−3 5.755−3 4.778−2 2.502−2 4.876−1 1.720−2 5.853+0 2.854−2 4.334−3 2.668−3 1.641−2 6.419−3 1.559−1 1.735−2 6.567−1 2.473−1 7.616+0 1.605+1 2.805+1 6.842−1 1.029+0 1.638−1 2.214−1 2.791−2 3.510−2 7.621−1 3.034+1 1.897−1 7.321−1 6.273−2 7.404−2 1.389−2 6.337+0 5.131+1 3.014−1 1.301+0 5.138−2 1.635−1 4.254−1 5.073+1 1.044−1 6.080−1 2.919−2 4.791+0 8.519+1 9.980−2 8.565−1 2.438−1 4.707+1 6.691−2 2.797+0 6.879+1 1.572−1
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Contents lists available at SciVerse ScienceDirect
Atomic Data and Nuclear Data Tables journal homepage: www.elsevier.com/locate/adt
Energy levels, radiative rates, and electron impact excitation rates for transitions in Li-like ions with 21 ≤ Z ≤ 28 Kanti M. Aggarwal ∗ , Francis P. Keenan Astrophysics Research Centre, School of Mathematics and Physics, Queen’s University Belfast, Belfast BT7 1NN, Northern Ireland, UK
article
info
Article history: Received 15 March 2011 Received in revised form 13 May 2011 Accepted 27 May 2011 Available online xxxx
∗
abstract We report calculations of energy levels, radiative rates, and electron impact excitation rates for transitions in Li-like ions with 21 ≤ Z ≤ 28. The General-Purpose Relativistic Atomic Structure Package is adopted for calculating energy levels and radiative rates, while for determining the collision strengths and subsequently the excitation rates, the Dirac Atomic R-matrix Code is used. Oscillator strengths, radiative rates, and line strengths are listed for all E1, E2, M1, and M2 transitions among the lowest 24 levels of the Li-like ions considered. Collision strengths have been averaged over a Maxwellian velocity distribution, and the effective collision strengths obtained are given over a wide temperature range up to 107.8 K. Additionally, lifetimes are listed for all calculated levels of these ions. Finally, extensive comparisons are made with results available in the literature, as well as with our analogous calculations for all parameters with the Flexible Atomic Code, in order to assess the accuracy of the results. © 2012 Elsevier Inc. All rights reserved.
Corresponding author. Tel.: +44 28 9097 3239; fax: +44 28 9097 3110. E-mail address: [email protected] (K.M. Aggarwal).
0092-640X/$ – see front matter © 2012 Elsevier Inc. All rights reserved. doi:10.1016/j.adt.2011.05.002
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Contents 1. 2. 3. 4. 5. 6. 7.
Introduction........................................................................................................................................................................................................................ Energy levels....................................................................................................................................................................................................................... Radiative rates .................................................................................................................................................................................................................... Lifetimes ............................................................................................................................................................................................................................. Collision strengths ............................................................................................................................................................................................................. Effective collision strengths .............................................................................................................................................................................................. Conclusions......................................................................................................................................................................................................................... Acknowledgment ............................................................................................................................................................................................................... Appendix. Supplementary data.................................................................................................................................................................................... References........................................................................................................................................................................................................................... Explanation of Tables ......................................................................................................................................................................................................... Table 1. Energy levels of Sc XIX, their threshold energies (in Ryd), and lifetimes (in s). ........................................................................................ Table 2. Energy levels of Ti XX, their threshold energies (in Ryd), and lifetimes (in s)........................................................................................... Table 3. Energy levels of V XXI, their threshold energies (in Ryd), and lifetimes (in s). ......................................................................................... Table 4. Energy levels of Cr XXII, their threshold energies (in Ryd), and lifetimes (in s). ....................................................................................... Table 5. Energy levels of Mn XXIII, their threshold energies (in Ryd), and lifetimes (in s). .................................................................................... Table 6. Energy levels of Fe XXIV, their threshold energies (in Ryd), and lifetimes (in s)....................................................................................... Table 7. Energy levels of Co XXV, their threshold energies (in Ryd), and lifetimes (in s). ...................................................................................... Table 8. Energy levels of Ni XXVI, their threshold energies (in Ryd), and lifetimes (in s)....................................................................................... Table 9. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Sc XIX. ................................................................................................................................................................................................................. Table 10. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ti XX. ............................................................................................................................................................................................... Table 11. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in V XXI. ............................................................................................................................................................................................... Table 12. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Cr XXII.............................................................................................................................................................................................. Table 13. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Mn XXIII........................................................................................................................................................................................... Table 14. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Fe XXIV. ........................................................................................................................................................................................... Table 15. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Co XXV. ............................................................................................................................................................................................ Table 16. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ni XXVI. ........................................................................................................................................................................................... Table 17. Collision strengths for resonance transitions in Sc XIX............................................................................................................................. Table 18. Collision strengths for resonance transitions in Ti XX. ............................................................................................................................. Table 19. Collision strengths for resonance transitions in V XXI. ............................................................................................................................. Table 20. Collision strengths for resonance transitions in Cr XXII............................................................................................................................ Table 21. Collision strengths for resonance transitions in Mn XXIII. ....................................................................................................................... Table 22. Collision strengths for resonance transitions in Fe XXIV. ......................................................................................................................... Table 23. Collision strengths for resonance transitions in Co XXV........................................................................................................................... Table 24. Collision strengths for resonance transitions in Ni XXVI. ......................................................................................................................... Table 25. Effective collision strengths for transitions in Sc XIX................................................................................................................................ Table 26. Effective collision strengths for transitions in Ti XX. ................................................................................................................................ Table 27. Effective collision strengths for transitions in V XXI. ................................................................................................................................ Table 28. Effective collision strengths for transitions in Cr XXII............................................................................................................................... Table 29. Effective collision strengths for transitions in Mn XXIII. .......................................................................................................................... Table 30. Effective collision strengths for transitions in Fe XXIV. ............................................................................................................................ Table 31. Effective collision strengths for transitions in Co XXV. ............................................................................................................................. Table 32. Effective collision strengths for transitions in Ni XXVI. ............................................................................................................................
1. Introduction
Emission lines of Li-like ions have been observed in the spectra of a variety of astrophysical [1,2] and laboratory plasmas [3,4]. Transitions of many Li-like ions are useful for temperature and density diagnostics of solar plasmas [2] as well as for the determination of chemical abundances [5]. However to analyse
2 3 3 5 6 8 11 11 11 11 12 12 12 12 12 12 12 12 12
12
12
12
12
12
12
12
13 13 13 13 13 13 13 13 13 13 13 13 13 13 13 13 13
observations, atomic data are required for a variety of parameters, such as energy levels, radiative rates (A-values), and excitation rates or equivalently the effective collision strengths (Υ ), which are obtained from the electron impact collision strengths (Ω ). These data are also required for the modelling of fusion plasmas, as many elements are present in the plasmas because of sputtering from the reactor walls. Similarly, data are required for diagnostics of laboratory plasmas [6]. With this in view we have already
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
reported calculations for Li-like ions with Z ≤ 20 [7–10] and in this paper we provide similar results for ions with 21 ≤ Z ≤ 28. Experimentally, there have been some measurements of energy levels for Li-like ions, which have been compiled by the National Institute of Standards and Technology (NIST) and are available at their website www.nist.gov/pml/data/asd.cfm. Theoretically, energy levels and A-values have been calculated by Nahar [11] for transitions in 15 Li-like ions with 6 ≤ Z ≤ 28. However, collisional atomic data are limited to transitions among the lowest three levels of Li-like ions with 8 ≤ Z ≤ 92, and from these levels to the higher excited levels of the n ≤ 5 configurations [12]. The calculations of Zhang et al. [12] are based on the relativistic distortedwave (DW) method, and collision strengths are reported only at six energies above thresholds. Since resonances in the threshold region have not been resolved, the subsequent results for effective collision strengths are significantly underestimated over a wide temperature range for a large number of transitions (in particular forbidden transitions), as already demonstrated in our earlier papers for ions with Z ≤ 20 [7–10]. In this paper we report a complete set of results (namely, energy levels, radiative rates, and effective collision strengths) for all transitions among the lowest 24 levels of Li-like ions with 21 ≤ Z ≤ 28. Additionally, we provide the A-values for four types of transitions, namely electric dipole (E1), electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions, because these are also required for plasma modelling. For our calculations of wavefunctions we employ the fully relativistic General-Purpose Relativistic Atomic Structure Package (grasp), originally developed by Grant et al. [13] and revised by P.H. Norrington. It is a fully relativistic code, and is based on the jj coupling scheme. Further relativistic corrections arising from the Breit interaction and QED effects (vacuum polarization and Lamb shift) have also been included. In calculating energy levels, we have kept the 1s shell frozen and have used the option of extended average level, in which a weighted (proportional to 2j+1) trace of the Hamiltonian matrix is minimized. This produces a compromise set of orbitals describing closely lying states with moderate accuracy. Similarly, for our calculations of Ω , we have adopted the Dirac Atomic R-matrix Code (darc) of P.H. Norrington and I.P. Grant (web.am.qub.ac.uk/DARC/). Finally, to make comparisons and to assess the accuracy of our results, we have performed analogous calculations from the Flexible Atomic Code (fac) of Gu [14], available from the website sprg.ssl.berkeley.edu/~mfgu/fac/. This is also a fully relativistic code that provides a variety of atomic parameters, and yields results comparable to grasp and darc — see, for example, Ref. [15] and references therein. Generally, there is no major discrepancy in the determination of energy levels and radiative rates between results of grasp and fac, but the former code allows more flexibility in terms of optimizations. Furthermore, in cases of strong mixing, the identification of different J levels belonging to a particular configuration is a greater problem in fac than in grasp, although it should not apply to simple Li-like ions. On the other hand, differences in collision strengths can sometimes be larger, particularly for the forbidden transitions, as discussed and demonstrated in some of our earlier papers [7–10]. Similarly, results for Υ can be significantly underestimated by fac, particularly for forbidden transitions and at lower temperatures, due to the neglect of the contribution of resonances. Nevertheless, results from fac will be helpful in assessing the accuracy of our energy levels, radiative rates, and collision strengths, and in estimating the contribution of resonances for the determination of Υ .
)
–
3
2. Energy levels The 1s2 nℓ (2 ≤ n ≤ 5) configurations of Li-like ions give rise to the lowest 24 energy levels listed in Tables 1–8. Included in these tables are the level energies from grasp, obtained without and with the inclusion of Breit and QED effects, plus the experimental energies compiled by NIST. Also listed in these tables are the theoretical energies obtained from our analogous calculations from fac and those by Nahar [11] from the Breit–Pauli R-matrix (BPRM) code of Berrington et al. [16]. The inclusion of the Breit and QED corrections decreases the energy levels (except for level 2, i.e., 2p 2 Po1/2 ) by a maximum of ∼0.1 Ryd, depending on the ion. As the ion nuclear charge Z increases, so does the effect of the Breit and QED corrections. For example, energy levels of Sc XIX decrease by ∼0.04 Ryd, but for Ni XXVI by ∼0.1 Ryd. Clearly, the importance of relativistic effects increases with increasing Z . Our Breit and QED corrected energies from grasp agree closely (generally within 0.02 Ryd) with those of NIST and the orderings are also nearly the same, although there is a noticeable difference for the 3s 2 S1/2 level of Sc XIX for which the NIST energy appears to be higher by ∼0.1 Ryd. Furthermore, the NIST energies for some levels are the same — see, for example, the 4f 2 Fo5/2,7/2 and 5p 2 Po1/2,3/2 levels of Sc XIX. Similarly, NIST energies are not available for some levels — see, for example, the 5f 2 Fo5/2,7/2 and 5g 2 G7/2,9/2 levels of all Li-like ions under consideration. The energies obtained from fac are generally comparable with the experimental compilations of NIST and/or our calculations from grasp. However, the orderings of some of the levels are slightly different from fac than from the experimental and other theoretical energies. As examples, see the 13–14 and 22–23 levels of Sc XIX and Ni XXVI. Nevertheless, the energy differences among these levels are very small. Finally, the BPRM energies of Nahar [11] have the same orderings as NIST and our calculations from grasp, but are higher for most of the levels by about 0.06 Ryd for Ti XX and 0.2 Ryd for Ni XXVI. Clearly, this is due to the neglect of the two-body relativistic effects in the BPRM calculations. Overall, we may state that there is no (major) discrepancy between theory and experiment for the energy levels of Li-like ions. 3. Radiative rates The absorption oscillator strength fij and radiative rate Aji (in s−1 ) for a transition i–j are related by the following expression: fij =
mc 8π 2 e2
λ2ji
ωj Aji = 1.49 × 10−16 λ2ji (ωj /ωi )Aji ωi
(1)
where m and e are the electron mass and charge, respectively, c is the velocity of light, λji is the transition wavelength in Å, and ωi and ωj are the statistical weights of the lower (i) and upper (j) levels, respectively. Similarly, the oscillator strength fij (dimensionless) and the line strength S (in atomic units, 1 a.u. = 6.460 × 10−36 cm2 esu2 ) are related by the following standard equations: for the electric dipole transitions Aji =
2.0261 × 1018
ωλ
3 j ji
S E1
and fij =
303.75
λji ωi
S E1 ,
(2)
for the magnetic dipole transitions Aji =
2.6974 × 1013
ωλ
3 j ji
S M1
and
fij =
4.044 × 10−3
λji ωi
S M1 ,
(3)
for the electric quadrupole transitions Aji =
1.1199 × 1018
ωj λ5ji
S E2
and fij =
167.89
λ3ji ωi
S E2 ,
(4)
4
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table A Comparison of radiative rates (A-values, s−1 ) for some transitions in Sc XIX. (a ± b ≡ a × 10±b ).
)
–
Table B Comparison of radiative rates (A-values, s−1 ) for some transitions in Ti XX. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 6 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.4088+09 2.2436+09 2.9037+12 2.8418+12 1.2853+12 1.2661+12 6.6475+11 6.5628+11 7.2211+12 2.3558+12 1.0869+12 8.5877+12 2.7892+12 1.2837+12 2.9760+08 3.7765+11 3.6813+11 2.0806+11 2.0405+11 7.5949+11 3.7414+11 9.1135+11 4.4674+11 5.1265+09 1.6828+12 2.2009+09 5.5580+11 1.1980+11 1.7984+12 3.9440+10 5.9323+11 8.8555+10 8.6131+10 1.5739+11 1.8974+11 2.7380+09 3.1477+11 2.2480+10 3.3695+11 5.3544+11
1.4170+09 2.2490+09 2.9520+12 2.8950+12 1.3450+12 1.3280+12 7.4680+11 7.3940+11 7.2530+12 2.3980+12 1.1650+12 8.6360+12 2.8420+12 1.3730+12 2.9670+08 3.8310+11 3.7380+11 2.2220+11 2.1810+11 7.6540+11 3.8740+11 9.1850+11 4.6190+11 5.2060+09 1.6820+12 2.4010+09 5.5650+11 1.1960+11 1.7980+12 3.9420+10 5.9440+11 9.1090+10 8.8640+10 1.6070+11 1.9360+11 2.7950+09 3.1380+11 2.2400+10 3.3600+11 5.3550+11
2.2257−02 5.2315−02 1.2380−01 2.4111−01 3.0979−02 6.0936−02 1.2900−02 2.5452−02 6.7380−01 1.2235−01 4.5196−02 6.1083−01 1.1005−01 4.0508−02 8.8766−02 1.3575−01 2.6303−01 3.5963−02 7.0385−02 5.8296−01 1.3622−01 5.3159−01 1.2319−01 2.0927−03 1.0135+00 4.1604−04 1.5669−01 4.8336−02 9.6650−01 7.4375−03 1.4911−01 1.5091−01 2.9156−01 5.6643−01 5.1813−01 5.2232−03 8.8440−01 4.2296−02 8.4432−01 1.3437+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
1.4907+09 2.5447+09 3.5749+12 3.4911+12 1.5800+12 1.5542+12 8.1676+11 8.0541+11 8.8657+12 2.8917+12 1.3340+12 1.0533+13 3.4188+12 1.5731+12 1.9328+08 3.3925+08 4.6591+11 4.5300+11 2.5631+11 2.5088+11 2.4095+07 9.3273+11 4.5946+11 1.2640+07 1.1192+12 5.4834+11 6.2633+09 2.0665+12 2.6896+09 6.8262+11 1.4706+11 2.2079+12 4.8404+10 7.2830+11 4.5265+07 8.0239+07 1.0936+11 1.0607+11 7.4663+06 1.9329+11 3.8843+06 2.3314+11 1.6307+04 3.3472+09 3.8650+11 1.4472+01 4.0837+03 2.7602+10 4.1369+11 6.5745+11 1.4704+07 2.6185+07 2.6949+06 1.3974+06 8.3660+03 9.2274+00 2.1866+03 2.7721+02
1.4990+09 2.5500+09 3.6310+12 3.5540+12 1.6500+12 1.6270+12 9.1200+11 9.0220+11 8.9040+12 2.9410+12 1.4250+12 1.0590+13 3.4810+12 1.6780+12
1.4030+09 2.5930+09 3.6770+12 3.5830+12 1.3880+12 1.3630+12 7.4220+11 7.3070+11 8.8800+12 2.8480+12 1.3250+12 1.0540+13 3.3630+12 1.5610+12 1.6820+08 3.2530+08 4.3630+11 4.2210+11 2.4470+11 2.3870+11 2.6690+07 9.2720+11 4.6000+11 1.2510+07 1.1130+12 5.4910+11 1.7550+12 2.0740+12 1.2150+06 6.8420+11 1.4750+11 2.2150+12 4.8480+10 7.2960+11 2.9160+08 4.2270+08 1.0170+11 9.7840+10 2.0560+07 1.9160+11 1.2340+07 2.3150+11 1.8750+04 1.8630+11 3.8590+11 7.7210+00 3.9990+03 2.7560+10 4.1310+11 6.5660+11 8.2050+07 1.2070+08 5.7560+06 3.2770+06 9.5790+03 5.0810+00 2.1250+03 3.0120+02
2.1176−02 5.0977−02 1.2474−01 2.4228−01 3.1126−02 6.1127−02 1.2949−02 2.5518−02 6.7361−01 1.2229−01 4.5170−02 6.1113−01 1.0998−01 4.0469−02 3.5750−02 8.6622−02 1.3690−01 2.6440−01 3.6170−02 7.0638−02 2.6693−02 5.8285−01 1.3620−01 1.8246−02 5.3223−01 1.2323−01 2.0804−03 1.0132+00 4.1388−04 1.5669−01 4.8328−02 9.6633−01 7.4344−03 1.4908−01 4.9417−02 1.1998−01 1.5227−01 2.9315−01 4.7484−02 5.6630−01 3.2363−02 5.1892−01 3.6407−03 5.1952−03 8.8399−01 4.0115−05 2.1363−03 4.2296−02 8.4414−01 1.3435+00 6.2748−02 1.5249−01 6.6087−02 4.4991−02 6.8101−03 8.0693−05 4.0532−03 1.3874−03
GRASP: Present results from grasp. FAC: Present results from fac.
and for the magnetic quadrupole transitions Aji =
1.4910 × 1013
ωj λ5ji
S M2
and fij =
2.236 × 10−3
λ3ji ωi
S M2 .
(5)
In Tables 9–16 we present transition wavelengths, radiative rates, oscillator strengths, and line strengths, in length form only, for all 92 electric dipole transitions among the 24 levels of Lilike ions with 21 ≤ Z ≤ 28. The indices used to represent the lower and upper levels of a transition have already been defined in Tables 1–8. Similarly, there are 100 electric quadrupole, 79 magnetic dipole, and 108 magnetic quadrupole transitions among the 24 levels. However, for these transitions only the A-values are listed in Tables 9–16, and the corresponding results for f - or Svalues may be easily obtained using Eqs. (1)–(5). In Tables A–H we compare our A-values from grasp and fac for some of the common E1 transitions with those of Nahar [11] from the BPRM code of Berrington et al. [16]. Also included in these tables are the f -values from our grasp calculations. In general, the A-values from grasp and fac agree satisfactorily (within ∼10%) for a majority of transitions for all ions. However, there are significant differences with the Nahar calculations, of up to two orders of magnitude, particularly for the comparatively weaker (f ≤ 0.01) transitions, such as 7–11, 7–18, and 12–18. Similar large differences have also been noted for transitions of other
4.7240+11 4.5970+11 2.7290+11 2.6730+11 9.3960+11 4.7490+11 1.1280+12 5.6610+11 6.3600+09 2.0650+12 2.9250+09 6.8360+11 1.4680+11 2.2080+12 4.8380+10 7.2980+11
1.1230+11 1.0900+11 1.9710+11 2.3760+11 3.4160+09 3.8550+11
2.7510+10 4.1270+11 6.5750+11
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
Li-like ions with Z ≤ 20 [8–10]. The A-values for such weak transitions from the BPRM code are likely to be less accurate, as discussed by Hibbert [17] and Aggarwal et al. [18]. In addition, several transitions are missing from the Nahar calculations, and examples include 2p 2 Po1/2 –3s 2 S1/2 (2–4), 2p 2 Po3/2 –3s 2 S1/2 (3–4), and 2p 2 Po3/2 –3d 2 D3/2 (3–7). Finally, there are significantly large differences (of over an order of magnitude) between the BPRM A-values of Nahar and our calculations from grasp for several transitions among levels 16 and higher. For all such transitions, the
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables ( Table C Comparison of radiative rates (A-values, s−1 ) for some transitions in V XXI. (a ± b ≡ a × 10±b ).
)
–
5
Table D Comparison of radiative rates (A-values, s−1 ) for some transitions in Cr XXII. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.5739+09 2.8950+09 4.3570+12 4.2452+12 1.9230+12 1.8887+12 9.9358+11 9.7857+11 1.0778+13 3.5149+12 1.6215+12 1.2792+13 4.1493+12 1.9088+12 5.6888+11 5.5162+11 3.1253+11 3.0531+11 1.1340+12 5.5866+11 1.3607+12 6.6637+11 7.5793+09 2.5125+12 3.2555+09 8.3005+11 1.7873+11 2.6836+12 5.8814+10 8.8520+11 1.3364+11 1.2923+11 2.3498+11 2.8357+11 4.0527+09 4.6984+11 3.3554+10 5.0285+11 7.9923+11
1.5830+09 2.9010+09 4.4220+12 4.3200+12 2.0030+12 1.9740+12 1.1030+12 1.0910+12 1.0820+13 3.5730+12 1.7270+12 1.2870+13 4.2230+12 2.0300+12 5.7650+11 5.5950+11 3.3170+11 3.2440+11 1.1420+12 5.7660+11 1.3710+12 6.8690+11 7.6950+09 2.5110+12 3.5310+09 8.3120+11 1.7840+11 2.6840+12 5.8770+10 8.8710+11 1.3710+11 1.3270+11 2.3940+11 2.8870+11 4.1350+09 4.6870+11 3.3450+10 5.0180+11 7.9940+11
2.0198−02 4.9883−02 1.2559−01 2.4323−01 3.1258−02 6.1281−02 1.2993−02 2.5571−02 6.7331−01 1.2222−01 4.5146−02 6.1136−01 1.0992−01 4.0432−02 1.3794−01 2.6550−01 3.6356−02 7.0841−02 5.8258−01 1.3616−01 5.3277−01 1.2326−01 2.0692−03 1.0128+00 4.1191−04 1.5668−01 4.8320−02 9.6614−01 7.4312−03 1.4906−01 1.5351−01 2.9442−01 5.6599−01 5.1959−01 5.1697−03 8.8355−01 4.2295−02 8.4395−01 1.3433+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
1.6584+09 3.3042+09 5.2619+12 5.1146+12 2.3192+12 2.2743+12 1.1978+12 1.1782+12 1.2985+13 4.2346+12 1.9535+12 1.5395+13 4.9910+12 2.2955+12 2.1571+08 4.4502+08 6.8816+11 6.6537+11 3.7759+11 3.6809+11 3.7274+07 1.3663+12 6.7317+11 1.6271+07 1.6394+12 8.0251+11 9.0925+09 3.0271+12 3.9065+09 1.0002+12 2.1525+11 3.2322+12 7.0816+10 1.0662+12 5.0559+07 1.0560+08 1.6177+11 1.5596+11 1.1585+07 2.8304+11 5.0104+06 3.4177+11 3.5887+04 4.8642+09 5.6600+11 1.6902+01 8.0438+03 4.0420+10 6.0570+11 9.6280+11 1.6430+07 3.4515+07 4.1868+06 1.8042+06 1.8175+04 1.0772+01 4.2329+03 7.1401+02
1.6680+09 3.3100+09 5.3370+12 5.2020+12 2.4110+12 2.3730+12 1.3240+12 1.3070+12 1.3040+13 4.3020+12 2.0760+12 1.5480+13 5.0770+12 2.4350+12
1.5480+09 3.3930+09 5.4330+12 5.2700+12 1.9700+12 1.9270+12 1.0580+12 1.0390+12 1.3010+13 4.1670+12 1.9440+12 1.5410+13 4.9040+12 2.2810+12 1.8410+08 4.2800+08 6.3280+11 6.0820+11 3.5550+11 3.4520+11 4.2150+07 1.3580+12 6.7520+11 1.6270+07 1.6300+12 8.0490+11 2.5660+12 3.0400+12 1.3600+06 1.0030+12 2.1610+11 3.2450+12 7.0950+10 1.0690+12 5.5190+08 8.2890+08 1.4640+11 1.3960+11 3.4530+07 2.8070+11 1.8440+07 3.3960+11 4.0690+04 2.7310+11 5.6500+11 7.0400+00 7.6720+03 4.0350+10 6.0460+11 9.6120+11 1.5970+08 2.4260+08 8.7510+06 4.2630+06 2.0560+04 4.7010+00 4.0070+03 7.6510+02
1.9307−02 4.9008−02 1.2637−01 2.4400−01 3.1376−02 6.1403−02 1.3033−02 2.5613−02 6.7293−01 1.2216−01 4.5124−02 6.1154−01 1.0986−01 4.0396−02 3.2636−02 8.3532−02 1.3889−01 2.6637−01 3.6524−02 7.1002−02 2.7168−02 5.8217−01 1.3611−01 1.7470−02 5.3322−01 1.2329−01 2.0589−03 1.0125+00 4.1011−04 1.5667−01 4.8312−02 9.6594−01 7.4278−03 1.4904−01 4.5132−02 1.1582−01 1.5463−01 2.9541−01 4.8385−02 5.6550−01 3.1012−02 5.2014−01 4.1696−03 5.1462−03 8.8308−01 3.7188−05 2.3579−03 4.2295−02 8.4375−01 1.3430+00 5.7320−02 1.4726−01 6.7376−02 4.3129−02 7.7661−03 7.4800−05 4.4480−03 1.6746−03
GRASP: Present results from grasp. FAC: Present results from fac.
energy differences (∆Eij ) are very small and hence small changes in these affect the A-values significantly. One of the general criteria to assess the accuracy of radiative rates is to compare the length and velocity forms of the f - or Avalues. However, such comparisons are only desirable, and are not a fully sufficient test to assess accuracy, as different calculations (or combinations of configurations) may give comparable f -values in the two forms, but entirely different results in magnitude. Generally, there is good agreement between the length and velocity forms of the f -values for strong transitions, but differences between the two forms can sometimes be substantial even for some very strong transitions, as demonstrated by Aggarwal et al. [19]. However, for transitions of Li-like ions, there is no discrepancy between the two forms, and this is irrespective of the magnitude of a transition. Furthermore, to assess the importance of configuration interaction (CI), we have performed another calculation including the levels of the n = 6 configurations. Only for two transitions, namely 2–16 (2p 2 Po1/2 –5s 2 S1/2 ) and 3–16 (2p 2 Po3/2 –5s 2 S1/2 ), have the A-values decreased by 20% for Sc XIX and by 15% for Ni XXVI. For the remaining transitions the effect of additional CI is much less noticeable. Based on this and other comparisons discussed above, we may state that the A-values listed in Tables 9–16 from our grasp calculations are accurate to better than 20% for all transitions and all ions, and hence should be the best currently available.
6.9700+11 6.7460+11 3.9970+11 3.9010+11 1.3760+12 6.9390+11 1.6510+12 8.2620+11 9.2300+09 3.0260+12 4.2260+09 1.0020+12 2.1480+11 3.2330+12 7.0750+10 1.0690+12
1.6580+11 1.5990+11 2.8810+11 3.4760+11 4.9610+09 5.6480+11
4.0310+10 6.0470+11 9.6300+11
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
4. Lifetimes The lifetime τ for a level j is defined as follows: 1
τj =
Aji
.
(6)
i
Since this is a measurable parameter, it provides a check on the accuracy of the calculations. Therefore, in Tables 1–8 we have also listed our calculated lifetimes from grasp, which include
6
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table E Comparison of radiative rates (A-values, s−1 ) for some transitions in Mn XXIII. (a ± b ≡ a × 10±b ).
)
–
Table F Comparison of radiative rates (A-values, s−1 ) for some transitions in Fe XXIV. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.7445+09 3.7834+09 6.3020+12 6.1102+12 2.7742+12 2.7159+12 1.4322+12 1.4069+12 1.5516+13 5.0604+12 2.3345+12 1.8376+13 5.9545+12 2.7381+12 8.2540+11 7.9568+11 4.5238+11 4.4003+11 1.6324+12 8.0451+11 1.9588+12 9.5852+11 1.0822+10 3.6171+12 4.6506+09 1.1954+12 2.5710+11 3.8610+12 8.4564+10 1.2736+12 1.9416+11 1.8658+11 3.3810+11 4.0849+11 5.7920+09 6.7621+11 4.8291+10 7.2357+11 1.1503+12
1.7540+09 3.7890+09 6.3880+12 6.2120+12 2.8790+12 2.8290+12 1.5760+12 1.5550+12 1.5580+13 5.1380+12 2.4750+12 1.8480+13 6.0550+12 2.8980+12 8.3560+11 8.0640+11 4.7770+11 4.6530+11 1.6430+12 8.2830+11 1.9720+12 9.8560+11 1.0980+10 3.6160+12 5.0190+09 1.1970+12 2.5660+11 3.8630+12 8.4470+10 1.2770+12 1.9880+11 1.9120+11 3.4380+11 4.1510+11 5.9060+09 6.7500+11 4.8170+10 7.2250+11 1.1510+12
1.8494−02 4.8329−02 1.2707−01 2.4459−01 3.1482−02 6.1496−02 1.3068−02 2.5645−02 6.7245−01 1.2210−01 4.5105−02 6.1166−01 1.0980−01 4.0362−02 1.3976−01 2.6702−01 3.6677−02 7.1123−02 5.8162−01 1.3604−01 5.3359−01 1.2331−01 2.0495−03 1.0121+00 4.0846−04 1.5666−01 4.8302−02 9.6573−01 7.4243−03 1.4901−01 1.5566−01 2.9616−01 5.6484−01 5.2060−01 5.1247−03 8.8258−01 4.2294−02 8.4353−01 1.3428+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.8321+09 4.3461+09 7.4905+12 7.2436+12 3.2936+12 3.2188+12 1.6997+12 1.6673+12 1.8404+13 6.0027+12 2.7694+12 2.1770+13 7.0510+12 3.2417+12 9.8236+11 9.4404+11 5.3784+11 5.2195+11 1.9357+12 9.5426+11 2.3227+12 1.1363+12 1.2787+10 4.2896+12 5.4965+09 1.4179+12 3.0476+11 4.5773+12 1.0022+11 1.5099+12 2.3121+11 2.2143+11 4.0078+11 4.8453+11 6.8467+09 8.0181+11 5.7259+10 8.5786+11 1.3640+12
1.8420+09 4.3510+09 7.5880+12 7.3630+12 3.4130+12 3.3490+12 1.8630+12 1.8360+12 1.8480+13 6.0910+12 2.9300+12 2.1900+13 7.1670+12 3.4250+12 9.9410+11 9.5650+11 5.6670+11 5.5070+11 1.9480+12 9.8150+11 2.3380+12 1.1670+12 1.2980+10 4.2890+12 5.9190+09 1.4200+12 3.0420+11 4.5810+12 1.0010+11 1.5140+12 2.3650+11 2.2670+11 4.0730+11 4.9190+11 6.9800+09 8.0060+11 5.7120+10 8.5690+11 1.3640+12
1.7748−02 4.7827−02 1.2772−01 2.4502−01 3.1578−02 6.1563−02 1.3099−02 2.5668−02 6.7190−01 1.2204−01 4.5087−02 6.1173−01 1.0973−01 4.0328−02 1.4055−01 2.6748−01 3.6817−02 7.1209−02 5.8094−01 1.3596−01 5.3388−01 1.2332−01 2.0408−03 1.0117+00 4.0695−04 1.5664−01 4.8293−02 9.6551−01 7.4207−03 1.4899−01 1.5660−01 2.9667−01 5.6403−01 5.2096−01 5.1047−03 8.8205−01 4.2292−02 8.4330−01 1.3425+00
GRASP: Present results from grasp. FAC: Present results from fac.
GRASP: Present results from grasp. FAC: Present results from fac.
the contributions from four types of transitions (i.e., E1, E2, M1, and M2). To our knowledge, no measurements are available for lifetimes in most of the Li-like ions with 21 ≤ Z ≤ 28. However, Grandin et al. [20] have measured the lifetime for the 2p 2 Po3/2 level of Cr XXII to be 307 ± 20 ps, which agrees very well with our result and the other [21] calculated value of 303 ps. Froese-Fischer has calculated lifetimes for all the Li-like ions under discussion here and has posted results for some levels up to 4s 2 S1/2 on the website www.vuse.vanderbilt.edu/~cff/mchf_collection/. For all levels and ions the discrepancies between the Froese-Fischer results and our calculations are generally less than ∼10%. However, discrepancies between the two independent calculations for the 2p 2 Po1/2 level are significantly larger, up to a factor of two depending on the ion. In Table I we compare our calculations using grasp with her work using the mchf code for the 2p 2 Po1/2 level of Li-like ions with 11 ≤ Z ≤ 28. For ions up to Z = 22 (Ti XX), the two sets of lifetimes agree within 10%, but for heavier ions the discrepancy increases with increasing nuclear charge. As Z increases, the lifetimes in our calculations from grasp decrease for all ions. However, this is also the case in the mchf calculations, but only up to Z = 23. After that the mchf lifetimes increase with increasing Z and thus widen the discrepancy with our calculations from grasp. We have confidence in our calculations and hope the present results for all levels will be useful for future comparisons, and may also encourage experimentalists to measure lifetimes for the Li-like ions.
5. Collision strengths For the computation of collision strengths we have employed darc, which includes the relativistic effects in a systematic way, in both the target description and the scattering model. It is based on the jj coupling scheme, and uses the Dirac–Coulomb Hamiltonian in the R-matrix approach. The R-matrix radii adopted for Li-like ions with 21 ≤ Z ≤ 28 are 4.80, 4.48, 4.16, 4.00, 3.84, 3.68, 3.52, and 3.36 atomic units, respectively. For all eight ions, 56 continuum orbitals have been included for each channel angular momentum for the expansion of the wavefunction. This allows us to compute Ω up to an energy of 700, 800, 920, 1000, 1070, 1160, 1280, and 1400 Ryd, for 21 ≤ Z ≤ 28, respectively. Furthermore, these energy ranges are sufficient to calculate values of Υ up to Te = 107.8 K, (i.e., well above the temperature of maximum abundance of these ions in ionization equilibrium — see Bryans et al. [22]). The maximum number of channels for a partial wave is 108, and the corresponding size of the Hamiltonian matrix is 6086. To obtain convergence of Ω for all transitions and at all energies, we have included all partial waves with angular momentum J ≤ 60, although a larger number would have been preferable for the convergence of some allowed transitions, especially at higher energies. However, to account for the neglected higher partial waves, we have included a ‘‘top-up’’, based on the Coulomb–Bethe [23] approximation for allowed transitions and geometric series for others.
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables ( Table G Comparison of radiative rates (A-values, s−1 ) for some transitions in Co XXV. (a ± b ≡ a × 10±b ).
)
–
7
Table H Comparison of radiative rates (A-values, s−1 ) for some transitions in Ni XXVI. (a ± b ≡ a × 10±b ).
i
j
A(GRASP)
A(FAC)
f (GRASP)
i
j
A(GRASP)
A(FAC)
A(BPRM)
f (GRASP)
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 5 5 6 6 7 7 7 7 8 8 8 8 9 9 10 11 12 12 13 13 14
2 3 5 6 10 11 17 18 7 12 19 8 13 20 10 11 17 18 12 19 13 20 11 14 18 21 14 15 21 22 17 18 19 20 18 21 21 22 23
1.9213+09 5.0082+09 8.8414+12 8.5266+12 3.8833+12 3.7882+12 2.0032+12 1.9622+12 2.1679+13 7.0723+12 3.2630+12 2.5613+13 8.2923+12 3.8118+12 1.1609+12 1.1120+12 6.3497+11 6.1473+11 2.2794+12 1.1241+12 2.7350+12 1.3377+12 1.5009+10 5.0520+12 6.4531+09 1.6702+12 3.5876+11 5.3889+12 1.1795+11 1.7777+12 2.7337+11 2.6088+11 4.7176+11 5.7070+11 8.0395+09 9.4415+11 6.7423+10 1.0100+12 1.6061+12
1.9320+09 5.0130+09 8.9520+12 8.6650+12 4.0180+12 3.9370+12 2.1870+12 2.1540+12 2.1770+13 7.1730+12 3.4460+12 2.5770+13 8.4270+12 4.0200+12 1.1740+12 1.1260+12 6.6760+11 6.4740+11 2.2940+12 1.1550+12 2.7530+12 1.3730+12 1.5230+10 5.0520+12 6.9300+09 1.6730+12 3.5810+11 5.3940+12 1.1780+11 1.7820+12 2.7940+11 2.6680+11 4.7910+11 5.7900+11 8.1930+09 9.4290+11 6.7270+10 1.0090+12 1.6070+12
1.7061−02 4.7486−02 1.2831−01 2.4532−01 3.1664−02 6.1606−02 1.3126−02 2.5682−02 6.7127−01 1.2197−01 4.5070−02 6.1176−01 1.0967−01 4.0295−02 1.4128−01 2.6777−01 3.6944−02 7.1263−02 5.8014−01 1.3587−01 5.3411−01 1.2332−01 2.0327−03 1.0113+00 4.0555−04 1.5663−01 4.8282−02 9.6527−01 7.4170−03 1.4896−01 1.5746−01 2.9697−01 5.6308−01 5.2124−01 5.0862−03 8.8150−01 4.2291−02 8.4305−01 1.3422+00
1 1 1 1 1 1 1 1 2 2 2 3 3 3 4 4 4 4 4 4 5 5 5 6 6 6 7 7 7 7 8 8 8 8 9 9 9 9 10 10 11 11 12 12 12 13 13 13 13 14 16 16 17 18 19 20 20 21
2 3 5 6 10 11 17 18 7 12 19 8 13 20 5 6 10 11 17 18 7 12 19 8 13 20 11 14 18 21 14 15 21 22 10 11 17 18 12 19 13 20 14 18 21 14 15 21 22 23 17 18 19 20 21 21 22 23
2.0122+09 5.7889+09 1.0369+13 9.9716+12 4.5496+12 4.4298+12 2.3460+12 2.2945+12 2.5376+13 8.2804+12 3.8207+12 2.9943+13 9.6906+12 4.4538+12 2.6303+08 7.9566+08 1.3630+12 1.3011+12 7.4481+11 7.1927+11 9.1748+07 2.6669+12 1.3158+12 2.7488+07 3.2000+12 1.5647+12 1.7510+10 5.9119+12 7.5298+09 1.9549+12 4.1963+11 6.3040+12 1.3792+11 2.0796+12 6.1708+07 1.9002+08 3.2108+11 3.0528+11 2.8687+07 5.5170+11 8.5089+06 6.6787+11 1.5389+05 9.3819+09 1.1047+12 2.1655+01 2.9248+04 7.8884+10 1.1816+12 1.8792+12 2.0060+07 6.2283+07 1.0393+07 3.0712+06 7.6541+04 1.3801+01 1.4987+04 3.7657+03
2.0230+09 5.7940+09 1.0490+13 1.0130+13 4.7010+12 4.6000+12 2.5530+12 2.5110+12 2.5480+13 8.3950+12 4.0280+12 3.0130+13 9.8450+12 4.6900+12
1.9590+09 6.3140+09 1.0810+13 1.0380+13 4.1760+12 4.0690+12 1.8090+12 1.7710+12 2.5470+13 8.1070+12 3.8080+12 3.0000+13 9.4740+12 4.4300+12 2.4260+08 8.4070+08 1.2850+12 1.2190+12 6.3580+11 6.1100+11 1.0570+08 2.6390+12 1.3210+12 2.7010+07 3.1710+12 1.5710+12 4.9960+12 5.9380+12 1.5460+06 1.9600+12 4.2120+11 6.3290+12 1.3810+11 2.0840+12 6.7760+08 1.2810+09 2.6400+11 2.4650+11 1.0700+08 5.4630+11 4.6560+07 6.6310+11 1.7420+05 5.3220+11 1.1020+12 6.2430+00 2.8090+04 7.8700+10 1.1790+12 1.8750+12 1.2070+09 1.7500+09 2.3810+07 8.7950+06 8.6850+04 4.4410+00 1.4400+04 3.9950+03
1.6427−02 4.7293−02 1.2886−01 2.4548−01 3.1743−02 6.1628−02 1.3151−02 2.5689−02 6.7056−01 1.2191−01 4.5055−02 6.1175−01 1.0961−01 4.0262−02 2.7840−02 8.1123−02 1.4196−01 2.6789−01 3.7061−02 7.1287−02 2.9316−02 5.7923−01 1.3577−01 1.6634−02 5.3427−01 1.2332−01 2.0253−03 1.0108+00 4.0425−04 1.5662−01 4.8272−02 9.6503−01 7.4130−03 1.4893−01 3.8532−02 1.1271−01 1.5826−01 2.9709−01 5.2329−02 5.6198−01 2.9586−02 5.2144−01 5.4191−03 5.0691−03 8.8092−01 3.2295−05 2.9008−03 4.2289−02 8.4279−01 1.3419+00 4.8958−02 1.4344−01 7.2938−02 4.1184−02 1.0033−02 6.4969−05 5.4239−03 2.3324−03
GRASP: Present results from grasp. FAC: Present results from fac.
For illustration, in Figs. 1–3 we show the variation of Ω with angular momentum J for three transitions in Fe XXIV, namely 1–3 (2s 2 S1/2 –2p 2 Po3/2 ), 1–8 (2s 2 S1/2 –3d 2 D5/2 ), and 1–10 (2s 2 S1/2 –4p
2 o P1/2 ), respectively, and at five energies, 200, 400, 600, 800, and 1000 Ryd. Values of Ω have fully converged for all forbidden (such as 1–8) and most of the allowed (such as 1–10) transitions. However, for some allowed transitions, such as 1–3 shown in Fig. 1, our adopted range of partial waves (J ≤ 60) is not sufficient for the convergence of Ω at most of the energies, particularly above thresholds. For such transitions the top-up has been included as mentioned above, and has been found to be appreciable. A similar conclusion applies to the transitions in other Li-like ions. In Tables 17–24 we list our values of Ω for resonance transitions in Li-like ions with 21 ≤ Z ≤ 28 at energies above thresholds. The indices used to represent the levels of a transition have already been defined in Tables 1–8. Very limited data are available for comparison, as already stated in Section 1. Therefore, to make an accuracy assessment of the values of Ω , we have performed another calculation using fac. This code is also fully relativistic, and is based on the well-known and widely-used DW method. Furthermore, the same CI is included in fac as in the calculations from darc. Therefore, also included in Tables 17–24 for comparison purposes are the Ω values from fac at a single excited energy Ej , which corresponds to ∼ 500, 560, 600, 660, 750, 820, 900, and 980 Ryd for 21 ≤ Z ≤ 28, respectively. Generally, the two sets of Ω from darc and fac agree to within 20% for a majority of transitions. However, for ∼15% of the tran-
1.3780+12 1.3180+12 7.8170+11 7.5620+11 2.6830+12 1.3510+12 3.2200+12 1.6040+12 1.7770+10 5.9130+12 8.0710+09 1.9580+12 4.1880+11 6.3110+12 1.3770+11 2.0850+12
3.2800+11 3.1200+11 5.5990+11 6.7720+11 9.5590+09 1.1030+12
7.8720+10 1.1810+12 1.8800+12
GRASP: Present results from grasp. FAC: Present results from fac. BPRM: Nahar [11].
sitions there are differences of over 20%, and for ∼5% the discrepancies between the two independent calculations are up to a factor of two. Most of the transitions for which the discrepancies are large are forbidden, and one of the main reasons is the anomalous behaviour of Ω in the calculations from fac. To illustrate this, in Fig. 4 we compare the two sets of Ω from darc and fac for three allowed transitions in Fe XXIV, namely 4–6 (3s 2 S1/2 –3p 2 Po3/2 ), 6–8 (3p 2 Po3/2 –3d 2 D5/2 ), and 10–12 (4p 2 o P1/2 –4d 2 D3/2 ).
For these three and many other allowed transitions there are no major discrepancies between the two sets of
8
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table I Comparison of lifetimes (τ , s) for the 2p 2 Po1/2 level of Li-like ions with 11 ≤ Z ≤ 28. (a ± b ≡ a × 10±b ). Ion
GRASP
MCHF
Na IX Mg X Al XI Si XII P XIII S XIV Cl XV Ar XVI K XVII Ca XVIII Sc XIX Ti XX V XXI Cr XXII Mn XXIII Fe XXIV Co XXV Ni XXVI
1.552−09 1.394−09 1.264−09 1.155−09 1.063−09 9.840−10 9.151−10 8.546−10 8.009−10 7.530−10 7.098−10 6.708−10 6.354−10 6.030−10 5.732−10 5.458−10 5.208−10 4.970−10
1.603−09 1.437−09 1.301−09 1.189−09 1.094−09 1.014−09 9.452−10 8.863−10 8.363−10 7.943−10 7.601−10 7.341−10 7.180−10 7.136−10 7.255−10 7.629−10 8.444−10 1.018−09
GRASP: Present results from grasp. MCHF: Earlier results from mchf.
Fig. 1. Partial collision strengths for the 2s 2 S1/2 –2p 2 Po3/2 (1–3) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
Fig. 3. Partial collision strengths for the 2s 2 S1/2 –4p 2 Po1/2 (1–10) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
(and some other) transitions are generally within 50%, but are up to a factor of two for a few, such as 12–16, 13–16, 16–18, 19–21, and 20–22. For some transitions, such as 6–11, there are differences over the entire energy range, while for others such as 8–13, the discrepancies are mainly at the lower end of the energy range, and completely disappear at large energies. In some cases, such as 10–13, the differences between the two sets of Ω are mainly at the higher end of the energy range due to a sudden anomaly in Ω from fac. Such anomalies are larger, up to an order of magnitude in the case of Ni XXVI, and common for all ions particularly for the 9–21, 9–22, and 21–24 transitions. Discrepancies in the values of Ω for some transitions from darc and fac are partly due to the differences in the methodology, that is, the R-matrix and DW methods, respectively, but mainly because fac is designed to generate a large amount of atomic data in a comparatively very short period of time, and without too much loss of accuracy. This aim is achieved by employing various interpolation and extrapolation techniques, which result in significant differences in the values of Ω for some transitions and at some energies, as noted above. Overall, we may state that for transitions for which there is no anomaly in the calculations of Ω from fac, the differences between the darc and fac calculations of collision strengths are generally lower than 20%. However, the discrepancies are significant for those transitions for which values of Ω from fac are anomalous. A similar conclusion applies to transitions in other Li-like ions. Finally, based on the comparisons made above as well as for other Li-like ions [7– 10], we estimate our results for Ω to be accurate to better than 20% for a majority of the transitions of all eight Li-like ions. 6. Effective collision strengths
Fig. 2. Partial collision strengths for the 2s 2 S1/2 –3d 2 D5/2 (1–8) transition in Fe XXIV, at five energies, 200 Ryd (circles), 400 Ryd (triangles), 600 Ryd (stars), 800 Ryd (squares), and 1000 Ryd (diamonds).
Excitation rates, along with energy levels and radiative rates, are required for plasma modelling, and are determined from the collision strengths. Since the threshold energy region is dominated by numerous closed-channel (Feshbach) resonances, values of Ω need to be calculated using a fine energy mesh in order to accurately account for their contribution. Furthermore, in a hot plasma electrons have a wide distribution of velocities, and therefore values of Ω are generally weighted over a Maxwellian distribution as follows:
Ω , although there is a fall in magnitude in ΩFAC for these (and
Υ (Te ) =
some other) transitions at the lower end of the energy range for all ions. In Fig. 5 we show similar comparisons for three forbidden transitions, namely 6–11 (3p 2 Po3/2 –4p 2 Po3/2 ), 8–13 (3d 2 D5/2 –4d 2
D5/2 ), and 10–13 (4p 2 Po1/2 –4d 2 D5/2 ). Differences for these three
∞
Ω (Ej ) exp(−Ej /kTe )d(Ej /kTe ),
(7)
0
where k (= 6.334 × 10−6 Ryd/K) is Boltzmann constant, Te is electron temperature in K, and Ej is the electron energy (in Ryd) with respect to the final (excited) state. Once the value of Υ is
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Fig. 4. Comparison of collision strengths from our calculations using darc (continuous curves) and fac (broken curves) for the 4–6 (circles: 3s 2 S1/2 –3p 2 Po3/2 ), 6–8 (triangles: 3p 2 Po3/2 –3d2 D5/2 ), and 10–12 (stars: 4p 2 Po1/2 –4d 2 D3/2 ) allowed transitions in Fe XXIV.
Fig. 7. Collision strengths for the 2s 2 S1/2 –2p 2 Po3/2 (1–3) transition in Fe XXIV.
Fig. 5. Comparison of collision strengths from our calculations using darc (continuous curves) and fac (broken curves) for the 6–11 (triangles: 3p 2 Po3/2 –4p 2 o P3/2 ), 8–13 (stars: 3d 2 D5/2 –4d 2 D5/2 ), and 10–13 (circles: 4p 2 Po1/2 –4d 2 D5/2 ) forbidden transitions in Fe XXIV.
Fig. 8. Collision strengths for the 2p 2 Po1/2 –2p 2 Po3/2 (2–3) transition in Fe XXIV.
Fig. 9. Collision strengths for the 3d 2 D3/2 –3d 2 D5/2 (7–8) transition in Fe XXIV. 2
Fig. 6. Collision strengths for the 2s S1/2 –2p
2 o P1/2
(1–2) transition in Fe XXIV.
and
known the corresponding results for the excitation rate q(i, j) and de-excitation rate q(j, i) can be easily obtained from the following equations: q(i, j) =
8.63 × 10−6 1/2
ωi Te
Υ exp(−Eij /kTe ) cm s
3 −1
(8)
q(j, i) =
8.63 × 10−6 1/2
ωj Te
Υ cm3 s−1 ,
(9)
where, as above, ωi and ωj are the statistical weights of the lower (i) and upper (j) levels, respectively, and Eij is the transition energy. The contribution of resonances may enhance the values of Υ
10
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Fig. 10. Comparison of effective collision strengths for the 7–8 (circles: 3d 2 D3/2 –3d D5/2 ), 12–13 (triangles: 4d 2 D3/2 –4d 2 D5/2 ), and 14–15 (stars: 4f 2 Fo5/2 –4f 2 Fo7/2 ) transitions in Fe XXIV. Continuous and broken curves are from the present darc and earlier BPRM calculations [25], respectively. 2
over those of the background values of collision strengths (ΩB ), especially for the forbidden transitions, by up to a factor of ten (or even more) depending on the transition and/or the temperature. Similarly, values of Ω need to be calculated over a wide energy range (above thresholds) in order to obtain convergence of the integral in Eq. (7), as demonstrated in Fig. 7 of Ref. [24]. To delineate resonances, we have performed our calculations of Ω in the threshold region at over 73 000 energies, depending on the ion. Close to thresholds (∼0.1 Ryd above a threshold) the energy mesh is 0.001 Ryd, and away from thresholds is 0.002 Ryd. Thus, care has been taken to include as many resonances as possible, and with as fine a resolution as is computationally feasible. The density and importance of resonances can be appreciated from Figs. 6–8, where we show Ω in the threshold region for three transitions in Fe XXIV, namely 1–2 (2s 2 S1/2 –2p 2 Po1/2 ), 1–3
(2s 2 S1/2 –2p 2 Po3/2 ), and 2–3 (2p 2 Po1/2 –2p 2 Po3/2 ). Similar resonances are observed for transitions in other Li-like ions. These resonances affect the values of Υ particularly towards the lower end of the temperature range. Our calculated values of Υ are listed in Tables 25–32 over a wide temperature range up to 107.8 K, suitable for applications to astrophysical and laboratory plasmas. As stated in Section 1, there are no similar results available for comparison purposes for most of the ions. Therefore, as for collision strengths we have also calculated values of Υ from our non-resonant Ω data from fac, which are included in Tables 25–32 at the lowest and the highest calculated temperatures for each ion. This provides a comparison between the two independent calculations, and also gives an estimate of the importance of resonances. For example, at Te = 106.1 K, our resonance-resolved values of Υ differ by over 20% for 76 transitions (∼28%) in Sc XIX, and in some instances by up to a factor of five, see, for example, 2–4, 3–4, and 7–9. Many of these are resonance transitions, such as 1–5/6/7/8/10/11, and our results from darc are invariably higher due to the inclusion of resonances. However, at Te = 107.5 K, only 9 transitions differ by over 20%, with a maximum discrepancy of 30%. For the 21–24 (5f 2 Fo5/2 –5g 2 G9/2 ) transition, values of Υ from fac are higher by a factor of 5 because of a sudden rise in the corresponding values of Ω , as shown for the 10–13 transition in Fe XXIV in Fig. 5. Overall we may state that the contribution of resonances is more dominant and appreciable at lower temperatures. Similar conclusions apply for transitions in other Li-like ions. The only Li-like ion considered here for which results for Υ are available in the literature is Fe XXIV. Whiteford et al. [25] have reported values of Υ for all transitions among the lowest 24 levels
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over a wide range of electron temperature. They have adopted the standard R-matrix code of Berrington et al. [16] and have included one-body relativistic operators in the calculations, which may be nearly sufficient for a moderately heavy ion such as Fe XXIV. Furthermore, they included a comparable large range of partial waves with angular momentum J ≤ 58, but resolved resonances in the threshold region in a comparatively coarser energy mesh of ∼0.005 Ryd. Therefore, some differences are expected between their results for Υ and our calculations from the fully relativistic darc. A comparison between the two independent sets of Υ shows that, at the lowest common temperature of 105.6 K, for about 40% transitions the differences are over 20%. For most of these transitions the differences are within a factor of two, but in some instances are over an order of magnitude, such as 7–8, 12–13, 14–15, 19–20, 21–22, and 23–24. All of these transitions are forbidden, there is no (major) discrepancy between the Ω values from darc and fac, and there is no large variation of their Ω values with increasing energy (i.e., ΩB is quite stable). Therefore, the differences in the values of Υ should not be due to the corresponding differences in the values of Ω , but because of the contribution of resonances. However, all of these transitions belong to the same n and therefore their ∆Eij are very small, but resonances in the collision strengths are neither too dense nor too high in magnitude. In fact, 7–8 (3d 2 D3/2 –3d 2 D5/2 ) is the only transition for which both the thresholds range and resonances are appreciable, as shown in Fig. 9. In Fig. 10 we compare values of Υ from the BPRM calculations of Whiteford et al. [25] with our own from darc for three transitions, namely 7–8 (3d 2 D3/2 –3d 2 D5/2 ), 12–13 (4d 2 D3/2 –4d 2 D5/2 ), and 14–15 (4f 2 Fo5/2 –4f 2 Fo7/2 ). At the lowest common temperature of
105.6 K, values of Υ from the BPRM calculations are higher, by up to a factor of ∼70, for these three and some other transitions, as noted above. As the electron temperature increases the discrepancy between the two calculations decreases significantly, and towards the higher end of the temperature range the two independent calculations become comparable. In fact, for only 5 transitions (7–8, 12–13, 14–15, 21–22, and 23–24) do the values of Υ differ at the highest common temperature of 107.46 K by over 20%, and by up to a factor of 5. The resonances for the 7–8 transition are neither too high in magnitude nor dense (see Fig. 9), and hence cannot make a large contribution to the determination of Υ as shown by our calculations from darc. Clearly, the BPRM calculations of Υ have overestimated the contribution of resonances for these seven transitions. The main reason for such a large discrepancy between the two R-matrix calculations for a few transitions, particularly those between the degenerate levels of a state, is the limitation of the BPRM method, as recently discussed and demonstrated by Bautista et al. [26]. The jj coupling method adopted in darc includes fine-structure in the definition of channel coupling and hence gives a better representation of resonances, particularly for transitions within the degenerate levels of a state. These near-threshold resonances affect the subsequent results for Υ , especially at lower temperatures as shown in Fig. 10. We discuss this further below. Another source of higher values of Υ from the BPRM calculations of Whiteford et al. [25], for some transitions and at lower temperatures, could be their inclusion of higher levels of the 1snℓn′ ℓ′ configurations. These additional levels in the 486–580 Ryd energy range, well above the highest threshold of our calculations (i.e., ∼127 Ryd) may give rise to some resonances that may affect the values of Υ . However, although this may be true for the calculations of Υ at very high temperatures, such as Te = 107.4 K (equivalent to ∼163 Ryd), resonances will not contribute to Υ values at lower temperatures, such as Te = 105.6 K (equivalent to ∼2.52 Ryd) unless there are very high spurious resonances. Therefore, we are confident in our results listed in Tables 25–32, which are assessed to be accurate to better than ∼20% for a majority of transitions and
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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over a wide range of temperatures. However, the contribution of higher neglected resonances, from the 1s2 nℓ (n ≥ 6) and 1snℓn′ ℓ′ configurations, may affect these results towards the higher end of the temperature range, as discussed above, and particularly for transitions involving the levels of the n = 5 configurations. Finally, we note that differences in values of Υ between our calculations from darc and those of Whiteford et al. [25] for transitions in Fe XXIV are similar to those observed earlier for transitions in Ar XVI [10]. However, differences in the case of Fe XXIV are comparatively larger in magnitude apart from affecting a larger number of transitions. This may be due to two reasons. First, relativistic effects are comparatively more important for Fe XXIV than for Ar XVI. Second, Whiteford et al. adopted a coarser mesh of 0.005 Ryd to resolve resonances for transitions in Fe XXIV in comparison to 0.002 Ryd for Ar XVI, whereas our energy mesh for these two (and other) ions is better than 0.002 Ryd.
but there is no evidence of a similar (significant) effect for the transitions considered in this paper. We believe the present set of complete results for radiative and excitation rates for eight Li-like ions are probably the best currently available and will be highly useful for the modelling of a variety of plasmas.
7. Conclusions
References
In this paper we have presented results for energy levels and radiative rates for four types of transitions (E1, E2, M1, and M2) among the lowest 24 levels belonging to the n ≤ 5 configurations of Li-like ions with 21 ≤ Z ≤ 28. Additionally, lifetimes of all the levels have been reported, although measurements or other theoretical results are not available for comparison for most of the ions/levels. However, based on a variety of comparisons among various calculations from grasp and fac, our energy levels are assessed to be accurate to better than 1%, and the results for radiative rates, oscillator strengths, line strengths, and lifetimes are assessed to be accurate to better than 20% for a majority of strong transitions (levels). Similarly, the accuracy of our results for collision strengths and effective collision strengths is estimated to be better than 20% for a majority of the transitions. This accuracy estimate is based on the comparison made between two independent calculations performed with darc and fac, as well as with other results available in the literature, particularly for Fe XXIV. Additionally, we have considered a large range of partial waves to achieve convergence of Ω at all energies, included a wide energy range to accurately calculate the values of Υ up to Te = 107.8 K, and resolved resonances on a fine energy mesh to account for their contributions. Hence we see no obvious deficiency in our calculated results. However, the present results for effective collision strengths for transitions involving the levels of the n = 5 configurations may (perhaps) be improved by the inclusion of the levels of the n = 6 configurations, as has been noted for the A-values. Finally, we would like to note that inclusion of radiation and Auger damping may reduce the contribution of resonances, particularly at lower temperatures, for some of the transitions. However, it is certainly true for transitions involving the inner-shell, as demonstrated by Whiteford et al. [25],
[1] K.P. Dere, E. Landi, P.R. Young, G. Del Zanna, Astrophys. J. Suppl. Ser. 134 (2001) 331. [2] G.A. Doschek, U. Feldman, J. Phys. B 43 (2010) 232001. [3] F.B. Rosmej, D. Reiter, V.S Lisitsa, M. Bitter, O. Herzog, G. Bertschinger, H.J. Kunze, Plasma Phys. Contr. Fusion 41 (1999) 191. [4] S. Fujioka, H. Takabe, Y. Yamamoto, D. Salzman, F. Wang, H. Nishimura, Y. Li, Q. Dong, S. Wang, Y. Zhang, Y.J. Rhee, Y.W. Lee, J.M. Han, M. Tanabe, T. Fujiwara, Y. Nakabayashi, G. Zhao, J. Zhang, K. Mima, Nature Phys. 5 (2009) 821. [5] J.R. Lemen, J. Sylwester, R.D. Bentley, Advances Space Res. 6 (1986) 245. [6] N.J. Peacock, R. Barnsley, I.H. Coffey, R. Giannella, N.C. Hawkes, K.D. Lawson, I.M. Melnick, M.G. O’Mullane, M.A. Singleton, A. Patel, Fusion Eng. Design 3435 (1997) 171. [7] K.M. Aggarwal, F.P. Keenan, Phys. Scr. 70 (2004) 222. [8] K.M. Aggarwal, F.P. Keenan, R.F. Heeter, Phys. Scr. 81 (2010) 015303. [9] K.M. Aggarwal, F.P. Keenan, Phys. Scr. 82 (2010) 065302. [10] K.M. Aggarwal, F.P. Keenan, At. Data Nucl. Data Tables xx, 2012, in press, (http://dx.doi.org/10.1016/j.adt.2012.03.001). [11] S.N. Nahar, Astron. Astrophys. 389 (2002) 716. [12] H.L. Zhang, D.H. Sampson, C.J. Fontes, At. Data Nucl. Data Tables 44 (1990) 31. [13] I.P. Grant, B.J. McKenzie, P.H. Norrington, D.F. Mayers, N.C. Pyper, Comput. Phys. Commun. 21 (1980) 207. [14] M.F. Gu, Can. J. Phys. 86 (2008) 675. [15] K.M. Aggarwal, K. Hamada, A. Igarashi, V. Jonauskas, F.P. Keenan, S. Nakazaki, Astron. Astrophys. 484 (2008) 879. [16] K.A. Berrington, W.B. Eissner, P.H. Norrington, Comput. Phys. Commun. 92 (1995) 290. [17] A. Hibbert, J. Phys. B 36 (2003) 4703. [18] K.M. Aggarwal, F.P. Keenan, R. Kisielius, Astron. Astrophys. 420 (2004) 783. [19] K.M. Aggarwal, V. Tayal, G.P. Gupta, F.P. Keenan, At. Data Nucl. Data Tables 93 (2007) 615. [20] J.P. Grandin, M. Huet, X. Husson, D. Lecler, D. Touvet, J.P. Buchet, M.C. BuchetPoulizac, A. Denis, J. Desesquelles, M. Druetta, J. Physique 45 (1984) 1423. [21] K.T. Cheng, Y.K. Kim, J.P. Desclaux, At. Data Nucl. Data Tables 24 (1979) 95. [22] P. Bryans, E. Landi, D.W. Savin, Astrophys. J. 691 (2009) 1540. [23] A. Burgess, V.B. Sheorey, J. Phys. B 7 (1974) 2403. [24] K.M. Aggarwal, F.P. Keenan, Eur. Phys. J. D 46 (2008) 205. [25] A.D. Whiteford, N.R. Badnell, C.P. Ballance, S.D. Loch, M.G. O’Mullane, H.P. Summers, J. Phys. B 35 (2002) 3729. [26] M.A. Bautista, C.P. Ballance, P. Quinet, Astrophys. J. Lett. 718 (2010) L189.
Acknowledgment FPK is grateful to AWE Aldermaston for the award of a William Penney Fellowship. Appendix. Supplementary data Supplementary material related to this article can be found online at http://dx.doi.org/10.1016/j.adt.2011.05.002.
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Explanation of Tables
Table 1
Table 2
Table 3 Table 4 Table 5 Table 6 Table 7 Table 8 Table 9
Table 10
Table 11
Table 12
Table 13
Table 14
Table 15
Energy levels of Sc XIX, their threshold energies (in Ryd), and lifetimes (in s). Index Level Index Configuration The configuration to which the level belongs NIST Experimentally compiled energies from NIST (www.nist.gov/pml/data/asd.cfm) GRASP1 Present energies from grasp without Breit and QED corrections GRASP2 Present energies from grasp with Breit and QED corrections FAC Present energies from fac τ (s) Lifetime of the level in s Energy levels of Ti XX, their threshold energies (in Ryd), and lifetimes (in s). Index Level Index Configuration The configuration to which the level belongs NIST Experimentally compiled energies from NIST (www.nist.gov/pml/data/asd.cfm) GRASP1 Present energies from grasp without Breit and QED corrections GRASP2 Present energies from grasp with Breit and QED corrections FAC Present energies from fac BPRM Energies of Nahar [11] from the BPRM code [16] τ (s) Lifetime of the level in s Energy levels of V XXI, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Cr XXII, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 2. Energy levels of Mn XXIII, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Fe XXIV, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Co XXV, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 1. Energy levels of Ni XXVI, their threshold energies (in Ryd), and lifetimes (in s). Same as for Table 2. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Sc XIX. i and j The lower (i) and upper (j) levels of a transition as defined in Table 1.
λij
Transition wavelength (in Å)
AE1 ji
Radiative transition probability (in s−1 ) for the E1 transitions
fijE1 E1
Absorption oscillator strength (dimensionless) for the E1 transitions
S
Line strength in atomic unit (a.u.), 1 a.u. = 6.460 × 10−36 cm2 esu2 for the E1 transitions
AE2 ji AjiM1 AjiM2
Radiative transition probability (in s−1 ) for the E2 transitions Radiative transition probability (in s−1 ) for the M1 transitions
Radiative transition probability (in s−1 ) for the M2 transitions a±b ≡ a × 10±b Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ti XX. Same as for Table 9 for transitions as defined in Table 2. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in V XXI. Same as for Table 9 for transitions as defined in Table 3. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Cr XXII. Same as for Table 9 for transitions as defined in Table 4. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Mn XXIII. Same as for Table 9 for transitions as defined in Table 5. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Fe XXIV. Same as for Table 9 for transitions as defined in Table 6. Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Co XXV. Same as for Table 9 for transitions as defined in Table 7.
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
Table 16
Table 17
Table 18 Table 19 Table 20 Table 21 Table 22 Table 23 Table 24 Table 25
Table 26 Table 27 Table 28 Table 29 Table 30 Table 31 Table 32
)
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Transition wavelengths (λij in Å), radiative rates (Aji in s ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for electric quadrupole (E2), magnetic dipole (M1), and magnetic quadrupole (M2) transitions in Ni XXVI. Same as for Table 9 for transitions as defined in Table 8. Collision strengths for resonance transitions in Sc XIX. Transition The lower (i) and upper (j) levels are defined in Table 1. Energy Energy (in Ryd) at which collision strengths obtained from the darc code are listed. FAC Collision strengths obtained from fac at a single excited energy of ∼500 Ryd. a±b ≡ a × 10±b Collision strengths for resonance transitions in Ti XX. Same as for Table 17 for levels defined in Table 2. Results from the FAC are at ∼560 Ryd. Collision strengths for resonance transitions in V XXI. Same as for Table 17 for levels defined in Table 3. Results from the FAC are at ∼600 Ryd. Collision strengths for resonance transitions in Cr XXII. Same as for Table 17 for levels defined in Table 4. Results from the FAC are at ∼660 Ryd. Collision strengths for resonance transitions in Mn XXIII. Same as for Table 17 for levels defined in Table 5. Results from the FAC are at ∼750 Ryd. Collision strengths for resonance transitions in Fe XXIV. Same as for Table 17 for levels defined in Table 6. Results from the FAC are at ∼820 Ryd. Collision strengths for resonance transitions in Co XXV. Same as for Table 17 for levels defined in Table 7. Results from the FAC are at ∼900 Ryd. Collision strengths for resonance transitions in Ni XXVI. Same as for Table 17 for levels defined in Table 8. Results from the FAC are at ∼980 Ryd. Effective collision strengths for transitions in Sc XIX. Transition The lower (i) and upper (j) levels are defined in Table 1. Temperature Temperatures (in log K) at which effective collision strengths from darc are listed. FAC Effective collision strengths from fac at the lowest (LHS) and the highest (RHS) temperature. a±b ≡ a × 10±b Effective collision strengths for transitions in Ti XX. Same as for Table 25 for levels defined in Table 2. Effective collision strengths for transitions in V XXI. Same as for Table 25 for levels defined in Table 3. Effective collision strengths for transitions in Cr XXII. Same as for Table 25 for levels defined in Table 4. Effective collision strengths for transitions in Mn XXIII. Same as for Table 25 for levels defined in Table 5. Effective collision strengths for transitions in Fe XXIV. Same as for Table 25 for levels defined in Table 6. Effective collision strengths for transitions in Co XXV. Same as for Table 25 for levels defined in Table 7. Effective collision strengths for transitions in Ni XXVI. Same as for Table 25 for levels defined in Table 8. −1
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Table 1 Experimental and theoretical energy levels (in Ryd) for Sc XIX and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.000 2.795 3.257 53.360 54.050 54.180 54.480 54.510
0.00000 2.80532 3.28673 53.28735 54.06380 54.20600 54.50117 54.54433 71.58356 71.90314 71.96299 72.08550 72.10374 72.11010 72.11915 79.97088 80.13250 80.16309 80.22533 80.23467 80.23825 80.24289 80.24296 80.24574
0.00000 2.80715 3.26772 53.25951 54.03701 54.17315 54.46362 54.50651 71.54981 71.86980 71.92713 72.04777 72.06586 72.07214 72.08119 79.93505 80.09689 80.12620 80.18750 80.19676 80.20030 80.20493 80.20500 80.20778
0.00000 2.81952 3.27812 53.26471 54.04351 54.17891 54.46530 54.50798 71.54525 71.86118 71.91811 72.05228 72.07013 72.06516 72.07420 79.92707 80.08757 80.11649 80.18900 80.19736 80.19810 80.19767 80.19305 80.20014
71.900 72.070 72.100 72.100 72.100 80.100 80.100 80.200 80.200
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 7.098−10 4.457−10 8.863−13 3.442−13 3.517−13 1.155−13 1.164−13 1.310−12 5.822−13 5.928−13 2.680−13 2.702−13 5.538−13 5.551−13 2.068−12 9.866−13 1.003−12 5.142−13 5.189−13 1.070−12 1.073−12 1.799−12 1.801−12
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Table 2 Experimental and theoretical energy levels (in Ryd) for Ti XX and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 2.94814 3.51495 58.92244 59.73921 59.90706 60.21762 60.27047 79.16195 79.50504 70.57585 79.70671 79.72894 79.73587 79.74498 88.44913 88.62437 88.66054 88.72752 88.73891
0.00000 2.95843 3.54785 58.94397 59.76326 59.93739 60.24985 60.30285 79.19708 79.53436 79.60766 79.73733 79.75972 79.76650 79.77762 88.48424 88.65482 88.69228 88.75816 88.76962 88.77345 88.77914 88.77921 88.78262
0.00000 2.96034 3.52549 58.91143 59.73184 59.89893 60.20592 60.25860 79.15763 79.49532 79.56569 79.69318 79.71540 79.72211 79.73322 88.44234 88.61314 88.64912 88.71390 88.72527 88.72904 88.73473 88.73480 88.73821
0.00000 2.97295 3.53597 58.91679 59.73847 59.90476 60.20768 60.26015 79.15313 79.48676 79.55669 79.69778 79.71973 79.71511 79.72622 88.43439 88.60387 88.63941 88.71542 88.72663 88.72179 88.72747 88.72717 88.73058
0.00000 2.90900 3.55600 58.96600 59.75200 59.94280 60.24240 60.30120 78.84310 79.47540 79.55750 79.75280 79.77760 79.78310 79.79539 88.33580 88.63940 88.68069 88.76910 88.78180 88.78500 88.79120 88.79090 88.79460
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 6.708−10 3.930−10 7.279−13 2.796−13 2.863−13 9.412−14 9.490−14 1.074−12 4.732−13 4.827−13 2.183−13 2.203−13 4.509−13 4.520−13 1.695−12 8.021−13 8.169−13 4.190−13 4.232−13 8.712−13 8.736−13 1.465−12 1.467−12
16
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 3 Experimental and theoretical energy levels (in Ryd) for V XXI and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.10227 3.79028 64.86700 65.72669 65.93063 66.25768 66.32192 87.16324 87.52438 87.61040 87.74818 87.77525
0.00000 3.11270 3.82747 64.89302 65.75546 65.96665 66.29641 66.36085 87.20456 87.55965 87.64854 87.78538 87.81261 87.81982 87.83333 97.43819 97.61780 97.66324 97.73275 97.74670 97.75075 97.75767 97.75774 97.76189
0.00000 3.11464 3.80137 64.85526 65.71887 65.92195 66.24540 66.30946 87.15875 87.51426 87.59979 87.73412 87.76114 87.76825 87.78176 97.38955 97.56937 97.61310 97.68135 97.69518 97.69919 97.70611 97.70618 97.71033
0.00000 3.12752 3.81195 64.86079 65.72564 65.92786 66.24724 66.31107 87.15432 87.50578 87.59082 87.73879 87.76553 87.76127 87.77477 97.38163 97.56014 97.60340 97.68291 97.69656 97.69194 97.69885 97.69854 97.70268
97.39659 97.58103 97.62495
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 6.354−10 3.454−10 6.030−13 2.294−13 2.354−13 7.743−14 7.814−14 8.889−13 3.885−13 3.970−13 1.796−13 1.814−13 3.708−13 3.718−13 1.402−12 6.588−13 6.720−13 3.447−13 3.485−13 7.164−13 7.186−13 1.205−12 1.207−12
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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17
Table 4 Experimental and theoretical energy levels (in Ryd) for Cr XXII and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 3.25756 4.08607 71.10243 72.00541 72.25090 72.59445 72.67172 95.55729 95.93956 95.04008 96.18478 96.21741
0.00000 3.26819 4.12747 71.13598 72.04188 72.29581 72.64289 72.72052 95.60789 95.98091 96.08781 96.23182 96.26462 96.27225 96.28853 106.83485 107.02353 107.07817 107.15131 107.16812 107.17242 107.18076 107.18083 107.18583
0.00000 3.27012 4.09721 71.09246 71.99957 72.24420 72.58404 72.66124 95.55507 95.92852 96.03155 96.17268 96.20525 96.21277 96.22904 106.77873 106.96764 107.02031 107.09203 107.10870 107.11293 107.12126 107.12135 107.12634
0.00000 3.28326 4.10787 71.09813 72.00645 72.25014 72.58591 72.66286 95.55066 95.92004 96.02255 96.17736 96.20962 96.20573 96.22200 106.77079 106.95840 107.01057 107.09356 107.11003 107.10562 107.11395 107.11364 107.11864
0.00000 3.20500 4.14301 71.16300 72.02690 72.30380 72.63580 72.72100 95.07121 95.90580 96.02520 96.25730 96.29340 96.29900 96.31680 106.60690 107.01100 107.07090 107.17000 107.18851 107.19170 107.20090 107.20040 107.20580
106.78355 106.97719 107.03014 107.10413 107.12090
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 6.030−10 3.026−10 5.034−13 1.899−13 1.954−13 6.428−14 6.493−14 7.416−13 3.219−13 3.296−13 1.491−13 1.508−13 3.077−13 3.087−13 1.169−12 5.459−13 5.579−13 2.862−13 2.896−13 5.944−13 5.964−13 1.000−12 1.002−12
18
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 5 Experimental and theoretical energy levels (in Ryd) for Mn XXIII and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.41410 4.40374 77.63449 78.58111 78.87426 79.23412 79.32662 104.35010 104.74778 104.87135 105.02289 105.06198
0.00000 3.42497 4.44982 77.67440 78.62411 78.92703 79.29143 79.38419 104.40911 104.80020 104.92772 105.07890 105.11810 105.12616 105.14561 116.67639 116.87422 116.93939 117.01619 117.03627 117.04080 117.05077 117.05085 117.05682
0.00000 3.42684 4.41495 77.62454 78.57549 78.86780 79.22395 79.31622 104.34856 104.74007 104.86319 105.01109 105.05003 105.05795 105.07740 116.61206 116.81010 116.87304 116.94820 116.96812 116.97259 116.98255 116.98263 116.98860
0.00000 3.44029 4.42575 77.63040 78.58252 78.87383 79.22588 79.31790 104.34423 104.73168 104.85423 105.01585 105.05443 105.05092 105.07035 116.60416 116.80093 116.86331 116.94976 116.96948 116.96529 116.97523 116.97492 116.98089
116.61630 116.81924 116.88257 116.96003 116.98008
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.732−10 2.643−10 4.234−13 1.586−13 1.635−13 5.380−14 5.439−14 6.232−13 2.689−13 2.759−13 1.248−13 1.263−13 2.574−13 2.583−13 9.816−13 4.562−13 4.671−13 2.396−13 2.427−13 4.973−13 4.991−13 8.371−13 8.383−13
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 6 Experimental and theoretical energy levels (in Ryd) for Fe XXIV and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.57201 4.74549 84.49724 85.46045 85.81493 86.19675 86.32068 113.58397 113.98948 114.13529 114.26560 114.32027 114.34214 114.37860 126.89804 127.06161 127.13633 127.21744 127.26118
0.00000 3.58311 4.79661 84.50994 85.50381 85.86255 86.24429 86.35430 113.61034 114.01965 114.17065 114.32903 114.37552 114.38400 114.40707 126.96514 127.17218 127.24937 127.32980 127.35362 127.35839 127.37021 127.37029 127.37737
0.00000 3.58487 4.75665 84.45313 85.44825 85.79495 86.16734 86.27679 113.54131 113.95103 114.09705 114.25170 114.29788 114.30622 114.32928 126.89179 127.09904 127.17369 127.25228 127.27592 127.28061 127.29242 127.29250 127.29958
0.00000 3.59862 4.76759 84.45915 85.45541 85.80104 86.16928 86.27847 113.53700 113.94265 114.08807 114.25646 114.30227 114.29912 114.32217 126.88386 127.08985 127.16391 127.25381 127.27722 127.27324 127.28504 127.28473 127.29179
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.458−10 2.301−10 3.585−13 1.334−13 1.380−13 4.537−14 4.591−14 5.273−13 2.264−13 2.328−13 1.053−13 1.067−13 2.170−13 2.179−13 8.301−13 3.841−13 3.940−13 2.020−13 2.049−13 4.192−13 4.209−13 7.058−13 7.070−13
20
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 7 Experimental and theoretical energy levels (in Ryd) for Co XXV and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
0.00000 3.73114 5.11313 91.59291 92.62747 93.03681 93.42911 93.55833 123.13879 123.57319 123.74578 123.91100 123.96558
0.00000 3.74268 5.17001 91.64433 92.68274 93.10475 93.50383 93.63341 123.21382 123.64148 123.81913 123.98470 124.03945 124.04836 124.07552 137.70354 137.91985 138.01065 138.09474 138.12279 138.12781 138.14171 138.14180 138.15015
0.00000 3.74427 5.12446 91.57992 92.61957 93.02801 93.41653 93.54547 123.13553 123.56358 123.73560 123.89697 123.95138 123.96011 123.98727 137.62033 137.83684 137.92479 138.00679 138.03464 138.03955 138.05347 138.05356 138.06189
0.00000 3.75836 5.13557 91.58613 92.62685 93.03418 93.41850 93.54715 123.13127 123.55524 123.72662 123.90176 123.95576 123.95298 123.98013 137.61240 137.82768 137.91498 138.00832 138.03590 138.03215 138.04604 138.04572 138.05406
137.62638 137.84810 137.93631 138.02078 138.04876
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac.
τ (s) ........ 5.205−10 1.997−10 3.053−13 1.130−13 1.172−13 3.852−14 3.902−14 4.489−13 1.919−13 1.977−13 8.939−14 9.066−14 1.843−13 1.850−13 7.064−13 3.256−13 3.347−13 1.715−13 1.742−13 3.559−13 3.574−13 5.993−13 6.004−13
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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21
Table 8 Experimental and theoretical energy levels (in Ryd) for Ni XXVI and their lifetimes (τ , s). (a ± b ≡ a × 10±b ). Index
Configuration
Level
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
1s2 2s 1s2 2p 1s2 2p 1s2 3s 1s2 3p 1s2 3p 1s2 3d 1s2 3d 1s2 4s 1s2 4p 1s2 4p 1s2 4d 1s2 4d 1s2 4f 1s2 4f 1s2 5s 1s2 5p 1s2 5p 1s2 5d 1s2 5d 1s2 5f 1s2 5f 1s2 5g 1s2 5g
2
S1/2 2 o P1/2 2 o P3/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 S1/2 2 o P1/2 2 o P3/2 2 D3/2 2 D5/2 2 o F5/2 2 o F7/2 2 G7/2 2 G9/2
NIST
GRASP1
GRASP2
FAC
BPRM
0.00000 3.89178 5.50927 99.02019 100.09931 100.57828 100.98671 101.13798 133.13657 133.58956 133.79150 133.96346 134.02734
0.00000 3.90376 5.57232 99.07935 100.16271 100.65613 101.07256 101.22420 133.22189 133.66806 133.87576 134.04854 134.11261 134.12195 134.15372 148.89410 149.11978 149.22594 149.31369 149.34651 149.35176 149.36804 149.36813 149.37788
0.00000 3.90511 5.52065 99.00668 100.09123 100.56940 100.97398 101.12491 133.13351 133.58003 133.78142 133.94948 134.01317 134.02229 134.05408 148.80017 149.02602 149.12897 149.21437 149.24698 149.25212 149.26840 149.26849 149.27824
0.00000 3.91952 5.53194 99.01307 100.09864 100.57562 100.97593 101.12655 133.12926 133.57172 133.77240 133.95422 134.01749 134.01509 134.04684 148.79221 149.01685 149.11909 149.21584 149.24818 149.24463 149.26088 149.26057 149.27032
0.00000 3.88501 5.70100 99.15861 100.21990 100.75800 101.14600 101.31030 132.58530 133.58981 133.82431 134.16301 134.23280 134.23880 134.27321 148.27220 149.16661 149.28311 149.41470 149.45050 149.45401 149.47160 149.47070 149.48120
148.80599 149.03718 149.14052 149.22836 149.26108
NIST: www.nist.gov/pml/data/asd.cfm. GRASP1: Present results from grasp without the Breit and QED effects. GRASP2: Present results from grasp with the Breit and QED effects. FAC: Present results from fac. BPRM: Nahar [11].
τ (s) ........ 4.970−10 1.727−10 2.615−13 9.637−14 1.002−13 3.291−14 3.338−14 3.843−13 1.637−13 1.691−13 7.638−14 7.755−14 1.574−13 1.581−13 6.046−13 2.778−13 2.862−13 1.466−13 1.490−13 3.040−13 3.054−13 5.122−13 5.132−13
22
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 9 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Sc XIX. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
3.246+02 2.789+02 1.711+01 1.686+01 1.682+01 1.673+01 1.672+01 1.274+01 1.268+01 1.267+01 1.265+01 1.265+01 1.264+01 1.140+01 1.138+01 1.137+01 1.136+01 1.136+01 1.136+01 1.979+03 1.806+01 1.779+01 1.774+01 1.764+01 1.763+01 1.326+01 1.319+01 1.318+01 1.316+01 1.316+01 1.316+01 1.181+01 1.179+01 1.179+01 1.178+01 1.177+01 1.177+01 1.823+01 1.795+01 1.790+01 1.780+01 1.778+01 1.335+01 1.328+01 1.327+01 1.325+01 1.325+01 1.324+01 1.324+01 1.189+01 1.186+01 1.186+01 1.185+01 1.185+01 1.185+01 1.184+01 1.184+01 1.172+03 9.974+02 7.568+02 7.308+02 4.982+01 4.897+01 4.881+01 4.850+01 4.846+01 4.844+01 3.416+01 3.396+01 3.392+01 3.384+01 3.383+01 3.383+01
1.409+09 2.244+09 0.000+00 2.904+12 2.842+12 0.000+00 0.000+00 0.000+00 1.285+12 1.266+12 0.000+00 0.000+00 0.000+00 0.000+00 6.647+11 6.563+11 0.000+00 0.000+00 0.000+00 0.000+00 3.680+11 0.000+00 0.000+00 7.221+12 0.000+00 1.470+11 0.000+00 0.000+00 2.356+12 0.000+00 0.000+00 7.359+10 0.000+00 0.000+00 1.087+12 0.000+00 0.000+00 7.602+11 0.000+00 0.000+00 1.431+12 8.588+12 3.021+11 0.000+00 0.000+00 4.632+11 2.789+12 0.000+00 0.000+00 1.501+11 0.000+00 0.000+00 2.129+11 1.284+12 0.000+00 0.000+00 0.000+00 1.823+08 2.976+08 0.000+00 0.000+00 0.000+00 3.776+11 3.681+11 0.000+00 0.000+00 0.000+00 0.000+00 2.081+11 2.041+11 0.000+00 0.000+00 0.000+00
2.226−02 5.232−02 0.000+00 1.238−01 2.411−01 0.000+00 0.000+00 0.000+00 3.098−02 6.094−02 0.000+00 0.000+00 0.000+00 0.000+00 1.290−02 2.545−02 0.000+00 0.000+00 0.000+00 0.000+00 1.800−02 0.000+00 0.000+00 6.738−01 0.000+00 3.872−03 0.000+00 0.000+00 1.223−01 0.000+00 0.000+00 1.540−03 0.000+00 0.000+00 4.520−02 0.000+00 0.000+00 1.894−02 0.000+00 0.000+00 6.796−02 6.108−01 4.033−03 0.000+00 0.000+00 1.219−02 1.101−01 0.000+00 0.000+00 1.590−03 0.000+00 0.000+00 4.480−03 4.051−02 0.000+00 0.000+00 0.000+00 3.755−02 8.877−02 0.000+00 0.000+00 0.000+00 1.357−01 2.630−01 0.000+00 0.000+00 0.000+00 0.000+00 3.596−02 7.039−02 0.000+00 0.000+00 0.000+00
4.757−02 9.606−02 0.000+00 1.375−02 2.670−02 0.000+00 0.000+00 0.000+00 2.586−03 5.083−03 0.000+00 0.000+00 0.000+00 0.000+00 9.663−04 1.906−03 0.000+00 0.000+00 0.000+00 0.000+00 2.141−03 0.000+00 0.000+00 7.826−02 0.000+00 3.379−04 0.000+00 0.000+00 1.060−02 0.000+00 0.000+00 1.198−04 0.000+00 0.000+00 3.504−03 0.000+00 0.000+00 4.545−03 0.000+00 0.000+00 1.593−02 1.431−01 7.088−04 0.000+00 0.000+00 2.127−03 1.919−02 0.000+00 0.000+00 2.488−04 0.000+00 0.000+00 6.990−04 6.319−03 0.000+00 0.000+00 0.000+00 2.898−01 5.829−01 0.000+00 0.000+00 0.000+00 4.377−02 8.454−02 0.000+00 0.000+00 0.000+00 0.000+00 8.040−03 1.572−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.006+09 3.014+09 0.000+00 0.000+00 0.000+00 4.168+08 4.227+08 0.000+00 0.000+00 0.000+00 0.000+00 1.090+08 1.116+08 0.000+00 4.734−02 0.000+00 0.000+00 5.849+08 0.000+00 0.000+00 0.000+00 0.000+00 2.535+08 0.000+00 0.000+00 2.261+09 0.000+00 0.000+00 1.354+08 0.000+00 0.000+00 1.515+09 0.000+00 1.163+09 5.790+08 0.000+00 0.000+00 0.000+00 4.949+08 2.485+08 0.000+00 0.000+00 6.454+08 2.897+09 0.000+00 2.566+08 1.293+08 0.000+00 0.000+00 4.328+08 1.944+09 0.000+00 0.000+00 0.000+00 1.373+02 1.643+02 0.000+00 0.000+00 0.000+00 2.048+08 2.051+08 0.000+00 0.000+00 0.000+00 0.000+00 6.974+07 7.026+07 0.000+00
0.000+00 0.000+00 1.511+04 0.000+00 0.000+00 8.459+02 0.000+00 1.273+04 0.000+00 0.000+00 4.970+02 0.000+00 0.000+00 8.339+03 0.000+00 0.000+00 2.794+02 0.000+00 0.000+00 1.158+03 0.000+00 3.429+03 2.373+04 0.000+00 0.000+00 0.000+00 2.689+03 1.213+04 0.000+00 0.000+00 0.000+00 0.000+00 1.736+03 6.692+03 0.000+00 0.000+00 0.000+00 0.000+00 8.956+04 2.444+04 0.000+00 0.000+00 0.000+00 5.221+04 1.918+04 0.000+00 0.000+00 2.757+02 0.000+00 0.000+00 3.012+04 1.222+04 0.000+00 0.000+00 2.424+02 0.000+00 0.000+00 0.000+00 0.000+00 7.621−04 0.000+00 1.514+02 0.000+00 0.000+00 3.541+00 0.000+00 0.000+00 1.887+02 0.000+00 0.000+00 4.714+00 0.000+00 0.000+00
0.000+00 3.181+00 0.000+00 0.000+00 1.109+06 0.000+00 0.000+00 0.000+00 0.000+00 8.704+05 0.000+00 0.000+00 2.199−01 0.000+00 0.000+00 5.597+05 0.000+00 0.000+00 1.960−01 0.000+00 0.000+00 0.000+00 0.000+00 1.020+05 7.287+05 0.000+00 0.000+00 0.000+00 5.968+04 4.273+05 0.000+00 0.000+00 0.000+00 0.000+00 3.437+04 2.463+05 0.000+00 2.534+05 0.000+00 0.000+00 0.000+00 3.880+06 1.879+05 0.000+00 0.000+00 0.000+00 2.268+06 0.000+00 0.000+00 1.177+05 0.000+00 0.000+00 0.000+00 1.305+06 0.000+00 0.000+00 2.772−02 0.000+00 3.301−02 0.000+00 0.000+00 0.000+00 0.000+00 1.706+04 0.000+00 0.000+00 1.206−03 0.000+00 0.000+00 1.958+04 0.000+00 0.000+00 3.393−04
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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23
Table 9 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
6.693+03 2.136+03 1.941+03 5.203+01 5.110+01 5.094+01 5.060+01 5.054+01 5.053+01 3.519+01 3.497+01 3.493+01 3.485+01 3.483+01 3.483+01 3.137+03 2.734+03 5.244+01 5.149+01 5.133+01 5.098+01 5.093+01 5.091+01 5.089+01 3.537+01 3.515+01 3.511+01 3.503+01 3.502+01 3.501+01 3.501+01 3.501+01 2.125+04 5.333+01 5.235+01 5.218+01 5.182+01 5.177+01 5.175+01 5.172+01 3.578+01 3.555+01 3.551+01 3.542+01 3.541+01 3.541+01 3.540+01 3.540+01 5.347+01 5.248+01 5.231+01 5.195+01 5.190+01 5.188+01 5.185+01 3.584+01 3.561+01 3.557+01 3.548+01 3.547+01 3.547+01 3.546+01 3.546+01 3.546+01 2.848+03 2.415+03 1.830+03 1.766+03 1.745+03 1.087+02 1.066+02 1.062+02 1.055+02 1.054+02 1.053+02
0.000+00 1.946+07 0.000+00 1.027+11 0.000+00 0.000+00 7.595+11 0.000+00 0.000+00 4.976+10 0.000+00 0.000+00 3.741+11 0.000+00 0.000+00 1.226+06 1.116+07 2.118+11 0.000+00 0.000+00 1.524+11 9.113+11 0.000+00 0.000+00 1.020+11 0.000+00 0.000+00 7.451+10 4.467+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.404+10 5.126+09 0.000+00 0.000+00 1.683+12 0.000+00 0.000+00 2.318+10 2.201+09 0.000+00 0.000+00 5.558+11 0.000+00 0.000+00 0.000+00 0.000+00 4.683+10 0.000+00 0.000+00 1.198+11 1.798+12 0.000+00 0.000+00 2.009+10 0.000+00 0.000+00 3.944+10 5.932+11 0.000+00 0.000+00 4.268+07 7.027+07 0.000+00 0.000+00 0.000+00 0.000+00 8.856+10 8.613+10 0.000+00 0.000+00 0.000+00
0.000+00 2.663−02 0.000+00 4.170−02 0.000+00 0.000+00 5.830−01 0.000+00 0.000+00 9.236−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.809−03 1.875−02 4.366−02 0.000+00 0.000+00 5.938−02 5.316−01 0.000+00 0.000+00 9.570−03 0.000+00 0.000+00 1.371−02 1.232−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.110−02 2.093−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.196−03 4.160−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.281−02 0.000+00 0.000+00 4.834−02 9.665−01 0.000+00 0.000+00 2.540−03 0.000+00 0.000+00 7.438−03 1.491−01 0.000+00 0.000+00 5.189−02 1.229−01 0.000+00 0.000+00 0.000+00 0.000+00 1.509−01 2.916−01 0.000+00 0.000+00 0.000+00
0.000+00 3.745−01 0.000+00 1.429−02 0.000+00 0.000+00 1.942−01 0.000+00 0.000+00 2.140−03 0.000+00 0.000+00 3.125−02 0.000+00 0.000+00 7.474−02 6.748−01 3.015−02 0.000+00 0.000+00 3.987−02 3.565−01 0.000+00 0.000+00 4.458−03 0.000+00 0.000+00 6.322−03 5.680−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.654−03 1.438−03 0.000+00 0.000+00 6.907−01 0.000+00 0.000+00 1.028−03 1.945−04 0.000+00 0.000+00 7.306−02 0.000+00 0.000+00 0.000+00 0.000+00 1.323−02 0.000+00 0.000+00 4.953−02 9.899−01 0.000+00 0.000+00 1.785−03 0.000+00 0.000+00 5.210−03 1.044−01 0.000+00 0.000+00 9.731−01 1.954+00 0.000+00 0.000+00 0.000+00 0.000+00 1.059−01 2.040−01 0.000+00 0.000+00 0.000+00
3.953−03 0.000+00 0.000+00 0.000+00 0.000+00 6.192+07 0.000+00 0.000+00 2.310+08 0.000+00 0.000+00 3.509+07 0.000+00 0.000+00 2.516+06 0.000+00 0.000+00 0.000+00 1.235+08 6.152+07 0.000+00 0.000+00 6.437+07 2.903+08 0.000+00 6.864+07 3.446+07 0.000+00 0.000+00 5.617+05 2.635+06 0.000+00 1.784−06 2.170+07 0.000+00 0.000+00 3.929+07 1.122+07 0.000+00 0.000+00 1.316+07 0.000+00 0.000+00 1.890+07 5.415+06 0.000+00 0.000+00 4.916+08 3.258+07 0.000+00 0.000+00 1.679+07 4.477+07 0.000+00 0.000+00 1.972+07 0.000+00 0.000+00 8.051+06 2.153+07 0.000+00 0.000+00 5.458+07 5.454+08 0.000+00 0.000+00 2.371+01 2.842+01 0.000+00 0.000+00 0.000+00 0.000+00 2.827+07 2.829+07 0.000+00
2.995+01 0.000+00 0.000+00 0.000+00 4.325+01 1.342+03 0.000+00 0.000+00 0.000+00 0.000+00 5.189+01 9.408+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.694+03 3.080+02 0.000+00 0.000+00 9.553+00 0.000+00 0.000+00 2.851+03 3.691+02 0.000+00 0.000+00 4.609+00 0.000+00 0.000+00 1.124+00 4.766−02 0.000+00 0.000+00 1.132+02 8.779+01 0.000+00 0.000+00 2.881−02 0.000+00 0.000+00 1.168+02 5.238+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.339+02 3.744+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.491+02 3.863+02 0.000+00 0.000+00 8.520+00 0.000+00 0.000+00 0.000+00 3.250−05 0.000+00 0.000+00 5.214+00 0.000+00 0.000+00 5.131−02 0.000+00 0.000+00
0.000+00 1.879−05 2.168−04 0.000+00 0.000+00 0.000+00 1.308+03 9.299+03 0.000+00 0.000+00 0.000+00 0.000+00 1.357+03 9.663+03 0.000+00 0.000+00 2.135−04 8.512+03 0.000+00 0.000+00 0.000+00 5.026+04 0.000+00 0.000+00 9.015+03 0.000+00 0.000+00 0.000+00 5.209+04 0.000+00 0.000+00 3.910−03 0.000+00 0.000+00 8.722+01 0.000+00 0.000+00 0.000+00 1.649+04 2.116+04 0.000+00 8.119+01 0.000+00 0.000+00 0.000+00 1.162+04 1.493+04 0.000+00 0.000+00 9.393+02 2.454+03 0.000+00 0.000+00 0.000+00 1.446+05 0.000+00 8.748+02 2.277+03 0.000+00 0.000+00 0.000+00 1.019+05 0.000+00 0.000+00 0.000+00 1.329−03 0.000+00 0.000+00 4.403−12 0.000+00 0.000+00 8.425+02 0.000+00 0.000+00 1.820−05
(continued on next page)
24
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 9 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.589+04 5.120+03 4.648+03 4.503+03 1.130+02 1.108+02 1.104+02 1.096+02 1.094+02 1.094+02 7.554+03 6.569+03 6.284+03 5.915+03 1.138+02 1.115+02 1.111+02 1.103+02 1.102+02 1.102+02 1.101+02 1.101+02 5.038+04 3.738+04 2.726+04 1.155+02 1.132+02 1.128+02 1.119+02 1.118+02 1.118+02 1.117+02 1.117+02 1.449+05 5.941+04 1.158+02 1.135+02 1.131+02 1.122+02 1.121+02 1.120+02 1.120+02 1.120+02 1.119+02 1.007+05 1.159+02 1.136+02 1.131+02 1.123+02 1.122+02 1.121+02 1.121+02 1.121+02 1.120+02 1.133+02 1.124+02 1.123+02 1.122+02 1.122+02 1.122+02 1.121+02 5.631+03 4.767+03 3.610+03 3.482+03 3.436+03 3.109+04 1.006+04 9.124+03 8.812+03 1.486+04 1.292+04 1.230+04 1.157+04 1.156+04
0.000+00 6.023+06 0.000+00 0.000+00 3.531+10 0.000+00 0.000+00 1.574+11 0.000+00 0.000+00 3.746+05 3.425+06 0.000+00 0.000+00 7.268+10 0.000+00 0.000+00 3.178+10 1.897+11 0.000+00 0.000+00 0.000+00 0.000+00 1.082+04 0.000+00 0.000+00 2.870+10 2.738+09 0.000+00 0.000+00 3.148+11 0.000+00 0.000+00 1.326+01 2.889+03 0.000+00 0.000+00 2.497+10 0.000+00 0.000+00 2.248+10 3.370+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.774+09 3.164+08 0.000+00 0.000+00 5.354+11 0.000+00 0.000+00 0.000+00 6.385+09 0.000+00 0.000+00 1.980+10 5.547+11 1.386+07 2.291+07 0.000+00 0.000+00 0.000+00 0.000+00 2.172+06 0.000+00 0.000+00 1.344+05 1.232+06 0.000+00 0.000+00 0.000+00
0.000+00 4.734−02 0.000+00 0.000+00 6.759−02 0.000+00 0.000+00 5.664−01 0.000+00 0.000+00 3.205−03 3.324−02 0.000+00 0.000+00 7.055−02 0.000+00 0.000+00 5.799−02 5.181−01 0.000+00 0.000+00 0.000+00 0.000+00 3.401−03 0.000+00 0.000+00 2.757−02 5.223−03 0.000+00 0.000+00 8.844−01 0.000+00 0.000+00 4.173−05 2.038−03 0.000+00 0.000+00 3.190−02 0.000+00 0.000+00 4.230−02 8.443−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.537−03 5.968−04 0.000+00 0.000+00 1.344+00 0.000+00 0.000+00 0.000+00 9.052−03 0.000+00 0.000+00 3.734−02 1.307+00 6.589−02 1.561−01 0.000+00 0.000+00 0.000+00 0.000+00 6.587−02 0.000+00 0.000+00 4.452−03 4.620−02 0.000+00 0.000+00 0.000+00
0.000+00 1.596+00 0.000+00 0.000+00 5.028−02 0.000+00 0.000+00 4.086−01 0.000+00 0.000+00 3.188−01 2.875+00 0.000+00 0.000+00 1.057−01 0.000+00 0.000+00 8.424−02 7.519−01 0.000+00 0.000+00 0.000+00 0.000+00 1.674+00 0.000+00 0.000+00 4.111−02 7.759−03 0.000+00 0.000+00 1.302+00 0.000+00 0.000+00 1.194−01 2.392+00 0.000+00 0.000+00 7.125−02 0.000+00 0.000+00 9.359−02 1.867+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.894−02 1.322−03 0.000+00 0.000+00 2.974+00 0.000+00 0.000+00 0.000+00 2.677−02 0.000+00 0.000+00 1.103−01 3.860+00 2.443+00 4.902+00 0.000+00 0.000+00 0.000+00 0.000+00 4.362+00 0.000+00 0.000+00 8.715−01 7.857+00 0.000+00 0.000+00 0.000+00
5.889−04 0.000+00 0.000+00 1.252−01 0.000+00 0.000+00 1.098+07 0.000+00 0.000+00 3.667+07 0.000+00 0.000+00 6.746−03 4.118−02 0.000+00 2.190+07 1.092+07 0.000+00 0.000+00 1.028+07 4.636+07 0.000+00 3.815−07 0.000+00 0.000+00 6.680+06 0.000+00 0.000+00 8.786+06 2.509+06 0.000+00 0.000+00 4.290+07 0.000+00 0.000+00 1.002+07 0.000+00 0.000+00 3.758+06 1.002+07 0.000+00 0.000+00 4.728+06 4.736+07 3.060−09 0.000+00 2.352+06 3.307+05 0.000+00 0.000+00 6.172+06 7.716+05 0.000+00 0.000+00 1.988+06 0.000+00 0.000+00 1.027+06 6.421+06 0.000+00 0.000+00 0.000+00 0.000+00 5.439+00 6.527+00 0.000+00 1.294−04 0.000+00 0.000+00 4.256−02 0.000+00 0.000+00 2.294−03 1.400−02 0.000+00
2.238+00 0.000+00 0.000+00 0.000+00 0.000+00 1.621+00 1.458+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.033−07 0.000+00 0.000+00 3.527+02 1.154+01 0.000+00 0.000+00 2.372−01 0.000+00 0.000+00 8.432−02 0.000+00 0.000+00 5.150−03 0.000+00 0.000+00 5.417+00 1.288+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.456+01 1.792+01 0.000+00 0.000+00 3.308−01 0.000+00 1.131−02 0.000+00 0.000+00 2.837−04 0.000+00 0.000+00 7.881+00 1.849+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.333+00 1.854+01 0.000+00 0.000+00 0.000+00 0.000+00 2.413−06 0.000+00 0.000+00 2.991−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.479−08 0.000+00 0.000+00
0.000+00 1.013−06 1.173−05 0.000+00 0.000+00 0.000+00 0.000+00 5.786+01 4.105+02 0.000+00 0.000+00 1.136−05 0.000+00 0.000+00 6.200+02 0.000+00 0.000+00 0.000+00 2.236+03 0.000+00 0.000+00 2.408−05 0.000+00 2.034−10 1.264−09 0.000+00 9.896+00 0.000+00 0.000+00 0.000+00 6.618+02 8.475+02 0.000+00 0.000+00 1.770−10 0.000+00 1.065+02 2.799+02 0.000+00 0.000+00 0.000+00 5.814+03 0.000+00 0.000+00 0.000+00 1.335−08 0.000+00 0.000+00 1.414+01 0.000+00 0.000+00 0.000+00 2.846+03 1.489+03 0.000+00 2.429+01 1.097+02 0.000+00 0.000+00 0.000+00 1.376+04 0.000+00 1.113−04 0.000+00 0.000+00 2.809−13 0.000+00 9.478−08 1.099−06 0.000+00 0.000+00 1.057−06 0.000+00 0.000+00 2.086−16
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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25
Table 9 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
9.843+04 7.120+04 5.227+04 5.208+04 2.573+05 1.115+05 1.106+05 8.271+04 1.967+05 1.940+05 1.219+05 1.416+07 3.206+05 3.280+05
0.000+00 5.595+03 0.000+00 0.000+00 8.456+00 1.562+03 0.000+00 0.000+00 0.000+00 1.668+02 0.000+00 1.586−05 3.831+01 0.000+00
0.000+00 6.378−03 0.000+00 0.000+00 8.394−05 3.880−03 0.000+00 0.000+00 0.000+00 1.254−03 0.000+00 4.768−07 7.378−04 0.000+00
0.000+00 5.979+00 0.000+00 0.000+00 4.266−01 8.543+00 0.000+00 0.000+00 0.000+00 4.805+00 0.000+00 1.778−01 6.229+00 0.000+00
9.627−08 0.000+00 0.000+00 3.245−06 0.000+00 0.000+00 8.335−09 3.568−07 1.053−09 0.000+00 0.000+00 0.000+00 0.000+00 2.662−11
1.131−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.877−12 0.000+00 1.519−03 0.000+00 0.000+00 0.000+00 0.000+00 3.396−04
0.000+00 2.900−11 1.742−10 0.000+00 0.000+00 2.719−11 0.000+00 0.000+00 0.000+00 2.958−13 1.579−12 0.000+00 1.164−13 0.000+00
26
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 10 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Ti XX. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
3.078+02 2.585+02 1.547+01 1.526+01 1.521+01 1.514+01 1.512+01 1.151+01 1.146+01 1.145+01 1.144+01 1.143+01 1.143+01 1.030+01 1.028+01 1.028+01 1.027+01 1.027+01 1.027+01 1.612+03 1.629+01 1.605+01 1.600+01 1.592+01 1.590+01 1.196+01 1.191+01 1.190+01 1.188+01 1.187+01 1.187+01 1.066+01 1.064+01 1.064+01 1.063+01 1.062+01 1.062+01 1.645+01 1.621+01 1.617+01 1.608+01 1.606+01 1.205+01 1.199+01 1.198+01 1.196+01 1.196+01 1.196+01 1.196+01 1.073+01 1.071+01 1.070+01 1.070+01 1.070+01 1.069+01 1.069+01 1.069+01 1.111+03 9.228+02 7.040+02 6.764+02 4.501+01 4.427+01 4.412+01 4.385+01 4.380+01 4.379+01 3.086+01 3.068+01 3.064+01 3.058+01 3.057+01 3.056+01
1.491+09 2.545+09 0.000+00 3.575+12 3.491+12 0.000+00 0.000+00 0.000+00 1.580+12 1.554+12 0.000+00 0.000+00 0.000+00 0.000+00 8.168+11 8.054+11 0.000+00 0.000+00 0.000+00 0.000+00 4.470+11 0.000+00 0.000+00 8.866+12 0.000+00 1.788+11 0.000+00 0.000+00 2.892+12 0.000+00 0.000+00 8.960+10 0.000+00 0.000+00 1.334+12 0.000+00 0.000+00 9.269+11 0.000+00 0.000+00 1.755+12 1.053+13 3.687+11 0.000+00 0.000+00 5.676+11 3.419+12 0.000+00 0.000+00 1.833+11 0.000+00 0.000+00 2.608+11 1.573+12 0.000+00 0.000+00 0.000+00 1.933+08 3.392+08 0.000+00 0.000+00 0.000+00 4.659+11 4.530+11 0.000+00 0.000+00 0.000+00 0.000+00 2.563+11 2.509+11 0.000+00 0.000+00 0.000+00
2.118−02 5.098−02 0.000+00 1.247−01 2.423−01 0.000+00 0.000+00 0.000+00 3.113−02 6.113−02 0.000+00 0.000+00 0.000+00 0.000+00 1.295−02 2.552−02 0.000+00 0.000+00 0.000+00 0.000+00 1.778−02 0.000+00 0.000+00 6.736−01 0.000+00 3.833−03 0.000+00 0.000+00 1.223−01 0.000+00 0.000+00 1.527−03 0.000+00 0.000+00 4.517−02 0.000+00 0.000+00 1.881−02 0.000+00 0.000+00 6.801−02 6.111−01 4.012−03 0.000+00 0.000+00 1.218−02 1.100−01 0.000+00 0.000+00 1.582−03 0.000+00 0.000+00 4.474−03 4.047−02 0.000+00 0.000+00 0.000+00 3.575−02 8.662−02 0.000+00 0.000+00 0.000+00 1.369−01 2.644−01 0.000+00 0.000+00 0.000+00 0.000+00 3.617−02 7.064−02 0.000+00 0.000+00 0.000+00
4.292−02 8.676−02 0.000+00 1.253−02 2.427−02 0.000+00 0.000+00 0.000+00 2.349−03 4.610−03 0.000+00 0.000+00 0.000+00 0.000+00 8.768−04 1.727−03 0.000+00 0.000+00 0.000+00 0.000+00 1.906−03 0.000+00 0.000+00 7.060−02 0.000+00 3.018−04 0.000+00 0.000+00 9.562−03 0.000+00 0.000+00 1.072−04 0.000+00 0.000+00 3.160−03 0.000+00 0.000+00 4.075−03 0.000+00 0.000+00 1.440−02 1.293−01 6.365−04 0.000+00 0.000+00 1.919−03 1.732−02 0.000+00 0.000+00 2.236−04 0.000+00 0.000+00 6.302−04 5.700−03 0.000+00 0.000+00 0.000+00 2.614−01 5.263−01 0.000+00 0.000+00 0.000+00 3.990−02 7.681−02 0.000+00 0.000+00 0.000+00 0.000+00 7.307−03 1.425−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.060+09 4.073+09 0.000+00 0.000+00 0.000+00 5.578+08 5.666+08 0.000+00 0.000+00 0.000+00 0.000+00 1.448+08 1.487+08 0.000+00 1.073−01 0.000+00 0.000+00 7.954+08 0.000+00 0.000+00 0.000+00 0.000+00 3.451+08 0.000+00 0.000+00 3.075+09 0.000+00 0.000+00 1.847+08 0.000+00 0.000+00 2.060+09 0.000+00 1.580+09 7.866+08 0.000+00 0.000+00 0.000+00 6.719+08 3.376+08 0.000+00 0.000+00 8.778+08 3.940+09 0.000+00 3.486+08 1.758+08 0.000+00 0.000+00 5.884+08 2.642+09 0.000+00 0.000+00 0.000+00 1.606+02 1.969+02 0.000+00 0.000+00 0.000+00 2.776+08 2.780+08 0.000+00 0.000+00 0.000+00 0.000+00 9.408+07 9.486+07 0.000+00
0.000+00 0.000+00 2.504+04 0.000+00 0.000+00 1.402+03 0.000+00 2.111+04 0.000+00 0.000+00 8.230+02 0.000+00 0.000+00 1.383+04 0.000+00 0.000+00 4.622+02 0.000+00 0.000+00 2.139+03 0.000+00 5.723+03 3.963+04 0.000+00 0.000+00 0.000+00 4.487+03 2.026+04 0.000+00 0.000+00 0.000+00 0.000+00 2.898+03 1.118+04 0.000+00 0.000+00 0.000+00 0.000+00 1.492+05 4.062+04 0.000+00 0.000+00 0.000+00 8.698+04 3.188+04 0.000+00 0.000+00 4.603+02 0.000+00 0.000+00 5.017+04 2.031+04 0.000+00 0.000+00 4.046+02 0.000+00 0.000+00 0.000+00 0.000+00 1.154−03 0.000+00 2.517+02 0.000+00 0.000+00 5.912+00 0.000+00 0.000+00 3.139+02 0.000+00 0.000+00 7.862+00 0.000+00 0.000+00
0.000+00 4.199+00 0.000+00 0.000+00 1.666+06 0.000+00 0.000+00 0.000+00 0.000+00 1.307+06 0.000+00 0.000+00 4.049−01 0.000+00 0.000+00 8.407+05 0.000+00 0.000+00 3.614−01 0.000+00 0.000+00 0.000+00 0.000+00 1.537+05 1.099+06 0.000+00 0.000+00 0.000+00 8.990+04 6.442+05 0.000+00 0.000+00 0.000+00 0.000+00 5.177+04 3.713+05 0.000+00 3.793+05 0.000+00 0.000+00 0.000+00 5.833+06 2.814+05 0.000+00 0.000+00 0.000+00 3.409+06 0.000+00 0.000+00 1.764+05 0.000+00 0.000+00 0.000+00 1.960+06 0.000+00 0.000+00 5.121−02 0.000+00 4.395−02 0.000+00 0.000+00 0.000+00 0.000+00 2.570+04 0.000+00 0.000+00 2.214−03 0.000+00 0.000+00 2.950+04 0.000+00 0.000+00 6.181−04
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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27
Table 10 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
5.454+03 1.922+03 1.730+03 4.691+01 4.611+01 4.594+01 4.565+01 4.560+01 4.559+01 3.174+01 3.155+01 3.151+01 3.144+01 3.143+01 3.143+01 2.968+03 2.534+03 4.732+01 4.650+01 4.633+01 4.604+01 4.599+01 4.597+01 4.594+01 3.193+01 3.174+01 3.170+01 3.162+01 3.161+01 3.161+01 3.160+01 3.160+01 1.730+04 4.808+01 4.724+01 4.707+01 4.676+01 4.671+01 4.669+01 4.667+01 3.227+01 3.208+01 3.204+01 3.197+01 3.195+01 3.195+01 3.194+01 3.194+01 4.822+01 4.737+01 4.720+01 4.689+01 4.683+01 4.682+01 4.679+01 3.233+01 3.214+01 3.210+01 3.203+01 3.201+01 3.201+01 3.200+01 3.200+01 3.200+01 2.698+03 2.233+03 1.702+03 1.634+03 1.614+03 9.815+01 9.637+01 9.601+01 9.536+01 9.525+01 9.521+01
0.000+00 2.410+07 0.000+00 1.250+11 0.000+00 0.000+00 9.327+11 0.000+00 0.000+00 6.059+10 0.000+00 0.000+00 4.595+11 0.000+00 0.000+00 1.305+06 1.264+07 2.585+11 0.000+00 0.000+00 1.872+11 1.119+12 0.000+00 0.000+00 1.246+11 0.000+00 0.000+00 9.146+10 5.483+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.640+10 6.263+09 0.000+00 0.000+00 2.067+12 0.000+00 0.000+00 2.848+10 2.690+09 0.000+00 0.000+00 6.826+11 0.000+00 0.000+00 0.000+00 0.000+00 5.731+10 0.000+00 0.000+00 1.471+11 2.208+12 0.000+00 0.000+00 2.459+10 0.000+00 0.000+00 4.840+10 7.283+11 0.000+00 0.000+00 4.526+07 8.024+07 0.000+00 0.000+00 0.000+00 0.000+00 1.094+11 1.061+11 0.000+00 0.000+00 0.000+00
0.000+00 2.669−02 0.000+00 4.123−02 0.000+00 0.000+00 5.828−01 0.000+00 0.000+00 9.152−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.724−03 1.825−02 4.338−02 0.000+00 0.000+00 5.949−02 5.322−01 0.000+00 0.000+00 9.523−03 0.000+00 0.000+00 1.371−02 1.232−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.111−02 2.080−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.197−03 4.139−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.276−02 0.000+00 0.000+00 4.833−02 9.663−01 0.000+00 0.000+00 2.532−03 0.000+00 0.000+00 7.434−03 1.491−01 0.000+00 0.000+00 4.942−02 1.200−01 0.000+00 0.000+00 0.000+00 0.000+00 1.523−01 2.932−01 0.000+00 0.000+00 0.000+00
0.000+00 3.378−01 0.000+00 1.273−02 0.000+00 0.000+00 1.752−01 0.000+00 0.000+00 1.913−03 0.000+00 0.000+00 2.820−02 0.000+00 0.000+00 6.741−02 6.088−01 2.703−02 0.000+00 0.000+00 3.606−02 3.223−01 0.000+00 0.000+00 4.004−03 0.000+00 0.000+00 5.711−03 5.130−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.911−03 1.290−03 0.000+00 0.000+00 6.230−01 0.000+00 0.000+00 9.281−04 1.746−04 0.000+00 0.000+00 6.592−02 0.000+00 0.000+00 0.000+00 0.000+00 1.190−02 0.000+00 0.000+00 4.470−02 8.932−01 0.000+00 0.000+00 1.605−03 0.000+00 0.000+00 4.700−03 9.424−02 0.000+00 0.000+00 8.780−01 1.764+00 0.000+00 0.000+00 0.000+00 0.000+00 9.662−02 1.853−01 0.000+00 0.000+00 0.000+00
8.965−03 0.000+00 0.000+00 0.000+00 0.000+00 8.424+07 0.000+00 0.000+00 3.144+08 0.000+00 0.000+00 4.778+07 0.000+00 0.000+00 3.442+06 0.000+00 0.000+00 0.000+00 1.679+08 8.363+07 0.000+00 0.000+00 8.740+07 3.943+08 0.000+00 9.328+07 4.685+07 0.000+00 0.000+00 7.479+05 3.526+06 0.000+00 4.060−06 2.946+07 0.000+00 0.000+00 5.347+07 1.527+07 0.000+00 0.000+00 1.787+07 0.000+00 0.000+00 2.571+07 7.368+06 0.000+00 0.000+00 6.688+08 4.422+07 0.000+00 0.000+00 2.284+07 6.090+07 0.000+00 0.000+00 2.679+07 0.000+00 0.000+00 1.095+07 2.928+07 0.000+00 0.000+00 7.424+07 7.418+08 0.000+00 0.000+00 2.777+01 3.415+01 0.000+00 0.000+00 0.000+00 0.000+00 3.836+07 3.840+07 0.000+00
5.536+01 0.000+00 0.000+00 0.000+00 7.225+01 2.241+03 0.000+00 0.000+00 0.000+00 0.000+00 8.668+01 1.571+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.160+03 5.131+02 0.000+00 0.000+00 1.593+01 0.000+00 0.000+00 4.755+03 6.148+02 0.000+00 0.000+00 7.676+00 0.000+00 0.000+00 2.082+00 7.941−02 0.000+00 0.000+00 1.892+02 1.469+02 0.000+00 0.000+00 4.774−02 0.000+00 0.000+00 1.951+02 8.762+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.580+02 6.252+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.163+02 6.450+02 0.000+00 0.000+00 1.423+01 0.000+00 0.000+00 0.000+00 4.937−05 0.000+00 0.000+00 8.683+00 0.000+00 0.000+00 8.620−02 0.000+00 0.000+00
0.000+00 2.873−05 3.478−04 0.000+00 0.000+00 0.000+00 1.973+03 1.402+04 0.000+00 0.000+00 0.000+00 0.000+00 2.047+03 1.457+04 0.000+00 0.000+00 2.816−04 1.276+04 0.000+00 0.000+00 0.000+00 7.572+04 0.000+00 0.000+00 1.352+04 0.000+00 0.000+00 0.000+00 7.844+04 0.000+00 0.000+00 7.229−03 0.000+00 0.000+00 1.316+02 0.000+00 0.000+00 0.000+00 2.487+04 3.192+04 0.000+00 1.226+02 0.000+00 0.000+00 0.000+00 1.753+04 2.252+04 0.000+00 0.000+00 1.419+03 3.689+03 0.000+00 0.000+00 0.000+00 2.180+05 0.000+00 1.322+03 3.424+03 0.000+00 0.000+00 0.000+00 1.536+05 0.000+00 0.000+00 0.000+00 1.776−03 0.000+00 0.000+00 7.162−12 0.000+00 0.000+00 1.271+03 0.000+00 0.000+00 3.350−05
(continued on next page)
28
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 10 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.295+04 4.606+03 4.141+03 4.018+03 1.018+02 9.994+01 9.955+01 9.885+01 9.873+01 9.869+01 7.148+03 6.087+03 5.826+03 5.440+03 1.027+02 1.007+02 1.003+02 9.961+01 9.949+01 9.945+01 9.939+01 9.938+01 4.101+04 3.151+04 2.276+04 1.042+02 1.022+02 1.018+02 1.010+02 1.009+02 1.008+02 1.008+02 1.008+02 1.360+05 5.116+04 1.044+02 1.024+02 1.020+02 1.013+02 1.011+02 1.011+02 1.010+02 1.010+02 1.010+02 8.201+04 1.045+02 1.025+02 1.021+02 1.013+02 1.012+02 1.012+02 1.011+02 1.011+02 1.011+02 1.022+02 1.015+02 1.013+02 1.013+02 1.012+02 1.012+02 1.012+02 5.335+03 4.407+03 3.356+03 3.221+03 3.178+03 2.533+04 9.044+03 8.126+03 7.862+03 1.407+04 1.196+04 1.140+04 1.064+04 1.063+04
0.000+00 7.466+06 0.000+00 0.000+00 4.299+10 0.000+00 0.000+00 1.933+11 0.000+00 0.000+00 3.988+05 3.884+06 0.000+00 0.000+00 8.877+10 0.000+00 0.000+00 3.907+10 2.331+11 0.000+00 0.000+00 0.000+00 0.000+00 1.631+04 0.000+00 0.000+00 3.526+10 3.347+09 0.000+00 0.000+00 3.865+11 0.000+00 0.000+00 1.447+01 4.084+03 0.000+00 0.000+00 3.058+10 0.000+00 0.000+00 2.760+10 4.137+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.334+09 3.885+08 0.000+00 0.000+00 6.575+11 0.000+00 0.000+00 0.000+00 7.846+09 0.000+00 0.000+00 2.430+10 6.810+11 1.470+07 2.618+07 0.000+00 0.000+00 0.000+00 0.000+00 2.695+06 0.000+00 0.000+00 1.431+05 1.397+06 0.000+00 0.000+00 0.000+00
0.000+00 4.748−02 0.000+00 0.000+00 6.686−02 0.000+00 0.000+00 5.663−01 0.000+00 0.000+00 3.055−03 3.236−02 0.000+00 0.000+00 7.012−02 0.000+00 0.000+00 5.812−02 5.189−01 0.000+00 0.000+00 0.000+00 0.000+00 3.641−03 0.000+00 0.000+00 2.759−02 5.195−03 0.000+00 0.000+00 8.840−01 0.000+00 0.000+00 4.011−05 2.136−03 0.000+00 0.000+00 3.180−02 0.000+00 0.000+00 4.230−02 8.441−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.555−03 5.966−04 0.000+00 0.000+00 1.344+00 0.000+00 0.000+00 0.000+00 9.060−03 0.000+00 0.000+00 3.734−02 1.307+00 6.275−02 1.525−01 0.000+00 0.000+00 0.000+00 0.000+00 6.609−02 0.000+00 0.000+00 4.244−03 4.499−02 0.000+00 0.000+00 0.000+00
0.000+00 1.440+00 0.000+00 0.000+00 4.484−02 0.000+00 0.000+00 3.686−01 0.000+00 0.000+00 2.875−01 2.594+00 0.000+00 0.000+00 9.480−02 0.000+00 0.000+00 7.624−02 6.798−01 0.000+00 0.000+00 0.000+00 0.000+00 1.511+00 0.000+00 0.000+00 3.711−02 6.961−03 0.000+00 0.000+00 1.174+00 0.000+00 0.000+00 1.077−01 2.159+00 0.000+00 0.000+00 6.406−02 0.000+00 0.000+00 8.446−02 1.685+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.712−02 1.193−03 0.000+00 0.000+00 2.683+00 0.000+00 0.000+00 0.000+00 2.418−02 0.000+00 0.000+00 9.955−02 3.483+00 2.204+00 4.425+00 0.000+00 0.000+00 0.000+00 0.000+00 3.935+00 0.000+00 0.000+00 7.862−01 7.089+00 0.000+00 0.000+00 0.000+00
1.336−03 0.000+00 0.000+00 1.802−01 0.000+00 0.000+00 1.494+07 0.000+00 0.000+00 4.993+07 0.000+00 0.000+00 8.017−03 5.097−02 0.000+00 2.979+07 1.485+07 0.000+00 0.000+00 1.397+07 6.300+07 0.000+00 8.687−07 0.000+00 0.000+00 9.073+06 0.000+00 0.000+00 1.196+07 3.414+06 0.000+00 0.000+00 5.842+07 0.000+00 0.000+00 1.361+07 0.000+00 0.000+00 5.112+06 1.363+07 0.000+00 0.000+00 6.433+06 6.445+07 6.956−09 0.000+00 3.202+06 4.494+05 0.000+00 0.000+00 8.396+06 1.050+06 0.000+00 0.000+00 2.702+06 0.000+00 0.000+00 1.397+06 8.734+06 0.000+00 0.000+00 0.000+00 0.000+00 6.379+00 7.851+00 0.000+00 2.934−04 0.000+00 0.000+00 6.129−02 0.000+00 0.000+00 2.726−03 1.734−02 0.000+00
4.138+00 0.000+00 0.000+00 0.000+00 0.000+00 2.708+00 2.435+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.125−07 0.000+00 0.000+00 5.884+02 1.924+01 0.000+00 0.000+00 3.959−01 0.000+00 0.000+00 1.563−01 0.000+00 0.000+00 8.594−03 0.000+00 0.000+00 9.053+00 2.154+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.778+01 2.994+01 0.000+00 0.000+00 5.527−01 0.000+00 2.094−02 0.000+00 0.000+00 4.722−04 0.000+00 0.000+00 1.317+01 3.089+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.225+01 3.097+01 0.000+00 0.000+00 0.000+00 0.000+00 3.669−06 0.000+00 0.000+00 5.531−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.812−08 0.000+00 0.000+00
0.000+00 1.552−06 1.886−05 0.000+00 0.000+00 0.000+00 0.000+00 8.728+01 6.191+02 0.000+00 0.000+00 1.500−05 0.000+00 0.000+00 9.305+02 0.000+00 0.000+00 0.000+00 3.370+03 0.000+00 0.000+00 4.447−05 0.000+00 4.314−10 2.812−09 0.000+00 1.493+01 0.000+00 0.000+00 0.000+00 9.981+02 1.278+03 0.000+00 0.000+00 3.375−10 0.000+00 1.608+02 4.210+02 0.000+00 0.000+00 0.000+00 8.765+03 0.000+00 0.000+00 0.000+00 2.495−08 0.000+00 0.000+00 2.136+01 0.000+00 0.000+00 0.000+00 4.291+03 2.245+03 0.000+00 3.672+01 1.655+02 0.000+00 0.000+00 0.000+00 2.075+04 0.000+00 1.488−04 0.000+00 0.000+00 4.576−13 0.000+00 1.454−07 1.769−06 0.000+00 0.000+00 1.396−06 0.000+00 0.000+00 3.510−16
(continued on next page)
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29
Table 10 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
8.012+04 6.016+04 4.374+04 4.359+04 2.415+05 9.630+04 9.560+04 7.040+04 1.602+05 1.582+05 9.937+04 1.320+07 2.618+05 2.671+05
0.000+00 8.366+03 0.000+00 0.000+00 9.227+00 2.187+03 0.000+00 0.000+00 0.000+00 2.772+02 0.000+00 1.767−05 6.346+01 0.000+00
0.000+00 6.810−03 0.000+00 0.000+00 8.069−05 4.053−03 0.000+00 0.000+00 0.000+00 1.387−03 0.000+00 4.616−07 8.152−04 0.000+00
0.000+00 5.396+00 0.000+00 0.000+00 3.850−01 7.710+00 0.000+00 0.000+00 0.000+00 4.336+00 0.000+00 1.604−01 5.622+00 0.000+00
2.193−07 0.000+00 0.000+00 6.433−06 0.000+00 0.000+00 1.407−08 6.503−07 2.394−09 0.000+00 0.000+00 0.000+00 0.000+00 6.049−11
2.097−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.688−11 0.000+00 2.813−03 0.000+00 0.000+00 0.000+00 0.000+00 6.287−04
0.000+00 6.071−11 3.835−10 0.000+00 0.000+00 5.100−11 0.000+00 0.000+00 0.000+00 7.390−13 3.958−12 0.000+00 2.890−13 0.000+00
30
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 11 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in V XXI. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.926+02 2.397+02 1.405+01 1.387+01 1.382+01 1.376+01 1.374+01 1.045+01 1.041+01 1.040+01 1.039+01 1.038+01 1.038+01 9.357+00 9.340+00 9.335+00 9.329+00 9.328+00 9.327+00 1.327+03 1.476+01 1.456+01 1.451+01 1.444+01 1.442+01 1.084+01 1.080+01 1.079+01 1.077+01 1.077+01 1.077+01 9.666+00 9.648+00 9.643+00 9.636+00 9.635+00 9.634+00 1.493+01 1.472+01 1.467+01 1.459+01 1.458+01 1.093+01 1.089+01 1.088+01 1.086+01 1.085+01 1.085+01 1.085+01 9.737+00 9.718+00 9.714+00 9.707+00 9.705+00 9.705+00 9.704+00 9.704+00 1.055+03 8.543+02 6.555+02 6.267+02 4.086+01 4.022+01 4.006+01 3.983+01 3.978+01 3.977+01 2.801+01 2.785+01 2.782+01 2.776+01 2.775+01 2.775+01
1.574+09 2.895+09 0.000+00 4.357+12 4.245+12 0.000+00 0.000+00 0.000+00 1.923+12 1.889+12 0.000+00 0.000+00 0.000+00 0.000+00 9.936+11 9.786+11 0.000+00 0.000+00 0.000+00 0.000+00 5.382+11 0.000+00 0.000+00 1.078+13 0.000+00 2.155+11 0.000+00 0.000+00 3.515+12 0.000+00 0.000+00 1.081+11 0.000+00 0.000+00 1.621+12 0.000+00 0.000+00 1.120+12 0.000+00 0.000+00 2.131+12 1.279+13 4.460+11 0.000+00 0.000+00 6.886+11 4.149+12 0.000+00 0.000+00 2.219+11 0.000+00 0.000+00 3.163+11 1.909+12 0.000+00 0.000+00 0.000+00 2.044+08 3.879+08 0.000+00 0.000+00 0.000+00 5.689+11 5.516+11 0.000+00 0.000+00 0.000+00 0.000+00 3.125+11 3.053+11 0.000+00 0.000+00 0.000+00
2.020−02 4.988−02 0.000+00 1.256−01 2.432−01 0.000+00 0.000+00 0.000+00 3.126−02 6.128−02 0.000+00 0.000+00 0.000+00 0.000+00 1.299−02 2.557−02 0.000+00 0.000+00 0.000+00 0.000+00 1.758−02 0.000+00 0.000+00 6.733−01 0.000+00 3.798−03 0.000+00 0.000+00 1.222−01 0.000+00 0.000+00 1.514−03 0.000+00 0.000+00 4.515−02 0.000+00 0.000+00 1.871−02 0.000+00 0.000+00 6.804−02 6.114−01 3.995−03 0.000+00 0.000+00 1.217−02 1.099−01 0.000+00 0.000+00 1.577−03 0.000+00 0.000+00 4.467−03 4.043−02 0.000+00 0.000+00 0.000+00 3.412−02 8.489−02 0.000+00 0.000+00 0.000+00 1.379−01 2.655−01 0.000+00 0.000+00 0.000+00 0.000+00 3.636−02 7.084−02 0.000+00 0.000+00 0.000+00
3.891−02 7.874−02 0.000+00 1.147−02 2.214−02 0.000+00 0.000+00 0.000+00 2.143−03 4.197−03 0.000+00 0.000+00 0.000+00 0.000+00 7.990−04 1.572−03 0.000+00 0.000+00 0.000+00 0.000+00 1.708−03 0.000+00 0.000+00 6.399−02 0.000+00 2.711−04 0.000+00 0.000+00 8.666−03 0.000+00 0.000+00 9.638−05 0.000+00 0.000+00 2.864−03 0.000+00 0.000+00 3.677−03 0.000+00 0.000+00 1.308−02 1.174−01 5.752−04 0.000+00 0.000+00 1.740−03 1.571−02 0.000+00 0.000+00 2.022−04 0.000+00 0.000+00 5.710−04 5.167−03 0.000+00 0.000+00 0.000+00 2.370−01 4.775−01 0.000+00 0.000+00 0.000+00 3.653−02 7.004−02 0.000+00 0.000+00 0.000+00 0.000+00 6.668−03 1.297−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.409+09 5.427+09 0.000+00 0.000+00 0.000+00 7.368+08 7.498+08 0.000+00 0.000+00 0.000+00 0.000+00 1.901+08 1.958+08 0.000+00 2.338−01 0.000+00 0.000+00 1.066+09 0.000+00 0.000+00 0.000+00 0.000+00 4.627+08 0.000+00 0.000+00 4.121+09 0.000+00 0.000+00 2.482+08 0.000+00 0.000+00 2.760+09 0.000+00 2.115+09 1.053+09 0.000+00 0.000+00 0.000+00 8.987+08 4.518+08 0.000+00 0.000+00 1.176+09 5.277+09 0.000+00 4.664+08 2.354+08 0.000+00 0.000+00 7.880+08 3.538+09 0.000+00 0.000+00 0.000+00 1.885+02 2.374+02 0.000+00 0.000+00 0.000+00 3.708+08 3.715+08 0.000+00 0.000+00 0.000+00 0.000+00 1.252+08 1.263+08 0.000+00
0.000+00 0.000+00 4.052+04 0.000+00 0.000+00 2.269+03 0.000+00 3.418+04 0.000+00 0.000+00 1.331+03 0.000+00 0.000+00 2.239+04 0.000+00 0.000+00 7.468+02 0.000+00 0.000+00 3.836+03 0.000+00 9.320+03 6.458+04 0.000+00 0.000+00 0.000+00 7.306+03 3.302+04 0.000+00 0.000+00 0.000+00 0.000+00 4.720+03 1.823+04 0.000+00 0.000+00 0.000+00 0.000+00 2.425+05 6.588+04 0.000+00 0.000+00 0.000+00 1.414+05 5.169+04 0.000+00 0.000+00 7.494+02 0.000+00 0.000+00 8.154+04 3.292+04 0.000+00 0.000+00 6.588+02 0.000+00 0.000+00 0.000+00 0.000+00 1.728−03 0.000+00 4.086+02 0.000+00 0.000+00 9.630+00 0.000+00 0.000+00 5.096+02 0.000+00 0.000+00 1.279+01 0.000+00 0.000+00
0.000+00 5.554+00 0.000+00 0.000+00 2.454+06 0.000+00 0.000+00 0.000+00 0.000+00 1.926+06 0.000+00 0.000+00 7.243−01 0.000+00 0.000+00 1.238+06 0.000+00 0.000+00 6.469−01 0.000+00 0.000+00 0.000+00 0.000+00 2.272+05 1.624+06 0.000+00 0.000+00 0.000+00 1.328+05 9.524+05 0.000+00 0.000+00 0.000+00 0.000+00 7.646+04 5.489+05 0.000+00 5.573+05 0.000+00 0.000+00 0.000+00 8.598+06 4.137+05 0.000+00 0.000+00 0.000+00 5.023+06 0.000+00 0.000+00 2.595+05 0.000+00 0.000+00 0.000+00 2.888+06 0.000+00 0.000+00 9.182−02 0.000+00 5.864−02 0.000+00 0.000+00 0.000+00 0.000+00 3.796+04 0.000+00 0.000+00 3.949−03 0.000+00 0.000+00 4.356+04 0.000+00 0.000+00 1.095−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 11 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
4.487+03 1.731+03 1.543+03 4.250+01 4.181+01 4.165+01 4.139+01 4.134+01 4.133+01 2.877+01 2.861+01 2.857+01 2.851+01 2.850+01 2.850+01 2.817+03 2.352+03 4.291+01 4.220+01 4.204+01 4.178+01 4.173+01 4.171+01 4.169+01 2.896+01 2.879+01 2.875+01 2.869+01 2.868+01 2.868+01 2.867+01 2.867+01 1.422+04 4.357+01 4.285+01 4.267+01 4.241+01 4.235+01 4.234+01 4.231+01 2.926+01 2.909+01 2.905+01 2.899+01 2.898+01 2.897+01 2.897+01 2.897+01 4.371+01 4.297+01 4.280+01 4.253+01 4.248+01 4.247+01 4.244+01 2.932+01 2.915+01 2.911+01 2.905+01 2.903+01 2.903+01 2.902+01 2.902+01 2.902+01 2.563+03 2.066+03 1.584+03 1.513+03 1.495+03 8.907+01 8.753+01 8.717+01 8.660+01 8.649+01 8.645+01
0.000+00 2.992+07 0.000+00 1.506+11 0.000+00 0.000+00 1.134+12 0.000+00 0.000+00 7.312+10 0.000+00 0.000+00 5.587+11 0.000+00 0.000+00 1.384+06 1.433+07 3.128+11 0.000+00 0.000+00 2.277+11 1.361+12 0.000+00 0.000+00 1.509+11 0.000+00 0.000+00 1.111+11 6.664+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.084+10 7.579+09 0.000+00 0.000+00 2.513+12 0.000+00 0.000+00 3.468+10 3.256+09 0.000+00 0.000+00 8.301+11 0.000+00 0.000+00 0.000+00 0.000+00 6.947+10 0.000+00 0.000+00 1.787+11 2.684+12 0.000+00 0.000+00 2.981+10 0.000+00 0.000+00 5.881+10 8.852+11 0.000+00 0.000+00 4.789+07 9.191+07 0.000+00 0.000+00 0.000+00 0.000+00 1.336+11 1.292+11 0.000+00 0.000+00 0.000+00
0.000+00 2.688−02 0.000+00 4.079−02 0.000+00 0.000+00 5.826−01 0.000+00 0.000+00 9.076−03 0.000+00 0.000+00 1.362−01 0.000+00 0.000+00 1.647−03 1.782−02 4.317−02 0.000+00 0.000+00 5.959−02 5.328−01 0.000+00 0.000+00 9.485−03 0.000+00 0.000+00 1.372−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.112−02 2.069−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.200−03 4.119−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.272−02 0.000+00 0.000+00 4.832−02 9.661−01 0.000+00 0.000+00 2.525−03 0.000+00 0.000+00 7.431−03 1.491−01 0.000+00 0.000+00 4.717−02 1.176−01 0.000+00 0.000+00 0.000+00 0.000+00 1.535−01 2.944−01 0.000+00 0.000+00 0.000+00
0.000+00 3.063−01 0.000+00 1.142−02 0.000+00 0.000+00 1.588−01 0.000+00 0.000+00 1.719−03 0.000+00 0.000+00 2.556−02 0.000+00 0.000+00 6.109−02 5.519−01 2.439−02 0.000+00 0.000+00 3.278−02 2.927−01 0.000+00 0.000+00 3.617−03 0.000+00 0.000+00 5.183−03 4.655−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.276−03 1.163−03 0.000+00 0.000+00 5.647−01 0.000+00 0.000+00 8.428−04 1.576−04 0.000+00 0.000+00 5.977−02 0.000+00 0.000+00 0.000+00 0.000+00 1.075−02 0.000+00 0.000+00 4.053−02 8.099−01 0.000+00 0.000+00 1.452−03 0.000+00 0.000+00 4.261−03 8.546−02 0.000+00 0.000+00 7.962−01 1.600+00 0.000+00 0.000+00 0.000+00 0.000+00 8.847−02 1.690−01 0.000+00 0.000+00 0.000+00
1.955−02 0.000+00 0.000+00 0.000+00 0.000+00 1.129+08 0.000+00 0.000+00 4.218+08 0.000+00 0.000+00 6.411+07 0.000+00 0.000+00 4.654+06 0.000+00 0.000+00 0.000+00 2.249+08 1.120+08 0.000+00 0.000+00 1.169+08 5.277+08 0.000+00 1.249+08 6.275+07 0.000+00 0.000+00 9.831+05 4.659+06 0.000+00 8.876−06 3.939+07 0.000+00 0.000+00 7.166+07 2.047+07 0.000+00 0.000+00 2.391+07 0.000+00 0.000+00 3.445+07 9.878+06 0.000+00 0.000+00 8.962+08 5.914+07 0.000+00 0.000+00 3.060+07 8.160+07 0.000+00 0.000+00 3.585+07 0.000+00 0.000+00 1.466+07 3.923+07 0.000+00 0.000+00 9.948+07 9.939+08 0.000+00 0.000+00 3.269+01 4.126+01 0.000+00 0.000+00 0.000+00 0.000+00 5.131+07 5.136+07 0.000+00
9.936+01 0.000+00 0.000+00 0.000+00 1.178+02 3.652+03 0.000+00 0.000+00 0.000+00 0.000+00 1.412+02 2.560+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.002+04 8.339+02 0.000+00 0.000+00 2.590+01 0.000+00 0.000+00 7.737+03 9.990+02 0.000+00 0.000+00 1.247+01 0.000+00 0.000+00 3.744+00 1.291−01 0.000+00 0.000+00 3.084+02 2.396+02 0.000+00 0.000+00 7.727−02 0.000+00 0.000+00 3.181+02 1.430+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.096+02 1.018+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 6.786+02 1.051+03 0.000+00 0.000+00 2.318+01 0.000+00 0.000+00 0.000+00 7.407−05 0.000+00 0.000+00 1.411+01 0.000+00 0.000+00 1.411−01 0.000+00 0.000+00
0.000+00 4.399−05 5.588−04 0.000+00 0.000+00 0.000+00 2.917+03 2.074+04 0.000+00 0.000+00 0.000+00 0.000+00 3.026+03 2.155+04 0.000+00 0.000+00 3.706−04 1.878+04 0.000+00 0.000+00 0.000+00 1.118+05 0.000+00 0.000+00 1.990+04 0.000+00 0.000+00 0.000+00 1.158+05 0.000+00 0.000+00 1.297−02 0.000+00 0.000+00 1.949+02 0.000+00 0.000+00 0.000+00 3.677+04 4.720+04 0.000+00 1.815+02 0.000+00 0.000+00 0.000+00 2.591+04 3.331+04 0.000+00 0.000+00 2.103+03 5.439+03 0.000+00 0.000+00 0.000+00 3.220+05 0.000+00 1.960+03 5.048+03 0.000+00 0.000+00 0.000+00 2.268+05 0.000+00 0.000+00 0.000+00 2.376−03 0.000+00 0.000+00 1.155−11 0.000+00 0.000+00 1.878+03 0.000+00 0.000+00 5.992−05
(continued on next page)
32
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 11 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
1.065+04 4.145+03 3.691+03 3.588+03 9.228+01 9.063+01 9.024+01 8.963+01 8.951+01 8.947+01 6.784+03 5.648+03 5.409+03 5.008+03 9.308+01 9.140+01 9.101+01 9.039+01 9.027+01 9.023+01 9.017+01 9.017+01 3.372+04 2.670+04 1.913+04 9.438+01 9.265+01 9.224+01 9.161+01 9.148+01 9.145+01 9.138+01 9.138+01 1.281+05 4.419+04 9.464+01 9.291+01 9.250+01 9.186+01 9.173+01 9.169+01 9.163+01 9.163+01 9.159+01 6.746+04 9.471+01 9.298+01 9.256+01 9.193+01 9.180+01 9.176+01 9.170+01 9.170+01 9.166+01 9.269+01 9.205+01 9.192+01 9.189+01 9.182+01 9.182+01 9.178+01 5.068+03 4.076+03 3.123+03 2.982+03 2.943+03 2.084+04 8.138+03 7.243+03 7.020+03 1.335+04 1.110+04 1.058+04 9.798+03 9.790+03
0.000+00 9.286+06 0.000+00 0.000+00 5.185+10 0.000+00 0.000+00 2.350+11 0.000+00 0.000+00 4.228+05 4.409+06 0.000+00 0.000+00 1.074+11 0.000+00 0.000+00 4.755+10 2.836+11 0.000+00 0.000+00 0.000+00 0.000+00 2.432+04 0.000+00 0.000+00 4.293+10 4.053+09 0.000+00 0.000+00 4.698+11 0.000+00 0.000+00 1.569+01 5.746+03 0.000+00 0.000+00 3.708+10 0.000+00 0.000+00 3.355+10 5.028+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.015+10 4.722+08 0.000+00 0.000+00 7.992+11 0.000+00 0.000+00 0.000+00 9.546+09 0.000+00 0.000+00 2.954+10 8.277+11 1.556+07 3.002+07 0.000+00 0.000+00 0.000+00 0.000+00 3.354+06 0.000+00 0.000+00 1.517+05 1.587+06 0.000+00 0.000+00 0.000+00
0.000+00 4.784−02 0.000+00 0.000+00 6.620−02 0.000+00 0.000+00 5.660−01 0.000+00 0.000+00 2.917−03 3.163−02 0.000+00 0.000+00 6.979−02 0.000+00 0.000+00 5.824−02 5.196−01 0.000+00 0.000+00 0.000+00 0.000+00 3.897−03 0.000+00 0.000+00 2.762−02 5.170−03 0.000+00 0.000+00 8.835−01 0.000+00 0.000+00 3.861−05 2.243−03 0.000+00 0.000+00 3.170−02 0.000+00 0.000+00 4.230−02 8.439−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.574−03 5.965−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.069−03 0.000+00 0.000+00 3.733−02 1.307+00 5.991−02 1.496−01 0.000+00 0.000+00 0.000+00 0.000+00 6.659−02 0.000+00 0.000+00 4.054−03 4.397−02 0.000+00 0.000+00 0.000+00
0.000+00 1.306+00 0.000+00 0.000+00 4.022−02 0.000+00 0.000+00 3.340−01 0.000+00 0.000+00 2.606−01 2.352+00 0.000+00 0.000+00 8.555−02 0.000+00 0.000+00 6.933−02 6.176−01 0.000+00 0.000+00 0.000+00 0.000+00 1.370+00 0.000+00 0.000+00 3.370−02 6.280−03 0.000+00 0.000+00 1.064+00 0.000+00 0.000+00 9.770−02 1.958+00 0.000+00 0.000+00 5.793−02 0.000+00 0.000+00 7.661−02 1.528+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.557−02 1.082−03 0.000+00 0.000+00 2.433+00 0.000+00 0.000+00 0.000+00 2.196−02 0.000+00 0.000+00 9.028−02 3.159+00 1.999+00 4.014+00 0.000+00 0.000+00 0.000+00 0.000+00 3.568+00 0.000+00 0.000+00 7.127−01 6.428+00 0.000+00 0.000+00 0.000+00
2.912−03 0.000+00 0.000+00 2.612−01 0.000+00 0.000+00 2.002+07 0.000+00 0.000+00 6.698+07 0.000+00 0.000+00 9.552−03 6.338−02 0.000+00 3.992+07 1.989+07 0.000+00 0.000+00 1.871+07 8.435+07 0.000+00 1.901−06 0.000+00 0.000+00 1.214+07 0.000+00 0.000+00 1.603+07 4.577+06 0.000+00 0.000+00 7.838+07 0.000+00 0.000+00 1.822+07 0.000+00 0.000+00 6.852+06 1.826+07 0.000+00 0.000+00 8.622+06 8.640+07 1.519−08 0.000+00 4.295+06 6.018+05 0.000+00 0.000+00 1.125+07 1.407+06 0.000+00 0.000+00 3.618+06 0.000+00 0.000+00 1.872+06 1.170+07 0.000+00 0.000+00 0.000+00 0.000+00 7.515+00 9.500+00 0.000+00 6.399−04 0.000+00 0.000+00 8.884−02 0.000+00 0.000+00 3.250−03 2.157−02 0.000+00
7.428+00 0.000+00 0.000+00 0.000+00 0.000+00 4.414+00 3.968+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.737−07 0.000+00 0.000+00 9.575+02 3.130+01 0.000+00 0.000+00 6.446−01 0.000+00 0.000+00 2.811−01 0.000+00 0.000+00 1.399−02 0.000+00 0.000+00 1.476+01 3.515+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.419+01 4.878+01 0.000+00 0.000+00 9.006−01 0.000+00 3.763−02 0.000+00 0.000+00 7.669−04 0.000+00 0.000+00 2.145+01 5.034+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.996+01 5.046+01 0.000+00 0.000+00 0.000+00 0.000+00 5.510−06 0.000+00 0.000+00 9.928−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.779−08 0.000+00 0.000+00
0.000+00 2.383−06 3.037−05 0.000+00 0.000+00 0.000+00 0.000+00 1.291+02 9.151+02 0.000+00 0.000+00 1.977−05 0.000+00 0.000+00 1.370+03 0.000+00 0.000+00 0.000+00 4.980+03 0.000+00 0.000+00 7.974−05 0.000+00 8.960−10 6.090−09 0.000+00 2.210+01 0.000+00 0.000+00 0.000+00 1.476+03 1.890+03 0.000+00 0.000+00 6.363−10 0.000+00 2.382+02 6.209+02 0.000+00 0.000+00 0.000+00 1.295+04 0.000+00 0.000+00 0.000+00 4.515−08 0.000+00 0.000+00 3.162+01 0.000+00 0.000+00 0.000+00 6.341+03 3.319+03 0.000+00 5.441+01 2.448+02 0.000+00 0.000+00 0.000+00 3.066+04 0.000+00 1.994−04 0.000+00 0.000+00 7.390−13 0.000+00 2.234−07 2.852−06 0.000+00 0.000+00 1.842−06 0.000+00 0.000+00 5.847−16
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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33
Table 11 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
6.588+04 5.109+04 3.681+04 3.670+04 2.276+05 8.344+04 8.288+04 6.018+04 1.317+05 1.303+05 8.181+04 1.236+07 2.159+05 2.197+05
0.000+00 1.239+04 0.000+00 0.000+00 1.000+01 3.049+03 0.000+00 0.000+00 0.000+00 4.498+02 0.000+00 1.951−05 1.027+02 0.000+00
0.000+00 7.273−03 0.000+00 0.000+00 7.765−05 4.243−03 0.000+00 0.000+00 0.000+00 1.527−03 0.000+00 4.470−07 8.967−04 0.000+00
0.000+00 4.893+00 0.000+00 0.000+00 3.491−01 6.992+00 0.000+00 0.000+00 0.000+00 3.933+00 0.000+00 1.455−01 5.099+00 0.000+00
4.798−07 0.000+00 0.000+00 1.250−05 0.000+00 0.000+00 2.363−08 1.172−06 5.229−09 0.000+00 0.000+00 0.000+00 0.000+00 1.321−10
3.771−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.150−11 0.000+00 5.055−03 0.000+00 0.000+00 0.000+00 0.000+00 1.129−03
0.000+00 1.247−10 8.233−10 0.000+00 0.000+00 9.472−11 0.000+00 0.000+00 0.000+00 1.767−12 9.490−12 0.000+00 6.874−13 0.000+00
34
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 12 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Cr XXII. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.787+02 2.224+02 1.282+01 1.266+01 1.261+01 1.256+01 1.254+01 9.537+00 9.499+00 9.489+00 9.475+00 9.472+00 9.471+00 8.534+00 8.519+00 8.515+00 8.509+00 8.508+00 8.507+00 1.102+03 1.344+01 1.326+01 1.321+01 1.315+01 1.313+01 9.875+00 9.835+00 9.824+00 9.809+00 9.805+00 9.805+00 8.804+00 8.788+00 8.783+00 8.777+00 8.776+00 8.775+00 1.360+01 1.342+01 1.337+01 1.331+01 1.329+01 9.964+00 9.923+00 9.912+00 9.897+00 9.894+00 9.893+00 9.891+00 8.875+00 8.858+00 8.854+00 8.848+00 8.846+00 8.846+00 8.845+00 8.845+00 1.005+03 7.912+02 6.109+02 5.809+02 3.725+01 3.669+01 3.654+01 3.633+01 3.629+01 3.628+01 2.554+01 2.540+01 2.536+01 2.531+01 2.530+01 2.530+01
1.658+09 3.304+09 0.000+00 5.262+12 5.115+12 0.000+00 0.000+00 0.000+00 2.319+12 2.274+12 0.000+00 0.000+00 0.000+00 0.000+00 1.198+12 1.178+12 0.000+00 0.000+00 0.000+00 0.000+00 6.427+11 0.000+00 0.000+00 1.299+13 0.000+00 2.576+11 0.000+00 0.000+00 4.235+12 0.000+00 0.000+00 1.294+11 0.000+00 0.000+00 1.953+12 0.000+00 0.000+00 1.344+12 0.000+00 0.000+00 2.565+12 1.539+13 5.353+11 0.000+00 0.000+00 8.279+11 4.991+12 0.000+00 0.000+00 2.664+11 0.000+00 0.000+00 3.801+11 2.296+12 0.000+00 0.000+00 0.000+00 2.157+08 4.450+08 0.000+00 0.000+00 0.000+00 6.882+11 6.654+11 0.000+00 0.000+00 0.000+00 0.000+00 3.776+11 3.681+11 0.000+00 0.000+00 0.000+00
1.931−02 4.901−02 0.000+00 1.264−01 2.440−01 0.000+00 0.000+00 0.000+00 3.138−02 6.140−02 0.000+00 0.000+00 0.000+00 0.000+00 1.303−02 2.561−02 0.000+00 0.000+00 0.000+00 0.000+00 1.740−02 0.000+00 0.000+00 6.729−01 0.000+00 3.766−03 0.000+00 0.000+00 1.222−01 0.000+00 0.000+00 1.504−03 0.000+00 0.000+00 4.512−02 0.000+00 0.000+00 1.863−02 0.000+00 0.000+00 6.807−02 6.115−01 3.983−03 0.000+00 0.000+00 1.216−02 1.099−01 0.000+00 0.000+00 1.573−03 0.000+00 0.000+00 4.461−03 4.040−02 0.000+00 0.000+00 0.000+00 3.264−02 8.353−02 0.000+00 0.000+00 0.000+00 1.389−01 2.664−01 0.000+00 0.000+00 0.000+00 0.000+00 3.652−02 7.100−02 0.000+00 0.000+00 0.000+00
3.542−02 7.177−02 0.000+00 1.053−02 2.026−02 0.000+00 0.000+00 0.000+00 1.962−03 3.836−03 0.000+00 0.000+00 0.000+00 0.000+00 7.310−04 1.436−03 0.000+00 0.000+00 0.000+00 0.000+00 1.539−03 0.000+00 0.000+00 5.825−02 0.000+00 2.449−04 0.000+00 0.000+00 7.890−03 0.000+00 0.000+00 8.715−05 0.000+00 0.000+00 2.608−03 0.000+00 0.000+00 3.337−03 0.000+00 0.000+00 1.193−02 1.070−01 5.226−04 0.000+00 0.000+00 1.584−03 1.431−02 0.000+00 0.000+00 1.838−04 0.000+00 0.000+00 5.197−04 4.706−03 0.000+00 0.000+00 0.000+00 2.159−01 4.352−01 0.000+00 0.000+00 0.000+00 3.355−02 6.408−02 0.000+00 0.000+00 0.000+00 0.000+00 6.109−03 1.186−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.113+09 7.140+09 0.000+00 0.000+00 0.000+00 9.618+08 9.806+08 0.000+00 0.000+00 0.000+00 0.000+00 2.467+08 2.549+08 0.000+00 4.917−01 0.000+00 0.000+00 1.408+09 0.000+00 0.000+00 0.000+00 0.000+00 6.122+08 0.000+00 0.000+00 5.446+09 0.000+00 0.000+00 3.291+08 0.000+00 0.000+00 3.647+09 0.000+00 2.794+09 1.390+09 0.000+00 0.000+00 0.000+00 1.186+09 5.965+08 0.000+00 0.000+00 1.554+09 6.972+09 0.000+00 6.155+08 3.110+08 0.000+00 0.000+00 1.041+09 4.673+09 0.000+00 0.000+00 0.000+00 2.224+02 2.879+02 0.000+00 0.000+00 0.000+00 4.890+08 4.899+08 0.000+00 0.000+00 0.000+00 0.000+00 1.645+08 1.662+08 0.000+00
0.000+00 0.000+00 6.418+04 0.000+00 0.000+00 3.594+03 0.000+00 5.416+04 0.000+00 0.000+00 2.106+03 0.000+00 0.000+00 3.546+04 0.000+00 0.000+00 1.181+03 0.000+00 0.000+00 6.699+03 0.000+00 1.484+04 1.029+05 0.000+00 0.000+00 0.000+00 1.164+04 5.263+04 0.000+00 0.000+00 0.000+00 0.000+00 7.519+03 2.906+04 0.000+00 0.000+00 0.000+00 0.000+00 3.855+05 1.045+05 0.000+00 0.000+00 0.000+00 2.248+05 8.197+04 0.000+00 0.000+00 1.193+03 0.000+00 0.000+00 1.296+05 5.218+04 0.000+00 0.000+00 1.049+03 0.000+00 0.000+00 0.000+00 0.000+00 2.558−03 0.000+00 6.488+02 0.000+00 0.000+00 1.534+01 0.000+00 0.000+00 8.093+02 0.000+00 0.000+00 2.036+01 0.000+00 0.000+00
0.000+00 7.363+00 0.000+00 0.000+00 3.551+06 0.000+00 0.000+00 0.000+00 0.000+00 2.787+06 0.000+00 0.000+00 1.262+00 0.000+00 0.000+00 1.792+06 0.000+00 0.000+00 1.128+00 0.000+00 0.000+00 0.000+00 0.000+00 3.297+05 2.359+06 0.000+00 0.000+00 0.000+00 1.927+05 1.383+06 0.000+00 0.000+00 0.000+00 0.000+00 1.109+05 7.971+05 0.000+00 8.051+05 0.000+00 0.000+00 0.000+00 1.245+07 5.979+05 0.000+00 0.000+00 0.000+00 7.269+06 0.000+00 0.000+00 3.752+05 0.000+00 0.000+00 0.000+00 4.178+06 0.000+00 0.000+00 1.602−01 0.000+00 7.842−02 0.000+00 0.000+00 0.000+00 0.000+00 5.505+04 0.000+00 0.000+00 6.864−03 0.000+00 0.000+00 6.317+04 0.000+00 0.000+00 1.894−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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35
Table 12 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
3.725+03 1.559+03 1.377+03 3.869+01 3.808+01 3.792+01 3.770+01 3.765+01 3.763+01 2.620+01 2.606+01 2.602+01 2.597+01 2.595+01 2.595+01 2.682+03 2.185+03 3.909+01 3.848+01 3.831+01 3.808+01 3.803+01 3.802+01 3.799+01 2.639+01 2.624+01 2.620+01 2.615+01 2.614+01 2.613+01 2.613+01 2.613+01 1.180+04 3.967+01 3.904+01 3.886+01 3.863+01 3.858+01 3.857+01 3.854+01 2.665+01 2.650+01 2.646+01 2.641+01 2.640+01 2.639+01 2.639+01 2.639+01 3.980+01 3.917+01 3.899+01 3.876+01 3.871+01 3.869+01 3.867+01 2.671+01 2.656+01 2.652+01 2.647+01 2.645+01 2.645+01 2.644+01 2.644+01 2.644+01 2.440+03 1.912+03 1.476+03 1.402+03 1.386+03 8.119+01 7.985+01 7.948+01 7.899+01 7.887+01 7.884+01
0.000+00 3.727+07 0.000+00 1.801+11 0.000+00 0.000+00 1.366+12 0.000+00 0.000+00 8.751+10 0.000+00 0.000+00 6.732+11 0.000+00 0.000+00 1.461+06 1.627+07 3.754+11 0.000+00 0.000+00 2.745+11 1.639+12 0.000+00 0.000+00 1.812+11 0.000+00 0.000+00 1.339+11 8.025+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.759+10 9.093+09 0.000+00 0.000+00 3.027+12 0.000+00 0.000+00 4.187+10 3.907+09 0.000+00 0.000+00 1.000+12 0.000+00 0.000+00 0.000+00 0.000+00 8.349+10 0.000+00 0.000+00 2.152+11 3.232+12 0.000+00 0.000+00 3.584+10 0.000+00 0.000+00 7.082+10 1.066+12 0.000+00 0.000+00 5.056+07 1.056+08 0.000+00 0.000+00 0.000+00 0.000+00 1.618+11 1.560+11 0.000+00 0.000+00 0.000+00
0.000+00 2.717−02 0.000+00 4.041−02 0.000+00 0.000+00 5.822−01 0.000+00 0.000+00 9.007−03 0.000+00 0.000+00 1.361−01 0.000+00 0.000+00 1.575−03 1.747−02 4.300−02 0.000+00 0.000+00 5.967−02 5.332−01 0.000+00 0.000+00 9.457−03 0.000+00 0.000+00 1.372−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.115−02 2.059−03 0.000+00 0.000+00 1.013+00 0.000+00 0.000+00 2.205−03 4.101−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.269−02 0.000+00 0.000+00 4.831−02 9.659−01 0.000+00 0.000+00 2.519−03 0.000+00 0.000+00 7.428−03 1.490−01 0.000+00 0.000+00 4.513−02 1.158−01 0.000+00 0.000+00 0.000+00 0.000+00 1.546−01 2.954−01 0.000+00 0.000+00 0.000+00
0.000+00 2.789−01 0.000+00 1.029−02 0.000+00 0.000+00 1.445−01 0.000+00 0.000+00 1.554−03 0.000+00 0.000+00 2.327−02 0.000+00 0.000+00 5.562−02 5.027−01 2.214−02 0.000+00 0.000+00 2.993−02 2.670−01 0.000+00 0.000+00 3.286−03 0.000+00 0.000+00 4.726−03 4.244−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.730−03 1.054−03 0.000+00 0.000+00 5.142−01 0.000+00 0.000+00 7.694−04 1.429−04 0.000+00 0.000+00 5.445−02 0.000+00 0.000+00 0.000+00 0.000+00 9.772−03 0.000+00 0.000+00 3.692−02 7.377−01 0.000+00 0.000+00 1.320−03 0.000+00 0.000+00 3.881−03 7.785−02 0.000+00 0.000+00 7.251−01 1.458+00 0.000+00 0.000+00 0.000+00 0.000+00 8.129−02 1.546−01 0.000+00 0.000+00 0.000+00
4.114−02 0.000+00 0.000+00 0.000+00 0.000+00 1.493+08 0.000+00 0.000+00 5.585+08 0.000+00 0.000+00 8.486+07 0.000+00 0.000+00 6.227+06 0.000+00 0.000+00 0.000+00 2.973+08 1.480+08 0.000+00 0.000+00 1.544+08 6.968+08 0.000+00 1.649+08 8.292+07 0.000+00 0.000+00 1.277+06 6.087+06 0.000+00 1.872−05 5.199+07 0.000+00 0.000+00 9.476+07 2.707+07 0.000+00 0.000+00 3.158+07 0.000+00 0.000+00 4.554+07 1.306+07 0.000+00 0.000+00 1.185+09 7.806+07 0.000+00 0.000+00 4.045+07 1.078+08 0.000+00 0.000+00 4.733+07 0.000+00 0.000+00 1.936+07 5.184+07 0.000+00 0.000+00 1.315+08 1.314+09 0.000+00 0.000+00 3.865+01 5.017+01 0.000+00 0.000+00 0.000+00 0.000+00 6.772+07 6.779+07 0.000+00
1.737+02 0.000+00 0.000+00 0.000+00 1.877+02 5.820+03 0.000+00 0.000+00 0.000+00 0.000+00 2.251+02 4.079+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.595+04 1.325+03 0.000+00 0.000+00 4.119+01 0.000+00 0.000+00 1.231+04 1.587+03 0.000+00 0.000+00 1.981+01 0.000+00 0.000+00 6.552+00 2.052−01 0.000+00 0.000+00 4.915+02 3.821+02 0.000+00 0.000+00 1.224−01 0.000+00 0.000+00 5.068+02 2.280+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.449+03 1.622+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.081+03 1.673+03 0.000+00 0.000+00 3.692+01 0.000+00 0.000+00 0.000+00 1.099−04 0.000+00 0.000+00 2.243+01 0.000+00 0.000+00 2.257−01 0.000+00 0.000+00
0.000+00 6.750−05 8.985−04 0.000+00 0.000+00 0.000+00 4.237+03 3.012+04 0.000+00 0.000+00 0.000+00 0.000+00 4.394+03 3.130+04 0.000+00 0.000+00 4.873−04 2.716+04 0.000+00 0.000+00 0.000+00 1.621+05 0.000+00 0.000+00 2.878+04 0.000+00 0.000+00 0.000+00 1.679+05 0.000+00 0.000+00 2.266−02 0.000+00 0.000+00 2.835+02 0.000+00 0.000+00 0.000+00 5.339+04 6.854+04 0.000+00 2.641+02 0.000+00 0.000+00 0.000+00 3.762+04 4.838+04 0.000+00 0.000+00 3.063+03 7.878+03 0.000+00 0.000+00 0.000+00 4.672+05 0.000+00 2.856+03 7.313+03 0.000+00 0.000+00 0.000+00 3.291+05 0.000+00 0.000+00 0.000+00 3.186−03 0.000+00 0.000+00 1.850−11 0.000+00 0.000+00 2.727+03 0.000+00 0.000+00 1.044−04
(continued on next page)
36
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 12 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
8.845+03 3.732+03 3.293+03 3.206+03 8.399+01 8.255+01 8.216+01 8.163+01 8.151+01 8.148+01 6.457+03 5.246+03 5.028+03 4.614+03 8.479+01 8.333+01 8.293+01 8.239+01 8.227+01 8.223+01 8.217+01 8.217+01 2.798+04 2.273+04 1.617+04 8.592+01 8.442+01 8.401+01 8.345+01 8.333+01 8.329+01 8.323+01 8.323+01 1.212+05 3.830+04 8.618+01 8.467+01 8.426+01 8.370+01 8.358+01 8.354+01 8.348+01 8.348+01 8.344+01 5.600+04 8.625+01 8.473+01 8.432+01 8.376+01 8.363+01 8.360+01 8.354+01 8.354+01 8.350+01 8.444+01 8.389+01 8.376+01 8.373+01 8.366+01 8.366+01 8.362+01 4.824+03 3.772+03 2.909+03 2.762+03 2.727+03 1.730+04 7.326+03 6.460+03 6.272+03 1.271+04 1.031+04 9.839+03 9.027+03 9.020+03
0.000+00 1.158+07 0.000+00 0.000+00 6.203+10 0.000+00 0.000+00 2.830+11 0.000+00 0.000+00 4.466+05 5.010+06 0.000+00 0.000+00 1.290+11 0.000+00 0.000+00 5.734+10 3.418+11 0.000+00 0.000+00 0.000+00 0.000+00 3.589+04 0.000+00 0.000+00 5.181+10 4.864+09 0.000+00 0.000+00 5.660+11 0.000+00 0.000+00 1.690+01 8.044+03 0.000+00 0.000+00 4.458+10 0.000+00 0.000+00 4.042+10 6.057+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.225+10 5.687+08 0.000+00 0.000+00 9.628+11 0.000+00 0.000+00 0.000+00 1.151+10 0.000+00 0.000+00 3.557+10 9.970+11 1.643+07 3.452+07 0.000+00 0.000+00 0.000+00 0.000+00 4.187+06 0.000+00 0.000+00 1.602+05 1.804+06 0.000+00 0.000+00 0.000+00
0.000+00 4.839−02 0.000+00 0.000+00 6.560−02 0.000+00 0.000+00 5.655−01 0.000+00 0.000+00 2.791−03 3.101−02 0.000+00 0.000+00 6.953−02 0.000+00 0.000+00 5.835−02 5.201−01 0.000+00 0.000+00 0.000+00 0.000+00 4.170−03 0.000+00 0.000+00 2.768−02 5.146−03 0.000+00 0.000+00 8.831−01 0.000+00 0.000+00 3.719−05 2.358−03 0.000+00 0.000+00 3.163−02 0.000+00 0.000+00 4.230−02 8.438−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.594−03 5.964−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.079−03 0.000+00 0.000+00 3.733−02 1.306+00 5.732−02 1.473−01 0.000+00 0.000+00 0.000+00 0.000+00 6.738−02 0.000+00 0.000+00 3.879−03 4.313−02 0.000+00 0.000+00 0.000+00
0.000+00 1.189+00 0.000+00 0.000+00 3.627−02 0.000+00 0.000+00 3.039−01 0.000+00 0.000+00 2.373−01 2.142+00 0.000+00 0.000+00 7.763−02 0.000+00 0.000+00 6.331−02 5.635−01 0.000+00 0.000+00 0.000+00 0.000+00 1.248+00 0.000+00 0.000+00 3.077−02 5.693−03 0.000+00 0.000+00 9.686−01 0.000+00 0.000+00 8.899−02 1.784+00 0.000+00 0.000+00 5.265−02 0.000+00 0.000+00 6.979−02 1.391+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.422−02 9.852−04 0.000+00 0.000+00 2.216+00 0.000+00 0.000+00 0.000+00 2.003−02 0.000+00 0.000+00 8.225−02 2.877+00 1.821+00 3.657+00 0.000+00 0.000+00 0.000+00 0.000+00 3.250+00 0.000+00 0.000+00 6.491−01 5.856+00 0.000+00 0.000+00 0.000+00
6.130−03 0.000+00 0.000+00 3.805−01 0.000+00 0.000+00 2.647+07 0.000+00 0.000+00 8.867+07 0.000+00 0.000+00 1.142−02 7.921−02 0.000+00 5.278+07 2.629+07 0.000+00 0.000+00 2.471+07 1.114+08 0.000+00 4.010−06 0.000+00 0.000+00 1.604+07 0.000+00 0.000+00 2.120+07 6.052+06 0.000+00 0.000+00 1.037+08 0.000+00 0.000+00 2.406+07 0.000+00 0.000+00 9.059+06 2.414+07 0.000+00 0.000+00 1.140+07 1.143+08 3.199−08 0.000+00 5.684+06 7.950+05 0.000+00 0.000+00 1.488+07 1.860+06 0.000+00 0.000+00 4.780+06 0.000+00 0.000+00 2.475+06 1.547+07 0.000+00 0.000+00 0.000+00 0.000+00 8.896+00 1.156+01 0.000+00 1.347−03 0.000+00 0.000+00 1.295−01 0.000+00 0.000+00 3.886−03 2.696−02 0.000+00
1.298+01 0.000+00 0.000+00 0.000+00 0.000+00 7.036+00 6.324+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.092−07 0.000+00 0.000+00 1.524+03 4.978+01 0.000+00 0.000+00 1.026+00 0.000+00 0.000+00 4.921−01 0.000+00 0.000+00 2.227−02 0.000+00 0.000+00 2.351+01 5.606+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.501+02 7.770+01 0.000+00 0.000+00 1.435+00 0.000+00 6.579−02 0.000+00 0.000+00 1.218−03 0.000+00 0.000+00 3.417+01 8.021+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.178+01 8.035+01 0.000+00 0.000+00 0.000+00 0.000+00 8.185−06 0.000+00 0.000+00 1.735+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.653−08 0.000+00 0.000+00
0.000+00 3.666−06 4.897−05 0.000+00 0.000+00 0.000+00 0.000+00 1.874+02 1.328+03 0.000+00 0.000+00 2.604−05 0.000+00 0.000+00 1.983+03 0.000+00 0.000+00 0.000+00 7.226+03 0.000+00 0.000+00 1.392−04 0.000+00 1.824−09 1.286−08 0.000+00 3.214+01 0.000+00 0.000+00 0.000+00 2.142+03 2.744+03 0.000+00 0.000+00 1.186−09 0.000+00 3.468+02 8.997+02 0.000+00 0.000+00 0.000+00 1.880+04 0.000+00 0.000+00 0.000+00 7.934−08 0.000+00 0.000+00 4.599+01 0.000+00 0.000+00 0.000+00 9.204+03 4.818+03 0.000+00 7.919+01 3.556+02 0.000+00 0.000+00 0.000+00 4.448+04 0.000+00 2.677−04 0.000+00 0.000+00 1.185−12 0.000+00 3.441−07 4.603−06 0.000+00 0.000+00 2.428−06 0.000+00 0.000+00 9.657−16
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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37
Table 12 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
5.466+04 4.359+04 3.117+04 3.108+04 2.152+05 7.250+04 7.206+04 5.165+04 1.093+05 1.083+05 6.796+04 1.162+07 1.796+05 1.824+05
0.000+00 1.818+04 0.000+00 0.000+00 1.077+01 4.233+03 0.000+00 0.000+00 0.000+00 7.140+02 0.000+00 2.137−05 1.625+02 0.000+00
0.000+00 7.766−03 0.000+00 0.000+00 7.480−05 4.448−03 0.000+00 0.000+00 0.000+00 1.675−03 0.000+00 4.330−07 9.821−04 0.000+00
0.000+00 4.458+00 0.000+00 0.000+00 3.180−01 6.370+00 0.000+00 0.000+00 0.000+00 3.583+00 0.000+00 1.326−01 4.646+00 0.000+00
1.012−06 0.000+00 0.000+00 2.383−05 0.000+00 0.000+00 3.948−08 2.089−06 1.101−08 0.000+00 0.000+00 0.000+00 0.000+00 2.781−10
6.602−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.776−11 0.000+00 8.839−03 0.000+00 0.000+00 0.000+00 0.000+00 1.974−03
0.000+00 2.512−10 1.725−09 0.000+00 0.000+00 1.742−10 0.000+00 0.000+00 0.000+00 4.061−12 2.186−11 0.000+00 1.573−12 0.000+00
38
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 13 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Mn XXIII. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.659+02 2.064+02 1.174+01 1.160+01 1.155+01 1.150+01 1.149+01 8.733+00 8.700+00 8.690+00 8.678+00 8.675+00 8.674+00 7.814+00 7.801+00 7.797+00 7.792+00 7.791+00 7.790+00 9.222+02 1.228+01 1.213+01 1.208+01 1.202+01 1.201+01 9.029+00 8.995+00 8.984+00 8.971+00 8.967+00 8.966+00 8.051+00 8.037+00 8.033+00 8.027+00 8.026+00 8.026+00 1.245+01 1.229+01 1.224+01 1.218+01 1.217+01 9.119+00 9.083+00 9.072+00 9.059+00 9.055+00 9.054+00 9.053+00 8.122+00 8.108+00 8.103+00 8.098+00 8.096+00 8.096+00 8.095+00 8.095+00 9.583+02 7.330+02 5.698+02 5.387+02 3.410+01 3.361+01 3.346+01 3.327+01 3.323+01 3.322+01 2.337+01 2.325+01 2.322+01 2.317+01 2.316+01 2.316+01
1.744+09 3.783+09 0.000+00 6.302+12 6.110+12 0.000+00 0.000+00 0.000+00 2.774+12 2.716+12 0.000+00 0.000+00 0.000+00 0.000+00 1.432+12 1.407+12 0.000+00 0.000+00 0.000+00 0.000+00 7.619+11 0.000+00 0.000+00 1.552+13 0.000+00 3.058+11 0.000+00 0.000+00 5.060+12 0.000+00 0.000+00 1.537+11 0.000+00 0.000+00 2.335+12 0.000+00 0.000+00 1.600+12 0.000+00 0.000+00 3.061+12 1.838+13 6.377+11 0.000+00 0.000+00 9.873+11 5.954+12 0.000+00 0.000+00 3.176+11 0.000+00 0.000+00 4.531+11 2.738+12 0.000+00 0.000+00 0.000+00 2.272+08 5.122+08 0.000+00 0.000+00 0.000+00 8.254+11 7.957+11 0.000+00 0.000+00 0.000+00 0.000+00 4.524+11 4.400+11 0.000+00 0.000+00 0.000+00
1.849−02 4.833−02 0.000+00 1.271−01 2.446−01 0.000+00 0.000+00 0.000+00 3.148−02 6.150−02 0.000+00 0.000+00 0.000+00 0.000+00 1.307−02 2.565−02 0.000+00 0.000+00 0.000+00 0.000+00 1.723−02 0.000+00 0.000+00 6.725−01 0.000+00 3.737−03 0.000+00 0.000+00 1.221−01 0.000+00 0.000+00 1.493−03 0.000+00 0.000+00 4.510−02 0.000+00 0.000+00 1.858−02 0.000+00 0.000+00 6.810−02 6.117−01 3.975−03 0.000+00 0.000+00 1.214−02 1.098−01 0.000+00 0.000+00 1.570−03 0.000+00 0.000+00 4.454−03 4.036−02 0.000+00 0.000+00 0.000+00 3.128−02 8.250−02 0.000+00 0.000+00 0.000+00 1.398−01 2.670−01 0.000+00 0.000+00 0.000+00 0.000+00 3.668−02 7.112−02 0.000+00 0.000+00 0.000+00
3.238−02 6.568−02 0.000+00 9.703−03 1.861−02 0.000+00 0.000+00 0.000+00 1.803−03 3.519−03 0.000+00 0.000+00 0.000+00 0.000+00 6.712−04 1.317−03 0.000+00 0.000+00 0.000+00 0.000+00 1.393−03 0.000+00 0.000+00 5.323−02 0.000+00 2.222−04 0.000+00 0.000+00 7.212−03 0.000+00 0.000+00 7.917−05 0.000+00 0.000+00 2.384−03 0.000+00 0.000+00 3.046−03 0.000+00 0.000+00 1.092−02 9.799−02 4.773−04 0.000+00 0.000+00 1.449−03 1.309−02 0.000+00 0.000+00 1.679−04 0.000+00 0.000+00 4.750−04 4.303−03 0.000+00 0.000+00 0.000+00 1.974−01 3.982−01 0.000+00 0.000+00 0.000+00 3.093−02 5.882−02 0.000+00 0.000+00 0.000+00 0.000+00 5.616−03 1.087−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 9.246+09 9.284+09 0.000+00 0.000+00 0.000+00 1.242+09 1.269+09 0.000+00 0.000+00 0.000+00 0.000+00 3.171+08 3.286+08 0.000+00 1.001+00 0.000+00 0.000+00 1.839+09 0.000+00 0.000+00 0.000+00 0.000+00 8.000+08 0.000+00 0.000+00 7.110+09 0.000+00 0.000+00 4.309+08 0.000+00 0.000+00 4.760+09 0.000+00 3.645+09 1.813+09 0.000+00 0.000+00 0.000+00 1.545+09 7.779+08 0.000+00 0.000+00 2.029+09 9.097+09 0.000+00 8.023+08 4.058+08 0.000+00 0.000+00 1.358+09 6.097+09 0.000+00 0.000+00 0.000+00 2.637+02 3.512+02 0.000+00 0.000+00 0.000+00 6.371+08 6.384+08 0.000+00 0.000+00 0.000+00 0.000+00 2.137+08 2.161+08 0.000+00
0.000+00 0.000+00 9.965+04 0.000+00 0.000+00 5.581+03 0.000+00 8.412+04 0.000+00 0.000+00 3.268+03 0.000+00 0.000+00 5.508+04 0.000+00 0.000+00 1.831+03 0.000+00 0.000+00 1.142+04 0.000+00 2.317+04 1.608+05 0.000+00 0.000+00 0.000+00 1.816+04 8.220+04 0.000+00 0.000+00 0.000+00 0.000+00 1.174+04 4.540+04 0.000+00 0.000+00 0.000+00 0.000+00 6.005+05 1.624+05 0.000+00 0.000+00 0.000+00 3.501+05 1.274+05 0.000+00 0.000+00 1.860+03 0.000+00 0.000+00 2.019+05 8.105+04 0.000+00 0.000+00 1.635+03 0.000+00 0.000+00 0.000+00 0.000+00 3.752−03 0.000+00 1.010+03 0.000+00 0.000+00 2.393+01 0.000+00 0.000+00 1.260+03 0.000+00 0.000+00 3.174+01 0.000+00 0.000+00
0.000+00 9.787+00 0.000+00 0.000+00 5.056+06 0.000+00 0.000+00 0.000+00 0.000+00 3.968+06 0.000+00 0.000+00 2.145+00 0.000+00 0.000+00 2.552+06 0.000+00 0.000+00 1.919+00 0.000+00 0.000+00 0.000+00 0.000+00 4.709+05 3.372+06 0.000+00 0.000+00 0.000+00 2.751+05 1.976+06 0.000+00 0.000+00 0.000+00 0.000+00 1.584+05 1.139+06 0.000+00 1.145+06 0.000+00 0.000+00 0.000+00 1.773+07 8.509+05 0.000+00 0.000+00 0.000+00 1.035+07 0.000+00 0.000+00 5.342+05 0.000+00 0.000+00 0.000+00 5.947+06 0.000+00 0.000+00 2.727−01 0.000+00 1.052−01 0.000+00 0.000+00 0.000+00 0.000+00 7.853+04 0.000+00 0.000+00 1.165−02 0.000+00 0.000+00 9.012+04 0.000+00 0.000+00 3.200−03
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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39
Table 13 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
3.118+03 1.405+03 1.230+03 3.536+01 3.483+01 3.467+01 3.447+01 3.442+01 3.441+01 2.396+01 2.383+01 2.379+01 2.375+01 2.374+01 2.373+01 2.559+03 2.032+03 3.576+01 3.522+01 3.506+01 3.486+01 3.481+01 3.479+01 3.477+01 2.414+01 2.402+01 2.398+01 2.393+01 2.392+01 2.392+01 2.391+01 2.391+01 9.875+03 3.627+01 3.571+01 3.554+01 3.534+01 3.528+01 3.527+01 3.525+01 2.437+01 2.425+01 2.420+01 2.416+01 2.414+01 2.414+01 2.413+01 2.413+01 3.640+01 3.584+01 3.567+01 3.547+01 3.541+01 3.540+01 3.537+01 2.443+01 2.430+01 2.426+01 2.422+01 2.420+01 2.420+01 2.419+01 2.419+01 2.419+01 2.328+03 1.771+03 1.375+03 1.299+03 1.285+03 7.431+01 7.313+01 7.276+01 7.232+01 7.221+01 7.218+01
0.000+00 4.655+07 0.000+00 2.137+11 0.000+00 0.000+00 1.632+12 0.000+00 0.000+00 1.039+11 0.000+00 0.000+00 8.045+11 0.000+00 0.000+00 1.538+06 1.850+07 4.472+11 0.000+00 0.000+00 3.281+11 1.959+12 0.000+00 0.000+00 2.160+11 0.000+00 0.000+00 1.599+11 9.585+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.169+11 1.082+10 0.000+00 0.000+00 3.617+12 0.000+00 0.000+00 5.017+10 4.651+09 0.000+00 0.000+00 1.195+12 0.000+00 0.000+00 0.000+00 0.000+00 9.956+10 0.000+00 0.000+00 2.571+11 3.861+12 0.000+00 0.000+00 4.274+10 0.000+00 0.000+00 8.456+10 1.274+12 0.000+00 0.000+00 5.327+07 1.217+08 0.000+00 0.000+00 0.000+00 0.000+00 1.942+11 1.866+11 0.000+00 0.000+00 0.000+00
0.000+00 2.756−02 0.000+00 4.005−02 0.000+00 0.000+00 5.816−01 0.000+00 0.000+00 8.944−03 0.000+00 0.000+00 1.360−01 0.000+00 0.000+00 1.509−03 1.718−02 4.288−02 0.000+00 0.000+00 5.975−02 5.336−01 0.000+00 0.000+00 9.437−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.118−02 2.049−03 0.000+00 0.000+00 1.012+00 0.000+00 0.000+00 2.210−03 4.085−04 0.000+00 0.000+00 1.567−01 0.000+00 0.000+00 0.000+00 0.000+00 1.266−02 0.000+00 0.000+00 4.830−02 9.657−01 0.000+00 0.000+00 2.515−03 0.000+00 0.000+00 7.424−03 1.490−01 0.000+00 0.000+00 4.327−02 1.145−01 0.000+00 0.000+00 0.000+00 0.000+00 1.557−01 2.962−01 0.000+00 0.000+00 0.000+00
0.000+00 2.550−01 0.000+00 9.324−03 0.000+00 0.000+00 1.320−01 0.000+00 0.000+00 1.411−03 0.000+00 0.000+00 2.127−02 0.000+00 0.000+00 5.085−02 4.597−01 2.019−02 0.000+00 0.000+00 2.743−02 2.446−01 0.000+00 0.000+00 3.000−03 0.000+00 0.000+00 4.326−03 3.884−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.257−03 9.592−04 0.000+00 0.000+00 4.701−01 0.000+00 0.000+00 7.057−04 1.302−04 0.000+00 0.000+00 4.980−02 0.000+00 0.000+00 0.000+00 0.000+00 8.921−03 0.000+00 0.000+00 3.378−02 6.748−01 0.000+00 0.000+00 1.205−03 0.000+00 0.000+00 3.549−03 7.121−02 0.000+00 0.000+00 6.631−01 1.334+00 0.000+00 0.000+00 0.000+00 0.000+00 7.495−02 1.419−01 0.000+00 0.000+00 0.000+00
8.383−02 0.000+00 0.000+00 0.000+00 0.000+00 1.950+08 0.000+00 0.000+00 7.305+08 0.000+00 0.000+00 1.110+08 0.000+00 0.000+00 8.253+06 0.000+00 0.000+00 0.000+00 3.882+08 1.931+08 0.000+00 0.000+00 2.013+08 9.089+08 0.000+00 2.151+08 1.082+08 0.000+00 0.000+00 1.642+06 7.871+06 0.000+00 3.818−05 6.779+07 0.000+00 0.000+00 1.238+08 3.535+07 0.000+00 0.000+00 4.119+07 0.000+00 0.000+00 5.947+07 1.706+07 0.000+00 0.000+00 1.547+09 1.018+08 0.000+00 0.000+00 5.281+07 1.408+08 0.000+00 0.000+00 6.174+07 0.000+00 0.000+00 2.527+07 6.767+07 0.000+00 0.000+00 1.717+08 1.715+09 0.000+00 0.000+00 4.593+01 6.137+01 0.000+00 0.000+00 0.000+00 0.000+00 8.831+07 8.842+07 0.000+00
2.962+02 0.000+00 0.000+00 0.000+00 2.931+02 9.090+03 0.000+00 0.000+00 0.000+00 0.000+00 3.515+02 6.369+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.486+04 2.063+03 0.000+00 0.000+00 6.418+01 0.000+00 0.000+00 1.920+04 2.471+03 0.000+00 0.000+00 3.084+01 0.000+00 0.000+00 1.119+01 3.198−01 0.000+00 0.000+00 7.672+02 5.969+02 0.000+00 0.000+00 1.901−01 0.000+00 0.000+00 7.910+02 3.562+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.262+03 2.529+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.688+03 2.609+03 0.000+00 0.000+00 5.758+01 0.000+00 0.000+00 0.000+00 1.616−04 0.000+00 0.000+00 3.494+01 0.000+00 0.000+00 3.535−01 0.000+00 0.000+00
0.000+00 1.037−04 1.445−03 0.000+00 0.000+00 0.000+00 6.053+03 4.302+04 0.000+00 0.000+00 0.000+00 0.000+00 6.278+03 4.472+04 0.000+00 0.000+00 6.405−04 3.868+04 0.000+00 0.000+00 0.000+00 2.313+05 0.000+00 0.000+00 4.099+04 0.000+00 0.000+00 0.000+00 2.395+05 0.000+00 0.000+00 3.861−02 0.000+00 0.000+00 4.059+02 0.000+00 0.000+00 0.000+00 7.625+04 9.791+04 0.000+00 3.783+02 0.000+00 0.000+00 0.000+00 5.372+04 6.911+04 0.000+00 0.000+00 4.390+03 1.123+04 0.000+00 0.000+00 0.000+00 6.668+05 0.000+00 4.095+03 1.042+04 0.000+00 0.000+00 0.000+00 4.696+05 0.000+00 0.000+00 0.000+00 4.284−03 0.000+00 0.000+00 2.945−11 0.000+00 0.000+00 3.892+03 0.000+00 0.000+00 1.775−04
(continued on next page)
40
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 13 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
7.402+03 3.362+03 2.940+03 2.867+03 7.676+01 7.550+01 7.511+01 7.464+01 7.452+01 7.450+01 6.161+03 4.877+03 4.679+03 4.254+03 7.756+01 7.628+01 7.588+01 7.540+01 7.528+01 7.525+01 7.519+01 7.519+01 2.341+04 1.945+04 1.374+04 7.855+01 7.723+01 7.682+01 7.634+01 7.621+01 7.618+01 7.612+01 7.612+01 1.149+05 3.329+04 7.882+01 7.749+01 7.708+01 7.659+01 7.646+01 7.643+01 7.637+01 7.637+01 7.633+01 4.686+04 7.887+01 7.754+01 7.713+01 7.664+01 7.651+01 7.648+01 7.642+01 7.642+01 7.638+01 7.725+01 7.676+01 7.664+01 7.661+01 7.654+01 7.654+01 7.650+01 4.601+03 3.492+03 2.711+03 2.559+03 2.528+03 1.448+04 6.599+03 5.767+03 5.608+03 1.212+04 9.584+03 9.154+03 8.322+03 8.315+03
0.000+00 1.449+07 0.000+00 0.000+00 7.365+10 0.000+00 0.000+00 3.381+11 0.000+00 0.000+00 4.700+05 5.703+06 0.000+00 0.000+00 1.538+11 0.000+00 0.000+00 6.858+10 4.085+11 0.000+00 0.000+00 0.000+00 0.000+00 5.242+04 0.000+00 0.000+00 6.206+10 5.792+09 0.000+00 0.000+00 6.762+11 0.000+00 0.000+00 1.811+01 1.120+04 0.000+00 0.000+00 5.317+10 0.000+00 0.000+00 4.829+10 7.236+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.468+10 6.794+08 0.000+00 0.000+00 1.150+12 0.000+00 0.000+00 0.000+00 1.377+10 0.000+00 0.000+00 4.249+10 1.191+12 1.731+07 3.982+07 0.000+00 0.000+00 0.000+00 0.000+00 5.240+06 0.000+00 0.000+00 1.687+05 2.055+06 0.000+00 0.000+00 0.000+00
0.000+00 4.912−02 0.000+00 0.000+00 6.505−02 0.000+00 0.000+00 5.648−01 0.000+00 0.000+00 2.675−03 3.051−02 0.000+00 0.000+00 6.934−02 0.000+00 0.000+00 5.846−02 5.206−01 0.000+00 0.000+00 0.000+00 0.000+00 4.458−03 0.000+00 0.000+00 2.775−02 5.125−03 0.000+00 0.000+00 8.826−01 0.000+00 0.000+00 3.585−05 2.481−03 0.000+00 0.000+00 3.157−02 0.000+00 0.000+00 4.229−02 8.435−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.615−03 5.962−04 0.000+00 0.000+00 1.343+00 0.000+00 0.000+00 0.000+00 9.090−03 0.000+00 0.000+00 3.732−02 1.306+00 5.496−02 1.455−01 0.000+00 0.000+00 0.000+00 0.000+00 6.841−02 0.000+00 0.000+00 3.718−03 4.244−02 0.000+00 0.000+00 0.000+00
0.000+00 1.087+00 0.000+00 0.000+00 3.288−02 0.000+00 0.000+00 2.776−01 0.000+00 0.000+00 2.170−01 1.960+00 0.000+00 0.000+00 7.083−02 0.000+00 0.000+00 5.805−02 5.161−01 0.000+00 0.000+00 0.000+00 0.000+00 1.142+00 0.000+00 0.000+00 2.822−02 5.184−03 0.000+00 0.000+00 8.854−01 0.000+00 0.000+00 8.139−02 1.632+00 0.000+00 0.000+00 4.806−02 0.000+00 0.000+00 6.385−02 1.273+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.304−02 9.011−04 0.000+00 0.000+00 2.027+00 0.000+00 0.000+00 0.000+00 1.835−02 0.000+00 0.000+00 7.524−02 2.632+00 1.665+00 3.346+00 0.000+00 0.000+00 0.000+00 0.000+00 2.972+00 0.000+00 0.000+00 5.936−01 5.356+00 0.000+00 0.000+00 0.000+00
1.249−02 0.000+00 0.000+00 5.569−01 0.000+00 0.000+00 3.458+07 0.000+00 0.000+00 1.160+08 0.000+00 0.000+00 1.370−02 9.950−02 0.000+00 6.893+07 3.432+07 0.000+00 0.000+00 3.224+07 1.454+08 0.000+00 8.184−06 0.000+00 0.000+00 2.092+07 0.000+00 0.000+00 2.768+07 7.904+06 0.000+00 0.000+00 1.356+08 0.000+00 0.000+00 3.140+07 0.000+00 0.000+00 1.183+07 3.152+07 0.000+00 0.000+00 1.489+07 1.493+08 6.518−08 0.000+00 7.432+06 1.037+06 0.000+00 0.000+00 1.942+07 2.428+06 0.000+00 0.000+00 6.239+06 0.000+00 0.000+00 3.230+06 2.020+07 0.000+00 0.000+00 0.000+00 0.000+00 1.058+01 1.416+01 0.000+00 2.744−03 0.000+00 0.000+00 1.895−01 0.000+00 0.000+00 4.664−03 3.389−02 0.000+00
2.215+01 0.000+00 0.000+00 0.000+00 0.000+00 1.099+01 9.876+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.050−06 0.000+00 0.000+00 2.376+03 7.756+01 0.000+00 0.000+00 1.600+00 0.000+00 0.000+00 8.404−01 0.000+00 0.000+00 3.472−02 0.000+00 0.000+00 3.671+01 8.757+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.344+02 1.212+02 0.000+00 0.000+00 2.239+00 0.000+00 1.122−01 0.000+00 0.000+00 1.897−03 0.000+00 0.000+00 5.332+01 1.252+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.958+01 1.253+02 0.000+00 0.000+00 0.000+00 0.000+00 1.204−05 0.000+00 0.000+00 2.960+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.282−07 0.000+00 0.000+00
0.000+00 5.649−06 7.896−05 0.000+00 0.000+00 0.000+00 0.000+00 2.677+02 1.897+03 0.000+00 0.000+00 3.429−05 0.000+00 0.000+00 2.824+03 0.000+00 0.000+00 0.000+00 1.031+04 0.000+00 0.000+00 2.371−04 0.000+00 3.639−09 2.650−08 0.000+00 4.600+01 0.000+00 0.000+00 0.000+00 3.060+03 3.920+03 0.000+00 0.000+00 2.186−09 0.000+00 4.969+02 1.283+03 0.000+00 0.000+00 0.000+00 2.683+04 0.000+00 0.000+00 0.000+00 1.358−07 0.000+00 0.000+00 6.579+01 0.000+00 0.000+00 0.000+00 1.314+04 6.879+03 0.000+00 1.134+02 5.081+02 0.000+00 0.000+00 0.000+00 6.348+04 0.000+00 3.604−04 0.000+00 0.000+00 1.888−12 0.000+00 5.308−07 7.430−06 0.000+00 0.000+00 3.200−06 0.000+00 0.000+00 1.584−15
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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41
Table 13 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
4.573+04 3.736+04 2.653+04 2.647+04 2.042+05 6.319+04 6.283+04 4.451+04 9.151+04 9.075+04 5.692+04 1.097+07 1.506+05 1.527+05
0.000+00 2.640+04 0.000+00 0.000+00 1.154+01 5.850+03 0.000+00 0.000+00 0.000+00 1.111+03 0.000+00 2.324−05 2.522+02 0.000+00
0.000+00 8.289−03 0.000+00 0.000+00 7.212−05 4.669−03 0.000+00 0.000+00 0.000+00 1.829−03 0.000+00 4.196−07 1.072−03 0.000+00
0.000+00 4.078+00 0.000+00 0.000+00 2.909−01 5.828+00 0.000+00 0.000+00 0.000+00 3.278+00 0.000+00 1.213−01 4.250+00 0.000+00
2.067−06 0.000+00 0.000+00 4.457−05 0.000+00 0.000+00 6.556−08 3.680−06 2.245−08 0.000+00 0.000+00 0.000+00 0.000+00 5.665−10
1.128−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.042−10 0.000+00 1.508−02 0.000+00 0.000+00 0.000+00 0.000+00 3.366−03
0.000+00 4.968−10 3.531−09 0.000+00 0.000+00 3.169−10 0.000+00 0.000+00 0.000+00 9.001−12 4.854−11 0.000+00 3.471−12 0.000+00
42
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 14 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Fe XXIV. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.542+02 1.916+02 1.079+01 1.066+01 1.062+01 1.058+01 1.056+01 8.026+00 7.997+00 7.987+00 7.976+00 7.973+00 7.972+00 7.181+00 7.170+00 7.166+00 7.161+00 7.160+00 7.160+00 7.777+02 1.127+01 1.113+01 1.109+01 1.103+01 1.102+01 8.288+00 8.257+00 8.246+00 8.234+00 8.231+00 8.230+00 7.390+00 7.378+00 7.373+00 7.369+00 7.367+00 7.367+00 1.143+01 1.129+01 1.124+01 1.119+01 1.118+01 8.377+00 8.345+00 8.334+00 8.322+00 8.319+00 8.318+00 8.317+00 7.461+00 7.449+00 7.444+00 7.439+00 7.438+00 7.438+00 7.437+00 7.437+00 9.157+02 6.791+02 5.316+02 4.997+02 3.133+01 3.089+01 3.074+01 3.058+01 3.053+01 3.052+01 2.147+01 2.137+01 2.133+01 2.129+01 2.128+01 2.128+01
1.832+09 4.346+09 0.000+00 7.491+12 7.244+12 0.000+00 0.000+00 0.000+00 3.294+12 3.219+12 0.000+00 0.000+00 0.000+00 0.000+00 1.700+12 1.667+12 0.000+00 0.000+00 0.000+00 0.000+00 8.972+11 0.000+00 0.000+00 1.840+13 0.000+00 3.604+11 0.000+00 0.000+00 6.003+12 0.000+00 0.000+00 1.813+11 0.000+00 0.000+00 2.769+12 0.000+00 0.000+00 1.892+12 0.000+00 0.000+00 3.626+12 2.177+13 7.548+11 0.000+00 0.000+00 1.169+12 7.051+12 0.000+00 0.000+00 3.760+11 0.000+00 0.000+00 5.361+11 3.242+12 0.000+00 0.000+00 0.000+00 2.389+08 5.913+08 0.000+00 0.000+00 0.000+00 9.824+11 9.440+11 0.000+00 0.000+00 0.000+00 0.000+00 5.378+11 5.220+11 0.000+00 0.000+00 0.000+00
1.775−02 4.783−02 0.000+00 1.277−01 2.450−01 0.000+00 0.000+00 0.000+00 3.158−02 6.156−02 0.000+00 0.000+00 0.000+00 0.000+00 1.310−02 2.567−02 0.000+00 0.000+00 0.000+00 0.000+00 1.708−02 0.000+00 0.000+00 6.719−01 0.000+00 3.711−03 0.000+00 0.000+00 1.220−01 0.000+00 0.000+00 1.485−03 0.000+00 0.000+00 4.509−02 0.000+00 0.000+00 1.855−02 0.000+00 0.000+00 6.812−02 6.117−01 3.970−03 0.000+00 0.000+00 1.213−02 1.097−01 0.000+00 0.000+00 1.569−03 0.000+00 0.000+00 4.448−03 4.033−02 0.000+00 0.000+00 0.000+00 3.004−02 8.178−02 0.000+00 0.000+00 0.000+00 1.406−01 2.675−01 0.000+00 0.000+00 0.000+00 0.000+00 3.682−02 7.121−02 0.000+00 0.000+00 0.000+00
2.970−02 6.033−02 0.000+00 8.968−03 1.714−02 0.000+00 0.000+00 0.000+00 1.663−03 3.237−03 0.000+00 0.000+00 0.000+00 0.000+00 6.183−04 1.211−03 0.000+00 0.000+00 0.000+00 0.000+00 1.267−03 0.000+00 0.000+00 4.882−02 0.000+00 2.025−04 0.000+00 0.000+00 6.617−03 0.000+00 0.000+00 7.224−05 0.000+00 0.000+00 2.188−03 0.000+00 0.000+00 2.792−03 0.000+00 0.000+00 1.004−02 9.005−02 4.379−04 0.000+00 0.000+00 1.330−03 1.202−02 0.000+00 0.000+00 1.541−04 0.000+00 0.000+00 4.357−04 3.950−03 0.000+00 0.000+00 0.000+00 1.811−01 3.657−01 0.000+00 0.000+00 0.000+00 2.859−02 5.414−02 0.000+00 0.000+00 0.000+00 0.000+00 5.180−03 1.000−02 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.189+10 1.194+10 0.000+00 0.000+00 0.000+00 1.589+09 1.626+09 0.000+00 0.000+00 0.000+00 0.000+00 4.037+08 4.200+08 0.000+00 1.979+00 0.000+00 0.000+00 2.375+09 0.000+00 0.000+00 0.000+00 0.000+00 1.034+09 0.000+00 0.000+00 9.177+09 0.000+00 0.000+00 5.580+08 0.000+00 0.000+00 6.143+09 0.000+00 4.703+09 2.337+09 0.000+00 0.000+00 0.000+00 1.991+09 1.003+09 0.000+00 0.000+00 2.618+09 1.174+10 0.000+00 1.034+09 5.236+08 0.000+00 0.000+00 1.753+09 7.864+09 0.000+00 0.000+00 0.000+00 3.143+02 4.311+02 0.000+00 0.000+00 0.000+00 8.210+08 8.229+08 0.000+00 0.000+00 0.000+00 0.000+00 2.747+08 2.781+08 0.000+00
0.000+00 0.000+00 1.520+05 0.000+00 0.000+00 8.511+03 0.000+00 1.283+05 0.000+00 0.000+00 4.981+03 0.000+00 0.000+00 8.399+04 0.000+00 0.000+00 2.789+03 0.000+00 0.000+00 1.904+04 0.000+00 3.550+04 2.465+05 0.000+00 0.000+00 0.000+00 2.782+04 1.260+05 0.000+00 0.000+00 0.000+00 0.000+00 1.798+04 6.962+04 0.000+00 0.000+00 0.000+00 0.000+00 9.181+05 2.476+05 0.000+00 0.000+00 0.000+00 5.353+05 1.942+05 0.000+00 0.000+00 2.846+03 0.000+00 0.000+00 3.086+05 1.236+05 0.000+00 0.000+00 2.502+03 0.000+00 0.000+00 0.000+00 0.000+00 5.458−03 0.000+00 1.543+03 0.000+00 0.000+00 3.664+01 0.000+00 0.000+00 1.925+03 0.000+00 0.000+00 4.856+01 0.000+00 0.000+00
0.000+00 1.305+01 0.000+00 0.000+00 7.093+06 0.000+00 0.000+00 0.000+00 0.000+00 5.567+06 0.000+00 0.000+00 3.566+00 0.000+00 0.000+00 3.580+06 0.000+00 0.000+00 3.194+00 0.000+00 0.000+00 0.000+00 0.000+00 6.626+05 4.747+06 0.000+00 0.000+00 0.000+00 3.870+05 2.782+06 0.000+00 0.000+00 0.000+00 0.000+00 2.228+05 1.604+06 0.000+00 1.606+06 0.000+00 0.000+00 0.000+00 2.487+07 1.194+06 0.000+00 0.000+00 0.000+00 1.451+07 0.000+00 0.000+00 7.498+05 0.000+00 0.000+00 0.000+00 8.339+06 0.000+00 0.000+00 4.538−01 0.000+00 1.414−01 0.000+00 0.000+00 0.000+00 0.000+00 1.104+05 0.000+00 0.000+00 1.936−02 0.000+00 0.000+00 1.266+05 0.000+00 0.000+00 5.296−03 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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43
Table 14 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
2.628+03 1.267+03 1.100+03 3.244+01 3.197+01 3.181+01 3.164+01 3.159+01 3.158+01 2.199+01 2.188+01 2.184+01 2.180+01 2.179+01 2.178+01 2.447+03 1.891+03 3.284+01 3.237+01 3.220+01 3.202+01 3.197+01 3.196+01 3.194+01 2.217+01 2.206+01 2.202+01 2.198+01 2.197+01 2.197+01 2.196+01 2.196+01 8.325+03 3.329+01 3.280+01 3.263+01 3.245+01 3.239+01 3.238+01 3.236+01 2.238+01 2.226+01 2.222+01 2.218+01 2.217+01 2.217+01 2.216+01 2.216+01 3.342+01 3.293+01 3.276+01 3.257+01 3.252+01 3.251+01 3.248+01 2.244+01 2.232+01 2.228+01 2.224+01 2.223+01 2.222+01 2.222+01 2.222+01 2.221+01 2.224+03 1.640+03 1.283+03 1.204+03 1.191+03 6.826+01 6.721+01 6.685+01 6.646+01 6.635+01 6.633+01
0.000+00 5.827+07 0.000+00 2.518+11 0.000+00 0.000+00 1.936+12 0.000+00 0.000+00 1.226+11 0.000+00 0.000+00 9.543+11 0.000+00 0.000+00 1.613+06 2.107+07 5.293+11 0.000+00 0.000+00 3.892+11 2.323+12 0.000+00 0.000+00 2.557+11 0.000+00 0.000+00 1.896+11 1.136+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.391+11 1.279+10 0.000+00 0.000+00 4.290+12 0.000+00 0.000+00 5.969+10 5.497+09 0.000+00 0.000+00 1.418+12 0.000+00 0.000+00 0.000+00 0.000+00 1.179+11 0.000+00 0.000+00 3.048+11 4.577+12 0.000+00 0.000+00 5.061+10 0.000+00 0.000+00 1.002+11 1.510+12 0.000+00 0.000+00 5.603+07 1.408+08 0.000+00 0.000+00 0.000+00 0.000+00 2.312+11 2.214+11 0.000+00 0.000+00 0.000+00
0.000+00 2.806−02 0.000+00 3.972−02 0.000+00 0.000+00 5.809−01 0.000+00 0.000+00 8.886−03 0.000+00 0.000+00 1.360−01 0.000+00 0.000+00 1.448−03 1.695−02 4.280−02 0.000+00 0.000+00 5.983−02 5.339−01 0.000+00 0.000+00 9.424−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.122−02 2.041−03 0.000+00 0.000+00 1.012+00 0.000+00 0.000+00 2.218−03 4.070−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.264−02 0.000+00 0.000+00 4.829−02 9.655−01 0.000+00 0.000+00 2.511−03 0.000+00 0.000+00 7.421−03 1.490−01 0.000+00 0.000+00 4.156−02 1.135−01 0.000+00 0.000+00 0.000+00 0.000+00 1.566−01 2.967−01 0.000+00 0.000+00 0.000+00
0.000+00 2.341−01 0.000+00 8.484−03 0.000+00 0.000+00 1.210−01 0.000+00 0.000+00 1.287−03 0.000+00 0.000+00 1.951−02 0.000+00 0.000+00 4.666−02 4.221−01 1.851−02 0.000+00 0.000+00 2.523−02 2.248−01 0.000+00 0.000+00 2.752−03 0.000+00 0.000+00 3.975−03 3.567−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.845−03 8.768−04 0.000+00 0.000+00 4.314−01 0.000+00 0.000+00 6.502−04 1.191−04 0.000+00 0.000+00 4.572−02 0.000+00 0.000+00 0.000+00 0.000+00 8.179−03 0.000+00 0.000+00 3.101−02 6.195−01 0.000+00 0.000+00 1.105−03 0.000+00 0.000+00 3.258−03 6.538−02 0.000+00 0.000+00 6.086−01 1.225+00 0.000+00 0.000+00 0.000+00 0.000+00 6.930−02 1.306−01 0.000+00 0.000+00 0.000+00
1.658−01 0.000+00 0.000+00 0.000+00 0.000+00 2.518+08 0.000+00 0.000+00 9.451+08 0.000+00 0.000+00 1.435+08 0.000+00 0.000+00 1.084+07 0.000+00 0.000+00 0.000+00 5.011+08 2.492+08 0.000+00 0.000+00 2.596+08 1.172+09 0.000+00 2.774+08 1.397+08 0.000+00 0.000+00 2.091+06 1.008+07 0.000+00 7.555−05 8.742+07 0.000+00 0.000+00 1.598+08 4.564+07 0.000+00 0.000+00 5.314+07 0.000+00 0.000+00 7.677+07 2.204+07 0.000+00 0.000+00 1.997+09 1.313+08 0.000+00 0.000+00 6.817+07 1.817+08 0.000+00 0.000+00 7.965+07 0.000+00 0.000+00 3.259+07 8.732+07 0.000+00 0.000+00 2.216+08 2.213+09 0.000+00 0.000+00 5.486+01 7.553+01 0.000+00 0.000+00 0.000+00 0.000+00 1.139+08 1.140+08 0.000+00
4.942+02 0.000+00 0.000+00 0.000+00 4.492+02 1.394+04 0.000+00 0.000+00 0.000+00 0.000+00 5.388+02 9.762+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.805+04 3.153+03 0.000+00 0.000+00 9.815+01 0.000+00 0.000+00 2.938+04 3.776+03 0.000+00 0.000+00 4.713+01 0.000+00 0.000+00 1.867+01 4.890−01 0.000+00 0.000+00 1.175+03 9.150+02 0.000+00 0.000+00 2.901−01 0.000+00 0.000+00 1.212+03 5.460+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.464+03 3.871+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.585+03 3.993+03 0.000+00 0.000+00 8.814+01 0.000+00 0.000+00 0.000+00 2.356−04 0.000+00 0.000+00 5.344+01 0.000+00 0.000+00 5.429−01 0.000+00 0.000+00
0.000+00 1.596−04 2.324−03 0.000+00 0.000+00 0.000+00 8.520+03 6.055+04 0.000+00 0.000+00 0.000+00 0.000+00 8.835+03 6.294+04 0.000+00 0.000+00 8.422−04 5.429+04 0.000+00 0.000+00 0.000+00 3.250+05 0.000+00 0.000+00 5.754+04 0.000+00 0.000+00 0.000+00 3.364+05 0.000+00 0.000+00 6.432−02 0.000+00 0.000+00 5.727+02 0.000+00 0.000+00 0.000+00 1.073+05 1.378+05 0.000+00 5.340+02 0.000+00 0.000+00 0.000+00 7.556+04 9.725+04 0.000+00 0.000+00 6.202+03 1.577+04 0.000+00 0.000+00 0.000+00 9.372+05 0.000+00 5.788+03 1.464+04 0.000+00 0.000+00 0.000+00 6.599+05 0.000+00 0.000+00 0.000+00 5.777−03 0.000+00 0.000+00 4.666−11 0.000+00 0.000+00 5.473+03 0.000+00 0.000+00 2.953−04 (continued on next page)
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 14 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
6.241+03 3.031+03 2.627+03 2.566+03 7.042+01 6.931+01 6.892+01 6.851+01 6.839+01 6.836+01 5.892+03 4.537+03 4.356+03 3.924+03 7.122+01 7.009+01 6.969+01 6.927+01 6.915+01 6.912+01 6.906+01 6.906+01 1.973+04 1.672+04 1.175+04 7.209+01 7.093+01 7.052+01 7.009+01 6.997+01 6.994+01 6.988+01 6.988+01 1.093+05 2.903+04 7.236+01 7.119+01 7.077+01 7.034+01 7.022+01 7.019+01 7.013+01 7.013+01 7.009+01 3.952+04 7.241+01 7.123+01 7.082+01 7.039+01 7.026+01 7.024+01 7.017+01 7.017+01 7.013+01 7.095+01 7.051+01 7.039+01 7.036+01 7.030+01 7.030+01 7.026+01 4.397+03 3.233+03 2.528+03 2.372+03 2.344+03 1.221+04 5.947+03 5.152+03 5.019+03 1.160+04 8.914+03 8.523+03 7.675+03 7.669+03
0.000+00 1.816+07 0.000+00 0.000+00 8.684+10 0.000+00 0.000+00 4.008+11 0.000+00 0.000+00 4.932+05 6.504+06 0.000+00 0.000+00 1.820+11 0.000+00 0.000+00 8.140+10 4.845+11 0.000+00 0.000+00 0.000+00 0.000+00 7.580+04 0.000+00 0.000+00 7.381+10 6.847+09 0.000+00 0.000+00 8.018+11 0.000+00 0.000+00 1.931+01 1.551+04 0.000+00 0.000+00 6.297+10 0.000+00 0.000+00 5.726+10 8.579+11 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.744+10 8.055+08 0.000+00 0.000+00 1.364+12 0.000+00 0.000+00 0.000+00 1.634+10 0.000+00 0.000+00 5.037+10 1.412+12 1.821+07 4.608+07 0.000+00 0.000+00 0.000+00 0.000+00 6.573+06 0.000+00 0.000+00 1.770+05 2.345+06 0.000+00 0.000+00 0.000+00
0.000+00 5.003−02 0.000+00 0.000+00 6.456−02 0.000+00 0.000+00 5.640−01 0.000+00 0.000+00 2.567−03 3.011−02 0.000+00 0.000+00 6.922−02 0.000+00 0.000+00 5.855−02 5.210−01 0.000+00 0.000+00 0.000+00 0.000+00 4.763−03 0.000+00 0.000+00 2.784−02 5.105−03 0.000+00 0.000+00 8.820−01 0.000+00 0.000+00 3.460−05 2.613−03 0.000+00 0.000+00 3.152−02 0.000+00 0.000+00 4.229−02 8.433−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.638−03 5.961−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.102−03 0.000+00 0.000+00 3.732−02 1.306+00 5.279−02 1.444−01 0.000+00 0.000+00 0.000+00 0.000+00 6.970−02 0.000+00 0.000+00 3.569−03 4.189−02 0.000+00 0.000+00 0.000+00
0.000+00 9.983−01 0.000+00 0.000+00 2.993−02 0.000+00 0.000+00 2.544−01 0.000+00 0.000+00 1.992−01 1.799+00 0.000+00 0.000+00 6.492−02 0.000+00 0.000+00 5.341−02 4.744−01 0.000+00 0.000+00 0.000+00 0.000+00 1.048+00 0.000+00 0.000+00 2.600−02 4.740−03 0.000+00 0.000+00 8.124−01 0.000+00 0.000+00 7.473−02 1.498+00 0.000+00 0.000+00 4.407−02 0.000+00 0.000+00 5.864−02 1.168+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.201−02 8.274−04 0.000+00 0.000+00 1.861+00 0.000+00 0.000+00 0.000+00 1.687−02 0.000+00 0.000+00 6.909−02 2.417+00 1.528+00 3.073+00 0.000+00 0.000+00 0.000+00 0.000+00 2.729+00 0.000+00 0.000+00 5.449−01 4.918+00 0.000+00 0.000+00 0.000+00
2.471−02 0.000+00 0.000+00 8.179−01 0.000+00 0.000+00 4.466+07 0.000+00 0.000+00 1.500+08 0.000+00 0.000+00 1.650−02 1.256−01 0.000+00 8.900+07 4.430+07 0.000+00 0.000+00 4.160+07 1.877+08 0.000+00 1.621−05 0.000+00 0.000+00 2.699+07 0.000+00 0.000+00 3.575+07 1.021+07 0.000+00 0.000+00 1.753+08 0.000+00 0.000+00 4.051+07 0.000+00 0.000+00 1.527+07 4.070+07 0.000+00 0.000+00 1.923+07 1.928+08 1.289−07 0.000+00 9.610+06 1.339+06 0.000+00 0.000+00 2.507+07 3.135+06 0.000+00 0.000+00 8.053+06 0.000+00 0.000+00 4.170+06 2.607+07 0.000+00 0.000+00 0.000+00 0.000+00 1.265+01 1.745+01 0.000+00 5.428−03 0.000+00 0.000+00 2.784−01 0.000+00 0.000+00 5.619−03 4.281−02 0.000+00
3.695+01 0.000+00 0.000+00 0.000+00 0.000+00 1.684+01 1.514+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.541−06 0.000+00 0.000+00 3.638+03 1.186+02 0.000+00 0.000+00 2.449+00 0.000+00 0.000+00 1.403+00 0.000+00 0.000+00 5.314−02 0.000+00 0.000+00 5.623+01 1.342+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.590+02 1.856+02 0.000+00 0.000+00 3.428+00 0.000+00 1.871−01 0.000+00 0.000+00 2.898−03 0.000+00 0.000+00 8.164+01 1.917+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.591+01 1.918+02 0.000+00 0.000+00 0.000+00 0.000+00 1.757−05 0.000+00 0.000+00 4.939+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.881−07 0.000+00 0.000+00
0.000+00 8.715−06 1.272−04 0.000+00 0.000+00 0.000+00 0.000+00 3.767+02 2.668+03 0.000+00 0.000+00 4.518−05 0.000+00 0.000+00 3.966+03 0.000+00 0.000+00 0.000+00 1.450+04 0.000+00 0.000+00 3.949−04 0.000+00 7.121−09 5.336−08 0.000+00 6.487+01 0.000+00 0.000+00 0.000+00 4.304+03 5.514+03 0.000+00 0.000+00 3.981−09 0.000+00 7.014+02 1.802+03 0.000+00 0.000+00 0.000+00 3.772+04 0.000+00 0.000+00 0.000+00 2.267−07 0.000+00 0.000+00 9.272+01 0.000+00 0.000+00 0.000+00 1.848+04 9.675+03 0.000+00 1.599+02 7.151+02 0.000+00 0.000+00 0.000+00 8.923+04 0.000+00 4.866−04 0.000+00 0.000+00 2.995−12 0.000+00 8.197−07 1.199−05 0.000+00 0.000+00 4.221−06 0.000+00 0.000+00 2.582−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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45
Table 14 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
3.855+04 3.216+04 2.270+04 2.265+04 1.943+05 5.523+04 5.494+04 3.851+04 7.716+04 7.660+04 4.803+04 1.039+07 1.272+05 1.288+05
0.000+00 3.800+04 0.000+00 0.000+00 1.230+01 8.046+03 0.000+00 0.000+00 0.000+00 1.696+03 0.000+00 2.511−05 3.843+02 0.000+00
0.000+00 8.841−03 0.000+00 0.000+00 6.960−05 4.906−03 0.000+00 0.000+00 0.000+00 1.990−03 0.000+00 4.067−07 1.165−03 0.000+00
0.000+00 3.745+00 0.000+00 0.000+00 2.670−01 5.352+00 0.000+00 0.000+00 0.000+00 3.010+00 0.000+00 1.113−01 3.903+00 0.000+00
4.094−06 0.000+00 0.000+00 8.183−05 0.000+00 0.000+00 1.082−07 6.405−06 4.439−08 0.000+00 0.000+00 0.000+00 0.000+00 1.120−09
1.882−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.848−10 0.000+00 2.514−02 0.000+00 0.000+00 0.000+00 0.000+00 5.611−03
0.000+00 9.646−10 7.067−09 0.000+00 0.000+00 5.706−10 0.000+00 0.000+00 0.000+00 1.930−11 1.042−10 0.000+00 7.415−12 0.000+00
46
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 15 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Co XXV. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.434+02 1.778+02 9.950+00 9.839+00 9.796+00 9.755+00 9.741+00 7.400+00 7.375+00 7.365+00 7.355+00 7.352+00 7.351+00 6.622+00 6.611+00 6.607+00 6.603+00 6.602+00 6.602+00 6.602+02 1.038+01 1.025+01 1.021+01 1.016+01 1.015+01 7.633+00 7.605+00 7.594+00 7.584+00 7.581+00 7.580+00 6.807+00 6.796+00 6.791+00 6.787+00 6.786+00 6.786+00 1.054+01 1.041+01 1.037+01 1.032+01 1.031+01 7.722+00 7.694+00 7.683+00 7.672+00 7.669+00 7.668+00 7.667+00 6.878+00 6.866+00 6.862+00 6.858+00 6.856+00 6.856+00 6.855+00 6.855+00 8.765+02 6.293+02 4.962+02 4.636+02 2.888+01 2.849+01 2.834+01 2.820+01 2.815+01 2.814+01 1.979+01 1.970+01 1.966+01 1.963+01 1.962+01 1.961+01
1.921+09 5.008+09 0.000+00 8.841+12 8.527+12 0.000+00 0.000+00 0.000+00 3.883+12 3.788+12 0.000+00 0.000+00 0.000+00 0.000+00 2.003+12 1.962+12 0.000+00 0.000+00 0.000+00 0.000+00 1.050+12 0.000+00 0.000+00 2.168+13 0.000+00 4.222+11 0.000+00 0.000+00 7.072+12 0.000+00 0.000+00 2.125+11 0.000+00 0.000+00 3.263+12 0.000+00 0.000+00 2.225+12 0.000+00 0.000+00 4.266+12 2.561+13 8.879+11 0.000+00 0.000+00 1.373+12 8.292+12 0.000+00 0.000+00 4.424+11 0.000+00 0.000+00 6.299+11 3.812+12 0.000+00 0.000+00 0.000+00 2.509+08 6.849+08 0.000+00 0.000+00 0.000+00 1.161+12 1.112+12 0.000+00 0.000+00 0.000+00 0.000+00 6.350+11 6.147+11 0.000+00 0.000+00 0.000+00
1.706−02 4.749−02 0.000+00 1.283−01 2.453−01 0.000+00 0.000+00 0.000+00 3.166−02 6.161−02 0.000+00 0.000+00 0.000+00 0.000+00 1.313−02 2.568−02 0.000+00 0.000+00 0.000+00 0.000+00 1.694−02 0.000+00 0.000+00 6.713−01 0.000+00 3.687−03 0.000+00 0.000+00 1.220−01 0.000+00 0.000+00 1.476−03 0.000+00 0.000+00 4.507−02 0.000+00 0.000+00 1.853−02 0.000+00 0.000+00 6.813−02 6.118−01 3.969−03 0.000+00 0.000+00 1.212−02 1.097−01 0.000+00 0.000+00 1.569−03 0.000+00 0.000+00 4.441−03 4.030−02 0.000+00 0.000+00 0.000+00 2.889−02 8.132−02 0.000+00 0.000+00 0.000+00 1.413−01 2.678−01 0.000+00 0.000+00 0.000+00 0.000+00 3.694−02 7.126−02 0.000+00 0.000+00 0.000+00
2.734−02 5.560−02 0.000+00 8.312−03 1.582−02 0.000+00 0.000+00 0.000+00 1.538−03 2.987−03 0.000+00 0.000+00 0.000+00 0.000+00 5.714−04 1.117−03 0.000+00 0.000+00 0.000+00 0.000+00 1.157−03 0.000+00 0.000+00 4.492−02 0.000+00 1.853−04 0.000+00 0.000+00 6.091−03 0.000+00 0.000+00 6.616−05 0.000+00 0.000+00 2.014−03 0.000+00 0.000+00 2.572−03 0.000+00 0.000+00 9.260−03 8.303−02 4.035−04 0.000+00 0.000+00 1.225−03 1.108−02 0.000+00 0.000+00 1.421−04 0.000+00 0.000+00 4.011−04 3.638−03 0.000+00 0.000+00 0.000+00 1.668−01 3.370−01 0.000+00 0.000+00 0.000+00 2.650−02 4.996−02 0.000+00 0.000+00 0.000+00 0.000+00 4.792−03 9.226−03 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.514+10 1.522+10 0.000+00 0.000+00 0.000+00 2.013+09 2.065+09 0.000+00 0.000+00 0.000+00 0.000+00 5.098+08 5.322+08 0.000+00 3.805+00 0.000+00 0.000+00 3.034+09 0.000+00 0.000+00 0.000+00 0.000+00 1.322+09 0.000+00 0.000+00 1.172+10 0.000+00 0.000+00 7.152+08 0.000+00 0.000+00 7.846+09 0.000+00 6.005+09 2.983+09 0.000+00 0.000+00 0.000+00 2.539+09 1.280+09 0.000+00 0.000+00 3.344+09 1.498+10 0.000+00 1.318+09 6.685+08 0.000+00 0.000+00 2.238+09 1.004+10 0.000+00 0.000+00 0.000+00 3.765+02 5.324+02 0.000+00 0.000+00 0.000+00 1.048+09 1.050+09 0.000+00 0.000+00 0.000+00 0.000+00 3.498+08 3.544+08 0.000+00
0.000+00 0.000+00 2.279+05 0.000+00 0.000+00 1.277+04 0.000+00 1.925+05 0.000+00 0.000+00 7.466+03 0.000+00 0.000+00 1.260+05 0.000+00 0.000+00 4.178+03 0.000+00 0.000+00 3.110+04 0.000+00 5.349+04 3.716+05 0.000+00 0.000+00 0.000+00 4.191+04 1.900+05 0.000+00 0.000+00 0.000+00 0.000+00 2.709+04 1.050+05 0.000+00 0.000+00 0.000+00 0.000+00 1.380+06 3.714+05 0.000+00 0.000+00 0.000+00 8.046+05 2.913+05 0.000+00 0.000+00 4.279+03 0.000+00 0.000+00 4.638+05 1.852+05 0.000+00 0.000+00 3.763+03 0.000+00 0.000+00 0.000+00 0.000+00 7.884−03 0.000+00 2.319+03 0.000+00 0.000+00 5.515+01 0.000+00 0.000+00 2.893+03 0.000+00 0.000+00 7.305+01 0.000+00 0.000+00
0.000+00 1.745+01 0.000+00 0.000+00 9.818+06 0.000+00 0.000+00 0.000+00 0.000+00 7.705+06 0.000+00 0.000+00 5.811+00 0.000+00 0.000+00 4.956+06 0.000+00 0.000+00 5.208+00 0.000+00 0.000+00 0.000+00 0.000+00 9.198+05 6.593+06 0.000+00 0.000+00 0.000+00 5.370+05 3.865+06 0.000+00 0.000+00 0.000+00 0.000+00 3.091+05 2.228+06 0.000+00 2.223+06 0.000+00 0.000+00 0.000+00 3.442+07 1.654+06 0.000+00 0.000+00 0.000+00 2.008+07 0.000+00 0.000+00 1.039+06 0.000+00 0.000+00 0.000+00 1.153+07 0.000+00 0.000+00 7.397−01 0.000+00 1.908−01 0.000+00 0.000+00 0.000+00 0.000+00 1.530+05 0.000+00 0.000+00 3.152−02 0.000+00 0.000+00 1.755+05 0.000+00 0.000+00 8.599−03 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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47
Table 15 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
2.231+03 1.143+03 9.842+02 2.986+01 2.945+01 2.929+01 2.914+01 2.908+01 2.908+01 2.025+01 2.015+01 2.011+01 2.008+01 2.007+01 2.006+01 2.345+03 1.761+03 3.027+01 2.984+01 2.968+01 2.952+01 2.947+01 2.946+01 2.943+01 2.044+01 2.034+01 2.030+01 2.026+01 2.025+01 2.025+01 2.024+01 2.024+01 7.067+03 3.066+01 3.023+01 3.006+01 2.990+01 2.984+01 2.983+01 2.981+01 2.061+01 2.051+01 2.047+01 2.044+01 2.042+01 2.042+01 2.042+01 2.042+01 3.080+01 3.036+01 3.018+01 3.002+01 2.997+01 2.996+01 2.993+01 2.067+01 2.057+01 2.053+01 2.050+01 2.048+01 2.048+01 2.047+01 2.047+01 2.047+01 2.129+03 1.519+03 1.197+03 1.117+03 1.105+03 6.291+01 6.199+01 6.162+01 6.128+01 6.116+01 6.114+01
0.000+00 7.306+07 0.000+00 2.949+11 0.000+00 0.000+00 2.279+12 0.000+00 0.000+00 1.437+11 0.000+00 0.000+00 1.124+12 0.000+00 0.000+00 1.687+06 2.404+07 6.226+11 0.000+00 0.000+00 4.585+11 2.735+12 0.000+00 0.000+00 3.009+11 0.000+00 0.000+00 2.232+11 1.338+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.645+11 1.501+10 0.000+00 0.000+00 5.052+12 0.000+00 0.000+00 7.057+10 6.453+09 0.000+00 0.000+00 1.670+12 0.000+00 0.000+00 0.000+00 0.000+00 1.386+11 0.000+00 0.000+00 3.588+11 5.389+12 0.000+00 0.000+00 5.954+10 0.000+00 0.000+00 1.179+11 1.778+12 0.000+00 0.000+00 5.884+07 1.633+08 0.000+00 0.000+00 0.000+00 0.000+00 2.734+11 2.609+11 0.000+00 0.000+00 0.000+00
0.000+00 2.864−02 0.000+00 3.943−02 0.000+00 0.000+00 5.801−01 0.000+00 0.000+00 8.833−03 0.000+00 0.000+00 1.359−01 0.000+00 0.000+00 1.391−03 1.677−02 4.276−02 0.000+00 0.000+00 5.990−02 5.341−01 0.000+00 0.000+00 9.418−03 0.000+00 0.000+00 1.373−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.126−02 2.033−03 0.000+00 0.000+00 1.011+00 0.000+00 0.000+00 2.226−03 4.056−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.263−02 0.000+00 0.000+00 4.828−02 9.653−01 0.000+00 0.000+00 2.509−03 0.000+00 0.000+00 7.417−03 1.490−01 0.000+00 0.000+00 3.998−02 1.129−01 0.000+00 0.000+00 0.000+00 0.000+00 1.575−01 2.970−01 0.000+00 0.000+00 0.000+00
0.000+00 2.156−01 0.000+00 7.752−03 0.000+00 0.000+00 1.113−01 0.000+00 0.000+00 1.178−03 0.000+00 0.000+00 1.796−02 0.000+00 0.000+00 4.297−02 3.888−01 1.704−02 0.000+00 0.000+00 2.328−02 2.073−01 0.000+00 0.000+00 2.535−03 0.000+00 0.000+00 3.664−03 3.288−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.484−03 8.045−04 0.000+00 0.000+00 3.973−01 0.000+00 0.000+00 6.014−04 1.093−04 0.000+00 0.000+00 4.212−02 0.000+00 0.000+00 0.000+00 0.000+00 7.527−03 0.000+00 0.000+00 2.857−02 5.708−01 0.000+00 0.000+00 1.018−03 0.000+00 0.000+00 3.000−03 6.024−02 0.000+00 0.000+00 5.605−01 1.129+00 0.000+00 0.000+00 0.000+00 0.000+00 6.427−02 1.205−01 0.000+00 0.000+00 0.000+00
3.192−01 0.000+00 0.000+00 0.000+00 0.000+00 3.219+08 0.000+00 0.000+00 1.210+09 0.000+00 0.000+00 1.836+08 0.000+00 0.000+00 1.413+07 0.000+00 0.000+00 0.000+00 6.402+08 3.183+08 0.000+00 0.000+00 3.313+08 1.497+09 0.000+00 3.541+08 1.784+08 0.000+00 0.000+00 2.639+06 1.280+07 0.000+00 1.454−04 1.116+08 0.000+00 0.000+00 2.042+08 5.832+07 0.000+00 0.000+00 6.785+07 0.000+00 0.000+00 9.808+07 2.816+07 0.000+00 0.000+00 2.551+09 1.676+08 0.000+00 0.000+00 8.708+07 2.321+08 0.000+00 0.000+00 1.017+08 0.000+00 0.000+00 4.161+07 1.115+08 0.000+00 0.000+00 2.830+08 2.826+09 0.000+00 0.000+00 6.587+01 9.349+01 0.000+00 0.000+00 0.000+00 0.000+00 1.454+08 1.456+08 0.000+00
8.078+02 0.000+00 0.000+00 0.000+00 6.770+02 2.101+04 0.000+00 0.000+00 0.000+00 0.000+00 8.118+02 1.471+04 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.724+04 4.737+03 0.000+00 0.000+00 1.475+02 0.000+00 0.000+00 4.421+04 5.671+03 0.000+00 0.000+00 7.079+01 0.000+00 0.000+00 3.051+01 7.352−01 0.000+00 0.000+00 1.769+03 1.379+03 0.000+00 0.000+00 4.354−01 0.000+00 0.000+00 1.824+03 8.227+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.214+03 5.823+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.890+03 6.006+03 0.000+00 0.000+00 1.326+02 0.000+00 0.000+00 0.000+00 3.409−04 0.000+00 0.000+00 8.035+01 0.000+00 0.000+00 8.190−01 0.000+00 0.000+00
0.000+00 2.458−04 3.731−03 0.000+00 0.000+00 0.000+00 1.183+04 8.405+04 0.000+00 0.000+00 0.000+00 0.000+00 1.226+04 8.738+04 0.000+00 0.000+00 1.108−03 7.520+04 0.000+00 0.000+00 0.000+00 4.505+05 0.000+00 0.000+00 7.973+04 0.000+00 0.000+00 0.000+00 4.662+05 0.000+00 0.000+00 1.050−01 0.000+00 0.000+00 7.974+02 0.000+00 0.000+00 0.000+00 1.488+05 1.912+05 0.000+00 7.438+02 0.000+00 0.000+00 0.000+00 1.048+05 1.350+05 0.000+00 0.000+00 8.645+03 2.185+04 0.000+00 0.000+00 0.000+00 1.299+06 0.000+00 8.072+03 2.029+04 0.000+00 0.000+00 0.000+00 9.147+05 0.000+00 0.000+00 0.000+00 7.813−03 0.000+00 0.000+00 7.362−11 0.000+00 0.000+00 7.590+03 0.000+00 0.000+00 4.815−04 (continued on next page)
48
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 15 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
5.297+03 2.733+03 2.350+03 2.298+03 6.483+01 6.384+01 6.345+01 6.309+01 6.297+01 6.295+01 5.647+03 4.223+03 4.059+03 3.621+03 6.563+01 6.462+01 6.422+01 6.385+01 6.373+01 6.371+01 6.365+01 6.365+01 1.675+04 1.443+04 1.009+04 6.640+01 6.537+01 6.496+01 6.458+01 6.446+01 6.443+01 6.437+01 6.437+01 1.043+05 2.539+04 6.667+01 6.563+01 6.521+01 6.483+01 6.471+01 6.468+01 6.462+01 6.462+01 6.458+01 3.356+04 6.671+01 6.567+01 6.525+01 6.487+01 6.475+01 6.472+01 6.466+01 6.466+01 6.462+01 6.538+01 6.500+01 6.487+01 6.485+01 6.478+01 6.478+01 6.475+01 4.209+03 2.993+03 2.358+03 2.200+03 2.174+03 1.036+04 5.362+03 4.607+03 4.495+03 1.111+04 8.295+03 7.940+03 7.082+03 7.076+03
0.000+00 2.281+07 0.000+00 0.000+00 1.017+11 0.000+00 0.000+00 4.718+11 0.000+00 0.000+00 5.161+05 7.432+06 0.000+00 0.000+00 2.142+11 0.000+00 0.000+00 9.594+10 5.707+11 0.000+00 0.000+00 0.000+00 0.000+00 1.085+05 0.000+00 0.000+00 8.722+10 8.039+09 0.000+00 0.000+00 9.442+11 0.000+00 0.000+00 2.049+01 2.136+04 0.000+00 0.000+00 7.408+10 0.000+00 0.000+00 6.742+10 1.010+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.059+10 9.484+08 0.000+00 0.000+00 1.606+12 0.000+00 0.000+00 0.000+00 1.926+10 0.000+00 0.000+00 5.930+10 1.662+12 1.913+07 5.349+07 0.000+00 0.000+00 0.000+00 0.000+00 8.260+06 0.000+00 0.000+00 1.853+05 2.681+06 0.000+00 0.000+00 0.000+00
0.000+00 5.110−02 0.000+00 0.000+00 6.410−02 0.000+00 0.000+00 5.631−01 0.000+00 0.000+00 2.467−03 2.981−02 0.000+00 0.000+00 6.915−02 0.000+00 0.000+00 5.864−02 5.212−01 0.000+00 0.000+00 0.000+00 0.000+00 5.083−03 0.000+00 0.000+00 2.794−02 5.086−03 0.000+00 0.000+00 8.815−01 0.000+00 0.000+00 3.341−05 2.753−03 0.000+00 0.000+00 3.149−02 0.000+00 0.000+00 4.229−02 8.431−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.662−03 5.960−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.114−03 0.000+00 0.000+00 3.731−02 1.306+00 5.080−02 1.437−01 0.000+00 0.000+00 0.000+00 0.000+00 7.121−02 0.000+00 0.000+00 3.430−03 4.148−02 0.000+00 0.000+00 0.000+00
0.000+00 9.196−01 0.000+00 0.000+00 2.736−02 0.000+00 0.000+00 2.339−01 0.000+00 0.000+00 1.834−01 1.658+00 0.000+00 0.000+00 5.976−02 0.000+00 0.000+00 4.931−02 4.374−01 0.000+00 0.000+00 0.000+00 0.000+00 9.660−01 0.000+00 0.000+00 2.405−02 4.351−03 0.000+00 0.000+00 7.480−01 0.000+00 0.000+00 6.884−02 1.381+00 0.000+00 0.000+00 4.056−02 0.000+00 0.000+00 5.403−02 1.076+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.110−02 7.623−04 0.000+00 0.000+00 1.714+00 0.000+00 0.000+00 0.000+00 1.557−02 0.000+00 0.000+00 6.366−02 2.227+00 1.408+00 2.832+00 0.000+00 0.000+00 0.000+00 0.000+00 2.514+00 0.000+00 0.000+00 5.019−01 4.531+00 0.000+00 0.000+00 0.000+00
4.757−02 0.000+00 0.000+00 1.204+00 0.000+00 0.000+00 5.709+07 0.000+00 0.000+00 1.920+08 0.000+00 0.000+00 1.995−02 1.595−01 0.000+00 1.137+08 5.659+07 0.000+00 0.000+00 5.312+07 2.397+08 0.000+00 3.121−05 0.000+00 0.000+00 3.447+07 0.000+00 0.000+00 4.569+07 1.304+07 0.000+00 0.000+00 2.242+08 0.000+00 0.000+00 5.174+07 0.000+00 0.000+00 1.951+07 5.200+07 0.000+00 0.000+00 2.457+07 2.464+08 2.477−07 0.000+00 1.230+07 1.710+06 0.000+00 0.000+00 3.203+07 4.006+06 0.000+00 0.000+00 1.029+07 0.000+00 0.000+00 5.326+06 3.330+07 0.000+00 0.000+00 0.000+00 0.000+00 1.521+01 2.162+01 0.000+00 1.045−02 0.000+00 0.000+00 4.100−01 0.000+00 0.000+00 6.799−03 5.436−02 0.000+00
6.040+01 0.000+00 0.000+00 0.000+00 0.000+00 2.538+01 2.282+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.242−06 0.000+00 0.000+00 5.474+03 1.783+02 0.000+00 0.000+00 3.683+00 0.000+00 0.000+00 2.294+00 0.000+00 0.000+00 7.994−02 0.000+00 0.000+00 8.466+01 2.023+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.405+02 2.792+02 0.000+00 0.000+00 5.159+00 0.000+00 3.055−01 0.000+00 0.000+00 4.355−03 0.000+00 0.000+00 1.228+02 2.885+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.142+02 2.886+02 0.000+00 0.000+00 0.000+00 0.000+00 2.544−05 0.000+00 0.000+00 8.073+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.737−07 0.000+00 0.000+00
0.000+00 1.345−05 2.048−04 0.000+00 0.000+00 0.000+00 0.000+00 5.227+02 3.702+03 0.000+00 0.000+00 5.959−05 0.000+00 0.000+00 5.495+03 0.000+00 0.000+00 0.000+00 2.011+04 0.000+00 0.000+00 6.443−04 0.000+00 1.368−08 1.051−07 0.000+00 9.027+01 0.000+00 0.000+00 0.000+00 5.971+03 7.650+03 0.000+00 0.000+00 7.166−09 0.000+00 9.771+02 2.497+03 0.000+00 0.000+00 0.000+00 5.231+04 0.000+00 0.000+00 0.000+00 3.701−07 0.000+00 0.000+00 1.289+02 0.000+00 0.000+00 0.000+00 2.562+04 1.342+04 0.000+00 2.225+02 9.926+02 0.000+00 0.000+00 0.000+00 1.237+05 0.000+00 6.589−04 0.000+00 0.000+00 4.730−12 0.000+00 1.267−06 1.932−05 0.000+00 0.000+00 5.573−06 0.000+00 0.000+00 4.189−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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49
Table 15 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
3.272+04 2.781+04 1.952+04 1.948+04 1.853+05 4.841+04 4.817+04 3.344+04 6.552+04 6.509+04 4.080+04 9.876+06 1.082+05 1.094+05
0.000+00 5.418+04 0.000+00 0.000+00 1.306+01 1.101+04 0.000+00 0.000+00 0.000+00 2.548+03 0.000+00 2.697−05 5.760+02 0.000+00
0.000+00 9.423−03 0.000+00 0.000+00 6.722−05 5.157−03 0.000+00 0.000+00 0.000+00 2.158−03 0.000+00 3.944−07 1.263−03 0.000+00
0.000+00 3.451+00 0.000+00 0.000+00 2.460−01 4.931+00 0.000+00 0.000+00 0.000+00 2.774+00 0.000+00 1.026−01 3.597+00 0.000+00
7.886−06 0.000+00 0.000+00 1.476−04 0.000+00 0.000+00 1.771−07 1.101−05 8.536−08 0.000+00 0.000+00 0.000+00 0.000+00 2.152−09
3.078−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.229−10 0.000+00 4.106−02 0.000+00 0.000+00 0.000+00 0.000+00 9.161−03
0.000+00 1.840−09 1.384−08 0.000+00 0.000+00 1.016−09 0.000+00 0.000+00 0.000+00 4.012−11 2.170−10 0.000+00 1.537−11 0.000+00
50
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 16 Transition wavelengths (λij in Å), radiative rates (Aji in s−1 ), oscillator strengths (fij , dimensionless), and line strengths (S, in atomic units) for electric dipole (E1), and Aji for E2, M1, and M2 transitions in Ni XXVI. (a ± b ≡ a × 10±b ). i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
2 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 3 4 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 5 6 7 8 9 10 11 12 13 14 16 17 18 19 20 21
2.334+02 1.651+02 9.204+00 9.104+00 9.061+00 9.025+00 9.011+00 6.845+00 6.822+00 6.812+00 6.803+00 6.800+00 6.799+00 6.124+00 6.115+00 6.111+00 6.107+00 6.106+00 6.106+00 5.641+02 9.582+00 9.474+00 9.427+00 9.388+00 9.373+00 7.052+00 7.027+00 7.016+00 7.007+00 7.004+00 7.003+00 6.289+00 6.279+00 6.275+00 6.271+00 6.270+00 6.270+00 9.748+00 9.636+00 9.587+00 9.547+00 9.532+00 7.141+00 7.116+00 7.105+00 7.095+00 7.092+00 7.091+00 7.090+00 6.360+00 6.350+00 6.345+00 6.342+00 6.340+00 6.340+00 6.339+00 6.339+00 8.402+02 5.831+02 4.632+02 4.302+02 2.670+01 2.636+01 2.620+01 2.608+01 2.603+01 2.602+01 1.830+01 1.822+01 1.818+01 1.815+01 1.814+01 1.814+01
2.012+09 5.789+09 0.000+00 1.037+13 9.972+12 0.000+00 0.000+00 0.000+00 4.550+12 4.430+12 0.000+00 0.000+00 0.000+00 0.000+00 2.346+12 2.295+12 0.000+00 0.000+00 0.000+00 0.000+00 1.222+12 0.000+00 0.000+00 2.538+13 0.000+00 4.916+11 0.000+00 0.000+00 8.280+12 0.000+00 0.000+00 2.477+11 0.000+00 0.000+00 3.821+12 0.000+00 0.000+00 2.602+12 0.000+00 0.000+00 4.987+12 2.994+13 1.039+12 0.000+00 0.000+00 1.604+12 9.691+12 0.000+00 0.000+00 5.177+11 0.000+00 0.000+00 7.355+11 4.454+12 0.000+00 0.000+00 0.000+00 2.630+08 7.957+08 0.000+00 0.000+00 0.000+00 1.363+12 1.301+12 0.000+00 0.000+00 0.000+00 0.000+00 7.448+11 7.193+11 0.000+00 0.000+00 0.000+00
1.643−02 4.729−02 0.000+00 1.289−01 2.455−01 0.000+00 0.000+00 0.000+00 3.174−02 6.163−02 0.000+00 0.000+00 0.000+00 0.000+00 1.315−02 2.569−02 0.000+00 0.000+00 0.000+00 0.000+00 1.681−02 0.000+00 0.000+00 6.706−01 0.000+00 3.665−03 0.000+00 0.000+00 1.219−01 0.000+00 0.000+00 1.469−03 0.000+00 0.000+00 4.505−02 0.000+00 0.000+00 1.853−02 0.000+00 0.000+00 6.814−02 6.118−01 3.970−03 0.000+00 0.000+00 1.211−02 1.096−01 0.000+00 0.000+00 1.570−03 0.000+00 0.000+00 4.435−03 4.026−02 0.000+00 0.000+00 0.000+00 2.784−02 8.112−02 0.000+00 0.000+00 0.000+00 1.420−01 2.679−01 0.000+00 0.000+00 0.000+00 0.000+00 3.706−02 7.129−02 0.000+00 0.000+00 0.000+00
2.524−02 5.140−02 0.000+00 7.724−03 1.464−02 0.000+00 0.000+00 0.000+00 1.426−03 2.764−03 0.000+00 0.000+00 0.000+00 0.000+00 5.295−04 1.034−03 0.000+00 0.000+00 0.000+00 0.000+00 1.061−03 0.000+00 0.000+00 4.145−02 0.000+00 1.702−04 0.000+00 0.000+00 5.625−03 0.000+00 0.000+00 6.082−05 0.000+00 0.000+00 1.860−03 0.000+00 0.000+00 2.379−03 0.000+00 0.000+00 8.567−03 7.678−02 3.733−04 0.000+00 0.000+00 1.131−03 1.024−02 0.000+00 0.000+00 1.315−04 0.000+00 0.000+00 3.703−04 3.362−03 0.000+00 0.000+00 0.000+00 1.540−01 3.115−01 0.000+00 0.000+00 0.000+00 2.464−02 4.622−02 0.000+00 0.000+00 0.000+00 0.000+00 4.446−03 8.534−03 0.000+00 0.000+00 0.000+00
0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.911+10 1.921+10 0.000+00 0.000+00 0.000+00 2.531+09 2.601+09 0.000+00 0.000+00 0.000+00 0.000+00 6.388+08 6.693+08 0.000+00 7.137+00 0.000+00 0.000+00 3.841+09 0.000+00 0.000+00 0.000+00 0.000+00 1.676+09 0.000+00 0.000+00 1.483+10 0.000+00 0.000+00 9.080+08 0.000+00 0.000+00 9.925+09 0.000+00 7.594+09 3.771+09 0.000+00 0.000+00 0.000+00 3.206+09 1.618+09 0.000+00 0.000+00 4.229+09 1.895+10 0.000+00 1.665+09 8.454+08 0.000+00 0.000+00 2.830+09 1.269+10 0.000+00 0.000+00 0.000+00 4.533+02 6.611+02 0.000+00 0.000+00 0.000+00 1.324+09 1.328+09 0.000+00 0.000+00 0.000+00 0.000+00 4.414+08 4.478+08 0.000+00
0.000+00 0.000+00 3.367+05 0.000+00 0.000+00 1.886+04 0.000+00 2.844+05 0.000+00 0.000+00 1.102+04 0.000+00 0.000+00 1.860+05 0.000+00 0.000+00 6.165+03 0.000+00 0.000+00 4.985+04 0.000+00 7.933+04 5.516+05 0.000+00 0.000+00 0.000+00 6.214+04 2.819+05 0.000+00 0.000+00 0.000+00 0.000+00 4.018+04 1.558+05 0.000+00 0.000+00 0.000+00 0.000+00 2.042+06 5.482+05 0.000+00 0.000+00 0.000+00 1.191+06 4.299+05 0.000+00 0.000+00 6.332+03 0.000+00 0.000+00 6.862+05 2.733+05 0.000+00 0.000+00 5.570+03 0.000+00 0.000+00 0.000+00 0.000+00 1.131−02 0.000+00 3.431+03 0.000+00 0.000+00 8.170+01 0.000+00 0.000+00 4.280+03 0.000+00 0.000+00 1.082+02 0.000+00 0.000+00
0.000+00 2.341+01 0.000+00 0.000+00 1.342+07 0.000+00 0.000+00 0.000+00 0.000+00 1.053+07 0.000+00 0.000+00 9.293+00 0.000+00 0.000+00 6.774+06 0.000+00 0.000+00 8.336+00 0.000+00 0.000+00 0.000+00 0.000+00 1.261+06 9.044+06 0.000+00 0.000+00 0.000+00 7.358+05 5.301+06 0.000+00 0.000+00 0.000+00 0.000+00 4.235+05 3.056+06 0.000+00 3.041+06 0.000+00 0.000+00 0.000+00 4.704+07 2.263+06 0.000+00 0.000+00 0.000+00 2.742+07 0.000+00 0.000+00 1.422+06 0.000+00 0.000+00 0.000+00 1.575+07 0.000+00 0.000+00 1.183+00 0.000+00 2.581−01 0.000+00 0.000+00 0.000+00 0.000+00 2.093+05 0.000+00 0.000+00 5.041−02 0.000+00 0.000+00 2.402+05 0.000+00 0.000+00 1.372−02 (continued on next page)
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51
Table 16 (continued) i 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
6 7 8 9 10 11 12 13 14 16 17 18 19 20 21 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 10 11 12 13 14 16 17 18 19 20 21
1.906+03 1.032+03 8.816+02 2.758+01 2.721+01 2.705+01 2.691+01 2.686+01 2.686+01 1.871+01 1.862+01 1.858+01 1.855+01 1.854+01 1.854+01 2.252+03 1.640+03 2.798+01 2.760+01 2.744+01 2.730+01 2.725+01 2.724+01 2.721+01 1.889+01 1.881+01 1.877+01 1.873+01 1.872+01 1.872+01 1.871+01 1.871+01 6.038+03 2.834+01 2.795+01 2.778+01 2.764+01 2.758+01 2.757+01 2.755+01 1.905+01 1.896+01 1.892+01 1.889+01 1.888+01 1.888+01 1.887+01 1.887+01 2.847+01 2.808+01 2.791+01 2.776+01 2.771+01 2.770+01 2.767+01 1.911+01 1.902+01 1.898+01 1.895+01 1.894+01 1.893+01 1.893+01 1.893+01 1.892+01 2.041+03 1.406+03 1.117+03 1.036+03 1.025+03 5.817+01 5.734+01 5.697+01 5.667+01 5.655+01 5.653+01
0.000+00 9.175+07 0.000+00 3.434+11 0.000+00 0.000+00 2.667+12 0.000+00 0.000+00 1.674+11 0.000+00 0.000+00 1.316+12 0.000+00 0.000+00 1.760+06 2.749+07 7.283+11 0.000+00 0.000+00 5.366+11 3.200+12 0.000+00 0.000+00 3.520+11 0.000+00 0.000+00 2.611+11 1.565+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.933+11 1.751+10 0.000+00 0.000+00 5.912+12 0.000+00 0.000+00 8.294+10 7.530+09 0.000+00 0.000+00 1.955+12 0.000+00 0.000+00 0.000+00 0.000+00 1.621+11 0.000+00 0.000+00 4.196+11 6.304+12 0.000+00 0.000+00 6.962+10 0.000+00 0.000+00 1.379+11 2.080+12 0.000+00 0.000+00 6.171+07 1.900+08 0.000+00 0.000+00 0.000+00 0.000+00 3.211+11 3.053+11 0.000+00 0.000+00 0.000+00
0.000+00 2.932−02 0.000+00 3.915−02 0.000+00 0.000+00 5.792−01 0.000+00 0.000+00 8.785−03 0.000+00 0.000+00 1.358−01 0.000+00 0.000+00 1.338−03 1.663−02 4.275−02 0.000+00 0.000+00 5.996−02 5.343−01 0.000+00 0.000+00 9.419−03 0.000+00 0.000+00 1.374−02 1.233−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.132−02 2.025−03 0.000+00 0.000+00 1.011+00 0.000+00 0.000+00 2.236−03 4.042−04 0.000+00 0.000+00 1.566−01 0.000+00 0.000+00 0.000+00 0.000+00 1.261−02 0.000+00 0.000+00 4.827−02 9.650−01 0.000+00 0.000+00 2.507−03 0.000+00 0.000+00 7.413−03 1.489−01 0.000+00 0.000+00 3.853−02 1.127−01 0.000+00 0.000+00 0.000+00 0.000+00 1.583−01 2.971−01 0.000+00 0.000+00 0.000+00
0.000+00 1.993−01 0.000+00 7.110−03 0.000+00 0.000+00 1.027−01 0.000+00 0.000+00 1.082−03 0.000+00 0.000+00 1.658−02 0.000+00 0.000+00 3.969−02 3.593−01 1.575−02 0.000+00 0.000+00 2.156−02 1.917−01 0.000+00 0.000+00 2.343−03 0.000+00 0.000+00 3.388−03 3.040−02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 4.165−03 7.408−04 0.000+00 0.000+00 3.670−01 0.000+00 0.000+00 5.584−04 1.007−04 0.000+00 0.000+00 3.893−02 0.000+00 0.000+00 0.000+00 0.000+00 6.953−03 0.000+00 0.000+00 2.641−02 5.275−01 0.000+00 0.000+00 9.402−04 0.000+00 0.000+00 2.773−03 5.568−02 0.000+00 0.000+00 5.178−01 1.044+00 0.000+00 0.000+00 0.000+00 0.000+00 5.975−02 1.114−01 0.000+00 0.000+00 0.000+00
5.993−01 0.000+00 0.000+00 0.000+00 0.000+00 4.075+08 0.000+00 0.000+00 1.536+09 0.000+00 0.000+00 2.328+08 0.000+00 0.000+00 1.829+07 0.000+00 0.000+00 0.000+00 8.103+08 4.027+08 0.000+00 0.000+00 4.189+08 1.893+09 0.000+00 4.476+08 2.256+08 0.000+00 0.000+00 3.304+06 1.613+07 0.000+00 2.729−04 1.411+08 0.000+00 0.000+00 2.584+08 7.381+07 0.000+00 0.000+00 8.582+07 0.000+00 0.000+00 1.241+08 3.565+07 0.000+00 0.000+00 3.227+09 2.120+08 0.000+00 0.000+00 1.102+08 2.937+08 0.000+00 0.000+00 1.287+08 0.000+00 0.000+00 5.260+07 1.410+08 0.000+00 0.000+00 3.581+08 3.575+09 0.000+00 0.000+00 7.950+01 1.164+02 0.000+00 0.000+00 0.000+00 0.000+00 1.839+08 1.842+08 0.000+00
1.296+03 0.000+00 0.000+00 0.000+00 1.004+03 3.118+04 0.000+00 0.000+00 0.000+00 0.000+00 1.204+03 2.183+04 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.477+04 7.004+03 0.000+00 0.000+00 2.183+02 0.000+00 0.000+00 6.548+04 8.385+03 0.000+00 0.000+00 1.047+02 0.000+00 0.000+00 4.892+01 1.088+00 0.000+00 0.000+00 2.622+03 2.044+03 0.000+00 0.000+00 6.436−01 0.000+00 0.000+00 2.702+03 1.220+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 7.724+03 8.619+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.762+03 8.890+03 0.000+00 0.000+00 1.963+02 0.000+00 0.000+00 0.000+00 4.901−04 0.000+00 0.000+00 1.189+02 0.000+00 0.000+00 1.216+00 0.000+00 0.000+00
0.000+00 3.786−04 5.982−03 0.000+00 0.000+00 0.000+00 1.621+04 1.152+05 0.000+00 0.000+00 0.000+00 0.000+00 1.681+04 1.198+05 0.000+00 0.000+00 1.460−03 1.029+05 0.000+00 0.000+00 0.000+00 6.165+05 0.000+00 0.000+00 1.091+05 0.000+00 0.000+00 0.000+00 6.378+05 0.000+00 0.000+00 1.680−01 0.000+00 0.000+00 1.096+03 0.000+00 0.000+00 0.000+00 2.038+05 2.620+05 0.000+00 1.023+03 0.000+00 0.000+00 0.000+00 1.436+05 1.850+05 0.000+00 0.000+00 1.190+04 2.990+04 0.000+00 0.000+00 0.000+00 1.778+06 0.000+00 1.112+04 2.777+04 0.000+00 0.000+00 0.000+00 1.252+06 0.000+00 0.000+00 0.000+00 1.060−02 0.000+00 0.000+00 1.158−10 0.000+00 0.000+00 1.039+04 0.000+00 0.000+00 7.707−04 (continued on next page)
52
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 16 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13 14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 16 16 16 16 16 17 17 17 17 18 18 18 18 18
11 12 13 14 16 17 18 19 20 21 12 13 14 15 16 17 18 19 20 21 22 23 13 14 15 16 17 18 19 20 21 22 23 14 15 16 17 18 19 20 21 22 23 24 15 16 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 17 18 19 20 21 18 19 20 21 19 20 21 22 23
4.525+03 2.466+03 2.104+03 2.060+03 5.987+01 5.900+01 5.861+01 5.829+01 5.817+01 5.815+01 5.422+03 3.932+03 3.783+03 3.342+03 6.067+01 5.978+01 5.938+01 5.905+01 5.892+01 5.890+01 5.884+01 5.884+01 1.431+04 1.251+04 8.712+03 6.136+01 6.044+01 6.003+01 5.970+01 5.957+01 5.955+01 5.949+01 5.949+01 9.974+04 2.228+04 6.163+01 6.070+01 6.029+01 5.995+01 5.982+01 5.980+01 5.974+01 5.973+01 5.970+01 2.868+04 6.166+01 6.074+01 6.032+01 5.998+01 5.985+01 5.983+01 5.977+01 5.977+01 5.973+01 6.045+01 6.011+01 5.998+01 5.996+01 5.990+01 5.990+01 5.986+01 4.035+03 2.772+03 2.200+03 2.040+03 2.016+03 8.852+03 4.838+03 4.124+03 4.030+03 1.067+04 7.722+03 7.400+03 6.536+03 6.531+03
0.000+00 2.869+07 0.000+00 0.000+00 1.185+11 0.000+00 0.000+00 5.517+11 0.000+00 0.000+00 5.386+05 8.509+06 0.000+00 0.000+00 2.505+11 0.000+00 0.000+00 1.124+11 6.679+11 0.000+00 0.000+00 0.000+00 0.000+00 1.539+05 0.000+00 0.000+00 1.025+11 9.382+09 0.000+00 0.000+00 1.105+12 0.000+00 0.000+00 2.166+01 2.925+04 0.000+00 0.000+00 8.662+10 0.000+00 0.000+00 7.888+10 1.182+12 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 2.416+10 1.110+09 0.000+00 0.000+00 1.879+12 0.000+00 0.000+00 0.000+00 2.256+10 0.000+00 0.000+00 6.937+10 1.945+12 2.006+07 6.228+07 0.000+00 0.000+00 0.000+00 0.000+00 1.039+07 0.000+00 0.000+00 1.934+05 3.071+06 0.000+00 0.000+00 0.000+00
0.000+00 5.233−02 0.000+00 0.000+00 6.368−02 0.000+00 0.000+00 5.620−01 0.000+00 0.000+00 2.374−03 2.959−02 0.000+00 0.000+00 6.914−02 0.000+00 0.000+00 5.872−02 5.214−01 0.000+00 0.000+00 0.000+00 0.000+00 5.419−03 0.000+00 0.000+00 2.806−02 5.069−03 0.000+00 0.000+00 8.809−01 0.000+00 0.000+00 3.229−05 2.901−03 0.000+00 0.000+00 3.146−02 0.000+00 0.000+00 4.229−02 8.428−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.687−03 5.960−04 0.000+00 0.000+00 1.342+00 0.000+00 0.000+00 0.000+00 9.127−03 0.000+00 0.000+00 3.731−02 1.306+00 4.896−02 1.434−01 0.000+00 0.000+00 0.000+00 0.000+00 7.294−02 0.000+00 0.000+00 3.301−03 4.118−02 0.000+00 0.000+00 0.000+00
0.000+00 8.498−01 0.000+00 0.000+00 2.510−02 0.000+00 0.000+00 2.157−01 0.000+00 0.000+00 1.695−01 1.532+00 0.000+00 0.000+00 5.524−02 0.000+00 0.000+00 4.566−02 4.046−01 0.000+00 0.000+00 0.000+00 0.000+00 8.930−01 0.000+00 0.000+00 2.234−02 4.007−03 0.000+00 0.000+00 6.908−01 0.000+00 0.000+00 6.363−02 1.276+00 0.000+00 0.000+00 3.747−02 0.000+00 0.000+00 4.995−02 9.944−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.029−02 7.046−04 0.000+00 0.000+00 1.584+00 0.000+00 0.000+00 0.000+00 1.442−02 0.000+00 0.000+00 5.885−02 2.058+00 1.301+00 2.618+00 0.000+00 0.000+00 0.000+00 0.000+00 2.323+00 0.000+00 0.000+00 4.638−01 4.188+00 0.000+00 0.000+00 0.000+00
8.933−02 0.000+00 0.000+00 1.776+00 0.000+00 0.000+00 7.228+07 0.000+00 0.000+00 2.435+08 0.000+00 0.000+00 2.423−02 2.034−01 0.000+00 1.440+08 7.161+07 0.000+00 0.000+00 6.720+07 3.033+08 0.000+00 5.859−05 0.000+00 0.000+00 4.362+07 0.000+00 0.000+00 5.784+07 1.651+07 0.000+00 0.000+00 2.842+08 0.000+00 0.000+00 6.547+07 0.000+00 0.000+00 2.469+07 6.580+07 0.000+00 0.000+00 3.110+07 3.120+08 4.643−07 0.000+00 1.559+07 2.163+06 0.000+00 0.000+00 4.054+07 5.069+06 0.000+00 0.000+00 1.302+07 0.000+00 0.000+00 6.738+06 4.213+07 0.000+00 0.000+00 0.000+00 0.000+00 1.837+01 2.695+01 0.000+00 1.962−02 0.000+00 0.000+00 6.048−01 0.000+00 0.000+00 8.261−03 6.936−02 0.000+00
9.691+01 0.000+00 0.000+00 0.000+00 0.000+00 3.764+01 3.386+03 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.237−06 0.000+00 0.000+00 8.108+03 2.638+02 0.000+00 0.000+00 5.453+00 0.000+00 0.000+00 3.679+00 0.000+00 0.000+00 1.184−01 0.000+00 0.000+00 1.254+02 3.000+02 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 8.008+02 4.134+02 0.000+00 0.000+00 7.641+00 0.000+00 4.895−01 0.000+00 0.000+00 6.441−03 0.000+00 0.000+00 1.819+02 4.274+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 1.691+02 4.272+02 0.000+00 0.000+00 0.000+00 0.000+00 3.660−05 0.000+00 0.000+00 1.295+01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 3.953−07 0.000+00 0.000+00
0.000+00 2.077−05 3.291−04 0.000+00 0.000+00 0.000+00 0.000+00 7.162+02 5.070+03 0.000+00 0.000+00 7.870−05 0.000+00 0.000+00 7.522+03 0.000+00 0.000+00 0.000+00 2.753+04 0.000+00 0.000+00 1.032−03 0.000+00 2.579−08 2.026−07 0.000+00 1.241+02 0.000+00 0.000+00 0.000+00 8.179+03 1.048+04 0.000+00 0.000+00 1.274−08 0.000+00 1.344+03 3.417+03 0.000+00 0.000+00 0.000+00 7.161+04 0.000+00 0.000+00 0.000+00 5.919−07 0.000+00 0.000+00 1.769+02 0.000+00 0.000+00 0.000+00 3.508+04 1.838+04 0.000+00 3.056+02 1.360+03 0.000+00 0.000+00 0.000+00 1.693+05 0.000+00 8.948−04 0.000+00 0.000+00 7.444−12 0.000+00 1.958−06 3.106−05 0.000+00 0.000+00 7.367−06 0.000+00 0.000+00 6.763−15 (continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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53
Table 16 (continued) i
j
λij
AE1 ji
fijE1
S E1
AE2 ji
AM1 ji
AM2 ji
19 19 19 19 20 20 20 20 21 21 21 22 22 23
20 21 22 23 21 22 23 24 22 23 24 23 24 24
2.795+04 2.414+04 1.687+04 1.684+04 1.772+05 4.255+04 4.236+04 2.915+04 5.600+04 5.566+04 3.489+04 9.410+06 9.255+04 9.346+04
0.000+00 7.654+04 0.000+00 0.000+00 1.380+01 1.499+04 0.000+00 0.000+00 0.000+00 3.766+03 0.000+00 2.882−05 8.500+02 0.000+00
0.000+00 1.003−02 0.000+00 0.000+00 6.497−05 5.424−03 0.000+00 0.000+00 0.000+00 2.332−03 0.000+00 3.826−07 1.364−03 0.000+00
0.000+00 3.190+00 0.000+00 0.000+00 2.274−01 4.559+00 0.000+00 0.000+00 0.000+00 2.565+00 0.000+00 9.483−02 3.325+00 0.000+00
1.481−05 0.000+00 0.000+00 2.617−04 0.000+00 0.000+00 2.880−07 1.871−05 1.600−07 0.000+00 0.000+00 0.000+00 0.000+00 4.031−09
4.937−01 0.000+00 0.000+00 0.000+00 0.000+00 0.000+00 5.559−10 0.000+00 6.579−02 0.000+00 0.000+00 0.000+00 0.000+00 1.467−02
0.000+00 3.448−09 2.658−08 0.000+00 0.000+00 1.790−09 0.000+00 0.000+00 0.000+00 8.110−11 4.391−10 0.000+00 3.097−11 0.000+00
54
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 17 Collision strengths for transitions in Sc XIX. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
200
300
400
500
600
700
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.955−1 7.600−1 2.289−2 9.468−3 1.809−2 1.930−2 2.893−2 4.307−3 1.971−3 3.814−3 3.217−3 4.836−3 1.771−3 2.357−3 1.670−3 8.296−4 1.614−3 1.270−3 1.910−3 9.794−4 1.304−3 1.100−4 1.369−4
4.541−1 8.765−1 2.508−2 1.667−2 3.200−2 2.434−2 3.650−2 4.774−3 3.283−3 6.379−3 3.564−3 5.365−3 1.816−3 2.420−3 1.822−3 1.275−3 2.487−3 1.243−3 1.874−3 8.964−4 1.196−3 6.776−5 8.462−5
4.892−1 9.461−1 2.604−2 2.213−2 4.259−2 2.712−2 4.068−2 4.986−3 4.336−3 8.445−3 3.891−3 5.860−3 1.907−3 2.542−3 1.899−3 1.667−3 3.261−3 1.330−3 2.006−3 9.313−4 1.243−3 6.803−5 8.504−5
5.140−1 9.960−1 2.660−2 2.647−2 5.100−2 2.883−2 4.324−2 5.117−3 5.172−3 1.009−2 4.113−3 6.196−3 1.959−3 2.612−3 1.946−3 1.981−3 3.880−3 1.398−3 2.109−3 9.556−4 1.275−3 7.027−5 8.786−5
5.332−1 1.035+0 2.701−2 3.008−2 5.799−2 2.999−2 4.498−2 5.210−3 5.864−3 1.145−2 4.269−3 6.431−3 1.993−3 2.657−3 1.981−3 2.241−3 4.393−3 1.448−3 2.185−3 9.726−4 1.298−3 7.238−5 9.050−5
5.488−1 1.066+0 2.732−2 3.318−2 6.397−2 3.084−2 4.624−2 5.280−3 6.458−3 1.261−2 4.384−3 6.605−3 2.019−3 2.692−3 2.007−3 2.463−3 4.832−3 1.485−3 2.241−3 9.857−4 1.316−3 7.417−5 9.274−5
5.618−1 1.092+0 2.758−2 3.592−2 6.924−2 3.147−2 4.723−2 5.340−3 6.979−3 1.363−2 4.475−3 6.743−3 2.039−3 2.720−3 2.029−3 2.658−3 5.215−3 1.516−3 2.288−3 9.965−4 1.330−3 7.567−5 9.464−5
5.588−1 1.091+0 2.780−2 3.697−2 7.132−2 3.167−2 4.742−2 5.567−3 7.368−3 1.436−2 4.463−3 6.712−3 2.090−3 2.780−3 2.173−3 2.838−3 5.539−3 1.500−3 2.259−3 1.031−3 1.373−3 7.533−5 9.394−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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55
Table 18 Collision strengths for transitions in Ti XX. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
200
300
400
500
600
700
800
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.546−1 6.781−1 2.042−2 7.955−3 1.512−2 1.692−2 2.535−2 3.839−3 1.680−3 3.239−3 2.901−3 4.361−3 1.642−3 2.184−3 1.501−3 7.271−4 1.410−3 1.181−3 1.775−3 9.378−4 1.248−3 1.177−4 1.465−4
4.073−1 7.822−1 2.252−2 1.414−2 2.702−2 2.142−2 3.212−2 4.278−3 2.779−3 5.381−3 3.151−3 4.745−3 1.628−3 2.170−3 1.634−3 1.080−3 2.102−3 1.107−3 1.669−3 8.079−4 1.077−3 6.256−5 7.808−5
4.389−1 8.447−1 2.345−2 1.895−2 3.630−2 2.402−2 3.603−2 4.485−3 3.701−3 7.186−3 3.443−3 5.186−3 1.714−3 2.286−3 1.708−3 1.422−3 2.774−3 1.179−3 1.778−3 8.373−4 1.117−3 6.140−5 7.673−5
4.618−1 8.903−1 2.399−2 2.280−2 4.374−2 2.566−2 3.848−2 4.610−3 4.442−3 8.639−3 3.651−3 5.502−3 1.766−3 2.355−3 1.753−3 1.700−3 3.322−3 1.241−3 1.872−3 8.608−4 1.149−3 6.317−5 7.898−5
4.793−1 9.255−1 2.439−2 2.602−2 4.996−2 2.678−2 4.017−2 4.698−3 5.060−3 9.849−3 3.800−3 5.727−3 1.800−3 2.401−3 1.787−3 1.932−3 3.778−3 1.288−3 1.944−3 8.775−4 1.171−3 6.505−5 8.134−5
4.934−1 9.541−1 2.468−2 2.879−2 5.530−2 2.761−2 4.140−2 4.765−3 5.590−3 1.089−2 3.911−3 5.895−3 1.826−3 2.434−3 1.812−3 2.131−3 4.170−3 1.324−3 1.999−3 8.901−4 1.188−3 6.671−5 8.343−5
5.053−1 9.781−1 2.493−2 3.124−2 6.001−2 2.823−2 4.237−2 4.821−3 6.056−3 1.180−2 3.999−3 6.028−3 1.846−3 2.462−3 1.832−3 2.305−3 4.514−3 1.353−3 2.043−3 9.006−4 1.202−3 6.813−5 8.521−5
5.156−1 9.990−1 2.515−2 3.344−2 6.422−2 2.876−2 4.312−2 4.871−3 6.474−3 1.262−2 4.071−3 6.137−3 1.864−3 2.485−3 1.851−3 2.461−3 4.821−3 1.377−3 2.079−3 9.098−4 1.214−3 6.936−5 8.674−5
4.775−1 9.272−1 2.482−2 2.805−2 5.383−2 2.732−2 4.089−2 4.945−3 5.623−3 1.091−2 3.840−3 5.777−3 1.859−3 2.472−3 1.921−3 2.171−3 4.222−3 1.288−3 1.940−3 9.105−4 1.212−3 6.764−5 8.434−5
56
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 19 Collision strengths for transitions in V XXI. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
100
300
500
700
900
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.133−1 5.971−1 1.836−2 6.738−3 1.273−2 1.492−2 2.235−2 3.453−3 1.453−3 2.791−3 2.641−3 3.970−3 1.541−3 2.049−3 1.363−3 6.565−4 1.270−3 1.102−3 1.657−3 9.107−4 1.212−3 1.300−4 1.618−4
3.959−1 7.577−1 2.121−2 1.630−2 3.108−2 2.136−2 3.203−2 4.052−3 3.176−3 6.144−3 3.062−3 4.614−3 1.547−3 2.062−3 1.543−3 1.220−3 2.372−3 1.050−3 1.585−3 7.559−4 1.009−3 5.579−5 6.970−5
4.327−1 8.315−1 2.211−2 2.261−2 4.323−2 2.400−2 3.600−2 4.256−3 4.386−3 8.513−3 3.397−3 5.122−3 1.632−3 2.176−3 1.618−3 1.674−3 3.265−3 1.151−3 1.737−3 7.947−4 1.061−3 5.870−5 7.340−5
4.567−1 8.798−1 2.263−2 2.730−2 5.224−2 2.543−2 3.812−2 4.374−3 5.281−3 1.026−2 3.589−3 5.412−3 1.677−3 2.236−3 1.662−3 2.009−3 3.924−3 1.213−3 1.832−3 8.171−4 1.091−3 6.156−5 7.698−5
4.745−1 9.158−1 2.302−2 3.108−2 5.947−2 2.634−2 3.953−2 4.459−3 5.998−3 1.166−2 3.718−3 5.606−3 1.709−3 2.279−3 1.695−3 2.277−3 4.452−3 1.256−3 1.897−3 8.337−4 1.113−3 6.374−5 7.973−5
4.395−1 8.496−1 2.260−2 2.583−2 4.937−2 2.496−2 3.735−2 4.496−3 5.160−3 9.985−3 3.498−3 5.263−3 1.700−3 2.261−3 1.745−3 1.989−3 3.859−3 1.172−3 1.766−3 8.324−4 1.108−3 6.206−5 7.737−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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57
Table 20 Collision strengths for transitions in Cr XXII. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.325−1 6.312−1 1.841−2 1.035−2 1.955−2 1.682−2 2.522−2 3.488−3 2.028−3 3.895−3 2.515−3 3.788−3 1.330−3 1.772−3 1.332−3 7.926−4 1.531−3 9.008−4 1.358−3 6.706−4 8.939−4 5.566−5 6.936−5
3.777−1 7.201−1 1.978−2 1.715−2 3.260−2 2.055−2 3.081−2 3.790−3 3.325−3 6.422−3 2.914−3 4.395−3 1.451−3 1.934−3 1.442−3 1.271−3 2.469−3 9.915−4 1.498−3 7.063−4 9.427−4 5.181−5 6.476−5
4.045−1 7.739−1 2.041−2 2.197−2 4.185−2 2.236−2 3.354−2 3.933−3 4.247−3 8.224−3 3.151−3 4.754−3 1.509−3 2.012−3 1.494−3 1.617−3 3.148−3 1.065−3 1.610−3 7.343−4 9.802−4 5.456−5 6.823−5
4.233−1 8.119−1 2.083−2 2.575−2 4.907−2 2.346−2 3.519−2 4.029−3 4.964−3 9.624−3 3.301−3 4.981−3 1.545−3 2.061−3 1.531−3 1.885−3 3.676−3 1.114−3 1.684−3 7.524−4 1.005−3 5.689−5 7.116−5
4.377−1 8.412−1 2.117−2 2.888−2 5.504−2 2.421−2 3.634−2 4.102−3 5.557−3 1.078−2 3.407−3 5.141−3 1.573−3 2.098−3 1.559−3 2.107−3 4.110−3 1.150−3 1.738−3 7.666−4 1.024−3 5.874−5 7.348−5
4.052−1 7.798−1 2.065−2 2.391−2 4.553−2 2.290−2 3.427−2 4.096−3 4.756−3 9.176−3 3.200−3 4.817−3 1.561−3 2.075−3 1.596−3 1.830−3 3.541−3 1.071−3 1.615−3 7.640−4 1.017−3 5.715−5 7.123−5
58
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 21 Collision strengths for transitions in Mn XXIII. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
3.015−1 5.687−1 1.675−2 8.915−3 1.675−2 1.500−2 2.248−2 3.168−3 1.748−3 3.342−3 2.269−3 3.418−3 1.213−3 1.615−3 1.212−3 6.863−4 1.321−3 8.229−4 1.241−3 6.184−4 8.239−4 5.375−5 6.692−5
3.437−1 6.512−1 1.806−2 1.497−2 2.830−2 1.848−2 2.771−2 3.456−3 2.895−3 5.570−3 2.620−3 3.953−3 1.320−3 1.760−3 1.315−3 1.106−3 2.141−3 8.926−4 1.349−3 6.430−4 8.582−4 4.728−5 5.907−5
3.684−1 7.008−1 1.867−2 1.931−2 3.661−2 2.022−2 3.033−2 3.595−3 3.726−3 7.190−3 2.845−3 4.294−3 1.378−3 1.838−3 1.366−3 1.418−3 2.752−3 9.615−4 1.454−3 6.701−4 8.948−4 4.961−5 6.203−5
3.858−1 7.359−1 1.906−2 2.273−2 4.313−2 2.128−2 3.193−2 3.683−3 4.374−3 8.454−3 2.989−3 4.512−3 1.413−3 1.885−3 1.400−3 1.660−3 3.229−3 1.008−3 1.525−3 6.876−4 9.181−4 5.176−5 6.474−5
3.993−1 7.631−1 1.938−2 2.557−2 4.853−2 2.204−2 3.303−2 3.753−3 4.912−3 9.501−3 3.090−3 4.666−3 1.440−3 1.920−3 1.426−3 1.861−3 3.623−3 1.042−3 1.577−3 7.012−4 9.362−4 5.352−5 6.694−5
3.759−1 7.194−1 1.893−2 2.219−2 4.207−2 2.109−2 3.155−2 3.760−3 4.398−3 8.460−3 2.940−3 4.427−3 1.439−3 1.912−3 1.462−3 1.691−3 3.262−3 9.832−4 1.483−3 7.040−4 9.365−4 5.281−5 6.580−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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59
Table 22 Collision strengths for transitions in Fe XXIV. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.753−1 5.151−1 1.528−2 7.714−3 1.440−2 1.344−2 2.013−2 2.886−3 1.516−3 2.884−3 2.061−3 3.105−3 1.113−3 1.481−3 1.105−3 5.983−4 1.147−3 7.583−4 1.144−3 5.753−4 7.661−4 5.276−5 6.563−5
3.143−1 5.916−1 1.654−2 1.311−2 2.465−2 1.666−2 2.498−2 3.164−3 2.530−3 4.849−3 2.364−3 3.569−3 1.205−3 1.606−3 1.204−3 9.663−4 1.864−3 8.070−4 1.220−3 5.871−4 7.837−4 4.335−5 5.416−5
3.371−1 6.372−1 1.713−2 1.704−2 3.214−2 1.834−2 2.750−2 3.296−3 3.280−3 6.307−3 2.577−3 3.891−3 1.262−3 1.683−3 1.252−3 1.247−3 2.414−3 8.705−4 1.317−3 6.133−4 8.189−4 4.525−5 5.658−5
3.531−1 6.696−1 1.751−2 2.014−2 3.803−2 1.937−2 2.906−2 3.382−3 3.869−3 7.453−3 2.714−3 4.100−3 1.297−3 1.729−3 1.284−3 1.468−3 2.846−3 9.151−4 1.385−3 6.304−4 8.418−4 4.723−5 5.907−5
3.655−1 6.948−1 1.781−2 2.272−2 4.294−2 2.009−2 3.014−2 3.449−3 4.358−3 8.404−3 2.814−3 4.250−3 1.322−3 1.763−3 1.310−3 1.651−3 3.204−3 9.478−4 1.435−3 6.434−4 8.592−4 4.888−5 6.114−5
3.496−1 6.656−1 1.743−2 2.065−2 3.896−2 1.950−2 2.916−2 3.464−3 4.078−3 7.818−3 2.711−3 4.083−3 1.331−3 1.768−3 1.345−3 1.568−3 3.017−3 9.063−4 1.368−3 6.514−4 8.664−4 4.899−5 6.103−5
60
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 23 Collision strengths for transitions in Co XXV. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
1200
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.525−1 4.696−1 1.399−2 6.707−3 1.243−2 1.208−2 1.810−2 2.639−3 1.322−3 2.502−3 1.883−3 2.838−3 1.028−3 1.368−3 1.012−3 5.256−4 1.003−3 7.042−4 1.062−3 5.398−4 7.185−4 5.263−5 6.539−5
2.876−1 5.377−1 1.520−2 1.152−2 2.154−2 1.507−2 2.259−2 2.904−3 2.219−3 4.235−3 2.142−3 3.234−3 1.102−3 1.469−3 1.105−3 8.474−4 1.629−3 7.328−4 1.109−3 5.378−4 7.178−4 3.997−5 4.991−5
3.088−1 5.800−1 1.577−2 1.508−2 2.829−2 1.667−2 2.500−2 3.031−3 2.898−3 5.550−3 2.340−3 3.535−3 1.159−3 1.545−3 1.151−3 1.101−3 2.124−3 7.909−4 1.197−3 5.627−4 7.514−4 4.142−5 5.179−5
3.238−1 6.102−1 1.614−2 1.790−2 3.364−2 1.768−2 2.651−2 3.114−3 3.434−3 6.591−3 2.473−3 3.738−3 1.193−3 1.590−3 1.183−3 1.302−3 2.517−3 8.336−4 1.263−3 5.794−4 7.738−4 4.321−5 5.405−5
3.354−1 6.335−1 1.642−2 2.026−2 3.810−2 1.838−2 2.756−2 3.176−3 3.880−3 7.457−3 2.569−3 3.884−3 1.217−3 1.623−3 1.207−3 1.469−3 2.844−3 8.650−4 1.310−3 5.919−4 7.906−4 4.476−5 5.599−5
3.448−1 6.527−1 1.667−2 2.231−2 4.196−2 1.892−2 2.838−2 3.231−3 4.266−3 8.204−3 2.644−3 3.996−3 1.238−3 1.651−3 1.227−3 1.613−3 3.125−3 8.897−4 1.348−3 6.024−4 8.046−4 4.606−5 5.763−5
3.268−1 6.378−1 1.611−2 1.928−2 3.620−2 1.806−2 2.701−2 3.205−3 3.797−3 7.254−3 2.507−3 3.778−3 1.237−3 1.642−3 1.241−3 1.457−3 2.795−3 8.378−4 1.265−3 6.042−4 8.035−4 4.558−5 5.676−5
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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61
Table 24 Collision strengths for transitions in Ni XXVI. (a ± b ≡ a × 10±b ). Transition
Energy (Ryd)
i
j
200
400
600
800
1000
1200
1400
FAC
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24
2.314−1 4.266−1 1.286−2 5.855−3 1.077−2 1.090−2 1.633−2 2.426−3 1.160−3 2.184−3 1.732−3 2.609−3 9.564−4 1.272−3 9.321−4 4.657−4 8.849−4 6.597−4 9.947−4 5.117−4 6.807−4 5.333−5 6.617−5
2.643−1 4.908−1 1.402−2 1.016−2 1.888−2 1.366−2 2.048−2 2.676−3 1.953−3 3.711−3 1.947−3 2.941−3 1.011−3 1.347−3 1.017−3 7.459−4 1.428−3 6.683−4 1.011−3 4.941−4 6.593−4 3.706−5 4.626−5
2.841−1 5.299−1 1.456−2 1.339−2 2.498−2 1.520−2 2.278−2 2.795−3 2.568−3 4.899−3 2.132−3 3.222−3 1.066−3 1.421−3 1.062−3 9.756−4 1.875−3 7.211−4 1.092−3 5.176−4 6.912−4 3.804−5 4.756−5
2.982−1 5.581−1 1.491−2 1.596−2 2.984−2 1.616−2 2.424−2 2.876−3 3.057−3 5.846−3 2.259−3 3.416−3 1.099−3 1.466−3 1.092−3 1.159−3 2.233−3 7.612−4 1.154−3 5.338−4 7.130−4 3.964−5 4.958−5
3.089−1 5.799−1 1.519−2 1.812−2 3.391−2 1.685−2 2.528−2 2.936−3 3.465−3 6.636−3 2.352−3 3.557−3 1.124−3 1.499−3 1.115−3 1.311−3 2.531−3 7.918−4 1.200−3 5.460−4 7.292−4 4.108−5 5.139−5
3.178−1 5.978−1 1.542−2 1.999−2 3.743−2 1.737−2 2.606−2 2.988−3 3.818−3 7.319−3 2.424−3 3.667−3 1.143−3 1.525−3 1.135−3 1.443−3 2.788−3 8.154−4 1.236−3 5.561−4 7.428−4 4.231−5 5.294−5
3.253−1 6.130−1 1.564−2 2.166−2 4.057−2 1.781−2 2.669−2 3.033−3 4.131−3 7.925−3 2.485−3 3.759−3 1.161−3 1.548−3 1.152−3 1.560−3 3.017−3 8.361−4 1.268−3 5.651−4 7.547−4 4.338−5 5.428−5
3.059−1 5.926−1 1.496−2 1.798−2 3.358−2 1.679−2 2.510−2 2.971−3 3.545−3 6.749−3 2.328−3 3.509−3 1.150−3 1.527−3 1.152−3 1.358−3 2.597−3 7.776−4 1.175−3 5.635−4 7.497−4 4.252−5 5.294−5
62
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 25 Effective collision strengths for transitions in Sc XIX. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.573−1 5.045−1 2.305−2 6.441−3 1.223−2 1.755−2 2.625−2 4.622−3 1.624−3 3.124−3 3.188−3 4.781−3 1.882−3 2.503−3 1.805−3 6.944−4 1.337−3 1.231−3 1.847−3 9.951−4 1.323−3 1.285−4 1.603−4 4.563−2 1.639−3 2.521−2 6.600−3 8.495−2 1.216−2 5.175−4 5.239−3 2.156−3 1.558−2 3.780−3 2.623−3 1.578−3 2.450−4 2.102−3 1.036−3 5.849−3 1.766−3 1.389−3 9.530−4 1.290−4 1.268−4 3.315−3 6.743−3 5.736−2 3.222−2 1.657−1 1.032−3 2.174−3 1.266−2 7.725−3 3.146−2 2.844−3 5.749−3 4.871−4 1.042−3 5.238−3 3.313−3 1.206−2 1.654−3 3.118−3 2.178−4 3.071−4 1.684+0 3.297+0 1.225−1 1.840−1 1.082−1 1.762−2 3.317−2
2.639−1 5.138−1 2.483−2 8.036−3 1.558−2 1.886−2 2.864−2 4.934−3 2.257−3 4.457−3 3.749−3 5.664−3 2.496−3 3.336−3 1.704−3 8.260−4 1.592−3 1.322−3 1.986−3 1.061−3 1.414−3 1.408−4 1.753−4 6.651−2 7.258−3 2.562−2 1.090−2 8.571−2 1.916−2 1.601−3 5.583−3 3.405−3 1.671−2 5.192−3 4.078−3 2.969−3 4.710−4 1.915−3 1.131−3 6.140−3 1.886−3 1.559−3 9.975−4 1.519−4 1.285−4 1.633−2 1.126−2 6.389−2 4.087−2 1.736−1 3.118−3 3.470−3 1.443−2 9.782−3 3.455−2 5.191−3 9.270−3 9.377−4 1.150−3 4.975−3 3.532−3 1.270−2 1.775−3 3.468−3 2.298−4 3.483−4 1.678+0 3.282+0 1.600−1 2.437−1 1.096−1 2.140−2 4.547−2
2.759−1 5.376−1 2.431−2 8.231−3 1.596−2 1.909−2 2.896−2 4.755−3 2.182−3 4.293−3 3.623−3 5.465−3 2.322−3 3.094−3 1.693−3 8.322−4 1.610−3 1.307−3 1.963−3 1.036−3 1.381−3 1.314−4 1.636−4 7.323−2 5.885−3 2.548−2 1.024−2 8.896−2 1.808−2 1.314−3 5.337−3 2.991−3 1.693−2 4.644−3 3.800−3 2.508−3 4.207−4 1.889−3 1.062−3 6.271−3 1.764−3 1.558−3 9.214−4 1.447−4 1.161−4 1.297−2 1.051−2 6.247−2 4.016−2 1.786−1 2.577−3 3.044−3 1.357−2 9.144−3 3.453−2 4.489−3 8.462−3 8.406−4 1.077−3 4.856−3 3.409−3 1.284−2 1.674−3 3.410−3 2.103−4 3.278−4 1.784+0 3.477+0 1.564−1 2.379−1 1.086−1 2.279−2 4.731−2
2.901−1 5.653−1 2.392−2 8.541−3 1.652−2 1.925−2 2.913−2 4.631−3 2.160−3 4.233−3 3.516−3 5.298−3 2.163−3 2.879−3 1.693−3 8.531−4 1.654−3 1.289−3 1.937−3 1.008−3 1.344−3 1.208−4 1.504−4 7.505−2 4.793−3 2.517−2 9.220−3 9.332−2 1.620−2 1.085−3 5.127−3 2.598−3 1.738−2 4.069−3 3.598−3 2.071−3 3.773−4 1.865−3 9.811−4 6.468−3 1.609−3 1.573−3 8.295−4 1.380−4 1.020−4 1.039−2 9.442−3 6.053−2 3.875−2 1.850−1 2.143−3 2.642−3 1.280−2 8.516−3 3.492−2 3.837−3 7.807−3 7.563−4 9.945−4 4.730−3 3.259−3 1.308−2 1.557−3 3.371−3 1.885−4 3.069−4 1.922+0 3.734+0 1.491−1 2.264−1 1.085−1 2.561−2 5.167−2
3.072−1 5.982−1 2.372−2 9.157−3 1.766−2 1.957−2 2.954−2 4.570−3 2.221−3 4.338−3 3.450−3 5.194−3 2.038−3 2.712−3 1.705−3 8.959−4 1.740−3 1.272−3 1.913−3 9.808−4 1.307−3 1.097−4 1.366−4 7.135−2 3.973−3 2.489−2 8.117−3 9.976−2 1.402−2 9.127−4 4.973−3 2.247−3 1.818−2 3.500−3 3.521−3 1.685−3 3.398−4 1.844−3 8.921−4 6.764−3 1.427−3 1.617−3 7.272−4 1.326−4 8.709−5 8.512−3 8.318−3 5.866−2 3.743−2 1.950−1 1.815−3 2.285−3 1.218−2 7.968−3 3.594−2 3.293−3 7.406−3 6.831−4 9.040−4 4.600−3 3.096−3 1.347−2 1.434−3 3.374−3 1.660−4 2.879−4 2.094+0 4.052+0 1.408−1 2.134−1 1.093−1 3.033−2 5.978−2
3.284−1 6.387−1 2.375−2 1.027−2 1.977−2 2.021−2 3.045−2 4.569−3 2.390−3 4.658−3 3.436−3 5.171−3 1.953−3 2.599−3 1.726−3 9.704−4 1.888−3 1.262−3 1.899−3 9.578−4 1.276−3 9.929−5 1.237−4 6.384−2 3.436−3 2.473−2 7.122−3 1.093−1 1.192−2 7.915−4 4.877−3 1.946−3 1.944−2 2.959−3 3.586−3 1.361−3 3.092−4 1.828−3 7.999−4 7.198−3 1.231−3 1.701−3 6.226−4 1.297−4 7.250−5 7.301−3 7.318−3 5.724−2 3.684−2 2.108−1 1.586−3 1.981−3 1.172−2 7.550−3 3.784−2 2.874−3 7.299−3 6.237−4 8.109−4 4.478−3 2.944−3 1.410−2 1.321−3 3.446−3 1.449−4 2.731−4 2.289+0 4.419+0 1.333−1 2.017−1 1.108−1 3.732−2 7.248−2
3.542−1 6.878−1 2.401−2 1.202−2 2.312−2 2.124−2 3.194−2 4.617−3 2.689−3 5.234−3 3.477−3 5.233−3 1.906−3 2.537−3 1.756−3 1.086−3 2.117−3 1.264−3 1.903−3 9.423−4 1.256−3 9.042−5 1.127−4 5.509−2 3.176−3 2.475−2 6.325−3 1.226−1 1.009−2 7.178−4 4.829−3 1.697−3 2.125−2 2.468−3 3.793−3 1.099−3 2.877−4 1.818−3 7.114−4 7.805−3 1.036−3 1.831−3 5.247−4 1.294−4 5.935−5 6.719−3 6.527−3 5.641−2 3.736−2 2.339−1 1.450−3 1.730−3 1.139−2 7.309−3 4.077−2 2.583−3 7.484−3 5.829−4 7.220−4 4.372−3 2.829−3 1.505−2 1.229−3 3.604−3 1.267−4 2.640−4 2.499+0 4.817+0 1.273−1 1.922−1 1.126−1 4.685−2 9.022−2
3.822−1 7.411−1 2.430−2 1.436−2 2.762−2 2.245−2 3.373−2 4.672−3 3.095−3 6.026−3 3.548−3 5.340−3 1.879−3 2.503−3 1.781−3 1.237−3 2.415−3 1.271−3 1.915−3 9.303−4 1.240−3 8.327−5 1.039−4 4.692−2 3.152−3 2.478−2 5.725−3 1.391−1 8.584−3 6.838−4 4.794−3 1.494−3 2.346−2 2.042−3 4.089−3 8.955−4 2.756−4 1.806−3 6.309−4 8.527−3 8.582−4 1.989−3 4.398−4 1.308−4 4.827−5 6.662−3 5.937−3 5.584−2 3.890−2 2.630−1 1.392−3 1.527−3 1.114−2 7.229−3 4.446−2 2.396−3 7.863−3 5.611−4 6.416−4 4.269−3 2.756−3 1.622−2 1.163−3 3.821−3 1.118−4 2.589−4 2.697+0 5.199+0 1.221−1 1.842−1 1.139−1 5.824−2 1.117−1
4.004−1 7.758−1 2.397−2 1.647−2 3.170−2 2.305−2 3.461−2 4.596−3 3.442−3 6.703−3 3.532−3 5.318−3 1.818−3 2.422−3 1.751−3 1.359−3 2.655−3 1.248−3 1.880−3 8.972−4 1.197−3 7.616−5 9.505−5 3.972−2 3.206−3 2.420−2 5.194−3 1.523−1 7.299−3 6.618−4 4.643−3 1.311−3 2.503−2 1.673−3 4.282−3 7.328−4 2.647−4 1.745−3 5.527−4 9.001−3 6.987−4 2.086−3 3.658−4 1.291−4 3.900−5 6.778−3 5.411−3 5.412−2 4.003−2 2.861−1 1.357−3 1.343−3 1.066−2 7.091−3 4.702−2 2.234−3 8.090−3 5.414−4 5.632−4 4.070−3 2.657−3 1.695−2 1.094−3 3.938−3 9.848−5 2.499−4 2.792+0 5.386+0 1.152−1 1.736−1 1.116−1 6.775−2 1.296−1
4.165−1 8.099−1 2.581−2 1.844−2 3.542−2 2.446−2 3.662−2 5.123−3 3.830−3 7.429−3 3.644−3 5.476−3 1.883−3 2.504−3 1.986−3 1.508−3 2.929−3 1.268−3 1.907−3 9.353−4 1.245−3 7.776−5 9.694−5 3.012−2 3.132−3 2.640−2 5.102−3 1.666−1 6.573−3 6.377−4 5.329−3 1.311−3 2.685−2 1.547−3 4.578−3 6.701−4 2.472−4 2.099−3 5.685−4 9.510−3 6.697−4 2.285−3 3.755−4 1.363−4 4.090−5 6.574−3 5.330−3 5.838−2 4.212−2 3.111−1 1.312−3 1.342−3 1.202−2 7.304−3 5.018−2 2.228−3 8.539−3 5.062−4 5.799−4 4.777−3 2.727−3 1.784−2 1.161−3 4.276−3 1.073−4 2.810−4 2.952+0 5.725+0 1.156−1 1.740−1 1.214−1 7.670−2 1.468−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
63
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
4.487−2 6.690−2 4.562−2 6.080−2 2.040−2 4.049−3 7.739−3 9.440−3 1.412−2 5.278−3 7.049−3 8.138−3 1.016−2 2.019−1 2.467+0 3.102−2 7.211−3 1.156−1 1.630−2 1.438−1 2.087−2 1.515−1 2.210−2 1.708−3 2.255−2 4.476−3 2.990−2 5.917−3 1.603−2 5.069−3 1.947−2 6.332−3 5.652−1 4.672+0 1.488−2 1.706−2 2.488−1 5.559−2 2.838−1 7.244−2 2.785−1 3.416−3 4.600−3 4.972−2 1.334−2 5.981−2 1.110−2 3.105−2 1.517−2 3.727−2 1.455−1 6.195−3 1.161−2 1.186−2 2.227−1 2.817−2 9.829−1 4.972−2 2.008−3 3.616−3 4.547−3 4.273−2 1.029−2 1.548−1 1.651−2 4.241−2 9.552−3 9.335−3 8.043−3 2.735−2 2.827−2 3.486−1 1.241−1 1.431+0
4.625−2 7.435−2 5.405−2 7.443−2 1.894−2 4.691−3 8.964−3 9.712−3 1.454−2 6.397−3 8.547−3 8.698−3 1.087−2 2.417−1 2.491+0 1.032−1 1.758−2 1.092−1 2.294−2 1.440−1 3.056−2 1.518−1 3.519−2 2.778−3 1.950−2 4.396−3 3.197−2 6.417−3 1.717−2 5.789−3 2.011−2 6.712−3 6.446−1 4.710+0 3.687−2 2.331−2 2.504−1 6.613−2 3.037−1 8.995−2 2.956−1 5.664−3 4.551−3 4.347−2 1.438−2 6.400−2 1.238−2 3.361−2 1.592−2 3.865−2 4.077−1 1.852−2 2.561−2 2.960−2 2.310−1 5.361−2 9.753−1 8.885−2 3.175−3 5.073−3 5.692−3 4.149−2 1.126−2 1.583−1 1.773−2 4.427−2 9.620−3 2.732−2 2.030−2 6.301−2 5.282−2 3.868−1 1.661−1 1.442+0
4.744−2 7.503−2 5.235−2 7.164−2 1.911−2 5.061−3 9.691−3 9.960−3 1.492−2 6.092−3 8.139−3 8.501−3 1.063−2 2.345−1 2.628+0 9.553−2 1.509−2 1.091−1 2.121−2 1.555−1 2.762−2 1.564−1 3.091−2 2.599−3 1.971−2 4.309−3 3.406−2 6.044−3 1.732−2 5.269−3 2.060−2 6.219−3 6.649−1 4.956+0 3.185−2 2.146−2 2.474−1 6.521−2 3.204−1 8.564−2 2.989−1 5.302−3 4.454−3 4.383−2 1.434−2 6.754−2 1.174−2 3.347−2 1.542−2 3.915−2 3.747−1 1.473−2 2.222−2 2.451−2 2.273−1 4.507−2 1.023+0 7.452−2 2.750−3 4.700−3 5.098−3 4.108−2 1.012−2 1.639−1 1.571−2 4.602−2 8.527−3 2.185−2 1.654−2 5.385−2 4.443−2 3.743−1 1.540−1 1.503+0
4.947−2 7.695−2 5.090−2 6.918−2 1.939−2 5.658−3 1.085−2 1.031−2 1.546−2 5.769−3 7.707−3 8.337−3 1.042−2 2.234−1 2.831+0 8.201−2 1.390−2 1.096−1 1.990−2 1.735−1 2.495−2 1.633−1 2.703−2 2.543−3 1.999−2 4.250−3 3.710−2 5.641−3 1.757−2 4.711−3 2.125−2 5.700−3 6.961−1 5.349+0 2.941−2 2.024−2 2.455−1 6.594−2 3.489−1 8.253−2 3.067−1 5.200−3 4.392−3 4.436−2 1.447−2 7.280−2 1.109−2 3.347−2 1.493−2 3.991−2 3.182−1 1.188−2 1.968−2 2.001−2 2.244−1 3.711−2 1.095+0 6.105−2 2.405−3 4.384−3 4.502−3 4.073−2 8.887−3 1.719−1 1.351−2 4.869−2 7.391−3 1.770−2 1.325−2 4.645−2 3.666−2 3.632−1 1.446−1 1.600+0
5.250−2 8.053−2 4.986−2 6.740−2 1.977−2 6.556−3 1.260−2 1.078−2 1.617−2 5.461−3 7.295−3 8.242−3 1.030−2 2.115−1 3.095+0 6.751−2 1.398−2 1.107−1 1.922−2 1.997−1 2.281−2 1.730−1 2.390−2 2.616−3 2.032−2 4.232−3 4.138−2 5.243−3 1.796−2 4.166−3 2.203−2 5.201−3 7.411−1 5.869+0 2.957−2 1.974−2 2.456−1 6.900−2 3.938−1 8.118−2 3.199−1 5.367−3 4.375−3 4.504−2 1.485−2 8.032−2 1.048−2 3.372−2 1.453−2 4.091−2 2.573−1 9.838−3 1.815−2 1.644−2 2.229−1 3.044−2 1.200+0 4.954−2 2.126−3 4.148−3 3.940−3 4.046−2 7.653−3 1.832−1 1.132−2 5.246−2 6.313−3 1.472−2 1.060−2 4.136−2 3.016−2 3.554−1 1.397−1 1.745+0
5.640−2 8.565−2 4.926−2 6.630−2 2.019−2 7.831−3 1.508−2 1.136−2 1.704−2 5.198−3 6.944−3 8.242−3 1.030−2 2.009−1 3.397+0 5.503−2 1.527−2 1.123−1 1.917−2 2.360−1 2.122−2 1.849−1 2.160−2 2.828−3 2.068−2 4.265−3 4.717−2 4.882−3 1.847−2 3.681−3 2.289−2 4.763−3 7.963−1 6.463+0 3.230−2 1.988−2 2.477−1 7.475−2 4.580−1 8.159−2 3.381−1 5.826−3 4.413−3 4.583−2 1.559−2 9.062−2 9.998−3 3.423−2 1.422−2 4.207−2 2.035−1 8.464−3 1.766−2 1.384−2 2.228−1 2.523−2 1.342+0 4.034−2 1.909−3 4.016−3 3.450−3 4.032−2 6.522−3 1.983−1 9.322−3 5.732−2 5.378−3 1.270−2 8.586−3 3.866−2 2.509−2 3.509−1 1.399−1 1.945+0
6.088−2 9.184−2 4.902−2 6.577−2 2.063−2 9.537−3 1.840−2 1.202−2 1.803−2 5.000−3 6.680−3 8.340−3 1.042−2 1.924−1 3.715+0 4.561−2 1.772−2 1.141−1 1.962−2 2.831−1 2.012−2 1.982−1 2.007−2 3.190−3 2.105−2 4.349−3 5.465−2 4.581−3 1.909−2 3.286−3 2.373−2 4.408−3 8.569−1 7.079+0 3.753−2 2.050−2 2.511−1 8.331−2 5.433−1 8.339−2 3.593−1 6.596−3 4.504−3 4.668−2 1.675−2 1.041−1 9.657−3 3.498−2 1.403−2 4.325−2 1.613−1 7.598−3 1.817−2 1.210−2 2.237−1 2.138−2 1.526+0 3.337−2 1.751−3 4.006−3 3.060−3 4.029−2 5.567−3 2.178−1 7.630−3 6.304−2 4.635−3 1.143−2 7.113−3 3.818−2 2.135−2 3.491−1 1.457−1 2.206+0
6.509−2 9.780−2 4.877−2 6.531−2 2.093−2 1.155−2 2.232−2 1.262−2 1.893−2 4.846−3 6.474−3 8.464−3 1.058−2 1.849−1 4.007+0 3.899−2 2.103−2 1.153−1 2.026−2 3.376−1 1.929−2 2.103−1 1.905−2 3.659−3 2.127−2 4.447−3 6.319−2 4.329−3 1.962−2 2.979−3 2.432−2 4.124−3 9.133−1 7.639+0 4.458−2 2.128−2 2.537−1 9.373−2 6.427−1 8.551−2 3.790−1 7.592−3 4.608−3 4.723−2 1.819−2 1.195−1 9.405−3 3.564−2 1.384−2 4.406−2 1.299−1 7.064−3 1.938−2 1.100−2 2.238−1 1.862−2 1.735+0 2.824−2 1.637−3 4.089−3 2.765−3 4.013−2 4.800−3 2.395−1 6.282−3 6.870−2 4.073−3 1.065−2 6.055−3 3.933−2 1.866−2 3.471−1 1.553−1 2.504+0
6.665−2 9.993−2 4.727−2 6.321−2 2.052−2 1.317−2 2.546−2 1.274−2 1.911−2 4.610−3 6.160−3 8.348−3 1.043−2 1.744−1 4.141+0 3.393−2 2.383−2 1.129−1 2.032−2 3.805−1 1.822−2 2.139−1 1.795−2 4.032−3 2.078−2 4.414−3 6.950−2 4.029−3 1.947−2 2.692−3 2.400−2 3.813−3 9.361−1 7.891+0 5.060−2 2.143−2 2.485−1 1.014−1 7.207−1 8.508−2 3.842−1 8.385−3 4.577−3 4.623−2 1.912−2 1.308−1 8.987−3 3.516−2 1.331−2 4.329−2 1.061−1 6.581−3 2.034−2 1.013−2 2.174−1 1.636−2 1.885+0 2.415−2 1.521−3 4.111−3 2.500−3 3.882−2 4.140−3 2.530−1 5.187−3 7.147−2 3.594−3 9.929−3 5.212−3 4.025−2 1.644−2 3.359−1 1.619−1 2.718+0
7.191−2 1.073−1 4.901−2 6.534−2 2.305−2 1.499−2 2.899−2 1.341−2 2.008−2 4.528−3 6.050−3 8.836−3 1.103−2 1.788−1 4.460+0 2.667−2 2.689−2 1.254−1 2.235−2 4.252−1 1.895−2 2.292−1 1.797−2 4.594−3 2.455−2 5.006−3 7.561−2 4.145−3 1.993−2 2.695−3 2.544−2 3.998−3 1.005+0 8.531+0 5.662−2 2.358−2 2.750−1 1.112−1 8.001−1 8.950−2 4.098−1 9.508−3 5.178−3 5.422−2 2.048−2 1.418−1 9.126−3 3.595−2 1.405−2 4.579−2 7.924−2 6.258−3 2.098−2 9.623−3 2.295−1 1.547−2 2.061+0 2.259−2 1.547−3 4.365−3 2.570−3 4.192−2 4.173−3 2.726−1 5.210−3 7.675−2 3.834−3 9.460−3 4.719−3 4.078−2 1.564−2 3.526−1 1.723−1 2.966+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
64
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
3.017−3 3.208−3 9.073−3 1.029−2 6.928−2 2.880−2 2.288−1 1.539−2 6.294−2 5.977+0 1.159+1 5.491−1 8.238−1 5.027−2 6.718−2 3.263−1 4.542−2 8.579−2 9.662−2 1.438−1 1.058−1 1.408−1 5.457−2 6.816−2 7.085−1 1.096+1 9.048−2 4.314−1 4.129−2 2.573−2 3.474−1 4.446−2 2.569−1 4.695−2 3.227−1 3.775−2 1.920−1 3.637−2 2.359+0 2.003+1 1.764−1 7.706−1 5.339−2 4.682−2 7.418−1 1.119−1 5.174−1 1.430−1 5.893−1 1.131−1 3.464−1 3.547−1 1.230+1 8.231−2 2.167−2 3.876−2 2.988−2 7.115−1 4.546−2 1.375+0 6.506−2 8.800−1 6.537−2 9.501−1 1.753+1 3.272−2 1.887−2 8.471−2 4.587−2 1.091+0 1.693−1 2.004+0 1.708−1 1.250+0
4.725−3 3.967−3 1.221−2 1.131−2 6.775−2 3.040−2 2.344−1 1.574−2 6.561−2 6.165+0 1.208+1 5.867−1 1.056+0 1.327−1 1.691−1 3.027−1 4.769−2 8.765−2 9.421−2 1.408−1 1.071−1 1.428−1 5.749−2 7.187−2 7.699−1 1.130+1 1.927−1 5.403−1 1.497−1 3.470−2 3.061−1 3.992−2 2.563−1 4.376−2 3.135−1 3.965−2 1.988−1 3.980−2 2.651+0 2.291+1 3.926−1 1.065+0 7.147−2 4.382−2 6.493−1 1.078−1 5.143−1 1.429−1 5.756−1 1.197−1 3.595−1 6.200−1 1.497+1 3.757−1 2.929−2 5.183−2 3.176−2 6.538−1 4.496−2 1.345+0 6.356−2 8.558−1 6.516−2 1.664+0 2.655+1 4.446−2 1.968−2 1.028−1 4.551−2 1.004+0 1.655−1 1.958+0 1.678−1 1.218+0
4.105−3 3.519−3 1.121−2 1.016−2 6.664−2 2.861−2 2.415−1 1.470−2 6.763−2 6.696+0 1.303+1 5.710−1 9.999−1 1.139−1 1.449−1 3.086−1 5.591−2 1.042−1 1.008−1 1.506−1 1.080−1 1.439−1 5.774−2 7.218−2 7.359−1 1.239+1 1.716−1 5.062−1 1.201−1 3.615−2 3.119−1 4.214−2 2.953−1 4.397−2 3.340−1 3.932−2 1.996−1 3.763−2 2.883+0 2.479+1 3.363−1 9.774−1 7.506−2 4.555−2 6.650−1 1.162−1 5.871−1 1.484−1 6.110−1 1.171−1 3.595−1 5.432−1 1.753+1 2.945−1 2.704−2 5.176−2 3.111−2 6.659−1 4.386−2 1.485+0 5.992−2 9.023−1 6.055−2 1.830+0 2.992+1 4.106−2 1.868−2 1.037−1 4.440−2 1.022+0 1.716−1 2.157+0 1.678−1 1.281+0
3.599−3 3.063−3 1.030−2 8.915−3 6.555−2 2.682−2 2.521−1 1.373−2 7.092−2 7.306+0 1.414+1 5.555−1 9.398−1 9.691−2 1.239−1 3.155−1 6.859−2 1.289−1 1.091−1 1.630−1 1.087−1 1.449−1 5.840−2 7.300−2 7.041−1 1.361+1 1.528−1 4.744−1 9.409−2 4.050−2 3.190−1 4.514−2 3.514−1 4.416−2 3.591−1 3.921−2 2.004−1 3.559−2 3.144+0 2.690+1 2.839−1 8.963−1 8.467−2 4.837−2 6.834−1 1.282−1 6.914−1 1.556−1 6.544−1 1.146−1 3.593−1 4.723−1 2.011+1 2.236−1 2.603−2 5.424−2 3.106−2 6.799−1 4.309−2 1.681+0 5.639−2 9.589−1 5.633−2 1.991+0 3.317+1 3.953−2 1.796−2 1.086−1 4.362−2 1.043+0 1.820−1 2.438+0 1.694−1 1.357+0
3.188−3 2.626−3 9.534−3 7.676−3 6.457−2 2.526−2 2.672−1 1.294−2 7.576−2 7.971+0 1.536+1 5.415−1 8.872−1 8.382−2 1.080−1 3.229−1 8.667−2 1.637−1 1.188−1 1.774−1 1.093−1 1.456−1 5.949−2 7.436−2 6.767−1 1.491+1 1.389−1 4.479−1 7.381−2 4.799−2 3.264−1 4.883−2 4.281−1 4.432−2 3.876−1 3.935−2 2.010−1 3.384−2 3.418+0 2.915+1 2.416−1 8.296−1 1.009−1 5.205−2 7.031−1 1.444−1 8.339−1 1.640−1 7.040−1 1.125−1 3.592−1 4.151−1 2.251+1 1.686−1 2.589−2 5.951−2 3.165−2 6.945−1 4.276−2 1.945+0 5.325−2 1.023+0 5.285−2 2.143+0 3.621+1 3.931−2 1.745−2 1.180−1 4.330−2 1.065+0 1.978−1 2.818+0 1.727−1 1.445+0
2.868−3 2.235−3 8.985−3 6.543−3 6.381−2 2.419−2 2.880−1 1.243−2 8.219−2 8.670+0 1.669+1 5.293−1 8.450−1 7.474−2 9.708−2 3.300−1 1.110−1 2.102−1 1.292−1 1.930−1 1.097−1 1.461−1 6.090−2 7.613−2 6.537−1 1.624+1 1.300−1 4.269−1 5.911−2 5.885−2 3.337−1 5.294−2 5.282−1 4.446−2 4.176−1 3.972−2 2.017−1 3.251−2 3.696+0 3.148+1 2.101−1 7.775−1 1.242−1 5.625−2 7.227−1 1.655−1 1.020+0 1.732−1 7.564−1 1.110−1 3.593−1 3.721−1 2.468+1 1.292−1 2.633−2 6.782−2 3.293−2 7.088−1 4.289−2 2.286+0 5.070−2 1.090+0 5.030−2 2.283+0 3.900+1 3.997−2 1.710−2 1.327−1 4.344−2 1.087+0 2.199−1 3.309+0 1.773−1 1.537+0
2.633−3 1.909−3 8.700−3 5.586−3 6.330−2 2.376−2 3.152−1 1.224−2 8.990−2 9.385+0 1.806+1 5.186−1 8.120−1 6.897−2 9.029−2 3.364−1 1.417−1 2.688−1 1.395−1 2.085−1 1.100−1 1.466−1 6.247−2 7.810−2 6.337−1 1.755+1 1.251−1 4.104−1 4.897−2 7.307−2 3.402−1 5.708−2 6.523−1 4.459−2 4.465−1 4.024−2 2.024−1 3.160−2 3.969+0 3.381+1 1.874−1 7.372−1 1.546−1 6.050−2 7.406−1 1.917−1 1.250+0 1.822−1 8.067−1 1.100−1 3.599−1 3.408−1 2.661+1 1.024−1 2.704−2 7.920−2 3.485−2 7.214−1 4.333−2 2.706+0 4.879−2 1.154+0 4.864−2 2.410+0 4.154+1 4.107−2 1.689−2 1.528−1 4.389−2 1.106+0 2.487−1 3.914+0 1.826−1 1.625+0
2.464−3 1.649−3 8.632−3 4.819−3 6.268−2 2.386−2 3.457−1 1.224−2 9.758−2 1.003+1 1.931+1 5.064−1 7.824−1 6.527−2 8.598−2 3.397−1 1.763−1 3.346−1 1.477−1 2.210−1 1.097−1 1.462−1 6.363−2 7.955−2 6.126−1 1.869+1 1.224−1 3.953−1 4.203−2 8.928−2 3.436−1 6.045−2 7.893−1 4.450−2 4.685−1 4.057−2 2.021−1 3.091−2 4.204+0 3.584+1 1.707−1 7.020−1 1.893−1 6.392−2 7.512−1 2.201−1 1.505+0 1.889−1 8.445−1 1.090−1 3.590−1 3.169−1 2.815+1 8.466−2 2.765−2 9.236−2 3.697−2 7.273−1 4.362−2 3.163+0 4.723−2 1.202+0 4.742−2 2.510+0 4.357+1 4.203−2 1.670−2 1.759−1 4.419−2 1.115+0 2.807−1 4.575+0 1.864−1 1.690+0
2.291−3 1.424−3 8.482−3 4.158−3 6.039−2 2.366−2 3.647−1 1.201−2 1.012−1 1.026+1 1.979+1 4.816−1 7.376−1 6.138−2 8.120−2 3.313−1 2.035−1 3.860−1 1.490−1 2.231−1 1.062−1 1.415−1 6.258−2 7.824−2 5.773−1 1.907+1 1.178−1 3.726−1 3.658−2 1.019−1 3.351−1 6.106−2 8.928−1 4.308−2 4.693−1 3.960−2 1.959−1 2.960−2 4.269+0 3.644+1 1.547−1 6.551−1 2.163−1 6.444−2 7.352−1 2.397−1 1.696+0 1.876−1 8.443−1 1.051−1 3.476−1 2.914−1 2.848+1 7.173−2 2.731−2 1.021−1 3.785−2 7.084−1 4.250−2 3.490+0 4.481−2 1.197+0 4.531−2 2.512+0 4.385+1 4.151−2 1.608−2 1.926−1 4.306−2 1.086+0 3.024−1 5.049+0 1.835−1 1.682+0
2.331−3 1.443−3 8.926−3 4.193−3 6.503−2 2.508−2 3.924−1 1.287−2 1.087−1 1.083+1 2.086+1 5.081−1 7.637−1 6.015−2 8.039−2 3.607−1 2.256−1 4.307−1 1.597−1 2.379−1 1.236−1 1.647−1 6.755−2 8.445−2 6.183−1 2.029+1 1.174−1 3.878−1 3.156−2 1.168−1 3.740−1 6.918−2 9.895−1 4.934−2 4.907−1 4.236−2 2.118−1 3.156−2 4.346+0 3.712+1 1.505−1 6.844−1 2.459−1 7.305−2 8.205−1 2.662−1 1.872+0 1.976−1 8.836−1 1.131−1 3.755−1 2.952−1 3.209+1 5.706−2 2.719−2 1.120−1 4.264−2 7.575−1 5.518−2 3.820+0 4.980−2 1.270+0 4.842−2 2.608+0 5.229+1 4.111−2 1.803−2 2.105−1 5.389−2 1.165+0 3.287−1 5.508+0 1.953−1 1.786+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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65
Table 25 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
3.129−1 7.948−3 1.627−2 1.667−2 6.269−2 3.109−2 8.961−1 6.437−2 4.907+0 1.164−1 1.062−2 9.465−3 3.438−2 2.490−2 1.003−1 6.445−2 1.217+0 3.029−1 6.405+0 1.525+1 2.961+1 1.549+0 2.323+0 1.793−1 2.395−1 4.967−2 6.226−2 1.816+0 2.952+1 2.451−1 1.684+0 1.171−1 1.072−1 3.347−2 6.403+0 5.469+1 6.320−1 2.978+0 7.996−2 1.993−1 9.221−1 4.154+1 1.702−1 1.393+0 8.320−2 3.106+0 7.092+1 2.478−1 1.967+0 5.986−1 3.378+1 1.569−1 1.695+0 4.576+1 5.566−1
1.046+0 1.519−2 1.984−2 1.929−2 7.600−2 3.248−2 8.569−1 6.312−2 4.816+0 1.120−1 1.820−2 1.132−2 3.961−2 2.545−2 1.178−1 6.327−2 1.164+0 2.953−1 6.282+0 1.713+1 3.287+1 1.523+0 2.294+0 2.010−1 2.675−1 5.262−2 6.579−2 1.727+0 3.514+1 2.769−1 1.638+0 1.215−1 1.213−1 3.334−2 8.048+0 6.745+1 6.233−1 2.898+0 8.439−2 2.229−1 8.881−1 7.272+1 1.821−1 1.353+0 8.046−2 6.696+0 1.131+2 2.395−1 1.911+0 5.731−1 7.075+1 1.442−1 4.720+0 9.960+1 4.943−1
8.308−1 1.220−2 1.836−2 1.707−2 7.376−2 2.892−2 8.619−1 5.604−2 5.162+0 9.878−2 1.498−2 9.697−3 3.672−2 2.222−2 1.139−1 5.616−2 1.168+0 2.944−1 6.729+0 1.861+1 3.563+1 1.505+0 2.266+0 2.025−1 2.696−1 5.050−2 6.314−2 1.696+0 3.817+1 2.811−1 1.609+0 1.192−1 1.204−1 3.079−2 8.727+0 7.333+1 6.114−1 2.843+0 8.067−2 2.196−1 8.706−1 7.889+1 1.796−1 1.323+0 7.332−2 7.182+0 1.224+2 2.281−1 1.865+0 5.495−1 7.620+1 1.305−1 4.935+0 1.069+2 4.470−1
6.389−1 1.007−2 1.732−2 1.510−2 7.267−2 2.554−2 8.684−1 4.923−2 5.643+0 8.598−2 1.262−2 8.252−3 3.441−2 1.910−2 1.113−1 4.935−2 1.175+0 2.989−1 7.351+0 2.022+1 3.870+1 1.484+0 2.232+0 2.046−1 2.727−1 4.863−2 6.081−2 1.663+0 4.140+1 2.864−1 1.576+0 1.170−1 1.200−1 2.857−2 9.436+0 7.951+1 5.990−1 2.783+0 7.756−2 2.175−1 8.523−1 8.494+1 1.781−1 1.291+0 6.694−2 7.649+0 1.313+2 2.175−1 1.819+0 5.267−1 8.144+1 1.184−1 5.135+0 1.139+2 4.033−1
4.869−1 8.559−3 1.664−2 1.346−2 7.313−2 2.260−2 8.758−1 4.323−2 6.285+0 7.457−2 1.091−2 7.032−3 3.269−2 1.632−2 1.110−1 4.334−2 1.183+0 3.110−1 8.184+0 2.192+1 4.198+1 1.459+0 2.194+0 2.075−1 2.766−1 4.709−2 5.888−2 1.627+0 4.476+1 2.924−1 1.541+0 1.152−1 1.201−1 2.680−2 1.016+1 8.585+1 5.861−1 2.718+0 7.524−2 2.165−1 8.334−1 9.079+1 1.778−1 1.259+0 6.163−2 8.093+0 1.399+2 2.080−1 1.771+0 5.057−1 8.643+1 1.088−1 5.323+0 1.205+2 3.653−1
3.747−1 7.501−3 1.627−2 1.219−2 7.544−2 2.030−2 8.834−1 3.837−2 7.109+0 6.520−2 9.689−3 6.063−3 3.156−2 1.401−2 1.135−1 3.849−2 1.191+0 3.323−1 9.255+0 2.367+1 4.540+1 1.431+0 2.151+0 2.109−1 2.812−1 4.591−2 5.741−2 1.586+0 4.816+1 2.988−1 1.501+0 1.138−1 1.208−1 2.553−2 1.088+1 9.220+1 5.728−1 2.648+0 7.373−2 2.166−1 8.138−1 9.640+1 1.787−1 1.225+0 5.752−2 8.512+0 1.481+2 1.997−1 1.722+0 4.866−1 9.114+1 1.017−1 5.499+0 1.267+2 3.339−1
2.955−1 6.787−3 1.612−2 1.126−2 7.968−2 1.869−2 8.899−1 3.471−2 8.117+0 5.806−2 8.858−3 5.341−3 3.092−2 1.223−2 1.189−1 3.483−2 1.199+0 3.632−1 1.057+1 2.544+1 4.888+1 1.401+0 2.105+0 2.147−1 2.864−1 4.505−2 5.635−2 1.539+0 5.153+1 3.051−1 1.457+0 1.126−1 1.216−1 2.470−2 1.158+1 9.843+1 5.585−1 2.570+0 7.289−2 2.175−1 7.929−1 1.017+2 1.803−1 1.190+0 5.448−2 8.903+0 1.558+2 1.922−1 1.671+0 4.692−1 9.553+1 9.692−2 5.662+0 1.324+2 3.089−1
2.403−1 6.295−3 1.602−2 1.058−2 8.496−2 1.760−2 8.899−1 3.193−2 9.204+0 5.275−2 8.278−3 4.813−3 3.045−2 1.090−2 1.261−1 3.207−2 1.198+0 3.995−1 1.199+1 2.699+1 5.195+1 1.365+0 2.049+0 2.175−1 2.902−1 4.424−2 5.534−2 1.480+0 5.440+1 3.086−1 1.400+0 1.109−1 1.217−1 2.407−2 1.216+1 1.037+2 5.402−1 2.473+0 7.204−2 2.171−1 7.662−1 1.059+2 1.811−1 1.145+0 5.205−2 9.202+0 1.619+2 1.845−1 1.609+0 4.506−1 9.893+1 9.342−2 5.775+0 1.368+2 2.877−1
1.990−1 5.815−3 1.551−2 9.835−3 8.776−2 1.648−2 8.615−1 2.918−2 9.930+0 4.783−2 7.685−3 4.339−3 2.928−2 9.722−3 1.297−1 2.931−2 1.159+0 4.226−1 1.294+1 2.742+1 5.288+1 1.296+0 1.945+0 2.135−1 2.849−1 4.236−2 5.299−2 1.383+0 5.506+1 3.011−1 1.307+0 1.060−1 1.178−1 2.296−2 1.226+1 1.048+2 5.071−1 2.310+0 6.925−2 2.099−1 7.188−1 1.060+2 1.760−1 1.070+0 4.884−2 9.151+0 1.616+2 1.724−1 1.503+0 4.213−1 9.854+1 8.846−2 5.683+0 1.360+2 2.637−1
1.637−1 6.003−3 1.600−2 1.054−2 8.587−2 1.749−2 9.063−1 3.122−2 1.077+1 5.220−2 8.024−3 4.731−3 3.051−2 1.069−2 1.269−1 3.136−2 1.220+0 4.540−1 1.400+1 2.475+1 4.823+1 1.285+0 1.930+0 2.460−1 3.295−1 4.586−2 5.746−2 1.426+0 5.011+1 3.890−1 1.369+0 1.228−1 1.463−1 2.625−2 1.145+1 9.612+1 5.413−1 2.425+0 8.086−2 2.522−1 7.594−1 1.132+2 1.930−1 1.137+0 5.394−2 8.007+0 2.079+2 1.859−1 1.599+0 4.524−1 9.516+1 4.487−1 4.931+0 1.354+2 2.950−1
66
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
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Table 26 Effective collision strengths for transitions in Ti XX. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.325−1 4.546−1 2.080−2 5.840−3 1.103−2 1.587−2 2.372−2 4.168−3 1.472−3 2.820−3 2.884−3 4.325−3 1.713−3 2.277−3 1.628−3 6.287−4 1.205−3 1.114−3 1.672−3 9.061−4 1.205−3 1.180−4 1.471−4 4.146−2 1.475−3 2.270−2 5.985−3 7.619−2 1.108−2 4.696−4 4.714−3 1.960−3 1.401−2 3.453−3 2.353−3 1.441−3 2.226−4 1.890−3 9.415−4 5.260−3 1.614−3 1.250−3 8.714−4 1.168−4 1.162−4 2.984−3 6.127−3 5.173−2 2.918−2 1.491−1 9.357−4 1.978−3 1.142−2 7.018−3 2.836−2 2.592−3 5.191−3 4.421−4 9.473−4 4.720−3 3.013−3 1.088−2 1.509−3 2.821−3 1.997−4 2.797−4 1.518+0 2.943+0 1.109−1 1.666−1 9.751−2 1.571−2 2.937−2
2.391−1 4.626−1 2.251−2 7.611−3 1.411−2 1.709−2 2.596−2 4.581−3 2.082−3 4.059−3 3.432−3 5.171−3 2.285−3 3.093−3 1.554−3 7.390−4 1.429−3 1.195−3 1.798−3 9.651−4 1.285−3 1.292−4 1.609−4 5.880−2 6.931−3 2.418−2 1.019−2 7.701−2 1.733−2 1.526−3 5.069−3 3.145−3 1.507−2 4.781−3 3.699−3 2.762−3 4.517−4 1.732−3 1.026−3 5.518−3 1.721−3 1.400−3 9.113−4 1.372−4 1.181−4 1.550−2 1.100−2 5.774−2 3.711−2 1.565−1 3.072−3 3.170−3 1.343−2 8.955−3 3.139−2 4.782−3 8.565−3 9.555−4 1.044−3 4.518−3 3.209−3 1.146−2 1.619−3 3.129−3 2.112−4 3.179−4 1.508+0 2.947+0 1.449−1 2.208−1 9.816−2 1.960−2 3.847−2
2.493−1 4.835−1 2.213−2 7.690−3 1.446−2 1.730−2 2.629−2 4.391−3 2.000−3 3.896−3 3.314−3 4.984−3 2.129−3 2.868−3 1.540−3 7.450−4 1.442−3 1.181−3 1.777−3 9.435−4 1.256−3 1.209−4 1.505−4 6.558−2 5.603−3 2.375−2 9.588−3 7.976−2 1.652−2 1.244−3 4.850−3 2.764−3 1.523−2 4.297−3 3.444−3 2.348−3 3.964−4 1.710−3 9.667−4 5.624−3 1.617−3 1.397−3 8.462−4 1.307−4 1.074−4 1.228−2 1.015−2 5.672−2 3.665−2 1.610−1 2.502−3 2.793−3 1.258−2 8.384−3 3.130−2 4.154−3 7.813−3 8.277−4 9.816−4 4.413−3 3.103−3 1.157−2 1.531−3 3.077−3 1.940−4 2.993−4 1.600+0 3.115+0 1.426−1 2.169−1 9.753−2 2.059−2 4.018−2
2.617−1 5.079−1 2.180−2 7.871−3 1.491−2 1.742−2 2.643−2 4.253−3 1.964−3 3.819−3 3.208−3 4.821−3 1.982−3 2.661−3 1.537−3 7.625−4 1.478−3 1.165−3 1.753−3 9.187−4 1.223−3 1.114−4 1.388−4 6.831−2 4.542−3 2.327−2 8.649−3 8.336−2 1.494−2 1.020−3 4.659−3 2.403−3 1.558−2 3.780−3 3.248−3 1.945−3 3.513−4 1.690−3 8.972−4 5.786−3 1.483−3 1.407−3 7.664−4 1.245−4 9.487−5 9.799−3 9.065−3 5.510−2 3.542−2 1.663−1 2.053−3 2.432−3 1.182−2 7.808−3 3.152−2 3.557−3 7.173−3 7.266−4 9.100−4 4.301−3 2.972−3 1.175−2 1.429−3 3.038−3 1.746−4 2.801−4 1.721+0 3.334+0 1.364−1 2.070−1 9.759−2 2.282−2 4.411−2
2.765−1 5.367−1 2.159−2 8.314−3 1.581−2 1.766−2 2.672−2 4.176−3 2.001−3 3.883−3 3.135−3 4.711−3 1.864−3 2.496−3 1.545−3 7.980−4 1.548−3 1.150−3 1.730−3 8.934−4 1.190−3 1.015−4 1.263−4 6.597−2 3.732−3 2.286−2 7.609−3 8.866−2 1.301−2 8.511−4 4.516−3 2.080−3 1.622−2 3.264−3 3.158−3 1.587−3 3.136−4 1.671−3 8.191−4 6.031−3 1.323−3 1.441−3 6.757−4 1.194−4 8.145−5 7.964−3 7.935−3 5.341−2 3.413−2 1.745−1 1.716−3 2.109−3 1.120−2 7.293−3 3.228−2 3.051−3 6.753−3 6.448−4 8.306−4 4.186−3 2.826−3 1.207−2 1.318−3 3.033−3 1.542−4 2.623−4 1.872+0 3.612+0 1.289−1 1.951−1 9.839−2 2.670−2 5.121−2
2.950−1 5.719−1 2.158−2 9.189−3 1.751−2 1.818−2 2.743−2 4.159−3 2.132−3 4.134−3 3.109−3 4.673−3 1.781−3 2.381−3 1.562−3 8.601−4 1.670−3 1.139−3 1.714−3 8.716−4 1.161−3 9.185−5 1.144−4 5.970−2 3.180−3 2.259−2 6.653−3 9.657−2 1.110−2 7.306−4 4.423−3 1.802−3 1.725−2 2.769−3 3.194−3 1.284−3 2.832−4 1.657−3 7.368−4 6.392−3 1.148−3 1.509−3 5.813−4 1.164−4 6.813−5 6.740−3 6.929−3 5.206−2 3.340−2 1.874−1 1.478−3 1.831−3 1.073−2 6.887−3 3.379−2 2.655−3 6.596−3 5.803−4 7.474−4 4.075−3 2.684−3 1.259−2 1.213−3 3.085−3 1.347−4 2.482−4 2.047+0 3.937+0 1.218−1 1.841−1 9.977−2 3.261−2 6.223−2
3.177−1 6.149−1 2.177−2 1.064−2 2.031−2 1.904−2 2.866−2 4.190−3 2.379−3 4.611−3 3.134−3 4.713−3 1.734−3 2.315−3 1.588−3 9.583−4 1.863−3 1.138−3 1.714−3 8.564−4 1.141−3 8.351−5 1.041−4 5.179−2 2.884−3 2.252−2 5.875−3 1.079−1 9.397−3 6.545−4 4.376−3 1.570−3 1.878−2 2.315−3 3.360−3 1.036−3 2.613−4 1.648−3 6.564−4 6.906−3 9.711−4 1.619−3 4.913−4 1.158−4 5.593−5 6.096−3 6.126−3 5.122−2 3.362−2 2.068−1 1.331−3 1.599−3 1.040−2 6.633−3 3.622−2 2.373−3 6.710−3 5.352−4 6.667−4 3.977−3 2.572−3 1.338−2 1.126−3 3.215−3 1.177−4 2.391−4 2.238+0 4.295+0 1.160−1 1.751−1 1.015−1 4.081−2 7.770−2
3.437−1 6.640−1 2.207−2 1.271−2 2.429−2 2.017−2 3.032−2 4.247−3 2.742−3 5.317−3 3.200−3 4.815−3 1.712−3 2.284−3 1.616−3 1.095−3 2.131−3 1.147−3 1.728−3 8.473−4 1.129−3 7.689−5 9.588−5 4.415−2 2.821−3 2.255−2 5.293−3 1.226−1 7.995−3 6.178−4 4.355−3 1.382−3 2.078−2 1.920−3 3.628−3 8.432−4 2.489−4 1.642−3 5.832−4 7.566−3 8.071−4 1.764−3 4.123−4 1.173−4 4.555−5 5.966−3 5.535−3 5.078−2 3.492−2 2.327−1 1.264−3 1.412−3 1.017−2 6.547−3 3.955−2 2.194−3 7.044−3 5.106−4 5.936−4 3.893−3 2.504−3 1.445−2 1.064−3 3.414−3 1.038−4 2.347−4 2.428+0 4.658+0 1.113−1 1.679−1 1.031−1 5.113−2 9.722−2
3.653−1 7.051−1 2.206−2 1.490−2 2.853−2 2.103−2 3.159−2 4.236−3 3.116−3 6.049−3 3.231−3 4.864−3 1.678−3 2.238−3 1.613−3 1.230−3 2.397−3 1.142−3 1.721−3 8.283−4 1.105−3 7.100−5 8.858−5 3.749−2 2.886−3 2.228−2 4.825−3 1.368−1 6.835−3 6.023−4 4.275−3 1.221−3 2.260−2 1.582−3 3.871−3 6.923−4 2.412−4 1.609−3 5.152−4 8.143−3 6.614−4 1.887−3 3.450−4 1.176−4 3.697−5 6.116−3 5.064−3 4.981−2 3.641−2 2.580−1 1.240−3 1.252−3 9.854−3 6.497−3 4.260−2 2.063−3 7.363−3 4.963−4 5.256−4 3.760−3 2.441−3 1.538−2 1.011−3 3.582−3 9.203−5 2.295−4 2.558+0 4.911+0 1.061−1 1.599−1 1.025−1 6.115−2 1.162−1
3.736−1 7.238−1 2.324−2 1.607−2 3.071−2 2.185−2 3.270−2 4.603−3 3.339−3 6.454−3 3.261−3 4.900−3 1.703−3 2.264−3 1.783−3 1.315−3 2.546−3 1.137−3 1.710−3 8.463−4 1.126−3 7.140−5 8.899−5 2.758−2 2.676−3 2.375−2 4.607−3 1.454−1 6.051−3 5.540−4 4.785−3 1.197−3 2.354−2 1.447−3 4.028−3 6.215−4 2.173−4 1.883−3 5.217−4 8.358−3 6.302−4 2.011−3 3.502−4 1.260−4 3.839−5 5.640−3 4.832−3 5.258−2 3.722−2 2.723−1 1.142−3 1.228−3 1.082−2 6.522−3 4.413−2 2.008−3 7.557−3 4.453−4 5.328−4 4.298−3 2.449−3 1.573−2 1.050−3 3.786−3 9.405−5 2.318−4 2.657+0 5.211+0 1.044−1 1.572−1 1.087−1 6.679−2 1.272−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
67
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
4.040−2 6.019−2 4.123−2 5.494−2 1.836−2 3.621−3 6.884−3 8.507−3 1.273−2 4.789−3 6.398−3 7.383−3 9.217−3 1.827−1 2.184+0 2.819−2 6.324−3 1.040−1 1.461−2 1.275−1 1.888−2 1.357−1 2.010−2 1.526−3 2.024−2 4.036−3 2.665−2 5.387−3 1.444−2 4.639−3 1.745−2 5.772−3 5.039−1 4.149+0 1.307−2 1.536−2 2.239−1 4.991−2 2.527−1 6.534−2 2.498−1 3.047−3 4.158−3 4.467−2 1.206−2 5.352−2 1.009−2 2.802−2 1.375−2 3.354−2 1.329−1 5.591−3 1.044−2 1.079−2 2.008−1 2.576−2 8.778−1 4.554−2 1.822−3 3.269−3 4.147−3 3.858−2 9.427−3 1.388−1 1.517−2 3.786−2 8.760−3 8.427−3 7.341−3 2.468−2 2.585−2 3.146−1 1.121−1 1.279+0
4.172−2 6.699−2 4.881−2 6.972−2 1.708−2 4.238−3 8.047−3 8.712−3 1.307−2 5.770−3 7.710−3 7.866−3 9.833−3 2.247−1 2.227+0 9.440−2 1.421−2 9.922−2 2.012−2 1.285−1 2.775−2 1.368−1 3.294−2 2.474−3 1.769−2 3.988−3 2.854−2 5.845−3 1.539−2 5.276−3 1.798−2 6.119−3 5.813−1 4.227+0 3.064−2 2.136−2 2.227−1 6.009−2 2.753−1 8.206−2 2.746−1 5.630−3 4.200−3 3.951−2 1.298−2 5.735−2 1.121−2 3.021−2 1.442−2 3.472−2 3.723−1 1.819−2 2.466−2 2.755−2 2.096−1 4.978−2 8.756−1 8.273−2 3.255−3 4.583−3 5.185−3 3.744−2 1.034−2 1.418−1 1.622−2 3.957−2 8.878−3 2.652−2 1.924−2 6.424−2 4.943−2 3.647−1 1.523−1 1.317+0
4.268−2 6.762−2 4.731−2 6.690−2 1.723−2 4.524−3 8.612−3 8.925−3 1.339−2 5.505−3 7.355−3 7.688−3 9.610−3 2.175−1 2.338+0 8.895−2 1.244−2 9.903−2 1.861−2 1.380−1 2.517−2 1.404−1 2.900−2 2.304−3 1.784−2 3.903−3 3.024−2 5.515−3 1.552−2 4.822−3 1.840−2 5.683−3 5.985−1 4.424+0 2.673−2 1.961−2 2.207−1 5.905−2 2.886−1 7.800−2 2.758−1 5.075−3 4.083−3 3.974−2 1.292−2 6.021−2 1.065−2 3.007−2 1.397−2 3.513−2 3.482−1 1.428−2 2.112−2 2.279−2 2.063−1 4.212−2 9.144−1 6.983−2 2.735−3 4.241−3 4.659−3 3.711−2 9.333−3 1.464−1 1.446−2 4.097−2 7.897−3 2.104−2 1.569−2 5.387−2 4.178−2 3.519−1 1.411−1 1.364+0
4.438−2 6.918−2 4.599−2 6.418−2 1.749−2 5.008−3 9.555−3 9.228−3 1.384−2 5.218−3 6.973−3 7.535−3 9.419−3 2.067−1 2.507+0 7.727−2 1.162−2 9.931−2 1.750−2 1.527−1 2.276−2 1.461−1 2.529−2 2.241−3 1.807−2 3.841−3 3.275−2 5.154−3 1.573−2 4.327−3 1.896−2 5.216−3 6.241−1 4.750+0 2.487−2 1.842−2 2.196−1 5.936−2 3.114−1 7.490−2 2.804−1 4.821−3 4.004−3 4.015−2 1.300−2 6.454−2 1.007−2 3.006−2 1.353−2 3.578−2 2.995−1 1.137−2 1.843−2 1.858−2 2.035−1 3.478−2 9.741−1 5.740−2 2.338−3 3.950−3 4.127−3 3.681−2 8.227−3 1.531−1 1.252−2 4.318−2 6.866−3 1.687−2 1.256−2 4.549−2 3.453−2 3.389−1 1.319−1 1.439+0
4.696−2 7.217−2 4.504−2 6.207−2 1.782−2 5.756−3 1.101−2 9.635−3 1.445−2 4.940−3 6.601−3 7.440−3 9.299−3 1.950−1 2.734+0 6.392−2 1.176−2 1.001−1 1.695−2 1.746−1 2.079−2 1.543−1 2.224−2 2.288−3 1.835−2 3.814−3 3.634−2 4.792−3 1.607−2 3.834−3 1.966−2 4.762−3 6.627−1 5.202+0 2.510−2 1.787−2 2.202−1 6.166−2 3.480−1 7.335−2 2.898−1 4.849−3 3.970−3 4.071−2 1.330−2 7.084−2 9.518−3 3.025−2 1.315−2 3.666−2 2.438−1 9.293−3 1.672−2 1.522−2 2.018−1 2.852−2 1.061+0 4.662−2 2.030−3 3.729−3 3.618−3 3.658−2 7.107−3 1.626−1 1.055−2 4.637−2 5.874−3 1.387−2 1.003−2 3.957−2 2.837−2 3.288−1 1.265−1 1.555+0
5.037−2 7.659−2 4.447−2 6.067−2 1.820−2 6.837−3 1.311−2 1.014−2 1.522−2 4.699−3 6.279−3 7.427−3 9.283−3 1.846−1 3.000+0 5.203−2 1.289−2 1.014−1 1.693−2 2.052−1 1.931−2 1.646−1 1.995−2 2.456−3 1.867−2 3.833−3 4.125−2 4.459−3 1.652−2 3.387−3 2.044−2 4.356−3 7.117−1 5.732+0 2.746−2 1.790−2 2.224−1 6.634−2 4.017−1 7.343−2 3.042−1 5.164−3 3.988−3 4.138−2 1.389−2 7.958−2 9.063−3 3.068−2 1.286−2 3.770−2 1.933−1 7.890−3 1.602−2 1.275−2 2.015−1 2.357−2 1.182+0 3.790−2 1.795−3 3.597−3 3.168−3 3.644−2 6.065−3 1.755−1 8.718−3 5.056−2 5.000−3 1.183−2 8.084−3 3.611−2 2.351−2 3.222−1 1.258−1 1.721+0
5.438−2 8.209−2 4.424−2 5.990−2 1.860−2 8.308−3 1.596−2 1.073−2 1.610−2 4.514−3 6.032−3 7.505−3 9.381−3 1.760−1 3.285+0 4.285−2 1.500−2 1.030−1 1.736−2 2.457−1 1.827−2 1.764−1 1.840−2 2.757−3 1.900−2 3.900−3 4.768−2 4.179−3 1.708−2 3.018−3 2.122−2 4.024−3 7.665−1 6.292+0 3.195−2 1.840−2 2.257−1 7.357−2 4.744−1 7.486−2 3.222−1 5.774−3 4.058−3 4.213−2 1.487−2 9.115−2 8.737−3 3.134−2 1.268−2 3.880−2 1.528−1 6.998−3 1.625−2 1.107−2 2.021−1 1.988−2 1.340+0 3.123−2 1.626−3 3.574−3 2.804−3 3.641−2 5.172−3 1.923−1 7.142−3 5.563−2 4.295−3 1.053−2 6.659−3 3.492−2 1.990−2 3.187−1 1.299−1 1.943+0
5.846−2 8.786−2 4.416−2 5.949−2 1.895−2 1.014−2 1.952−2 1.133−2 1.699−2 4.382−3 5.856−3 7.641−3 9.550−3 1.691−1 3.564+0 3.638−2 1.797−2 1.045−1 1.803−2 2.949−1 1.754−2 1.882−1 1.741−2 3.176−3 1.926−2 3.997−3 5.545−2 3.952−3 1.763−2 2.733−3 2.187−2 3.765−3 8.212−1 6.832+0 3.831−2 1.915−2 2.291−1 8.301−2 5.642−1 7.698−2 3.408−1 6.647−3 4.161−3 4.278−2 1.618−2 1.052−1 8.521−3 3.206−2 1.255−2 3.973−2 1.226−1 6.460−3 1.727−2 1.002−2 2.028−1 1.724−2 1.530+0 2.633−2 1.509−3 3.652−3 2.531−3 3.639−2 4.454−3 2.124−1 5.878−3 6.101−2 3.764−3 9.739−3 5.642−3 3.556−2 1.731−2 3.167−1 1.384−1 2.212+0
6.096−2 9.140−2 4.341−2 5.827−2 1.887−2 1.188−2 2.289−2 1.164−2 1.746−2 4.224−3 5.644−3 7.655−3 9.567−3 1.611−1 3.749+0 3.172−2 2.096−2 1.037−1 1.841−2 3.407−1 1.676−2 1.948−1 1.655−2 3.584−3 1.910−2 4.029−3 6.245−2 3.719−3 1.779−2 2.491−3 2.194−2 3.518−3 8.560−1 7.184+0 4.473−2 1.959−2 2.279−1 9.170−2 6.480−1 7.778−2 3.510−1 7.504−3 4.195−3 4.251−2 1.733−2 1.178−1 8.248−3 3.213−2 1.223−2 3.967−2 1.002−1 6.057−3 1.841−2 9.304−3 1.998−1 1.523−2 1.698+0 2.260−2 1.411−3 3.731−3 2.308−3 3.570−2 3.865−3 2.289−1 4.876−3 6.475−2 3.342−3 9.146−3 4.876−3 3.673−2 1.533−2 3.100−1 1.467−1 2.452+0
6.442−2 9.605−2 4.418−2 5.890−2 2.071−2 1.300−2 2.505−2 1.198−2 1.794−2 4.076−3 5.448−3 7.944−3 9.920−3 1.619−1 3.945+0 2.400−2 2.285−2 1.125−1 1.988−2 3.684−1 1.711−2 2.045−1 1.620−2 3.923−3 2.201−2 4.460−3 6.573−2 3.764−3 1.785−2 2.458−3 2.280−2 3.633−3 9.005−1 7.600+0 4.839−2 2.110−2 2.466−1 9.757−2 6.959−1 8.016−2 3.661−1 8.149−3 4.630−3 4.861−2 1.805−2 1.237−1 8.230−3 3.223−2 1.268−2 4.115−2 7.258−2 5.590−3 1.834−2 8.606−3 2.069−1 1.411−2 1.803+0 2.076−2 1.391−3 3.847−3 2.330−3 3.781−2 3.854−3 2.398−1 4.873−3 6.799−2 3.531−3 8.458−3 4.303−3 3.574−2 1.428−2 3.181−1 1.519−1 2.595+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
68
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.739−3 2.932−3 8.229−3 9.429−3 6.262−2 2.621−2 2.053−1 1.401−2 5.630−2 5.347+0 1.033+1 4.966−1 7.450−1 4.520−2 6.042−2 2.938−1 3.991−2 7.486−2 8.666−2 1.289−1 9.553−2 1.271−1 4.913−2 6.137−2 6.408−1 9.699+0 8.128−2 3.902−1 3.759−2 2.217−2 3.124−1 3.953−2 2.248−1 4.226−2 2.878−1 3.401−2 1.731−1 3.304−2 2.091+0 1.772+1 1.599−1 6.974−1 4.610−2 4.187−2 6.670−1 9.986−2 4.556−1 1.282−1 5.267−1 1.023−1 3.125−1 3.215−1 1.086+1 7.515−2 1.935−2 3.432−2 2.683−2 6.409−1 4.110−2 1.217+0 5.916−2 7.868−1 5.955−2 8.251−1 1.471+1 2.922−2 1.706−2 7.530−2 4.150−2 9.831−1 1.517−1 1.775+0 1.540−1 1.119+0
4.766−3 3.691−3 1.108−2 1.037−2 6.148−2 2.759−2 2.101−1 1.438−2 5.881−2 5.482+0 1.118+1 5.476−1 8.914−1 1.184−1 1.690−1 2.740−1 4.223−2 7.733−2 8.452−2 1.263−1 9.668−2 1.288−1 5.168−2 6.460−2 7.537−1 9.988+0 1.651−1 4.854−1 1.472−1 2.943−2 2.757−1 3.587−2 2.245−1 3.951−2 2.801−1 3.567−2 1.789−1 3.612−2 2.436+0 2.034+1 3.384−1 1.013+0 6.665−2 3.949−2 5.858−1 9.630−2 4.537−1 1.281−1 5.151−1 1.082−1 3.241−1 5.360−1 1.295+1 3.763−1 2.744−2 4.468−2 2.842−2 5.885−1 4.067−2 1.189+0 5.786−2 7.660−1 5.926−2 1.553+0 2.579+1 4.366−2 1.757−2 9.281−2 4.115−2 9.051−1 1.483−1 1.733+0 1.513−1 1.090+0
4.034−3 3.270−3 1.017−2 9.357−3 6.047−2 2.602−2 2.159−1 1.344−2 6.038−2 5.958+0 1.196+1 5.320−1 8.534−1 1.022−1 1.446−1 2.788−1 4.912−2 9.109−2 9.018−2 1.347−1 9.746−2 1.299−1 5.182−2 6.477−2 7.148−1 1.092+1 1.477−1 4.563−1 1.188−1 3.072−2 2.810−1 3.763−2 2.574−1 3.967−2 2.975−1 3.533−2 1.797−1 3.413−2 2.633+0 2.203+1 2.921−1 9.269−1 6.769−2 4.085−2 5.993−1 1.034−1 5.152−1 1.327−1 5.452−1 1.058−1 3.239−1 4.732−1 1.517+1 2.984−1 2.491−2 4.489−2 2.781−2 5.995−1 3.961−2 1.307+0 5.453−2 8.056−1 5.503−2 1.693+0 2.872+1 3.911−2 1.674−2 9.275−2 4.009−2 9.211−1 1.532−1 1.902+0 1.510−1 1.144+0
3.468−3 2.848−3 9.336−3 8.247−3 5.946−2 2.441−2 2.248−1 1.253−2 6.307−2 6.512+0 1.286+1 5.149−1 8.129−1 8.724−2 1.222−1 2.847−1 5.983−2 1.119−1 9.737−2 1.454−1 9.812−2 1.308−1 5.233−2 6.541−2 6.749−1 1.201+1 1.324−1 4.286−1 9.297−2 3.436−2 2.873−1 4.014−2 3.047−1 3.981−2 3.191−1 3.518−2 1.804−1 3.225−2 2.853+0 2.393+1 2.486−1 8.437−1 7.443−2 4.322−2 6.154−1 1.134−1 6.032−1 1.389−1 5.827−1 1.035−1 3.237−1 4.148−1 1.747+1 2.271−1 2.366−2 4.710−2 2.770−2 6.120−1 3.883−2 1.473+0 5.128−2 8.546−1 5.113−2 1.826+0 3.121+1 3.676−2 1.613−2 9.618−2 3.932−2 9.395−1 1.616−1 2.140+0 1.521−1 1.210+0
3.024−3 2.444−3 8.628−3 7.125−3 5.854−2 2.297−2 2.375−1 1.177−2 6.713−2 7.119+0 1.388+1 4.989−1 7.769−1 7.550−2 1.047−1 2.911−1 7.526−2 1.414−1 1.059−1 1.581−1 9.861−2 1.314−1 5.326−2 6.657−2 6.396−1 1.317+1 1.213−1 4.051−1 7.240−2 4.064−2 2.940−1 4.331−2 3.697−1 3.993−2 3.441−1 3.528−2 1.809−1 3.062−2 3.088+0 2.596+1 2.132−1 7.741−1 8.722−2 4.640−2 6.330−1 1.272−1 7.243−1 1.463−1 6.263−1 1.015−1 3.235−1 3.673−1 1.964+1 1.705−1 2.331−2 5.164−2 2.814−2 6.252−1 3.845−2 1.698+0 4.836−2 9.109−1 4.788−2 1.951+0 3.343+1 3.593−2 1.568−2 1.037−1 3.896−2 9.592−1 1.748−1 2.462+0 1.548−1 1.287+0
2.685−3 2.080−3 8.105−3 6.082−3 5.781−2 2.191−2 2.552−1 1.126−2 7.266−2 7.759+0 1.501+1 4.851−1 7.473−1 6.727−2 9.236−2 2.975−1 9.621−2 1.813−1 1.153−1 1.720−1 9.898−2 1.319−1 5.452−2 6.815−2 6.104−1 1.436+1 1.142−1 3.864−1 5.732−2 4.980−2 3.007−1 4.692−2 4.553−1 4.002−2 3.710−1 3.560−2 1.815−1 2.937−2 3.330+0 2.807+1 1.866−1 7.197−1 1.065−1 5.013−2 6.507−1 1.453−1 8.837−1 1.545−1 6.733−1 1.000−1 3.236−1 3.314−1 2.162+1 1.291−1 2.356−2 5.879−2 2.919−2 6.382−1 3.850−2 1.990+0 4.597−2 9.710−1 4.547−2 2.068+0 3.552+1 3.612−2 1.538−2 1.159−1 3.903−2 9.787−1 1.935−1 2.883+0 1.587−1 1.370+0
2.438−3 1.774−3 7.815−3 5.189−3 5.732−2 2.142−2 2.786−1 1.103−2 7.946−2 8.415+0 1.621+1 4.735−1 7.237−1 6.200−2 8.444−2 3.034−1 1.231−1 2.323−1 1.247−1 1.863−1 9.931−2 1.323−1 5.597−2 6.997−2 5.865−1 1.555+1 1.106−1 3.716−1 4.684−2 6.196−2 3.067−1 5.066−2 5.628−1 4.013−2 3.974−1 3.608−2 1.822−1 2.851−2 3.573+0 3.020+1 1.674−1 6.781−1 1.324−1 5.402−2 6.672−1 1.681−1 1.084+0 1.628−1 7.194−1 9.912−2 3.241−1 3.052−1 2.340+1 1.007−1 2.416−2 6.868−2 3.083−2 6.500−1 3.888−2 2.354+0 4.417−2 1.030+0 4.389−2 2.177+0 3.750+1 3.693−2 1.519−2 1.330−1 3.943−2 9.966−1 2.183−1 3.408+0 1.635−1 1.451+0
2.268−3 1.530−3 7.752−3 4.472−3 5.692−2 2.149−2 3.068−1 1.104−2 8.676−2 9.042+0 1.739+1 4.625−1 7.030−1 5.881−2 7.960−2 3.076−1 1.548−1 2.923−1 1.329−1 1.988−1 9.945−2 1.325−1 5.729−2 7.163−2 5.649−1 1.667+1 1.091−1 3.591−1 3.975−2 7.652−2 3.110−1 5.402−2 6.875−1 4.019−2 4.197−1 3.653−2 1.826−1 2.796−2 3.799+0 3.219+1 1.535−1 6.445−1 1.635−1 5.750−2 6.797−1 1.943−1 1.316+0 1.698−1 7.579−1 9.852−2 3.244−1 2.855−1 2.492+1 8.188−2 2.482−2 8.075−2 3.285−2 6.582−1 3.930−2 2.772+0 4.283−2 1.079+0 4.289−2 2.273+0 3.927+1 3.787−2 1.508−2 1.540−1 3.987−2 1.009+0 2.477−1 4.012+0 1.678−1 1.518+0
2.122−3 1.329−3 7.724−3 3.883−3 5.559−2 2.161−2 3.302−1 1.098−2 9.181−2 9.423+0 1.812+1 4.446−1 6.734−1 5.604−2 7.551−2 3.046−1 1.839−1 3.472−1 1.366−1 2.045−1 9.766−2 1.301−1 5.727−2 7.160−2 5.365−1 1.731+1 1.069−1 3.427−1 3.458−2 8.983−2 3.079−1 5.562−2 7.988−1 3.948−2 4.280−1 3.622−2 1.795−1 2.714−2 3.921+0 3.330+1 1.411−1 6.069−1 1.921−1 5.910−2 6.754−1 2.165−1 1.523+0 1.715−1 7.711−1 9.639−2 3.187−1 2.664−1 2.567+1 6.891−2 2.494−2 9.159−2 3.424−2 6.508−1 3.887−2 3.135+0 4.115−2 1.093+0 4.154−2 2.309+0 4.002+1 3.802−2 1.474−2 1.727−1 3.945−2 9.977−1 2.727−1 4.536+0 1.678−1 1.537+0
2.097−3 1.328−3 7.911−3 3.873−3 5.870−2 2.238−2 3.454−1 1.156−2 9.638−2 9.730+0 1.864+1 4.599−1 6.914−1 5.384−2 7.196−2 3.236−1 1.974−1 3.751−1 1.437−1 2.140−1 1.113−1 1.484−1 6.053−2 7.568−2 5.605−1 1.805+1 1.052−1 3.512−1 2.858−2 9.956−2 3.349−1 6.155−2 8.577−1 4.457−2 4.408−1 3.801−2 1.902−1 2.837−2 3.906+0 3.329+1 1.362−1 6.198−1 2.108−1 6.537−2 7.351−1 2.339−1 1.629+0 1.778−1 7.951−1 1.017−1 3.375−1 2.674−1 2.785+1 5.159−2 2.450−2 9.748−2 3.770−2 6.828−1 4.217−2 3.330+0 4.506−2 1.139+0 4.380−2 2.372+0 4.466+1 3.707−2 1.629−2 1.832−1 4.286−2 1.047+0 2.886−1 4.804+0 1.756−1 1.603+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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69
Table 26 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.10
6.30
6.50
6.70
6.90
7.10
7.30
7.50
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.863−1 7.219−3 1.471−2 1.521−2 5.643−2 2.848−2 8.084−1 5.900−2 4.371+0 1.068−1 9.644−3 8.678−3 3.115−2 2.288−2 9.052−2 5.908−2 1.098+0 2.731−1 5.707+0 1.354+1 2.675+1 1.402+0 2.102+0 1.604−1 2.144−1 4.497−2 5.638−2 1.644+0 2.599+1 2.196−1 1.524+0 1.059−1 9.634−2 3.051−2 5.652+0 4.823+1 5.719−1 2.696+0 7.240−2 1.793−1 8.347−1 3.486+1 1.534−1 1.262+0 7.603−2 2.683+0 5.763+1 2.243−1 1.781+0 5.436−1 2.870+1 1.435−1 1.456+0 3.882+1 5.095−1
1.012+0 1.388−2 1.810−2 1.799−2 6.745−2 2.979−2 7.735−1 5.774−2 4.289+0 1.032−1 1.835−2 1.103−2 3.682−2 2.354−2 1.071−1 5.790−2 1.050+0 2.664−1 5.601+0 1.532+1 2.924+1 1.392+0 2.093+0 1.793−1 2.388−1 4.757−2 5.947−2 1.579+0 3.100+1 2.469−1 1.495+0 1.094−1 1.088−1 3.040−2 7.162+0 5.982+1 5.672−1 2.639+0 7.628−2 2.002−1 8.094−1 6.287+1 1.641−1 1.234+0 7.362−2 5.906+0 9.828+1 2.189−1 1.742+0 5.228−1 6.093+1 1.330−1 4.190+0 8.598+1 4.569−1
8.127−1 1.114−2 1.668−2 1.583−2 6.561−2 2.654−2 7.776−1 5.134−2 4.583+0 9.110−2 1.476−2 9.318−3 3.382−2 2.056−2 1.030−1 5.147−2 1.054+0 2.647−1 5.978+0 1.666+1 3.171+1 1.372+0 2.063+0 1.805−1 2.405−1 4.558−2 5.699−2 1.547+0 3.371+1 2.506−1 1.465+0 1.072−1 1.079−1 2.801−2 7.784+0 6.516+1 5.554−1 2.585+0 7.276−2 1.970−1 7.919−1 6.860+1 1.614−1 1.204+0 6.694−2 6.367+0 1.069+2 2.080−1 1.697+0 5.005−1 6.605+1 1.198−1 4.396+0 9.286+1 4.122−1
6.275−1 9.184−3 1.568−2 1.394−2 6.463−2 2.342−2 7.833−1 4.513−2 4.990+0 7.929−2 1.220−2 7.846−3 3.147−2 1.767−2 1.002−1 4.525−2 1.059+0 2.676−1 6.505+0 1.812+1 3.446+1 1.349+0 2.029+0 1.824−1 2.432−1 4.381−2 5.479−2 1.514+0 3.662+1 2.553−1 1.434+0 1.053−1 1.074−1 2.591−2 8.434+0 7.079+1 5.433−1 2.527+0 6.981−2 1.948−1 7.740−1 7.424+1 1.598−1 1.174+0 6.095−2 6.811+0 1.154+2 1.979−1 1.653+0 4.789−1 7.098+1 1.082−1 4.589+0 9.944+1 3.708−1
4.773−1 7.786−3 1.502−2 1.237−2 6.494−2 2.069−2 7.899−1 3.960−2 5.537+0 6.870−2 1.036−2 6.627−3 2.973−2 1.508−2 9.940−2 3.972−2 1.067+0 2.770−1 7.213+0 1.966+1 3.742+1 1.325+0 1.992+0 1.849−1 2.466−1 4.237−2 5.299−2 1.479+0 3.965+1 2.606−1 1.400+0 1.036−1 1.075−1 2.424−2 9.094+0 7.656+1 5.311−1 2.467+0 6.760−2 1.937−1 7.561−1 7.967+1 1.593−1 1.143+0 5.598−2 7.229+0 1.234+2 1.889−1 1.608+0 4.592−1 7.565+1 9.895−2 4.767+0 1.056+2 3.348−1
3.649−1 6.805−3 1.465−2 1.115−2 6.686−2 1.853−2 7.967−1 3.509−2 6.244+0 5.993−2 9.064−3 5.666−3 2.858−2 1.292−2 1.011−1 3.520−2 1.074+0 2.945−1 8.131+0 2.125+1 4.052+1 1.299+0 1.952+0 1.880−1 2.508−1 4.127−2 5.163−2 1.441+0 4.272+1 2.665−1 1.363+0 1.023−1 1.080−1 2.304−2 9.751+0 8.234+1 5.189−1 2.403+0 6.616−2 1.938−1 7.380−1 8.485+1 1.600−1 1.112+0 5.212−2 7.622+0 1.310+2 1.812−1 1.563+0 4.416−1 8.004+1 9.214−2 4.933+0 1.114+2 3.053−1
2.850−1 6.140−3 1.451−2 1.026−2 7.052−2 1.698−2 8.030−1 3.165−2 7.120+0 5.319−2 8.187−3 4.952−3 2.792−2 1.125−2 1.056−1 3.178−2 1.082+0 3.208−1 9.272+0 2.287+1 4.368+1 1.272+0 1.911+0 1.916−1 2.556−1 4.050−2 5.067−2 1.400+0 4.578+1 2.725−1 1.324+0 1.013−1 1.089−1 2.226−2 1.040+1 8.804+1 5.061−1 2.333+0 6.538−2 1.946−1 7.190−1 8.974+1 1.615−1 1.080+0 4.930−2 7.987+0 1.381+2 1.744−1 1.517+0 4.258−1 8.413+1 8.756−2 5.086+0 1.168+2 2.818−1
2.296−1 5.699−3 1.448−2 9.636−3 7.552−2 1.598−2 8.062−1 2.913−2 8.120+0 4.827−2 7.604−3 4.442−3 2.755−2 1.001−2 1.123−1 2.926−2 1.085+0 3.540−1 1.058+1 2.438+1 4.668+1 1.245+0 1.872+0 1.952−1 2.602−1 3.991−2 4.993−2 1.352+0 4.862+1 2.771−1 1.278+0 1.002−1 1.094−1 2.175−2 1.098+1 9.326+1 4.911−1 2.252+0 6.486−2 1.952−1 6.970−1 9.404+1 1.629−1 1.043+0 4.719−2 8.300+0 1.443+2 1.678−1 1.465+0 4.101−1 8.766+1 8.452−2 5.213+0 1.214+2 2.628−1
1.897−1 5.328−3 1.424−2 9.055−3 7.951−2 1.513−2 7.919−1 2.688−2 8.955+0 4.417−2 7.112−3 4.031−3 2.687−2 8.997−3 1.176−1 2.703−2 1.065+0 3.820−1 1.167+1 2.522+1 4.838+1 1.203+0 1.813+0 1.950−1 2.599−1 3.879−2 4.853−2 1.281+0 5.010+1 2.749−1 1.210+0 9.719−2 1.076−1 2.103−2 1.126+1 9.588+1 4.667−1 2.130+0 6.325−2 1.915−1 6.618−1 9.575+1 1.608−1 9.869−1 4.484−2 8.392+0 1.466+2 1.588−1 1.386+0 3.882−1 8.883+1 8.106−2 5.212+0 1.228+2 2.434−1
1.499−1 5.418−3 1.450−2 9.580−3 7.677−2 1.570−2 8.185−1 2.864−2 9.442+0 4.784−2 7.244−3 4.322−3 2.764−2 9.829−3 1.130−1 2.878−2 1.102+0 4.002−1 1.227+1 2.274+1 4.964+1 1.176+0 1.767+0 2.236−1 2.998−1 4.176−2 5.235−2 1.307+0 4.493+1 3.575−1 1.253+0 1.124−1 1.337−1 2.398−2 1.043+1 8.690+1 4.943−1 2.219+0 7.350−2 2.294−1 6.956−1 9.707+1 1.770−1 1.038+0 4.908−2 7.361+0 1.736+2 1.695−1 1.459+0 4.123−1 8.355+1 8.950−2 4.430+0 1.211+2 2.689−1
70
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 27 Effective collision strengths for transitions in V XXI. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
2.148−1 4.183−1 1.893−2 5.452−3 1.024−2 1.451−2 2.169−2 3.788−3 1.362−3 2.599−3 2.619−3 3.929−3 1.558−3 2.070−3 1.477−3 5.793−4 1.107−3 1.009−3 1.514−3 8.223−4 1.093−3 1.063−4 1.325−4 3.731−2 1.339−3 2.057−2 5.387−3 6.972−2 9.939−3 4.246−4 4.262−3 1.760−3 1.279−2 3.089−3 2.147−3 1.287−3 2.008−4 1.706−3 8.436−4 4.797−3 1.443−3 1.139−3 7.778−4 1.054−4 1.034−4 2.712−3 5.530−3 4.687−2 2.651−2 1.365−1 8.459−4 1.778−3 1.032−2 6.340−3 2.588−2 2.334−3 4.728−3 3.986−4 8.494−4 4.255−3 2.716−3 9.910−3 1.357−3 2.564−3 1.787−4 2.521−4 1.408+0 2.720+0 1.005−1 1.509−1 8.873−2 1.500−2 2.788−2
2.194−1 4.271−1 2.107−2 7.020−3 1.333−2 1.581−2 2.383−2 4.225−3 1.897−3 3.673−3 3.101−3 4.700−3 2.043−3 2.739−3 1.398−3 6.773−4 1.303−3 1.079−3 1.622−3 8.705−4 1.158−3 1.154−4 1.436−4 5.584−2 6.510−3 2.158−2 9.306−3 7.104−2 1.571−2 1.349−3 4.604−3 2.736−3 1.378−2 4.245−3 3.298−3 2.384−3 3.529−4 1.577−3 9.180−4 5.031−3 1.529−3 1.261−3 8.080−4 1.218−4 1.046−4 1.318−2 9.801−3 5.538−2 3.399−2 1.437−1 2.550−3 2.837−3 1.185−2 8.038−3 2.866−2 4.237−3 7.573−3 7.192−4 9.340−4 4.086−3 2.883−3 1.042−2 1.445−3 2.817−3 1.879−4 2.831−4 1.399+0 2.726+0 1.314−1 2.004−1 9.375−2 1.845−2 3.484−2
2.301−1 4.472−1 2.051−2 7.139−3 1.360−2 1.596−2 2.403−2 4.045−3 1.831−3 3.541−3 2.991−3 4.522−3 1.899−3 2.539−3 1.394−3 6.857−4 1.322−3 1.065−3 1.602−3 8.499−4 1.131−3 1.076−4 1.339−4 6.110−2 5.164−3 2.135−2 8.596−3 7.371−2 1.471−2 1.091−3 4.393−3 2.403−3 1.396−2 3.784−3 3.072−3 2.008−3 3.205−4 1.555−3 8.606−4 5.139−3 1.427−3 1.263−3 7.452−4 1.163−4 9.448−5 1.046−2 8.999−3 5.330−2 3.327−2 1.477−1 2.095−3 2.478−3 1.115−2 7.500−3 2.862−2 3.654−3 6.907−3 6.512−4 8.742−4 3.989−3 2.778−3 1.054−2 1.362−3 2.774−3 1.718−4 2.665−4 1.489+0 2.887+0 1.280−1 1.947−1 9.253−2 1.967−2 3.706−2
2.424−1 4.704−1 2.009−2 7.374−3 1.405−2 1.606−2 2.416−2 3.915−3 1.813−3 3.502−3 2.898−3 4.375−3 1.771−3 2.364−3 1.398−3 7.057−4 1.363−3 1.050−3 1.580−3 8.272−4 1.101−3 9.884−5 1.230−4 6.216−2 4.127−3 2.101−2 7.657−3 7.731−2 1.311−2 8.908−4 4.220−3 2.089−3 1.433−2 3.306−3 2.916−3 1.656−3 2.909−4 1.535−3 7.943−4 5.304−3 1.298−3 1.278−3 6.698−4 1.110−4 8.286−5 8.377−3 7.995−3 5.111−2 3.202−2 1.532−1 1.734−3 2.146−3 1.053−2 6.978−3 2.892−2 3.120−3 6.379−3 5.902−4 8.063−4 3.885−3 2.654−3 1.074−2 1.266−3 2.748−3 1.538−4 2.495−4 1.607+0 3.099+0 1.218−1 1.848−1 9.183−2 2.208−2 4.156−2
2.569−1 4.979−1 1.985−2 7.883−3 1.501−2 1.631−2 2.451−2 3.843−3 1.867−3 3.603−3 2.841−3 4.284−3 1.672−3 2.231−3 1.409−3 7.438−4 1.438−3 1.037−3 1.561−3 8.053−4 1.072−3 8.977−5 1.117−4 5.874−2 3.368−3 2.070−2 6.694−3 8.267−2 1.132−2 7.435−4 4.097−3 1.809−3 1.500−2 2.835−3 2.864−3 1.347−3 2.642−4 1.518−3 7.214−4 5.552−3 1.149−3 1.318−3 5.862−4 1.069−4 7.057−5 6.865−3 6.987−3 4.918−2 3.091−2 1.617−1 1.465−3 1.856−3 1.003−2 6.525−3 2.976−2 2.678−3 6.066−3 5.362−4 7.323−4 3.780−3 2.520−3 1.107−2 1.167−3 2.758−3 1.353−4 2.341−4 1.753+0 3.364+0 1.149−1 1.740−1 9.188−2 2.611−2 4.914−2
2.751−1 5.320−1 1.983−2 8.821−3 1.679−2 1.684−2 2.529−2 3.828−3 2.014−3 3.885−3 2.828−3 4.262−3 1.607−3 2.142−3 1.428−3 8.087−4 1.566−3 1.030−3 1.551−3 7.874−4 1.049−3 8.130−5 1.012−4 5.232−2 2.874−3 2.053−2 5.849−3 9.059−2 9.614−3 6.419−4 4.020−3 1.569−3 1.605−2 2.392−3 2.929−3 1.088−3 2.423−4 1.506−3 6.463−4 5.916−3 9.892−4 1.391−3 5.014−4 1.048−4 5.863−5 5.901−3 6.111−3 4.776−2 3.043−2 1.751−1 1.279−3 1.609−3 9.653−3 6.186−3 3.133−2 2.342−3 5.998−3 4.925−4 6.566−4 3.681−3 2.398−3 1.161−2 1.076−3 2.826−3 1.180−4 2.225−4 1.919+0 3.670+0 1.088−1 1.644−1 9.261−2 3.208−2 6.045−2
2.973−1 5.733−1 2.001−2 1.032−2 1.964−2 1.770−2 2.655−2 3.858−3 2.270−3 4.384−3 2.863−3 4.314−3 1.573−3 2.096−3 1.454−3 9.091−4 1.763−3 1.032−3 1.556−3 7.763−4 1.034−3 7.419−5 9.244−5 4.502−2 2.631−3 2.051−2 5.183−3 1.018−1 8.140−3 5.813−4 3.985−3 1.371−3 1.757−2 1.992−3 3.111−3 8.806−4 2.272−4 1.499−3 5.747−4 6.428−3 8.324−4 1.502−3 4.226−4 1.050−4 4.794−5 5.453−3 5.430−3 4.692−2 3.091−2 1.946−1 1.172−3 1.407−3 9.397−3 5.997−3 3.379−2 2.110−3 6.171−3 4.635−4 5.850−4 3.598−3 2.308−3 1.241−2 1.004−3 2.967−3 1.032−4 2.157−4 2.097+0 4.005+0 1.039−1 1.568−1 9.377−2 4.021−2 7.587−2
3.215−1 6.188−1 2.026−2 1.235−2 2.353−2 1.874−2 2.811−2 3.903−3 2.627−3 5.078−3 2.928−3 4.412−3 1.557−3 2.076−3 1.479−3 1.042−3 2.024−3 1.042−3 1.571−3 7.692−4 1.025−3 6.862−5 8.556−5 3.831−2 2.599−3 2.053−2 4.691−3 1.157−1 6.941−3 5.553−4 3.964−3 1.211−3 1.946−2 1.649−3 3.371−3 7.196−4 2.199−4 1.492−3 5.106−4 7.053−3 6.897−4 1.640−3 3.548−4 1.066−4 3.900−5 5.442−3 4.934−3 4.641−2 3.230−2 2.195−1 1.133−3 1.245−3 9.206−3 5.955−3 3.697−2 1.967−3 6.516−3 4.505−4 5.210−4 3.521−3 2.259−3 1.344−2 9.541−4 3.162−3 9.137−5 2.125−4 2.268+0 4.331+0 9.984−2 1.506−1 9.472−2 5.006−2 9.454−2
3.387−1 6.511−1 2.007−2 1.428−2 2.724−2 1.935−2 2.902−2 3.856−3 2.950−3 5.712−3 2.934−3 4.422−3 1.517−3 2.023−3 1.463−3 1.158−3 2.252−3 1.031−3 1.554−3 7.473−4 9.965−4 6.328−5 7.895−5 3.251−2 2.652−3 2.013−2 4.274−3 1.277−1 5.935−3 5.424−4 3.861−3 1.069−3 2.094−2 1.356−3 3.562−3 5.925−4 2.141−4 1.451−3 4.498−4 7.515−3 5.635−4 1.736−3 2.967−4 1.062−4 3.162−5 5.600−3 4.513−3 4.514−2 3.352−2 2.408−1 1.117−3 1.103−3 8.864−3 5.892−3 3.944−2 1.850−3 6.763−3 4.409−4 4.602−4 3.379−3 2.197−3 1.417−2 9.050−4 3.290−3 8.097−5 2.068−4 2.362+0 4.513+0 9.463−2 1.427−1 9.313−2 5.870−2 1.109−1
3.518−1 6.786−1 2.126−2 1.574−2 2.998−2 2.035−2 3.045−2 4.208−3 3.242−3 6.250−3 3.007−3 4.521−3 1.566−3 2.082−3 1.629−3 1.271−3 2.455−3 1.043−3 1.570−3 7.767−4 1.033−3 6.473−5 8.066−5 2.466−2 2.546−3 2.159−2 4.160−3 1.381−1 5.364−3 5.208−4 4.341−3 1.066−3 2.224−2 1.258−3 3.780−3 5.451−4 2.023−4 1.705−3 4.614−4 7.873−3 5.444−4 1.886−3 3.931−4 1.085−4 3.303−5 5.402−3 4.390−3 4.783−2 3.497−2 2.589−1 1.079−3 1.098−3 9.805−3 6.034−3 4.165−2 1.840−3 7.084−3 4.164−4 4.727−4 3.884−3 2.250−3 1.479−2 9.556−4 3.542−3 8.313−5 2.111−4 2.494+0 4.866+0 9.473−2 1.426−1 9.930−2 6.536−2 1.239−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
71
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.724−2 5.545−2 3.749−2 4.996−2 1.670−2 3.407−3 6.447−3 7.790−3 1.165−2 4.314−3 5.763−3 6.704−3 8.368−3 1.650−1 2.012+0 2.540−2 5.854−3 9.431−2 1.329−2 1.182−1 1.705−2 1.242−1 1.808−2 1.400−3 1.833−2 3.649−3 2.459−2 4.840−3 1.315−2 4.145−3 1.592−2 5.169−3 4.670−1 3.841+0 1.215−2 1.405−2 2.033−1 4.589−2 2.346−1 5.947−2 2.288−1 2.798−3 3.772−3 4.047−2 1.099−2 4.940−2 9.087−3 2.545−2 1.244−2 3.060−2 1.189−1 5.043−3 9.513−3 9.687−3 1.822−1 2.302−2 8.064−1 4.061−2 1.635−3 2.950−3 3.702−3 3.493−2 8.397−3 1.270−1 1.348−2 3.478−2 7.789−3 7.606−3 6.578−3 2.239−2 2.312−2 2.853−1 1.017−1 1.175+0
3.935−2 6.600−2 4.517−2 7.107−2 1.562−2 3.950−3 7.457−3 7.967−3 1.194−2 5.137−3 6.867−3 7.115−3 8.892−3 1.997−1 2.041+0 8.517−2 1.366−2 9.051−2 1.752−2 1.189−1 2.519−2 1.256−1 3.193−2 2.146−3 1.617−2 3.597−3 2.635−2 5.220−3 1.396−2 4.679−3 1.637−2 5.466−3 5.335−1 3.882+0 2.775−2 1.986−2 2.023−1 5.760−2 2.720−1 7.712−2 3.017−1 4.430−3 3.768−3 3.599−2 1.181−2 5.291−2 1.003−2 2.732−2 1.301−2 3.161−2 3.361−1 1.400−2 2.140−2 2.316−2 1.897−1 4.364−2 8.044−1 7.315−2 2.371−3 4.028−3 4.573−3 3.411−2 9.158−3 1.299−1 1.435−2 3.608−2 7.930−3 2.234−2 1.664−2 5.633−2 4.416−2 3.580−1 1.431−1 1.313+0
4.020−2 6.572−2 4.359−2 6.667−2 1.579−2 4.269−3 8.086−3 8.180−3 1.226−2 4.894−3 6.542−3 6.963−3 8.702−3 1.928−1 2.153+0 7.790−2 1.179−2 9.039−2 1.633−2 1.287−1 2.271−2 1.292−1 2.775−2 2.040−3 1.633−2 3.524−3 2.809−2 4.916−3 1.409−2 4.258−3 1.679−2 5.064−3 5.499−1 4.087+0 2.438−2 1.832−2 2.005−1 5.634−2 2.822−1 7.288−2 2.928−1 4.201−3 3.680−3 3.628−2 1.179−2 5.588−2 9.520−3 2.723−2 1.261−2 3.205−2 3.052−1 1.122−2 1.837−2 1.911−2 1.868−1 3.657−2 8.445−1 6.112−2 2.096−3 3.748−3 4.103−3 3.378−2 8.224−3 1.346−1 1.271−2 3.757−2 7.032−3 1.795−2 1.351−2 4.767−2 3.703−2 3.395−1 1.319−1 1.341+0
4.176−2 6.648−2 4.222−2 6.251−2 1.604−2 4.777−3 9.074−3 8.481−3 1.271−2 4.637−3 6.198−3 6.836−3 8.543−3 1.831−1 2.319+0 6.636−2 1.097−2 9.073−2 1.554−2 1.438−1 2.048−2 1.349−1 2.388−2 2.019−3 1.654−2 3.475−3 3.062−2 4.587−3 1.432−2 3.806−3 1.735−2 4.638−3 5.765−1 4.417+0 2.296−2 1.723−2 1.999−1 5.643−2 3.023−1 6.967−2 2.871−1 4.162−3 3.623−3 3.670−2 1.191−2 6.027−2 8.992−3 2.727−2 1.222−2 3.270−2 2.571−1 9.127−3 1.617−2 1.562−2 1.845−1 3.005−2 9.054−1 4.991−2 1.861−3 3.509−3 3.624−3 3.349−2 7.208−3 1.413−1 1.092−2 3.983−2 6.087−3 1.455−2 1.079−2 4.056−2 3.043−2 3.218−1 1.228−1 1.397+0
4.416−2 6.877−2 4.124−2 5.928−2 1.634−2 5.540−3 1.055−2 8.877−3 1.331−2 4.393−3 5.872−3 6.766−3 8.456−3 1.732−1 2.535+0 5.441−2 1.114−2 9.156−2 1.522−2 1.658−1 1.870−2 1.428−1 2.075−2 2.094−3 1.680−2 3.460−3 3.417−2 4.262−3 1.466−2 3.364−3 1.801−2 4.228−3 6.151−1 4.854+0 2.351−2 1.672−2 2.009−1 5.854−2 3.366−1 6.803−2 2.878−1 4.329−3 3.607−3 3.723−2 1.224−2 6.655−2 8.510−3 2.750−2 1.189−2 3.355−2 2.069−1 7.639−3 1.488−2 1.290−2 1.833−1 2.462−2 9.930−1 4.039−2 1.664−3 3.331−3 3.172−3 3.327−2 6.196−3 1.507−1 9.137−3 4.299−2 5.186−3 1.209−2 8.624−3 3.558−2 2.493−2 3.083−1 1.177−1 1.496+0
4.731−2 7.251−2 4.065−2 5.708−2 1.669−2 6.623−3 1.265−2 9.365−3 1.404−2 4.189−3 5.599−3 6.775−3 8.467−3 1.646−1 2.783+0 4.432−2 1.227−2 9.278−2 1.537−2 1.961−1 1.739−2 1.526−1 1.846−2 2.279−3 1.709−2 3.488−3 3.899−2 3.970−3 1.511−2 2.973−3 1.872−2 3.870−3 6.622−1 5.351+0 2.606−2 1.674−2 2.032−1 6.302−2 3.880−1 6.799−2 2.950−1 4.731−3 3.639−3 3.786−2 1.286−2 7.517−2 8.124−3 2.796−2 1.164−2 3.452−2 1.634−1 6.642−3 1.450−2 1.093−2 1.832−1 2.041−2 1.112+0 3.283−2 1.508−3 3.240−3 2.779−3 3.315−2 5.273−3 1.634−1 7.513−3 4.706−2 4.407−3 1.041−2 6.980−3 3.280−2 2.067−2 2.993−1 1.172−1 1.646+0
5.097−2 7.730−2 4.040−2 5.575−2 1.705−2 8.073−3 1.546−2 9.917−3 1.487−2 4.040−3 5.400−3 6.866−3 8.580−3 1.577−1 3.043+0 3.679−2 1.433−2 9.422−2 1.587−2 2.354−1 1.648−2 1.635−1 1.693−2 2.584−3 1.738−2 3.560−3 4.523−2 3.729−3 1.563−2 2.658−3 1.942−2 3.584−3 7.136−1 5.866+0 3.057−2 1.719−2 2.064−1 6.996−2 4.577−1 6.922−2 3.071−1 5.386−3 3.716−3 3.854−2 1.385−2 8.643−2 7.860−3 2.860−2 1.149−2 3.551−2 1.295−1 6.021−3 1.495−2 9.630−3 1.840−1 1.733−2 1.265+0 2.714−2 1.395−3 3.249−3 2.469−3 3.314−2 4.500−3 1.797−1 6.148−3 5.184−2 3.792−3 9.357−3 5.785−3 3.206−2 1.755−2 2.942−1 1.215−1 1.852+0
5.451−2 8.212−2 4.023−2 5.487−2 1.732−2 9.813−3 1.883−2 1.044−2 1.566−2 3.932−3 5.255−3 6.989−3 8.735−3 1.520−1 3.289+0 3.158−2 1.710−2 9.528−2 1.651−2 2.815−1 1.583−2 1.736−1 1.595−2 2.983−3 1.757−2 3.648−3 5.249−2 3.533−3 1.612−2 2.418−3 1.994−2 3.361−3 7.624−1 6.341+0 3.661−2 1.781−2 2.091−1 7.871−2 5.411−1 7.090−2 3.200−1 6.241−3 3.811−3 3.905−2 1.510−2 9.961−2 7.680−3 2.923−2 1.137−2 3.625−2 1.046−1 5.649−3 1.602−2 8.841−3 1.843−1 1.514−2 1.442+0 2.300−2 1.315−3 3.341−3 2.240−3 3.306−2 3.889−3 1.983−1 5.071−3 5.664−2 3.334−3 8.712−3 4.935−3 3.286−2 1.534−2 2.905−1 1.294−1 2.097+0
5.609−2 8.419−2 3.919−2 5.304−2 1.707−2 1.129−2 2.169−2 1.060−2 1.591−2 3.771−3 5.040−3 6.942−3 8.676−3 1.443−1 3.418+0 2.769−2 1.959−2 9.369−2 1.671−2 3.199−1 1.502−2 1.775−1 1.500−2 3.323−3 1.726−2 3.644−3 5.826−2 3.309−3 1.610−2 2.201−3 1.979−2 3.127−3 7.859−1 6.587+0 4.203−2 1.798−2 2.061−1 8.573−2 6.108−1 7.082−2 3.235−1 6.972−3 3.809−3 3.843−2 1.601−2 1.100−1 7.390−3 2.902−2 1.100−2 3.583−2 8.593−2 5.318−3 1.698−2 8.239−3 1.800−1 1.338−2 1.579+0 1.977−2 1.235−3 3.398−3 2.041−3 3.216−2 3.373−3 2.113−1 4.209−3 5.932−2 2.955−3 8.157−3 4.272−3 3.374−2 1.357−2 2.811−1 1.357−1 2.289+0
5.988−2 8.924−2 4.039−2 5.384−2 1.887−2 1.268−2 2.435−2 1.110−2 1.661−2 3.717−3 4.969−3 7.316−3 9.135−3 1.468−1 3.648+0 2.193−2 2.180−2 1.023−1 1.828−2 3.526−1 1.552−2 1.886−1 1.475−2 3.749−3 1.997−2 4.090−3 6.274−2 3.400−3 1.641−2 2.208−3 2.088−2 3.274−3 8.381−1 7.057+0 4.645−2 1.951−2 2.248−1 9.264−2 6.671−1 7.377−2 3.379−1 7.824−3 4.263−3 4.417−2 1.703−2 1.181−1 7.500−3 2.957−2 1.156−2 3.771−2 6.485−2 5.099−3 1.739−2 7.879−3 1.882−1 1.266−2 1.706+0 1.847−2 1.263−3 3.598−3 2.099−3 3.434−2 3.405−3 2.255−1 4.246−3 6.323−2 3.133−3 7.722−3 3.859−3 3.362−2 1.283−2 2.892−1 1.425−1 2.456+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
72
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.458−3 2.614−3 7.401−3 8.399−3 5.665−2 2.356−2 1.878−1 1.259−2 5.165−2 4.982+0 9.586+0 4.500−1 6.752−1 4.108−2 5.492−2 2.672−1 3.866−2 7.209−2 8.035−2 1.194−1 8.712−2 1.159−1 4.479−2 5.594−2 5.788−1 8.924+0 7.421−2 3.529−1 3.383−2 2.086−2 2.834−1 3.617−2 2.118−1 3.832−2 2.645−1 3.087−2 1.572−1 2.976−2 1.949+0 1.648+1 1.443−1 6.306−1 4.360−2 3.854−2 6.056−1 9.258−2 4.294−1 1.175−1 4.845−1 9.264−2 2.839−1 2.900−1 1.032+1 6.738−2 1.762−2 3.186−2 2.441−2 5.821−1 3.718−2 1.130+0 5.317−2 7.215−1 5.347−2 7.965−1 1.433+1 2.664−2 1.546−2 6.952−2 3.759−2 8.930−1 1.391−1 1.648+0 1.400−1 1.026+0
3.644−3 3.249−3 9.861−3 9.205−3 5.571−2 2.473−2 1.923−1 1.294−2 5.356−2 5.254+0 9.998+0 4.860−1 8.106−1 1.088−1 1.515−1 2.505−1 4.173−2 7.702−2 7.862−2 1.173−1 8.753−2 1.167−1 4.724−2 5.904−2 6.259−1 9.257+0 1.610−1 4.624−1 1.255−1 2.797−2 2.517−1 3.292−2 2.176−1 3.576−2 2.583−1 3.252−2 1.618−1 3.284−2 2.212+0 1.966+1 3.001−1 1.008+0 5.958−2 3.642−2 5.376−1 9.076−2 4.396−1 1.178−1 4.756−1 9.811−2 2.932−1 4.994−1 1.225+1 3.136−1 2.307−2 4.225−2 2.588−2 5.385−1 3.714−2 1.128+0 5.266−2 7.061−1 5.423−2 1.564+0 2.526+1 3.504−2 1.583−2 8.695−2 3.782−2 8.275−1 1.389−1 1.653+0 1.391−1 1.005+0
3.204−3 2.872−3 9.052−3 8.259−3 5.481−2 2.330−2 1.983−1 1.210−2 5.529−2 5.686+0 1.078+1 4.723−1 7.724−1 9.310−2 1.285−1 2.550−1 4.943−2 9.178−2 8.414−2 1.255−1 8.816−2 1.175−1 4.749−2 5.936−2 6.005−1 1.012+1 1.423−1 4.306−1 1.002−1 2.976−2 2.569−1 3.476−2 2.520−1 3.587−2 2.750−1 3.228−2 1.624−1 3.109−2 2.404+0 2.110+1 2.569−1 9.039−1 6.332−2 3.795−2 5.501−1 9.806−2 5.040−1 1.224−1 5.046−1 9.597−2 2.930−1 4.368−1 1.422+1 2.444−1 2.155−2 4.280−2 2.545−2 5.486−1 3.626−2 1.250+0 4.968−2 7.442−1 5.054−2 1.661+0 2.717+1 3.277−2 1.511−2 8.761−2 3.688−2 8.425−1 1.445−1 1.829+0 1.393−1 1.057+0
2.834−3 2.493−3 8.313−3 7.234−3 5.390−2 2.185−2 2.072−1 1.129−2 5.808−2 6.180+0 1.170+1 4.583−1 7.340−1 7.910−2 1.083−1 2.605−1 6.054−2 1.129−1 9.102−2 1.357−1 8.873−2 1.182−1 4.803−2 6.004−2 5.756−1 1.112+1 1.260−1 4.002−1 7.816−2 3.357−2 2.628−1 3.721−2 2.992−1 3.597−2 2.954−1 3.217−2 1.629−1 2.937−2 2.620+0 2.270+1 2.183−1 8.072−1 7.148−2 4.031−2 5.648−1 1.081−1 5.922−1 1.283−1 5.401−1 9.386−2 2.927−1 3.802−1 1.622+1 1.847−1 2.091−2 4.517−2 2.544−2 5.600−1 3.557−2 1.415+0 4.667−2 7.903−1 4.696−2 1.754+0 2.897+1 3.181−2 1.457−2 9.134−2 3.616−2 8.595−1 1.531−1 2.064+0 1.404−1 1.120+0
2.527−3 2.132−3 7.698−3 6.218−3 5.308−2 2.060−2 2.199−1 1.063−2 6.216−2 6.725+0 1.273+1 4.456−1 7.010−1 6.835−2 9.297−2 2.664−1 7.592−2 1.421−1 9.901−2 1.475−1 8.919−2 1.189−1 4.889−2 6.111−2 5.536−1 1.218+1 1.142−1 3.748−1 6.108−2 3.968−2 2.689−1 4.021−2 3.624−1 3.606−2 3.187−1 3.225−2 1.635−1 2.786−2 2.849+0 2.444+1 1.876−1 7.286−1 8.463−2 4.336−2 5.807−1 1.214−1 7.101−1 1.352−1 5.806−1 9.203−2 2.926−1 3.350−1 1.811+1 1.389−1 2.090−2 4.965−2 2.591−2 5.719−1 3.523−2 1.633+0 4.393−2 8.424−1 4.391−2 1.845+0 3.075+1 3.179−2 1.417−2 9.875−2 3.581−2 8.773−1 1.658−1 2.374+0 1.428−1 1.191+0
2.287−3 1.811−3 7.267−3 5.293−3 5.245−2 1.975−2 2.374−1 1.021−2 6.755−2 7.302+0 1.384+1 4.347−1 6.743−1 6.093−2 8.244−2 2.721−1 9.636−2 1.807−1 1.076−1 1.603−1 8.957−2 1.193−1 5.002−2 6.253−2 5.348−1 1.327+1 1.066−1 3.549−1 4.877−2 4.839−2 2.749−1 4.356−2 4.443−1 3.614−2 3.433−1 3.252−2 1.641−1 2.670−2 3.081+0 2.627+1 1.649−1 6.688−1 1.034−1 4.685−2 5.964−1 1.388−1 8.630−1 1.427−1 6.236−1 9.068−2 2.928−1 3.011−1 1.983+1 1.062−1 2.133−2 5.655−2 2.694−2 5.833−1 3.526−2 1.911+0 4.168−2 8.970−1 4.162−2 1.936+0 3.252+1 3.242−2 1.390−2 1.105−1 3.584−2 8.946−1 1.836−1 2.773+0 1.463−1 1.265+0
2.112−3 1.546−3 7.059−3 4.519−3 5.204−2 1.945−2 2.601−1 1.005−2 7.400−2 7.895+0 1.499+1 4.252−1 6.529−1 5.624−2 7.578−2 2.773−1 1.222−1 2.296−1 1.160−1 1.728−1 8.992−2 1.198−1 5.130−2 6.413−2 5.186−1 1.435+1 1.026−1 3.395−1 4.031−2 5.980−2 2.801−1 4.694−2 5.460−1 3.625−2 3.671−1 3.292−2 1.648−1 2.592−2 3.309+0 2.814+1 1.487−1 6.241−1 1.281−1 5.040−2 6.107−1 1.604−1 1.053+0 1.501−1 6.650−1 8.989−2 2.935−1 2.767−1 2.139+1 8.409−2 2.199−2 6.597−2 2.850−2 5.935−1 3.559−2 2.255+0 4.002−2 9.491−1 4.010−2 2.025+0 3.426+1 3.339−2 1.374−2 1.267−1 3.618−2 9.100−1 2.070−1 3.267+0 1.504−1 1.337+0
1.989−3 1.338−3 7.044−3 3.907−3 5.162−2 1.962−2 2.864−1 1.008−2 8.054−2 8.440+0 1.606+1 4.151−1 6.329−1 5.332−2 7.164−2 2.803−1 1.518−1 2.851−1 1.229−1 1.830−1 8.993−2 1.198−1 5.233−2 6.542−2 5.019−1 1.532+1 1.005−1 3.264−1 3.457−2 7.302−2 2.832−1 4.975−2 6.601−1 3.623−2 3.857−1 3.323−2 1.650−1 2.537−2 3.511+0 2.983+1 1.367−1 5.882−1 1.567−1 5.333−2 6.201−1 1.844−1 1.266+0 1.558−1 6.971−1 8.924−2 2.935−1 2.582−1 2.267+1 6.952−2 2.260−2 7.706−2 3.030−2 5.992−1 3.586−2 2.636+0 3.874−2 9.890−1 3.906−2 2.100+0 3.574+1 3.428−2 1.362−2 1.459−1 3.645−2 9.186−1 2.337−1 3.818+0 1.536−1 1.391+0
1.867−3 1.162−3 6.992−3 3.392−3 5.001−2 1.963−2 3.047−1 9.948−3 8.412−2 8.682+0 1.656+1 3.960−1 6.012−1 5.042−2 6.761−2 2.749−1 1.761−1 3.309−1 1.246−1 1.855−1 8.760−2 1.167−1 5.175−2 6.471−2 4.749−1 1.573+1 9.724−2 3.083−1 3.019−2 8.385−2 2.776−1 5.054−2 7.512−1 3.529−2 3.884−1 3.262−2 1.610−1 2.442−2 3.585+0 3.046+1 1.252−1 5.471−1 1.802−1 5.409−2 6.100−1 2.021−1 1.436+0 1.555−1 7.006−1 8.660−2 2.860−1 2.389−1 2.308+1 5.911−2 2.253−2 8.585−2 3.123−2 5.867−1 3.511−2 2.928+0 3.693−2 9.898−1 3.747−2 2.106+0 3.603+1 3.416−2 1.321−2 1.609−1 3.569−2 8.995−1 2.533−1 4.240+0 1.519−1 1.392+0
1.905−3 1.177−3 7.336−3 3.425−3 5.329−2 2.068−2 3.247−1 1.059−2 8.961−2 9.078+0 1.731+1 4.160−1 6.257−1 4.956−2 6.626−2 2.950−1 1.918−1 3.625−1 1.328−1 1.975−1 1.028−1 1.370−1 5.572−2 6.966−2 5.068−1 1.660+1 9.701−2 3.180−1 2.595−2 9.440−2 3.043−1 5.628−2 8.199−1 4.116−2 4.024−1 3.474−2 1.741−1 2.595−2 3.640+0 3.093+1 1.234−1 5.611−1 2.011−1 6.017−2 6.687−1 2.226−1 1.561+0 1.626−1 7.269−1 9.306−2 3.090−1 2.421−1 2.515+1 4.693−2 2.204−2 9.289−2 3.496−2 6.209−1 3.693−2 3.163+0 4.094−2 1.043+0 3.978−2 2.231+0 4.053+1 3.337−2 1.483−2 1.734−1 3.844−2 9.513−1 2.723−1 4.565+0 1.605−1 1.468+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
73
Table 27 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.558−1 6.480−3 1.333−2 1.361−2 5.140−2 2.544−2 7.336−1 5.263−2 4.030+0 9.516−2 8.658−3 7.734−3 2.812−2 2.037−2 8.220−2 5.271−2 9.963−1 2.484−1 5.261+0 1.265+1 2.476+1 1.270+0 1.905+0 1.464−1 1.956−1 4.061−2 5.091−2 1.485+0 2.415+1 2.009−1 1.377+0 9.597−2 8.784−2 2.743−2 5.298+0 4.510+1 5.173−1 2.438+0 6.544−2 1.631−1 7.541−1 3.339+1 1.394−1 1.140+0 6.811−2 2.596+0 5.186+1 2.020−1 1.609+0 4.897−1 2.742+1 1.284−1 1.408+0 3.685+1 4.552−1
8.545−1 1.052−2 1.603−2 1.626−2 6.280−2 2.715−2 7.040−1 5.278−2 4.030+0 9.460−2 1.367−2 1.027−2 3.378−2 2.144−2 9.722−2 5.286−2 9.571−1 2.481−1 5.266+0 1.406+1 2.676+1 1.263+0 1.898+0 1.613−1 2.147−1 4.338−2 5.424−2 1.432+0 2.774+1 2.222−1 1.355+0 9.907−2 9.822−2 2.825−2 6.426+0 5.351+1 5.139−1 2.390+0 6.990−2 1.812−1 7.341−1 5.518+1 1.495−1 1.119+0 6.859−2 5.299+0 8.668+1 2.006−1 1.579+0 4.773−1 5.338+1 1.247−1 3.782+0 7.549+1 4.260−1
6.753−1 8.796−3 1.495−2 1.438−2 6.105−2 2.430−2 7.086−1 4.710−2 4.334+0 8.382−2 1.151−2 8.654−3 3.103−2 1.881−2 9.422−2 4.718−2 9.614−1 2.481−1 5.657+0 1.531+1 2.907+1 1.243+0 1.869+0 1.627−1 2.167−1 4.170−2 5.215−2 1.403+0 3.026+1 2.259−1 1.328+0 9.725−2 9.764−2 2.621−2 7.009+0 5.851+1 5.034−1 2.341+0 6.698−2 1.788−1 7.184−1 6.027+1 1.475−1 1.092+0 6.285−2 5.707+0 9.435+1 1.911−1 1.539+0 4.577−1 5.787+1 1.135−1 3.960+0 8.151+1 3.870−1
5.179−1 7.493−3 1.415−2 1.268−2 6.013−2 2.145−2 7.141−1 4.138−2 4.737+0 7.291−2 9.858−3 7.255−3 2.885−2 1.616−2 9.215−2 4.147−2 9.667−1 2.517−1 6.177+0 1.671+1 3.169+1 1.222+0 1.836+0 1.646−1 2.194−1 4.008−2 5.013−2 1.372+0 3.305+1 2.304−1 1.297+0 9.548−2 9.734−2 2.427−2 7.642+0 6.399+1 4.919−1 2.285+0 6.427−2 1.769−1 7.014−1 6.561+1 1.461−1 1.064+0 5.725−2 6.127+0 1.023+2 1.816−1 1.497+0 4.375−1 6.252+1 1.026−1 4.140+0 8.771+1 3.480−1
3.943−1 6.520−3 1.362−2 1.124−2 6.043−2 1.892−2 7.200−1 3.620−2 5.261+0 6.294−2 8.615−3 6.093−3 2.722−2 1.374−2 9.177−2 3.630−2 9.729−1 2.609−1 6.856+0 1.820+1 3.451+1 1.198+0 1.800+0 1.671−1 2.228−1 3.867−2 4.837−2 1.338+0 3.599+1 2.355−1 1.265+0 9.392−2 9.742−2 2.261−2 8.295+0 6.967+1 4.802−1 2.227+0 6.208−2 1.759−1 6.840−1 7.094+1 1.456−1 1.035+0 5.231−2 6.539+0 1.102+2 1.728−1 1.454+0 4.183−1 6.710+1 9.334−2 4.315+0 9.378+1 3.125−1
3.034−1 5.818−3 1.333−2 1.012−2 6.228−2 1.690−2 7.259−1 3.196−2 5.930+0 5.467−2 7.714−3 5.181−3 2.613−2 1.173−2 9.369−2 3.208−2 9.793−1 2.775−1 7.725+0 1.972+1 3.745+1 1.173+0 1.763+0 1.700−1 2.267−1 3.756−2 4.699−2 1.301+0 3.895+1 2.410−1 1.230+0 9.265−2 9.788−2 2.137−2 8.943+0 7.533+1 4.682−1 2.166+0 6.055−2 1.758−1 6.663−1 7.604+1 1.460−1 1.005+0 4.836−2 6.929+0 1.178+2 1.650−1 1.411+0 4.009−1 7.144+1 8.621−2 4.479+0 9.951+1 2.827−1
2.395−1 5.337−3 1.323−2 9.308−3 6.577−2 1.549−2 7.312−1 2.877−2 6.753+0 4.837−2 7.095−3 4.511−3 2.550−2 1.018−2 9.815−2 2.889−2 9.853−1 3.023−1 8.798+0 2.125+1 4.042+1 1.148+0 1.725+0 1.733−1 2.312−1 3.677−2 4.601−2 1.261+0 4.186+1 2.465−1 1.192+0 9.165−2 9.859−2 2.053−2 9.565+0 8.081+1 4.557−1 2.100+0 5.965−2 1.763−1 6.480−1 8.080+1 1.471−1 9.741−1 4.543−2 7.287+0 1.247+2 1.583−1 1.368+0 3.853−1 7.543+1 8.127−2 4.628+0 1.048+2 2.589−1
1.952−1 5.010−3 1.319−2 8.726−3 7.031−2 1.456−2 7.322−1 2.640−2 7.661+0 4.377−2 6.671−3 4.033−3 2.510−2 9.033−3 1.042−1 2.653−2 9.857−1 3.324−1 9.984+0 2.260+1 4.309+1 1.122+0 1.688+0 1.762−1 2.351−1 3.612−2 4.520−2 1.215+0 4.440+1 2.501−1 1.148+0 9.040−2 9.882−2 1.993−2 1.009+1 8.554+1 4.406−1 2.021+0 5.889−2 1.763−1 6.261−1 8.471+1 1.478−1 9.377−1 4.317−2 7.571+0 1.304+2 1.516−1 1.317+0 3.695−1 7.865+1 7.777−2 4.740+0 1.089+2 2.395−1
1.624−1 4.689−3 1.288−2 8.136−3 7.317−2 1.368−2 7.125−1 2.416−2 8.317+0 3.973−2 6.252−3 3.631−3 2.425−2 8.065−3 1.080−1 2.430−2 9.587−1 3.536−1 1.085+1 2.312+1 4.416+1 1.079+0 1.630+0 1.747−1 2.332−1 3.479−2 4.355−2 1.144+0 4.530+1 2.458−1 1.078+0 8.691−2 9.621−2 1.904−2 1.025+1 8.708+1 4.150−1 1.897+0 5.680−2 1.713−1 5.895−1 8.553+1 1.444−1 8.795−1 4.053−2 7.588+0 1.313+2 1.420−1 1.235+0 3.464−1 7.905+1 7.358−2 4.698+0 1.093+2 2.192−1
1.342−1 4.904−3 1.313−2 8.644−3 7.048−2 1.411−2 7.434−1 2.558−2 8.915+0 4.281−2 6.559−3 3.897−3 2.500−2 8.585−3 1.039−1 2.572−2 1.000+0 3.754−1 1.159+1 2.077+1 4.527+1 1.049+0 1.576+0 2.108−1 2.830−1 3.847−2 4.826−2 1.166+0 4.063+1 3.416−1 1.119+0 1.046−1 1.263−1 2.220−2 9.466+0 7.863+1 4.468−1 1.984+0 6.909−2 2.176−1 6.287−1 9.469+1 1.671−1 9.302−1 4.456−2 6.791+0 1.543+2 1.525−1 1.308+0 3.707−1 7.561+1 1.265−1 4.116+0 1.050+2 2.459−1
74
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 28 Effective collision strengths for transitions in Cr XXII. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.958−1 3.801−1 1.726−2 5.029−3 9.395−3 1.314−2 1.963−2 3.445−3 1.253−3 2.382−3 2.387−3 3.580−3 1.433−3 1.903−3 1.344−3 5.290−4 1.006−3 9.216−4 1.383−3 7.549−4 1.003−3 9.837−5 1.226−4 3.420−2 1.220−3 1.870−2 4.921−3 6.331−2 9.146−3 3.908−4 3.868−3 1.612−3 1.162−2 2.849−3 1.902−3 1.183−3 1.843−4 1.548−3 7.738−4 4.357−3 1.331−3 1.029−3 7.176−4 9.600−5 9.483−5 2.469−3 5.064−3 4.267−2 2.427−2 1.243−1 7.781−4 1.630−3 9.382−3 5.815−3 2.359−2 2.130−3 4.229−3 3.654−4 7.793−4 3.871−3 2.493−3 9.027−3 1.248−3 2.331−3 1.640−4 2.306−4 1.277+0 2.460+0 9.175−2 1.378−1 8.090−2 1.356−2 2.514−2
2.002−1 3.877−1 1.928−2 6.459−3 1.213−2 1.436−2 2.184−2 3.808−3 1.725−3 3.318−3 2.844−3 4.296−3 1.893−3 2.513−3 1.280−3 6.114−4 1.170−3 9.854−4 1.480−3 7.982−4 1.061−3 1.056−4 1.318−4 4.986−2 5.389−3 2.008−2 8.413−3 6.432−2 1.449−2 1.209−3 4.276−3 2.571−3 1.256−2 3.905−3 3.034−3 2.218−3 3.263−4 1.433−3 8.297−4 4.559−3 1.407−3 1.138−3 7.437−4 1.090−4 9.593−5 1.195−2 8.844−3 4.925−2 3.114−2 1.313−1 2.483−3 2.698−3 1.106−2 7.431−3 2.617−2 3.962−3 6.948−3 6.580−4 8.560−4 3.710−3 2.645−3 9.477−3 1.328−3 2.555−3 1.720−4 2.567−4 1.272+0 2.462+0 1.204−1 1.845−1 8.374−2 1.678−2 3.462−2
2.097−1 4.056−1 1.883−2 6.548−3 1.239−2 1.452−2 2.209−2 3.662−3 1.657−3 3.191−3 2.743−3 4.138−3 1.761−3 2.336−3 1.275−3 6.175−4 1.185−3 9.731−4 1.463−3 7.801−4 1.037−3 9.888−5 1.233−4 5.519−2 4.397−3 1.981−2 7.893−3 6.661−2 1.374−2 9.843−4 4.066−3 2.255−3 1.269−2 3.498−3 2.821−3 1.879−3 2.937−4 1.415−3 7.825−4 4.649−3 1.319−3 1.138−3 6.893−4 1.042−4 8.705−5 9.579−3 8.253−3 4.804−2 3.065−2 1.349−1 2.014−3 2.345−3 1.038−2 6.941−3 2.608−2 3.430−3 6.344−3 5.927−4 8.026−4 3.631−3 2.553−3 9.572−3 1.255−3 2.517−3 1.579−4 2.420−4 1.350+0 2.605+0 1.181−1 1.804−1 8.287−2 1.768−2 3.589−2
2.206−1 4.262−1 1.846−2 6.722−3 1.276−2 1.462−2 2.219−2 3.555−3 1.634−3 3.145−3 2.655−3 4.001−3 1.640−3 2.176−3 1.277−3 6.341−4 1.219−3 9.593−4 1.443−3 7.596−4 1.010−3 9.115−5 1.136−4 5.691−2 3.591−3 1.944−2 7.103−3 6.962−2 1.236−2 8.075−4 3.894−3 1.957−3 1.297−2 3.071−3 2.664−3 1.556−3 2.655−4 1.400−3 7.267−4 4.787−3 1.207−3 1.150−3 6.229−4 9.959−5 7.680−5 7.722−3 7.412−3 4.644−2 2.956−2 1.394−1 1.649−3 2.024−3 9.766−3 6.453−3 2.627−2 2.931−3 5.845−3 5.361−4 7.427−4 3.546−3 2.442−3 9.734−3 1.170−3 2.491−3 1.420−4 2.269−4 1.454+0 2.793+0 1.127−1 1.717−1 8.255−2 1.965−2 3.892−2
2.334−1 4.505−1 1.822−2 7.126−3 1.352−2 1.482−2 2.243−2 3.496−3 1.675−3 3.222−3 2.596−3 3.911−3 1.544−3 2.050−3 1.287−3 6.667−4 1.284−3 9.465−4 1.425−3 7.393−4 9.835−4 8.304−5 1.035−4 5.446−2 2.970−3 1.910−2 6.239−3 7.410−2 1.072−2 6.750−4 3.769−3 1.694−3 1.351−2 2.646−3 2.598−3 1.270−3 2.407−4 1.386−3 6.637−4 4.997−3 1.074−3 1.183−3 5.482−4 9.603−5 6.583−5 6.333−3 6.511−3 4.487−2 2.846−2 1.463−1 1.378−3 1.746−3 9.271−3 6.022−3 2.692−2 2.511−3 5.532−3 4.870−4 6.770−4 3.457−3 2.321−3 1.001−2 1.080−3 2.496−3 1.255−4 2.131−4 1.585+0 3.029+0 1.063−1 1.615−1 8.289−2 2.305−2 4.469−2
2.494−1 4.804−1 1.817−2 7.903−3 1.499−2 1.527−2 2.303−2 3.484−3 1.798−3 3.458−3 2.577−3 3.881−3 1.479−3 1.965−3 1.303−3 7.222−4 1.393−3 9.384−4 1.413−3 7.222−4 9.613−4 7.532−5 9.387−5 4.896−2 2.548−3 1.888−2 5.453−3 8.081−2 9.114−3 5.820−4 3.689−3 1.467−3 1.439−2 2.242−3 2.638−3 1.028−3 2.203−4 1.375−3 5.972−4 5.307−3 9.297−4 1.244−3 4.709−4 9.415−5 5.499−5 5.411−3 5.701−3 4.363−2 2.786−2 1.574−1 1.190−3 1.511−3 8.898−3 5.689−3 2.821−2 2.187−3 5.438−3 4.469−4 6.090−4 3.370−3 2.206−3 1.046−2 9.949−4 2.550−3 1.097−4 2.025−4 1.736+0 3.305+0 1.004−1 1.522−1 8.377−2 2.820−2 5.389−2
2.692−1 5.170−1 1.831−2 9.177−3 1.740−2 1.600−2 2.409−2 3.513−3 2.018−3 3.884−3 2.601−3 3.918−3 1.443−3 1.919−3 1.327−3 8.088−4 1.563−3 9.390−4 1.415−3 7.110−4 9.469−4 6.869−5 8.563−5 4.232−2 2.328−3 1.880−2 4.818−3 9.037−2 7.705−3 5.248−4 3.649−3 1.279−3 1.569−2 1.873−3 2.786−3 8.318−4 2.059−4 1.369−3 5.324−4 5.747−3 7.853−4 1.341−3 3.978−4 9.429−5 4.512−5 4.945−3 5.054−3 4.287−2 2.809−2 1.739−1 1.078−3 1.318−3 8.640−3 5.488−3 3.030−2 1.958−3 5.566−3 4.195−4 5.435−4 3.296−3 2.117−3 1.115−2 9.259−4 2.669−3 9.597−5 1.960−4 1.899+0 3.607+0 9.565−2 1.447−1 8.502−2 3.531−2 6.695−2
2.916−1 5.586−1 1.854−2 1.097−2 2.082−2 1.695−2 2.548−2 3.561−3 2.335−3 4.500−3 2.659−3 4.006−3 1.428−3 1.901−3 1.351−3 9.275−4 1.796−3 9.475−4 1.429−3 7.047−4 9.391−4 6.349−5 7.918−5 3.604−2 2.293−3 1.882−2 4.345−3 1.028−1 6.551−3 4.991−4 3.631−3 1.127−3 1.737−2 1.553−3 3.016−3 6.787−4 1.985−4 1.365−3 4.737−4 6.307−3 6.523−4 1.465−3 3.341−4 9.596−5 3.676−5 4.886−3 4.580−3 4.245−2 2.923−2 1.959−1 1.031−3 1.163−3 8.460−3 5.429−3 3.313−2 1.815−3 5.869−3 4.067−4 4.846−4 3.231−3 2.066−3 1.206−2 8.777−4 2.845−3 8.489−5 1.933−4 2.060+0 3.912+0 9.183−2 1.387−1 8.619−2 4.418−2 8.344−2
3.096−1 5.925−1 1.849−2 1.284−2 2.439−2 1.765−2 2.651−2 3.547−3 2.654−3 5.122−3 2.683−3 4.044−3 1.400−3 1.864−3 1.347−3 1.042−3 2.022−3 9.433−4 1.423−3 6.893−4 9.191−4 5.879−5 7.336−5 3.062−2 2.355−3 1.856−2 3.963−3 1.146−1 5.599−3 4.892−4 3.559−3 9.975−4 1.887−2 1.281−3 3.217−3 5.590−4 1.940−4 1.337−3 4.190−4 6.785−3 5.346−4 1.568−3 2.798−4 9.647−5 2.987−5 5.037−3 4.198−3 4.157−2 3.048−2 2.169−1 1.017−3 1.032−3 8.192−3 5.393−3 3.565−2 1.710−3 6.143−3 3.999−4 4.297−4 3.121−3 2.017−3 1.284−2 8.355−4 2.988−3 7.546−5 1.895−4 2.166+0 4.115+0 8.744−2 1.320−1 8.550−2 5.264−2 9.924−2
3.189−1 6.116−1 1.930−2 1.393−2 2.640−2 1.833−2 2.742−2 3.815−3 2.865−3 5.502−3 2.717−3 4.086−3 1.430−3 1.901−3 1.478−3 1.122−3 2.159−3 9.445−4 1.422−3 7.085−4 9.423−4 5.980−5 7.450−5 2.276−2 2.220−3 1.959−2 3.787−3 1.221−1 4.972−3 4.605−4 3.930−3 9.809−4 1.973−2 1.184−3 3.354−3 5.085−4 1.801−4 1.546−3 4.267−4 6.999−3 5.139−4 1.677−3 2.857−4 9.824−5 3.122−5 4.731−3 4.014−3 4.346−2 3.128−2 2.296−1 9.564−4 1.012−3 8.900−3 5.443−3 3.706−2 1.671−3 6.323−3 3.710−4 4.377−4 3.532−3 2.037−3 1.319−2 8.718−4 3.168−3 7.780−5 1.935−4 2.261+0 4.385+0 8.640−2 1.301−1 8.979−2 5.756−2 1.085−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
75
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.380−2 5.029−2 3.389−2 4.517−2 1.432−2 3.224−3 6.169−3 7.127−3 1.065−2 3.906−3 5.218−3 6.150−3 7.675−3 1.506−1 1.803+0 2.329−2 5.185−3 8.569−2 1.204−2 1.056−1 1.553−2 1.125−1 1.660−2 1.610−3 1.589−2 3.227−3 2.124−2 4.269−3 1.235−2 4.003−3 1.420−2 4.812−3 4.205−1 3.449+0 1.078−2 1.279−2 1.848−1 4.154−2 2.106−1 5.422−2 2.076−1 3.250−3 3.345−3 3.511−2 9.559−3 4.284−2 8.679−3 2.399−2 1.138−2 2.748−2 1.095−1 4.597−3 8.628−3 8.887−3 1.660−1 2.125−2 7.271−1 3.751−2 1.466−3 3.128−3 3.530−3 3.135−2 7.796−3 1.109−1 1.219−2 3.276−2 7.215−3 6.937−3 6.058−3 2.039−2 2.135−2 2.601−1 9.275−2 1.061+0
3.536−2 6.333−2 4.076−2 6.103−2 1.428−2 3.513−3 6.602−3 7.240−3 1.086−2 4.666−3 6.232−3 6.454−3 8.062−3 1.818−1 1.840+0 7.858−2 1.242−2 8.290−2 1.762−2 1.066−1 2.521−2 1.142−1 2.723−2 1.896−3 1.471−2 3.253−3 2.362−2 4.759−3 1.271−2 4.268−3 1.473−2 4.976−3 4.849−1 3.520+0 2.706−2 1.811−2 2.084−1 5.075−2 2.526−1 6.859−2 2.600−1 4.040−3 3.499−3 3.287−2 1.071−2 4.763−2 9.146−3 2.485−2 1.181−2 2.856−2 3.105−1 1.372−2 2.100−2 2.317−2 1.746−1 4.264−2 7.280−1 6.867−2 2.267−3 3.643−3 4.151−3 3.103−2 8.372−3 1.178−1 1.316−2 3.218−2 7.209−3 2.189−2 1.577−2 4.827−2 4.054−2 3.075−1 1.253−1 1.101+0
3.614−2 6.255−2 3.942−2 5.812−2 1.440−2 3.776−3 7.117−3 7.418−3 1.113−2 4.451−3 5.945−3 6.315−3 7.889−3 1.767−1 1.935+0 7.306−2 1.070−2 8.269−2 1.624−2 1.146−1 2.264−2 1.173−1 2.390−2 1.794−3 1.486−2 3.191−3 2.507−2 4.490−3 1.282−2 3.896−3 1.510−2 4.617−3 4.992−1 3.689+0 2.353−2 1.666−2 2.029−1 4.977−2 2.597−1 6.509−2 2.553−1 3.778−3 3.393−3 3.310−2 1.067−2 5.010−2 8.688−3 2.475−2 1.144−2 2.894−2 2.868−1 1.092−2 1.770−2 1.911−2 1.717−1 3.590−2 7.608−1 5.769−2 1.976−3 3.377−3 3.729−3 3.075−2 7.545−3 1.217−1 1.170−2 3.347−2 6.402−3 1.745−2 1.280−2 4.139−2 3.419−2 2.954−1 1.160−1 1.139+0
3.754−2 6.242−2 3.826−2 5.519−2 1.461−2 4.211−3 7.958−3 7.674−3 1.152−2 4.222−3 5.640−3 6.200−3 7.745−3 1.684−1 2.076+0 6.290−2 9.856−3 8.288−2 1.514−2 1.272−1 2.016−2 1.220−1 2.081−2 1.770−3 1.505−2 3.148−3 2.721−2 4.199−3 1.300−2 3.493−3 1.559−2 4.237−3 5.219−1 3.970+0 2.166−2 1.563−2 1.973−1 4.997−2 2.747−1 6.244−2 2.527−1 3.704−3 3.324−3 3.346−2 1.075−2 5.383−2 8.212−3 2.475−2 1.110−2 2.951−2 2.445−1 8.808−3 1.531−2 1.552−2 1.692−1 2.945−2 8.117−1 4.722−2 1.738−3 3.157−3 3.304−3 3.050−2 6.642−3 1.274−1 1.011−2 3.545−2 5.559−3 1.401−2 1.022−2 3.556−2 2.821−2 2.836−1 1.087−1 1.202+0
3.968−2 6.370−2 3.742−2 5.285−2 1.488−2 4.872−3 9.234−3 8.018−3 1.203−2 4.002−3 5.348−3 6.135−3 7.665−3 1.594−1 2.265+0 5.179−2 9.874−3 8.353−2 1.450−2 1.460−1 1.812−2 1.288−1 1.828−2 1.832−3 1.529−2 3.132−3 3.026−2 3.907−3 1.328−2 3.096−3 1.619−2 3.869−3 5.559−1 4.355+0 2.158−2 1.513−2 1.937−1 5.191−2 3.022−1 6.112−2 2.551−1 3.825−3 3.297−3 3.393−2 1.102−2 5.922−2 7.772−3 2.493−2 1.080−2 3.029−2 1.980−1 7.287−3 1.384−2 1.266−2 1.678−1 2.399−2 8.862−1 3.823−2 1.545−3 2.995−3 2.900−3 3.031−2 5.734−3 1.354−1 8.505−3 3.824−2 4.754−3 1.151−2 8.151−3 3.138−2 2.316−2 2.744−1 1.045−1 1.301+0
4.252−2 6.646−2 3.692−2 5.124−2 1.519−2 5.817−3 1.106−2 8.448−3 1.267−2 3.815−3 5.099−3 6.140−3 7.672−3 1.514−1 2.486+0 4.212−2 1.075−2 8.457−2 1.435−2 1.720−1 1.658−2 1.374−1 1.640−2 1.989−3 1.555−2 3.154−3 3.443−2 3.641−3 1.367−2 2.739−3 1.685−2 3.544−3 5.985−1 4.803+0 2.337−2 1.513−2 1.922−1 5.588−2 3.450−1 6.117−2 2.629−1 4.158−3 3.314−3 3.449−2 1.155−2 6.667−2 7.414−3 2.532−2 1.058−2 3.119−2 1.566−1 6.258−3 1.327−2 1.057−2 1.675−1 1.971−2 9.887−1 3.102−2 1.393−3 2.910−3 2.546−3 3.021−2 4.894−3 1.463−1 7.021−3 4.186−2 4.050−3 9.798−3 6.576−3 2.902−2 1.920−2 2.685−1 1.042−1 1.442+0
4.586−2 7.038−2 3.672−2 5.029−2 1.553−2 7.093−3 1.352−2 8.945−3 1.342−2 3.676−3 4.914−3 6.220−3 7.773−3 1.449−1 2.721+0 3.476−2 1.246−2 8.584−2 1.460−2 2.062−1 1.551−2 1.471−1 1.514−2 2.252−3 1.582−2 3.215−3 3.988−2 3.419−3 1.414−2 2.447−3 1.752−2 3.281−3 6.455−1 5.274+0 2.700−2 1.552−2 1.927−1 6.202−2 4.048−1 6.235−2 2.749−1 4.720−3 3.377−3 3.510−2 1.240−2 7.652−2 7.164−3 2.589−2 1.045−2 3.214−2 1.238−1 5.607−3 1.350−2 9.159−3 1.679−1 1.655−2 1.122+0 2.554−2 1.282−3 2.913−3 2.262−3 3.020−2 4.179−3 1.605−1 5.754−3 4.617−2 3.486−3 8.707−3 5.426−3 2.840−2 1.627−2 2.653−1 1.081−1 1.629+0
4.924−2 7.467−2 3.665−2 4.974−2 1.581−2 8.665−3 1.655−2 9.443−3 1.416−2 3.580−3 4.786−3 6.344−3 7.928−3 1.396−1 2.950+0 2.962−2 1.488−2 8.695−2 1.508−2 2.476−1 1.476−2 1.567−1 1.434−2 2.608−3 1.603−2 3.300−3 4.642−2 3.240−3 1.461−2 2.225−3 1.806−2 3.078−3 6.917−1 5.723+0 3.221−2 1.613−2 1.938−1 6.999−2 4.792−1 6.408−2 2.882−1 5.484−3 3.466−3 3.563−2 1.352−2 8.840−2 7.003−3 2.651−2 1.036−2 3.293−2 9.954−2 5.221−3 1.440−2 8.289−3 1.684−1 1.431−2 1.281+0 2.155−2 1.206−3 2.999−3 2.051−3 3.019−2 3.609−3 1.774−1 4.745−3 5.069−2 3.064−3 8.046−3 4.610−3 2.918−2 1.419−2 2.634−1 1.154−1 1.855+0
5.122−2 7.711−2 3.598−2 4.855−2 1.571−2 1.013−2 1.938−2 9.690−3 1.453−2 3.457−3 4.621−3 6.357−3 7.944−3 1.333−1 3.096+0 2.591−2 1.727−2 8.616−2 1.531−2 2.853−1 1.400−2 1.618−1 1.364−2 2.946−3 1.587−2 3.326−3 5.219−2 3.052−3 1.473−2 2.033−3 1.810−2 2.879−3 7.198−1 6.005+0 3.740−2 1.646−2 1.914−1 7.715−2 5.476−1 6.462−2 2.948−1 6.210−3 3.492−3 3.535−2 1.448−2 9.884−2 6.783−3 2.655−2 1.010−2 3.285−2 8.155−2 4.924−3 1.536−2 7.685−3 1.657−1 1.261−2 1.419+0 1.851−2 1.137−3 3.077−3 1.878−3 2.959−2 3.140−3 1.910−1 3.946−3 5.373−2 2.727−3 7.539−3 3.993−3 3.028−2 1.259−2 2.574−1 1.223−1 2.052+0
5.410−2 8.056−2 3.670−2 4.892−2 1.722−2 1.080−2 2.065−2 1.006−2 1.505−2 3.393−3 4.538−3 6.749−3 8.426−3 1.340−1 3.264+0 1.993−2 1.882−2 9.272−2 1.643−2 3.092−1 1.413−2 1.700−1 1.342−2 3.202−3 1.820−2 3.667−3 5.409−2 3.082−3 1.495−2 2.028−3 1.863−2 2.975−3 7.580−1 6.353+0 4.034−2 1.765−2 2.038−1 8.222−2 5.873−1 6.675−2 3.051−1 6.696−3 3.839−3 4.023−2 1.490−2 1.022−1 6.845−3 2.694−2 1.041−2 3.375−2 5.988−2 4.607−3 1.539−2 7.118−3 1.714−1 1.165−2 1.510+0 1.711−2 1.136−3 3.236−3 2.082−3 3.171−2 3.179−3 1.992−1 3.974−3 5.679−2 2.938−3 6.983−3 3.564−3 2.982−2 1.181−2 2.635−1 1.271−1 2.176+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
2.203−3 2.445−3 7.598−3 7.799−3 5.095−2 2.109−2 1.641−1 1.174−2 4.863−2 4.498+0 8.628+0 4.109−1 6.164−1 3.732−2 4.991−2 2.429−1 3.427−2 6.340−2 7.268−2 1.079−1 7.939−2 1.056−1 4.067−2 5.080−2 5.282−1 7.954+0 6.733−2 3.221−1 3.107−2 1.822−2 2.573−1 3.249−2 1.873−1 3.481−2 2.381−1 2.805−2 1.430−1 2.730−2 1.761+0 1.485+1 1.320−1 5.760−1 3.820−2 3.484−2 5.498−1 8.345−2 3.823−1 1.063−1 4.373−1 8.463−2 2.586−1 2.652−1 9.235+0 6.204−2 1.591−2 2.849−2 2.213−2 5.294−1 3.393−2 1.010+0 4.881−2 6.516−1 4.916−2 7.100−1 1.235+1 2.406−2 1.412−2 6.244−2 3.434−2 8.124−1 1.259−1 1.476+0 1.274−1 9.269−1
3.361−3 2.953−3 8.755−3 8.427−3 5.079−2 2.259−2 1.745−1 1.171−2 4.795−2 4.676+0 1.117+1 4.974−1 7.436−1 9.661−2 1.347−1 2.285−1 3.646−2 6.712−2 7.123−2 1.060−1 7.999−2 1.066−1 4.233−2 5.291−2 6.789−1 8.281+0 1.394−1 4.086−1 1.194−1 2.517−2 2.305−1 2.992−2 1.921−1 3.263−2 2.327−1 2.918−2 1.473−1 2.929−2 2.328+0 1.825+1 2.720−1 8.561−1 5.308−2 3.319−2 4.928−1 8.196−2 3.893−1 1.063−1 4.294−1 8.858−2 2.668−1 4.464−1 1.077+1 2.986−1 2.188−2 3.583−2 2.312−2 4.933−1 3.335−2 1.008+0 4.716−2 6.371−1 4.808−2 1.339+0 1.918+1 3.323−2 1.503−2 7.519−2 3.403−2 7.583−1 1.240−1 1.469+0 1.246−1 9.074−1
2.943−3 2.617−3 8.067−3 7.584−3 4.998−2 2.130−2 1.794−1 1.095−2 4.942−2 5.084+0 1.153+1 4.754−1 7.089−1 8.309−2 1.150−1 2.325−1 4.286−2 7.916−2 7.598−2 1.131−1 8.063−2 1.075−1 4.251−2 5.314−2 6.415−1 9.055+0 1.243−1 3.823−1 9.586−2 2.603−2 2.349−1 3.137−2 2.202−1 3.274−2 2.472−1 2.893−2 1.480−1 2.770−2 2.447+0 1.955+1 2.337−1 7.798−1 5.518−2 3.441−2 5.032−1 8.791−2 4.423−1 1.102−1 4.546−1 8.665−2 2.667−1 3.928−1 1.252+1 2.344−1 2.002−2 3.650−2 2.269−2 5.018−1 3.250−2 1.109+0 4.446−2 6.702−1 4.468−2 1.450+0 2.162+1 3.046−2 1.414−2 7.576−2 3.311−2 7.708−1 1.283−1 1.613+0 1.245−1 9.520−1
2.599−3 2.280−3 7.437−3 6.671−3 4.917−2 1.998−2 1.869−1 1.022−2 5.185−2 5.552+0 1.192+1 4.514−1 6.732−1 7.087−2 9.733−2 2.374−1 5.246−2 9.724−2 8.200−2 1.221−1 8.116−2 1.082−1 4.303−2 5.379−2 5.974−1 9.947+0 1.110−1 3.574−1 7.482−2 2.894−2 2.400−1 3.342−2 2.603−1 3.283−2 2.651−1 2.884−2 1.485−1 2.621−2 2.577+0 2.091+1 1.991−1 7.068−1 6.166−2 3.642−2 5.157−1 9.640−2 5.176−1 1.153−1 4.858−1 8.483−2 2.665−1 3.435−1 1.434+1 1.777−1 1.915−2 3.879−2 2.268−2 5.113−1 3.189−2 1.249+0 4.184−2 7.109−1 4.157−2 1.553+0 2.398+1 2.915−2 1.350−2 7.920−2 3.246−2 7.850−1 1.356−1 1.815+0 1.256−1 1.007+0
2.316−3 1.959−3 6.909−3 5.757−3 4.844−2 1.883−2 1.977−1 9.626−3 5.543−2 6.064+0 1.245+1 4.299−1 6.423−1 6.142−2 8.378−2 2.426−1 6.596−2 1.227−1 8.915−2 1.327−1 8.157−2 1.087−1 4.387−2 5.485−2 5.571−1 1.090+1 1.013−1 3.367−1 5.828−2 3.405−2 2.453−1 3.602−2 3.149−1 3.290−2 2.858−1 2.896−2 1.490−1 2.494−2 2.726+0 2.238+1 1.713−1 6.463−1 7.286−2 3.909−2 5.293−1 1.080−1 6.202−1 1.216−1 5.221−1 8.330−2 2.664−1 3.037−1 1.606+1 1.334−1 1.898−2 4.293−2 2.311−2 5.215−1 3.162−2 1.438+0 3.951−2 7.577−1 3.902−2 1.650+0 2.619+1 2.888−2 1.306−2 8.595−2 3.218−2 8.001−1 1.468−1 2.086+0 1.279−1 1.071+0
2.093−3 1.670−3 6.533−3 4.915−3 4.787−2 1.801−2 2.127−1 9.239−3 6.022−2 6.602+0 1.314+1 4.125−1 6.173−1 5.486−2 7.441−2 2.478−1 8.403−2 1.567−1 9.699−2 1.444−1 8.190−2 1.091−1 4.499−2 5.624−2 5.239−1 1.189+1 9.515−2 3.204−1 4.625−2 4.153−2 2.505−1 3.899−2 3.864−1 3.297−2 3.081−1 2.926−2 1.495−1 2.399−2 2.891+0 2.395+1 1.507−1 5.997−1 8.919−2 4.220−2 5.431−1 1.232−1 7.542−1 1.285−1 5.610−1 8.219−2 2.666−1 2.738−1 1.764+1 1.014−1 1.927−2 4.919−2 2.404−2 5.315−1 3.170−2 1.682+0 3.762−2 8.074−1 3.716−2 1.742+0 2.824+1 2.931−2 1.276−2 9.647−2 3.228−2 8.152−1 1.625−1 2.438+0 1.314−1 1.140+0
1.930−3 1.428−3 6.345−3 4.199−3 4.750−2 1.766−2 2.326−1 9.086−3 6.603−2 7.152+0 1.396+1 3.987−1 5.977−1 5.073−2 6.849−2 2.525−1 1.071−1 1.999−1 1.049−1 1.562−1 8.221−2 1.095−1 4.626−2 5.783−2 4.976−1 1.287+1 9.195−2 3.078−1 3.793−2 5.146−2 2.552−1 4.208−2 4.759−1 3.306−2 3.299−1 2.969−2 1.501−1 2.335−2 3.067+0 2.558+1 1.359−1 5.651−1 1.109−1 4.543−2 5.561−1 1.423−1 9.222−1 1.354−1 5.992−1 8.157−2 2.673−1 2.520−1 1.907+1 7.967−2 1.982−2 5.768−2 2.544−2 5.406−1 3.205−2 1.984+0 3.621−2 8.561−1 3.597−2 1.829+0 3.013+1 3.015−2 1.259−2 1.110−1 3.265−2 8.290−1 1.833−1 2.876+0 1.354−1 1.207+0
1.817−3 1.237−3 6.337−3 3.628−3 4.719−2 1.777−2 2.563−1 9.116−3 7.220−2 7.673+0 1.481+1 3.868−1 5.807−1 4.826−2 6.492−2 2.558−1 1.340−1 2.504−1 1.116−1 1.664−1 8.236−2 1.097−1 4.739−2 5.925−2 4.753−1 1.378+1 9.058−2 2.973−1 3.233−2 6.330−2 2.584−1 4.483−2 5.791−1 3.310−2 3.481−1 3.009−2 1.506−1 2.296−2 3.236+0 2.712+1 1.251−1 5.381−1 1.367−1 4.825−2 5.657−1 1.641−1 1.116+0 1.411−1 6.306−1 8.118−2 2.677−1 2.359−1 2.028+1 6.535−2 2.039−2 6.788−2 2.713−2 5.468−1 3.241−2 2.331+0 3.518−2 8.961−1 3.523−2 1.905+0 3.176+1 3.104−2 1.248−2 1.286−1 3.303−2 8.384−1 2.078−1 3.377+0 1.389−1 1.262+0
1.714−3 1.079−3 6.342−3 3.158−3 4.606−2 1.789−2 2.755−1 9.075−3 7.635−2 7.971+0 1.531+1 3.698−1 5.560−1 4.603−2 6.178−2 2.529−1 1.582−1 2.957−1 1.143−1 1.706−1 8.083−2 1.077−1 4.734−2 5.920−2 4.485−1 1.428+1 8.859−2 2.835−1 2.822−2 7.391−2 2.554−1 4.604−2 6.695−1 3.247−2 3.542−1 2.982−2 1.480−1 2.230−2 3.319+0 2.792+1 1.154−1 5.081−1 1.599−1 4.938−2 5.610−1 1.822−1 1.285+0 1.424−1 6.402−1 7.943−2 2.629−1 2.199−1 2.085+1 5.543−2 2.046−2 7.683−2 2.824−2 5.395−1 3.204−2 2.624+0 3.382−2 9.064−1 3.415−2 1.929+0 3.245+1 3.118−2 1.218−2 1.438−1 3.267−2 8.273−1 2.280−1 3.802+0 1.388−1 1.276+0
1.714−3 1.090−3 6.699−3 3.199−3 4.923−2 1.853−2 2.870−1 9.659−3 8.059−2 8.238+0 1.562+1 3.804−1 5.721−1 4.468−2 5.975−2 2.669−1 1.696−1 3.188−1 1.205−1 1.791−1 9.458−2 1.261−1 5.046−2 6.309−2 4.637−1 1.486+1 8.785−2 2.909−1 2.371−2 8.173−2 2.764−1 5.061−2 7.192−1 3.754−2 3.652−1 3.166−2 1.581−1 2.355−2 3.306+0 2.799+1 1.128−1 5.132−1 1.752−1 5.446−2 6.091−1 1.979−1 1.375+0 1.481−1 6.610−1 8.387−2 2.774−1 2.214−1 2.223+1 4.282−2 2.008−2 8.196−2 3.130−2 5.650−1 3.462−2 2.792+0 3.750−2 9.458−1 3.633−2 2.064+0 3.536+1 3.043−2 1.353−2 1.530−1 3.526−2 8.663−1 2.421−1 4.032+0 1.459−1 1.331+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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77
Table 28 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.20
6.40
6.60
6.80
7.00
7.20
7.40
7.60
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.361−1 5.945−3 1.218−2 1.254−2 4.670−2 2.351−2 6.682−1 4.868−2 3.628+0 8.812−2 7.944−3 7.156−3 2.572−2 1.889−2 7.485−2 4.876−2 9.079−1 2.262−1 4.739+0 1.145+1 2.220+1 1.161+0 1.740+0 1.324−1 1.769−1 3.712−2 4.654−2 1.357+0 2.170+1 1.818−1 1.258+0 8.760−2 7.978−2 2.522−2 4.771+0 4.061+1 4.724−1 2.227+0 5.980−2 1.482−1 6.891−1 2.904+1 1.269−1 1.041+0 6.278−2 2.277+0 4.339+1 1.852−1 1.471+0 4.487−1 2.390+1 1.185−1 1.225+0 3.172+1 4.202−1
8.013−1 1.045−2 1.554−2 1.507−2 5.575−2 2.395−2 6.436−1 4.668−2 3.628+0 8.343−2 1.303−2 8.685−3 3.007−2 1.906−2 8.544−2 4.682−2 8.743−1 2.216−1 4.729+0 1.306+1 2.465+1 1.129+0 1.697+0 1.451−1 1.934−1 3.837−2 4.799−2 1.283+0 2.570+1 2.013−1 1.209+0 8.895−2 8.811−2 2.448−2 6.032+0 5.011+1 4.594−1 2.139+0 6.145−2 1.618−1 6.576−1 5.055+1 1.331−1 9.990−1 5.943−2 4.899+0 7.942+1 1.770−1 1.412+0 4.238−1 4.848+1 1.072−1 3.456+0 6.842+1 3.688−1
6.372−1 8.502−3 1.410−2 1.311−2 5.395−2 2.134−2 6.470−1 4.148−2 3.875+0 7.359−2 1.077−2 7.368−3 2.758−2 1.661−2 8.271−2 4.160−2 8.771−1 2.205−1 5.049+0 1.420+1 2.671+1 1.114+0 1.676+0 1.464−1 1.954−1 3.684−2 4.607−2 1.260+0 2.793+1 2.046−1 1.188+0 8.729−2 8.758−2 2.258−2 6.567+0 5.462+1 4.507−1 2.099+0 5.874−2 1.596−1 6.442−1 5.536+1 1.313−1 9.769−1 5.408−2 5.300+0 8.679+1 1.685−1 1.378+0 4.062−1 5.282+1 9.670−2 3.636+0 7.431+1 3.328−1
4.901−1 7.099−3 1.313−2 1.147−2 5.311−2 1.885−2 6.513−1 3.647−2 4.217+0 6.406−2 9.115−3 6.231−3 2.567−2 1.426−2 8.105−2 3.659−2 8.812−1 2.232−1 5.492+0 1.542+1 2.899+1 1.099+0 1.652+0 1.484−1 1.980−1 3.550−2 4.440−2 1.235+0 3.032+1 2.087−1 1.166+0 8.585−2 8.745−2 2.094−2 7.117+0 5.933+1 4.420−1 2.057+0 5.651−2 1.582−1 6.310−1 6.005+1 1.302−1 9.550−1 4.933−2 5.680+0 9.390+1 1.607−1 1.345+0 3.896−1 5.697+1 8.752−2 3.803+0 7.989+1 2.999−1
3.730−1 6.092−3 1.251−2 1.014−2 5.348−2 1.670−2 6.562−1 3.205−2 4.673+0 5.557−2 7.908−3 5.288−3 2.430−2 1.217−2 8.101−2 3.217−2 8.864−1 2.314−1 6.085+0 1.672+1 3.144+1 1.082+0 1.627+0 1.508−1 2.013−1 3.442−2 4.305−2 1.210+0 3.281+1 2.134−1 1.142+0 8.468−2 8.774−2 1.966−2 7.673+0 6.414+1 4.333−1 2.013+0 5.490−2 1.578−1 6.178−1 6.455+1 1.302−1 9.331−1 4.542−2 6.036+0 1.006+2 1.539−1 1.312+0 3.745−1 6.087+1 8.024−2 3.957+0 8.510+1 2.716−1
2.864−1 5.385−3 1.217−2 9.134−3 5.525−2 1.501−2 6.614−1 2.847−2 5.261+0 4.859−2 7.051−3 4.546−3 2.342−2 1.045−2 8.300−2 2.859−2 8.921−1 2.463−1 6.851+0 1.805+1 3.401+1 1.064+0 1.599+0 1.537−1 2.051−1 3.362−2 4.206−2 1.181+0 3.534+1 2.186−1 1.116+0 8.379−2 8.840−2 1.876−2 8.224+0 6.895+1 4.244−1 1.966+0 5.391−2 1.582−1 6.043−1 6.884+1 1.311−1 9.107−1 4.242−2 6.366+0 1.070+2 1.480−1 1.279+0 3.611−1 6.453+1 7.497−2 4.098+0 8.994+1 2.484−1
2.251−1 4.910−3 1.204−2 8.414−3 5.848−2 1.383−2 6.663−1 2.577−2 5.989+0 4.326−2 6.470−3 3.996−3 2.294−2 9.121−3 8.720−2 2.590−2 8.977−1 2.684−1 7.801+0 1.940+1 3.664+1 1.045+0 1.570+0 1.570−1 2.094−1 3.308−2 4.139−2 1.150+0 3.786+1 2.238−1 1.087+0 8.312−2 8.930−2 1.820−2 8.761+0 7.368+1 4.150−1 1.914+0 5.345−2 1.593−1 5.900−1 7.289+1 1.326−1 8.868−1 4.026−2 6.673+0 1.129+2 1.428−1 1.245+0 3.490−1 6.793+1 7.151−2 4.227+0 9.443+1 2.300−1
1.828−1 4.596−3 1.200−2 7.913−3 6.280−2 1.307−2 6.685−1 2.379−2 6.817+0 3.940−2 6.084−3 3.606−3 2.269−2 8.145−3 9.306−2 2.393−2 9.000−1 2.962−1 8.884+0 2.066+1 3.911+1 1.025+0 1.537+0 1.602−1 2.136−1 3.267−2 4.087−2 1.110+0 4.018+1 2.278−1 1.050+0 8.234−2 8.992−2 1.784−2 9.243+0 7.797+1 4.038−1 1.852+0 5.316−2 1.601−1 5.730−1 7.641+1 1.339−1 8.583−1 3.866−2 6.931+0 1.180+2 1.377−1 1.205+0 3.368−1 7.083+1 6.924−2 4.332+0 9.822+1 2.151−1
1.522−1 4.320−3 1.178−2 7.441−3 6.613−2 1.241−2 6.557−1 2.200−2 7.491+0 3.613−2 5.734−3 3.286−3 2.214−2 7.345−3 9.757−2 2.215−2 8.822−1 3.189−1 9.769+0 2.131+1 4.044+1 9.886−1 1.479+0 1.599−1 2.133−1 3.176−2 3.973−2 1.050+0 4.131+1 2.258−1 9.917−1 7.987−2 8.839−2 1.728−2 9.451+0 7.997+1 3.845−1 1.754+0 5.190−2 1.572−1 5.449−1 7.771+1 1.323−1 8.129−1 3.679−2 6.994+0 1.197+2 1.303−1 1.140+0 3.190−1 7.171+1 6.650−2 4.324+0 9.924+1 1.996−1
1.239−1 4.471−3 1.201−2 7.931−3 6.365−2 1.285−2 6.778−1 2.367−2 7.909+0 3.955−2 5.982−3 3.592−3 2.285−2 7.921−3 9.378−2 2.381−2 9.124−1 3.348−1 1.028+1 1.917+1 4.036+1 9.685−1 1.456+0 1.935−1 2.600−1 3.535−2 4.434−2 1.078+0 3.700+1 3.127−1 1.033+0 9.527−2 1.146−1 2.028−2 8.668+0 7.178+1 4.115−1 1.831+0 6.325−2 1.990−1 5.845−1 7.896+1 1.560−1 8.572−1 4.098−2 6.502+0 1.329+2 1.391−1 1.202+0 3.410−1 7.122+1 1.479−1 3.736+0 9.432+1 2.261−1
78
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 29 Effective collision strengths for transitions in Mn XXIII. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.825−1 3.526−1 1.584−2 4.742−3 8.808−3 1.210−2 1.807−2 3.157−3 1.170−3 2.215−3 2.185−3 3.278−3 1.313−3 1.743−3 1.231−3 4.915−4 9.310−4 8.415−4 1.263−3 6.900−4 9.166−4 8.921−5 1.111−4 3.101−2 1.118−3 1.709−2 4.461−3 5.849−2 8.264−3 3.565−4 3.528−3 1.458−3 1.071−2 2.568−3 1.745−3 1.063−3 1.676−4 1.410−3 6.988−4 4.009−3 1.199−3 9.454−4 6.449−4 8.725−5 8.480−5 2.267−3 4.605−3 3.900−2 2.225−2 1.150−1 7.101−4 1.476−3 8.550−3 5.295−3 2.173−2 1.930−3 3.874−3 3.322−4 7.042−4 3.521−3 2.264−3 8.296−3 1.131−3 2.135−3 1.476−4 2.093−4 1.196+0 2.291+0 8.382−2 1.259−1 7.250−2 1.382−2 2.558−2
1.879−1 3.609−1 1.777−2 6.020−3 1.108−2 1.330−2 2.018−2 3.656−3 1.594−3 2.998−3 2.598−3 3.902−3 1.710−3 2.289−3 1.172−3 5.604−4 1.072−3 8.957−4 1.346−3 7.256−4 9.649−4 9.483−5 1.179−4 4.766−2 4.718−3 1.852−2 7.421−3 5.957−2 1.300−2 1.036−3 3.855−3 2.249−3 1.153−2 3.486−3 2.682−3 1.929−3 2.754−4 1.314−3 7.470−4 4.186−3 1.261−3 1.032−3 6.637−4 9.732−5 8.491−5 1.088−2 8.220−3 4.412−2 2.850−2 1.214−1 2.105−3 2.362−3 1.018−2 6.712−3 2.399−2 3.476−3 6.183−3 5.600−4 7.624−4 3.395−3 2.393−3 8.688−3 1.194−3 2.320−3 1.532−4 2.286−4 1.190+0 2.298+0 1.101−1 1.682−1 7.612−2 1.568−2 2.898−2
1.968−1 3.781−1 1.728−2 6.111−3 1.135−2 1.340−2 2.031−2 3.492−3 1.537−3 2.904−3 2.503−3 3.757−3 1.587−3 2.121−3 1.170−3 5.689−4 1.090−3 8.842−4 1.330−3 7.083−4 9.421−4 8.836−5 1.098−4 5.163−2 3.821−3 1.818−2 6.890−3 6.179−2 1.208−2 8.450−4 3.677−3 1.968−3 1.167−2 3.100−3 2.501−3 1.620−3 2.507−4 1.297−3 7.004−4 4.281−3 1.174−3 1.036−3 6.107−4 9.302−5 7.645−5 8.588−3 7.488−3 4.319−2 2.782−2 1.248−1 1.723−3 2.057−3 9.562−3 6.246−3 2.395−2 2.988−3 5.646−3 5.089−4 7.134−4 3.314−3 2.303−3 8.791−3 1.124−3 2.288−3 1.399−4 2.153−4 1.270+0 2.441+0 1.068−1 1.626−1 7.545−2 1.677−2 3.112−2
2.071−1 3.981−1 1.693−2 6.319−3 1.180−2 1.349−2 2.041−2 3.365−3 1.527−3 2.895−3 2.424−3 3.640−3 1.480−3 1.976−3 1.175−3 5.885−4 1.129−3 8.719−4 1.312−3 6.895−4 9.174−4 8.114−5 1.008−4 5.196−2 3.109−3 1.781−2 6.159−3 6.488−2 1.071−2 6.960−4 3.535−3 1.708−3 1.199−2 2.702−3 2.385−3 1.334−3 2.284−4 1.282−3 6.465−4 4.425−3 1.065−3 1.053−3 5.475−4 8.916−5 6.689−5 6.853−3 6.621−3 4.188−2 2.675−2 1.294−1 1.423−3 1.777−3 8.991−3 5.801−3 2.423−2 2.551−3 5.238−3 4.635−4 6.581−4 3.231−3 2.198−3 8.968−3 1.044−3 2.273−3 1.251−4 2.021−4 1.375+0 2.627+0 1.013−1 1.538−1 7.543−2 1.898−2 3.528−2
2.197−1 4.219−1 1.674−2 6.783−3 1.270−2 1.373−2 2.072−2 3.290−3 1.582−3 3.008−3 2.377−3 3.572−3 1.399−3 1.866−3 1.186−3 6.247−4 1.200−3 8.614−4 1.297−3 6.717−4 8.941−4 7.378−5 9.174−5 4.864−2 2.582−3 1.750−2 5.405−3 6.953−2 9.224−3 5.861−4 3.434−3 1.479−3 1.257−2 2.313−3 2.359−3 1.086−3 2.088−4 1.269−3 5.873−4 4.643−3 9.399−4 1.091−3 4.781−4 8.643−5 5.688−5 5.617−3 5.775−3 4.063−2 2.585−2 1.368−1 1.201−3 1.534−3 8.526−3 5.424−3 2.498−2 2.194−3 5.014−3 4.240−4 5.979−4 3.148−3 2.088−3 9.266−3 9.626−4 2.291−3 1.101−4 1.906−4 1.503+0 2.856+0 9.548−2 1.446−1 7.601−2 2.262−2 4.208−2
2.356−1 4.512−1 1.674−2 7.631−3 1.433−2 1.421−2 2.140−2 3.265−3 1.718−3 3.277−3 2.368−3 3.562−3 1.347−3 1.796−3 1.204−3 6.844−4 1.317−3 8.564−4 1.290−3 6.579−4 8.761−4 6.699−5 8.334−5 4.306−2 2.245−3 1.732−2 4.744−3 7.641−2 7.829−3 5.111−4 3.373−3 1.284−3 1.349−2 1.948−3 2.432−3 8.781−4 1.929−4 1.261−3 5.266−4 4.962−3 8.070−4 1.158−3 4.082−4 8.538−5 4.722−5 4.848−3 5.057−3 3.970−2 2.551−2 1.485−1 1.050−3 1.330−3 8.179−3 5.148−3 2.638−2 1.926−3 4.994−3 3.929−4 5.366−4 3.071−3 1.988−3 9.742−3 8.889−4 2.360−3 9.619−5 1.823−4 1.648+0 3.118+0 9.038−2 1.367−1 7.704−2 2.793−2 5.206−2
2.548−1 4.867−1 1.690−2 8.962−3 1.687−2 1.496−2 2.249−2 3.282−3 1.948−3 3.727−3 2.400−3 3.613−3 1.321−3 1.761−3 1.227−3 7.744−4 1.493−3 8.599−4 1.297−3 6.498−4 8.658−4 6.136−5 7.640−5 3.695−2 2.095−3 1.728−2 4.225−3 8.602−2 6.636−3 4.681−4 3.346−3 1.123−3 1.480−2 1.621−3 2.598−3 7.118−4 1.826−4 1.256−3 4.689−4 5.404−3 6.777−4 1.257−3 3.440−4 8.615−5 3.863−5 4.511−3 4.505−3 3.917−2 2.600−2 1.653−1 9.665−4 1.163−3 7.941−3 5.003−3 2.852−2 1.744−3 5.172−3 3.738−4 4.789−4 3.007−3 1.918−3 1.045−2 8.321−4 2.490−3 8.443−5 1.779−4 1.800+0 3.400+0 8.635−2 1.304−1 7.829−2 3.507−2 6.547−2
2.752−1 5.245−1 1.709−2 1.070−2 2.019−2 1.582−2 2.376−2 3.305−3 2.252−3 4.320−3 2.450−3 3.691−3 1.307−3 1.742−3 1.245−3 8.875−4 1.715−3 8.670−4 1.308−3 6.436−4 8.579−4 5.690−5 7.091−5 3.142−2 2.098−3 1.725−2 3.839−3 9.764−2 5.666−3 4.507−4 3.322−3 9.924−4 1.637−2 1.342−3 2.816−3 5.829−4 1.779−4 1.249−3 4.169−4 5.920−3 5.607−4 1.371−3 2.888−4 8.775−5 3.146−5 4.523−3 4.102−3 3.878−2 2.719−2 1.861−1 9.366−4 1.030−3 7.750−3 4.969−3 3.117−2 1.631−3 5.469−3 3.663−4 4.271−4 2.942−3 1.877−3 1.129−2 7.921−4 2.654−3 7.494−5 1.760−4 1.940+0 3.662+0 8.292−2 1.252−1 7.908−2 4.342−2 8.115−2
2.873−1 5.469−1 1.678−2 1.220−2 2.304−2 1.618−2 2.428−2 3.231−3 2.495−3 4.797−3 2.433−3 3.667−3 1.264−3 1.685−3 1.221−3 9.736−4 1.884−3 8.501−4 1.283−3 6.206−4 8.276−4 5.226−5 6.518−5 2.660−2 2.138−3 1.677−2 3.487−3 1.064−1 4.833−3 4.389−4 3.209−3 8.726−4 1.740−2 1.100−3 2.947−3 4.793−4 1.727−4 1.205−3 3.658−4 6.235−3 4.564−4 1.437−3 2.407−4 8.687−5 2.546−5 4.621−3 3.737−3 3.748−2 2.795−2 2.017−1 9.174−4 9.077−4 7.392−3 4.877−3 3.286−2 1.527−3 5.626−3 3.577−4 3.759−4 2.803−3 1.812−3 1.178−2 7.470−4 2.735−3 6.623−5 1.704−4 1.997+0 3.773+0 7.807−2 1.178−1 7.717−2 5.005−2 9.360−2
3.031−1 5.783−1 1.781−2 1.381−2 2.606−2 1.724−2 2.578−2 3.520−3 2.814−3 5.389−3 2.531−3 3.807−3 1.327−3 1.763−3 1.363−3 1.097−3 2.106−3 8.755−4 1.319−3 6.559−4 8.721−4 5.461−5 6.802−5 2.051−2 2.145−3 1.797−2 3.451−3 1.174−1 4.442−3 4.387−4 3.602−3 8.815−4 1.886−2 1.035−3 3.182−3 4.492−4 1.698−4 1.415−3 3.804−4 6.670−3 4.458−4 1.590−3 2.508−4 1.102−4 2.707−5 4.605−3 3.685−3 3.990−2 2.973−2 2.209−1 9.162−4 9.135−4 8.147−3 5.091−3 3.539−2 1.546−3 5.994−3 3.517−4 3.917−4 3.226−3 1.890−3 1.255−2 8.025−4 2.998−3 6.962−5 1.779−4 2.141+0 4.105+0 7.910−2 1.192−1 8.237−2 5.665−2 1.063−1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
79
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
3.151−2 4.685−2 3.074−2 4.097−2 1.308−2 3.030−3 5.777−3 6.601−3 9.863−3 3.551−3 4.745−3 5.649−3 7.054−3 1.372−1 1.675+0 2.116−2 5.027−3 7.746−2 1.096−2 9.955−2 1.395−2 1.045−1 1.485−2 1.510−3 1.449−2 2.938−3 1.959−2 3.841−3 1.139−2 3.617−3 1.300−2 4.342−3 3.943−1 3.225+0 1.029−2 1.174−2 1.676−1 3.836−2 1.983−1 4.966−2 1.927−1 3.055−3 3.057−3 3.202−2 8.717−3 3.952−2 7.908−3 2.207−2 1.036−2 2.517−2 9.873−2 4.137−3 7.981−3 7.922−3 1.508−1 1.862−2 6.720−1 3.252−2 1.322−3 2.885−3 3.186−3 2.866−2 7.005−3 1.020−1 1.088−2 3.059−2 6.467−3 6.247−3 5.350−3 1.867−2 1.873−2 2.362−1 8.346−2 9.800−1
3.272−2 5.038−2 3.768−2 5.190−2 1.312−2 3.277−3 6.155−3 6.658−3 9.982−3 4.174−3 5.580−3 5.855−3 7.317−3 1.653−1 1.704+0 7.089−2 1.084−2 7.680−2 1.457−2 1.008−1 2.005−2 1.055−1 2.319−2 1.698−3 1.357−2 2.969−3 2.184−2 4.258−3 1.158−2 3.783−3 1.356−2 4.435−3 4.494−1 3.264+0 2.278−2 1.694−2 1.792−1 4.679−2 2.117−1 6.132−2 2.064−1 3.434−3 3.116−3 3.032−2 9.757−3 4.403−2 8.203−3 2.257−2 1.070−2 2.623−2 2.799−1 1.147−2 1.821−2 1.899−2 1.602−1 3.559−2 6.763−1 5.796−2 1.947−3 3.264−3 3.679−3 2.831−2 7.402−3 1.083−1 1.159−2 2.980−2 6.348−3 1.863−2 1.339−2 4.302−2 3.551−2 2.655−1 1.116−1 1.004+0
3.358−2 5.124−2 3.632−2 4.967−2 1.326−2 3.568−3 6.711−3 6.845−3 1.026−2 3.975−3 5.314−3 5.735−3 7.166−3 1.596−1 1.801+0 6.400−2 9.435−3 7.647−2 1.355−2 1.092−1 1.812−2 1.086−1 2.029−2 1.620−3 1.371−2 2.910−3 2.336−2 4.007−3 1.171−2 3.434−3 1.393−2 4.100−3 4.640−1 3.447+0 2.006−2 1.559−2 1.767−1 4.612−2 2.246−1 5.834−2 2.085−1 3.299−3 3.051−3 3.053−2 9.756−3 4.664−2 7.778−3 2.252−2 1.036−2 2.663−2 2.509−1 9.170−3 1.549−2 1.561−2 1.574−1 2.967−2 7.109−1 4.823−2 1.708−3 3.019−3 3.282−3 2.807−2 6.622−3 1.124−1 1.022−2 3.114−2 5.599−3 1.485−2 1.080−2 3.657−2 2.966−2 2.566−1 1.036−1 1.048+0
3.507−2 5.310−2 3.518−2 4.778−2 1.348−2 4.031−3 7.597−3 7.107−3 1.066−2 3.771−3 5.041−3 5.644−3 7.053−3 1.516−1 1.944+0 5.407−2 8.874−3 7.660−2 1.290−2 1.221−1 1.645−2 1.135−1 1.775−2 1.618−3 1.389−2 2.873−3 2.557−2 3.742−3 1.191−2 3.067−3 1.441−2 3.755−3 4.883−1 3.738+0 1.901−2 1.465−2 1.745−1 4.667−2 2.463−1 5.635−2 2.139−1 3.319−3 3.012−3 3.087−2 9.882−3 5.051−2 7.353−3 2.259−2 1.006−2 2.722−2 2.096−1 7.458−3 1.357−2 1.274−2 1.552−1 2.433−2 7.635−1 3.938−2 1.511−3 2.825−3 2.894−3 2.787−2 5.792−3 1.183−1 8.755−3 3.316−2 4.836−3 1.199−2 8.612−3 3.146−2 2.438−2 2.492−1 9.770−2 1.119+0
3.724−2 5.606−2 3.438−2 4.643−2 1.374−2 4.719−3 8.916−3 7.450−3 1.117−2 3.581−3 4.788−3 5.605−3 7.005−3 1.435−1 2.126+0 4.419−2 9.119−3 7.718−2 1.267−2 1.410−1 1.514−2 1.202−1 1.577−2 1.697−3 1.411−2 2.866−3 2.867−2 3.484−3 1.222−2 2.715−3 1.498−2 3.430−3 5.227−1 4.115+0 1.962−2 1.420−2 1.736−1 4.891−2 2.796−1 5.563−2 2.231−1 3.511−3 3.008−3 3.131−2 1.020−2 5.604−2 6.975−3 2.283−2 9.810−3 2.797−2 1.680−1 6.251−3 1.247−2 1.053−2 1.541−1 1.995−2 8.389−1 3.198−2 1.351−3 2.696−3 2.537−3 2.773−2 4.978−3 1.265−1 7.317−3 3.594−2 4.127−3 9.949−3 6.894−3 2.802−2 2.003−2 2.441−1 9.505−2 1.223+0
4.001−2 5.999−2 3.392−2 4.563−2 1.404−2 5.683−3 1.077−2 7.868−3 1.180−2 3.427−3 4.582−3 5.634−3 7.041−3 1.365−1 2.332+0 3.601−2 1.015−2 7.811−2 1.282−2 1.668−1 1.419−2 1.284−1 1.434−2 1.869−3 1.435−2 2.896−3 3.285−2 3.254−3 1.261−2 2.407−3 1.559−2 3.151−3 5.637−1 4.536+0 2.191−2 1.422−2 1.741−1 5.307−2 3.265−1 5.610−2 2.356−1 3.895−3 3.044−3 3.183−2 1.078−2 6.356−2 6.682−3 2.325−2 9.638−3 2.882−2 1.326−1 5.451−3 1.217−2 8.944−3 1.539−1 1.658−2 9.411−1 2.613−2 1.228−3 2.643−3 2.232−3 2.767−2 4.246−3 1.374−1 6.020−3 3.946−2 3.523−3 8.581−3 5.605−3 2.630−2 1.668−2 2.413−1 9.603−2 1.367+0
4.316−2 6.454−2 3.373−2 4.525−2 1.434−2 6.956−3 1.322−2 8.337−3 1.250−2 3.318−3 4.436−3 5.729−3 7.159−3 1.310−1 2.547+0 3.000−2 1.192−2 7.922−2 1.326−2 2.002−1 1.353−2 1.375−1 1.342−2 2.138−3 1.459−2 2.962−3 3.821−2 3.067−3 1.307−2 2.163−3 1.618−2 2.930−3 6.077−1 4.969+0 2.583−2 1.459−2 1.757−1 5.923−2 3.880−1 5.748−2 2.501−1 4.485−3 3.116−3 3.239−2 1.165−2 7.328−2 6.488−3 2.383−2 9.538−3 2.968−2 1.052−1 4.958−3 1.259−2 7.913−3 1.543−1 1.413−2 1.072+0 2.175−2 1.141−3 2.674−3 1.995−3 2.768−2 3.637−3 1.514−1 4.939−3 4.353−2 3.051−3 7.727−3 4.676−3 2.613−2 1.425−2 2.403−1 1.007−1 1.552+0
4.608−2 6.873−2 3.355−2 4.492−2 1.453−2 8.426−3 1.604−2 8.755−3 1.313−2 3.234−3 4.325−3 5.832−3 7.289−3 1.262−1 2.742+0 2.585−2 1.420−2 7.985−2 1.377−2 2.381−1 1.303−2 1.454−1 1.282−2 2.471−3 1.471−2 3.032−3 4.421−2 2.909−3 1.344−2 1.975−3 1.658−2 2.754−3 6.472−1 5.350+0 3.084−2 1.506−2 1.767−1 6.658−2 4.582−1 5.897−2 2.631−1 5.211−3 3.192−3 3.273−2 1.269−2 8.421−2 6.346−3 2.432−2 9.435−3 3.024−2 8.521−2 4.655−3 1.349−2 7.282−3 1.542−1 1.238−2 1.217+0 1.855−2 1.078−3 2.764−3 1.820−3 2.758−2 3.153−3 1.667−1 4.087−3 4.743−2 2.698−3 7.196−3 4.012−3 2.705−2 1.252−2 2.388−1 1.078−1 1.760+0
4.699−2 6.995−2 3.243−2 4.336−2 1.419−2 9.548−3 1.820−2 8.808−3 1.321−2 3.084−3 4.124−3 5.748−3 7.183−3 1.191−1 2.818+0 2.263−2 1.602−2 7.777−2 1.383−2 2.664−1 1.230−2 1.471−1 1.210−2 2.720−3 1.431−2 3.003−3 4.839−2 2.711−3 1.331−2 1.792−3 1.631−2 2.551−3 6.601−1 5.496+0 3.488−2 1.504−2 1.721−1 7.164−2 5.102−1 5.849−2 2.651−1 5.756−3 3.161−3 3.191−2 1.331−2 9.175−2 6.068−3 2.395−2 9.064−3 2.963−2 6.990−2 4.354−3 1.415−2 6.751−3 1.493−1 1.092−2 1.315+0 1.596−2 1.007−3 2.795−3 1.656−3 2.661−2 2.731−3 1.755−1 3.391−3 4.910−2 2.390−3 6.693−3 3.472−3 2.766−2 1.106−2 2.304−1 1.122−1 1.900+0
5.070−2 7.545−2 3.376−2 4.501−2 1.591−2 1.061−2 2.023−2 9.407−3 1.408−2 3.127−3 4.184−3 6.274−3 7.833−3 1.226−1 3.049+0 1.839−2 1.825−2 8.471−2 1.520−2 2.981−1 1.287−2 1.585−1 1.235−2 3.082−3 1.678−2 3.399−3 5.220−2 2.808−3 1.388−2 1.837−3 1.723−2 2.703−3 7.130−1 5.959+0 3.938−2 1.645−2 1.865−1 7.867−2 5.677−1 6.206−2 2.845−1 6.476−3 3.574−3 3.712−2 1.420−2 9.861−2 6.291−3 2.496−2 9.582−3 3.125−2 5.396−2 4.242−3 1.481−2 6.590−3 1.574−1 1.050−2 1.443+0 1.526−2 1.043−3 3.052−3 1.748−3 2.916−2 2.834−3 1.895−1 3.490−3 5.336−2 2.630−3 6.437−3 3.224−3 2.845−2 1.067−2 2.419−1 1.204−1 2.081+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
80
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.987−3 2.198−3 6.965−3 7.009−3 4.652−2 1.906−2 1.508−1 1.067−2 4.535−2 4.234+0 8.070+0 3.753−1 5.632−1 3.424−2 4.580−2 2.233−1 3.349−2 6.145−2 6.794−2 1.007−1 7.308−2 9.723−2 3.719−2 4.643−2 4.810−1 7.429+0 6.203−2 2.938−1 2.819−2 1.733−2 2.353−1 3.007−2 1.790−1 3.185−2 2.205−1 2.558−2 1.318−1 2.499−2 1.663+0 1.430+1 1.202−1 5.252−1 3.664−2 3.243−2 5.036−1 7.830−2 3.654−1 9.818−2 4.054−1 7.776−2 2.380−1 2.412−1 8.907+0 5.606−2 1.464−2 2.667−2 2.036−2 4.852−1 3.108−2 9.508−1 4.451−2 6.025−1 4.480−2 6.993−1 1.202+1 2.217−2 1.295−2 5.808−2 3.150−2 7.446−1 1.170−1 1.389+0 1.171−1 8.572−1
2.978−3 2.592−3 7.968−3 7.434−3 4.628−2 2.028−2 1.603−1 1.048−2 4.424−2 4.729+0 8.811+0 4.153−1 6.918−1 8.584−2 1.227−1 2.114−1 3.433−2 6.340−2 6.658−2 9.922−2 7.351−2 9.795−2 3.868−2 4.835−2 5.408−1 8.591+0 1.303−1 3.674−1 1.047−1 2.136−2 2.126−1 2.778−2 1.779−1 2.986−2 2.168−1 2.650−2 1.348−1 2.620−2 2.047+0 1.645+1 2.488−1 8.239−1 4.630−2 3.017−2 4.555−1 7.559−2 3.628−1 9.830−2 4.003−1 8.027−2 2.438−1 3.995−1 1.032+1 2.578−1 1.969−2 3.369−2 2.153−2 4.539−1 3.016−2 9.329−1 4.225−2 5.928−1 4.284−2 1.175+0 1.762+1 3.030−2 1.317−2 7.133−2 3.087−2 6.980−1 1.134−1 1.362+0 1.138−1 8.433−1
2.602−3 2.285−3 7.273−3 6.647−3 4.553−2 1.907−2 1.655−1 9.789−3 4.583−2 5.076+0 9.441+0 4.022−1 6.586−1 7.328−2 1.040−1 2.150−1 4.119−2 7.610−2 7.136−2 1.063−1 7.406−2 9.869−2 3.895−2 4.868−2 5.159−1 9.203+0 1.158−1 3.440−1 8.307−2 2.316−2 2.168−1 2.926−2 2.075−1 2.996−2 2.311−1 2.632−2 1.354−1 2.478−2 2.189+0 1.773+1 2.120−1 7.420−1 5.000−2 3.175−2 4.654−1 8.194−2 4.185−1 1.023−1 4.252−1 7.855−2 2.437−1 3.489−1 1.192+1 1.996−1 1.818−2 3.430−2 2.102−2 4.621−1 2.946−2 1.038+0 3.980−2 6.252−1 3.981−2 1.289+0 1.985+1 2.791−2 1.254−2 7.141−2 3.009−2 7.099−1 1.183−1 1.512+0 1.141−1 8.873−1
2.296−3 1.982−3 6.676−3 5.812−3 4.481−2 1.790−2 1.733−1 9.156−3 4.836−2 5.462+0 1.016+1 3.883−1 6.235−1 6.252−2 8.791−2 2.194−1 5.126−2 9.484−2 7.727−2 1.151−1 7.451−2 9.928−2 3.952−2 4.940−2 4.911−1 9.867+0 1.032−1 3.223−1 6.455−2 2.673−2 2.215−1 3.128−2 2.489−1 3.004−2 2.484−1 2.631−2 1.359−1 2.349−2 2.343+0 1.914+1 1.798−1 6.654−1 5.769−2 3.396−2 4.770−1 9.079−2 4.963−1 1.073−1 4.554−1 7.699−2 2.436−1 3.049−1 1.352+1 1.504−1 1.752−2 3.667−2 2.099−2 4.711−1 2.901−2 1.182+0 3.750−2 6.643−1 3.713−2 1.400+0 2.205+1 2.684−2 1.210−2 7.475−2 2.960−2 7.233−1 1.262−1 1.719+0 1.154−1 9.406−1
2.050−3 1.698−3 6.208−3 4.997−3 4.419−2 1.693−2 1.845−1 8.669−3 5.198−2 5.887+0 1.097+1 3.757−1 5.927−1 5.450−2 7.580−2 2.241−1 6.515−2 1.208−1 8.408−2 1.251−1 7.486−2 9.973−2 4.039−2 5.049−2 4.692−1 1.059+1 9.402−2 3.044−1 5.036−2 3.225−2 2.263−1 3.374−2 3.041−1 3.010−2 2.678−1 2.648−2 1.363−1 2.243−2 2.508+0 2.064+1 1.546−1 6.030−1 6.971−2 3.664−2 4.895−1 1.026−1 6.002−1 1.133−1 4.895−1 7.573−2 2.437−1 2.704−1 1.502+1 1.130−1 1.745−2 4.095−2 2.144−2 4.805−1 2.888−2 1.372+0 3.551−2 7.080−1 3.501−2 1.504+0 2.411+1 2.669−2 1.178−2 8.157−2 2.946−2 7.373−1 1.378−1 1.992+0 1.179−1 1.001+0
1.861−3 1.448−3 5.902−3 4.263−3 4.373−2 1.630−2 1.997−1 8.383−3 5.668−2 6.344+0 1.185+1 3.650−1 5.676−1 4.909−2 6.758−2 2.287−1 8.340−2 1.548−1 9.131−2 1.359−1 7.514−2 1.001−1 4.148−2 5.186−2 4.510−1 1.137+1 8.824−2 2.903−1 4.021−2 3.988−2 2.309−1 3.645−2 3.751−1 3.016−2 2.881−1 2.681−2 1.368−1 2.167−2 2.681+0 2.220+1 1.361−1 5.555−1 8.640−2 3.959−2 5.018−1 1.178−1 7.335−1 1.196−1 5.253−1 7.489−2 2.440−1 2.449−1 1.640+1 8.651−2 1.777−2 4.728−2 2.238−2 4.895−1 2.905−2 1.613+0 3.393−2 7.535−1 3.352−2 1.599+0 2.601+1 2.714−2 1.158−2 9.213−2 2.964−2 7.509−1 1.538−1 2.341+0 1.213−1 1.063+0
1.727−3 1.243−3 5.782−3 3.654−3 4.345−2 1.614−2 2.193−1 8.307−3 6.220−2 6.818+0 1.277+1 3.558−1 5.475−1 4.575−2 6.244−2 2.327−1 1.061−1 1.972−1 9.826−2 1.464−1 7.541−2 1.005−1 4.266−2 5.334−2 4.355−1 1.217+1 8.518−2 2.792−1 3.328−2 4.963−2 2.350−1 3.910−2 4.620−1 3.024−2 3.074−1 2.723−2 1.375−1 2.119−2 2.855+0 2.377+1 1.229−1 5.206−1 1.078−1 4.248−2 5.130−1 1.364−1 8.971−1 1.258−1 5.596−1 7.448−2 2.448−1 2.265−1 1.764+1 6.872−2 1.827−2 5.565−2 2.375−2 4.974−1 2.943−2 1.907+0 3.279−2 7.965−1 3.262−2 1.686+0 2.773+1 2.789−2 1.147−2 1.064−1 3.003−2 7.629−1 1.742−1 2.765+0 1.251−1 1.123+0
1.632−3 1.081−3 5.799−3 3.171−3 4.304−2 1.631−2 2.408−1 8.346−3 6.754−2 7.234+0 1.360+1 3.458−1 5.281−1 4.364−2 5.915−2 2.345−1 1.311−1 2.437−1 1.035−1 1.543−1 7.523−2 1.002−1 4.350−2 5.438−2 4.195−1 1.286+1 8.347−2 2.689−1 2.856−2 6.045−2 2.367−1 4.112−2 5.562−1 3.014−2 3.215−1 2.749−2 1.374−1 2.082−2 3.001+0 2.510+1 1.130−1 4.922−1 1.315−1 4.468−2 5.189−1 1.562−1 1.074+0 1.303−1 5.848−1 7.397−2 2.445−1 2.122−1 1.861+1 5.699−2 1.867−2 6.501−2 2.521−2 5.005−1 2.968−2 2.221+0 3.185−2 8.274−1 3.195−2 1.751+0 2.907+1 2.849−2 1.136−2 1.224−1 3.029−2 7.676−1 1.964−1 3.220+0 1.277−1 1.165+0
1.525−3 9.390−4 5.728−3 2.749−3 4.137−2 1.620−2 2.532−1 8.187−3 6.979−2 7.341+0 1.384+1 3.268−1 4.965−1 4.114−2 5.553−2 2.278−1 1.496−1 2.782−1 1.035−1 1.545−1 7.261−2 9.673−2 4.268−2 5.337−2 3.933−1 1.302+1 8.021−2 2.525−1 2.483−2 6.839−2 2.298−1 4.116−2 6.232−1 2.907−2 3.201−1 2.678−2 1.328−1 1.995−2 3.022+0 2.536+1 1.030−1 4.571−1 1.490−1 4.473−2 5.055−1 1.689−1 1.199+0 1.289−1 5.821−1 7.130−2 2.363−1 1.958−1 1.874+1 4.835−2 1.836−2 7.153−2 2.570−2 4.855−1 2.890−2 2.431+0 3.023−2 8.203−1 3.055−2 1.744+0 2.915+1 2.801−2 1.093−2 1.332−1 2.949−2 7.445−1 2.103−1 3.526+0 1.253−1 1.154+0
1.575−3 9.746−4 6.206−3 2.855−3 4.523−2 1.732−2 2.730−1 8.936−3 7.571−2 7.754+0 1.462+1 3.470−1 5.222−1 4.166−2 5.573−2 2.464−1 1.526−1 2.824−1 1.063−1 1.576−1 2.427−1 3.310−1 4.998−2 6.252−2 4.227−1 1.380+1 8.192−2 2.657−1 2.177−2 7.564−2 2.555−1 4.470−2 6.684−1 3.455−2 3.357−1 3.050−2 1.505−1 2.295−2 3.108+0 2.695+1 1.031−1 4.686−1 1.658−1 4.916−2 5.588−1 1.853−1 1.290+0 1.380−1 6.096−1 8.068−2 2.660−1 2.023−1 2.041+1 3.935−2 1.823−2 7.713−2 3.348−2 5.172−1 3.833−2 2.656+0 3.503−2 8.737−1 3.367−2 1.966+0 3.233+1 2.765−2 1.459−2 1.457−1 3.768−2 7.964−1 2.299−1 3.842+0 1.348−1 1.230+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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81
Table 29 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
2.125−1 5.413−3 1.116−2 1.139−2 4.288−2 2.136−2 6.116−1 4.420−2 3.382+0 8.005−2 7.234−3 6.484−3 2.351−2 1.713−2 6.869−2 4.428−2 8.309−1 2.087−1 4.418+0 1.095+1 2.087+1 1.060+0 1.589+0 1.219−1 1.630−1 3.381−2 4.240−2 1.235+0 2.042+1 1.679−1 1.147+0 8.008−2 7.342−2 2.285−2 4.509+0 3.839+1 4.309−1 2.031+0 5.451−2 1.360−1 6.277−1 2.828+1 1.164−1 9.488−1 5.668−2 2.234+0 4.137+1 1.682−1 1.340+0 4.074−1 2.313+1 1.068−1 1.201+0 3.065+1 3.782−1
6.859−1 8.749−3 1.304−2 1.325−2 4.871−2 2.098−2 5.889−1 4.099−2 3.338+0 7.309−2 1.161−2 7.428−3 2.864−2 1.663−2 7.700−2 4.141−2 7.996−1 2.000−1 4.359+0 1.236+1 2.313+1 1.043+0 1.571+0 1.327−1 1.769−1 3.444−2 4.306−2 1.183+0 2.397+1 1.843−1 1.117+0 8.057−2 8.002−2 2.167−2 5.705+0 4.717+1 4.217−1 1.970+0 5.507−2 1.464−1 6.035−1 4.712+1 1.205−1 9.185−1 5.241−2 4.633+0 7.435+1 1.602−1 1.296+0 3.848−1 4.505+1 9.417−2 3.230+0 6.365+1 3.268−1
5.375−1 7.201−3 1.213−2 1.152−2 4.781−2 1.865−2 5.925−1 3.630−2 3.596+0 6.420−2 9.573−3 6.314−3 2.581−2 1.442−2 7.465−2 3.661−2 8.029−1 2.003−1 4.693+0 1.344+1 2.511+1 1.028+0 1.547+0 1.342−1 1.789−1 3.312−2 4.142−2 1.159+0 2.607+1 1.877−1 1.095+0 7.918−2 7.975−2 2.004−2 6.206+0 5.139+1 4.132−1 1.930+0 5.278−2 1.448−1 5.905−1 5.143+1 1.192−1 8.970−1 4.775−2 4.992+0 8.094+1 1.525−1 1.263+0 3.686−1 4.891+1 8.502−2 3.390+0 6.886+1 2.948−1
4.108−1 6.084−3 1.151−2 1.009−2 4.772−2 1.649−2 5.970−1 3.190−2 3.949+0 5.581−2 8.100−3 5.356−3 2.377−2 1.236−2 7.356−2 3.214−2 8.074−1 2.047−1 5.148+0 1.460+1 2.726+1 1.010+0 1.521+0 1.362−1 1.816−1 3.201−2 4.003−2 1.133+0 2.830+1 1.919−1 1.071+0 7.799−2 7.985−2 1.867−2 6.716+0 5.577+1 4.045−1 1.887+0 5.097−2 1.440−1 5.774−1 5.563+1 1.186−1 8.751−1 4.370−2 5.331+0 8.726+1 1.455−1 1.231+0 3.534−1 5.259+1 7.730−2 3.537+0 7.379+1 2.659−1
3.128−1 5.284−3 1.114−2 8.960−3 4.870−2 1.467−2 6.019−1 2.812−2 4.409+0 4.851−2 7.045−3 4.569−3 2.238−2 1.056−2 7.413−2 2.831−2 8.126−1 2.143−1 5.746+0 1.581+1 2.956+1 9.919−1 1.493+0 1.386−1 1.849−1 3.113−2 3.894−2 1.107+0 3.058+1 1.965−1 1.046+0 7.706−2 8.031−2 1.763−2 7.227+0 6.019+1 3.958−1 1.841+0 4.973−2 1.440−1 5.642−1 5.965+1 1.190−1 8.532−1 4.045−2 5.647+0 9.325+1 1.394−1 1.199+0 3.397−1 5.605+1 7.135−2 3.673+0 7.839+1 2.414−1
2.416−1 4.729−3 1.097−2 8.119−3 5.093−2 1.329−2 6.068−1 2.512−2 4.992+0 4.265−2 6.311−3 3.960−3 2.153−2 9.113−3 7.666−2 2.529−2 8.182−1 2.303−1 6.504+0 1.705+1 3.194+1 9.722−1 1.463+0 1.414−1 1.887−1 3.050−2 3.816−2 1.078+0 3.290+1 2.014−1 1.019+0 7.637−2 8.108−2 1.693−2 7.730+0 6.458+1 3.870−1 1.793+0 4.903−2 1.448−1 5.511−1 6.348+1 1.201−1 8.308−1 3.801−2 5.941+0 9.889+1 1.341−1 1.166+0 3.275−1 5.929+1 6.718−2 3.797+0 8.267+1 2.216−1
1.919−1 4.360−3 1.094−2 7.533−3 5.442−2 1.236−2 6.111−1 2.291−2 5.700+0 3.827−2 5.824−3 3.517−3 2.109−2 8.018−3 8.117−2 2.307−2 8.232−1 2.527−1 7.428+0 1.828+1 3.433+1 9.516−1 1.431+0 1.445−1 1.928−1 3.009−2 3.765−2 1.046+0 3.518+1 2.062−1 9.888−1 7.584−2 8.198−2 1.651−2 8.215+0 6.885+1 3.776−1 1.741+0 4.875−2 1.459−1 5.372−1 6.706+1 1.216−1 8.069−1 3.627−2 6.211+0 1.041+2 1.295−1 1.133+0 3.164−1 6.229+1 6.452−2 3.911+0 8.661+1 2.060−1
1.574−1 4.106−3 1.092−2 7.107−3 5.845−2 1.175−2 6.105−1 2.125−2 6.447+0 3.504−2 5.487−3 3.196−3 2.078−2 7.204−3 8.659−2 2.139−2 8.217−1 2.781−1 8.406+0 1.932+1 3.638+1 9.266−1 1.392+0 1.468−1 1.957−1 2.966−2 3.710−2 1.005+0 3.708+1 2.088−1 9.498−1 7.487−2 8.220−2 1.618−2 8.603+0 7.234+1 3.652−1 1.674+0 4.837−2 1.461−1 5.192−1 6.984+1 1.224−1 7.766−1 3.485−2 6.408+0 1.081+2 1.245−1 1.090+0 3.041−1 6.454+1 6.256−2 3.984+0 8.952+1 1.926−1
1.311−1 3.826−3 1.057−2 6.617−3 6.039−2 1.105−2 5.889−1 1.948−2 6.909+0 3.191−2 5.115−3 2.897−3 1.995−2 6.459−3 8.907−2 1.962−2 7.923−1 2.929−1 9.013+0 1.950+1 3.682+1 8.783−1 1.317+0 1.441−1 1.920−1 2.842−2 3.554−2 9.367−1 3.734+1 2.034−1 8.836−1 7.153−2 7.947−2 1.546−2 8.617+0 7.267+1 3.422−1 1.561+0 4.649−2 1.411−1 4.862−1 6.964+1 1.189−1 7.241−1 3.277−2 6.341+0 1.075+2 1.162−1 1.016+0 2.839−1 6.409+1 5.936−2 3.904+0 8.872+1 1.767−1
1.118−1 4.089−3 1.098−2 7.251−3 5.954−2 1.196−2 6.208−1 2.143−2 7.536+0 3.589−2 5.472−3 3.291−3 2.087−2 7.290−3 8.785−2 2.156−2 8.357−1 3.172−1 9.802+0 2.054+1 3.708+1 8.698−1 1.308+0 1.867−1 2.513−1 3.314−2 4.161−2 9.680−1 3.365+1 3.025−1 9.291−1 8.904−2 1.088−1 1.884−2 8.078+0 6.582+1 3.751−1 1.649+0 6.052−2 1.927−1 5.316−1 7.082+1 1.476−1 7.735−1 3.769−2 6.022+0 1.094+2 1.275−1 1.085+0 3.091−1 6.571+1 1.634−1 3.505+0 8.486+1 2.062−1
82
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 30 Effective collision strengths for transitions in Fe XXIV. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.674−1 3.225−1 1.453−2 4.372−3 8.069−3 1.108−2 1.655−2 2.899−3 1.070−3 2.014−3 2.013−3 3.020−3 1.210−3 1.606−3 1.129−3 4.510−4 8.506−4 7.734−4 1.161−3 6.351−4 8.435−4 8.207−5 1.022−4 2.864−2 1.028−3 1.566−2 4.110−3 5.342−2 7.652−3 3.285−4 3.235−3 1.350−3 9.783−3 2.382−3 1.611−3 9.886−4 1.542−4 1.293−3 6.456−4 3.661−3 1.107−3 8.748−4 5.948−4 8.051−5 7.939−5 2.083−3 4.253−3 3.579−2 2.050−2 1.054−1 6.537−4 1.367−3 7.854−3 4.889−3 1.991−2 1.795−3 3.587−3 3.056−4 6.526−4 3.237−3 2.093−3 7.602−3 1.054−3 1.995−3 1.404−4 1.971−4 1.089+0 2.086+0 7.711−2 1.158−1 6.651−2 1.248−2 2.292−2
1.716−1 3.298−1 1.597−2 5.709−3 1.078−2 1.234−2 1.861−2 3.248−3 1.462−3 2.821−3 2.407−3 3.605−3 1.584−3 2.109−3 1.087−3 5.100−4 9.769−4 8.240−4 1.237−3 6.688−4 8.893−4 8.789−5 1.092−4 4.313−2 4.088−3 1.717−2 7.223−3 5.452−2 1.206−2 9.586−4 3.616−3 2.130−3 1.061−2 3.260−3 2.492−3 1.812−3 2.723−4 1.202−3 6.860−4 3.827−3 1.168−3 9.413−4 6.148−4 8.895−5 7.882−5 1.045−2 7.897−3 4.267−2 2.659−2 1.115−1 1.939−3 2.213−3 9.382−3 6.237−3 2.206−2 3.309−3 5.807−3 5.329−4 7.018−4 3.119−3 2.211−3 7.965−3 1.105−3 2.128−3 1.424−4 2.105−4 1.086+0 2.093+0 1.015−1 1.549−1 6.985−2 1.417−2 2.661−2
1.799−1 3.453−1 1.569−2 5.750−3 1.079−2 1.244−2 1.876−2 3.116−3 1.407−3 2.716−3 2.316−3 3.469−3 1.473−3 1.957−3 1.082−3 5.181−4 9.923−4 8.134−4 1.223−3 6.536−4 8.692−4 8.217−5 1.020−4 4.726−2 3.370−3 1.686−2 6.652−3 5.644−2 1.130−2 7.827−4 3.438−3 1.864−3 1.072−2 2.909−3 2.320−3 1.529−3 2.427−4 1.190−3 6.462−4 3.908−3 1.092−3 9.440−4 5.684−4 8.514−5 7.137−5 8.221−3 7.172−3 4.115−2 2.594−2 1.145−1 1.584−3 1.927−3 8.798−3 5.810−3 2.199−2 2.855−3 5.294−3 4.795−4 6.596−4 3.052−3 2.132−3 8.052−3 1.044−3 2.099−3 1.306−4 1.988−4 1.157+0 2.218+0 9.884−2 1.506−1 6.928−2 1.509−2 2.827−2
1.893−1 3.632−1 1.545−2 5.888−3 1.101−2 1.250−2 1.883−2 3.023−3 1.393−3 2.682−3 2.239−3 3.357−3 1.373−3 1.824−3 1.084−3 5.353−4 1.025−3 8.019−4 1.206−3 6.367−4 8.469−4 7.568−5 9.401−5 4.813−2 2.776−3 1.650−2 5.916−3 5.905−2 1.009−2 6.448−4 3.293−3 1.617−3 1.097−2 2.543−3 2.201−3 1.263−3 2.179−4 1.178−3 5.994−4 4.031−3 9.956−4 9.576−4 5.123−4 8.162−5 6.282−5 6.531−3 6.331−3 3.951−2 2.490−2 1.184−1 1.307−3 1.666−3 8.274−3 5.395−3 2.218−2 2.436−3 4.885−3 4.339−4 6.111−4 2.980−3 2.037−3 8.201−3 9.722−4 2.083−3 1.173−4 1.868−4 1.251+0 2.383+0 9.397−2 1.428−1 6.925−2 1.699−2 3.168−2
2.006−1 3.842−1 1.532−2 6.243−3 1.166−2 1.266−2 1.905−2 2.974−3 1.436−3 2.757−3 2.189−3 3.286−3 1.296−3 1.722−3 1.093−3 5.664−4 1.086−3 7.917−4 1.192−3 6.202−4 8.253−4 6.895−5 8.567−5 4.553−2 2.321−3 1.618−2 5.165−3 6.299−2 8.722−3 5.421−4 3.188−3 1.398−3 1.144−2 2.184−3 2.161−3 1.030−3 1.971−4 1.168−3 5.467−4 4.217−3 8.832−4 9.893−4 4.496−4 7.901−5 5.371−5 5.311−3 5.508−3 3.804−2 2.396−2 1.246−1 1.102−3 1.439−3 7.850−3 5.036−3 2.279−2 2.088−3 4.642−3 3.951−4 5.574−4 2.907−3 1.935−3 8.453−3 8.973−4 2.095−3 1.035−4 1.761−4 1.368+0 2.588+0 8.855−2 1.343−1 6.976−2 2.015−2 3.745−2
2.147−1 4.103−1 1.534−2 6.940−3 1.297−2 1.304−2 1.960−2 2.966−3 1.550−3 2.971−3 2.174−3 3.268−3 1.245−3 1.655−3 1.108−3 6.178−4 1.185−3 7.860−4 1.184−3 6.069−4 8.080−4 6.261−5 7.785−5 4.059−2 2.020−3 1.599−2 4.506−3 6.887−2 7.411−3 4.709−4 3.122−3 1.211−3 1.222−2 1.844−3 2.211−3 8.339−4 1.804−4 1.160−3 4.916−4 4.492−3 7.621−4 1.046−3 3.854−4 7.786−5 4.478−5 4.530−3 4.802−3 3.696−2 2.352−2 1.345−1 9.615−4 1.247−3 7.534−3 4.765−3 2.396−2 1.821−3 4.587−3 3.643−4 5.018−4 2.837−3 1.841−3 8.859−3 8.280−4 2.151−3 9.054−5 1.681−4 1.500+0 2.825+0 8.371−2 1.267−1 7.068−2 2.482−2 4.608−2
2.322−1 4.420−1 1.551−2 8.077−3 1.512−2 1.368−2 2.054−2 2.992−3 1.750−3 3.352−3 2.198−3 3.307−3 1.218−3 1.620−3 1.128−3 6.961−4 1.338−3 7.879−4 1.188−3 5.988−4 7.977−4 5.727−5 7.126−5 3.494−2 1.878−3 1.593−2 3.985−3 7.721−2 6.277−3 4.285−4 3.090−3 1.057−3 1.335−2 1.538−3 2.349−3 6.757−4 1.692−4 1.157−3 4.384−4 4.878−3 6.424−4 1.132−3 3.253−4 7.838−5 3.671−5 4.155−3 4.254−3 3.632−2 2.381−2 1.491−1 8.810−4 1.091−3 7.317−3 4.611−3 2.582−2 1.637−3 4.719−3 3.443−4 4.485−4 2.778−3 1.771−3 9.469−3 7.729−4 2.262−3 7.937−5 1.637−4 1.641+0 3.082+0 7.984−2 1.207−1 7.185−2 3.115−2 5.788−2
2.515−1 4.772−1 1.571−2 9.637−3 1.808−2 1.447−2 2.171−2 3.029−3 2.025−3 3.882−3 2.245−3 3.381−3 1.206−3 1.606−3 1.148−3 7.991−4 1.539−3 7.951−4 1.200−3 5.939−4 7.916−4 5.306−5 6.609−5 2.971−2 1.876−3 1.592−2 3.600−3 8.772−2 5.351−3 4.107−4 3.071−3 9.321−4 1.478−2 1.274−3 2.547−3 5.525−4 1.637−4 1.153−3 3.902−4 5.352−3 5.328−4 1.239−3 2.733−4 7.996−5 2.991−5 4.122−3 3.856−3 3.593−2 2.482−2 1.679−1 8.515−4 9.652−4 7.156−3 4.569−3 2.823−2 1.522−3 4.985−3 3.360−4 4.004−4 2.723−3 1.731−3 1.025−2 7.345−4 2.414−3 7.036−5 1.619−4 1.776+0 3.333+0 7.667−2 1.158−1 7.277−2 3.882−2 7.218−2
2.652−1 5.023−1 1.557−2 1.112−2 2.091−2 1.493−2 2.240−2 2.994−3 2.275−3 4.365−3 2.248−3 3.389−3 1.176−3 1.566−3 1.136−3 8.883−4 1.714−3 7.862−4 1.188−3 5.774−4 7.700−4 4.898−5 6.106−5 2.519−2 1.927−3 1.559−2 3.272−3 9.671−2 4.572−3 4.018−4 2.989−3 8.218−4 1.589−2 1.047−3 2.694−3 4.549−4 1.594−4 1.121−3 3.439−4 5.700−3 4.354−4 1.313−3 2.284−4 7.992−5 2.427−5 4.225−3 3.519−3 3.495−2 2.570−2 1.840−1 8.397−4 8.543−4 6.882−3 4.511−3 3.009−2 1.429−3 5.176−3 3.297−4 3.541−4 2.615−3 1.681−3 1.080−2 6.963−4 2.515−3 6.240−5 1.580−4 1.849+0 3.472+0 7.263−2 1.096−1 7.167−2 4.552−2 8.468−2
2.769−1 5.251−1 1.631−2 1.230−2 2.310−2 1.567−2 2.342−2 3.224−3 2.504−3 4.775−3 2.307−3 3.471−3 1.218−3 1.617−3 1.246−3 9.776−4 1.870−3 7.991−4 1.204−3 6.023−4 8.007−4 5.064−5 6.306−5 1.905−2 1.889−3 1.645−2 3.166−3 1.047−1 4.141−3 3.899−4 3.297−3 8.171−4 1.688−2 9.788−4 2.861−3 4.216−4 1.523−4 1.294−3 3.542−4 5.988−3 4.234−4 1.431−3 2.359−4 8.312−5 2.556−5 4.078−3 3.396−3 3.656−2 2.682−2 1.978−1 8.163−4 8.486−4 7.473−3 4.629−3 3.179−2 1.419−3 5.419−3 3.157−4 3.654−4 2.958−3 1.727−3 1.130−2 7.384−4 2.715−3 6.465−5 1.634−4 1.986+0 3.722+0 7.271−2 1.096−1 7.547−2 5.044−2 9.411−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
83
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.879−2 4.278−2 2.826−2 3.766−2 1.208−2 2.716−3 5.145−3 6.054−3 9.043−3 3.286−3 4.392−3 5.201−3 6.493−3 1.261−1 1.514+0 1.955−2 4.514−3 7.097−2 9.996−3 8.975−2 1.282−2 9.523−2 1.372−2 1.344−3 1.334−2 2.705−3 1.778−2 3.560−3 1.043−2 3.351−3 1.187−2 4.029−3 3.581−1 2.919+0 9.241−3 1.077−2 1.537−1 3.505−2 1.797−1 4.556−2 1.759−1 2.718−3 2.823−3 2.949−2 8.029−3 3.602−2 7.292−3 2.023−2 9.562−3 2.307−2 9.162−2 3.804−3 7.296−3 7.325−3 1.385−1 1.730−2 6.115−1 3.028−2 1.223−3 2.616−3 2.945−3 2.643−2 6.535−3 9.343−2 1.019−2 2.776−2 6.030−3 5.747−3 4.967−3 1.714−2 1.741−2 2.170−1 7.673−2 8.924−1
3.010−2 4.726−2 3.391−2 4.801−2 1.209−2 2.985−3 5.557−3 6.113−3 9.131−3 3.835−3 5.129−3 5.387−3 6.731−3 1.543−1 1.547+0 6.549−2 9.421−3 7.055−2 1.365−2 9.130−2 1.930−2 9.636−2 2.212−2 1.597−3 1.249−2 2.726−3 1.981−2 3.934−3 1.060−2 3.510−3 1.236−2 4.107−3 4.112−1 2.978+0 2.092−2 1.487−2 1.585−1 4.271−2 1.949−1 5.684−2 1.939−1 3.377−3 2.877−3 2.787−2 8.991−3 4.008−2 7.567−3 2.069−2 9.861−3 2.400−2 2.604−1 1.107−2 1.685−2 1.819−2 1.566−1 3.362−2 6.180−1 5.513−2 1.858−3 2.946−3 3.358−3 2.611−2 6.886−3 9.889−2 1.082−2 2.707−2 5.930−3 1.763−2 1.299−2 4.080−2 3.312−2 2.505−1 1.044−1 9.239−1
3.081−2 4.776−2 3.283−2 4.594−2 1.220−2 3.231−3 6.029−3 6.265−3 9.374−3 3.659−3 4.893−3 5.276−3 6.592−3 1.487−1 1.630+0 5.993−2 8.272−3 7.026−2 1.268−2 9.839−2 1.746−2 9.901−2 1.938−2 1.501−3 1.261−2 2.672−3 2.110−2 3.710−3 1.070−2 3.198−3 1.268−2 3.806−3 4.235−1 3.131+0 1.821−2 1.370−2 1.568−1 4.204−2 2.052−1 5.401−2 1.945−1 3.150−3 2.814−3 2.806−2 8.966−3 4.231−2 7.186−3 2.063−2 9.558−3 2.434−2 2.367−1 8.823−3 1.436−2 1.493−2 1.530−1 2.816−2 6.471−1 4.609−2 1.618−3 2.739−3 3.020−3 2.588−2 6.190−3 1.024−1 9.592−3 2.822−2 5.255−3 1.395−2 1.051−2 3.455−2 2.778−2 2.419−1 9.675−2 9.599−1
3.206−2 4.910−2 3.193−2 4.413−2 1.239−2 3.626−3 6.787−3 6.488−3 9.716−3 3.474−3 4.645−3 5.188−3 6.483−3 1.410−1 1.754+0 5.110−2 7.801−3 7.036−2 1.200−2 1.094−1 1.576−2 1.032−1 1.691−2 1.479−3 1.277−2 2.635−3 2.300−2 3.470−3 1.088−2 2.865−3 1.310−2 3.491−3 4.443−1 3.382+0 1.706−2 1.295−2 1.559−1 4.241−2 2.232−1 5.201−2 1.980−1 3.095−3 2.774−3 2.836−2 9.052−3 4.565−2 6.797−3 2.068−2 9.272−3 2.486−2 1.997−1 7.136−3 1.254−2 1.214−2 1.491−1 2.314−2 6.919−1 3.770−2 1.423−3 2.572−3 2.679−3 2.568−2 5.437−3 1.075−1 8.260−3 2.997−2 4.556−3 1.120−2 8.382−3 2.953−2 2.289−2 2.338−1 9.085−2 1.018+0
3.394−2 5.148−2 3.130−2 4.281−2 1.262−2 4.221−3 7.926−3 6.787−3 1.017−2 3.299−3 4.412−3 5.145−3 6.429−3 1.333−1 1.914+0 4.191−2 8.006−3 7.086−2 1.170−2 1.256−1 1.438−2 1.091−1 1.492−2 1.533−3 1.296−2 2.624−3 2.569−2 3.232−3 1.115−2 2.539−3 1.362−2 3.189−3 4.751−1 3.718+0 1.746−2 1.265−2 1.562−1 4.427−2 2.515−1 5.114−2 2.051−1 3.212−3 2.765−3 2.875−2 9.308−3 5.043−2 6.443−3 2.087−2 9.035−3 2.553−2 1.608−1 5.933−3 1.145−2 9.978−3 1.462−1 1.895−2 7.569−1 3.059−2 1.267−3 2.455−3 2.356−3 2.553−2 4.687−3 1.146−1 6.932−3 3.240−2 3.894−3 9.248−3 6.687−3 2.609−2 1.882−2 2.278−1 8.776−2 1.107+0
3.639−2 5.483−2 3.095−2 4.200−2 1.289−2 5.063−3 9.540−3 7.159−3 1.073−2 3.153−3 4.218−3 5.162−3 6.451−3 1.266−1 2.099+0 3.413−2 8.887−3 7.169−2 1.175−2 1.481−1 1.336−2 1.164−1 1.347−2 1.672−3 1.318−2 2.646−3 2.933−2 3.017−3 1.150−2 2.249−3 1.418−2 2.926−3 5.127−1 4.102+0 1.938−2 1.275−2 1.576−1 4.786−2 2.920−1 5.140−2 2.156−1 3.515−3 2.792−3 2.923−2 9.791−3 5.700−2 6.162−3 2.124−2 8.868−3 2.631−2 1.270−1 5.126−3 1.109−2 8.420−3 1.445−1 1.570−2 8.459−1 2.492−2 1.146−3 2.404−3 2.075−3 2.546−2 4.001−3 1.242−1 5.716−3 3.554−2 3.321−3 7.940−3 5.405−3 2.424−2 1.566−2 2.241−1 8.798−2 1.231+0
3.923−2 5.886−2 3.085−2 4.161−2 1.317−2 6.190−3 1.170−2 7.585−3 1.137−2 3.049−3 4.078−3 5.242−3 6.551−3 1.212−1 2.295+0 2.830−2 1.043−2 7.272−2 1.208−2 1.775−1 1.264−2 1.247−1 1.251−2 1.900−3 1.340−2 2.701−3 3.406−2 2.839−3 1.192−2 2.016−3 1.473−2 2.716−3 5.536−1 4.502+0 2.278−2 1.316−2 1.598−1 5.328−2 3.461−1 5.255−2 2.284−1 4.013−3 2.854−3 2.974−2 1.055−2 6.559−2 5.972−3 2.176−2 8.770−3 2.712−2 1.006−1 4.622−3 1.140−2 7.390−3 1.439−1 1.331−2 9.613−1 2.065−2 1.059−3 2.427−3 1.853−3 2.547−2 3.423−3 1.366−1 4.688−3 3.923−2 2.867−3 7.122−3 4.475−3 2.386−2 1.334−2 2.223−1 9.164−2 1.395+0
4.198−2 6.284−2 3.079−2 4.137−2 1.338−2 7.539−3 1.429−2 7.993−3 1.198−2 2.975−3 3.979−3 5.348−3 6.683−3 1.168−1 2.480+0 2.426−2 1.249−2 7.348−2 1.254−2 2.122−1 1.213−2 1.325−1 1.190−2 2.200−3 1.354−2 2.770−3 3.957−2 2.694−3 1.230−2 1.838−3 1.516−2 2.551−3 5.921−1 4.870+0 2.733−2 1.369−2 1.617−1 6.004−2 4.103−1 5.401−2 2.409−1 4.664−3 2.930−3 3.013−2 1.150−2 7.564−2 5.845−3 2.228−2 8.691−3 2.774−2 8.112−2 4.320−3 1.221−2 6.761−3 1.434−1 1.161−2 1.095+0 1.753−2 9.990−4 2.511−3 1.688−3 2.543−2 2.963−3 1.507−1 3.873−3 4.297−2 2.527−3 6.630−3 3.815−3 2.460−2 1.169−2 2.210−1 9.795−2 1.585+0
4.323−2 6.461−2 3.004−2 4.026−2 1.319−2 8.685−3 1.649−2 8.129−3 1.219−2 2.859−3 3.824−3 5.320−3 6.648−3 1.109−1 2.578+0 2.125−2 1.433−2 7.221−2 1.267−2 2.409−1 1.150−2 1.355−1 1.128−2 2.454−3 1.330−2 2.769−3 4.394−2 2.526−3 1.231−2 1.675−3 1.507−2 2.377−3 6.105−1 5.059+0 3.141−2 1.387−2 1.592−1 6.542−2 4.636−1 5.406−2 2.453−1 5.221−3 2.931−3 2.965−2 1.220−2 8.356−2 5.631−3 2.215−2 8.420−3 2.746−2 6.651−2 4.058−3 1.293−2 6.283−3 1.395−1 1.026−2 1.198+0 1.509−2 9.386−4 2.565−3 1.543−3 2.475−2 2.573−3 1.606−1 3.218−3 4.508−2 2.244−3 6.208−3 3.300−3 2.534−2 1.036−2 2.147−1 1.029−1 1.733+0
4.620−2 6.871−2 3.096−2 4.127−2 1.456−2 9.436−3 1.791−2 8.565−3 1.282−2 2.866−3 3.835−3 5.731−3 7.154−3 1.128−1 2.751+0 1.685−2 1.598−2 7.760−2 1.378−2 2.643−1 1.180−2 1.441−1 1.132−2 2.710−3 1.532−2 3.090−3 4.644−2 2.587−3 1.267−2 1.701−3 1.571−2 2.496−3 6.496−1 5.400+0 3.470−2 1.503−2 1.708−1 7.054−2 5.054−1 5.663−2 2.591−1 5.719−3 3.264−3 3.391−2 1.278−2 8.802−2 5.774−3 2.280−2 8.798−3 2.857−2 5.015−2 3.868−3 1.326−2 6.002−3 1.444−1 9.724−3 1.291+0 1.421−2 9.561−4 2.744−3 1.609−3 2.674−2 2.652−3 1.704−1 3.301−3 4.830−2 2.453−3 5.877−3 2.985−3 2.552−2 9.894−3 2.221−1 1.084−1 1.863+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
84
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.838−3 2.042−3 6.358−3 6.539−3 4.294−2 1.771−2 1.383−1 9.873−3 4.124−2 3.856+0 7.321+0 3.453−1 5.182−1 3.137−2 4.197−2 2.045−1 2.997−2 5.453−2 6.188−2 9.168−2 6.706−2 8.919−2 3.406−2 4.253−2 4.423−1 6.690+0 5.674−2 2.703−1 2.609−2 1.532−2 2.154−1 2.724−2 1.596−1 2.915−2 2.001−1 2.343−2 1.208−1 2.307−2 1.511+0 1.293+1 1.108−1 4.835−1 3.250−2 2.957−2 4.609−1 7.114−2 3.281−1 8.959−2 3.690−1 7.156−2 2.185−1 2.223−1 8.251+0 5.200−2 1.335−2 2.406−2 1.862−2 4.448−1 2.858−2 8.576−1 4.115−2 5.487−1 4.149−2 6.223−1 1.065+1 2.022−2 1.193−2 5.266−2 2.900−2 6.827−1 1.067−1 1.254+0 1.075−1 7.811−1
2.762−3 2.386−3 7.203−3 6.949−3 4.266−2 1.876−2 1.465−1 9.718−3 4.027−2 3.989+0 7.674+0 3.655−1 5.567−1 7.836−2 1.123−1 1.937−1 3.095−2 5.601−2 6.072−2 9.045−2 6.744−2 8.985−2 3.541−2 4.425−2 4.851−1 7.386+0 1.108−1 3.301−1 9.364−2 1.970−2 1.955−1 2.507−2 1.593−1 2.738−2 1.970−1 2.430−2 1.235−1 2.417−2 1.674+0 1.448+1 2.244−1 6.867−1 4.389−2 2.763−2 4.170−1 6.889−2 3.270−1 8.978−2 3.646−1 7.381−2 2.236−1 3.566−1 9.107+0 2.373−1 1.791−2 2.973−2 1.913−2 4.171−1 2.779−2 8.442−1 3.909−2 5.403−1 3.969−2 1.057+0 1.730+1 2.748−2 1.218−2 6.302−2 2.872−2 6.418−1 1.037−1 1.234+0 1.045−1 7.691−1
2.415−3 2.118−3 6.620−3 6.234−3 4.198−2 1.768−2 1.510−1 9.085−3 4.162−2 4.360+0 8.289+0 3.559−1 5.406−1 6.708−2 9.515−2 1.970−1 3.690−2 6.718−2 6.490−2 9.662−2 6.796−2 9.053−2 3.562−2 4.452−2 4.646−1 8.002+0 9.926−2 3.101−1 7.450−2 2.091−2 1.991−1 2.639−2 1.846−1 2.747−2 2.094−1 2.411−2 1.240−1 2.288−2 1.837+0 1.570+1 1.926−1 6.262−1 4.599−2 2.898−2 4.262−1 7.433−2 3.748−1 9.321−2 3.863−1 7.225−2 2.236−1 3.142−1 1.053+1 1.845−1 1.652−2 3.044−2 1.884−2 4.242−1 2.712−2 9.341−1 3.687−2 5.687−1 3.692−2 1.163+0 1.910+1 2.532−2 1.159−2 6.349−2 2.788−2 6.521−1 1.077−1 1.363+0 1.046−1 8.075−1
2.132−3 1.848−3 6.103−3 5.470−3 4.132−2 1.659−2 1.577−1 8.492−3 4.380−2 4.780+0 9.005+0 3.465−1 5.250−1 5.731−2 8.036−2 2.011−1 4.567−2 8.356−2 7.013−2 1.044−1 6.839−2 9.111−2 3.611−2 4.513−2 4.444−1 8.675+0 8.950−2 2.919−1 5.810−2 2.375−2 2.033−1 2.819−2 2.202−1 2.754−2 2.247−1 2.407−2 1.245−1 2.169−2 2.018+0 1.707+1 1.643−1 5.711−1 5.193−2 3.091−2 4.368−1 8.198−2 4.421−1 9.766−2 4.130−1 7.081−2 2.235−1 2.765−1 1.199+1 1.394−1 1.590−2 3.261−2 1.890−2 4.323−1 2.665−2 1.059+0 3.474−2 6.033−1 3.441−2 1.268+0 2.079+1 2.434−2 1.116−2 6.661−2 2.732−2 6.639−1 1.144−1 1.542+0 1.057−1 8.547−1
1.902−3 1.589−3 5.683−3 4.713−3 4.073−2 1.566−2 1.673−1 8.019−3 4.696−2 5.231+0 9.800+0 3.381−1 5.112−1 4.995−2 6.926−2 2.054−1 5.784−2 1.062−1 7.625−2 1.134−1 6.874−2 9.156−2 3.688−2 4.609−2 4.266−1 9.396+0 8.254−2 2.769−1 4.549−2 2.837−2 2.076−1 3.040−2 2.683−1 2.760−2 2.421−1 2.420−2 1.249−1 2.069−2 2.205+0 1.852+1 1.418−1 5.263−1 6.192−2 3.332−2 4.483−1 9.228−2 5.328−1 1.030−1 4.437−1 6.962−2 2.236−1 2.464−1 1.338+1 1.048−1 1.583−2 3.641−2 1.934−2 4.407−1 2.647−2 1.224+0 3.286−2 6.427−1 3.238−2 1.367+0 2.239+1 2.421−2 1.087−2 7.266−2 2.710−2 6.765−1 1.244−1 1.780+0 1.078−1 9.087−1
1.724−3 1.358−3 5.398−3 4.023−3 4.029−2 1.503−2 1.806−1 7.724−3 5.113−2 5.698+0 1.065+1 3.307−1 4.993−1 4.497−2 6.172−2 2.096−1 7.391−2 1.361−1 8.289−2 1.232−1 6.904−2 9.193−2 3.786−2 4.733−2 4.115−1 1.015+1 7.834−2 2.650−1 3.646−2 3.490−2 2.118−1 3.288−2 3.304−1 2.767−2 2.606−1 2.449−2 1.255−1 1.994−2 2.391+0 2.002+1 1.251−1 4.921−1 7.623−2 3.605−2 4.597−1 1.056−1 6.499−1 1.088−1 4.762−1 6.880−2 2.239−1 2.239−1 1.466+1 8.021−2 1.613−2 4.200−2 2.019−2 4.490−1 2.658−2 1.436+0 3.135−2 6.841−1 3.092−2 1.457+0 2.391+1 2.465−2 1.067−2 8.194−2 2.721−2 6.888−1 1.383−1 2.086+0 1.107−1 9.659−1
1.596−3 1.166−3 5.275−3 3.443−3 4.001−2 1.481−2 1.979−1 7.625−3 5.614−2 6.169+0 1.153+1 3.241−1 4.890−1 4.189−2 5.703−2 2.135−1 9.414−2 1.737−1 8.952−2 1.328−1 6.936−2 9.232−2 3.896−2 4.871−2 3.986−1 1.092+1 7.634−2 2.558−1 3.027−2 4.339−2 2.156−1 3.542−2 4.073−1 2.777−2 2.786−1 2.488−2 1.261−1 1.947−2 2.572+0 2.152+1 1.133−1 4.666−1 9.493−2 3.885−2 4.703−1 1.222−1 7.950−1 1.145−1 5.077−1 6.839−2 2.246−1 2.076−1 1.582+1 6.361−2 1.664−2 4.945−2 2.142−2 4.564−1 2.689−2 1.696+0 3.024−2 7.239−1 3.002−2 1.539+0 2.534+1 2.540−2 1.057−2 9.456−2 2.755−2 7.002−1 1.563−1 2.462+0 1.141−1 1.021+0
1.507−3 1.013−3 5.291−3 2.983−3 3.972−2 1.494−2 2.179−1 7.659−3 6.125−2 6.597+0 1.235+1 3.171−1 4.781−1 4.004−2 5.417−2 2.158−1 1.172−1 2.163−1 9.504−2 1.408−1 6.942−2 9.237−2 3.987−2 4.984−2 3.857−1 1.162+1 7.553−2 2.476−1 2.609−2 5.318−2 2.178−1 3.759−2 4.935−1 2.778−2 2.929−1 2.520−2 1.264−1 1.916−2 2.729+0 2.285+1 1.047−1 4.459−1 1.165−1 4.121−2 4.773−1 1.405−1 9.577−1 1.189−1 5.326−1 6.805−2 2.248−1 1.950−1 1.678+1 5.271−2 1.713−2 5.812−2 2.282−2 4.606−1 2.716−2 1.986+0 2.939−2 7.548−1 2.943−2 1.605+0 2.655+1 2.611−2 1.049−2 1.093−1 2.783−2 7.065−1 1.768−1 2.881+0 1.169−1 1.064+0
1.417−3 8.833−4 5.270−3 2.592−3 3.850−2 1.494−2 2.318−1 7.575−3 6.410−2 6.783+0 1.273+1 3.029−1 4.568−1 3.808−2 5.131−2 2.116−1 1.361−1 2.514−1 9.654−2 1.428−1 6.764−2 9.000−2 3.952−2 4.941−2 3.649−1 1.190+1 7.358−2 2.350−1 2.289−2 6.120−2 2.135−1 3.826−2 5.622−1 2.706−2 2.951−1 2.479−2 1.233−1 1.851−2 2.786+0 2.336+1 9.642−2 4.196−1 1.343−1 4.186−2 4.694−1 1.540−1 1.087+0 1.189−1 5.357−1 6.615−2 2.192−1 1.813−1 1.709+1 4.492−2 1.710−2 6.496−2 2.354−2 4.510−1 2.665−2 2.206+0 2.809−2 7.561−1 2.836−2 1.615+0 2.682+1 2.602−2 1.018−2 1.208−1 2.731−2 6.916−1 1.917−1 3.201+0 1.157−1 1.066+0
1.444−3 9.096−4 5.604−3 2.672−3 4.151−2 1.575−2 2.456−1 8.177−3 6.861−2 7.088+0 1.329+1 3.197−1 4.812−1 3.781−2 5.056−2 2.259−1 1.380−1 2.539−1 9.798−2 1.452−1 1.807−1 2.460−1 4.476−2 5.598−2 3.898−1 1.246+1 7.487−2 2.449−1 2.003−2 6.659−2 2.347−1 4.074−2 5.957−1 3.313−2 3.074−1 2.746−2 1.366−1 2.072−2 2.848+0 2.451+1 9.492−2 4.318−1 1.469−1 4.510−2 5.134−1 1.668−1 1.154+0 1.259−1 5.588−1 7.318−2 2.416−1 1.863−1 1.862+1 3.617−2 1.675−2 6.919−2 3.266−2 4.746−1 2.885−2 2.374+0 3.241−2 7.992−1 3.091−2 1.821+0 2.884+1 2.544−2 1.380−2 1.317−1 2.955−2 7.280−1 2.069−1 3.436+0 1.235−1 1.125+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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85
Table 30 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.975−1 5.004−3 1.027−2 1.056−2 3.929−2 1.988−2 5.615−1 4.116−2 3.070+0 7.461−2 6.689−3 6.042−3 2.166−2 1.599−2 6.307−2 4.124−2 7.631−1 1.916−1 4.012+0 9.966+0 1.892+1 9.755−1 1.462+0 1.112−1 1.487−1 3.116−2 3.908−2 1.137+0 1.843+1 1.532−1 1.055+0 7.366−2 6.724−2 2.116−2 4.087+0 3.478+1 3.967−1 1.870+0 5.020−2 1.246−1 5.780−1 2.508+1 1.067−1 8.737−1 5.263−2 1.979+0 3.579+1 1.553−1 1.235+0 3.762−1 2.030+1 9.927−2 1.057+0 2.673+1 3.516−1
6.540−1 8.223−3 1.188−2 1.183−2 4.501−2 1.956−2 5.416−1 3.828−2 3.037+0 6.829−2 1.015−2 6.879−3 2.463−2 1.559−2 7.095−2 3.871−2 7.360−1 1.841−1 3.968+0 1.130+1 2.102+1 9.606−1 1.446+0 1.209−1 1.611−1 3.165−2 3.959−2 1.088+0 2.164+1 1.680−1 1.027+0 7.395−2 7.314−2 2.007−2 5.207+0 4.288+1 3.877−1 1.812+0 5.063−2 1.340−1 5.557−1 4.201+1 1.104−1 8.453−1 4.869−2 4.193+0 6.640+1 1.480−1 1.193+0 3.551−1 4.000+1 8.754−2 2.927+0 5.649+1 3.045−1
5.177−1 6.751−3 1.108−2 1.042−2 4.395−2 1.743−2 5.447−1 3.400−2 3.259+0 6.020−2 8.490−3 5.879−3 2.268−2 1.356−2 6.860−2 3.431−2 7.385−1 1.839−1 4.254+0 1.229+1 2.279+1 9.460−1 1.424+0 1.223−1 1.630−1 3.046−2 3.809−2 1.067+0 2.351+1 1.711−1 1.007+0 7.268−2 7.291−2 1.855−2 5.663+0 4.668+1 3.799−1 1.775+0 4.853−2 1.325−1 5.437−1 4.595+1 1.091−1 8.257−1 4.439−2 4.532+0 7.250+1 1.409−1 1.163+0 3.403−1 4.358+1 7.910−2 3.082+0 6.138+1 2.750−1
3.975−1 5.688−3 1.053−2 9.207−3 4.368−2 1.542−2 5.485−1 2.991−2 3.565+0 5.244−2 7.267−3 5.005−3 2.120−2 1.164−2 6.738−2 3.015−2 7.422−1 1.870−1 4.649+0 1.335+1 2.473+1 9.300−1 1.400+0 1.241−1 1.656−1 2.942−2 3.681−2 1.044+0 2.551+1 1.749−1 9.857−1 7.160−2 7.301−2 1.727−2 6.130+0 5.065+1 3.720−1 1.735+0 4.683−2 1.317−1 5.315−1 4.979+1 1.085−1 8.056−1 4.061−2 4.851+0 7.835+1 1.344−1 1.133+0 3.262−1 4.699+1 7.185−2 3.223+0 6.599+1 2.481−1
3.027−1 4.925−3 1.020−2 8.216−3 4.438−2 1.370−2 5.528−1 2.634−2 3.967+0 4.558−2 6.372−3 4.275−3 2.015−2 9.953−3 6.763−2 2.653−2 7.467−1 1.949−1 5.171+0 1.446+1 2.682+1 9.131−1 1.374+0 1.264−1 1.687−1 2.861−2 3.579−2 1.019+0 2.758+1 1.792−1 9.629−1 7.075−2 7.345−2 1.628−2 6.600+0 5.468+1 3.640−1 1.694+0 4.565−2 1.317−1 5.194−1 5.349+1 1.088−1 7.855−1 3.752−2 5.148+0 8.391+1 1.287−1 1.104+0 3.134−1 5.020+1 6.616−2 3.352+0 7.029+1 2.250−1
2.330−1 4.392−3 1.005−2 7.461−3 4.622−2 1.237−2 5.573−1 2.346−2 4.480+0 3.997−2 5.739−3 3.700−3 1.950−2 8.568−3 6.966−2 2.363−2 7.516−1 2.084−1 5.838+0 1.559+1 2.899+1 8.957−1 1.348+0 1.291−1 1.722−1 2.802−2 3.505−2 9.931−1 2.970+1 1.838−1 9.387−1 7.012−2 7.418−2 1.560−2 7.064+0 5.872+1 3.559−1 1.651+0 4.496−2 1.324−1 5.072−1 5.702+1 1.098−1 7.651−1 3.518−2 5.424+0 8.914+1 1.237−1 1.074+0 3.020−1 5.322+1 6.210−2 3.471+0 7.429+1 2.061−1
1.839−1 4.037−3 1.003−2 6.925−3 4.925−2 1.145−2 5.614−1 2.131−2 5.108+0 3.573−2 5.312−3 3.277−3 1.918−2 7.511−3 7.352−2 2.148−2 7.564−1 2.279−1 6.658+0 1.673+1 3.119+1 8.783−1 1.322+0 1.321−1 1.761−1 2.763−2 3.458−2 9.646−1 3.180+1 1.884−1 9.123−1 6.966−2 7.507−2 1.520−2 7.514+0 6.267+1 3.473−1 1.604+0 4.468−2 1.335−1 4.944−1 6.036+1 1.112−1 7.437−1 3.350−2 5.679+0 9.404+1 1.193−1 1.043+0 2.916−1 5.603+1 5.948−2 3.579+0 7.799+1 1.911−1
1.499−1 3.799−3 1.005−2 6.544−3 5.300−2 1.086−2 5.623−1 1.971−2 5.799+0 3.264−2 5.025−3 2.974−3 1.899−2 6.732−3 7.856−2 1.988−2 7.571−1 2.513−1 7.562+0 1.774+1 3.319+1 8.599−1 1.296+0 1.347−1 1.797−1 2.730−2 3.417−2 9.307−1 3.365+1 1.915−1 8.800−1 6.895−2 7.554−2 1.494−2 7.899+0 6.610+1 3.366−1 1.547+0 4.444−2 1.340−1 4.787−1 6.314+1 1.123−1 7.177−1 3.221−2 5.881+0 9.806+1 1.148−1 1.006+0 2.806−1 5.831+1 5.768−2 3.658+0 8.096+1 1.787−1
1.247−1 3.564−3 9.842−3 6.139−3 5.538−2 1.027−2 5.473−1 1.815−2 6.298+0 2.984−2 4.730−3 2.709−3 1.844−2 6.058−3 8.169−2 1.832−2 7.366−1 2.677−1 8.216+0 1.810+1 3.396+1 8.273−1 1.253+0 1.337−1 1.785−1 2.640−2 3.304−2 8.775−1 3.427+1 1.884−1 8.274−1 6.644−2 7.373−2 1.444−2 7.995+0 6.711+1 3.177−1 1.454+0 4.309−2 1.307−1 4.517−1 6.364+1 1.101−1 6.745−1 3.049−2 5.879+0 9.858+1 1.079−1 9.447−1 2.637−1 5.853+1 5.511−2 3.620+0 8.110+1 1.648−1
1.039−1 3.757−3 1.011−2 6.701−3 5.438−2 1.109−2 5.706−1 1.998−2 6.759+0 3.335−2 5.029−3 3.056−3 1.921−2 6.803−3 8.028−2 2.011−2 7.682−1 2.858−1 8.793+0 1.873+1 3.337+1 8.090−1 1.216+0 1.770−1 2.386−1 3.115−2 3.912−2 9.010−1 3.101+1 2.723−1 8.643−1 8.121−2 9.863−2 1.570−2 7.374+0 6.044+1 3.485−1 1.533+0 5.593−2 1.774−1 4.949−1 6.276+1 1.357−1 7.184−1 3.467−2 5.677+0 9.852+1 1.180−1 1.008+0 2.863−1 5.904+1 1.205−1 3.208+0 7.662+1 1.933−1
86
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 31 Effective collision strengths for transitions in Co XXV. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.540−1 2.960−1 1.338−2 4.051−3 7.426−3 1.019−2 1.521−2 2.673−3 9.738−4 1.819−3 1.863−3 2.795−3 1.111−3 1.474−3 1.039−3 4.162−4 7.812−4 7.141−4 1.072−3 5.883−4 7.811−4 7.648−5 9.518−5 2.652−2 9.508−4 1.439−2 3.796−3 4.900−2 7.106−3 3.019−4 2.982−3 1.257−3 8.946−3 2.213−3 1.546−3 9.267−4 1.432−4 1.188−3 5.988−4 3.362−3 1.030−3 8.047−4 5.540−4 7.456−5 7.411−5 1.929−3 3.937−3 3.294−2 1.896−2 9.700−2 6.001−4 1.273−3 7.254−3 4.527−3 1.826−2 1.696−3 3.425−3 2.831−4 6.040−4 2.978−3 1.934−3 6.994−3 9.751−4 1.836−3 1.299−4 1.818−4 1.034+0 1.942+0 7.112−2 1.068−1 6.137−2 1.123−2 2.044−2
1.575−1 3.023−1 1.585−2 5.377−3 9.392−3 1.133−2 1.715−2 3.009−3 1.366−3 2.584−3 2.241−3 3.341−3 1.483−3 1.976−3 1.002−3 4.814−4 9.027−4 7.596−4 1.144−3 6.194−4 8.230−4 8.176−5 1.016−4 3.903−2 4.250−3 1.586−2 6.454−3 5.011−2 1.121−2 8.507−4 3.381−3 1.972−3 9.785−3 3.042−3 2.322−3 1.713−3 2.444−4 1.153−3 6.432−4 3.517−3 1.089−3 8.636−4 5.724−4 8.171−5 7.359−5 9.890−3 7.623−3 3.866−2 2.446−2 1.027−1 1.788−3 2.095−3 8.615−3 5.838−3 2.037−2 3.108−3 5.408−3 4.946−4 6.877−4 2.919−3 2.049−3 7.347−3 1.029−3 1.963−3 1.330−4 1.951−4 9.973−1 1.915+0 9.409−2 1.437−1 6.782−2 1.343−2 2.448−2
1.652−1 3.162−1 1.524−2 5.372−3 9.628−3 1.145−2 1.732−2 2.889−3 1.312−3 2.486−3 2.155−3 3.214−3 1.378−3 1.833−3 9.990−4 4.837−4 9.128−4 7.504−4 1.130−3 6.057−4 8.050−4 7.665−5 9.526−5 4.321−2 3.440−3 1.566−2 6.100−3 5.183−2 1.061−2 7.066−4 3.212−3 1.738−3 9.863−3 2.724−3 2.158−3 1.451−3 2.197−4 1.127−3 6.056−4 3.585−3 1.021−3 8.651−4 5.313−4 7.827−5 6.695−5 7.810−3 6.932−3 3.777−2 2.407−2 1.054−1 1.468−3 1.826−3 8.109−3 5.440−3 2.028−2 2.689−3 4.929−3 4.446−4 6.371−4 2.849−3 1.979−3 7.416−3 9.738−4 1.937−3 1.224−4 1.844−4 1.059+0 2.024+0 9.230−2 1.404−1 6.673−2 1.407−2 2.573−2
1.738−1 3.322−1 1.478−2 5.457−3 9.928−3 1.150−2 1.737−2 2.801−3 1.292−3 2.449−3 2.078−3 3.106−3 1.282−3 1.705−3 1.001−3 4.955−4 9.392−4 7.399−4 1.115−3 5.901−4 7.845−4 7.079−5 8.796−5 4.452−2 2.791−3 1.536−2 5.510−3 5.407−2 9.535−3 5.882−4 3.070−3 1.514−3 1.006−2 2.390−3 2.037−3 1.202−3 1.987−4 1.107−3 5.621−4 3.690−3 9.344−4 8.757−4 4.810−4 7.501−5 5.922−5 6.213−3 6.122−3 3.653−2 2.318−2 1.087−1 1.214−3 1.578−3 7.645−3 5.047−3 2.040−2 2.297−3 4.537−3 4.023−4 5.852−4 2.778−3 1.894−3 7.540−3 9.089−4 1.920−3 1.103−4 1.734−4 1.142+0 2.168+0 8.802−2 1.335−1 6.599−2 1.558−2 2.851−2
1.838−1 3.509−1 1.449−2 5.736−3 1.053−2 1.164−2 1.754−2 2.753−3 1.322−3 2.508−3 2.026−3 3.034−3 1.207−3 1.605−3 1.009−3 5.205−4 9.898−4 7.301−4 1.100−3 5.746−4 7.643−4 6.460−5 8.029−5 4.257−2 2.294−3 1.506−2 4.848−3 5.741−2 8.272−3 4.972−4 2.966−3 1.312−3 1.046−2 2.060−3 1.986−3 9.821−4 1.805−4 1.091−3 5.135−4 3.850−3 8.325−4 9.018−4 4.240−4 7.249−5 5.087−5 5.037−3 5.314−3 3.528−2 2.229−2 1.139−1 1.023−3 1.363−3 7.265−3 4.702−3 2.090−2 1.966−3 4.290−3 3.661−4 5.313−4 2.706−3 1.800−3 7.752−3 8.398−4 1.926−3 9.763−5 1.634−4 1.248+0 2.352+0 8.291−2 1.255−1 6.579−2 1.823−2 3.342−2
1.965−1 3.740−1 1.438−2 6.320−3 1.168−2 1.196−2 1.799−2 2.742−3 1.416−3 2.689−3 2.006−3 3.010−3 1.156−3 1.537−3 1.022−3 5.636−4 1.075−3 7.240−4 1.092−3 5.618−4 7.476−4 5.868−5 7.296−5 3.826−2 1.956−3 1.485−2 4.238−3 6.246−2 7.039−3 4.324−4 2.899−3 1.138−3 1.112−2 1.746−3 2.018−3 7.958−4 1.655−4 1.080−3 4.623−4 4.088−3 7.214−4 9.501−4 3.648−4 7.124−5 4.257−5 4.260−3 4.609−3 3.428−2 2.178−2 1.224−1 8.907−4 1.180−3 6.977−3 4.435−3 2.189−2 1.710−3 4.216−3 3.370−4 4.768−4 2.638−3 1.711−3 8.098−3 7.743−4 1.970−3 8.546−5 1.556−4 1.370+0 2.566+0 7.819−2 1.182−1 6.613−2 2.226−2 4.090−2
2.123−1 4.025−1 1.445−2 7.302−3 1.355−2 1.251−2 1.880−2 2.764−3 1.587−3 3.018−3 2.021−3 3.039−3 1.128−3 1.501−3 1.041−3 6.311−4 1.207−3 7.246−4 1.094−3 5.536−4 7.372−4 5.360−5 6.669−5 3.306−2 1.776−3 1.476−2 3.741−3 6.971−2 5.957−3 3.924−4 2.864−3 9.930−4 1.211−2 1.459−3 2.132−3 6.443−4 1.551−4 1.074−3 4.124−4 4.426−3 6.101−4 1.025−3 3.085−4 7.154−5 3.497−5 3.858−3 4.056−3 3.365−2 2.192−2 1.351−1 8.119−4 1.030−3 6.776−3 4.272−3 2.349−2 1.530−3 4.315−3 3.173−4 4.251−4 2.581−3 1.642−3 8.627−3 7.209−4 2.065−3 7.484−5 1.511−4 1.501+0 2.803+0 7.437−2 1.123−1 6.686−2 2.785−2 5.129−2
2.304−1 4.353−1 1.461−2 8.707−3 1.623−2 1.325−2 1.989−2 2.803−3 1.835−3 3.498−3 2.065−3 3.109−3 1.117−3 1.487−3 1.061−3 7.244−4 1.389−3 7.319−4 1.105−3 5.497−4 7.325−4 4.962−5 6.179−5 2.815−2 1.740−3 1.476−2 3.370−3 7.921−2 5.071−3 3.751−4 2.848−3 8.754−4 1.341−2 1.211−3 2.312−3 5.260−4 1.498−4 1.071−3 3.671−4 4.861−3 5.074−4 1.124−3 2.593−4 7.307−5 2.852−5 3.787−3 3.655−3 3.332−2 2.277−2 1.522−1 7.816−4 9.105−4 6.638−3 4.223−3 2.570−2 1.418−3 4.555−3 3.089−4 3.789−4 2.532−3 1.602−3 9.341−3 6.838−4 2.205−3 6.626−5 1.494−4 1.630+0 3.041+0 7.138−2 1.077−1 6.764−2 3.486−2 6.434−2
2.455−1 4.627−1 1.459−2 1.020−2 1.907−2 1.382−2 2.074−2 2.798−3 2.092−3 3.995−3 2.088−3 3.148−3 1.098−3 1.463−3 1.061−3 8.173−4 1.571−3 7.308−4 1.105−3 5.395−4 7.194−4 4.609−5 5.745−5 2.393−2 1.785−3 1.457−2 3.074−3 8.849−2 4.343−3 3.697−4 2.796−3 7.753−4 1.461−2 9.993−4 2.476−3 4.338−4 1.471−4 1.051−3 3.251−4 5.246−3 4.165−4 1.207−3 2.175−4 7.385−5 2.320−5 3.898−3 3.341−3 3.268−2 2.378−2 1.689−1 7.763−4 8.093−4 6.442−3 4.200−3 2.773−2 1.338−3 4.785−3 3.055−4 3.364−4 2.453−3 1.568−3 9.972−3 6.524−4 2.325−3 5.902−5 1.472−4 1.718+0 3.207+0 6.807−2 1.027−1 6.715−2 4.169−2 7.704−2
2.542−1 4.809−1 1.498−2 1.102−2 2.056−2 1.429−2 2.136−2 2.968−3 2.233−3 4.239−3 2.111−3 3.177−3 1.118−3 1.484−3 1.143−3 8.757−4 1.668−3 7.323−4 1.104−3 5.552−4 7.378−4 4.717−5 5.871−5 1.775−2 1.678−3 1.510−2 2.915−3 9.387−2 3.874−3 3.465−4 3.034−3 7.611−4 1.518−2 9.286−4 2.594−3 3.977−4 1.378−4 1.185−3 3.310−4 5.399−3 4.034−4 1.291−3 2.230−4 7.573−5 2.429−5 3.642−3 3.142−3 3.360−2 2.432−2 1.779−1 7.276−4 7.921−4 6.892−3 4.230−3 2.867−2 1.311−3 4.940−3 2.860−4 3.418−4 2.718−3 1.585−3 1.022−2 6.816−4 2.465−3 5.991−5 1.501−4 1.868+0 3.427+0 6.706−2 1.011−1 6.949−2 4.505−2 8.353−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
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K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
87
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.640−2 3.918−2 2.609−2 3.477−2 1.134−2 2.397−3 4.490−3 5.580−3 8.332−3 3.065−3 4.097−3 4.805−3 5.997−3 1.164−1 1.374+0 1.811−2 4.064−3 6.534−2 9.149−3 8.113−2 1.183−2 8.709−2 1.273−2 1.148−3 1.244−2 2.516−3 1.626−2 3.327−3 9.551−3 3.093−3 1.088−2 3.751−3 3.271−1 2.659+0 8.341−3 9.916−3 1.415−1 3.213−2 1.633−1 4.196−2 1.612−1 2.320−3 2.634−3 2.752−2 7.466−3 3.309−2 6.710−3 1.854−2 8.863−3 2.123−2 8.524−2 3.513−3 6.693−3 6.799−3 1.277−1 1.615−2 5.588−1 2.831−2 1.139−3 2.321−3 2.716−3 2.457−2 6.127−3 8.644−2 9.624−3 2.517−2 5.649−3 5.311−3 4.630−3 1.579−2 1.625−2 2.002−1 7.086−2 8.163−1
2.826−2 4.331−2 3.306−2 4.482−2 1.116−2 2.715−3 5.037−3 5.603−3 8.401−3 3.542−3 4.736−3 4.968−3 6.212−3 1.432−1 1.412+0 6.133−2 9.763−3 6.551−2 1.269−2 8.245−2 1.755−2 8.897−2 2.158−2 1.427−3 1.156−2 2.512−3 1.806−2 3.659−3 9.756−3 3.266−3 1.128−2 3.817−3 3.790−1 2.731+0 2.114−2 1.431−2 1.463−1 4.183−2 1.780−1 5.314−2 1.788−1 2.921−3 2.686−3 2.575−2 8.268−3 3.675−2 7.011−3 1.908−2 9.114−3 2.205−2 2.418−1 9.547−3 1.567−2 1.684−2 1.373−1 3.197−2 5.666−1 5.293−2 1.699−3 2.891−3 3.138−3 2.407−2 6.453−3 9.093−2 1.012−2 2.460−2 5.561−3 1.661−2 1.193−2 3.687−2 3.154−2 2.278−1 1.024−1 8.678−1
2.874−2 4.374−2 3.176−2 4.284−2 1.126−2 2.929−3 5.442−3 5.739−3 8.608−3 3.383−3 4.525−3 4.865−3 6.083−3 1.386−1 1.482+0 5.704−2 8.282−3 6.515−2 1.175−2 8.836−2 1.590−2 9.111−2 1.887−2 1.347−3 1.165−2 2.462−3 1.918−2 3.455−3 9.847−3 2.986−3 1.156−2 3.544−3 3.896−1 2.857+0 1.790−2 1.318−2 1.446−1 4.062−2 1.866−1 5.040−2 1.791−1 2.766−3 2.618−3 2.591−2 8.246−3 3.867−2 6.667−3 1.902−2 8.836−3 2.234−2 2.229−1 7.762−3 1.330−2 1.395−2 1.348−1 2.691−2 5.909−1 4.446−2 1.487−3 2.637−3 2.827−3 2.388−2 5.819−3 9.393−2 9.020−3 2.559−2 4.947−3 1.318−2 9.692−3 3.132−2 2.656−2 2.203−1 9.431−2 8.938−1
2.968−2 4.487−2 3.054−2 4.105−2 1.142−2 3.275−3 6.099−3 5.936−3 8.903−3 3.214−3 4.299−3 4.781−3 5.977−3 1.318−1 1.588+0 4.914−2 7.530−3 6.512−2 1.107−2 9.779−2 1.438−2 9.460−2 1.636−2 1.328−3 1.178−2 2.426−3 2.082−2 3.233−3 9.999−3 2.682−3 1.194−2 3.255−3 4.074−1 3.071+0 1.628−2 1.235−2 1.437−1 4.027−2 2.017−1 4.834−2 1.818−1 2.743−3 2.573−3 2.616−2 8.314−3 4.155−2 6.310−3 1.904−2 8.570−3 2.279−2 1.900−1 6.365−3 1.156−2 1.139−2 1.327−1 2.214−2 6.289−1 3.642−2 1.313−3 2.440−3 2.512−3 2.370−2 5.127−3 9.831−2 7.806−3 2.712−2 4.302−3 1.057−2 7.757−3 2.682−2 2.190−2 2.135−1 8.746−2 9.390−1
3.121−2 4.694−2 2.962−2 3.971−2 1.163−2 3.798−3 7.093−3 6.201−3 9.301−3 3.052−3 4.083−3 4.736−3 5.920−3 1.244−1 1.729+0 4.046−2 7.472−3 6.547−2 1.073−2 1.119−1 1.316−2 9.965−2 1.431−2 1.375−3 1.195−2 2.412−3 2.317−2 3.012−3 1.023−2 2.381−3 1.241−2 2.974−3 4.346−1 3.371+0 1.620−2 1.193−2 1.439−1 4.134−2 2.261−1 4.731−2 1.878−1 2.859−3 2.558−3 2.651−2 8.526−3 4.572−2 5.978−3 1.919−2 8.347−3 2.339−2 1.539−1 5.342−3 1.050−2 9.367−3 1.313−1 1.811−2 6.852−1 2.951−2 1.172−3 2.303−3 2.211−3 2.357−2 4.431−3 1.045−1 6.579−3 2.929−2 3.683−3 8.696−3 6.206−3 2.370−2 1.798−2 2.086−1 8.323−2 1.012+0
3.333−2 4.993−2 2.904−2 3.887−2 1.187−2 4.540−3 8.509−3 6.535−3 9.801−3 2.915−3 3.900−3 4.745−3 5.931−3 1.179−1 1.895+0 3.288−2 8.081−3 6.616−2 1.074−2 1.316−1 1.225−2 1.061−1 1.279−2 1.493−3 1.214−2 2.426−3 2.636−2 2.809−3 1.054−2 2.109−3 1.293−2 2.726−3 4.689−1 3.722+0 1.760−2 1.191−2 1.451−1 4.408−2 2.615−1 4.734−2 1.970−1 3.131−3 2.575−3 2.693−2 8.937−3 5.147−2 5.708−3 1.950−2 8.186−3 2.411−2 1.217−1 4.644−3 1.011−2 7.883−3 1.308−1 1.495−2 7.631−1 2.396−2 1.061−3 2.233−3 1.947−3 2.350−2 3.785−3 1.129−1 5.439−3 3.210−2 3.140−3 7.428−3 5.027−3 2.199−2 1.490−2 2.056−1 8.221−2 1.117+0
3.587−2 5.360−2 2.875−2 3.844−2 1.213−2 5.540−3 1.042−2 6.924−3 1.038−2 2.814−3 3.766−3 4.813−3 6.015−3 1.127−1 2.074+0 2.710−2 9.335−3 6.706−2 1.102−2 1.577−1 1.161−2 1.136−1 1.176−2 1.693−3 1.235−2 2.473−3 3.054−2 2.639−3 1.092−2 1.886−3 1.346−2 2.525−3 5.067−1 4.091+0 2.044−2 1.220−2 1.471−1 4.860−2 3.094−1 4.828−2 2.085−1 3.575−3 2.627−3 2.741−2 9.593−3 5.907−2 5.520−3 1.997−2 8.091−3 2.487−2 9.625−2 4.203−3 1.033−2 6.884−3 1.310−1 1.261−2 8.652−1 1.975−2 9.794−4 2.236−3 1.733−3 2.351−2 3.235−3 1.239−1 4.462−3 3.546−2 2.702−3 6.627−3 4.165−3 2.159−2 1.263−2 2.043−1 8.458−2 1.260+0
3.852−2 5.746−2 2.864−2 3.826−2 1.235−2 6.779−3 1.279−2 7.322−3 1.098−2 2.748−3 3.677−3 4.919−3 6.147−3 1.086−1 2.250+0 2.307−2 1.114−2 6.790−2 1.146−2 1.895−1 1.117−2 1.211−1 1.113−2 1.965−3 1.251−2 2.540−3 3.560−2 2.505−3 1.131−2 1.717−3 1.391−2 2.371−3 5.439−1 4.446+0 2.450−2 1.268−2 1.492−1 5.465−2 3.684−1 4.968−2 2.206−1 4.176−3 2.701−3 2.784−2 1.047−2 6.831−2 5.405−3 2.048−2 8.033−3 2.553−2 7.740−2 3.947−3 1.107−2 6.275−3 1.314−1 1.095−2 9.883−1 1.668−2 9.241−4 2.307−3 1.575−3 2.352−2 2.795−3 1.370−1 3.682−3 3.903−2 2.375−3 6.151−3 3.554−3 2.229−2 1.103−2 2.037−1 8.990−2 1.434+0
4.018−2 5.987−2 2.814−2 3.757−2 1.231−2 7.960−3 1.504−2 7.540−3 1.131−2 2.664−3 3.565−3 4.947−3 6.182−3 1.039−1 2.368+0 2.019−2 1.298−2 6.738−2 1.173−2 2.192−1 1.069−2 1.254−1 1.059−2 2.230−3 1.241−2 2.567−3 4.019−2 2.365−3 1.144−2 1.573−3 1.399−2 2.224−3 5.675−1 4.677+0 2.862−2 1.297−2 1.485−1 6.030−2 4.236−1 5.026−2 2.274−1 4.761−3 2.731−3 2.768−2 1.125−2 7.667−2 5.253−3 2.059−2 7.859−3 2.556−2 6.349−2 3.750−3 1.189−2 5.860−3 1.295−1 9.698−3 1.098+0 1.436−2 8.753−4 2.378−3 1.447−3 2.311−2 2.436−3 1.480−1 3.066−3 4.156−2 2.117−3 5.796−3 3.093−3 2.325−2 9.801−3 2.000−1 9.525−2 1.591+0
4.224−2 6.277−2 2.850−2 3.799−2 1.337−2 8.468−3 1.599−2 7.827−3 1.171−2 2.637−3 3.529−3 5.226−3 6.523−3 1.042−1 2.493+0 1.550−2 1.405−2 7.137−2 1.254−2 2.353−1 1.086−2 1.315−1 1.042−2 2.397−3 1.404−2 2.825−3 4.169−2 2.401−3 1.160−2 1.573−3 1.442−2 2.320−3 5.960−1 4.928+0 3.074−2 1.378−2 1.571−1 6.355−2 4.519−1 5.187−2 2.369−1 5.078−3 2.998−3 3.109−2 1.160−2 7.927−2 5.301−3 2.087−2 8.133−3 2.630−2 4.680−2 3.544−3 1.193−2 5.495−3 1.330−1 9.047−3 1.161+0 1.331−2 8.829−4 2.473−3 1.488−3 2.457−2 2.495−3 1.541−1 3.144−3 4.387−2 2.297−3 5.389−3 2.781−3 2.299−2 9.215−3 2.047−1 9.804−2 1.675+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
88
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.712−3 1.900−3 5.718−3 6.130−3 3.995−2 1.660−2 1.281−1 9.161−3 3.748−2 3.527+0 6.670+0 3.187−1 4.782−1 2.884−2 3.860−2 1.880−1 2.704−2 4.874−2 5.654−2 8.369−2 6.166−2 8.199−2 3.136−2 3.916−2 4.080−1 6.050+0 5.210−2 2.494−1 2.421−2 1.377−2 1.978−1 2.470−2 1.435−1 2.672−2 1.818−1 2.158−2 1.111−1 2.143−2 1.365+0 1.171+1 1.024−1 4.465−1 2.939−2 2.697−2 4.231−1 6.497−2 2.971−1 8.188−2 3.358−1 6.614−2 2.013−1 2.056−1 7.420+0 4.836−2 1.219−2 2.204−2 1.712−2 4.087−1 2.639−2 7.792−1 3.820−2 5.000−1 3.868−2 5.569−1 9.540+0 1.849−2 1.102−2 4.827−2 2.679−2 6.276−1 9.793−2 1.141+0 9.893−2 7.123−1
2.546−3 2.325−3 6.670−3 6.467−3 3.966−2 1.743−2 1.348−1 9.035−3 3.673−2 3.683+0 7.067+0 3.433−1 5.557−1 7.295−2 1.111−1 1.792−1 2.833−2 5.087−2 5.562−2 8.274−2 6.199−2 8.259−2 3.252−2 4.066−2 4.458−1 6.315+0 1.053−1 3.079−1 9.076−2 1.768−2 1.808−1 2.295−2 1.452−1 2.519−2 1.798−1 2.237−2 1.135−1 2.242−2 1.542+0 1.477+1 2.154−1 6.735−1 3.966−2 2.570−2 3.854−1 6.344−2 2.995−1 8.238−2 3.336−1 6.814−2 2.058−1 3.345−1 8.210+0 2.286−1 1.649−2 2.925−2 1.745−2 3.853−1 2.578−2 7.739−1 3.636−2 4.940−1 3.704−2 1.009+0 1.342+1 2.434−2 1.136−2 5.812−2 2.641−2 5.933−1 9.565−2 1.131+0 9.643−2 7.042−1
2.232−3 2.046−3 6.134−3 5.832−3 3.898−2 1.645−2 1.387−1 8.453−3 3.788−2 4.010+0 7.593+0 3.334−1 5.337−1 6.268−2 9.380−2 1.820−1 3.351−2 6.045−2 5.934−2 8.822−2 6.249−2 8.326−2 3.268−2 4.085−2 4.267−1 6.892+0 9.430−2 2.892−1 7.263−2 1.869−2 1.839−1 2.411−2 1.669−1 2.526−2 1.908−1 2.217−2 1.140−1 2.122−2 1.686+0 1.564+1 1.852−1 6.096−1 4.147−2 2.681−2 3.934−1 6.816−2 3.406−1 8.538−2 3.527−1 6.669−2 2.058−1 2.948−1 9.452+0 1.788−1 1.517−2 2.905−2 1.720−2 3.916−1 2.512−2 8.518−1 3.430−2 5.190−1 3.443−2 1.101+0 1.542+1 2.266−2 1.078−2 5.823−2 2.568−2 6.023−1 9.903−2 1.243+0 9.631−2 7.379−1
1.976−3 1.776−3 5.655−3 5.141−3 3.832−2 1.544−2 1.444−1 7.897−3 3.977−2 4.388+0 8.222+0 3.235−1 5.109−1 5.355−2 7.854−2 1.854−1 4.101−2 7.441−2 6.411−2 9.524−2 6.293−2 8.385−2 3.309−2 4.137−2 4.085−1 7.566+0 8.458−2 2.719−1 5.667−2 2.105−2 1.875−1 2.573−2 1.970−1 2.533−2 2.045−1 2.211−2 1.145−1 2.010−2 1.849+0 1.657+1 1.574−1 5.503−1 4.644−2 2.849−2 4.028−1 7.465−2 3.977−1 8.934−2 3.764−1 6.534−2 2.058−1 2.591−1 1.076+1 1.353−1 1.458−2 3.035−2 1.724−2 3.987−1 2.464−2 9.579−1 3.230−2 5.500−1 3.203−2 1.189+0 1.740+1 2.197−2 1.036−2 6.061−2 2.518−2 6.127−1 1.045−1 1.395+0 9.709−2 7.796−1
1.765−3 1.522−3 5.260−3 4.444−3 3.774−2 1.456−2 1.528−1 7.441−3 4.256−2 4.799+0 8.934+0 3.148−1 4.907−1 4.656−2 6.690−2 1.893−1 5.148−2 9.393−2 6.977−2 1.036−1 6.328−2 8.432−2 3.377−2 4.222−2 3.927−1 8.296+0 7.746−2 2.576−1 4.420−2 2.495−2 1.913−1 2.774−2 2.379−1 2.539−2 2.204−1 2.220−2 1.149−1 1.914−2 2.021+0 1.761+1 1.351−1 5.021−1 5.493−2 3.064−2 4.130−1 8.345−2 4.753−1 9.416−2 4.041−1 6.422−2 2.058−1 2.303−1 1.203+1 1.016−1 1.449−2 3.326−2 1.760−2 4.062−1 2.442−2 1.100+0 3.052−2 5.857−1 3.007−2 1.272+0 1.927+1 2.197−2 1.007−2 6.559−2 2.496−2 6.238−1 1.129−1 1.599+0 9.887−2 8.280−1
1.600−3 1.297−3 4.982−3 3.800−3 3.729−2 1.393−2 1.644−1 7.142−3 4.630−2 5.229+0 9.707+0 3.074−1 4.742−1 4.175−2 5.887−2 1.931−1 6.560−2 1.201−1 7.595−2 1.127−1 6.357−2 8.469−2 3.467−2 4.334−2 3.795−1 9.049+0 7.301−2 2.463−1 3.517−2 3.059−2 1.951−1 3.002−2 2.919−1 2.544−2 2.376−1 2.245−2 1.154−1 1.843−2 2.193+0 1.876+1 1.185−1 4.656−1 6.739−2 3.309−2 4.234−1 9.510−2 5.777−1 9.952−2 4.341−1 6.342−2 2.061−1 2.088−1 1.320+1 7.734−2 1.475−2 3.795−2 1.833−2 4.137−1 2.449−2 1.285+0 2.906−2 6.240−1 2.864−2 1.350+0 2.099+1 2.244−2 9.871−3 7.357−2 2.503−2 6.349−1 1.248−1 1.866+0 1.015−1 8.805−1
1.479−3 1.109−3 4.850−3 3.250−3 3.700−2 1.365−2 1.797−1 7.025−3 5.084−2 5.666+0 1.052+1 3.009−1 4.607−1 3.876−2 5.380−2 1.967−1 8.375−2 1.537−1 8.214−2 1.219−1 6.385−2 8.505−2 3.569−2 4.463−2 3.683−1 9.804+0 7.075−2 2.375−1 2.895−2 3.810−2 1.986−1 3.235−2 3.603−1 2.550−2 2.546−1 2.280−2 1.160−1 1.796−2 2.361+0 1.998+1 1.067−1 4.386−1 8.403−2 3.562−2 4.332−1 1.099−1 7.072−1 1.050−1 4.642−1 6.301−2 2.068−1 1.932−1 1.428+1 6.087−2 1.519−2 4.450−2 1.943−2 4.206−1 2.478−2 1.517+0 2.799−2 6.619−1 2.774−2 1.422+0 2.254+1 2.314−2 9.759−3 8.476−2 2.533−2 6.454−1 1.408−1 2.202+0 1.047−1 9.328−1
1.396−3 9.608−4 4.859−3 2.812−3 3.679−2 1.375−2 1.982−1 7.054−3 5.571−2 6.079+0 1.130+1 2.947−1 4.487−1 3.702−2 5.076−2 1.993−1 1.052−1 1.932−1 8.751−2 1.300−1 6.403−2 8.529−2 3.664−2 4.582−2 3.577−1 1.051+1 6.989−2 2.302−1 2.478−2 4.709−2 2.012−1 3.442−2 4.400−1 2.554−2 2.692−1 2.315−2 1.165−1 1.769−2 2.514+0 2.116+1 9.829−2 4.180−1 1.040−1 3.785−2 4.408−1 1.270−1 8.583−1 1.096−1 4.899−1 6.282−2 2.075−1 1.816−1 1.521+1 5.008−2 1.566−2 5.249−2 2.076−2 4.256−1 2.510−2 1.785+0 2.722−2 6.941−1 2.720−2 1.485+0 2.388+1 2.386−2 9.697−3 9.844−2 2.567−2 6.529−1 1.599−1 2.592+0 1.077−1 9.772−1
1.323−3 8.394−4 4.885−3 2.453−3 3.599−2 1.388−2 2.137−1 7.044−3 5.915−2 6.325+0 1.178+1 2.839−1 4.309−1 3.549−2 4.825−2 1.975−1 1.248−1 2.294−1 8.989−2 1.336−1 6.301−2 8.394−2 3.675−2 4.595−2 3.418−1 1.093+1 6.863−2 2.203−1 2.174−2 5.532−2 1.992−1 3.537−2 5.114−1 2.511−2 2.749−1 2.303−2 1.149−1 1.725−2 2.597+0 2.180+1 9.094−2 3.956−1 1.223−1 3.887−2 4.380−1 1.416−1 9.930−1 1.109−1 4.996−1 6.167−2 2.044−1 1.702−1 1.568+1 4.267−2 1.578−2 5.970−2 2.168−2 4.209−1 2.490−2 2.019+0 2.624−2 7.045−1 2.645−2 1.508+0 2.451+1 2.403−2 9.498−3 1.106−1 2.548−2 6.458−1 1.762−1 2.931+0 1.080−1 9.913−1
1.334−3 8.533−4 5.075−3 2.514−3 3.818−2 1.442−2 2.223−1 7.511−3 6.239−2 6.517+0 1.214+1 2.954−1 4.447−1 3.465−2 4.635−2 2.076−1 1.220−1 2.249−1 9.023−2 1.337−1 1.512−1 2.044−1 4.074−2 5.093−2 3.604−1 1.131+1 6.857−2 2.264−1 1.853−2 5.277−2 2.146−1 3.593−2 5.172−1 3.083−2 2.818−1 2.581−2 1.274−1 1.941−2 2.616+0 2.236+1 8.772−2 3.991−1 1.151−1 3.946−2 4.681−1 1.473−1 1.001+0 1.169−1 5.140−1 6.914−2 2.276−1 1.722−1 1.669+1 3.343−2 1.547−2 5.562−2 1.166−1 4.356−1 2.597−2 2.107+0 4.246−2 7.330−1 2.892−2 1.693+0 2.585+1 2.353−2 2.345−2 1.506−1 2.658−2 6.679−1 1.983−1 3.056+0 1.140−1 1.033+0
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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89
Table 31 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.30
6.50
6.70
6.90
7.10
7.30
7.50
7.70
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.840−1 4.655−3 9.498−3 9.863−3 3.622−2 1.865−2 5.168−1 3.859−2 2.803+0 7.012−2 6.223−3 5.672−3 2.007−2 1.504−2 5.829−2 3.867−2 7.027−1 1.770−1 3.664+0 9.081+0 1.718+1 9.009−1 1.350+0 1.019−1 1.363−1 2.880−2 3.612−2 1.050+0 1.652+1 1.403−1 9.743−1 6.798−2 6.182−2 1.965−2 3.688+0 3.133+1 3.663−1 1.728+0 4.639−2 1.146−1 5.339−1 2.249+1 9.828−2 8.071−1 4.897−2 1.763+0 3.131+1 1.439−1 1.141+0 3.484−1 1.782+1 9.245−2 9.346−1 2.362+1 3.277−1
6.116−1 6.881−3 1.126−2 1.079−2 4.085−2 1.832−2 5.008−1 3.598−2 2.798+0 6.445−2 9.377−3 6.593−3 2.274−2 1.460−2 6.571−2 3.619−2 6.805−1 1.711−1 3.651+0 1.028+1 1.906+1 8.776−1 1.320+0 1.104−1 1.473−1 2.935−2 3.672−2 9.990−1 1.943+1 1.537−1 9.411−1 6.825−2 6.723−2 1.886−2 4.687+0 3.853+1 3.557−1 1.661+0 4.703−2 1.234−1 5.108−1 3.683+1 1.018−1 7.751−1 4.602−2 3.739+0 5.825+1 1.373−1 1.096+0 3.287−1 3.493+1 8.289−2 2.638+0 4.941+1 2.875−1
4.858−1 5.796−3 1.042−2 9.581−3 4.007−2 1.635−2 5.033−1 3.201−2 2.990+0 5.692−2 7.862−3 5.619−3 2.096−2 1.275−2 6.340−2 3.218−2 6.826−1 1.703−1 3.899+0 1.121+1 2.068+1 8.649−1 1.301+0 1.117−1 1.491−1 2.821−2 3.529−2 9.792−1 2.115+1 1.566−1 9.245−1 6.706−2 6.699−2 1.740−2 5.126+0 4.214+1 3.486−1 1.627+0 4.499−2 1.219−1 4.997−1 4.060+1 1.005−1 7.572−1 4.187−2 4.073+0 6.416+1 1.305−1 1.068+0 3.148−1 3.840+1 7.472−2 2.790+0 5.416+1 2.594−1
3.738−1 4.983−3 9.837−3 8.507−3 3.983−2 1.447−2 5.066−1 2.816−2 3.249+0 4.958−2 6.736−3 4.769−3 1.959−2 1.097−2 6.203−2 2.831−2 6.856−1 1.723−1 4.234+0 1.221+1 2.247+1 8.524−1 1.283+0 1.135−1 1.515−1 2.722−2 3.405−2 9.596−1 2.301+1 1.600−1 9.085−1 6.603−2 6.707−2 1.614−2 5.577+0 4.590+1 3.418−1 1.594+0 4.332−2 1.211−1 4.890−1 4.433+1 9.984−2 7.401−1 3.816−2 4.391+0 6.990+1 1.244−1 1.042+0 3.017−1 4.175+1 6.758−2 2.932+0 5.870+1 2.334−1
2.849−1 4.382−3 9.475−3 7.609−3 4.041−2 1.283−2 5.102−1 2.476−2 3.592+0 4.304−2 5.906−3 4.060−3 1.860−2 9.383−3 6.199−2 2.490−2 6.893−1 1.783−1 4.681+0 1.324+1 2.440+1 8.396−1 1.264+0 1.156−1 1.544−1 2.642−2 3.307−2 9.395−1 2.494+1 1.640−1 8.925−1 6.522−2 6.748−2 1.516−2 6.027+0 4.972+1 3.351−1 1.561+0 4.213−2 1.210−1 4.787−1 4.790+1 9.995−2 7.236−1 3.511−2 4.686+0 7.533+1 1.191−1 1.017+0 2.900−1 4.489+1 6.192−2 3.061+0 6.293+1 2.111−1
2.191−1 3.950−3 9.295−3 6.911−3 4.200−2 1.154−2 5.141−1 2.200−2 4.039+0 3.763−2 5.314−3 3.499−3 1.798−2 8.066−3 6.357−2 2.213−2 6.936−1 1.895−1 5.263+0 1.431+1 2.641+1 8.255−1 1.242+0 1.181−1 1.577−1 2.585−2 3.235−2 9.178−1 2.690+1 1.683−1 8.758−1 6.463−2 6.819−2 1.447−2 6.468+0 5.352+1 3.284−1 1.525+0 4.143−2 1.216−1 4.684−1 5.128+1 1.008−1 7.067−1 3.279−2 4.956+0 8.040+1 1.146−1 9.924−1 2.796−1 4.781+1 5.784−2 3.177+0 6.683+1 1.929−1
1.727−1 3.657−3 9.253−3 6.409−3 4.470−2 1.064−2 5.179−1 1.992−2 4.599+0 3.351−2 4.911−3 3.083−3 1.766−2 7.051−3 6.693−2 2.006−2 6.979−1 2.066−1 5.994+0 1.537+1 2.845+1 8.099−1 1.219+0 1.207−1 1.613−1 2.547−2 3.188−2 8.934−1 2.885+1 1.729−1 8.580−1 6.426−2 6.913−2 1.405−2 6.895+0 5.723+1 3.213−1 1.486+0 4.114−2 1.227−1 4.577−1 5.446+1 1.021−1 6.888−1 3.113−2 5.203+0 8.511+1 1.107−1 9.666−1 2.704−1 5.051+1 5.518−2 3.283+0 7.040+1 1.785−1
1.406−1 3.464−3 9.279−3 6.061−3 4.826−2 1.008−2 5.200−1 1.842−2 5.243+0 3.053−2 4.647−3 2.789−3 1.752−2 6.307−3 7.165−2 1.856−2 7.002−1 2.282−1 6.838+0 1.636+1 3.039+1 7.926−1 1.193+0 1.233−1 1.648−1 2.520−2 3.155−2 8.643−1 3.065+1 1.773−1 8.385−1 6.393−2 7.011−2 1.382−2 7.277+0 6.060+1 3.128−1 1.439+0 4.101−2 1.236−1 4.451−1 5.725+1 1.035−1 6.676−1 2.993−2 5.412+0 8.919+1 1.069−1 9.366−1 2.613−1 5.284+1 5.350−2 3.369+0 7.345+1 1.670−1
1.175−1 3.290−3 9.165−3 5.734−3 5.113−2 9.594−3 5.113−1 1.709−2 5.785+0 2.806−2 4.409−3 2.551−3 1.716−2 5.703−3 7.548−2 1.722−2 6.881−1 2.466−1 7.549+0 1.690+1 3.148+1 7.643−1 1.150+0 1.235−1 1.652−1 2.458−2 3.078−2 8.196−1 3.161+1 1.782−1 8.064−1 6.255−2 6.979−2 1.347−2 7.455+0 6.229+1 2.985−1 1.366+0 4.019−2 1.219−1 4.245−1 5.844+1 1.026−1 6.340−1 2.857−2 5.476+0 9.079+1 1.015−1 8.890−1 2.481−1 5.371+1 5.156−2 3.371+0 7.450+1 1.553−1
9.698−2 3.452−3 9.370−3 6.297−3 5.078−2 1.092−2 5.260−1 1.892−2 6.050+0 3.130−2 4.624−3 2.941−3 1.783−2 7.068−3 7.498−2 1.907−2 7.085−1 2.575−1 7.872+0 1.711+1 3.046+1 7.546−1 1.135+0 1.640−1 2.212−1 2.895−2 3.638−2 8.409−1 2.867+1 1.942−1 8.061−1 6.608−2 7.643−2 1.469−2 6.813+0 5.563+1 3.261−1 1.430+0 5.272−2 1.667−1 4.638−1 5.574+1 1.237−1 6.688−1 3.142−2 5.097+0 9.408+1 1.088−1 9.390−1 2.663−1 5.124+1 6.851−2 2.943+0 7.343+1 1.728−1
90
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
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Table 32 Effective collision strengths for transitions in Ni XXVI. (a ± b ≡ a × 10±b ). Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 5 6 7 8 9 10 11
1.449−1 2.771−1 1.240−2 3.775−3 6.860−3 9.619−3 1.436−2 2.472−3 9.209−4 1.712−3 1.724−3 2.588−3 1.028−3 1.364−3 9.620−4 3.904−4 7.294−4 6.585−4 9.889−4 5.425−4 7.200−4 6.993−5 8.700−5 2.428−2 8.777−4 1.330−2 3.490−3 4.551−2 6.475−3 2.776−4 2.748−3 1.146−3 8.324−3 2.004−3 1.432−3 8.346−4 1.316−4 1.093−3 5.463−4 3.127−3 9.368−4 7.474−4 5.027−4 6.852−5 6.699−5 1.789−3 3.629−3 3.045−2 1.752−2 9.031−2 5.504−4 1.163−3 6.682−3 4.150−3 1.697−2 1.547−3 3.180−3 2.603−4 5.516−4 2.738−3 1.774−3 6.496−3 8.927−4 1.703−3 1.184−4 1.671−4 9.784−1 1.823+0 6.561−2 9.859−2 5.736−2 1.060−2 1.907−2
1.492−1 2.839−1 1.381−2 4.748−3 8.756−3 1.059−2 1.598−2 2.788−3 1.236−3 2.380−3 2.056−3 3.094−3 1.345−3 1.786−3 9.430−4 4.417−4 8.328−4 6.985−4 1.050−3 5.681−4 7.552−4 7.428−5 9.220−5 3.765−2 3.138−3 1.454−2 5.943−3 4.685−2 1.029−2 7.999−4 3.075−3 1.785−3 9.052−3 2.789−3 2.111−3 1.505−3 2.147−4 1.041−3 5.787−4 3.264−3 9.817−4 7.947−4 5.162−4 7.431−5 6.618−5 8.127−3 6.506−3 3.516−2 2.272−2 9.621−2 1.599−3 1.853−3 8.116−3 5.304−3 1.899−2 2.785−3 4.893−3 4.377−4 6.027−4 2.661−3 1.872−3 6.802−3 9.362−4 1.806−3 1.206−4 1.776−4 9.437−1 1.802+0 8.697−2 1.328−1 5.985−2 1.247−2 2.587−2
1.564−1 2.974−1 1.357−2 4.847−3 8.954−3 1.066−2 1.609−2 2.676−3 1.200−3 2.301−3 1.975−3 2.972−3 1.248−3 1.657−3 9.373−4 4.482−4 8.477−4 6.894−4 1.037−3 5.549−4 7.378−4 6.929−5 8.601−5 4.070−2 2.629−3 1.436−2 5.493−3 4.854−2 9.554−3 6.494−4 2.938−3 1.564−3 9.150−3 2.475−3 1.964−3 1.264−3 1.940−4 1.027−3 5.441−4 3.336−3 9.145−4 7.986−4 4.755−4 7.116−5 5.969−5 6.477−3 5.929−3 3.437−2 2.215−2 9.878−2 1.303−3 1.615−3 7.614−3 4.925−3 1.892−2 2.392−3 4.461−3 3.949−4 5.625−4 2.607−3 1.803−3 6.881−3 8.820−4 1.783−3 1.102−4 1.676−4 1.006+0 1.910+0 8.426−2 1.281−1 5.949−2 1.336−2 2.688−2
1.646−1 3.129−1 1.337−2 5.031−3 9.295−3 1.072−2 1.615−2 2.599−3 1.198−3 2.287−3 1.909−3 2.873−3 1.165−3 1.546−3 9.380−4 4.636−4 8.787−4 6.798−4 1.024−3 5.406−4 7.189−4 6.370−5 7.907−5 4.089−2 2.196−3 1.410−2 4.894−3 5.087−2 8.466−3 5.336−4 2.821−3 1.356−3 9.385−3 2.151−3 1.868−3 1.041−3 1.760−4 1.014−3 5.033−4 3.447−3 8.307−4 8.126−4 4.267−4 6.831−5 5.228−5 5.208−3 5.245−3 3.329−2 2.126−2 1.023−1 1.075−3 1.397−3 7.151−3 4.567−3 1.910−2 2.038−3 4.130−3 3.580−4 5.180−4 2.546−3 1.721−3 7.019−3 8.201−4 1.773−3 9.863−5 1.575−4 1.089+0 2.053+0 7.982−2 1.210−1 5.954−2 1.513−2 2.942−2
1.746−1 3.313−1 1.326−2 5.411−3 1.000−2 1.088−2 1.638−2 2.561−3 1.246−3 2.371−3 1.868−3 2.813−3 1.101−3 1.463−3 9.447−4 4.922−4 9.349−4 6.717−4 1.012−3 5.270−4 7.012−4 5.797−5 7.198−5 3.824−2 1.861−3 1.386−2 4.282−3 5.440−2 7.281−3 4.489−4 2.735−3 1.172−3 9.825−3 1.836−3 1.841−3 8.470−4 1.604−4 1.004−3 4.579−4 3.617−3 7.338−4 8.430−4 3.730−4 6.629−5 4.448−5 4.292−3 4.578−3 3.226−2 2.049−2 1.079−1 9.095−4 1.207−3 6.773−3 4.265−3 1.966−2 1.748−3 3.946−3 3.268−4 4.703−4 2.484−3 1.635−3 7.253−3 7.564−4 1.790−3 8.684−5 1.487−4 1.193+0 2.232+0 7.510−2 1.137−1 6.000−2 1.803−2 3.417−2
1.873−1 3.543−1 1.328−2 6.094−3 1.128−2 1.124−2 1.690−2 2.558−3 1.357−3 2.578−3 1.859−3 2.801−3 1.061−3 1.410−3 9.573−4 5.395−4 1.027−3 6.680−4 1.008−3 5.167−4 6.878−4 5.269−5 6.546−5 3.384−2 1.645−3 1.372−2 3.746−3 5.967−2 6.170−3 3.915−4 2.681−3 1.015−3 1.053−2 1.542−3 1.893−3 6.852−4 1.481−4 9.969−4 4.109−4 3.865−3 6.307−4 8.957−4 3.188−4 6.559−5 3.694−5 3.722−3 4.010−3 3.150−2 2.018−2 1.169−1 7.992−4 1.047−3 6.491−3 4.045−3 2.073−2 1.530−3 3.927−3 3.027−4 4.221−4 2.426−3 1.557−3 7.627−3 6.988−4 1.846−3 7.588−5 1.424−4 1.311+0 2.438+0 7.098−2 1.073−1 6.080−2 2.227−2 4.156−2
2.029−1 3.823−1 1.342−2 7.164−3 1.328−2 1.182−2 1.775−2 2.584−3 1.542−3 2.931−3 1.883−3 2.839−3 1.041−3 1.385−3 9.751−4 6.112−4 1.167−3 6.712−4 1.014−3 5.110−4 6.807−4 4.832−5 6.010−5 2.904−2 1.556−3 1.368−2 3.326−3 6.711−2 5.223−3 3.587−4 2.655−3 8.854−4 1.156−2 1.281−3 2.021−3 5.556−4 1.402−4 9.939−4 3.662−4 4.213−3 5.303−4 9.740−4 2.688−4 6.632−5 3.022−5 3.479−3 3.575−3 3.106−2 2.053−2 1.301−1 7.396−4 9.170−4 6.300−3 3.929−3 2.240−2 1.383−3 4.066−3 2.883−4 3.769−4 2.378−3 1.503−3 8.183−3 6.545−4 1.951−3 6.660−5 1.392−4 1.435+0 2.661+0 6.775−2 1.023−1 6.179−2 2.798−2 5.182−2
2.198−1 4.127−1 1.359−2 8.585−3 1.595−2 1.252−2 1.878−2 2.616−3 1.791−3 3.408−3 1.926−3 2.906−3 1.033−3 1.375−3 9.912−4 7.036−4 1.347−3 6.785−4 1.026−3 5.078−4 6.768−4 4.493−5 5.594−5 2.471−2 1.578−3 1.367−2 3.017−3 7.633−2 4.459−3 3.465−4 2.638−3 7.817−4 1.281−2 1.060−3 2.196−3 4.555−4 1.369−4 9.901−4 3.261−4 4.631−3 4.394−4 1.068−3 2.260−4 6.785−5 2.462−5 3.509−3 3.261−3 3.079−2 2.148−2 1.468−1 7.224−4 8.136−4 6.157−3 3.909−3 2.454−2 1.293−3 4.311−3 2.839−4 3.367−4 2.333−3 1.474−3 8.876−3 6.245−4 2.088−3 5.920−5 1.382−4 1.551+0 2.875+0 6.511−2 9.830−2 6.253−2 3.478−2 6.421−2
2.310−1 4.330−1 1.342−2 9.878−3 1.839−2 1.288−2 1.932−2 2.578−3 2.006−3 3.822−3 1.925−3 2.906−3 1.006−3 1.340−3 9.776−4 7.800−4 1.496−3 6.701−4 1.014−3 4.932−4 6.577−4 4.154−5 5.177−5 2.098−2 1.632−3 1.335−2 2.747−3 8.386−2 3.814−3 3.403−4 2.561−3 6.893−4 1.374−2 8.703−4 2.316−3 3.759−4 1.340−4 9.606−4 2.874−4 4.921−3 3.590−4 1.129−3 1.891−4 6.776−5 1.999−5 3.625−3 2.987−3 2.991−2 2.223−2 1.603−1 7.165−4 7.210−4 5.905−3 3.862−3 2.609−2 1.216−3 4.471−3 2.800−4 2.978−4 2.236−3 1.433−3 9.341−3 5.929−4 2.172−3 5.257−5 1.349−4 1.607+0 2.982+0 6.158−2 9.296−2 6.138−2 4.051−2 7.468−2
2.443−1 4.597−1 1.401−2 1.099−2 2.041−2 1.362−2 2.035−2 2.768−3 2.227−3 4.215−3 1.990−3 2.996−3 1.047−3 1.390−3 1.068−3 8.680−4 1.650−3 6.868−4 1.036−3 5.193−4 6.901−4 4.342−5 5.404−5 1.615−2 1.637−3 1.404−2 2.688−3 9.134−2 3.490−3 3.348−4 2.820−3 6.901−4 1.472−2 8.170−4 2.492−3 3.533−4 1.316−4 1.098−3 2.977−4 5.215−3 3.522−4 1.241−3 1.970−4 7.097−5 2.173−5 3.591−3 2.921−3 3.126−2 2.339−2 1.734−1 7.067−4 7.222−4 6.397−3 4.004−3 2.776−2 1.227−3 4.745−3 2.751−4 3.089−4 2.511−3 1.487−3 9.852−3 6.340−4 2.363−3 5.678−5 1.417−4 1.776+0 3.246+0 6.209−2 9.367−2 6.483−2 4.526−2 8.348−2
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 4 4
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
91
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
12 13 14 15 16 17 18 19 20 21 22 23 24 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 9 10 11 12 13 14 15
2.474−2 3.669−2 2.428−2 3.235−2 1.087−2 2.234−3 4.105−3 5.197−3 7.761−3 2.847−3 3.807−3 4.428−3 5.527−3 1.070−1 1.291+0 1.661−2 3.796−3 6.076−2 8.494−3 7.635−2 1.090−2 8.124−2 1.169−2 9.407−4 1.178−2 2.367−3 1.565−2 3.117−3 8.727−3 2.760−3 1.017−2 3.422−3 3.096−1 2.512+0 7.903−3 9.274−3 1.316−1 3.012−2 1.543−1 3.897−2 1.505−1 1.898−3 2.487−3 2.608−2 7.127−3 3.185−2 6.049−3 1.689−2 8.191−3 1.983−2 7.760−2 3.242−3 6.198−3 6.232−3 1.185−1 1.479−2 5.245−1 2.588−2 1.058−3 1.981−3 2.441−3 2.289−2 5.587−3 8.225−2 8.886−3 2.317−2 5.168−3 4.906−3 4.246−3 1.457−2 1.489−2 1.856−1 6.583−2 7.663−1
2.606−2 4.361−2 2.891−2 4.406−2 1.041−2 2.597−3 4.792−3 5.212−3 7.804−3 3.212−3 4.296−3 4.568−3 5.708−3 1.287−1 1.318+0 5.562−2 7.724−3 6.065−2 1.217−2 8.022−2 1.711−2 8.284−2 1.976−2 1.355−3 1.076−2 2.305−3 1.696−2 3.310−3 9.003−3 2.937−3 1.050−2 3.452−3 3.535−1 2.556+0 1.796−2 1.257−2 1.496−1 3.668−2 1.865−1 5.011−2 1.747−1 2.683−3 2.466−3 2.396−2 7.641−3 3.447−2 6.374−3 1.756−2 8.367−3 2.045−2 2.210−1 8.446−3 1.406−2 1.537−2 1.276−1 2.963−2 5.308−1 4.683−2 1.511−3 2.511−3 2.796−3 2.238−2 5.774−3 8.467−2 9.066−3 2.307−2 5.010−3 1.458−2 1.080−2 3.676−2 2.806−2 2.299−1 8.959−2 8.500−1
2.668−2 4.355−2 2.796−2 4.165−2 1.051−2 2.824−3 5.223−3 5.356−3 8.024−3 3.062−3 4.096−3 4.476−3 5.593−3 1.243−1 1.391+0 5.008−2 6.874−3 6.047−2 1.123−2 8.626−2 1.531−2 8.517−2 1.714−2 1.275−3 1.085−2 2.262−3 1.813−2 3.118−3 9.108−3 2.669−3 1.078−2 3.192−3 3.646−1 2.694+0 1.579−2 1.168−2 1.458−1 3.611−2 1.925−1 4.741−2 1.739−1 2.565−3 2.411−3 2.413−2 7.641−3 3.650−2 6.048−3 1.752−2 8.106−3 2.077−2 1.977−1 6.841−3 1.191−2 1.258−2 1.250−1 2.461−2 5.571−1 3.889−2 1.325−3 2.323−3 2.513−3 2.216−2 5.173−3 8.782−2 7.999−3 2.413−2 4.423−3 1.164−2 8.677−3 3.087−2 2.339−2 2.194−1 8.287−2 8.689−1
2.779−2 4.416−2 2.718−2 3.945−2 1.067−2 3.188−3 5.910−3 5.559−3 8.331−3 2.907−3 3.890−3 4.407−3 5.506−3 1.182−1 1.497+0 4.226−2 6.565−3 6.055−2 1.054−2 9.574−2 1.369−2 8.887−2 1.479−2 1.259−3 1.099−2 2.234−3 1.983−2 2.913−3 9.277−3 2.385−3 1.116−2 2.922−3 3.839−1 2.917+0 1.489−2 1.111−2 1.423−1 3.654−2 2.050−1 4.543−2 1.755−1 2.571−3 2.378−3 2.439−2 7.738−3 3.951−2 5.720−3 1.758−2 7.864−3 2.123−2 1.651−1 5.620−3 1.043−2 1.022−2 1.230−1 2.005−2 5.973−1 3.165−2 1.172−3 2.175−3 2.226−3 2.198−2 4.527−3 9.239−2 6.855−3 2.571−2 3.818−3 9.393−3 6.897−3 2.615−2 1.919−2 2.092−1 7.780−2 9.095−1
2.945−2 4.577−2 2.666−2 3.778−2 1.087−2 3.730−3 6.939−3 5.827−3 8.735−3 2.764−3 3.700−3 4.378−3 5.471−3 1.120−1 1.635+0 3.452−2 6.816−3 6.096−2 1.020−2 1.099−1 1.241−2 9.400−2 1.294−2 1.310−3 1.115−2 2.228−3 2.222−2 2.713−3 9.522−3 2.111−3 1.161−2 2.668−3 4.120−1 3.213+0 1.531−2 1.091−2 1.401−1 3.832−2 2.272−1 4.448−2 1.804−1 2.715−3 2.373−3 2.473−2 7.987−3 4.381−2 5.428−3 1.778−2 7.670−3 2.183−2 1.322−1 4.748−3 9.603−3 8.392−3 1.218−1 1.630−2 6.555−1 2.559−2 1.048−3 2.078−3 1.957−3 2.186−2 3.892−3 9.876−2 5.730−3 2.790−2 3.253−3 7.787−3 5.503−3 2.291−2 1.575−2 2.013−1 7.529−2 9.794−1
3.159−2 4.831−2 2.639−2 3.669−2 1.109−2 4.493−3 8.389−3 6.156−3 9.229−3 2.650−3 3.546−3 4.404−3 5.503−3 1.067−1 1.792+0 2.813−2 7.634−3 6.164−2 1.019−2 1.296−1 1.147−2 1.004−1 1.161−2 1.436−3 1.132−2 2.251−3 2.546−2 2.536−3 9.840−3 1.873−3 1.209−2 2.450−3 4.456−1 3.547+0 1.705−2 1.104−2 1.394−1 4.162−2 2.611−1 4.456−2 1.884−1 3.013−3 2.400−3 2.513−2 8.438−3 4.968−2 5.203−3 1.813−2 7.538−3 2.252−2 1.043−1 4.167−3 9.408−3 7.091−3 1.214−1 1.343−2 7.347−1 2.083−2 9.534−4 2.042−3 1.726−3 2.180−2 3.320−3 1.073−1 4.714−3 3.067−2 2.772−3 6.712−3 4.462−3 2.118−2 1.311−2 1.962−1 7.573−2 1.084+0
3.405−2 5.153−2 2.633−2 3.610−2 1.133−2 5.506−3 1.032−2 6.530−3 9.790−3 2.571−3 3.441−3 4.483−3 5.602−3 1.025−1 1.959+0 2.344−2 9.012−3 6.248−2 1.044−2 1.553−1 1.082−2 1.074−1 1.075−2 1.640−3 1.151−2 2.302−3 2.965−2 2.392−3 1.021−2 1.684−3 1.257−2 2.279−3 4.816−1 3.891+0 2.008−2 1.142−2 1.400−1 4.650−2 3.075−1 4.545−2 1.987−1 3.475−3 2.458−3 2.557−2 9.126−3 5.732−2 5.058−3 1.861−2 7.467−3 2.322−2 8.275−2 3.812−3 9.781−3 6.244−3 1.217−1 1.135−2 8.367−1 1.727−2 8.865−4 2.073−3 1.547−3 2.181−2 2.844−3 1.183−1 3.868−3 3.389−2 2.397−3 6.042−3 3.713−3 2.080−2 1.120−2 1.932−1 7.918−2 1.224+0
3.640−2 5.470−2 2.629−2 3.570−2 1.150−2 6.700−3 1.259−2 6.878−3 1.031−2 2.516−3 3.368−3 4.579−3 5.722−3 9.896−2 2.113+0 2.023−2 1.080−2 6.306−2 1.079−2 1.853−1 1.035−2 1.139−1 1.020−2 1.901−3 1.162−2 2.363−3 3.444−2 2.275−3 1.055−2 1.542−3 1.293−2 2.146−3 5.147−1 4.202+0 2.406−2 1.188−2 1.406−1 5.246−2 3.625−1 4.659−2 2.086−1 4.060−3 2.525−3 2.589−2 9.976−3 6.612−2 4.962−3 1.905−2 7.406−3 2.374−2 6.703−2 3.602−3 1.056−2 5.733−3 1.217−1 9.893−3 9.531−1 1.470−2 8.406−4 2.156−3 1.415−3 2.177−2 2.469−3 1.307−1 3.204−3 3.708−2 2.120−3 5.638−3 3.184−3 2.141−2 9.852−3 1.910−1 8.482−2 1.387+0
3.733−2 5.587−2 2.560−2 3.455−2 1.130−2 7.673−3 1.445−2 6.971−3 1.045−2 2.419−3 3.237−3 4.546−3 5.681−3 9.391−2 2.187+0 1.781−2 1.233−2 6.175−2 1.085−2 2.093−1 9.780−3 1.160−1 9.627−3 2.113−3 1.137−2 2.356−3 3.808−2 2.133−3 1.052−2 1.408−3 1.281−2 2.000−3 5.285−1 4.346+0 2.749−2 1.199−2 1.374−1 5.696−2 4.064−1 4.643−2 2.111−1 4.535−3 2.519−3 2.539−2 1.056−2 7.273−2 4.778−3 1.890−2 7.163−3 2.343−2 5.516−2 3.401−3 1.120−2 5.332−3 1.185−1 8.717−3 1.039+0 1.266−2 7.913−4 2.203−3 1.297−3 2.113−2 2.148−3 1.388−1 2.668−3 3.873−2 1.885−3 5.276−3 2.765−3 2.196−2 8.747−3 1.845−1 8.889−2 1.508+0
4.007−2 5.950−2 2.664−2 3.551−2 1.240−2 8.621−3 1.622−2 7.386−3 1.105−2 2.420−3 3.231−3 4.850−3 6.053−3 9.634−2 2.359+0 1.446−2 1.384−2 6.633−2 1.179−2 2.317−1 1.006−2 1.240−1 9.673−3 2.378−3 1.295−2 2.658−3 4.133−2 2.223−3 1.087−2 1.436−3 1.359−2 2.143−3 5.672−1 4.677+0 3.055−2 1.305−2 1.463−1 6.201−2 4.457−1 4.877−2 2.235−1 5.077−3 2.833−3 2.877−2 1.134−2 7.860−2 4.914−3 1.951−2 7.625−3 2.481−2 4.255−2 3.313−3 1.163−2 5.145−3 1.235−1 8.276−3 1.129+0 1.207−2 8.249−4 2.365−3 1.367−3 2.264−2 2.239−3 1.493−1 2.791−3 4.173−2 2.062−3 5.043−3 2.552−3 2.218−2 8.447−3 1.901−1 9.448−2 1.630+0
4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 8 8 8 8 8 8 8
(continued on next page)
92
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
8 8 8 8 8 8 8 8 8 9 9 9 9 9 9 9 9 9 9 9 9 9 9 9 10 10 10 10 10 10 10 10 10 10 10 10 10 10 11 11 11 11 11 11 11 11 11 11 11 11 11 12 12 12 12 12 12 12 12 12 12 12 12 13 13 13 13 13 13 13 13 13 13 13
16 17 18 19 20 21 22 23 24 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 11 12 13 14 15 16 17 18 19 20 21 22 23 24 12 13 14 15 16 17 18 19 20 21 22 23 24 13 14 15 16 17 18 19 20 21 22 23 24 14 15 16 17 18 19 20 21 22 23 24
1.592−3 1.725−3 4.960−3 5.589−3 3.717−2 1.548−2 1.218−1 8.400−3 3.453−2 3.351+0 6.301+0 2.941−1 4.413−1 2.676−2 3.583−2 1.742−1 2.680−2 4.797−2 5.334−2 7.887−2 5.721−2 7.606−2 2.915−2 3.639−2 3.753−1 5.689+0 4.853−2 2.298−1 2.219−2 1.334−2 1.830−1 2.308−2 1.382−1 2.467−2 1.705−1 1.996−2 1.029−1 1.965−2 1.297+0 1.105+1 9.420−2 4.114−1 2.866−2 2.540−2 3.919−1 6.153−2 2.865−1 7.660−2 3.153−1 6.101−2 1.863−1 1.889−1 7.048+0 4.414−2 1.137−2 2.096−2 1.591−2 3.785−1 2.433−2 7.402−1 3.495−2 4.682−1 3.535−2 5.571−1 9.392+0 1.726−2 1.019−2 4.560−2 2.473−2 5.812−1 9.168−2 1.084+0 9.169−2 6.668−1
2.358−3 2.042−3 5.926−3 5.822−3 3.642−2 1.584−2 1.255−1 8.253−3 3.435−2 3.600+0 7.192+0 3.357−1 4.992−1 7.006−2 9.397−2 1.661−1 2.828−2 5.042−2 5.283−2 7.847−2 5.727−2 7.626−2 3.028−2 3.785−2 4.322−1 5.960+0 8.941−2 2.843−1 7.825−2 1.692−2 1.683−1 2.161−2 1.403−1 2.322−2 1.693−1 2.072−2 1.047−1 2.065−2 1.572+0 1.399+1 1.893−1 6.331−1 3.670−2 2.457−2 3.593−1 6.016−2 2.896−1 7.732−2 3.144−1 6.286−2 1.900−1 3.293−1 7.815+0 1.986−1 1.477−2 2.685−2 1.626−2 3.592−1 2.387−2 7.384−1 3.352−2 4.653−1 3.423−2 1.068+0 1.542+1 2.101−2 1.053−2 5.277−2 2.457−2 5.513−1 9.009−2 1.079+0 9.018−2 6.627−1
2.049−3 1.797−3 5.477−3 5.208−3 3.585−2 1.491−2 1.295−1 7.706−3 3.560−2 3.908+0 7.594+0 3.220−1 4.802−1 5.956−2 7.933−2 1.691−1 3.377−2 6.057−2 5.650−2 8.391−2 5.773−2 7.688−2 3.048−2 3.810−2 4.103−1 6.509+0 8.022−2 2.661−1 6.194−2 1.813−2 1.713−1 2.277−2 1.629−1 2.329−2 1.802−1 2.056−2 1.052−1 1.952−2 1.690+0 1.478+1 1.617−1 5.685−1 3.948−2 2.563−2 3.670−1 6.507−2 3.329−1 8.033−2 3.335−1 6.150−2 1.899−1 2.866−1 8.967+0 1.531−1 1.381−2 2.721−2 1.606−2 3.649−1 2.327−2 8.190−1 3.155−2 4.902−1 3.177−2 1.129+0 1.675+1 2.013−2 9.973−3 5.401−2 2.389−2 5.601−1 9.378−2 1.195+0 9.019−2 6.963−1
1.801−3 1.556−3 5.070−3 4.554−3 3.529−2 1.400−2 1.356−1 7.200−3 3.759−2 4.253+0 8.085+0 3.086−1 4.614−1 5.048−2 6.704−2 1.726−1 4.169−2 7.519−2 6.107−2 9.065−2 5.813−2 7.741−2 3.090−2 3.863−2 3.890−1 7.141+0 7.291−2 2.497−1 4.822−2 2.070−2 1.747−1 2.432−2 1.944−1 2.334−2 1.933−1 2.051−2 1.056−1 1.846−2 1.824+0 1.564+1 1.377−1 5.104−1 4.531−2 2.724−2 3.760−1 7.188−2 3.929−1 8.417−2 3.567−1 6.022−2 1.899−1 2.486−1 1.016+1 1.152−1 1.342−2 2.897−2 1.614−2 3.715−1 2.284−2 9.291−1 2.964−2 5.201−1 2.951−2 1.186+0 1.799+1 1.991−2 9.577−3 5.726−2 2.343−2 5.701−1 9.969−2 1.354+0 9.099−2 7.372−1
1.603−3 1.332−3 4.744−3 3.915−3 3.480−2 1.323−2 1.443−1 6.806−3 4.044−2 4.627+0 8.671+0 2.970−1 4.451−1 4.367−2 5.797−2 1.762−1 5.260−2 9.530−2 6.638−2 9.844−2 5.846−2 7.784−2 3.156−2 3.945−2 3.708−1 7.821+0 6.800−2 2.365−1 3.780−2 2.478−2 1.783−1 2.622−2 2.366−1 2.339−2 2.083−1 2.061−2 1.061−1 1.759−2 1.966+0 1.663+1 1.189−1 4.640−1 5.450−2 2.929−2 3.856−1 8.101−2 4.731−1 8.873−2 3.831−1 5.920−2 1.900−1 2.186−1 1.130+1 8.655−2 1.345−2 3.226−2 1.655−2 3.784−1 2.266−2 1.075+0 2.797−2 5.538−1 2.769−2 1.244+0 1.920+1 2.018−2 9.302−3 6.293−2 2.325−2 5.806−1 1.085−1 1.564+0 9.270−2 7.836−1
1.454−3 1.135−3 4.533−3 3.339−3 3.444−2 1.275−2 1.561−1 6.573−3 4.415−2 5.020+0 9.333+0 2.875−1 4.316−1 3.906−2 5.190−2 1.798−1 6.699−2 1.218−1 7.209−2 1.068−1 5.875−2 7.821−2 3.241−2 4.052−2 3.561−1 8.520+0 6.526−2 2.261−1 3.038−2 3.050−2 1.817−1 2.832−2 2.911−1 2.345−2 2.241−1 2.085−2 1.066−1 1.695−2 2.113+0 1.771+1 1.052−1 4.292−1 6.739−2 3.160−2 3.951−1 9.284−2 5.766−1 9.368−2 4.109−1 5.852−2 1.904−1 1.963−1 1.236+1 6.641−2 1.376−2 3.721−2 1.732−2 3.851−1 2.275−2 1.261+0 2.666−2 5.890−1 2.640−2 1.301+0 2.039+1 2.078−2 9.127−3 7.137−2 2.334−2 5.908−1 1.207−1 1.833+0 9.517−2 8.324−1
1.349−3 9.747−4 4.462−3 2.863−3 3.422−2 1.262−2 1.715−1 6.510−3 4.854−2 5.417+0 1.004+1 2.798−1 4.205−1 3.621−2 4.819−2 1.830−1 8.502−2 1.549−1 7.767−2 1.151−1 5.905−2 7.861−2 3.335−2 4.170−2 3.445−1 9.216+0 6.417−2 2.181−1 2.534−2 3.788−2 1.848−1 3.043−2 3.582−1 2.352−2 2.393−1 2.119−2 1.073−1 1.656−2 2.258+0 1.884+1 9.558−2 4.038−1 8.399−2 3.389−2 4.039−1 1.074−1 7.043−1 9.854−2 4.377−1 5.823−2 1.913−1 1.804−1 1.333+1 5.291−2 1.420−2 4.382−2 1.842−2 3.912−1 2.301−2 1.489+0 2.572−2 6.227−1 2.562−2 1.357+0 2.154+1 2.153−2 9.036−3 8.263−2 2.362−2 6.002−1 1.366−1 2.164+0 9.803−2 8.791−1
1.277−3 8.490−4 4.503−3 2.488−3 3.398−2 1.278−2 1.890−1 6.553−3 5.292−2 5.772+0 1.070+1 2.721−1 4.094−1 3.447−2 4.594−2 1.849−1 1.052−1 1.920−1 8.212−2 1.217−1 5.910−2 7.868−2 3.411−2 4.265−2 3.335−1 9.830+0 6.386−2 2.109−1 2.194−2 4.624−2 1.865−1 3.216−2 4.323−1 2.351−2 2.511−1 2.144−2 1.075−1 1.630−2 2.384+0 1.986+1 8.854−2 3.836−1 1.028−1 3.575−2 4.093−1 1.234−1 8.451−1 1.022−1 4.583−1 5.798−2 1.915−1 1.683−1 1.411+1 4.409−2 1.460−2 5.137−2 1.962−2 3.943−1 2.322−2 1.738+0 2.499−2 6.481−1 2.511−2 1.402+0 2.249+1 2.219−2 8.967−3 9.548−2 2.384−2 6.050−1 1.543−1 2.525+0 1.002−1 9.141−1
1.201−3 7.410−4 4.494−3 2.167−3 3.286−2 1.279−2 2.004−1 6.471−3 5.513−2 5.900+0 1.095+1 2.585−1 3.891−1 3.261−2 4.351−2 1.807−1 1.211−1 2.210−1 8.291−2 1.230−1 5.747−2 7.650−2 3.371−2 4.215−2 3.158−1 1.005+1 6.229−2 1.996−1 1.928−2 5.275−2 1.821−1 3.257−2 4.887−1 2.285−2 2.519−1 2.104−2 1.047−1 1.572−2 2.418+0 2.014+1 8.151−2 3.589−1 1.174−1 3.612−2 4.011−1 1.344−1 9.514−1 1.017−1 4.590−1 5.625−2 1.864−1 1.554−1 1.432+1 3.770−2 1.454−2 5.703−2 2.017−2 3.848−1 2.271−2 1.918+0 2.384−2 6.464−1 2.413−2 1.398+0 2.261+1 2.213−2 8.689−3 1.049−1 2.331−2 5.903−1 1.664−1 2.787+0 9.888−2 9.111−1
1.248−3 7.714−4 4.801−3 2.259−3 3.514−2 1.369−2 2.152−1 7.012−3 5.935−2 6.198+0 1.148+1 2.726−1 4.105−1 3.265−2 4.366−2 1.933−1 1.189−1 2.177−1 8.381−2 1.241−1 1.677−1 2.238−1 3.898−2 4.874−2 3.325−1 1.062+1 6.495−2 2.092−1 1.718−2 5.007−2 1.990−1 3.293−2 5.000−1 2.930−2 2.622−1 2.411−2 1.210−1 1.896−2 2.489+0 2.111+1 8.106−2 3.686−1 1.100−1 3.645−2 4.342−1 1.440−1 9.704−1 1.091−1 4.792−1 6.672−2 2.172−1 1.591−1 1.549+1 3.104−2 1.421−2 5.299−2 2.319−2 4.039−1 2.400−2 2.045+0 4.261−2 6.858−1 2.703−2 1.634+0 2.412+1 2.164−2 4.869−2 9.984−2 2.461−2 6.193−1 1.943−1 2.970+0 1.067−1 9.666−1
(continued on next page)
K.M. Aggarwal, F.P. Keenan / Atomic Data and Nuclear Data Tables (
)
–
93
Table 32 (continued) Transition
Temperature (log T e , K)
i
j
FAC
6.40
6.60
6.80
7.00
7.20
7.40
7.60
7.80
FAC
14 14 14 14 14 14 14 14 14 14 15 15 15 15 15 15 15 15 15 16 16 16 16 16 16 16 16 17 17 17 17 17 17 17 18 18 18 18 18 18 19 19 19 19 19 20 20 20 20 21 21 21 22 22 23
15 16 17 18 19 20 21 22 23 24 16 17 18 19 20 21 22 23 24 17 18 19 20 21 22 23 24 18 19 20 21 22 23 24 19 20 21 22 23 24 20 21 22 23 24 21 22 23 24 22 23 24 23 24 24
1.673−1 4.259−3 8.783−3 8.983−3 3.366−2 1.694−2 4.780−1 3.501−2 2.641+0 6.350−2 5.694−3 5.145−3 1.846−2 1.362−2 5.401−2 3.509−2 6.498−1 1.641−1 3.452+0 8.601+0 1.623+1 8.310−1 1.246+0 9.490−2 1.269−1 2.652−2 3.327−2 9.658−1 1.581+1 1.310−1 8.973−1 6.279−2 5.753−2 1.799−2 3.487+0 2.960+1 3.376−1 1.592+0 4.273−2 1.063−1 4.913−1 2.215+1 9.106−2 7.429−1 4.466−2 1.761+0 3.070+1 1.320−1 1.050+0 3.197−1 1.749+1 8.420−2 9.297−1 2.321+1 2.979−1
5.370−1 6.383−3 1.058−2 9.955−3 3.955−2 1.691−2 4.655−1 3.312−2 2.639+0 5.931−2 9.017−3 6.313−3 2.060−2 1.349−2 5.992−2 3.333−2 6.313−1 1.600−1 3.450+0 9.599+0 1.773+1 8.192−1 1.231+0 1.023−1 1.363−1 2.734−2 3.419−2 9.338−1 1.783+1 1.422−1 8.777−1 6.321−2 6.238−2 1.781−2 4.285+0 3.529+1 3.317−1 1.546+0 4.405−2 1.147−1 4.770−1 3.246+1 9.495−2 7.249−1 4.355−2 3.298+0 5.100+1 1.292−1 1.023+0 3.076−1 3.037+1 7.891−2 2.339+0 4.279+1 2.723−1
4.212−1 5.349−3 9.750−3 8.803−3 3.833−2 1.503−2 4.676−1 2.933−2 2.839+0 5.213−2 7.461−3 5.299−3 1.911−2 1.170−2 5.830−2 2.950−2 6.333−1 1.598−1 3.708+0 1.051+1 1.932+1 8.059−1 1.211+0 1.036−1 1.382−1 2.626−2 3.285−2 9.134−1 1.951+1 1.451−1 8.608−1 6.210−2 6.221−2 1.642−2 4.722+0 3.883+1 3.245−1 1.512+0 4.213−2 1.134−1 4.658−1 3.619+1 9.377−2 7.069−1 3.957−2 3.640+0 5.692+1 1.226−1 9.960−1 2.939−1 3.384+1 7.108−2 2.499+0 4.759+1 2.451−1
3.222−1 4.579−3 9.184−3 7.785−3 3.790−2 1.324−2 4.704−1 2.568−2 3.109+0 4.516−2 6.320−3 4.439−3 1.793−2 9.996−3 5.749−2 2.583−2 6.361−1 1.626−1 4.058+0 1.150+1 2.108+1 7.914−1 1.190+0 1.053−1 1.405−1 2.528−2 3.163−2 8.916−1 2.133+1 1.484−1 8.432−1 6.110−2 6.228−2 1.517−2 5.179+0 4.259+1 3.172−1 1.477+0 4.048−2 1.126−1 4.542−1 3.998+1 9.312−2 6.884−1 3.590−2 3.979+0 6.287+1 1.163−1 9.680−1 2.806−1 3.733+1 6.399−2 2.655+0 5.237+1 2.192−1
2.454−1 4.016−3 8.839−3 6.948−3 3.842−2 1.171−2 4.737−1 2.250−2 3.463+0 3.902−2 5.497−3 3.742−3 1.709−2 8.498−3 5.791−2 2.265−2 6.396−1 1.694−1 4.517+0 1.252+1 2.295+1 7.764−1 1.168+0 1.073−1 1.432−1 2.450−2 3.066−2 8.688−1 2.321+1 1.522−1 8.254−1 6.030−2 6.265−2 1.419−2 5.633+0 4.638+1 3.098−1 1.440+0 3.927−2 1.124−1 4.429−1 4.364+1 9.315−2 6.700−1 3.285−2 4.295+0 6.852+1 1.107−1 9.408−1 2.685−1 4.062+1 5.829−2 2.798+0 5.685+1 1.969−1
1.896−1 3.621−3 8.674−3 6.314−3 4.004−2 1.055−2 4.772−1 1.998−2 3.914+0 3.409−2 4.923−3 3.209−3 1.658−2 7.288−3 5.989−2 2.013−2 6.435−1 1.813−1 5.104+0 1.355+1 2.488+1 7.609−1 1.145+0 1.096−1 1.464−1 2.393−2 2.995−2 8.450−1 2.510+1 1.564−1 8.076−1 5.974−2 6.331−2 1.352−2 6.070+0 5.009+1 3.025−1 1.402+0 3.855−2 1.129−1 4.317−1 4.705+1 9.387−2 6.516−1 3.055−2 4.580+0 7.372+1 1.060−1 9.140−1 2.579−1 4.363+1 5.419−2 2.925+0 6.091+1 1.788−1
1.505−1 3.359−3 8.637−3 5.869−3 4.272−2 9.769−3 4.805−1 1.813−2 4.464+0 3.042−2 4.544−3 2.825−3 1.633−2 6.380−3 6.345−2 1.828−2 6.474−1 1.984−1 5.822+0 1.456+1 2.681+1 7.454−1 1.122+0 1.122−1 1.499−1 2.357−2 2.951−2 8.194−1 2.694+1 1.608−1 7.901−1 5.941−2 6.424−2 1.311−2 6.484+0 5.365+1 2.950−1 1.361+0 3.822−2 1.138−1 4.203−1 5.017+1 9.505−2 6.325−1 2.891−2 4.832+0 7.841+1 1.020−1 8.867−1 2.485−1 4.633+1 5.153−2 3.036+0 6.453+1 1.647−1
1.236−1 3.184−3 8.639−3 5.553−3 4.599−2 9.273−3 4.808−1 1.677−2 5.060+0 2.777−2 4.293−3 2.554−3 1.619−2 5.717−3 6.791−2 1.691−2 6.474−1 2.186−1 6.602+0 1.543+1 2.851+1 7.304−1 1.100+0 1.146−1 1.531−1 2.327−2 2.914−2 7.898−1 2.853+1 1.649−1 7.717−1 5.901−2 6.506−2 1.285−2 6.823+0 5.664+1 2.856−1 1.311+0 3.794−2 1.142−1 4.065−1 5.267+1 9.585−2 6.094−1 2.767−2 5.023+0 8.210+1 9.788−2 8.542−1 2.388−1 4.844+1 4.970−2 3.114+0 6.731+1 1.532−1
1.033−1 2.997−3 8.440−3 5.205−3 4.789−2 8.758−3 4.666−1 1.541−2 5.464+0 2.535−2 4.031−3 2.318−3 1.570−2 5.138−3 7.043−2 1.555−2 6.280−1 2.318−1 7.132+0 1.568+1 2.905+1 7.050−1 1.065+0 1.138−1 1.520−1 2.246−2 2.813−2 7.447−1 2.896+1 1.645−1 7.396−1 5.715−2 6.410−2 1.238−2 6.886+0 5.733+1 2.688−1 1.230+0 3.664−2 1.110−1 3.824−1 5.304+1 9.362−2 5.708−1 2.606−2 5.017+0 8.249+1 9.166−2 8.003−1 2.237−1 4.860+1 4.719−2 3.078+0 6.741+1 1.406−1
8.832−2 3.240−3 8.651−3 5.755−3 4.778−2 2.502−2 4.876−1 1.720−2 5.853+0 2.854−2 4.334−3 2.668−3 1.641−2 6.419−3 1.559−1 1.735−2 6.567−1 2.473−1 7.616+0 1.605+1 2.805+1 6.842−1 1.029+0 1.638−1 2.214−1 2.791−2 3.510−2 7.621−1 3.034+1 1.897−1 7.321−1 6.273−2 7.404−2 1.389−2 6.337+0 5.131+1 3.014−1 1.301+0 5.138−2 1.635−1 4.254−1 5.073+1 1.044−1 6.080−1 2.919−2 4.791+0 8.519+1 9.980−2 8.565−1 2.438−1 4.707+1 6.691−2 2.797+0 6.879+1 1.572−1