Contribution of outer atomic shells to total internalconversion coefficients

N U C L E A R DATA

TABLES

CONTRIBUTION

A9, 119-135 (1971)

OF OUTER ATOMIC SHELLS TO TOTAL INTERNAL CONVERSION

COEFFICIENTS

O. D R A G O U N ~uclear Research Institute, l~e~ near Prague, Czechoslovakia Z. PLAJNEt~,* Max-Planck-Institut fiar Kernphysik, Heidelberg, Germany and F. S C H M U T Z L E R t Institut ffir theoretische Physik der Universitfit, Heidelberg, Germany

The sums of approximate internal conversion coefficients for the (N + O + - - - ) shells are presented. All values of atomic number from Z = 37 to Z = 100 are treated. The conversion coefficients are tabulated for the El . . . . . E4, MI . . . . , M4 multipolarities and for transition energies from 50 to 500 keV. Internal-conversion-coefficient ratios ( N + 0 -I- 9 . . ) / ( K + L + ?,1) a n d ( N + O + - . . ) / M are given for atomic numbers Z = 40, 50 . . . . . 100.

*On leave, now at ihe Nuclear Research Institute, I~e~. near Prague, Czechoslovakia tPresent address: Max-Planck-lnstitut for Kernphysik, Heidelberg, Germany 119

DRAGOUN, PLAJNER, AND SCHMUTZLER

CONTENTS

INTRODUCTION Description of Calculations Comparison with Earlier Calculations Results and Conclusion TABLE I.

Comparison of Approximate ICC with Values of Anderson et al. for Z = 50

TABLE II.

Comparison of Approximate ICC with Values of I-lager and Seltzer for Z = 30

TABLEIII.

(N+ O + . . . ) / ( K + L + 3 0

TABLE IV.

(N + O + . . . ) / M

TABLE V.

Approximate Internal Conversion Coefficients for (N + O + . . . ) Shell Electrons

X 100

INTRODUCTION

number 37 <: Z_< 100, for the four lowest electric and magnetic multipoles, and for six values of the transition energy ranging from 50 to 500 keV. Most o f the NI-, . . . , Ns-subshell ICC for 60 < Z ~ 100 were taken from the previous tabulationP These calculations were performed with the program MONICA of Pauli, ix adapted for the CDC 3300 computer. Screening was taken into account by means of nonrelativistic Hartree-Fock-Slatei" screening functions, lz The same method was used to supply the K-, L-, and M-subshell ICC for the ratios, (N + 0 + . . . ) / 3 1 and (N + 0 + . . . ) / ( K + L + M), of this work. All remaining subshell ICC were computed with the code AICC.* The approximate conversion coefficient aap p was expressed in the form

Extensive tablesXr s of internal conversion coefficients (ICC) are now available for the atomic subshells, K, Lx_a, Mx_ 5, and N~_5. The ICC were calculated with the electron wavefunctions obtained by numerical solution of the Dirac equation for a spherically symmetric potential. Recently, a simple method 6 to obtain the approximate ICC for outer atomic shells was suggested: coefficients for a point nucleus, unscreened, were computed according to the fornmlas o f O'Connell and Carroll r and then were corrected for finite nuclear size and atomic screening. The values calculated in this way were found to be in surprising agreement with experiment, s,9 This fact stimulated the extensive tabulation ~~of the approximate ICC for the subshells, N6_7, O~_7, P~-5, and Ql. Together with the existing tables o f the K-, L-, M-, and N-shell ICC, the outer shell coefficients 1~ can now be used to obtain values of the total ICC. Since internal conversion lines corresponding to individual outer atomic subshells are usually not resolved in the contemporary spectrometer measurements, we present in this work the sums of approximate ICC for the (N + O + - - . ) atomic shells. In addition, conversion-coefficient ratios, (N + 0 + . . . ) / ( K + L + 31) and (N + 0 + ...)/M, are given for the atomic numbers Z = 40, 50, . . . , 100. These ratios make it possible to estimate easily the relative contribution of outer shells to the total conversion coefficient.

' % p = '~o'A,,'Lcr'Lcc,

(1)

where a o is the point nucleus-unscreened ICC and where ffn, fscr, and focc are, respectively, the correction factors for finite nuclear size, atomic screening, and fraction of total occupancy in the partially occupied subshell. The finite-nuclear-size correctionffn was calculated according to the simplified formulas of O'Connell and Carroll. 7 Therefore, the contribution of the intranuclear conversion, which is usually very small, was neglected. The screening correctionfscr , defined as the ratio of the *The computer program AICC computes the internal conversion coefficients for point and finite nuclei without atomic screening. Details of the calculations as well as the complete listings of the G I E R - A L G O L and F O R T R A N versions of the program can be found in Ref. 13. The program was tested successfully for all atomic subshells ( K . . . Qa), atomic numbers Z < 100, for electric and magnetic multipoles with 1 .< L < 5, and for transition energies higher than the electron binding energy in the pure Coulomb field up to 17 MeV.

Description of Calculations Internal conversion coefficients ~(N + O + . . . ) tabulated in this paper are the sums of the ICC of all atomic subshells higher than 315 which are at least partially occupied in the free-atom electron configuration. Calculations were performed for every value of atomic

120

INTERNAL CONVERSION IN OUTER SIIELLS

02 subshell ICC for several dipole and quadrupole t r a n sitions in 119DoSn. In TABLE I, our approximate values are compared with those which are based on the relativistic atomic model. Except for the low-energy E2 transitions, both sets of the conversion coefficients for the valence-shell electrons are in very good agreement. The ICC for the subshells, 3tl-315, calculated for Z = 30 according to Eq. (1), may be compared with the precise values of Hager and Seltzer, 15 to provide a further check of the present conversion coefficients since the M-shell electrons are the outer ones in this element. For different multipolarities and transition energies 88 pairs of the ICC were compared (see TABLE II). The mean-square deviation was found to be 8.5%. The largest deviation (27%) appears for the Ms-subshell and M4-multipolarity. For transitions involving small changes of angular momentum (L = I, 2 and sl/2, Pa/z bound electrons), both calculations agree within 5%. The alcove analysis led us to start the ICC tabulation at the transition energy of 50 keV.

screened and unscreened bound-electron densities at the nuclear vicinity, was derived from the tables of Herman and SkillmanJ 2 As a rule the values of the f~cr were computed for the smallest electron coordinate given in Ref. 12. This coordinate is equal to about 27 nuclear radii for Z = 37 and 13 nuclear radii for Z = 100. The density ratios for larger distances yielded practically the same screening factors. The wavefimctions of electrons with higher angular momentum had to be compared at larger coordinates since at small radii they are not tabulated precisely enough. For calculating the correction factorfo~ it was assumed that the conversion coefficient of the partially occupied subshell is proportional to the number of electrons involved in the subshell considered. In order to examine the consistency of the two methods employed in this work, the NI-, . . . . Ns-subshell ICC were computed in both ways for Z = 60, 80, and 94, for El . . . . . E4, add 311 . . . . . 3/!,14 multipolarities, and for transition energies of 50, 100, and 200 keV. In all 360 investigated cases, the ratios aapp/aMosmA of the corresponding ICC did not deviate from unity by more than - 2 4 % and +26%. Distribution of the deviations (a~pp/aMONlea -- 1) • 100 is shown in Fig. 1. It can be seen from Fig. 2 that large deviations occur mainly at the smaller transition energies.

Results and Conchtsion In TABLE III, the internal-conversion-coefficient ratio (N + 0 + . . . ) / ( K + L + 3t) is given for every tenth value of atomic number from Z = 40 to Z = 100. For transition energies exceeding the K-shell threshold, contribution of the (N + O + 9 9 .) shell electrons to the total ICC is often very small and does not reach 13%. The conversion-coefficient ratio, (N + O + .- . ) /

Comparison with Earlier Calculations Anderson et al? 4 calculated recently the Ox and

I I

I

I

I

I

I

I

I

I

I

15 -

I

I/

k=200keV

30

(/I (J tl. 0

20

0

t

n

I

~'

m 15

I

I

t

<: (J

I

k=100 keY

'rn" 10 :E

Z 2:0

D

'"

I -30

-20

I -10

I

I

0

10

1 2O

I

[

30

[

I

I

I

!

I

0

10

t

I

J

DEVIATION (%)

Fig 1. Distribution of deviations (aapp/aMOSleA - 1) • 100. The comparison was performed in 360 cases for N a to N s subshells, for E l , . . . , E4, M I , . . . , 314 multipolarities, for the transition energies of 50, 100, and 200 keV, and for Z = 60, 80, and 94. aapp and a~omeA are the approximate and more accurate values determined according to Eq. (1) and the Pauli H program respectively

o

[] I

-30

I -20

-10

IIII = I

I

20

30

DEVIATION (%)

Fig. 2. Distribution of deviations (Otapp/O:MONiCA-I) • 100 for transition energies of 50, 100, and 200 keV. See caption to Fig. 1

121

DRAGOUN,

PLAJNER,

AND

31, presented in TABLE IV is found to be an increasing function of atomic number almost independent of the transition energy and multipolarity. For all atomic numbers considered in TABLE IV the maximum and minimum values of the ratio ( N + 0 + . . . ) / 3 f define a rather narrow band (Fig. 3). Also plotted there are boundelectron density ratios, 4,2(N + O + ...)/~Z(M), calculated at the nuclear vicinity. Here 4,2 is the sum over the indicated subshells of one-electron densities 12 which is multiplied by the occupation numbers corresponding to free-atom electron configuration. It is interesting to see that the density ratios lie within the mentioned band for a(N + O + --.)/a(M). This fact emphasizes once more the importance of the quantity +2 for the internal conversion process. The values of TABLE IV are in agreement with the empirical rule a(N + O + 9 9.) ~ (0.26 -4- 0.04) a(M) proposed by Bogdanovic et al. xB for E2 transitions and the energy ihterval 80 to 600 keV in atomic nuclei with Z = 58 to 78. In TABLE V, sums of the approximate ICC for the (N + O + 99.) atomic shells are tabulated for every Z-value from Z = 37 to Z = 100. Taking into account the arguments discussed above and in Ref. 5 as well as the agreement of approximate ICC for outer atomic shells with experiment,s,9 we believe the (N + O + . . . ) coefficients of this work to be accurate within __+15%. Therefore, the use of the present a(N + O + ---) in calculating the total conversion coefficient should not introduce an error larger than about 3%.

SCttMUTZLER

Acknowledgment

The authors wish to express their gratitude to Professor W. Gentner for the opportunity to perform extensive calculations of this work in the Max-Plancklnstitut fiir Kernphysik.

References I. L. A. Sliv and I. M. Band, Alpha-, Beta- and GammaR a y Spectroscopy, p. 1639 (K. Siegbahn, ed.) North-

Holland, Amsterdam (1965) . M. E. Rose, Internal Conversion Coefficients, North-

Holland, Amsterdam (1958) . H. C. Pauli, "Tables of Internal Conversion Coeffi-

cients and Particle Parameters," Purdue University, Report COO-1420-137 (1967) . R. S. Hager and E. C. Seltzer, Nucl. Data A4, 1

(1968) . O. Dragoun, H. C. Pauli, and F. Schmutzler, Nucl.

Data A6, 235 (1969) o

7. R. F. O'Connell and C. O. Carroll, Phys. Rev. 138B, 1042 (1965) .

i

i

i

I

I

I

O. Dragoun et al., Phys. Letters 28B, 251 (1968)

O. Dragoun et al., Max-Planck-Institut fiJr Kernphysik, Report MPIH, VI1, Heidelberg, Germany (1968)

. O. Dragoun, Z. PIajner, and F. Schmutzler, Proc. Intern. Conf. Radioactivity in Nucl. Spectrosc., Vanderbilt University, Nashville, Tenn. (Aug. 1969); Czech. J. Phys. B20, 375 (1970)

I

O.S

(N+O+_) H 0.4

I0. O. Dragoun, Z. Plajner, and F. Schmutzler, MaxPlanck-Institut fiir Kernphysik, Report MPIH, V5, Heidelberg, Germany (1969) 0.2

I

I

I

I

I

I

I

~o

so

60

70

8o

90

~oo

11. It. C. Pauli, Computer Program for Internal Conversion Coefficients and Particle Parameters, The Niels Bohr Institute Report, University of Copenhagen, Denmark (1968)

ATOHIC NUMBER Z

12. F. Herman and S. Skillman, Atomic Structure Calculations, Prentice-Hall, Englewood Cliffs, N.J. (1963)

Fig. 3. Internal-conversion-coefficient ratios, (N + O + -..)/3t, versus atomic number. Full lines define band containing all ratios from TABLE IV. The points represent the bound-electron density ratios, ~2(N-tO + . . - ) / ~ 2 ( M ) . Open circle indicates the empirical ICC ratio 16 derived for E2 transitions

13. N. Dragounov,4, O. Dragoun, and G. Heuser, MaxPlanck-Institut for Kernphysik, Report MPIH, V9, Heidelberg, Germany (1969)

122

INTERNAL CONVERSION IN OUTER SHELLS

of Technology, Report CALT-63-60, Pasadena, i Calif. (1967)

14. E. M. Anderson, M. A. Listengartcn, and M. A. Khakonkind, Izv. Akad. Nauk SSSR, Ser. Fiz. 34, 850 (1970)

16. M. Bogdanovic, M. Mladjenovic, and R. Stepic, Nucl. Phys. A106, 209 (1968)

15. R. S. Hager and E. C. Seltzer, California Institute

123

DRAGOUN, PLAJNER, AND SCHMUTZLER

TABLE I. Comparison o f Approximate ICC with the Values of Anderson et al. for Z = 50

O~app/t~And O2-Subshell

Transition Energy (me 2)

Oa-Subshell E1

E2

M1

M2

MI

M2

0.03 0.04 0.05 0.I0" 0.20* 0.30"

1.12 1.10 1.10 1.09 1.09 1.10

1.97 1.43 1.23 1.08 1.08 1.09

1.12 1.12 1.13 1.12 !.12 1.12

1.28 1.27 1.25 1.21 1.17 1.16

0.91 0.91 0.92 0.93 0.94 0.95

1.05 1.02 1.00 0.97 0.96 0.96

a,pp Approximate internal conversion coefficients calculated according to Eq. (I) aA,ad Coefficients of Anderson et al. 14 based on the relativistic Hartree-Fock-Slater atomic model *

Energy region of,the main a (N + O + . . . ) table

TABLE II. Comparison of Approximate ICC with the Values of Hager and Seltzer for Z = 30 ( . a p p / a n s - I) X 100 Atomic

Transition

Transition .Multipolarity

Subshell

Energy (me z)

El

E2

E3

E4

MI

311

40.14 70.14 150.14

--2 -- 1 0

--3 - 1 --I

--5 --3 -1

-8 -5 --2

Mz

40.09 70.09 150.09

-- I I 2

2 3 4

4 4 5

Ma

40.09 70.09 150.09

0 2 5

4 5 5

M4

40.01

7

315

40.01

12

M2

M3

M4

2 1 1

5 4 2

10 6 4

14 9 5

6 5 5

3 3 4

4 5 5

6 5 5

7 6 5

6 6 6

7 8 7

3 5 5

7 7 7

11 I0 9

16 13 10

8

14

18

9

17

16

20

9

16

19

14

12

15

27

Otap p Approximate internal conversion coefficients calculated according to Eq. (I)

arts Coefficients of Hager and Seltzer ~5 based on the relativistic Hartree-Fock-Slater atomic model

124

INTERNAL CONVERSION IN OUTER StlELLS

TABLE Ill. (N + O + . . . ) / ( K + L + 31) • 100

Atomic

~ansition

Number Energy(keV)

~ansition Multipolarity El

E2

E3

E4

MI

M2

M3

M4

40

50 70 100 150 200 500

0.3 0.3 0.3 0.3 0.3 0.3

0.6 0.5 0.4 0.4 0.3 0.3

1.4 1.0 0.8 0.5 0.5 0.3

2.0 1.6 1.2 0.9 0.7 0.4

0.3 0.3 0.3 0.3 0.3 0.3

0.5 0.5 0.4 0.4 0.4 0.3

1.0 0.7 0.6 0.5 0.4 0.4

1.6 1.2 0.9 0.6 0.6 0.4

50

50 70 100 150 200 500

0.5 0.5 0.5 0.5 0.5 0.5

1.8 1.3 0.9 0.7 0.6 0.5

3.3 2.8 2.1 1.4 1.1 0.6

4.0 3.6 3.0 2.3 1.8 0.8

0.5 0.5 0.5 0.5 0.5 0.5

0.9 0.8 0.7 0.6 0.6 0.5

2.3 1.7 1.3 1.0 0.8 0.6

4.1 3.0 2.1 1.4 1.1 0.7

60

50 70 100 150 200 500

0.8 0.7 0.7 0.7 0.7 0.6

4.0 3.0 2.2 1.5 1.2 0.8

5.2 4.8 4.2 3.2 2.5 1.1

6.0 5.5 5.1 4.4 3.7 1.6

0.7 0.7 0.7 0.7 0.7 0.7

1.6 1.3 1.2 1.0 0.9 0.8

4.5 3.2 2.4 1.7 1.4 0.9

6.4 5.2 4.0 2.7 2.1 1.1

70

50 70 100 150 200 500

4.9 0.9 0.9 0.8 0.8 0.8

5.2 4.5 3.6 2.5 2.0 1.1

5.8 5.6 5.4 4.5 3.8 1.7

7.4 6.6 6.2 5.5 5.0 2.4

5.1 0.8 0.8 0.8 0.8 0.8

5.7 1.8 1.5 1.3 1.2 0.9

6.3 5.0 3.6 2.6 2.0 1.2

7.6 6.9 5.8 4.4 3.1 1.5

80

50 70 100 150 200 500

5.6 5.6 1.1 1.1 1.0 1.0

6.2 6.1 5.5 4.3 3.5 1.6

7.3 6.9 6.8 6.2 5.6 2.7

11 8.9 8.0 7.2 6.6 3.8

5.9 5.9 1.0 1.0 1.0 1.0

6.7 6.6 2.2 1.8 1.6 1.2

7.8 7.5 5.8 4.0 3.1 1.7

10 9.1 8.3 6.4 5.0 2.3

90

50 70 100 150 200 500

6.6 6.6 6.7 1.4 1.4 1.2

7.5 7.5 7.6 6.6 5.7 2.6

9.5 8.9 8.5 8.1 7.6 4.3

16 13 11 9.3 8.7 5.6

6.8 6.8 6.9 1.3 1.3 1.3

8.1 7.9 7.9 2.7 2.3 1.7

9.8 9.5 9.2 6.3 4.9 2.4

14 12 11 9.5 7.8 3.5

100

50 70 100 150 200 500

7.1 7. I 7.2 1.8 1.7 1.5

8.4 8.4 8.5 8.2 7.5 3.9

12 11 9.9 9.3 8.9 5.8

24 18 14 11 I0 7.2

7.4 7.4 7.4 1.6 1.6 1.6

9.1 8.9 8.7 3.7 3.2 2.2

11 11 11 9.0 7.1 3.3

17 15 14 12 10 4.9

125

DRAGOUN, PLAJNER, AND SCHMUTZLER

TABLE IV. (N + 0 + . . . ) / M

Atomic

Transition

Number Energy (keV)

Transition Multipolarity El

E2

E3

E4

MI

M2

M3

M4

40

50 70 100 150 200 500

0.16 0.16 0.16 0.17 0.17 0.17

0.14 0.15 0.15 0.16 0.16 0.17

0.14 0.14 0.14 0.15 0.15 0.17

0.14 0.14 0.14 0.14 0.15 0.16

0.17 0.17 0.17 0.17 0.17 0.18

0.17 0.18 0.17 0.17 0.18 0.18

0.17 0.17 0.17 0.17 0.17 0.18

0.17 0.17 0.17 0.17 0.17 0.17

50

50 70 100 150 200 500

0.20 0.21 0.21 0.21 0.22 0.22

0.19 0.20 0.20 0.20 0.21 0.22

0.20 0.20 0.20 0.20 0.20 0.21

0.21 0.20 0.20 0.20 0.20 0.21

0.22 0.22 0.22 0.22 0.22 0.22

0.23 0.23 0.22 0.22 0.22 0.22

0.23 0.23 0.23 0.23 0.23 0.22

0.24 0.24 0.23 0.23 0.23 0.22

60

50 70 100 150 200 500

0.26 0.26 0.27 0.27 0.27 0.27

0.26 0.25 0.26 0.26 0.26 0.26

0.26 0.26 0.26 0.26 0.26 0.26

0.26 0.26 0.26 0.26 0.26 0.26

0.27 0.27 0.28 0.28 0.27 0.27

0.28 0.27 0.28 0.28 0.27 0.27

0.27 0.27 0.28 0.27 0.27 0.27

0.28 0.27 0.28 0.27 0.27 0.28

70

50 70 100 150 200 500

0.26 0.27 0.27 0.26 0.27 0.28

0.26 0.26 0.26 0.25 0.26 0.27

0.27 0.26 0.27 0.26 0.26 0.27

0.27 0.27 0.27 0.27 0.27 0.27

0.28 0.28 0.28 0.26 0.28 0.28

0.28 0.28 0.28 0.27 0.28 0.28

0.28 0.28 0.28 0.29 0.28 0.28

0.29 0.28 0.28 0.30 0.28 0.28

80

50 70 100 150 200 500

0.29 0.29 0.30 0.30 0.30 0.31

0.30 0.29 0.30 0.30 0.30 0.30

0.31 0.30 0.30 0.30 0.30 0.30

0.32 0.31 0.31 0.31 0.30 0.30

0.31 0.31 0.31 0.31 0.31 0.31

0.32 0.31 0.32 0.31 0.31 0.31

0.32 0.32 0.32 0.32 0.31 0.31

0.34 0.33 0.33 0.32 0.32 0.31

90

50 70 100 150 200 500

0.33 0.33 0.34 0.34 0.34 0.34

0.35 0.35 0.35 0.35 0.35 0.35

0.37 0.36 0.36 0.35 0.35 0.35

0.40 0.38 0.37 0.36 0.36 0.35

0.35 0.35 0.35 0.35 0.35 0.35

0.36 0.36 0.36 0.36 0.36 0.35

0.38 0.38 0.37 0.37 0.37 0.36

0.41 0.40 0.39 0.38 0.38 0.36

100

50 70 100 150 200 500

0.34 0.35 0.35 0.36 0.36 0.36

0.37 0.37 0.37 0.37 0.37 0.37

0.40 0.40 0.39 0.38 0.38 0.37

0.47 0.45 0.42 0.40 0.39 0.38

0.37 0.37 0.37 0.37 0.37 0.37

0.39 0.39 0.38 0.38 0.38 0.37

0.41 0.41 0.40 0.40 0.39 0.38

0.46 0.45 0.44 0.42 0.41 0.39

126

INTERNAL CONVERSION IN OUTER SttELLS

TABLE V. Approximate Internal Conversion Coefficients for (N + O + . 9 .) Shell Electrons Conversion coefficients presented are sums over all atomic subshells higher than the ?,15 which are at least partially occupied in the free-atom electron configuration. The calculations were performed for the El . . . . . E4, MI . . . . . ?'t4 multipolarities, for transition energies from 50 to 500 keV, and for all atomic numbers in the interval 37 < Z < 100. K El . . . . .

Nuclear transition energy in keV M4

1.23 E-04

Multipolarities o f nuclear transitions 1.23 X 10 -4

127

DRAGOUN, PLAJNER, AND SCIlMUTZLER

(N+O+,.=)

- SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

H4

37

50 70 100 150 200 500

1.58E-03 5,96E-04 2.10E-04 6.39E-05 2.77E-05 2.34E-06

4.80E-02 1.16E-02 2.72E-03 5.56E-04 1~ 7.94E-06

2 . 0 5 E O0 2.99E-01 4.23E-02 5.17E-03 1.27E-03 2.49E-05

7 . 5 0 E 01 7 , 5 1 E O0 6~ 5.25E-02 9.27E-03 7.85E-05

2,48E-03 9.42E-04 3,46E-04 1,14E-04 5,31E-05 5,44E-06

7.26E-02 1.84E-02 4.53E-03 9.92E-04 3.56E-04 1.86E-05

2 . 1 3 E O0 3.60E-01 5.95E-02 8.57E-03 2.34E-03 5.89E-05

6 . 3 5 E 01 7 . 2 9 E O0 8.13E-01 7.68E-02 1,58E-02 1.87E-04

38

50 70 100 150 200 500

1.91E-03 7.20E-04 2.54E-04 7.77E-05 3.38E-05 2.87E-06

6.02E-02 1.44E-02 3,34E-03 6.79E-04 2.28E-04 g.73E-06

2 . 6 7 E O0 3.85E-01 5.38E-02 6.48E-03 1.57E-03 3.07E-05

9 , 8 3 E 01 9 . 8 1 E O0 9.04E-01 6.72E-62 1.17E-82 9.75E-05

3,18E-03 1,21E-03 4.42E-04 1,45E-04 6,76E-05 6.87E-06

9.50E-02 2.39E-02 5.86E-03 1.28E-03 4.56E-04 2~

2 . 8 4 E O0 4.76E-01 7.79E-02 1.11E-02 3.01E-03 7.49E-05

8 . 5 9 E 01 9 . 7 6 E O0 1 . 0 8 E O0 1.01E-01 2.06E-02 2.38E-04

39

50 70 100 150 200 500

2.19E;03 8.29E-04 2.93E-04 8.98E-05 3,91E-05 3.35E-06

7.26E-02 1.71E-02 3,93E-03 7.93E-04 2.65E-04 1.13E-05

3 . 3 5 E O0 4.79E-01 6.58E-02 7.79E-03 1.87E-03 3.60E-05

1 . 2 6 E 02 1 . 2 4 E 01 1 . 1 3 E O0 8.29E-02 1,43E-02 1.15E-04

3,89E-03 1~ 5,38E-04 1~ 8,19E-05 8,24E-06

1.18E-01 2.96E-02 7.22E-03 1.56E-03 5,56E-04 2.84E-05

3 . 6 3 E O0 6.00E-01 9.72E-02 1.37E-02 3.70E-03 9.05E-05

1 . 1 2 E 02 1 . 2 5 E 01 1 . 3 6 E O0 1,26E-01 2.55E-02 2,89E-04

40

50 70 100 150 200 500

2,46E-03 9.31E-04 3.30E-04 1.01E-04 4.44E-05 3.82E-06

8,48E-02 1,98E-02 4.50E-03 9.03E-04 3.02E-04 1.29E-05

4 . 0 3 E O0 5.72E-01 7.78E-02 9.09E-03 2.17E-03 4.12E-05

1 . 5 3 E 02 1 . 5 1 E 01 1 , 3 6 E O0 9.87E-02 1.69E-02 1.33E-04

4~ 1.76E-03 6,41E-04 2.10E-04 9~ 9.68E-06

1.44E-01 3.58E-02 8,68E-03 1.87E-03 6.62E-04 3.35E-05

4 . 4 ~ E O0 7.36E-01 1.18E-01 1.66E-02 4.43E-03 1.07E-04

1 . 4 1 E 02 1~ 01 1 . 6 7 E O0 1.53E-01 3.07E-02 3,43E-04

41

50 70 100 150 200 500

2.6BE-03 1.02E-03 3.61E-04 1.11E-04 4.88E-05 4.23E-06

9,79E-02 2.25E-02 5.06E-03 1.OOE-03 3.34E-04 1.43E-05

4 . 8 2 E O0 6.78E-01 9.11E-02 1.05E-02 2.47E-03 4.60E-05

1 . 8 4 E 02 1 . 8 0 E 01 1 . 6 2 E O0 1.16E-01 1.97E-02 1,51E-04

5.38E-03 2,04E-03 7.40E-04 2.41E-04 1.11E-04 1.10E-05

1.70E-01 4.21E-02 1.02E-02 2.17E-03 7.66E-04 3.83E-05

5 . 4 4 E O0 8.83E-01 1.40E-01 1.94E-02 5.17E-03 1.23E-04

1 . 7 3 E 02 1 . 9 0 E 01 2 . 0 2 E O0 1,81E-01 3.62E-02 3.95E-04

42

50 70 100 150 200 500

2.94E-03 1.12E-03 3.98E-04 1.23E-04 5.40E-05 4~

1.13E-01 2.56E-02 5.70E-03 1.12E-03 3.73E-04 1.60E-05

5 . 6 9 E O0 7.96E-01 1.06E-01 1.20E-02 2.81E-03 5.17E-05

2 . 1 8 E 02 2 . 1 3 E 01 1.91E O0 1.36E-01 2.28E-62 1.71E-04

6~ 2.37E-03 8,62E-04 2.80E-04 1~ 1.27E-05

2~ 4.99E-02 1.20E-02 2.54E-03 8.94E-04 4.42E-05

6 . 5 9 E O0 1 . 0 6 E O0 1.67E-01 2.29E-02 6.07E-03 1.42E-04

2 . 1 3 E 02 2 . 3 0 E 01 2 . 4 2 E O0 2.16E-01 4.28E-02 4.59E-04

43

50 70 100 150 200 500

3.31E-03 1.26E-03 4.50E-04 1.40E-04 6.15E-05 5.40E-06

1.32E-01 2.97E-02 6.57E-03 1.29E-03 4,26E-04 1~

6 . 8 5 E O0 g.52E-01 1.26E-01 1.41E-02 3.27E-03 5.97E-05

2 . 6 4 E 02 2 . 5 7 E 01 2 . 3 0 E O0 1.62E-01 2.70E-02 1.99E-04

7.53E-03 2.84E-03 1.03E-03 3.34E-04 1.54E-04 1,5DE-05

2.46E-01 6.05E-02 1.44E-02 3.05E-03 1.07E-03 5.24E-05

8 . 1 7 E O0 1o30E O0 2.04E-01 2.78E-02 7.31E-03 1.69E-04

2 . 6 7 E 02 2 . 8 6 E 01 2 . 9 8 E O0 2.63E-01 5,19E-02 5,48E-04

44

50 70 100 150 200 500

3.52E-03 1,34E-03 4.80E-04 1.49E-04 6.58E-05 5.82E-06

1.48E-01 3~ 7.22E-03 1.40E-03 4.61E-04 f.98E-05

7 . 8 9 E O0 1 . 0 9 E O0 1.43E-01 1.58E-02 3.64E-03 6.50E-05

3 . 0 5 E 02 2 . 9 7 E 01 2 . 6 4 E O0 1,85E-01 3.07E-02 2.20E-04

8~ 3~ 1.16E-03 3,75E-04 1.72E-04 1,66E-05

2.83E-01 6.92E-02 1.64E-02 3.45E-03 1.21E-03 5.85E-05

9.60E O0 1.52E O0 2.35E-01 3.17E-02 8.30E-03 1.89E-04

3,1gE 02 3.38E Ol 3.48E O0 3.04E-01 5.94E-02 6.15E-04

128

INTERNAL CONVERSION IN OUTER SHELLS

(N+O+,,.)

- SHELLS

Z

K

E1

E2

63

64

H1

H2

H3

H4

45

50 70 100 150 200 500

3.80E-03 1.45E-03 5.226-04 1.63E-04 7.196-05 6.40E-06

1.686-01 3.716-02 8.03E-03 1.546-03 5.086-04 2.186-05

9 . 1 5 6 O0 1 . 2 6 E O0 1.646-01 1.796-02 4.106-03 7.226-05

3 . 5 5 6 02 3 . 4 5 6 01 3 . 0 6 E O0 2.136-01 3.516-62 2.476-04

9.77E-03 3.686-03 1.33E-03 4.296-04 1.896-05

3.31E-01 8.066-02 1.906-02 3.98E-03 1.39E-03 6.66E-05

1 . 1 4 E 01 1 . 7 9 E O0 2.75E-01 3.696-02 9.606-03 2.16E-04

3 . 8 5 6 02 4 . 0 4 E 01 4 . 1 2 6 O0 3.566-01 6.926-02 7.05E-04

50 70 100 150 200 500

3.91E-03 1.49E-03 5.366-04 1.67E-04 7.39E-05 6.606-06

1.896-01 4.106-02 8.716-03 1.646-03 5,356-04 2.27E-05

1 . 0 6 6 01 1 . 4 5 6 O0 1.866-01 2.006-02 4.51E-03 7.646-05

4.11602 3 . 9 8 E 01 3 . 5 2 6 O0 2.436-01 3.96E-02 2.666-04

1.05E-02 3,976-03 1,436-03 4.616-04 2.11E-04 2.006-05

3.67E-01 8.886-02 2.08E-02 4.33E-03 1.50E-03 7.11E-05

1 . 3 2 E 01 2 . 0 4 6 O0 3.09E-01 4.08E-02 1.05E-02 2.326-04

4.53E

47

50 70 100 150 200 500

4.42E-03 1.706-03 6.11E-04 1.92E-04 8.516-05 7.68E-06

2.17E-01 4,696-02 9.966-03 1.88E-03 6.136-04 2.636-05

1 . 2 3 E 01 1 . 6 8 E O0 2.156-01 2.316-02 5.206-03 8.866-05

4 . 7 9 6 02 4 . 6 4 6 01 4 . 0 9 E O0 2.826-01 4.606-02 3.106-04

1.28E-02 4,81E-03 1.736-03 5.586-04 2,556-04 2o416-05

4.506-01 1.08E-01 2.546-02 5.26E-03 1.826-03 8.566-05

1 . 6 1 E 01 2.49E O0 3.76E-01 4.956-02 1.28E-02 2.806-04

5 . 5 8 6 02 5 . 7 4 6 01 5 . 7 5 6 O0 4.866-01 9.336-02 9.196-04

48

50 70 100 150 200 500

4.87E-03 1.876-03 6,766-04 2.136-04 9.466-05 8.60E-06

2.496-01 5.366-02 1.13E-02 2.126-03 6.886-04 2.95E-05

1 . 4 4 6 01 1 . 9 6 6 O0 2.506-01 2.67E-02 5.95E-03 1.006-04

5 . 6 4 6 02 5 . 4 4 6 01 4 . 7 8 6 O0 3.296-01 5,346-02 3,546-04

1o506-02 5.636-03 2.036-03 6,506-04 2,96E-04 2.796-05

5.35E-01 1.286-01 2,996-02 6.18E-03 2.13E-03 9.94E-05

1 . 9 5 6 01 2 . 9 9 E O0 4.48E-01 5.85E-02 1.506~ 3.25E-04

6 . 8 2 6 02 6 . 9 5 6 O1 6 . 9 0 6 O0 5.78E-01 1.10E-01 1.07E-03

49

50 70 100 150 200 500

5.39E-03 2.086-03 7.516-04 2.376-04 1.056-04 9.626-06

2.956-01 6.29E-02 1.316-02 2.426-03 7.826-04 3.326-05

1 . 7 3 E O1 2 . 3 5 6 O0 2.99E-01 3.156-02 6.98E-03 1.156-04

6.826 02 6 . 5 7 6 01 5 . 7 7 6 O0 3.946-01 6.376-02 4.116-04

1.766-02 6.59E-03 2.376-03 7,586-04 3.45E-04 3.226-05

6.39E-01 1.53E-01 3.54E-02 7.276-03 2.50E-03 1.156-04

2 . 3 9 E O1 3 . 6 3 6 O0 5.39E-01 6.98E-02 1.78E-02 3.796-04

8 . 5 1 6 02 8 . 5 9 6 O1 8 . 4 2 6 O0 6.98E-01 1.326-01 1.26E-03

5O

50 70 100 150 200 500

5.93E-03 2.296-03 8.286-04 2.616-04 1.176-04 1.076-05

3.436-01 7.256-02 1.506-02 2,746-03 8.806-04 3.716-05

2 . 0 4 E 01 2 . 7 7 6 O0 3.506-01 3.67E-02 8.07E-03 1.306-04

8 . 0 8 6 02 7 . 7 7 6 Ol 6 . 8 1 6 O0 4.646-01 7.466-02 4.726-04

2.04E-02 7.676-03 2.75E-03 8.806-04 4.00E-04 3~

7.58E-01 1.80E-01 4.17E-02 8.506-03 2.91E-03 1.33E-04

2 . 9 0 E 01 4 . 3 6 E O0 6.426-01 8,24E-02 2~ 4.396-04

1 . 0 4 6 03 1 . 0 4 E 02" 1 . 0 1 E O1 8.316-01 1.566-01 1.46E-03

51

50 70 100 150 200 500

6.456-03 2.49E-03 9.04E-04 2.866-04 1.28E-04 1.18E-05

3.966-01 8.306-02 1.706-02 3.07E-03 9.826-04 4.126-05

2 . 3 9 E 01 3 . 2 3 6 O0 4.07E-01 4.246-02 9~ 1.46E-04

9 . 4 8 6 02 9 , 0 9 6 01 7 . 9 5 E O0 5.406-01 8.666-02 5.586-04

2,366-02 8.836-03 3.17E-03 1.01E-03 4.586-04 4.22E-05

8.90E-01 2.11E-01 4.85E-02 9.85E-03 3~ 1.52E-04

3 . 4 8 E 01 5 . 1 9 6 O0 7.586-01 9.64E-02 2.436-02 5.04E~

1 . 2 7 E 03 1 . 2 6 6 02 1 . 2 1 6 01 9.81E-01 1,836-01 1.68E-03

52

50 70 100 150 200 500

7,04E-03 2.72E-03 9.89E-04 3.146-04 1.41E-04 1.316-05

4.566-01 9.506-02 1.926-02 3.466-03 1.106-03 4,58E-05

2 , 7 9 E 01 3 . 7 7 6 O0 4.73E-01 4.896-02 1.066-02 1.646-04

1 . 1 1 E 03 1 . 0 6 6 62 9 . 2 7 6 O0 6.296-61 1.006-01 6.146-04

2.726-02 1.02E-02 3.65E-03 1.166-03 5,27E-04 4,82E-05

1 . 0 5 6 O0 2.476-01 5.656-02 1.14E-02 3.89E-03 1.75E-04

4 . 1 7 6 01 6 . 1 7 6 O0 8.946-01 1,13E-01 2.836-02 5.806-04

1 . 5 4 E 03 1 . 5 1 6 02 1 . 4 4 6 01 1 . 1 6 E O0 2.156~ 1.94E-03

46

129

1~

02 O1 4 . 7 2 6 O0 4.016-01 7.71E-02 4.696

7.646-04

DRA(3OUN, PLAJNER, AND SCHMUTZLER

(N+O+,,,)

- SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

H4

53

50 70 100 150 200 500

7.63E-03 2.95E-03 1.07E-03 3,42E-04 1,53E-04 1,44E-05

5.22E-01 1.08E-01 2,17E-02 3~ 1,22E-03 5~

3 . 2 4 E 01 4 . 3 6 E O0 5.46E-01 5~ 1~ 1.84E-04

1 . 2 9 E 03 1 . 2 3 E 02 1 . 0 8 E 01 7,28E-01 1.16E-01 6,97E-04

3~ 1,17E-02 4,18E-03 1,33E-03 6.02E-04 5~

1 . 2 2 E O0 2,87E-01 6,55E-02 1.32E-02 4.47E-03 1.99E-04

4 , 9 7 E 01 7~ O0 1 . 0 5 E O0 1.31E-01 3,28E-02 6.62E-04

1~ 03 1 . 8 1 E 02 1~ 01 1 , 3 6 E O0 2,51E-01 2,23E~

54

50 70 100 150 200 500

8.25E-03 3.20E-03 1~ 3.72E-04 1,67E-04 1.58E-05

5.96E-01 1.23E-01 2.45E-02 4~ 1,36E-03 5~

3 . 7 3 E 01 5 . 0 2 E O0 6,27E-01 6~ 1~ 2.06E-04

1 . 4 9 E 03 1 . 4 2 E 02 1 . 2 4 E 01 8.37E-01 1,33E-01 7.90E-04

3.58E-02 1,34E-02 4~ 1~ 6~ 6,22E-05

1 . 4 2 E O0 3~ 7~ 1.52E-02 5.13E-03 2,27E-04

5o90E 01 8 . 6 0 E O0 1o23E O0 1,53E-01 3.79E-02 7,57E-04

2 , 2 4 E 03 2 . 1 6 E 02 2 . 0 2 E 01 1 , 5 9 E O0 2.92E-01 2.55E-03

55

50 70 100 150 200 500

8,97E-03 3,49E-03 1~ 4~ 1~ 1,74E-05

6,80E-01 1,39E-01 2~ 4,85E-03 1~ 6,22E-05

4o29E 01 5 , 7 7 E O0 7.20E-01 7.34E-02 1,57E-02 2~

1 . 7 2 E 03 1 . 6 4 E 02 1 . 4 3 E 01 9.62E-01 1,53E-01 8,99E-04

4,14E-02 1,55E-02 5~ 1,76E-03 7~ 7,12E-05

1~ O0 3,90E-01 8,83E-02 1~ 5.94E-03 2,61E-04

7~ 01 1 , 0 2 E 01 1 , 4 4 E O0 1,78E-01 4.41E-02 8,71E-04

2 , 6 9 E 03 2~ 02 2o39E 01 1~ O0 3~ 2.95E-03

56

50 70 100 150 200 500

9.79E-03 3.81E-03 1.40E-03 4~ 2,02E-04 1.93E-05

7.81E-01 1.60E-01 3,14E-02 5~ 1,70E-03 6.93E-05

4 . 9 8 E 01 6 , 6 9 E O0 8~ 8.45E-02 1,80E-02 2,63E-04

2 . 0 0 E 03 1 . 9 0 E 02 1 , 6 5 E 01 1 . 1 1 E O0 1~ 1.03E-03

4~ 1.79E-02 6,41E-03 2.03E-03 9~ 8,17E-05

1 , 9 6 E O0 4.57E-01 1~ 2.05E-02 6.89E-03 3.00E-04

8 , 4 6 E 01 1~ 0t 1 , 7 1 E O0 2.09E-01 5.14E-02 1.00E-03

3 . 2 5 E 03 3 , 0 9 E 02 2 . 8 5 E 01 2~ O0 4,00E-01 3,41E-03

57

50 70 100 150 200 500

1.05E-02 4.08E-03 1,50E-03 4.81E-04 2.17E-04 2.09E-05

8.84E-01 1.80E-01 3,52E-02 6,06E-03 1.87E-03 7.56E-05

5.69E

01 7 . 6 3 E O0 9,47E-01 9~ 2~ 2.91E-04

2 . 3 0 E 03 2 . 1 8 E 02 1 . 8 9 E 01 1 . 2 7 E O0 2,01E-01 1.15E-03

5,42E-02 2,03E-02 7,23E-03 2,29E-03 1,03E-03 9,14E-05

2 . 2 5 E O0 5~ 1~ 2,33E-02 7.80E-03 3.36E-04

9~ 01 1 . 4 1 E 01 1 , 9 7 E O0 2,39E-01 5,86E-02 1.13E-03

3 . 8 7 E 03 3 . 6 4 E 02 3o33E 01 2 , 5 5 E O0 4.60E-01 3.85E-03

58

50 70 100 150 200 500

1~ 4,23E-03 1.56E-03 5.02E-04 2,28E-04 2,20E-05

9,55E-01 1,93E-01 3,77E-02 6,46E-03 1.99E-03 8,02E-05

6 , 1 8 E 01 8~ O0 1~ O0 1,04E-01 2,20E-02 3.12E-04

2~ 03 2 . 3 6 E 02 2 , 0 5 E 01 1 , 3 8 E O0 2,19E-01 1,25E-03

5.98E-02 2,23E-02 7~ 2,52E-03 1,13E-03 1,00E-04

2 . 5 1 E O0 5~ 1~ 2,57E-02 8.61E-03 3.69E-04

1 , 1 1 E 02 1 , 5 8 E 01 2 , 2 0 E O0 2.66E-01 6,49E-02 1.24E-03

4 , 3 9 E 03 4 , 1 0 E 02 3~ 01 2~ O0 5,11E-01 4.23E-03

59

50 70 100 150 200 500

1.14E-02 4.45E-03 1.64E-03 5.31E-04 2.416-04 2.35E-05

1 . 0 6 E O0 2.15E-01 4.16E-02 7.07E-03 2~ 8.63E-05

6 . 9 3 E 01 9 . 2 8 E O0 1 . 1 5 E O0 1.16E-01 2~ 3.42E-04

2 . 8 0 E 03 2 . 6 5 E 02 2 . 3 0 E 01 1 , 5 5 E O0 2.45E-01 1.39E-03

6~ 2.49E-02 8~ 2,80E-03 1,26E-03

1.28E 1~ 2,50E

I,11E-04

2~ O0 6,56E-01 1,47E-01 2.88E-02 9.61E-03 4.08E-04

7.30E-02 1.38E-03

5 , 1 1 E 03 4~ 02 4 . 2 8 E 01 3 . 2 4 E O0 5,78E-01 4,72E-03

50 70 100 150 200 500

1~ 4.92E-03 1,83E-03 5.87E-04 2.63E-04 2.51E-05

1 . 2 2 E O0 2,42E-01 4,74E-02 7~ 2.40E-03 9,28E-05

7.66E 1.02E

01

I,30E

O0

2 . 9 9 E 03 2 . 8 3 E 02 2~ 01 1 . 7 2 E O0 2.69E-01 1.52E-03

7,70E-02 2.84E-02 1.03E-02 3.23E-03 1~ 1~

3 . 1 7 E O0 7~ 1.66E-01 3.25E-02 1~ 4.54E-04

1 . 3 7 E 02 1 , 9 3 E 01 2 . 7 4 E O0 3,30E-01 7,98E-02 1.53E-03

5 , 1 7 E 03 4 , 8 4 E 02 4 . 5 3 E 01 3 . 4 7 E O0 6.19E-01 5~

60

01

1,30E-01 2.71E-02 3.71E-04

130

02 01 O0

3,00E-01

INTERNAL CONVERSION IN OUTER SltELLS

(N+O+.,.)

-

SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

M4

61

50 70 100 150 200 500

1.34E-02 5.16E-03 1.93E-03 6.19E-04 2.78E-04 2,65E-05

1 . 3 4 E 00 2.65E-01 5,196-02 8.65E-03 2.59E-03 9,94E-05

8 . 4 8 E 01 1 . 1 3 E 01 1 , 4 3 E O0 1.44E-01 2.996-02 4,076-04

3 . 3 1 6 03 3 , 1 3 E 02 2 , 8 1 E 01 1 . 9 0 E OO 2,98E-01 1.68E-03

8,57E-02 3,16E-02 1.14E-02 3,59E-03 1,59E-03 1,346-04

3 . 5 7 E 00 8.156-01 1,85E-01 3.636-02 1.20E-02 4.98E-04

1 . 5 7 E 02 2 . 1 9 6 01 3 , 1 0 E 00 3.71E-01 8.93E-02 1.696-03

5 . 9 6 E 03 5 . 5 4 E 02 5 . 1 5 E 01 3 . 9 2 E 00 6.95E-01 5.81E-03

62

50 70 100 150 200 500

1.41E-02 5.42E-03 2.03E-03 6.53E-04 2.93E-04 2,84E-05

1 . 4 8 E 00 2.92E-01 5.68E-02 9.42E-03 2.81E-03 1,076-04

9 . 4 0 E 01 1 . 2 5 E 01 1 . 5 9 E 00 1.59E-01 3.30E-02 4.43E-04

3 . 6 7 E 03 3 . 4 8 E 02 3 . 1 1 6 01 2 . 1 1 E 00 3.31E-01 1,85E-03

9,53E-02 4 . 0 2 E 00 3,51E-02 9.16E-01 1,27E-02 2.08E-01 3,98E-O34,05E-02 1,76E-03 1,33E-02 1.50E-04 5,56E-04

1 . 7 9 E 02 2 . 5 0 E 01 3 . 5 0 E 00 4,17E-01 9,98E-02 1,88E-03

6 . 8 7 E 03 6 . 3 5 E 02 5 . 8 6 E 01 4 , 4 2 E 00 7,80E-01 6,49E-03

63

50 70 100 150 200 500

1.47E-02 5.68E-03 2,13E-03 6.87E-04 3.09E-04 3.00E-05

~ .6 3 E O0 3.20E-01 6,21E-02 1.02E-02 3.04E-03 1.156-04

1 , 0 4 E 02 1 . 3 8 E 01 1 , 7 5 E O0 1.75E-01 3.63E-02 4.86E-04

4 . 0 6 E 03 3 . 8 3 E 02 3 , 4 3 E 01 2 . 3 3 E 00 3,656-01 2.056-03

1,06E-01 3,91E-02 1,41E-02 4,42E-03 1.95E-03 1,64E-04

4 . 5 2 E 00 1 . 0 3 E O0 2.32E-01 4,51E-02 1,48E-02 6.10E-04

2 . 0 5 E 02 2 . 8 3 E 01 3 , 9 5 E O0 4,67E-01 1,11E-01 2.07E-03

7 . 9 0 E 03 7 . 2 5 E 02 6 , 6 4 E 01 4 , 9 8 E O0 8.75E-01 7.18E-03

64

5O 70 IO0 150 200 5OO

1.57E-02 6.05E-03 2.27E-03 7.35E-04 3.32E-04 3.19E-05

1 .8 2 E 00 3,58E-01 6.glE-D2 1,13E-02 3,35E-03 1.24E-04

1 . 1 7 E 02 1 . 5 5 E 01 1 . 9 7 E 00 1.97E-01 4.08E-02 5.31E-04

4. 62E 03 4 , 3 4 E 02 3 . 8 7 E 01 2 . 6 2 E O0 4,12E-01 2.26E-03

1,19E-01 4~ lo59E-D2 4,98E-03 2,20E-03 1.81E-04

5 . 1 7 E 00 1 . 1 7 E O0 2,64E-01 5.11E-02 1,68E-02 6.76E-04

2 . 3 8 E 02 3 . 2 7 E 01 4 . 5 3 E O0 5.32E-01 1,27E-01 2.30E-03

9 , 2 9 E 03 8 . 4 6 E 02 7o68E 01 5 , 7 1 E O0 1.00E-O0 7.98E-03

65

50 70 100 150 200 500

1.61E-02 6.22E-03 2.34E-03 7.59E-04 3.43E-04 3.30E-05

1 . 9 7 E 00 3.86E-01 7.43E-02 1.21E-02 3.57E-03 1.30E-04

1 . 2 6 E 02 1 . 6 8 E 01 2 . 1 3 E 00 2.13E-01 4.41E-02 5.66E-04

4 . 9 6 E 03 4 . 6 7 E 02 4 . 1 8 E 01 2 . 8 4 6 00 4,46E-01 2.43E-03

1,30E-01 4.81E-02 1,74E-02 5,43E-03 2.40E-03 1.95E-04

5 . 7 0 E 00 1 . 2 9 E 00 2.89E-01 5.59E-02 1.83E-02 7.28E-04

2 . 6 5 E 02 3 . 6 3 E 01 5 , 0 1 E 00 5.85E-01 1.39E-01 2.48E-03

1 . 0 4 E 04 9 . 4 3 E 02 8 , 5 2 E 01 6 . 3 0 E O0 1,10E 00 8,63E-03

66

50 70 100 150 200 500

1,68E-02 6.50E-03 2.45E-03 7.96E-04 3.62E-04 3.55E-05

2 ,1 6 E O0 4.24E-01 8,12E-02 1.32E-02 3.87E-03 1.42E-04

1,39E 02 1 . 8 5 E 01 2 , 3 5 E 00 2.35E-01 4,85E-02 6.29E-04

5 . 4 7 E 03 5. 15E 02 4 . 6 0 E 01 3 . 1 2 E 00 4.92E-61 2.73E-03

1.44E-01 5.33E-02 1,92E-02 6,01E-03 2.65E-03 2,18E-04

6 . 3 9 E 00 1. 44E 00 3.23E-01 6.22E-02 2,03E-02 8.15E-04

3 . 0 2 E 02 4 . 1 1 E 01 5 . 6 3 E 00 6.546-01 1.55E-01 2.78E-03

1 . 1 9 E 04 1 . 0 7 E 03 9 . 6 4 E 01 7 . 0 8 E 00 1 . 2 3 E O0 9.71E-03

67

50 70 100 150 200 500

1.75E-02 6.79E-03 2.56E-03 8.36E-04 3.80E-04 3,72E-05

2 . 3 7 E 00 4.64E-01 8.87E-02 1.43E-02 4.19E-03 1.51E-04

1 2 2 2 5 6

53E 02 04E 01 58E O0 58E-01 33E-02 78E-04

6 , 0 2 E 03 5 , 6 6 E 02 5 . 0 5 E 01 3 . 4 3 E 00 5.41E-01 2.96E-03

1,60E-01 5.91E-02 2,13E-02 6~ 2.93E-03 2,38E-04

7 , 1 6 E 00 1 , 6 1 E O0 3,59E-01 6.91El02 2.25E-02 8,90E-04

3 , 4 2 E 02 4 , 6 4 E 01 6 . 3 2 E 00 7,31E-01 1.72E-01 3,04E-03

1 , 3 6 E 04 1 , 2 2 E 03 1 . 0 9 6 02 7.93E O0 1 . 3 7 E O0 1.06E-02

68

50 70 100 150 200 500

1.82E-02 7.08E-03 2,68E-03 8.76E-04 3,99E-04 3.90E-05

2 , 6 0 E O0 5.08E-01 g,68E-02 1.566-02 4,54E-03 1,60E-04

1 , 6 8 E 02 2 . 2 4 E 01 2 . 8 4 E O0 2,84E-01 5.86E-02 7,32E-04

03 6 . 2 1 E 02 5 . 5 4 E 01 3 . 7 7 E 00 5.956-01 3.226-03

1,77E-01 6o55E-02 2~ 7.37E-03 3,25E-03 2,60E-04

8 , 0 1 E 00 1 . 8 0 E 00 4,00E-01 7,67E-02 2,49E-02 9,72E-04

3 . 8 8 E 02 5 , 2 4 E 01 7 . 1 0 E O0 8.16E-01 1.91E-01 3.33E-03

1 . 5 6 E 04 1 . 3 9 E 03 1o23E 02 8 . 8 9 E 00 1 , 5 3 E 00 1.16E-02

6.63E

131

DRAGOUN, PLAJNER, AND SCtlMUTZLER

(N+O+.,.)

- SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

H4

69

50 70 100 150 200 500

1.89E-02 7.37E-03 2.80E-03 9.17E-04 4.19E-04 4,19E-05

2 . 8 5 E O0 5.56E-01 1~ 1.69E-02 4~ 1,75E-04

1 . 8 4 E 02 2 . 4 5 E 01 3 , 1 1 E O0 3,11E-01 6~ 8.14E-04

7 . 2 8 E 03 6 . 8 1 E 62 6 . 0 7 E 01 4 , 1 4 E O0 6,55E-01 3,61E-03

1,96E-01 7.24E-02 2,61E-02 8~ 3,59E-03 2.90E-04

8 . 9 5 E O0 2 . 0 0 E O0 4~ 8.50E-02 2.76E-02 1,09E-03

4 . 3 9 E 02 5 . 9 0 E 01 7 . 9 5 E O0 9.09E-01 2.13E-01 3~

1 . 7 7 E 04 1 . 5 7 E 03 1 . 3 8 E 02 9.95E O0 1 , 7 1 E O0 1.31E-02

70

50 70 100 150 200 500

1.97E-02 7.69E-03 2.92E-03 9.01E-04 4.40E-04 4.57E-05

3 , 1 2 E O0 6,08E-01 1.15E-01 1.77E-02 5.34E-03 1.92E-04

2 . 0 2 E 02 2 . 6 9 E 01 3 . 4 2 E O0 3~ 7.07E-02 9.00E-04

8 . 0 1 E 03 7 , 4 7 E 02 6 , 6 6 E 01 4 . 5 4 E O0 7.20E-01 3.99E-03

2,17E-01 8,01E-02 2.89E-02 8.50E-03 3.97E-03 3,33E-04

1 . 0 0 E 01 2 . 2 4 E O0 4.95E-01 9.21E-02 3.06E-02 1.23E-03

4 . 9 8 E 02 6 . 6 6 E 01 8 . 9 2 E O0 1 . 0 3 E O0 2.36E-01 4.13E-03

2 . 0 2 E 04 1 . 7 8 E 03 1 . 5 6 E 02 1 . 1 8 E 01 1 . 9 0 E O0 1,42E-02

71

50 70 100 150 200 500

2.06E-02 8.07E-03 3.07E-03 9o37E-04 4,63E-04 4,86E-05

3 . 4 5 E O0 6.74E-01 1.27E-6Z 1~ 5.84E-03 2,08E-04

2 . 2 4 E 02 2 . 9 9 E 01 3o79E O0 3~ 7.84E-02 9.91E-04

8 . 9 9 E 03 8 . 3 5 E 02 7 . 4 1 E 01 4 . 9 8 E O0 8.00E-61 4,42E-03

2~ 8,91E-02 3o21E-02 9.34E-03 4,40E-03 3~

1 . 1 2 E 01 2 . 5 1 E O0 5~ 1.02E-01 3~ 1.36E-03

5 . 6 9 E 02 7 . 5 8 E 01 1 . 0 1 E 01 1 . 1 5 E O0 2,64E-01 4.58E-03

2 . 3 4 E 04 2 . 0 5 E 03 1 . 7 8 E 02 1 . 3 2 E 01 2 , 1 4 E O0 1.58E-02

72

50 70 100 150 200 500

2.17E-02 8.52E-03 3.24E-03 1.07E-03 4.93E-04 5.19E-05

3 .8 2 E O0 7.45E-01 1.41E-01 2.23E-02 6,42E-03 2.26E-04

2 . 4 8 E 02 3 . 3 2 E 01 4 . 2 1 E O0 4,21E-01 8.71E-02 1,10E-03

1 . 0 0 E 04 9 . 2 7 E 02 8 . 2 2 E 01 5 . 6 0 E O0 8.89E-01 4.92E-03

2o71E-01 1,00E-01 3,60E-02 1~ 4,94E-03 4.11E-04

1 . 2 7 E 01 2 , 8 4 E O0 6.24E-01 1.18E-01 3,82E-02 1,52E-03

6 . 5 2 E 02 8 , 6 5 E 01 1 . 1 4 E 01 1 . 2 9 E O0 2,98E-01 5.11E-03

2 . 7 1 E 04 2 . 3 5 E 03 2 , 0 3 E 02 1 . 4 3 E 01 2 . 4 2 E O0 1.77E-02

73

50 70 100 150 200 500

2,27E-02 8.91E-03 3.40E-03 1.12E-03 5.19E-04 5.49E-05

4 , 2 2 E O0 8.23E-01 1.55E-01 2.45E-02 7.03E-03 2.45E-04

2 . 7 5 E 02 3 . 6 7 E 01 4 . 6 5 E O0 4.66E-01 9.64E-02 1.21E-03

1 . 1 1 E 04 1 . 0 3 E 63 9 . 0 8 E 01 6 . 2 0 E O0 9.84E-01 5.46E-03

3,01E-01 1,11E-01 4,00E-02 1.25E-02 5.48E-03 4,55E-04

1 3 6 1 4 1

43E 01 18E O0 97E-01 32E-01 25E-02 68E-03

7 . 4 3 E 02 9 . 8 1 E 01 1 . 2 9 E 01 1 . 4 4 E O0 3o33E-01 5.66E-03

3 . 1 1 E 04 2 . 6 9 E 03 2 , 3 0 E 02 1 . 6 1 E 01 2~ O0 1.96E-02

74

50 70 100 150 200 500

2.38E-02 9.38E-03 3.58E-03 1,19E-03 5.50E-04 5.89E-05

4 . 6 7 E O0 9.10E-01 1.71E-01 2.70E-02 7.73E-03 2.67E-04

3 . 0 4 E 02 4 . 0 6 E 01 5~ O0 5,17E-01 1.07E-01 1.34E-03

1 . 2 3 E 04 1.14E 03 1 . 0 0 E 02 6 . 8 6 E O0 1 . 0 9 E O0 6.07E-63

3.37E-01 1,25E-01 4~ 1~ 6~ 5.09E-04

1 3 7 1 4 1

62E 01 59E O0 85E-01 48E-01 76E-02 87E-03

8 . 5 1 E 02 1 . 1 2 E 02 1 . 4 6 E 01 1 , 6 3 E O0 3~ 6.32E-03

3 . 5 9 E 04 3 . 0 8 E 03 2 . 6 2 E 02 1 , 8 2 E 01 3o06E O0 2.19E-02

75

50 70 100 150 200 500

2.49E-02 9.81E-03 3~76E-03 1.25E-03 5.79E-04 6.24E-05

5 . 1 5 E O0 1 . 0 1 E O0 1.89E-01 2.97E-02 8.47E-03 2.90E-04

3 . 3 6 E 02 4 . 4 8 E 01 5.69E O0 5.71E-01 1.18E-01 1.47E-63

1 . 3 7 E 04 1 . 2 6 E 03 1.11E 02 7 . 5 8 E O0 1 . 2 1 E O0 6.72E-03

3.75E-01 1.38E-01 4,98E-02 1o55E-02 6,82E-03 5o63E-04

1 . 8 1 E 01 4 . 0 1 E O0 8.76E-01 1.65E-01 5.29E-02 2.07E-03

9 . 6 8 E 02 1 . 2 7 E 02 1 , 6 5 E 01 1 . 8 2 E O0 4.17E-01 6.99E-03

4 . 1 2 E 04 3 . 5 2 E 03 2 . 9 7 E 02 2 . 0 5 E 01 3 . 4 3 E O0 2.43E-02

76

50 70 100 150 200 500

2.61E-02 1.03E-02 3.95E-03 1,32E-03 6.13E-04 6.64E-05

5 . 6 8 E O0 1 , 1 1 E O0 2.08E-01 3.27E-02 9.31E-03 3.~6E-04

3 . 7 0 E 02 4 . 9 5 E 01 6 , 2 8 E O0 6.32E-01 1.31E-01 1.63E-03

1 . 5 2 E 04 1 , 3 9 E 63 1 . 2 2 E 02 8 , 3 7 E O0 1 . 3 4 E 60 7.46E-03

4,20E-01 1o55E-01 5~ 1~ 7.64E-03 6.29E-04

2 . 0 5 E 01 4 . 5 3 E O0 9.85E-01 1,85E-01 5.93E-02 2.31E-03

1 . 1 0 E 03 1 . 4 4 E 02 1 . 8 7 E 01 2 . 0 5 E O0 4,69E-01 7.79E-03

4 . 7 3 E 04 4 , 0 2 E 03 3 . 3 8 E 02 2 . 3 2 E 01 3 , 8 6 E O0 2.71E-02

132

INTERNAL CONVERSION IN OUTER SHELLS

(N+O+...)

SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

H4

77

50 70 100 150 200 500

2.72E-02 1.08E-02 4.14E-03 1.39E-03 6.45E-04 7.04E-05

6 . 2 6 E O0 t . 2 2 E O0 2.29E-01 3.59E-02 1.02E-02 3,42E-04

4 . 0 8 E 02 5 . 4 5 E 01 6 . 9 2 E O0 6.97E-05 1.45E-01 1.79E-03

1 . 6 8 E 04 1. 53E 03 1. 35E 02 9 . 2 2 E O0 1 . 4 7 E O0 8.25E-03

4,66E-01 1,72E-01 6,19E-02 1.93E-02 8,48E-03 6,95E-04

2 . 2 9 E 01 5 . 0 6 E O0 1 . 1 0 E O0 2.05E-01 6.58E-02 2,55E-03

1 , 2 5 E 03 1 . 6 3 E 02 2 . 1 0 E 01 2 . 2 9 E O0 5.22E-01 8.60E-03

5 . 4 2 E 04 4 , 5 8 E 03 3 . 8 2 E 02 2 . 6 0 E 01 4 , 3 2 E O0 2.99E-02

78

50 70 100 150 200 500

2.84E-02 1.13E-02 4.33E-03 1.46E-03 6.80E-04 7.47E-05

6 . 8 9 E O0 1 . 3 4 E O0 2,52E-01 3.94E-02 1.12E-02 3.72E-04

4 . 4 8 E 02 5 . 9 9 E 01 7 . 6 1 E O0 7.68E-01 1,59E-01 1,98E-03

1 . 8 5 E 04 1 . 6 9 E 03 1 . 4 8 E 02 1 . 0 1 E 01 1. 62E O0 9.13E-03

5,21E-01 1,93E-01 6.92E-02 2,15E-02 9,47E-03 7.75E-04

2 . 5 8 E 01 5 . 6 8 E O0 1 . 2 3 E O0 2.30E-01 7.35E-02 2,84E-03

1 . 4 2 E 03 1 . 8 4 E 02 2 . 3 6 E 01 2 . 5 7 E O0 5.84E-01 9.57E-03

6.1gE 04 5 . 2 1 E 03 4 , 3 1 E 02 2 . 9 3 E 01 4 . 8 3 E O0 3.33E-02

79

50 70 100 150 200 500

2.97E-02 1.18E-02 4.54E-03 1.5~E-03 7.15E-04 7.93E-05

7 . 6 5 E O0 1 . 4 9 E O0 2.80E-01 4,36E-02 1,24E-02 4.06E-04

4 . 9 7 E 02 6 . 6 6 E 01 8.45E O0 8.54E-01 1.78E-01 2.19E-03

2 . 0 6 E 04 1. 87E 03 1,64E 02 1 , 1 2 E Ol 1 , 8 0 E O0 1.02E-02

5,79E-01 2,14E-01 7,68E-02 2,39E-02 1,05E-02 8.58E-04

2 , 8 9 E 01 6 . 3 6 E O0 1 . 3 7 E O0 2.56E-01 8.16E-02 3.14E-03

1 . 6 3 E 03 2 . 0 9 E 02 2 . 6 7 E 01 2 , 8 9 E O0 6,53E-01 1.06E-02

7 . 1 4 E 04 5 . 9 7 E 03 4 . 9 1 E 02 3 . 3 1 E 01 5 , 4 4 E O0 3.69E-02

80

50 70 100 150 200 500

3.09E-02 1.25E-02 4.76E-03 1.61E-03 7.55E-04 8.44E-05

8 , 3 5 E O0 1 . 6 3 E O0 3,06E-01 4.77E-02 1.356-02 4.42E-04

5 . 4 3 E 02 7 . 2 6 E 01 9.22E O0 g.33E-01 1.95E-01 2.41E-03

2.27E 2.05E 1.79E 1,23E 1.97E 1~

O~ 03 02 01 O0

6,49E-01 2,40E-01 8.61E-02 2~ 1,18E-02 9.60E-04

3 . 2 5 E 01 7 . 1 4 E O0 1 . 5 4 E O0 2.86E-01 9,15E-02 3.506-03

1 . 8 4 E 03 2 . 3 6 E 02 2 . 9 9 E 01 3 . 2 3 E O0 7.2gE-01 1,18E-02

8 . 1 0 E 04 6 . 7 4 E 03 5 , 5 2 E 02 3 . 7 0 E 01 6 , 0 6 E O0 4,10E-02

81

50 70 100 150 200 500 "

3.26E-02 1.30E-02 5.02E-03 1.70E-03 7.99E-04 8.93E-05

9 . 3 8 E O0 1 .8 3 E O0 3.43E-01 5.346-02 1.51E-02 4.86E-04

6 . 0 9 E 02 8 .1 5 E 01 1 . 0 4 E 01 1 . 0 5 E O0 2.19E-01 2.70E-03

2 . 5 5 E 04 2 . 3 0 E 03 2 . 0 1 E 02 1 . 3 8 E 01 2 . 2 2 E O0 1.26E-02

7,25E-01 2,69E-01 9,61E-02 2.99E-02 1o31E-02 1.07E-03

3 . 6 8 E 01 8 . 0 6 E O0 1 . 7 3 E O0 3,20E-01 1.02E-01 3.89E-03

2 . 1 2 E 03 2 . 7 1 E 02 3 . 4 2 E 01 3 . 6 6 E O0 8.21E-01 1.31E-02

9 , 4 6 E 04 7 , 8 2 E 03 6 . 3 5 E 02 4 . 2 2 E 01 6 . 8 9 E O0 4.59E-02

82

50 70 100 150 200 500

3,41E-02 1.36E-02 5.27E-03 1.79E-03 8.40E-04 9.49E-05

1.02E 01 2 .0 0 E O0 3,74E-01 5.82E-02 1.64E-02 5o27E-04

6 . 6 6 E 02 8 . 9 1 E 01 1 . 1 3 E 01 1 . 1 5 E O0 2.40E-01 2.95E-03

2 . 8 1 E 04 2. 53E 03 2 . 2 0 E 02 1 . 5 1 E 01 2 . 4 2 E O0 1.38E-02

8,10E-01 3,00E-01 1,07E-01 3.35E-02 1.47E-02 1,19E-03

4 . 1 1 E 01 8 . 9 8 E O0 1 . 9 2 E O0 3.55E-01 1.13E-01 4.28E-03

2 . 3 8 E 03 3 . 0 3 E 02 3 . 8 1 E 01 4 . 0 6 E O0 9.11E-01 1.44E-02

1 . 0 7 E 05 8 . 8 2 E 03 7 . 1 2 E 02 4 . 7 1 E 01 7 . 6 6 E O0 5.06E-02

83

50 70 100 150 200 500

3.57E-02 1.43E-02 5.56E-03 1.89E-03 8.93E-04 1.02E-04

1 .1 5 E 01 2 ,2 5 E O0 4.20E-01 6.53E-02 1,84E-02 5.85E-04

7 . 4 3 E 02 9 . 9 5 E 01 1 . 2 6 E 01 1 . 2 9 E O0 2.69E-01 3.32E-03

3 . 1 5 E 04 2 . 8 2 E 03 2 . 4 5 E 02 1. 68E 01 2 . 7 1 E O0 1.56E-02

9,15E-01 3,39E-01 1,21E-01 3.77E-02 1,66E-02 1.34E-03

4.EgE 01 1 . 0 2 E 01 2 . 1 9 E O0 4.04E-01 1.28E-01 4.85E-03

2 . 7 5 E 03 3 . 5 0 E 02 4 . 3 7 E O1 4 . 6 4 E O0 1 . 0 4 E O0 1,63E-02

1 . 2 5 E 05 1 . 0 2 E 04 8 . 2 0 E 02 5 . 3 9 E O1 8 . 7 3 E O0 5.70E-02

84

50 79 100 150 200 500

3.73E-02 1,50E-02 5.82E-03 1.99E-03 9.39E-04 1.08E-04

1 , 2 7 E 61 2 . 5 0 E O0 4.67E-01 7,26E-02 2.04E-02

8 . 2 4 E 02 1 . 1 0 E 02 1 . 4 0 E 01 1 . 4 3 E O0 3,00E-01 6.42E-~4 3 . 6 9 E - 0 3

3 . 5 1 E 04 3 , 1 3 E 03 2 , 7 1 E 62 1 . 8 6 E 01 3 , 0 1 E O0 1.74E-02

1 , 0 2 E O0 3.78E-01 1.35E-01 4,21E-02 1.85E-02 1.49E-03

5 , 2 7 E 01 1 . 1 5 E 01 2 . 4 5 E O0 4.50E-01 1.43E-01 5.37E-03

3,14E 3,97E 4,94E 5.21E

1 . 4 4 E 05 1 , 1 7 E 04 9 . 3 3 E 02 6 . 0 9 E 01 9 . 8 1 6 O0 6.34E-02

133

03 02 01 O0 1.16E O0 1,81E-02

DRAGOUN, PLAJNER, AND SCtIMUTZLER

(N+O+...)

- SHELLS

Z

K

E1

E2

E3

E4

H1

H2

H3

H4

85

50 70 100 150 200 500

3,88E-02 1.566-02 6.09E-03 2.09E-03 1.14E-04

1 , 4 0 6 01 2 . 7 4 E 00 5,136-01 7.98E-02 2,256-02 7.02E-04

9 . 0 3 E 02 1 . 2 1 6 02 1 , 5 4 E 01 1 , 5 7 E O0 3~ 4.086-03

3 . 8 7 6 04 3 , 4 4 6 03 2 , 9 7 6 02 2 . 0 4 E 01 3 , 3 1 E O0 1.92E-02

1 . 1 5 E 00 4,25E-01 1~ 4,726-02 2.08E-02 1,67E-03

5 . 9 3 E 01 1 . 2 9 E 01 2 . 7 5 E O0 5.046-01 1.60E-01 5,99E-03

3 . 5 6 6 03 4 . 4 8 6 02 5 . 5 5 E 01 5 . 8 4 6 O0 1 . 3 0 6 O0 2.01E-02

1 . 6 4 E 05 1 . 3 3 E 04 1 . 0 5 6 03 6 . 8 3 E 01 1 . 1 0 E 01 7,04E-02

86

50 70 100 150 200 500

4,05E-02 1.64E-02 6,38E-03 2.19E-03 1.04E-03 1.21E-04

1 . 5 5 E 01 3 . 0 5 6 00 5.70E-01 8.866-02 2.496-02 7,726-04

1 . 0 0 E 03 1 . 3 4 6 02 1~ 01 1 . 7 4 E 00 3.67E-01 4,54E-03

4 . 3 0 E 04 3 . 8 2 6 03 3~ 02 2 , 2 6 6 01 3 . 6 7 E 00 2.14E-02

1 . 2 8 E 00 4.746-01 1,69E-01 5,27E-02 2,31E-02 1,86E-03

6 , 6 5 E 01 1 . 4 5 E 01 3 . 0 7 E O0 5.62E-01 1.78E-01 6,64E-03

4 . 0 5 E 03 5 , 0 9 E 02 6 , 2 7 E 01 6 . 5 5 E O0 1 , 4 5 E 00 2,236-02

1 . 8 8 E 05 1 , 5 2 E 04 1 . 2 0 E 03 7 , 7 1 E 01 1 . 2 3 E 01 7.82E-02

87

50 70 100 150 200 500

4,23E=02 1.71E-02 6.69E-03 2,30E-03 1,10E-03 1.29E-04

1 . 7 1 E 01 3 . 3 6 E 00 6,286-01 9,77E-02 2.756-02 8.47E-04

1 . 1 0 E 03 1 .4 7 E 02 1 , 8 7 E 01 1 . 9 2 E O0 4.04E-01 5,02E-03

4 . 7 5 E 04 4 . 2 0 6 03 3 , 6 1 6 02 2 . 4 8 E 01 4~ 00 2,376-02

1 , 4 4 E 00 5,32E-01 1,90E-01 5,91E-02 2,606-02 2,08E-03

7 . 4 9 6 01 1 , 6 3 E 01 3 , 4 5 E 00 6.306-01 1.996-01 7.406-03

4 . 5 9 E 03 5 . 7 5 6 02 7 . 0 6 6 01 7 , 3 5 E 00 1~ O0 2.48E-02

2 , 1 4 E 05 1 . 7 2 E 04 1 . 3 5 E 03 8 , 6 6 E 01 1 . 3 8 E 01 8,696-02

88

50 70 100 150 200 500

4.41E-02 1.79E-02 7.00E-03 2,42E-03 1.166-03 1,37E-04

1 , 9 0 E 01 3 . 7 4 E 00 6.996-01 1.09E-01 3,06E-02 9,33E-04

1 . 2 2 6 03 1~ 02 2 . 0 8 6 01 2 . 1 3 6 O0 4.50E-01 5.596-03

5.286 4.65E 3,99E 2,75E 4.486 2~

04 03 02 01 O0

1 . 6 1 6 00 5,95E-01 2,13E-01 6~ 2,90E-02 2,32E-03

8 . 4 2 6 01 1 , 8 3 E 01 3 . 8 6 E 00 7.046-01 2,22E-01 8.226-03

5 , ~ 3E 03 6 , 5 3 E 02 7 . 9 8 E 01 8 , 2 6 6 00 1.82E 00 2.756-02

2 . 4 6 E 05 1 , 9 7 E 04 1 . 5 3 E 03 9 , 7 7 E 01 1 . 5 5 E 01 9.66E-02

89

50 70 100 150 200 500

4.596-02 1.87E-02 7.32E-03 2.54E-03 1.226-03 1.45E-04

2 . 0 8 6 01 4 . 1 1 E 00 7,69E-01 1.206-01 3.37E-02 1.02E-03

1 , 3 3 E 03 1 . 7 9 6 02 2 . 2 8 E 01 2 . 3 4 6 00 4.956-01 6.19E-03

5 . 8 6 6 04 5 . 1 4 6 03 4 . 3 9 6 02 3 . 0 2 E 01 4 . 9 2 E 00 2.926-02

1 , 8 1 E 00 6.70E-01 2,39E-01 7,43E-02 3~ 2.60E-03

9 , 4 8 6 01 2 . 0 5 E 01 4 . 3 3 6 O0 7.886-01 2.486-01 9,17E-03

5 , 9 2 E 03 7 . 3 6 E 02 8.966 01 9 . 2 5 E 00 2 . 0 3 E 00 3.06E-02

2 . 8 0 E 05 2 . 2 3 E 04 1 . 7 3 E 03 1 . 1 0 E 02 1 . 7 4 E 01 1.076-01

90

50 70 100 150 200 500

4.79E-02 1.95E-02 7.68E-03 2.67E-03 1.28E-03 1.55E-04

2 . 3 1 6 01 4 . 5 6 E 00 8.54E-01 1.336-01 3.756-02 1.136-03

1 . 4 8 6 03 1 . 9 8 E 02 2 . 5 2 6 01 2 . 6 0 E 00 5.50E-01 6.90E-03

6 . 5 0 E 04 5 . 6 8 E 03 4 . 8 5 E 02 3 . 3 3 E 01 5 . 4 5 E 00 3.25E-02

2~ 00 7.54E-01 2,696-01 8,36E-02 3,67E-02 2,92E-03

1 . 0 7 6 02 2 . 3 1 E 01 4o87E 00 8.85E-01 2.786-01 1.02E-02

6 . 7 4 E 03 8 . 3 6 E 02 1.01E 02 1. 04E 01 2 . 2 8 E 00 3.42E-02

3 . 2 1 E 05 2 . 5 5 E 04 I,966 03 1 , 2 4 E 02 1 , 9 5 E 01 1.20E-01

91

50 70 100 150 200 500

4.94E-02 2.02E-02 7.95E-03 2.78E-03 1.336-03 1.626-04

2 . 5 3 E 01 5o00E O0 9.366-01 1.466-01 4.11E-02 1.24E-03

1 . 6 1 E 03 2 . 1 5 6 02 2 . 7 5 E 01 2 . 8 4 E 00 6.03E-01 7.58E-03

7 , 1 2 6 04 6 . 2 0 6 03 5 . 2 8 E 02 3 . 6 3 E 01 5 . 9 4 E 00 3.58E-02

2~ 00 8,386-01 2.99E-01 9,30E-02 4~ 3~

1 . 1 9 6 02 2~ 01 5 . 4 0 6 00 9.796-01 3.08E-01 1.13E-02

7o55E 03 9 . 3 4 E 02 1 . 1 3 E 02 1 . 1 5 6 01 2 . 5 2 E 00 3.766-02

3 . 6 2 E 05 2 , 8 6 E 04 2 . 1 9 E 03 1 . 3 8 E 02 2 . 1 6 E 01 1.32E-01

92

50 70 100 150 200 500

5.07E-02 2.076-02 8.18E-03 2.86E-03 1.38E-03 1.68E-04

2 . 7 7 E 01 5 , 4 7 6 00 1 . 0 3 E 00 1.60E-01 4.50E-02 1.34E-03

1 . 7 5 6 03 2 . 3 4 6 02 2 . 9 9 E 01 3 . 1 0 6 00 6.59E-01 8.31E-03

7 . 7 8 E 04 6 , 7 6 E 03 5 , 7 4 E 02 3 . 9 5 E 01 6 . 4 7 E 00 3~

2 , 4 9 6 00 9.246-01 3~ 1~ 4.50E-02 3.566-03

1 . 3 1 6 02 2 . 8 3 E 01 5 . 9 4 6 00 1 . 0 8 6 00 3.386-01 1,23E-02

8 , 4 5 E 03 1 . 0 4 E 03 1 . 2 5 E 02 1 . 2 8 6 01 2 . 7 8 E 00 4.106-02

4 . 0 8 E 05 3 , 2 0 6 04 2 . 4 4 E 03 1 . 5 2 6 02 2 . 3 9 6 01 1.44E-01

9,91E-04

134

INTERNAl. CONVERSION IN OUTER SIIELLS

SHELLS

(N*O+.,.)

Z

K

El

E2

E3

E4

M1

H2

H3

H4

93

50 70 100 150 200 500

5,30E-02 2,17E-02 8.61E-03 3,02E-03 1,46E-03 1,80E-04

3 , 0 7 E 01 6 , 0 8 E O0 1 . 1 4 E 00 1~ 5,01E-02 1,50E-03

1 . 9 3 E 03 2 , 5 9 E 02 3 , 3 1 E 01 3~ O0 7,32E-01 9,29E-03

8 , 6 4 E 04 7 , 4 8 E 03 6 , 3 4 E 02 4 , 3 6 E 01 7 , 1 6 E O0 4~

2 , 8 3 E O0 1 , 0 5 E O0 3~ 1,16E-01 5,11E-02 4,04E-03

1 , 4 9 E 02 3 . 2 1 E 01 6~ O0 1 , 2 2 E O0 3,81E-01 1,39E-02

9 , 6 1 E 03 1 . 1 8 E 03 1 , 4 2 E 02 1 , 4 4 E 01 3 . 1 3 E O0 4~

4 . 6 6 E 05 3 , 6 5 E .04 2 . 7 7 E 03 1 , 7 2 E 02 2 , 6 9 E 01 1.61E-01

94

50 70 100 150 200 500

5,46E-02 2.24E-02 8~ 3,13E-03 1,52E-03 1.89E-04

3 , 3 6 E 01 6 , 6 5 E O0 1 , 2 5 E O0 1,95E-01 5,51E-02 1,63E-03

2 , 1 0 E 03 2 , 8 2 E 02 3 . 6 0 E 01 3 .7 5 E O0 8,01E-01 1,02E-02

9 , 3 9 E 04 8 , 1 1 E 63 6 , 8 7 E 02 4~ 01 7 , 8 0 E 60 4.80E-02

3 , 1 5 E O0 1 , 1 7 E O0 4,17E-01 1,29E-01 5~ 4,49E-03

1 , 6 6 E 02 3 , 5 7 E 01 7 , 4 6 E O0 1~ O0 4,22E-01 1~

1 . 0 7 E 04 1 , 3 2 E 03 1 . 5 8 E 02 1 . 5 9 E 01 3 , 4 5 E O0 5.06E-02

5 , 2 3 E 05 4 , 0 8 E 04 3 . 0 8 E 03 1 , 9 1 E 02 2 , 9 7 E 01 1,77E-01

95

5O 70 100 150 200 500

5,67E-02 2,33E-02 9.28E-03 3.28E-03 1.59E-03 1.99E-04

3 , 7 2 E 01 7 , 3 7 E O0 1 , 3 9 E O0 2,17E-01 6,12E-02 1,81E-03

2 . 3 2 E 03 3 . 1 1 E 02 3 . 9 7 E 01 4 . 1 4 E O0 8.87E-01 1,14E-02

$ , 0 4 E 05 8 , 9 4 E 03 7 , 5 6 E 02 5~ 61 8~ O0 5,34E-02

3 , 5 5 E O0 1 , 3 2 E O0 4,69E-01 1~ 6~ 5,03E-03

1, 87E 02 4 , 0 1 E 01 8, 36E O0 1 , 5 1 E O0 4.71E-01 1,71E-02

1 , 2 2 E 04 1 . 4 9 E 03 1 , 7 8 E 02 1 . 7 9 E 01 3 , 8 6 E O0 5.62E-02

5 , 9 7 E 05 4~ 04 3 , 4 8 E 03 2 . 1 4 E 02 3 , 3 3 E 01 1,96E-01

96

50 70 100 150 200 500

5,72E-02 2,39E-02 9,57E-03 3,41E-03 1.66E-03 2.11E-04

4 , 0 8 E 01 8 , 1 1 E O0 1 , 5 3 E O0 2~ 6,75E-02 1,99E-03

2 . 5 3 E 03 3o40E 02 4 . 3 5 E 01 4 , 5 4 E O0 9.75E-01 1.26E-02

1,17E 9,97E 8.33E 5.73E 9~ 5~

3.97E 1,47E 5~ 1~ 7~ 5~

O0 O0

2 , 0 8 E 02 4 , 4 7 E 01 9 , 3 1 E O0 1 , 6 7 E O0 5.23E-01 1.89E-02

1 . 3 7 E 04 1 . 6 7 E 03 1 . 9 8 E 02 1 . 9 9 E 01 4 , 2 9 E O0 6,20E-02

6 . 8 2 E 05 5 , 2 5 E 04 3 . 9 2 E 03 2 , 4 0 E 02 3 , 7 1 E 01 2,Z6E-01

97

50 70 100 150 200 500

5.89E-02 2,46E-02 9,90E-03 3,53E-03 1.73E-03 2,21E-04

4 , 4 8 E 01 8 , 9 1 E O0 1 ,6 8 E O0 2,63E-01 7,44E-02 2,19E-03

2 . 7 7 E 03 3 . 7 1 E 02 4 , 7 5 E 01 4 . 9 7 E O0 1 . 0 7 E O0 1.39E-02

1 , 2 9 E 05 1 . 0 9 E 04 9 , 1 0 E 02 6 , 2 5 E 01 1 , 0 3 E 01 6,48E-02

4 , 4 4 E O0 1~ O0 5,87E-01 1,82E-01 7,99E-02 6,27E-03

2 , 3 2 E 02 4 . 9 8 E 01 1 . 0 3 E 01 1 , 8 6 E O0 5.80E-01 2.09E-02

1 . 5 3 E 04 1 , 8 7 E 03 2 . 2 1 E 02 2 . 2 1 E 01 4 . 7 5 E O0 6.84E-02

7 . 6 8 E 05 5 , 8 9 E 04 4 , 3 8 E 03 2 , 6 6 E 02 4 , 1 1 E 01 2.38E-01

98

50 70 100 150 200 500

6,10E-02 2,56E-02 1,03E-02 3,69E-03 1.81E-03 2,33E-04

4 , 9 6 E 01 9~ O0 1 , 8 6 E O0 2~ 8,28E-02 2,43E-03

3 . 0 5 E 03 4 , 0 9 E 02 5 . 2 3 E 01 5 . 4 9 E O0 1 . 1 8 E O0 1.54E-02

1 , 4 2 E 05 1 , 2 0 E 04 I~ 03 6 , 8 8 E 01 1 , 1 4 E 61 7,19E-02

5,OOE O0 1 , 8 6 E O0 6~ 2,05E-01 8,99E-02 7~

2 . 6 1 E 02 5 . 5 9 E 01 1 . 1 6 E 01 2 , 0 8 E O0 6,49E-01 2,33E-02

1 , 7 4 E 04 2 . 1 1 E 03 2 . 4 8 E 02 2 , 4 7 E 01 5 . 3 1 E O0 7,60E-02

8 , 7 3 E 05 6 , 6 8 E 04 4 . 9 4 E 03 2 , 9 9 E 02 4 , 5 9 E 01 2,64E-01

99

50 70 100 150 200 500

6.28E-02 2.64E-02 1,07E-02 3.83E-03 1,88E-03 2,44E-04

5 . 4 5 E 01 1 . 0 9 E 01 2 , 0 5 E O0 3.23E-01 9,14E-02 2,67E-03

3 . 3 3 E 03 4 . 4 6 E 02 5 . 7 2 E 01 6 . 0 1 E O0 1 . 3 0 E O0 1,70E-02

1 . 5 7 E 05 1 . 3 2 E 04 1 , 0 9 E 03 7 , 5 1 E 01 1 , 2 4 E 01 7.92E-02

5 , 6 0 E O0 2 , 0 8 E O0 7,40E-01 2,30E-01 1,01E-01 7~

2 , 9 1 E 02 6 . 2 3 E 01 1 . 2 9 E 01 2 , 3 1 E O0 7,19E-01 2.58E-02

1 , 9 4 E 04 2 . 3 5 E 03 2 . 7 7 E 02 2 , 7 5 E 01 5 . 8 8 E O0 8,37E~

9 . 8 5 E 05 7 , 5 0 E 04 5 , 5 2 E 03 3 , 3 2 E 02 5 , 0 9 E 01 2,91E-01

100

5O 70 :tO0 150 200 500

6.47E-02 2.72E-02 1.10E-02 3,97E-03 1.96E-03 2.58E-04

5 . 9 9 E 01 1 . 1 9 E 01 2 ,2 6 E O0 3,56E-01 1,01E-01 2,95E-03

3 . 6 5 E 03 4 , 8 8 E 02 6 . 2 6 E 01 6 . 5 9 E O0 1 , 4 3 E O0 1.88E-02

1.75E 1.46E 1.20E 8.23E 1,36E 8~

6 , 2 8 E O0 2 . 3 3 E O0 8~ 2~ 1,13E-01 8,79E-03

3 . 2 5 E 02 6 . 9 4 E 01 1 . 4 3 E 01 2 , 5 6 E O0 7.98E-01 2.86E-02

2 . 1 8 E 04 2 . 6 3 E 03 3 , 0 8 E 02 3 . 0 5 E 01 6 , 5 1 E O0 9.23E-02

1 . 1 1 E 06 8 . 4 3 E 04 6 . 1 7 E 03 3 . 6 9 E 02 5 , 6 4 E 01 3.20E-01

135

05 03 02 01 O0

05 04 03 01 G1