ATOMIC
DATA AND NUCLEAR
DATA TABLES
26, 197-381 (1981)
ROOTHAAN-HARTREE-FOCK SLATER
BASIS-SET
ATOMIC EXPANSIONS
WAVE
FUNCTIONS
FOR 2 = 55-92
A. D. MCLEAN IBM Research Laboratory San Jose, California 95193 AND
R. S. MCLEAN Molecular Research Institute 701 Welsh Road Palo Alto, California 94304
Basis-set expansions of approximate Hartree-Fock orbitals are given for atoms and ions for 2 = 55-92. Expansions in Slater-type functions of double-zeta- and triple-zeta-valence dimensions are computed from the formalism of Roothaan and Bagus. Radial expectation values (r”), n from -3 to 2, for each orbital are given. Comparisons of expansion wave functions with numerical Hat-tree-Fock and numerical Dirac-Fock results for mercury are presented.
0092-640X/81/030197-185$02.00/0 Copyright 8 1981 by Academic Press, Inc. All rights of reproduction in any form reserved.
197
Atomic
Data and Nuclear
Data Tables,
Vol. 28. Nos. 3/4. May/July
1Wl
A. D. MCLEAN
and R. S. MCLEAN
Roothalan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
CONTENTS
INTRODUCTION ........................................... Definitions .............................................. Computational Details ................................... Accuracy ...............................................
199 199 201 202
EXPLANATION
207
TABLES.
OF TABLES
...............................
Basis-Set Expansions Z Element and Conf@uration 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78
Ba+ 6s1(?!Q, Ba 6s*(l,S) ......................... Cs+ (‘S), Cs 6~l(~S) ............................ La Sd’(*D), La 4f’(zF) ......................... Ce 4f2(3H), Ce 5d14f1(3JY). ..................... Pr 4f3(4Z), Pr 5d14f2(4J) ........................ Nd 4f4(50, Nd 5d’4f3(%) ...................... Pm 4f5(%), Pm 5d14f4(6K) ..................... Sm 4f6(‘F), Sm 5&4f5(‘.J). ..................... Eu 4f7(*.9), Eu 5d14f6(*H) ...................... Gd 5d14f7(sD), Gd 4f6(‘F). ..................... Tb 4fs(6H), Tb 5&4f6(sH). ..................... Dy 4f’O(“l), Dy 5d14fs(‘J) ...................... Ho 4f”(4Z), Ho 5d14d’0(6K). .................... Er 4f12(3H), Er 5&4f11(5K) ..................... Tm 4f ly2F), Tm 5d14f12(4J) .................... Yb 4f’q%), Yb Sd’4f 13(3H) .................... Lu+ 4f’4(‘S), Lu 5d1(2D) ....................... Hf+ 5d’(2D), Hf 5d2(3F) ........................ Ta+ 5d2(3F), Ta 5d3(4F). ........................ W+ 5d3(‘F), W 5d4(W) ......................... Re+ 5d4(5D), Re 5d5(6S) ........................
OS+ 5ds(6S), OS 5d6(5D) ........................ Ir+ 5de(5D), Ir 5d7(4F) .......................... Pt+ 5d7(4f’), Pt 5s25d10(‘S) Pt 6s’5de(3D1D), Pt 6s25d6(3F). .................. 79 Au+ 5s25d10(‘S), Au+ 6s15ds(3D) Au 6s15d’0(2S), Au 6s25ds(2D) Au 6s’6p’5d8(4FJ ..............................
209 213 217 221 225 229 233 237 241 245 249 253 257 261 265
269 273 277 281
285 289 293 297 301
311 321
80 81 82 83 84 85
Hg+ US’, Hg 6s2(‘S). ........................ Tl+ (‘S), Tl6~l(~P) ............................ Pb+ 6~‘(~f’), Pb ~P~(~I’, ‘D, ‘S) .................. Bi+ ~P~(~PP), Bi 6p3(‘S, 2D, “P) .................. PO+ OPT, PO ~P~(~I’, ‘D, ‘S) .................. At+ SP’(~P), At 6p”(‘P), At- (‘S) ................
326 330 336 342
86
Rn+ ~P~(~I’), Rn (‘S) ...........................
354
87 88 89 90 91 92
Fr+ (‘S), Fr 7s1(2S). ............................ Ra+ US’, Ra 7s2(lS) ......................... AC 6d’(2D), AC 5f1(2F) ......................... Th 6d’5f’(3H), Th 6d2(3F) ...................... Pa 5f3(4Z), Pa (6d15f2(4J) ........................ U Sf’(“l), U 6d’5f3(5K) ........................
358 362 366 370
198
Atomic
348
374 378
Data and Nuclear
Data Tables,
Vol. 26, No% 3/4. May/July
1961
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
INTRODUCTION
This compilation of approximate basis-set expansions of Hartree-Fock atomic orbitals for atoms with atomic number Z = 55-92 extends an earlier compilations of Clementi and Roetti’ (Z = l-54). Optimized basis sets for atomic-orbital expansions provide a necessary starting point for molecular calculations; this is the primary reason for generating the tables. The accuracy of these approximate basis-set expansions can be measured by comparison with numerical Hartree-Fock results which have been available for some time;2.3 detailed comparison is possible only for closed-shell configurations since the expansion wave functions minimize the energy of a specific L-S multiplet while the numerical wave functions minimize a weighted average of all multiplets arising from the electron configuration. The present tables, covering the heavy elements of the periodic table, do not take into account relativistic effects which are known to be important. However, nonrelativistic atomic and molecular calculations are needed to establish reference points from which the magnitude of relativistic efforts can be measured. It was our hope that these optimized nonrelativistic basis sets would also be a good starting point for relativistic calculations, but, for the heavy elements, this may not be the case. Exploratory calculations of Lee and McLean4 by means of an expansion program for closed-shell Dirac-Fock wave functions indicate a strong dependence of optimum innershell basis functions on the velocity of light, even for the large component of the relativistic spinors.
Dehitions
We tabulate single-configuration self-consistentfield (SCF) wave functions of the nonrelativistic Hamiltonian
which are eigenfunctions of the square of the total orbital-angular-momentum operator, Lz, and the square of the total spin-angular-momentum operator, S2. For all atoms we have computed the lowest L-S states from the expected lowest electronic configuration; for some atoms we have calculated excited states of a configuration, and for others the lowest state of a second configuration. Positive-ion wave functions are computed for all configurations except those with open f-shells. Using the method of Roothaan and Bagus,” we determine SCF atomic orbitals, +w\ru(,defined by 9Wi
=
C P
h&W
YAP(&
4)
=
fhiW
YAP(~,
d)
(2)
with R,(r)
= [(2~)2n+‘l(2n)!]1~2rn~1e-tr
= NF1e-@.
(3)
The radial dependence of the orbitals is an expansion in the radial Slater-type basis functions R@(r), whose indices are A, running over s, p, d,f, . . . symmetries, and p counting serially over basis-set members for a given symmetry. The radial expansion is independent of p; all electrons with a given A, i have the same radial dependence. The expansion coefficients of the ith orbital, cAfp, for the occupied orbitals, make up the wave-function tabulations of this report. The orbital angular dependence Yhfi(O, 4) is a normalized spherical harmonic. The radial basis functions RAP(r) are characterized by two parameters, n and 5, in addition to the symmetry index. Thus, in the tabulations, an entry 2s 15.6, labeling a row of the orbital expansion coefficient tables refers to a radial basis function with n = 2, A = 0, 5 = 15.6. The choice of n in the basis sets used here is a traditional one in which the n-values of the basis functions correspond to the principal quantum number of the orbital in which they are the dominant components. Alternative choices have never been demonstrated to have any real superiority. Inclusion of at least one function with n = A + 1 for each symmetry is important to satisfy approximately the orbital cusp condition
The most widely used analytic expansions are “double-zeta” (DZ), where two functions, each one containing an exponent to be optimized, are included in the basis set for each occupied atomic orbital. A set containing one extra basis function of each symmetry to improve the description of the outermost orbitals, and to add flexibility to the valence-shell basis in molecular calculations, is referred to as a “triplezeta-valence” (TZV) basis set. For Z = 55-92, TZV basis sets give total energies within a tenth of an atomic unit of the complete basis (Hartree-Fock) limit. For each of the atomic states presented in these tables we give both DZ and TZV orbital expansions. In a single case, that of Hg(‘S), we give TZV + 4forbital expansions, where one 4f-function is added to the TZV basis to improve the description of thef-electrons and to see if this basis can duplicate .numerical Hartree-Fock (NHF) results. This is indeed the case and, in fact, demonstrates the possibility of exceeding the available accuracy of NHF results.
199
Atomic
Data and Nuclear
Data Tables,
Vol. 26, Nos. W4, May/July
1961
A. D. MCLEAN
and It. S. MCLEAN
-2 1a.fu =h+l.’ -cfAL ar1To
Rootham-Hartree-Fock
Atomic Wave FJunctions, Z = 55-92
(4)
where fkt is defined in Eq. (2), and 2 is the nuclear charge. Carrying out the partial differentiation of Eq. (4) yields In Eq. (8), NA and N, are the number of electrons in open shells A and p, respectively; JicLv and Kw,, are the vector coupling coefficients required as program input, and A*,, are defined by A-I-C (9) letup&) = C (2~ + WLJ’vtx). V-IA-i4 P,(x) is the Legendre function
Inspection of Eq. (5) shows that use of a single basis function with II = A + 1 and exponent Z/(X + l), and no basis functions with n = A + 2, will give an orbital for which the cusp condition is exactly satisfied. This choice has been used in earlier tabulations;l but, for a basis set of a given size it is not quite as good as the traditional choice for total energies and other expectation values, even though the traditional choice gives orbitals which have rather large errors in the cusp. One other factor that goes into the choice of n is making a selection which minimizes problems of linear dependence in a basis set which is becoming saturated (nearing completeness). Experience has shown that the use of different powers of r in the radial functions, as in the traditional choice, is effective in this regard. For configurations with open f-shells we need previously untabulated vector coupling coefficients used in the Roothaan-Bagus formalism for describing open-shell energy contributions to an L-S state of an electronic configuration. These were generated from Slater coefficientsf,(A, cl) and g,(A, CL)obtained from an energy-expression program of SasakP contained in the ALCHEMY programs. The Slater coefficients detine the open-shell two-electron energy contribution in configurations with a maximum of one open shell per symmetry species as E = C 1: fYt& P)FA Aebbv-0
PA(X) = $ $ . Explicitly, A
A+&
A- Aicl-l-vA A-w+vA A-w-v
*” = (A + /.L+ v + l)A*+,+,
with P!
A, =
(p/2)!(p/2)! * The summation index v of Eqs. (6), (8), and (9) steps by 2. Malii and Olive? have shown that, after setting J AAV= 0, J AM- - 0, J WV = -fY(A, CL)INdJ,,
(11) y f 0,
(12)
ho = Lo - ~!NA, Km = Auv + 4f,(A, /dlNO,, v + 0,
(13) (14)
K WV ---bJ
(15)
and
~1
+ p;w,, g,@, /-WA
(x2 - 1)‘.
+ %(A,
CL)INJ’p,
A + ~1.
We have used the above relations with the Slater coefficients from Sasaki’s program to generate vector coupling coefficients for thef-electrons inf” and the interaction of d- and&electrons in d’f” for the highspin, high-orbital-angular-momentum states of configurations with these open shells. They are given in Tables I and II. Orbital expectation values of powers of r are
141 (6)
with the Slater integrals F,(A, p) and G,(A, p)
(4~ IrO14~) = C CA~~~~~R!$A~,
(16)
P.Q
= f~trlIf~trlIf~tr~lf,tr~)tr~~r~+:+l)rfrtdrtdrs (7) I andfA(r) the radial dependence of the open-shell orbital of symmetry A. This same energy, Eq. (6), in the RoothaanBagus formalism5 is
where Rlpd.&, =
O”drr”+zRb( r)R kQ(r) I0
= NN’(n (5
200
Atomic
Data and Nuclear
+ n’ + a)! +
~r)n+7l’+u+l
Data Tables,
*
Vol. 26, Nos. ~3’4. May/July
(17)
1981
A. D. MCLEAN
TABLE
and R. S. MCLEAN
Roothaau-Hartree-Fock
Atomic Wave Functions, Z = 55-92
I. Vector Coupling Coefficients for High-Spin, High-Angular-Momentum States off” Configurationsa
K330
KFFO f’(2F) f2(3H) f3(41) f4(%) f5(‘jH) +6(‘F) f’(%) f”(‘F)
f9t6H) fqq f”(41) f’2(3H) f ‘3(2F)
-1.8571428571 -0.8571428571 -0.5238095237 -0.3571428571 -0.2571428571 -0.1904761905 -0.1428571429 -0.1071428571 -0.0793650793 -0.0571428571 -0.0389610390 -0.0238095238 -0.0109890110
K332
K334
ICFFZ
K336
KFF4
0.038095238 1 -0.0730158730 -0.0902998236 -0.0674603 175 -0.0436825397 -0.0359788360 -0.0380952381 -0.0202380952 -0.0134822653 -0.0107936508 -0.0067165158 -0.0020282187 0.0902254156
IiFF6
0.0259740260 -0.0208579299 -0.0315711225 -0.0291223928 -0.0251554506 -0.02453 10245 -0.0259740260 -0.0137987013 -0.0077640280 -0.0046595828 -0.0023482653 -0.0005793870 0.0001536925
The upper cohunn headings are KAp,, Eq. (81, the lower are their identification tabulations.
In Eq. (17) the unprimed normalization constant N (Eq. (3)) and radial parameters n and 5 come from RAP,; the corresponding primed quantities come from R,,. Rf&, becomes infinite when (a + 2) < 0; thus, KS:,, is infinite, and there are no tabulations of ($J1r+ 14) for s-orbitals . The orbital expectation values ( +ti(r 1ra 14&i) are independent of p and contain no dependence on A other than that in the radial expansion coefficients. Calculation of electronic interactions with nuclear electronic quadrupoles and magnetic hyperfrne effects requires expectation values of operators (3 co& - 1)/2r3 and sin2f3/r3;there is a contribution to the orbital expectation values due to the angular integration which introduces a factor dependent on both the A and p values of the orbital. The results for these operators are 3 co&J d> ANi ( I 23
1 I
(18)
2(A2 + A - 1 + p2) = (2A - 1)(2A + 3)
(19)
iu the wavefuuction
Computational
Details
The computer program used to generate the tables is an outgrowth of that used -by Clementi and Roetti’ with changes and extensions made by several workers. The version modified by one of us (A.D.M.) to provide radial expectation values and to handle open f-shells was provided by Dr. W. Ermler. The earliest version of the program was written in the IBM San Jose Research Laboratory by Roos, Salez, Veillard, and Clementi.s The program was thoroughly checked by comparing with test calculations by means of the totally independent IBM San Jose ALCHEMY molecular programs.9 The calculations were done over the last few years, first on an IBM 360/195 and later on an IBM 360/168 computer, at the IBM San Jose Research Laboratory. Earlier tabulations are updated and extended in the present compilation.10 The DZ basis sets, composed of two basis functions per occupied atomic orbital of each symmetry, are essentially complete in their ability to describe the inner-shell orbitals. In fact, the s-set gave considerable trouble during exponent optimizatian because of near linear dependence. From the point of view of energy, the biggest deficiency in the DZ basis is in the doublezeta representation of the 4f-shell where the motion of 14 electrons is described by only two functions. However, the 4fielectrons for 2 > 70 are not even valence electrons, and from the point of view of chemical application, augmenting the diffuse (low exponent) s-functions may be of greater importance in improving the basis set than adding to the 4f-set.
+ Awi )
= X(X + 1) - 3/.L* (2A _ 1)(2A + 3) Gh&-“b~&
0.0333000333 0.0315341224 0.0199575957 -0.0033426170 -0.0229265684 -0.0314500315 -0.0333000333 -0.0176906427 -0.0070761014 -0.0005348 187 -0.0014844493 -0.0008759479 _ 0.0001970416
and (hil~lb)
201
Atomic
Data and Nuclear
Data Tables.
Vol. 26. Nos. 3/4. May/July
1061
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
TABLE II. Vector Coupling Coefficients for the d-f Interaction in the High-Spin, High-Orbital-Angular-Momentum States of dlf” Configuration9
‘322 JDF2 -0.0952380952 -0.0476190476 -0.0126984127 0.0095238095 0.0190476191 0.0158730159 0. -0.0119047619 -0.0105820106 -0.0038095238 0.0034632035 0.0079365079 0.0073260073
‘324
K323
KDFl
KDF3
-0.0043290043 0.0028860029 0.0014430014 -0.0010822511 -0.0011544012 0.0007215007 0. -0.0005411255 0.0006413340 0.ooo4329004 -0.0003935458 -0.ooo481ooo5 0.0003330003
-0.7714285714 -0.4857142857 -0.3142857143 -0.2142857143 -0.1542857143 -0.1142857143 -0.0857142857 -0.0642857143 -0.0476190476 -0.0342857143 -0.0233766234 -0.0142857143 -0.0065934066
-0.0253968253 -0.0571428571 -0.0761904762 -0.0793650794 -0.0685714286 -0.0507936508 -0.0380952381 -0.0285714286 -0.0211640212 -0.0152380952 -0.0103896104 -0.0063492064 -0.0029304029
The uppercolumnheadingsan JXp,, the wavefunction
K321
JDF4
K+
K32S
KDFS 0.0419782238 0.0393545849 0.0341073068 0.0249245704 0.0102323309 -0.0118063755 -0.0432900433 -0.0324675325 -0.0240500240 -0.0173160173 -0.0118063754 -0.0072150072 -0.0033300033
of Eq. (8). The lower headings are their identification
in
tabulations.
Adding one low-exponent basis function in each symmetry, with reoptimization of exponents, generates the TZV basis which is of near Hartree-Fock quality; although it is still deficient (by -0.03 hartree in mercury) in reproducing the Hartree-Fock energy because of the description of the 4f-electrons. One more addition of a single 4f-basis function to generate a TZV + 4f basis set does not significantly change any of the computed properties, but it reduces the error in total energy by an order of magnitude in calculations on mercury. For each basis’set variational optimization of the basis function exponents, which seeks a point in the space of the exponents at which (IX/&,) = 0 for all p, was done. Optimization is done first as a sequence of quadratic fits to the total energy determined as a function of the exponents taken one at a time in some specified order. Denoting the exponent set at the start of a cycle by the vector C and at the conclusion by 4 + A(, a series of calculations is performed at points [ + mA( to minimize the energy with respect to a scalar multiplying factor m to give a starting point for the next cycle of optimizations. The latter phase of exponent optimization is effective in speeding convergence and shaking the cyclic optimization out of undesirable local minima. For basis sets of the size used in this study, there are multiple minima of the energy in the space of the exponents which offer essentially equivalent descriptions of the electronic structure. In generating some of the TZV basis sets, we had to strike a balance between obtaining a minimum energy and keeping a triple-zeta description of the
outermost shells. In a few cases, energy minimization optimizes an outer-shell basis into an inner one because the improved description of the inner shell gains more energy than an improved description of the outer shell. In these cases we constrained the optimization to prevent this exponent drift; the flexibility of the triplezeta outer-shell description is required for any subsequent molecular calculation. We emphasize that for most cases this constraint is not necessary; for heavy atoms, the accumulation of double-zeta functions for several shells gives a near-complete description of the inner shells. Thus, we have no trouble with s- and p-electrons, only sometimes with d andf. Accuracy For a given DZ basis, with a specific choice of n-values (Eq. (3)), there must be a best possible energy, but this is difficult to find because of multiple energy minima in the space of the exponents. However, experience has shown that these minima are essentially equivalent in their description of the electronic structure so that their existence does not pose a serious problem. More limited experience indicates that the traditional choice of n-values, discussed earlier, is as effective as any other choice. We estimate that our DZ energies are within l-2 millihartrees of the best possible DZ energy, that orbital energies are converged to two decimal places, and that radial expectation values are converged to four significant figures possibly decreasing to three for the outermost orbitals. Any error in these DZ properties is at least an order 202
Atomic
Data and Nuclear
Data Tables.
Vol. 26, Nos. 314, May/July
1981
Roothaan-Hartree-Fock
A. D. MCLEAN and R. S. MCLEAN
Atomic Wave Functions, 2 = 55-92
TABLE III. Properties of Ground-State Hg from Basis-Set Expansions and Numerical Hartree - Fock and Dirac- Fock Calculations
Wavefunction TZV+4F
property DZ” Energy Orbital Energies
-18408.48705 IS 2s 3s 4s
TZV8 -18408.96673
- 18408.98443
NH@
NDP
-18409.99
-19623.5
-2778.64479 -470.69099 -113.06366 -25.5 1975 -4.15797 -0.25711
-2778.67614 -470.73162 -113.13264 -25.56998 -4.18086 -0.26103
-2778.67858 -470.73495 -113.13642 -25.57302 -4.18161 -0.26082
-2778.639 -470.7341 -113.1363 -25.5733 -4.1820 -0.2610
-3074.235 -550.25 12 -133.1131 -30.64834 -5.10306 -0.32804
-452.13873
-452.17678
-452.17988
-452.1794
3P 3P’ 4p 4P’ sp. 5P
-104.26851
-104.33648
-104.34034
-104.3405
-21.64625
-21.69553
-21.69852
-21.6989
-2.82970
-2.84977
-2.85048
-2.8508
-455.1564 -526.8528 - 106.5450 -122.6384 -22.18857 -26.12401 -2.84195 -3.53789
3d 3d’ 4d 4d’ 5d 5d*
-88.07614
-88.14103
-88.14509
-88.1452
-14.55962
-14.60644
-14.60930
-14.6096
-0.69991
-0.71329
-0.71388
-0.7142
-4.93020
-5.00825
-5.01189
-5.0124
0.01892 0.0796 1 0.2004 1 0.43940 1.01211 3.32383
0.01892 0.07962 0.20041 0.43929 1.01026 3.32865
0.01892 0.07962 0.20041 0.43929 1.01020 3.32803
0.01892 0.07961 0.2004 1 0.43929 1.01019 3.32842
0.01659 0.06922 0.17979 0.39904 0.91518 2.84340
0.06734
0.06734
0.06734
0.06734
0.19109
0.19110
0.19109
0.19109
0.44345
0.44333
0.44332
0.44332
1.09750
1.09547
1.09538
1.09540
0.06563 0.05700 0.18612 0.17040 0.43398 0.40156 1.07915 0.98713
0.16701
0.16702
0.16701
0.16701
0.45050
0.45036
0.45034
0.45034
1.43014
1.43295
1.43226
1.43268
0.46380
0.46877
0.46923
0.4692 1
5S
66 2Pd
2P’
4f
4f’
IS
2s 3s 4s 5s 6s 2P 2P’ 3P. 3P 4P. 4P 5P 5d 3d 3d’ 4d 4d’ 5d 5d* 41 41’
203
Atomic
Data and Nuclear
Data Tables,
-86.02006 -89.43668 -14.05255 -14.79671 -0.57465 -0.65007 4.31166 -4.47286
0.16704 0.16225 0.45248 0.44158 1.49875 1.43117 0.48315 0.47672
Vol. 26, Nos. 3/4, May/July
198
A. D. MCLEAN
aod R. S. MCLEAN
Rootbaau-Hartree-F
TABLE
Atomic Wave Functions. 2 = 55-92
III-Continued
Wavefunction
c?>
DZ’
TZV
0.00048
1.14731 12.68716
O.OOQ48 0.00743 0.04577 0.21719 1.14300 12.80227
0.00048 0.00743 0.04577 0.21719 1.14288 12.79066
0.00048 0.00743 0.04577 0.21719 1.14285 12.79939
0.00038 o.oos74 0.03712 0.17977 0.93961 9.35291
2Q. 2Q
0.00549
osKM49
0.00549
0.00549
3Q.
0.04222
0.04222
0.04222
0.04221
0.22294
0.22282
0.22281
0.22281
1.35944
1.35528
1.3s500
1.35516
0.00525 0.00406 0.04024 0.03391 0.21406 0.18350 1.31850 1.10187
0.03256
0.03256
0.03256
0.03256
0.23379
0.23366
0.23364
0.23364
2.38098
2.41020
2.40674
2.40982
0.25324
0.26235
0.26341
0.26337
79.44732 18.73219 7.28395
18.73184
1s 2s 3s 4a 51
6~
3Q 4Q 4Q' SQ SQ' 3d 3d' 3 Sd
0.00743 0.04577 0.21730
Tzv+4r
N&J
NDF
5d’ 4f
4f’ Cl/r>
1
0.28069 0.27330
0.37552
7.28395 3.19305 1.30247 0.37606
79.44732 18.73182 7.28398 3.19312 1.30257 0.37604
79.4479 18.7319 7.2840 3.1931 1.3026 0.3761
97.49815 24.02617 8.82984 3.72018 1.48774 0.45063
18.73868
18.73843
18.73841
18.7385
7.22569
7.22562
7.22566
7.2258
3.10166
3.10272
3.10278
3.1027
SQ,
1.18985
1.19278
1.19287
1.1929
19.40109 23.93842 7.55016 8.72808 3.21899 3.60824 1.22333 1.36420
3d
7.14395
7.14351
7.14353
7.1436
2.91818
2.91950
2.91962
2.9196
0.90773
0.91011
0.91040
0.9103
2.59062
2.58400
2.58344
2.5835
ii 3s 4s 5s 6s
2Q. 2Q 3Q 3Q= 4Q 49.
3.19211 1.29968
79.4473
0.03264 0.03092 0.23636 0.22S32 2.66446 2.41921
SQ
3d' 4d 4d* Sd
5d’
204
Atomic
Data and Nuclear
Data Tables.
7.16217 7.42922 2.92077 3.01389 0.87710 0.92012 2.52127 2.55711
Vol. 26. Nos. 314, May/July
1981
Roothaan-Hartrec-Fock
A. D. MCLEAN aud R. S. MCLEAN
TABLE
ROpeflY
DZs Is 2s 3s 4s 5s 6s
12651.2180 1418.3996 324.1374 82.1069 15.5064 1.1063
zp. 2P 3P 3P’ 4P 4P. SP.
Atomic Wave Functions, Z = 55-92
III-Continued
Wwefunction Tzv+4p
TZV
NH@
12641.2277 1418.3607 324.1339 82.1524 15.5883 1.1099
12651.3261 1418.3251 324.1524 82.1578 15.5916 1.1095
12652.40 1418.381 324.1371 82.1670 15.5936 1.1098
472.9677
472.9580
472.9578
472.9835
108.4082
108.4096
108.4115
108.43S4
27.3267
27.3461
27.3469
27.3423
4.8475
4.8733
4.8739
4.8737
62.7178
62.7129
62.7137
62.7 169
14.8491
14.8611
14.8620
14.8623
1.8415
1.8563
1.8575
1.8573
8.2101
8.2189
8.2186
8.2196
5P 3d
3d* 4d 4d* 5d Sd’ 4f 4f* Cl/?>
2p 2P. 3P. 3P 4P 4P* 3P 3P’ 3d
3d’ 4d 4d* Sd Sd* 4f 4f.
NDFG 23710.10
3383.351 775.5946 196.2944 38.2294 3.3482 J 14.848 1063.752 122.8150 249.3 105 31.1S68 62.1760 5.5194 11.0770
63.2936 69.2457 15.0434 16.4777 1.7591 1.9998 7.8655 8.1064
18104.492
18104.292
18104.419
18110.78
21389.21
3970.238
3970.821
3971.006
3975.73
5021.11
941.902
942.805
942.813
942.46
1211.71
149.848
150.637
150.633
150.60
194.73
705.896
705.930
705.967
706.21
148.943
149.024
149.030
149.09
14.520
14.689
14.701
14.71
721.72 873.20 154.08 190.54 14.179 18.571
32.362
32.804
32.836
32.86
30.975 32.598
*Results from the present compilation. DZ denotes a double zeta expansion (Table 80-3). TZV improves the description of the outer shells by addin one more low exponent basis function of each symmetry type (Table 80-4). TZV+U adds one more 4f function to the TZV basis (Table 80-5). %umerlcai Hartree-Fock results. Ref. 2. Dirac-Fock results. R f. 11. > 0 relativistic spinors j= t +I/2 (no asterisk) and j=e-l/2 (asterisk) are determined.
205
Atomic
Data and Nuclear
Data Tables.
Vol. 26. Noa. 314, May/July
1081
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
of magnitude less than the changes resulting from increase of basis-set size from DZ to TZV. Our TZV energies and properties are estimated to be similarly close to the best possible TZV values in those cases where constraints are not imposed on exponent drift. All TZV calculations are much closer to the Hartree-Fock limit. The most important statement on accuracy comes from comparing our well-optimized DZ and TZV resuits with the complete-basis Hartree-Fock values; for I-&(‘S), this is done in Table III, which also shows the effect of adding one more f-function to the TZV basis. We believe that the convergence demonstrated in Table III will be typical for all our wave functions. The last column of Table III presents the Dirac-Fock results of Desclauxll to show the dramatic changes in structure that come from using a relativistic Hamiltonian. It is clear that relativistic calculations are absolutely necessary for heavy-atom systems. We believe it is important to understand how relativistic results differ from nonrelativistic both qualitatively and quantitatively as we move through the periodic table. We hope that this tabulation serves to stimulate activity in molecular applications.
References
1. E. Clementi and C. Roetti, ATOMIC DATA AND NUCLEAR DATA TABLES~~, 177(1974) 2. J. B. Mann, Jr., Los Alamos Scientific Laboratory Report LA 3690, Atomic Structure Calculations. I. Hartree-Fock Energy Results for the Elements Hydrogen to Lawrencium (1%7); and Report LA3691, Atomic Structure Calculations. II.
Atomic Wave Functions, Z = 55-92
Hartree -Fock Wavefunctions and Radial Expectation Values: Hydrogen to Lawrencium (1%8)
3. C. Froese Fischer, Atomic Data 4,301(1972), with corrections ~~ATOMICDATAANDNUCLEARDATA TABLES 12, 87 (1973) 4. Y. S. Lee and A. D. McLean, unpublished 5. C. C. J. Roothaan and P. S. Bagus, Methods in Computational Physics (Academic Press, New York, 1963), Vol. 2 6. F. Sasaki, Znt. J. Quantum Chem. 8, 605 (1974) 7. G. L. Malli and J. F. Olive, Vector Coupling Coeficients for Atomic Self-Consistent Field Calculations, Laboratory of Molecular Structure and
Spectra, Technical Report 1962-3, part 2, The University of Chicago, p. 258 8. B. Roos, C. Salez, A. Veillard, and E. Clementi, A General Program for Calculati&of Orbitals by the Expansion Method,
Atomic SCF
Technical Report RJS18, IBM Research Laboratory (1968) 9. The ALCHEMY programs are general SCF, MCSCF, and CI molecular programs written by the computational chemistry staff of the IBM San Jose Research Laboratory Analytical Atomic 10. A. D. McLean, Nonrelativistic SCF Wavefunctions and Radial Expectation Values, Z = 55, 56, 71-80, Technical Report
RJ2295, IBM Research Laboratory (1978); A. D. McLean, Nonrelativistic Analytical Atomic SCF Wavefunctions
and Radial
Expectation
Values,
Z = 81-88, Technical Report RJ22%, IBM Research Laboratory (1978) 11. J. P. Desclaux, ATOMIC DATA AND NUCLEAR DATA TABLES 12,311(1973)
Atomic
Data and Nuclear
Data Tables,
Vol. 28. Nos. 3/4, May/July
lW1
A. D. MCLEAN
Roothaan-Hartree-Fock
and R. S. MCLEAN
EXPLANATION Order
Atomic Wave Functions, Z = 55-92
OF TABLES
of Tables
Our results are presented in order of atomic number, and.for ease of reference our Table numbers contain the atomic number. Thus, all mercury (Z = 80) wave functions are in Tables 80-n with n counting through the different wave functions. Positive-ion wave functions are given before neutral-atom wave functions, and in the case of the single negative ion included in the tables, that of astatine, the negative-ion wave functions follow the neutral. When, for a given atom or ion, two electronic configurations are calculated, wave functions for the configuration with the lower HartreeFock energy are given first. When, for a given atom or ion, two multiplets of an electronic configuration are calculated, wave functions for the one with the lowest Hartree-Fock energy are given first. When, for a given electronic state, more than one basis set is used, wave functions are given in order of increasing size of basis sets.
Thefirst block of each table gives the electronic configuration, basisset dimension, symmetry, and vector coupling coefficients for the designated multiplet and total energies. Example from Table 84-2 Polonium + Quartet S. TZ outer shellsa Nuclear Charge = 84.000000a No. of Electrons = 83 Symmetry
Species
SPDF
Number of basis function@ Number of closed shellsC Open shell occupationC
13 6 0
11 7 43 300
3 1
Vector Coupling Coefficientsd KPPQ = -0.33333333333 KPP2 = -0.13333333333 Total Energy -20676.21478479
Potential Energy -41352.34027992
Kinetic Energy 20676.12549513
Virial Theoreme -2.OOOOO
” PO+(a) b Basis-set size c Configuration ---6s’~--5ps 6p5---5d1°4f I4 d Open-shell vector coupling coefficients, notation of text and Refs. 5 and 7. See Eqs. (13h (14) c Potential energy/kinetic energy. Fully optimized wave functions have a value of -2. All energies are in hartrees
207
Atomic
Data and Nuclear
Data Tables.
Vol. 26, Nos. 3i4, Mny/July
IS3
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, 2 = 55-92
The following blocks, one for each symmetry, give orbital expectation values and expansion coefficients. Example from Table 84-2 for d-Symmetry
D Basis, Orbitals, and Expectation Values 3D 4D 5D ORB ENERGY - 103.164692 - 19.263453 -2.056633 0.157308 0.415821 1.148880 W (R**2) 0.028861 0.198860 1.509722 7.576652 3.160904 1.129148 (l/R) (l/R**2) 70.469014 17.341168 2.851790 (l/R**3) 839.315141 185.392353 25.290088 3D 33.824030 -0.149928 0.071528 -0.025944 3D 21.571628 -0.834702 0.480393 -0.18483 1 4D 14.379864 -0.065815 -0.454602 0.219674 4D 9.987310 0.015286 -0.690272 0.291961 5D 6.658163 -0.004267 -0.031703 -0.496864 5D 4.335265 0.002143 0.003854 -0.565212 5D 2.796994 ,o.q00672 -0.000752 -0.120579 -nh Orbital d434 $444 4&O exponents expansion expansion expansion coefficients coefficients coefficients P The 3d atomic orbital expanded in five Slater-type d-functions of an optimized TZV basis is $(3d) = -0.149928 3d(33.82403) - 0.834702 3d(21.571628) - 0.065815 4dt14.379864) + 0.015286 4d(9.987310) - 0.004267 5d(6.658163) + 0.002143 5d(4.335265) - 0.000672 5d(2.7%994). The basis functions nh(<), 3d(33.82403), etc., have the radial dependence N,+z+ defined in Eq. (3). The orbital energy for #(3d) is - 103.164692hartrees. (P) Expectation values of P are in atomic units (1 a.u. = a0 = 0.52917706(44) x 1Oe8cm).
Atomic
Data and Nuclear
Data Tables.
Vol. 28, Noa. 314. May/July
1981
A. D. MCLEAN
Roothaan-Hartree-Fock
and R. S. MCLEAN
Atomic Wave Functions, 2 = 55-9’2
TABLES. Basis-Set Expansions See page 207 for Explanatiom
TABLE
CESIUH+ SINGLET
55-1
S. DOUBLE ZETA
SYMETRY SPECIES NUMBER OF 8ASIi FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 55.000000 NO.OF ELECTRONS= 54 POTENTIAL
TOTAL ENERGY -7553.79326541 S BASIS,ORBITALS
of Tables
ENERGY
-15107.59073552
AND EXPECTATION
VIRIAL
KINETIC ENERGY 7553.79747012
S
16 5 0
THEOREM
-1.99999944
VALUES 5s
ORB.ENERGY
4*‘2>
WR**2>
1s 56.214333 1s 37.443464 25 25 3s 35 4s 4s 5s 55
27.469696 23.892906 17.824286 12.650645 7.410618 5.354037 3.682564 2.380983
P BASIS,ORBITALS ORB-ENERGY
2P 2P 3P 3P 4P 4P 5P 5P
-198.3::916 0.118528
0.016498 12.554951 639.479676
54.467955 5951.507215 0.883327 0.137488 -0.083587 0.068424 -0.010114 0.003757
0.027728 0.522821 -0.190479 -0.045111 0.006257
-0.001110
-0.000889
0.000769 -0.000247 0.000083
0.000671 -0.000208 0.000065
-1.025549
AND EXPECTATION -186.4;;514 0.101038 0.012405 12.537866
-42.8;;036
0.311597 0.110752 4.633539
131.474997 -0.009544 -0.240116 -0.413387 1.183772 0.035803 -1.234641 -0.038263 0.013164 -0.002838 0.000886
-37.7::087 0.302188 0.105677 4.552154
-6.9:!806 0.751156 0.640202 1.804057
43.598526 1056.511894
207.627850
35.036432 23.652788 12.656603
-0.147758 -0.855518 -0.041696
-0 -030929 -0.501342
-0.009939 -0.235255
11.190568
0.029521 -0.001609
8.087281 5.586627 3.375538 2.063752
ORB.ENERGY
4**2>
20.224082
11.916855 7.095698 4.363055
0.000249 0.000028
-0.000019
-8.8::243 0.722858 0.588280
-1.405029 1.839354 3.803077
1.903178
0.699139 4.163199
28.707509
-0.001859 -0.115276
0.000070 0.043949 0.059267
-0.184764
0.547941 0.129759 -0.909514 8%::: -Oh01841 0.001686
-0.192782 -0.067586 0.379635 -0.467811 -0.095222 0.692039 0.454789
VALUES
212.623979 5492.825245
0 BASIS,ORBITALS
30 30 40 .~ 40
-1272.9::392 0.027624 0.001021
1.028509 0.077649 0.054868 -0.011665 0.002261
-0.000811
9.318696
0.331933 0.396269 -0.566910 -0.678084 -0.016204 0.001663
-0.8::427 2.101238 5.003304 0.608155 1.217415 23.327401 -0.003353 -0.079008 0.076693 0.192407 -0.273950 -0.227662 0.620727 0.515130
AND EXPECTATION VALUES 30 -28.400668 -3.5!:565 0.273065 0.830625 0.087829 0.798651 4.414773 1.578797 24.234040 4.471329 172.701623 27.021144 0.210358 0.805102 0.044554 -0.008603
-0.092609 -0.352543 0.601425 0.543499
209
Atomic
Data and Nuclear
Data Tables.
Vol. 28, Nos. 3l4. May/July
1%
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations
TABLE CESIUH+
SINGLET
55-2
S. TZ OUTER SHELLS
SYMETRY SPECIES NLMER OF BASIS FUNCTIONS= NLMBER Of CLOSE0 SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 55.000000 NO.OF ELECTRONS= 54 TOTAL ENERGY -7553.80499562 S BASIS,ORBITALS ORB.ENERGY
1s 56.298677 1s 37.532876 2s 25 3s 3s 4s 4s 5s 5s 5s
29.450168 24.023001
15.329424 13.222807 7.846238 6.325925 5.390462 3.510614 2.317725
P BASISJMIBITALS ORB.ENERGY
2P 3P 2P 3P 4P 4P 5P 5P 5P
35.064052 12.460038 23.644180
11.363909 8.055023 5.675050
-1272.9::530 0.027624
-198.3::901 0.118527
0.001021
0.016498 12.554996
54.467946
5951.576089
639.484056
x*x:
0.874953 0.148780 -0.060749 0.040442
-01082387 -1.138999 -0.072886
-0.018116 0.014554
0.043192 -0.008759 0.008395
-0.005320 0.005337 -0.001854 o.ooo451 -0.ooo114
-0.002721 O.OOO612 -0.ooo153
AND EXPECTATION VALUES 2P 3P -186.463713 -37.773144 0.101038 0.302191
0.012405 12.537856
0.105679
212.626712
4.552095 43.598463
5493.151682
1056.625896
-0.147612 -0.047124 -0.856118 0.034650 0.000205
-0.031349 -EE: -0:152W6 0.080903
-p;;;
4.429683 3.013474
-0.000462
-0:004545
1.947091
ORB.ENERGY
4*+2>
21.522235
12.632830 8.895374 6.074621
3.869931
O.WO129 AND EXPECTATION -28.4::014 0.273096 0.087~40 4.414530 24.238029
172.906535 0.150238 O.BO81a6 0.111672
-0.016985 0.003286
KINETIC ENERGY 7553.77531005
s
P
5 0
II
5
11 s 0
:
VIRIAL THEOREM -2.00000393
VALUES
-0.001259 0.006929
0 BASIS,ORBITALS
30 3D 40 40 40
POTENTIAL ENERGY -15107.58030567
AN0 EXPECTATION
of Tables
O.oollW
-42.8%40
0.311601 0.110754 4.633508
131.488796 -0.012803 -0.233294 -0.261357 1.007165 0.429678 -1.585022 -0.097898 0.060355 -0.014795
0.002606 -0.OW51B
-6.9:!592 0.751116 0.640140
1. a04207 9.320585 207.688074 -0.010056
-0.235179 0.373367 0.343241
-0.540043 -0.676002 -0.026997 -0.005921 0.000881
-a.e::192 0.722814 0.588208
-1.4::242
1.903340 28.718636
1.839138 3.802678 0.699256 4.166522
-0.004158 -0.110692
0.001588 0.041056
-0.131016 0.488799 0.514161 -1.288747 0.534592 0.616271 0.083577
0.002743 o.wo409
0.050566 -0.184643 -0.221603 0.532365 -0.242216 -0.349000 0.094489 0.696640 0.390023
-0.8~~542 2.101356 5.007273 0.608372 1.218889 23.341861 -0.002964 -0.079960
0.113769 0.142779 -0.226949 -0.290386 0.167061 0.622491 0.387567
VALUES -3.5ii586 0.831407 0.801415 1.578549 4.470902 27.007491 -0.062772 -0.366667 0.115514
0.701787 0.314634
210
Atomic
Dsta and Nuclear
Dnta Tables,
Vol. 26, Nos. W4. May/July
1881
A. D. MCLEAN
Roothaan-Hartree-Fock
and R. S. MCLEAN
Atomic
Wave
Functions.
Z = 55-92
i
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE CESIUM
S*l
DOUBLET
55-3
S. DOUBLE ZETA
SYMMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 55.000000 NO.OF ELECTRONS= 55
1; 5 1
VECTOR COUPLING COEFFICIENTS KSSO- -1.00000000000 TOTAL ENERGY -7553.91633764 S BASIS,ORBITALS ORB.ENERGY
1S 1S 2S 2s 3S 3S 45 4s 55 55 6S 65
56.219117 37.566991 27.460490 23.778942 16.977234 12.653157 7.456744 5.377117 3.721135 2.423665 1.393434 0.823743
P BASIS,ORBITAI ORB.ENERGY
2P 2P 3P 3P 4P 4P 5P 5P
34.957172 23.628775 12.658736 10.663267 8.126391 5.572441 3.333120 2.018224
0 BASIS,ORBITALS ORB.ENERGY
30 30 4D 40
20.217897 11.914584 7.098909 4.364964
POTENTIAL ENERGY -15107.83816314
AND EXPECTATION
KINETIC ENERGY 7553.92182550
VIRIAL THEOREM -1.99999927
VALUES
-1272.7:;389 0.027624 0.001021 54.467993 5951.541646
-198.&03 0.118528 0.016498 12.554962 639.472269
-42.6;;380 0.311597 0.110752 4.633564 131.474643
-B.6i:OOO 0.722843 0.588260 1.903240 28.710936
5s -1.230085 1 .a39823 3.807318 0.699226 4.166382
-0.lE339 6.300282 44.784803 0.192032 0.238682
0.882875 0.137446 -0.078024 0.062782 -0.010446 0.004902 -0.001348 0.000950 -0.000344 0.000145 -0.000041 0.000017
0.026690 0.522125 -0.200644 -1.018928 -0.041950 0.009364 -0.001300 o.ooo943 -0.000323 0.000128 -0.000036 0.000014
-0.008941 -0.240028 -0.395433 1.170251 0.031975 -1.236215 -0.038588 0.013291 -0.003226 0.001242 -0.000317 0.000125
-0.002052 -0.114369 -0.190982 0.560476 0.141599 -0.933187 0.871850 0.369348 -0.003991 0.002800 -0.000525 0.000199
0.000292 0.043351 0.065389 -0.202195 -0.073340 0.391375 -0.458428 -0.111639 0.671821 0.475370 0.008327 -0.000950
-0.000285 -0.009399 -0.018142 0.049666 0.013953 -0.086381 0.101009 0.035248 -0.205988 -0.035690 0.502926 0.606831
-37.5:!234 0.302189 0.105677 4.552137 43.598242 1056.510069
-6.7&I 0.751193 0.640271 1.803983 9.317930 207.586391
-0.6:!043 2.110292 5.055120 0.606118 1.209562 23.162194
-0.031671 -0.501120 1.047268 0.060838 0.052265 -0.010359 0.001991 -0.000717
-0.010031 -0.235667 0.406723 0.338890 -0.588660 -0.675279 -0.015224 0.001638
-0.003420 -0.078771 0.109103 0.168978 -0.288261 -0.218935 0.651059 0.492544
.S AND EXPECTAl 'ION -186.3:!565 0.101038 0.012405 12.537857 212.623097 5492.721056 -0.150091 -0.853625 -0.033073 0.021827 -0.002179 0.000356 O.OOOOO6 -0.000011 AND EXPECTATION
VALUES
VALUES
-28.2E792 0.273067 0.087830 4.414748 24.233799 172.698631
-3.3:!063 0.830659 0.798702 1.578720 4.470891 27.017221
0.210669 0.804856 0.044422 -0.008535
-0.092709 -0.352520 0.600560 0.544446
211
Atomic
Data and Nuclear
Data Tables.
Vol. 28, Nos. W4. May/July
198
A. D. MCLEAN
and R. S. MCLEAN
Roothan-Hartret-Fock
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations
TABLE
55-4
S*l DOUBLET S. TZ OUTER SHELLS
CESIUN
SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 55.ODOOOO NO.OF ELECTRONS= 55 VECTOR COUPLIN6
of Tables
D 1: 5
!
1
t
z 0
COEFFICIENTS
Ksso= -1 .ooOOOOOOOO0 TOTAL ENERGY
POTENTIAL ENERGY -15107.83717002
-7553.92861872 S BASIS,ORBITALS
AND EXPECTATION
KINETIC ENERGY 7553.90855131
VIRIAL THEOREM -2.00000266
VALUES 5s
ORB.ENERGY
1s 56.231412 1s 37.677605 25 2s
27.973164 23.863798
35
16.001179
35 45 45 5s 5s 65 6s 6s
12.807302 7.762725 5.858331
3.958971 2.658013
1.914259 1.179036 0.755359
P BASIS,ORBITALS ORB.ENERGY
2P 2P 3P 3P 4P 4P 5P 5P 5P
-198.1::930 0.118527
0.016498
54.467951 5951.522031
12.555617
0.881328 0.139127
131.473681
0.025934
-0.009408 -0.238121 -0.355018 1.120451 0.109646
-0.068453
0.052196 -0.011899
-0.048622
-1.075688 0.019049 -0.002923 0.002055 -0.000684
0.000319 -0.000140
0.000389 -0.000~68 0.000076 -0.000027
0.000063 -0.000023
0.311599 0.110754 4.633516
639.475914 0.521186 -0.144088
0.007538 -0.002060 0.001482 -0.000536
-42.6::551
AND EXPECTATION VALUES 2P -186.315708 -37.5;!318 0.101037 0.302193 0.012405 0.105680 12.537935 4.552068 212.627204 43.598611
-1.298637 -0.050555 0.018374 -0.004262 0.002272 -0.000898 0.000392
-0.000139
-6.7:!268 0.751147 0.640207 1.804087
9.319905
5493.131221
1056.678721
207.800888
35.277273 23.712551
-0.141173 -0.861413
-0.029711 -0.500331
11.909618
-0.079917
10.450074 10.006642 6.171388 4.133844 2.789953
0.080521 -0.016017
-0.010355 -0.232720 0.314764 0.621541 -0.497147
1.801024
D BASIS.ORBITALS ORB.ENERGY
4**2>
30 30 4D 4D 4D
-1272.7:;492 0.027624 0.001021
21.563487 12.657761 8.945584 6.058925 3.844229
2.163141 -1.339829 0.355369
0.000091
-0.013639
0.000238
0.004711 -0.002485
-0.000180 0.000061 AND EXPECTATION -28.2;:073 0.273097 0.087842
4.414522 24.237968
0.000711
-0.929133 -0.068989 0.010487 -0.002435
-8.6::254 0.722793 0.588175
-1.231495 1.839371 3.805443 0.699409 4.169404
1.903419 28.717551 -0.002338 -0.113358 -0.175661 0.542452 0.236710 -1.030800 0.676972 0.555202 0.014134 -0.001630 0.000808 -0.000305
0.000100
-0.1::627 6.304669 44.953018
0.192166 0.239612
0.000643 0.042547 0.064327 -0.201140
-0.000121 -0.009671 -0.014314 0.045249
-0.112599
0.026484 -0.099676 0.082486 0.055398
0.432774 -0.351104 -0.238624 0.540133 0.586105 0.051434 -0.003317 0.001226
-0.149640 -0.125989 0.156234 0.571532 0.423044
-0.6:!348 2.111006 5.064705 0.606312 1.211245 23.200255 -0.003150 -0.078657 0.053942 0.302615 -0.219290 -0.389365
0.236781 0.643721 0.284540
VALUES -3.3::334 0.831517 0.801723 1.578436 4.470384
172.907181
27.002393
0.148551 0 307592 0.113687 -0.016558 0.003297
-0.061879 -0.366941 0.113244 0.711323 0.306992
212
Atomic
Data and Nuclear
Data Tables.
Vol. 28. Nos. 3’4. May/July
IS81
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
TABLES.
Atomic Wave Functions. 2 = 55-92
Basis-Set Expansions of Tables
See page 207 for Explanations
TABLE
56-1
S*l DOUBLET S. DOUBLE ZETA
BARIUM+
SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 56.000000 NO.OF ELECTRONS= 55
1; 5
1
VECTOR COUPLING COEFFICIENTS KSSO= -1.WWOOWOOO TOTAL ENERGY -7883.37629694 S BASIS,ORBITALS ORB.ENERGY
POTENTIAL
AND EXPECTATION
-207.33:772 0.116270 0.015874 12.800234 664.593050 0.026981 0.522880 -0.098892
57.257003
0.881235
IS
38.225356
0.140204
2s 25 3s 35 4s 4s SS 5s
27.937702 24.756005
65 65
12.972578 7.510425 5.326364 3.953863 2.675364
1.712483 1.142034
P BASIS,ORBITALS ORB.ENERGY CR>
2P
35.314543
-0.101426 0.086607 -0.010836 0.003248
AND EXPECTATION 2P
-195.245463 0.011924 12.784507 221.018004 5818.789068
0.017156 0.001671 -0.001069 0.000333 -0.000133
3D 3D
20.715875
12.252829 4D 7.357644 4D 4.597533
0.295277
0.100883 4.659648 45.645528 1128.723328
-0.157012
AND EXPECTATION -30.5:!798 0.266200
0.083402
-0.033072 -0,503744 0.111904 0.997709 0.057549 -0.015473 0.002883
-0.001029
-45.4::830 0.304800
0.105961 4.739941 137.576558
-9.7:;941 0.701638 0.554048
1.964369 30.642797
-0.009478 -0.240561 -0.528412 1.287382 0.061353 -1.245545 -0.041045 0.017329 -0.005972
-0.001202 -0.117843
-0.914318 0.953147 0.287498 -0.009292
0.002444 -0.000758 0.000304
0.003728 -0.000714 0.000244
-7.7:;385 0.726960 0.599274
-1.oz731
-0.215748 0.571252 0.141504
5s -1.701080 1.722475 3.324314 0.749454 4.872783 -0.owo77 0.046932 0.073343 -0.210305 -0.072635 0.396909 -0.517863
-0.091333 ZiE 0:009161 -0.000185
-0.3::573 4.692678 24.504377 0.261489 0.545701 -0.000059
-0.015039 -0.025425 0.070043 0.023183 -0.129396 0.171473 0.036735 -0.291023
-0.089179 0.550936 0.544658
1.866704. 9.973781 227.523085
1.937628 4.236231 0.662030 1.462856
29.152588
-0.011679
-0.004260
-0.237822 -0.260202 0.965484 -0 * 549450 -0.660954 -0.017183 0.002095
-0.281159
-0.085190 -0.146982 0.420420 -0.245557 0.656908 0.489733
VALUES
-4.1:!318 0.795622
0.731525 1.647866
4.524895 25.436401 185.478647
4.855452 30.224815
0.206486 0.807549
-0.092450 -0.363899
0.045003 -0.008752
VIRIAL THEOREM -2.00000084
VALUES
-40.2;;917
0.099069
3P 4P 4P 5P 5P
ORB.ENERGY
O.OW160 -0.owo55 0.000023
-0. WOO76 0.000032
-0.846990 -0.030281
0 BASIS,ORBITALS
-0.056041 0.004866 -0.000832 0.000765 -0.000366
0.000973 -0.000479 0.000221
2P 24.047131 3P 13.8OOWO 12.750401 8.111346 5.796638 3.574133 2.259693
-1.104593
-0.001169
KINETIC ENERGY 7883.36963624
VALUES
-1322.2;:986 0.027125 0.000984 55.466671 6171.513438
1s
19.107490
ENERGY
-15766.74593318
0.601073 0.544302
213
Atomic
Data and Nuclear
Data Tables,
Vol. 28, Nos. 314. MayiJuly
1981
A. D. MCLEAN
Roothaan-Hartme-Pock
and R. S. MCLEAN
Atomic Wave Ffunctions, 2 = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE
56-2
S*l DOUBLET S. TZ OUTER SHELLS
BARIUM
SYIMETRY SPECIES MIMER OF BASIS FUNCTIONS= NUUBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE - 56.000000 NO.OF ELECTRONS= 55
1:
;
5
1
ii
VECTOR COUPLIN6 COEFFICIENTS KSSO- -1.00000000000 POTENTIAL ENER6Y -15766.74791683
TOTAL ENERGY -7883.386776% S BASIS,ORBITALS ORB.ENERGY
4**2>
1s 57.248683 1s 38.812642 2s 25 3s 3s 4s 4s 5s 5s 65 65 6s
27.755098 24.548687 16.437852
AND EXPECTATION -1322.2:415 0.027125 o.DDo984 55.466677 6171.503945
X%X . 12.8OD284 664.572772 0.022902 0.518332 -0.085211
-0.081633 0.067476 -0.011677
-1.124581
7.793887 5.816944 4.020171 2.724912
-0.W2Wl 0.601527 -0.000666 0.000441
1.961227 1.406475 1.052462
-0.052563 0.020232 -0.003311 0.002464 -0.WlW6 O.ODD643 -0.000405 o.OOD28B
-0: OODo73
-0.000104
13.055529
P BASIS,DRBITALS
0.007132
-EE:
AND EXPECTATION
4**2> 2P 2P 3P 3P 4P 4P 5P 5P 5P
35.8246% 24.202808
14.342869 13.555707
8.819160 6.394352 4.383258 3.051909 2.053781
D BASIS,ORBITALS ORB.ENERGY
4**2>
3D 3D
21.723382
12.797698 4D 8.685416 40 6.071039 4D 3.984477
0.011924 12.784618
0.100885 4.659529
221.023256
45.646102
5819.323810
1129.022903
-0.141914 -0.859409 -0.040435 0.023765
0.003239 -0.002382 0.001136 -0.DW703 0.000213
VIRIAL THEOREM -2.ODDW325
-45.4::317 0 * 304803 0.105963 4.739910 137.566433 -0.007074 -0.239400 -0.542036 1.312362 0.087757 -1.285217 -0.046885 0.018265 -0.005069 0.002972 -0.w1704 0.001175 -0.DOD420
-9.7:;567 0.701604 0.553997
1.964496 30.650716 -0.001487 -0.114705 -0.274909 0.648793 0.217611 -1.026723 0.797606 8%::: o:w1439 -0.wo414 0.000266 -0.wo103
5s -1.702119 1.722255 3.323406 0.749546 4.874923 0.000267 0.045278 0.104771 -0.250895 -0.112050 0.455222 -0.437880 -0.186942 0.634673 0.521553 0.012633 0.003065 -0.000727
-0.3::726 4.692684 24.508399 0.261498 0.545815 -0.OOW85 -0.014655 -0.034038 0.081382 0.037311 -0.149702 0.146847 0.064359 -0.266528 -; . :;;m;;
0: 547194 0.292369
VALUES
ORB.ENERGY
ENERGY
7883.36113994
VALUES
-207.3:;554
0.881102 0.137609
KINETIC
-0.029830 -0.501651 -0.836833
1.912619 0.096743 -0.027470 0.007985 -0.004233 O.Wl175
-7.7::864 0.726925 0.599228
1.866831 9.976558 227.750862
-0.011439 -0.234127 -0.933486 1.611605 -0.245683 -0.892024 -0.076835 0.013604 -0.w31w
-1 .oz739 1.937659 4.238425 0.662186 1.463952 29.179964 -0.003856 -0.084568 -0.381262 0.639784
-0.115295 -0.406160 0.216403 8. p6;:
AND EXPECTATION VALUES 3D 4Q -30.595297 -4.19iOl8
0.266225 0.083412 4.5246% 25.439278 185.638511
0.159482 0.814167 0.098276 -0.022260 0.004425
0.796217 0.733575
1.647680 4.855122 30.210833
-0.068512 -0.377250 0.187315 0.685827 0.26U32
214
Atomic
Data and Nuclear
Data Tables.
Vol. 28. Nos. W4, May/July
lW1
A. D. MCLEAN and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, 2 = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE 56-3 BARIUM
SINGLET
S. DOUBLE
ZETA
SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 56.000000 NO.OF ELECTRONS= 56 TOTAL ENERGY
POTENTIAL
-7883.52795195 S BASIS,ORBITALS
ENERGY
-15767.05252081
AND EXPECTATION
KINETIC ENERGY 7883.52456886
1; 6 0
VIRIAL THEOREM -2.00000043
VALUES 55
ORB.ENERGY
1s 1s 25 2s 35 35 4s 4s 5s 55 6s 65
57.233372 38.044430 27.987527 24.645535 19.152848 12.964381 7.498241 5.270719 3.857420 2.597580 1.588608 0.952513
P BASIS,ORBITALS ORB.ENERGY
2P 2P 3P 3P 4P 4P 5P 5P
35.334997 24.048465 13.500000 12.626688 8.132328 5.775321
3.533916 2.213392
0 BASIS,ORBITALS ORB.ENERGY
30 30 40 40
20.717658 12.253458 7.358290 4.597467
-1322.0::228 0.027125 0.000984 55.466649 6171.472915
-207. I::333 0.116270 0.015874 12.800243 664.598886
-45.2::647 0.304798 4.739976 137.579057
0.701623 0.554031 1.964442 30.645639
0.027983 0.524805 -0.141534 -1.066334 -0.054531 0.W4404 -0.000678 0.000620
-0.009873 -0.241567 -0.479789
-0.001384 -0.118357 -0.193561
0.883524 0.137969 -0.096359 0.081397 -0.010587 0.003049 -0.001023 0.000814 -0.000385 0.000169 -0.000048 0.000018
-0.000288 0.000120 -0.000034 0.000013
AND EXPECTATION -195.0:!850 0.099069
0.100884 4.659653
221.018370
45.645396
5818.879889
1128.685614
-0.156554 -0.847541 -0.038184 0.025321
-0.032831
-0.504129
-0.wo903 o.wo288
0.287276 0.823457 0.055280 -0.014034 0.002570
-0.000116
-0.000915
0.001359
AND EXPECTATION
1.242444 0.056845 -1.243813 -0.039475 0.015891 -0.005298 0.002095 -0.000538 0.000196
8E: -0: 912388 0.964233 0.277928 -0.011157 0.004235 -0.000767 0.000264
-1.511364 1.721456 3.320099 0.749969 4.881546
5.252328 31.158857 0.233611 0.403007
-0.000223 0.047575 0.060863 -0.197727 -0.073940 0.398602 -0.532030 -0.065830 0.710478 0.434554 0.003540 -0.000176
-0.000128 -0.012751 -0.020361 0.058667 0.018841 -0.109416 0.147337 0.027911 -0.272884 -0.030707 0.582415 0.529369
-0.1::209
VALUES -4O.O::512 0.295278
0.011924 12.784485
0.105960
-9.5::394
-7.5::439 0.727006 0.599357 1.866602 9.972633 227.470530
-0.9K542 1.944019 4.269532 0.660265 1.455275 28.986181
-0.011398 -0.238384 -0.243519 0.955012 -0.561065 -0.657069 -0.015438 0.001798
-0.004186 -0.085075 -0.157982 0.434399 -0.289258 -0.237289 0.680176 0.466091
VALUES.
-30.3::364 0.266201 0.083402 4.524886 25.436327 185.478347
-3.9G490 0.795682 0.731640 1.647750 4.854828 30.220132
0.206404 0.807605 0.045039 -0.008759
-0.092398
-0.363917 0.600844 0.544543
215
Atomic
Data and Nuclear
Data Tables,
Vol. 26. Nos. 3/4, May/July
1W.r
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartme-Fock
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE 56-4 BARIUM SINGLET S. TZ OUTER SHELLS
SYMETRY SPECIES NUNBEROF BASIS FUNCTIONS= 1: NUMBEROF CLOSED SHELLS = 6 OPEN SHELL OCCUPATION = D
NUCLEARCHARGE= 56.OOODOO NO.OF ELECTRONS= 56 TOTAL ENERGY -7883.53870176
POTENTIAL ENERGY -15767.04657291
KINETIC ENERGY 7883.50787114
VIRIAL THEOREM -2.00000391
S BASIS,ORBITALS AN0 EXPECTATION VALUES 1s
ORB.ENERGY -132;&48& ohD9B4 55.466670 6171.503092 1s IS 25 2s 3s 3s 4s 4s 5s 5s 65 6s 65
57.238506 38.212341 28.382587 24.369288 17.203998 13.053315 7.704401 5.699028 4.101114 2.801991 1.923224 1.266145 0.839756
0.882939 0.137928 -0.074394 0.058290 -0.010810 0.005572 -0.001791 0.001438 -0.000640 O.ODO346 -0.DOO150 O.DWDB4 -0.DDw29
2s
-207.15i752 0.116269 0.015874 12.800299 664.590940
0.026358 0.524300 -0.154397 -1.0658BD -0.045248 0.011939 -0.002043 0.001635 -0.DOO683 0.000352 -0.000151 o.DDDoB4 -0.oDDD29
P BASIS,ORBITALS AN0 EXPECTATION VALUES -195.0:!666 0.099068 0.011924 12.784581 221.027181 5819.921342
rENERGY 2P 2P 3P 3P 4P 4P 5P 5P 5P
36.098869 24.267342 14.401868 13.500919 8.761436 6.308644 4.228894 2.885258 1.894744
-0.135158 -0.865148 -0.OU365 0.026882 0.002542 -0.001879 O.DOO877 -0.DDD540 0.000167
-4O.Oii226 0.295281 O.lODB86 4.659528 45.645901 1128.982707 -0.027652 -0.502622 -0.692306 1.769554 0.091899 -00-E: -O:W3612 O.WlO30
-45.2;449 0.304801 0.105962 4.739935 137.574912 -0.009448 -0.240744 -0.374299 1.143979 0.083318 -1.275377 -; . cM;lM;; -0:006125 0.002936 -D.W1145 D.ODO618 -D.O00210
-9.5::322 0.701588 0.553974 1.964580 30.653339
-1.5::674 1.721193 3.319044 0.750065 4.883505
-0.1::506 5.256541 31.264895 0.233636 0.403629
-0.002130 -0.116243 -0.179622 0.549867 0.187718 -0.984975 0.841524 0.399578 -0.000562 0.002843 -0.ow701 O.ODO378 -0.000127
o.wo580 0.045822 0.068371 -0.213123 -0.093817 0.430998 -0.453568 -0.175214 0.590119 0.564675 0.027022 -0.003710 0.000845
-0.WO166 -0.012608 -0.019w2 0.058925 0.026403 -0.120305 0.128829 0.052453 -0.211072 -0.133680 0.291490 8. ;;7m; .
4P -7.549215 0.726965 0.599298 1.866735 9.975687 227.739138
-0,9:!815 1.944515 4.275486 0.660386 1.456391 29.015659
-0.010665 -0.234098 -po;80~~
-0.003570 -0.084322 -00.ym;;
-0:279082 -0.874097 -0.062307 0.010995 -0.002412
-0:130123 -0.395433 0.291647 8: %E
0 BASIS,ORBITALS AND EXPECTATION VALUES ORB.ENERGY
30 21.804696 3D 12.831889 40 8.769651 4D 6.083189 4D 3.965924
-30.4&79 0.266226 0.083413 4.524669 25.439624 185.657092
-4.Ot471 0.796319 0.733835 1.647547 4.854496 30.206780
tpm&
-0.067016 -0.377982 0.176593 0.699056 0.261361
0: 100159 -0.021056 0.004178
216
Atomic
Data and Nuclear
Data Tables.
Vol. 26, Non. 3/4. May/July
lSE1
A. D. MCLEAN
and R. S. MCLEAN
RorXhaan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE LANTHANUM
57-1
0*1 DOUBLET 0. DOUBLE ZETA
SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 57.000000 NO.OF ELECTRONS= 57 VECTOR COUPLING COEFFICIENTS KDOO- -1.80000000000 KDOP= TOTAL ENERGY
POTENTIAL ENERGY -16442.11883712
-8221.05671682 S BASIS,ORBITALS ORB.ENERGY
1s
IS 2s 2s
58.237307 38.741843 28.743063 24.839994
35 18.178526 3s 13.316311 45 4s 5s 55 6s 6s
7.810476 5.754674 4.067849 2.755443
1.693788 1.008657
P BASIS,ORBITALS
-1372.2::732 0.026644 0.000949 56.465456 6395.478806
-216.2::007 0.114096 0.015285 13.045622
0.885216
0.026734
0.135798
0.527513
690.191892
-0.079731 0.063987
-0.175516
-0.010519
-0.044700 0.008524 -0.001363 O.WlO75 -0.000400
-1.045981
0.004547 -0.001447 O.Wl105 -0.000430
o.wo194
o.wo171
-0.000054 0.000020
-0.woo47 0.000017
AND EXPECTATION 2P
4.767114 47.739404
6158.601129
1204.171015
36.146269 24.568856
-0.150811 -0.852943
-0.030829 -0.507660
12.834031 11.967284
-0.062175
9.048150 6.214501 3.735056 2.358652
0 BASIS,ORBITALS ORB.ENERGY
21.578871 12.760686 7.982846 5.200731 2.986856
1.588598
0.096411
0.050873 -0.001083 -0.ow155 0.000133 -0.000061 AND EXPECTATION -32.5;:739 0.259688
0.05714285714
KINETIC ENERGY 8221.06212030
-47.8::184 0.298294 0.101475 4.846337 143.811306 -0.009376 -0.243555 -0.393425
1.169048 0.070605 -1.266651 -0.044169
0.017872 -0.004624 0.001884 -0.000472 0.000168
1.610096 -0.522110 0.077953 -0.012627 0.002251 -0.000829
-8.2::425 0.704317 0.562234
1.929342 10.649598 248.405278 -0.010137 -0.243990
0.296139 0.479018 -0.476048 -0.795539 -0.022539 0.003389
-4.5::190 0.764110
0.674579
8.541111
1.716455 5.252677
0.470707 0.492823 2.353862
0.060190 -0.013925 0.002688 -0.000898
THEOREM
-1.99999934
4s -10.343031 0.681701 0.522840 2.025357 32.636157
5s -1.702250 1.637244 3.000372
0.791489 5.506950 0.000115 0.049084
-0.001927
-0.119055 -0.183453 0.557792 0.169418 -0.973612 0.906343
0.065045 -0.214428 -0.093068 0.444009 -0.520794
0.337722 -0.001066 0.001872 -0.000237 0.000077
0.726222 0.435477 0.004105 -0.000203
-0.119515
-0.1:;346 4.933207 27.527735 0.249737 0.474297 -0.000255 -0.013425 -0.021781 0.064533 0.024056
-0.124129 0.145724 0.047389
-0.291204 -0.028189 0.588064 0.526678
5P -1.047477 1.832638 3.789253 0.703017 1.663871 34.196550 -0.003796 -0.090734 0.003305 0.320922 -0.265687 -0.327533 0.695796 0.458945
-0.2::324 2.715513
4.634870
0.185408 0.817066
VIRIAL
VALUES
0.079314 26.669119 198.953505
d
VALUES
0.011470 13.031166 229.583967
KUO4=
i
VALUES
-42.4iEBl3 0.288680
30 30 40 40 50 50
AND EXPECTATION
-203.903510 0.097175
ORB.ENERGY CR>
2P 2P 3P 3P 4P 4P 5P 5P
0.05714285714
1; 6 0
33.636153 -0.082592 -0.383821 0.473983
0.650513 0.029574 -0.004011
0.021532 0.104142 -0.158047 -0.161415 0.518241 0.636097
217
Atomic
Data and Nuclear
Data Tables.
Vol. 26. Nos. 3/4, May/July
lSS1
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
TABLES.
Basis-Set Expansions
See page 207 for Explanations
TABLE LANTHANUM
SYMETRY SPECIES NUM8ER OF BASIS FUNCTIONS= NUHBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 57.000000 NO.OF ELECTRONS= 57
KOOP= 0.05714285714
TOTAL ENERGY -8221.06120236
ORB.ENERSY
58.248396 38.840453 29.109703 24.822670
17.126317 13.441594 8.039003 6.165896 4.292941 2.961003
2P 24.912197 3P 15.149975
0.114095 0.015285 13.045661 690.190506
0.025931 0.52696i
-0.071096 0.054519 -0.011763 0.006902 -0.002189 0.001699
-0.150038 -1.074086 -0.046915 0.015815 -0.002707 0.002065 -0.000712 0.000371
-0.000632 0.000346
-0.WO152 0.000085 -0.000030
AND EXPECTATION VALUES 2P 3P -203.906221 -42.457874 0.097173 0.288681
0.011470 13.031292
0.096411
229.594934
4.766991 47.740668
6159.959343
1204.559336
9.373215
0 BASIS,ORBITALS ORB.ENERGY
22.109356 13.030803 8.552946 5.763841 3.955944 2.478508
1.403810
:
d
1
KOO4= 0.05714285714 KINETIC ENERGY 8221.04970146
-47.835292 0.298296 0.101476 4.846316 143.810818 -0.009550 -0.242306 -0.353776
1.126269 0.128832 -1.317551 -0.054917 0.023339 -0.005520 0.002697 -0. ooo997 0.000544
10.651156 248.712648
-0.009125
-00.;;;a;;
-0.926369 1.982109 0.113574
-0.237138 -; .m;m;g
AND EXPECTATION -32.5:!696 0.259694 0.079315 4.634816 26.670724
199.033659 0.162400 0.820827 0.087162 -0.022805 0.006794 -0.002841 0.000776
0.681692 0.522830 2.025421 32.639357 -0.002264 -0.117993 -0.173918 0.550021 0.244305 -1.055376 0.752135 0.486657 0.011132 -0.000702 0.000478 -0.000228
5P -1.048950 1.832935 3.792738 0.703112 1.664905 34.236145
-0.023457
-0.029627 0.007865 -0.003402 0.000856
4s -10.344861
-8.2::215 0.704334 0.562270 1.929300
-0.504519
0: 002695
THEOREN
-2.00000140
0.000077
-0.876643
-0.002236 0.001078 -0.000583 0.000167
VIRIAL
-0.000188
-0.120291
14.136181 6.825183 4.868265 3.327934 2.163558
E
VALUES
-216.2::369
0.884022 0.137014
-0.000029
30 30 4D 40 50 50 50
-1372.2::620 0.026644 o.ooo949 56.465452 6395.486059
0.874638
ORB.ENERGY
3P 4P 4P 5P 5P 5P
AND EXPECTATION
-0.000144 O.WOO81
P BASIS,ORBITALS
2P
POTENTIAL ENERGY -16442.11090383
1.315979
2.008920 6s 6S
0 1: 6 0
COEFFICIENTS
KOOO= -1.80000000000
S 8ASIS.OR8ITALS
of Tables
57-2
O*l DOUBLET 0. TZ OUTER SHELLS
VECTOR COUPLING
Atomic Wave Functions, Z = 55-92
-0:134786 -0.965473 -0.100517 0.011315
-0.002470
5s -1.703874 1.636969 2.999324 0.791619 5.509544
-0.1%13 4.933386 27.584321 0.249998 0.476213
0.000653 0.047936 0.068623 -0.220353 -0.124664 0.479763 -0.419956 -0.241559 0.603437 0.561460 0.025939 -0.003867 0.000937
-0.000219 -0.013468 -0.019924 0.062892 0.035514 -0.136939 0.120943 0.076054 -0.227932 -0.130919 0.327404 0.568124 0.262791
-0.003135 -0.088815 -0.365680 0.630085 -0.062549 -0.471760 0.141189 0.723617 0.294169
VALUES -4.5::973 0.764167 0.674696
1.716452 5.252862 33.636889 -0.071081 -0.389204 0.295326 0.756542 0.102610 -0.008916
0.002370
-0.22849 2.744523 8.804364 0.468023 0.487975 2.328947 0.018768 0.103648 -0.092515 -0.225487 0.130807 0.576683 0.464102
218
Atomic
Data and
Nuclear
Data Tables.
Vol. 26, Nos. 314. May/July
1881
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic
Wave
Functions,
Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE LANTHANUM
4F*1
DOUBLET
57-3 SYWETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
F. DOUBLE ZETA
NUCLEAR CHARGE = 57.000000 NO.OF ELECTRONS= 57 VECTOR COUPLING COEFFICIENTS KFFO= -1.85714285714 KFFZ= TOTAL ENERGY -8221.00847050 S BASIS,ORBITALS ORB.ENERGY
1S 1S 25 2S 35 3s 45 4s 5S 5S 65 6S
58.256773 39.005580 28.706346 25.026660 18.234889 13.322909 7.827227 5.729117 4.026252 2.702241 1.630125 0.971094
P BASIS,ORBITALS ORB.ENERGY
CR**@ 2P 2P 3P 3P 4P 4P 5P 5P
36.184088 24.576055 12.964241 10.916585 9.258206 6.158073 3.659833 2.281695
0 BASIS,ORBITALS ORB.ENERGY CR>
30 3D 40 40
21.169560 12.575574 7.576935 4.736610
0.03809523810
POTENTIAL ENERGY -16442.02112826
AND EXPECTATION
KFF4=
0.02597402597
KFF6=
KINETIC ENERGY 8221.01265776
1; 6 0
0.03330003330
VIRIAL THEOREM -1.99999949
VALUES
-1371.9;;355 0.026644 0.000949 56.465608 6395.521974
-215.9::083 0.114088 0.015283 13.046508 690.272622
-47.42709 0.298269 0.101460 4.846883 143.843737
-10.0!;882 0.684246 0.526968 2.016855 32.346078
5s -1.557875 1.682249 3.171890 0.767753 5.122128
0.883078 0.137530 -0.082492 0.067085 -0.010229 0.004384 -0.001361 0.001018 -0.000390 0.000173 -0.000049 0.000018
0.025444 0.524533 -0.116734 -1.097429 -0.047854 0.009149 -0.001492 0.001144 -0.000419 0.000177 -0.000049 0.000018
-0.009054 -0.241701 -0.452699 1.222139 0.077117 -1.269073 -0.043478 0.016864 -0.004345 0.001746 -0.000440 0.000163
-0.001716 -0.117670 -0.209557 0.578831 0.170868 -0.968175 0.889470 0.353668 -0.000780 0.001800 -0.000236 0.000081
0.000049 0.046894 0.072900 -0.215465 -0.089628 0.425635 -0.492721 -0.118477 0.680589 0.473203 0.006441 -0.000815
-42.0;;257 0.288653 0.096398 4.767703 47.750760 1204.527258
-7.9:!640 0.707798 0.568164 1.919269 10.540466 245.548408
-0.9;!786 1.899379 4.077316 0.675896 1.523981 30.965910
-0.030491 -0.508059 1.264766 -0.190014 0.090704 -0.010953 0.002074 -0.000770
-0.009854 -0.242891 0.421191 0.410047 -0.539601 -0.796602 -0.022810 0.003477
-0.003575 -0.086339 0.102360 0.240199 -0.291149 -0.305593 0.663027 0.485786
AND EXPECTATION -203.5::484 0.097168 0.011469 13.031925 229.608405 6159.537975 -0.149855 -0.853974 -yw9~ -0:003299 0.000161 0.000065 -0.000034 AND EXPECTATION
-0.1:;232 5.182043 30.337154 0.236620 0.410900 -0.000236 -0.012312 -; . p; 0:022113 -0.114199 0.132217 0.044034 -0.256917 -0.049320 : : EZ
VALUES
VALUES
-32.2:!865 0.259649 0.079297 4.635729 26.676510 198.961919
-4.2:!655 0.770917 0.686875 1.701537 5.169533 33.019024
0.204663 0.808756 0.044342 -0.008392
-0.092396 -0.369366 0.608325 0.539332
F BASIS,ORBITALS ORB.ENERGY
4F 4F
219
AND EXPECTATION
VALUES
-0.3::479 1.056317 1.350261 1.187811 1.814221 3.597143
7.802388 3.370747
0.412589 0.739737
Atomic
Data and Nucle.sr
Data Tables.
Vol. 26. NIX
314, May/July
lS81
A. D. MCLEAN
aad R. S. MCLEAN
Raothsaa-Hartrce-Fock
Atomic Wave Fur&ions,
Z = 55-92
TABLES. Basis-Set Expansions Seepage207 for Explanations of Tables
TABLE LANTHARUR
4F*l
DOUBLET
F.
57-4
TZ OUTER SHELLS
SYMTRY SPECIES NUMBER OF BASIS FUNCTIONS= NUM8ER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 57.000000 NO.OF ELECTRONS= 57 VECTOR COUPLING COEFFICIENTS KFFO- -1.85714285714 KFFP= TOTAL ENERGY -8221.05498035 S BASIS,ORBITALS ORB-ENERGY
POTENTIAL
AND EXPECTATION -1372.0&07 0.026644 o.oDo949 56.455589
-0.071349 0.054678 -0.011527 0.006563 -0.002064 0.001587 -0.OOD608 0.000342 -0.000151 O.ODOO81 -0.000027
8.046041
6.113319 4.255208 2.905023 2.016072
1.322547 0.865618
P BASIS.DRBITALS ORB.ENERGY
4**2>
2P 2P 3P 3P 4P 4P 5P 5P 5P
36.125757 24.554489 12.652715 11.644802 9.787932 6.402615 4.153722 2.839633
1.892417
D BASIS,ORBITALS ORB.ENERGY
d/R+*3> 30 30
22.092241 13.062113
40 ID
8.743113 6.119195
ID
4.033363
0.884031
0.026079 0.527331 -0.151079 -1.073399 -0.045905 0.014489
0.137148
-0.002437 0.001847 -0.OOD654 0.000350 -0.ODO152 O.OWO81 -0.OWO27
AND EXPECTATION -203.6:!790
0.095402
229.508072
4.767596 47.749085
6159.489673
1204.517829
-0.151691
-0.031289
-0.852581
-0.507464
-0.051769 0.040828 -0.000283 -0.ow930 0.000576 -0.000398
0.000132 AND EXPECTATION -32.2:;587 0.259678
0.079311 4.635417
0.02597402597
KFFC=
KINETIC ENERGY 8221.03954145
:
5 0
0
1
0.03330003330
VIRIAL -2
THEOREU
.ooooo1BB
-47.4&23 0.298275 0.101465 4.846752 143.836500
-1o.ofZ924
-0.009688 -0.242357 -0.350941 1.123415 0.121754
-0.002251 -0.117609
-1.310496 -0.053349 0.021937
0.684136 0.526794 2.017271 32.361584
5.142452
-1.039208
-0.000184
-7.9::235
-0.9::303
-0.005436 0.002722 -0.w1074 0.000556
0.768985
-0.170183 0.544087 0.233287 0.748358 0.489457 0.011453 -0.000787 0.000549 -0.000253 0.000083
-1.5::685 1.679824 3.162486
0.000615 0.046318 0.064696 -0.210733 -0.115293 0.466533 -0.405341 -0.226984 0.564077 0.586397 0.033532 -0.004348 0.000994
-0. ii795 5.180720 30.386921
0.236951 0.412701 -0.000168 -0.012555 -0.017643 0.057285
0.031991 -0.125560 0.113263 0.065968 -0.196958 -0.144717 0.258131 0.579424 0.320443
VALUES -42.1:!356 0.288660
0.097168 0.011469 13.031927
KFH=
ii 4 0
VALUES
-215.9::25 0.114088 0.015283 13.046504 690.272685
6395.512213
25 35 3s 45 45 5s 55 6s 6s 65
13.431294
ENERGY
-16442.09452180
1s 58.248713 1s 38.810693 25 29.135065 24.824374 17.253546
0.03809523810
D 1: 6 0
1.922597 -0.882358 0.128603
-0.012499 0.003835 -0.002213 O.ODO665 VALUES
0.707672 0.567957
1.919665 10.545431 245.756092
-0.010692 -0.241647 0.314691 0.510701 -0.426727 -0.883887 yl404~;;
5:171754
199.102408
33.022298
0.162192 0.816960 0.091537 -0.022631
-0.070411 -0.383128 0.230895 0.677002
0.004658
0.234338
0.170190
F BASIS,ORBITALS ORB.ENERGY
AND EXPECTATION
1.122746 1.607224 1.162905
4F 4F 4F
220
VALUES
-0.3z740
!EE
26.677906
-0.003511 -0.086930 0.045034 0.283146 -0.206753 -0.389172 0.373003 0.624394
-O:W2023
-4.2::616 0.771254
1.896754 4.069985 0.677329 1.532085 31.143701
1.790270 3.682795
10.469122
0.159105
5.254855 2.456786
0.576558 0.475488
Atomic
Data and Nuclear
Data Taths,
Vol. 28. Nos. 314. M9/July
1961
A. D. MCLEAN
Roothaan-Hartree-Fock
and R. S. MCLEAN
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE CERIUM
4F*2
TRIPLET
H. DOUBLE
58-l SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
ZETA
NUCLEAR CHARGE = 5B.000000 NO.OF ELECTRONS= 58 VECTOR COUPLING COEFFICIENTS KFFO= -0.85714285714 KFFP= -0.07301587302 TOTAL ENERGY -8566.82528069 S BASIS,ORBITALS ORB.ENERGY
POTENTIAL
AND EXPECTATION
-1422.:398 0.026180
0.000917 57.464570
6623.486919
1s 59.209935 1s 39.003989 2s 29.348911 2s 24.993189 35 18.144311 3S 13.624986
0.890034 0.131298 -0.073629
4S 4S
8.042903 5.860575
-0.001423 0.001036
55
4.113416
-0.000392
5s 65 65
2.750359
0.000172 -0.000048 O.OWO18
1.654078 0.982308
P BASIS,ORBITALS ORB.ENERGY
2P 2P 3P 3P 4P 4P 5P 5P
36.463869 24.959065 13.181230 12.045176 9.289143
6.291945
3.741314 2.322640
0 BASIS.ORBITALS ORB.ENERGY
30 30
40 40
21.613636
12.895249 7.791698 4.867933
ENERGY
-17133.64169547
0.027895
-0.009691 -0.248179 -0.317545 1.109787 0.067391 -1.274228 -0.043115 0.016326
-0.255213 -0.981652 -0.037580
0.008168 -0.W1034 0.000789 -0.000282 o.wo115 -0.000032 0.000012
-44.1;:344 0.282326
0.092210
238.361202
6512.444931
1283.555382
-0.159336
-0.032779
-0.845743 -0.036414 0.025753 0.000476 -0.000604
-0.510466
1.459601 -0.368779 0.077396
-0.011390 0.002106 -0.000773
AND EXPECTATION VALUES 30 40 -34.016693 -4.5d9815 0.253429 0.748520 0.075501 LT.647671 4.746376 1.753284 27.944417 5.482074 213.066733 35.889667 0.203302 0.809597 0.043653
-0.008019
: 2F
d
i
0 2
0.03153412250
VIRIAL
THEOREM
-2.OWOO103
4s -10.466870 0.668093 0.502440
150.240826
-0.004243 0.001705 -0.000433 0.000161
5s
-1.599121 1.647917
2.067913 34.043545 -0.002471 -0.120473 -0.155586 0.540117
0.178420 -0.994422 0.891743 0.357971 -0.001794 0.002116 -0.000320 0.000113
3.045045 0.783852 5.341060 0.000373 0.047722 0.053484 -0.201502 -0.095024 0.438002 -0.493657 -0.116675 0.680181
0.472491 0.006506 -0.000827
-0.1::146
5.119719 29.626587 0.239439 0.418744 -0.000327 -0.012362 -0.017529 E:f:i -0:115697 0.130634 0.043033 -0.252613 -0.048473 0.570892 0.546303
VALUES
4.875624 49.900028
0.000217 -0.owo91
i
VALUES
0.534742
AND EXPECTATION
KFF6=
KINETIC ENER6Y 8566.81641479
-49.6;:316 0.292018 0.097246 4.953713
-0.010899 0.005118
13.279552
-0.02085792993
-224.9;:250 0.111985 0.014723 13.292995 716.476607
0.057326
-212.2;:828 0.095336 0.011038
KFH=
1; 6 0
-0.092426 -0.373837 0.615070 0.534765
-8.3::987 0.690085 0.540164
1.970338 11.106047 264.139077
-0.010771 -0.245490 0.326776 0.463371 -0.508842 -0.779286 -0.022210 0.003374 F BASIS,ORBITAtS ORB.ENERGY
-0.9&94 1.861332 3.918007
0.689714 1.585274 32.835850 -0.003935 -0.086508
0.027179 0.289586 -0.272670
-0.291943 0.661159 0.486925 AND EXPECTATION -0.4::099
0.992817 1.190429 1.258720
2.026883 4.218041
4F 4F
221
VALUES
0.414511
8.168280 3.583616
0.733979
Atomic
Data and Nuclear
Date Tables.
Vol. 26, Noa. 3/4. May/July
1961
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE CERIUn
4F*2
TRIPLET
58-2
H. TZ OUTER SHELLS
SYIMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUHBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 58.OOOOOO NO.OF ELECTRONS= 58 VECTOR COUPLING COEFFICIENTS KFFO= -0.85714285714 KFF2= -0.07301587302 TOTAL ENERGY -8566.90777274 S BASIS,ORBITALS DRB.ENERGY
4+*2> *l/R**2,
1s 2s 2s 35 3s 4s 45 55 5s 6s 65 6s
59.246387 39.387265 29.666386 25.245851 17.389458 13.770574 8.308742 6.321626 4.340583 2.946D58 2.006823 1.313021 0.863770
P BASIS,ORBITALS ORB.ENER6Y
cl/R**3> 2P 2P 3P 3P 4P 4P 5P 5P 5P
36.035792 24.818188 13.079557
12.311907 9.884111 6.553618
4.269119 2.902795
1.927901
D BASIS,ORBITALS ORB.ENERGY
30 30
22.570594
4D 4D
6.318737
13.390533 4D 8.979315 4.171967
POTENTIAL
ENERGY
-17133.79030811
AND EXPECTATION -1422.8::937 0.026180
$:266
0:111985 0.014723 13.292963
6623.511747
716.467264
0.886249 0.134869
EXE
-0.070396
-0:164683
0.053670 -0.012046 0.007208 -0.002076 0.001538 -0.000550 0.000304 -0.000134 0.000075
-1.064159 -0.045811 0.016077 -0.002493 0.001817 -0.0006W 0.000315 -0.000136 0.000076
-0.000026
-0.000026
AND EXPECTATION -212.3::608 0.095336 238.355544 6511.673824
0.092216 4.875429 49.8%4)5
1283.498278
-0.173254 -0.834041 -0.006458 -0.005686
0.006106 -0.002487
0.001089 -0.WD695 0.000224 AND EXPECTATION
-0.037394 -0.508585
1.924544 -0.851822
0.098563 -0.010383
o.w3105 -0.001736
0.000519 VALUES
-34.0::373 0.253462 0.075516 4.745958 27.944833 213.207339
-4.5:!960 0.748683 0.648708
0.160367
-0.070056
0.818618
-0.388060
0.090544 -0.022259
0.004545
d
:
5 0
0
2
0.03153412250
KFFB=
VIRIAL THEOREM
KINETIC ENERGY 8566.88253538
-2.oowo295
-49.7&0 0 * 292029 0.097252 4.953497
150.230208
-10.4:so70 0.667936 0.502196 2.068521 34.064958
-0.009648 -0.2U625 -0.345859
1.124958 0.143218 -1.334405 -0.053998 0.021201 -0.w4889 0.002419 -0.000954 0.000519 -0.000178
-0.002338 -0.118996 -0.170644 0.549964 0.264584 -1.080547 0.722252 0.519612 0.013109 -0.001238 0.000671 -0.000328 0.000110
1.644102 3.030530 0.785882 5.374821
-0.1~;815 5.116266 29.656084 0.239874 0.420680
O.WO616 0.046745 0.064332 -0.211904 -0.130773 0.475681 -0.393077 -0.238688 0.572439 0.579819 0.030370 -0.004464 0.001060
-0.WO182 -0.012475 -0.017518 0.057088 0.035509 -0.128811 0.107817 0.068915 -0.197729 -0.136340 0.280750 0.575907 0.299859
-1.6::319
VALUES -44.1:;869 0.282337
0.011038 13.279554
-0.02085792993
E
VALUES
-224
0.000917 57.464555
KFN=
D 1: 6 0
1.753895 5.486205 35.907356
0.233382 0.671527
-8.3:!518 0.689897 0.539858 1.970943 11.113588 264.437836
-0.013267 ‘0.243874 0.142432 0.668224 -0.415453 -0.873529 -0 *045879 0.008577 -0.w1912 F BASIS,ORBITALS ORB.ENERGY
-0.9:;205 1.856497 3.901271 0.692114 1.598612 33.138416 -0.004373 -0.087293 -0.033883 0.351273 -0.198607 -0.382896 0.370749
0.626537 0.171622 AND EXPECTATION
VALUES
-0.4::886 1.045075 1.382630
1.237982 2.010776 4.332712
4F 10.961203 4F 5.567004 4F 2.648988
0.156227 0.580305 0.465884
0.239283
222
Atomic
Data and
Nuclear
Data Tables,
Vol. 26, Nos. 3/4, May/July
198:
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartree-Fock
Atomic Wave Functions, 2 = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE
O*lF*l
CERIUH
TRIPLET
H. DOUBLE
58-3
ZETA
SYmETRY SPECIES NLMBER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 58.WOOOO NO.OF ELECTRONS= 58 VECTOR COUPLING 0.0 -0.02539682600
JOFP= KDF5=
TOTAL ENERGY -8566.81037272 S BASIS.ORBITALS ORB.ENERGY
4**2>
1s 1s 25 25 35 35 4s 4s 55 5s 65 65
59.219559 39.218576 29.346875 25.078692 17.679738 13.665310 8.143811 6.112953 4.185517 2.824027 1.723791 1.021721
P BASIS,ORBITALS ORB.ENERGY
2P
36.623234
2P 25.002727 3P 13.048758 3P 11.865722 4P 4P 5P 5P
9.604963 6.424681 3.832894 2.410315
0 BASIS,ORBITALS ORB.ENERGY
4**2> 30 30 4D 40 50 50
22.041396 13.085380 8.203674 5.343376 3.075288 1.626084
d
ii 02F
2 1
1
COEFFICIENTS
KOW= -1.8OOOOOOWW KOO2= 0.05714285714 KFFO= -1.85714285714 KFFP= 0.03809523810 JOFO= KDF3=
i
1; 6 0
-0.09523809524 ENERGY
-17133.61971658
AND EXPECTATION
0.026875 0.532193 -0.223967 -1.008978 -0.040739 0.011763 -0.001667 O.Wl211 -0. W0382 0.000164 -0.000045 0.000017
-0.009334 -0.246772 -0.341211 1.129840 0.088469 -1.291915 -0.046563 0.017778 -0.003839 0.001606 -0.000404 0.000145
-0.002337 -0.120299 -0.170656 0.556397 0.211248 -1.035048 0.833512 0.415430 0.004055 0.000784 -0.000034 0.000011
0.282351
0.092222 4.875064 49.889163
13.278789
238.338668
1283.204122
-0.154653 -0.849813 -0.043834
-0.031453 -0.510666 1.621288
0.033444 -0.000735 -0.000393 0.000183 -0.000080
-0.550313
AND EXPECTATION
0.002620 -0.000851
-1.7:;901
-0.lE971
1.604214 2.881683 0.807841 5.738229
4.880765 25.956358 0.252274 0.480885
0.000325 0.049254 0.061704 -0.215416 -0.115753 0.475152 -0.481542 -0.163383 0.713062 0.450738 0.005021 -0.000383
-0.000332 -0.013236 -0.020546 0.063918 0.029140 q.129959 0.131015 0.0599Sl -0.279978 -0.036346 0.582961 0.534381
VALUES
-44.5:!786
0.011040
THEOREM
-2.00000012
4s -10.798911 0.665660 0.498586 2.076468 34.342393
0.095343
0.183659 0.818388 0.059329 -0.013456
VIRIAL
KINETIC ENERGY 8566.80934387
VALUES
-212.6:!213
213.064901
0.03330003330 -0.77142857143
-50 .ois737 0.292042 0.097259 4.953181 150.209463
AND EXPECTATION
-34.3;!328 0.253464 0.075515 4.745551 27.937304
KFFC= KOFl-
-225.2::650 0.111992 0.014725 13.292108 716.385087
0.888908 0.131908 -0.072392 0.056278 -0.011305 0.006056 -0.001692 0.001218 -0.000408 0 .WO187 -0 .WOO52 0.000019
6511.827316
0.02597402597 -0.00432900433
0.04197822380
POTENTIAL
1s -1423.094659 0.026180 0.000917 57.464425 6623.465392
KDO4= 0.05714285714 KFN= JOF4=
0.097381 -0.011559 0.002108 -0.000782
-8.6:!677 0.686779 0.534673 1.980416 11.218017 267.139635 -0.010426 -0.246602 0.353964 0.465735 -0.484091 -0.830100 -0.024038 0.003652
VALUES
-l.o:~sBl
1.796083 3.641353 0.717235 1.729914 36.241461 -0.003917 -0.090946 0.031789 0.316280 -0.273199 -0.342320 0.686972 0.468063 F BASIS,ORBITALS
-4.8?460 0.742068 0.636325 1.768233 5.567613 36.539094
-0.2::923 2.638076 8.075579 0.486064 0.528435 2.600878
-0.082275 -0.388626 0.481605 0.645460 0.029102 -0.004015
0.021554 0.106719 -0.163881 -0.158122 0.524328 0.632184
223
ORB.ENERGY CR>
AND EXPECTATION
-0.6:L35 0.953528
1.094177 1.302339
2.153448 4.572538
4F 4F
Atomic
8.312599
0.415520
3.733694
0.726711
Data and Nuclear
VALUES
Data Tables,
Vol. 26. Nos. 3/4, May/July
1981
A. D. MCLEAN
and R. S. MCLEAN
Roothaan-Hartm-Fock
Atomic Wave Functions, 2 = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables TABLE
O*lFfl
CERILBI
TRIPLET
58-4
H. TZ OUTER SHELLS
SYMETRY SPECIES NUHBER OF BASIS FUNCTIONS= NMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION *
NUCLEAR CHARGE = 5B.OOODOO NO.OF ELECTRONS= 58 VECTOR KOW= KFFO= JOFO= KDF3-
CDUPLINB COEFFICIENTS -1.80000000000 KDDP= 0.05714285714 -1.85714285714 KFFZ= 0.03BO9523810 0.0 JOFZ= -0.09523809524 -0.02539682600 KDF5= 0.04197822380 TOTAL ENERGY -8566.84937822
S BASIS,ORBITALS OR$.ENERGY
1s 1s 59.244237 39.382259
45 45 5s 5s 6S 6S 65
8.328571 6.404988 4.399980
-O:W2274 0.001701
3.018190
O.OoO323 -0.oOo135 O.oooO76 -0.000027
O.BtB423
P BASIS,ORBITALS ORB.ENERGY CR> 2P 2P 3P 3P 4P 4P 5P 5P 5P
36.697673 25.019186 12.708466
11.089909 10.702162 6.675445 4.287934 2.920107 1.907784
0 BASIS,ORBITALS
3D 30 ID 4D 50 50 50
6511.899694
0.05714285714 0.02597102597 -0.W432900433
-5$&o& ~:%;~; 150:205649 :;*:;:t -0:341BB3 1.122081 0.154B41 -1.346416 -0.056012 0.022634 -yooo;;; -poops
o.oWo77 -0.OoOO27
-0hOD172
-0.031198 -0.510179 2.207867
-1.400679
0.379262 -0.013123 0.003918 -0.002238 0.000656
-B.6:!647 0.686705 0.534554
1.980666 11.221357 267.299936 -0.010737 -0.245499
0.273914 0.760393 -0.597535 y292:; o:w9603 -0.062070
VALUES
36.556373
0.159356 0.821517 0.089202 -0.023433 0.006520
-0.070111 -0.393769 0.279556
0.019087 0.105604 -0.OB4016
-0.002217
-0.004327
0:636oBl 1.768623
5.570019
0.755191 0.117947 0.001394
0 :
; 3
3F 0
1
1
0.0333OW3330
-0.77142857143
VIRIAL THEOREM -2.00000069
-1O.Bh6 0.665588
-1.7::702 1.602632 2.875868 0.808739
!K:i 34:352583
5.754019
-0.002354
-0.119532 -0.171177 0.553307 0.284130
-1.106219 0.709558 0.533167 0.013631 -0.w129o OBOO634 -0.oOo305 o.oOo104
0.000696 0.048347 0.067496 -0.221121 -0.144136 0.503311
-0.396216 -0.265797 0.600925 0.564289 0.025256
-$cw8;
-0.1%07 4.880868
27.019512 0.252565 0.482716 -0.000233 -0.013360
-0.019367 0.062203 0.04o310 -0.141268
0.111967 0.081824 -0.222210 -0.129956 0.327761 0.571976 0.259247
-1.0:;740
1.794791 3.639559 0.718195 1.735789 36.365755 -0.003607
-0.091619 0.013863 0.437721 -0.30768) -0.432370 0.417322 0.630297 0.125788 F BASIS,ORBITALS
-0.2:!692 2.650839 8.229162 0.486018 0.529077 2.608896
0.000650
-@6:;
KFF6= KDFl=
KINETIC ENERGY 8566.84318509
-0.00013B
1283.250666
AND EXPECTATION
0.075518 4.745408 27.937727 213.130995
2.539641 1.422654
-0:ooo648 0.000336
-0.152590 -0.851826 -0.046377 0.010506 -0.005305 -0BOOB72 0.000538 '8%% .
8.850064 6.028040 4.291447
-0.046680 0.017782 -yla~oa~~
AND EXPECTATION VALUES 2P 3P -212.620660 -44.553088 0.095343 0.011040 EE. 13.278801 4.8749BO 238.339120 49.888250
-34.3&92 0.253474
13.382092
-1.058302
-0.m591
ORB.ENERGY CR>
22.608975
0.025990 0.530474 -0.171350
z25i: -0: 069988 0.053300 -yl~ol:f
29.642466 25.214697 17.207730 13.789025
1.327079
ENERGY
AND EXPECTATION VALUES 1s -22;.&: -1423.1i3143 0.026180 0.000917 0:014725 57.464418 13.292093 6623.484852 716.380777
PS 2s 35 3S
2.038389
POTENTIAL
-17133.69286331
KW4= KFFI= JOF4=
1: 6 0
ORB.ENERGY
ql/R*2> 4F 4F 4F
11.150390 5.704824 2.761498
AND EXPECTATION
VALUES
-0.6::692 0.998742
1.253473 1.282305 2.135203 4.677683 0.152881 0.592773 0.447236
-8%E! 0:610742 0.440490
224
Atomic
Data and Nuclear
Data Table8.
Vol. 28. Nos. 3/4, May/July
19El
A. D. MCLEAN
Root&n-Hartree-Fock
and R. S. MCLEAN
Atomic Wave Functions, Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations
TABLE PRASEODYMIUM
4F*3
QUARTET
I.
59-l
DOUBLE ZETA
SYMHETRY SPECIES NUM8ER OF BASIS FUNCTIONS= NUMBER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
NUCLEAR CHARGE = 59.000000 NO.OF ELECTRONS= 59 VECTOR COUPLING COEFFICIENTS KFFD= -0.52380952381 KFF2= -0.09029982363 TOTAL ENERGY
POTENTIAL
-8921.04599240 S BASIS,ORBITALS ORB.ENERGY
45%
1s 1s 2s 2s 3s 3s 45 4s 5s 5s 65 6s
60.213606 39.755329 29.741218 25.473191 18.185381 13.951473 8.346946 6.178184 4.210516 2.801236 1.679605 0.993929
P BASIS,ORBITALS ORB-ENERGY
2P
36.925879
2P 25.389944 3P 13.425243 3P 12.338963 4P 9.424331 4P 6.405485 5P 3.818442 5P
2.360999
D BASIS.ORBITALS
30 3D 40
ID
AND EXPECTATION -1474.5:;264 0.025731
0.000885 58.463579 6855.489601
-0.254055
-0.983033 -0.038619 0.010278 -0.001359 0.000969 -0.000305 D.000128
-0. WOO36
0.000017
0.000014
AND EXPECTATION
-221.1:!542 0.093571 0.010631
-0.03157112247 KINETIC
ENERGY
0.276278 0.088296
4.983418
THEOREM
-0.002259 -0.121487 -0.170961 0 s560236
0.000228 0.047949 0.058134 -0.207041 -0.108658 0.455282 -0.465489 -0.145949 0.675702 0.477614 0.006703 -0.000834
-0.DW3DO
1.141311
0.079114 -1.288759 -0.044153 0.015680
-0.003460 0.001423 -0.000366 0.000136
-;A~&;; 0: 514677
-0.163667 -0.842036
-0.033466 -0.513402
-0.010742 -0.248639 0.347908 0.445475 -0.529995 -0.758867 -0.020603 0.002982
-0.007687
3
-2.00000130
-0.009199 -0.249552 -0.343647
283.256951
0.810481 0.043188
VIRIAL
-0.1::945 5.062061 28.975945 0.242132 0.426503
52.093952
0.201794
0
-1.6::458 1.616751 2.932194 0.798945 5.547480
1365.872893
0.071981 4.856832 29.239981 227.807839
i
-10.9&23 0.652933 0.479958 2.118057 35.748820
6879.060526
AND EXPECTATION
d
-51.9%57 0.286032 0.093293 5.060431 156.770589
2.020380 11.674201
0.020621 0.001267 -0.000825 0.000260 -0.OW106
9 :
0.203697 -1.030861
0.835443 0.417095 0.003287 0.000915
-0. WOO78 0.000028
-0.012270 -0.018913 0.059084 0.025769 -;. pm;
0: 050635 -0.246419 -0.051145 :: :2
VALUES
-46.2:!364
-0.030902
i
0.01995759572
KFR-
8921.03440373
13.527314 247.284214
8.009981 4.998756
0.535520
O.DOO161
-35.8::123 0.247514
22.061168 13.216664
0.027052
-0. WOO46
KFH-
1; 6 0
VALUES
-234.0:;616 0.109957 0.014193 13.539662 743.176443
0.891384 0.129365 -0.073992 0.058143 -0.011328 0.005802 -0.001543 0.001074 -0.000360
DRB.ENERGY
ENERGY
-17842.08039613
of Tables
1.538870
-0.445371 0.077613 -0.012252 0.002269 -0.000825 VALUES
F BASIS,ORBITALS
-4.7:!088 0.727901 0.6i2617 1.803742 5.795945
ORB.ENERGY
4**2>
38.857145 -0.092233 -0.377963
4F
8.496839
4F
3.765429
-0.9::437 1 .a27187 3.777840 0.702505 1.642346 34.640092 -0.003892 -0.086910 0.027255
0.288190 -0.281832 -0.276801 0.658849 0.488476 AND EXPECTATION
VALUES
-0.4::705 0.943491 1.073953 1.321352 2.226345 4.833182 0.417155 0.729049
0.619552 0.532374
225
Atomic
Data and Nuclear
Data Tables.
Vol. 28. Nos. 3l4. May/July
1961
A. D. MCLEAN
Roothaan-Hartne-Fock
and R. S. MCLEAN
Atomic Wave Functions, 2 = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE PRASEODYMIUM
4F*3
QUARTET
I.
59-2 SYMETRY SPECIES NUMBER OF BASIS FUNCTIONS= NUneER OF CLOSED SHELLS = OPEN SHELL OCCUPATION =
TZ OUTER SHELLS
NUCLEAR CHARGE = 59.000000 NO.OF ELECTRONS- 59 VECTOR COUPLING COEFFICIENTS KFFO- -0.52380952381 KFFP= -0.09029982363 TOTAL ENERGY
POTENTIAL
-8921.16604578 S BASIS.ORBITALS ORB.ENERGY
1s 60.238447 1s 39.955559 2s 2s 3s 3s 4s 45 5s 5s 6s 65 6s
29.976073 25.636283 17.779931 14.050543 8.493020 6.411705 4.420672 2.986439 2.013670
1 .X3445 0.865528
P BASIS,ORBITALS
-1474.5:;907 0.025731 0.000885 58.463563 6855.508648
0.014193
-0.009257 -0.247551 -0.356435
-0.043704
0.014947 -0.002218 0.001604 -0.000536 0.000274 -0.000118 0.000067 -0.000024
AN0 EXPECTATION
0:479664
0.026035
-1.037062
4s -18Mff
i%%~ 5:060164 156.755045
-0.195664
-t 'EE -0:000025
-51.9::952
13.539604 743.166969
0.533341
-0.072439 0.056166 -0.012226 0.007182 -0.002002 0.001465 -0.000530 0.000286
VIRIAL THEOREM -2.00000398
VALUES
-234.0::908 0.109957
0.888943 0.131905
ENERGY
8921.13050209
1.145247 0.130801 -1.329425 -0.051515 0.019554 -0.004565 o.QO2201 -0.000860
0 .WO477 -0.000167
2.118811 35.775959
-0.w2191 -0.120744 -0.177138 0.562610 0.260214 -1.085902 0.746212 0.502217 0.010167 -0.000239 0.000302 -0.ow139 0.000046
-B.7:!477 0.673309 0.514291 2.021179 11.684077
13.527300 247.287718 6879.704624
52.089770 1365.810438
37.385955 25.517243 12.868122
-0.150253 -0.853953 -0.051648
-0.029835 -0.513862 2.417516
-0.009872 -0.247331
10.943948 10.945735
0.052529 -0.012651
-1.831580 0.618639
-0.W3181 -0.087857 -0.009432
8-z:: -01735688
0.510357 -0.378291
-0.000665 0.000458
-0.015510 0.004698
-0.912473
-0.396129 0.378669 0.624934 0.164293
2.937412 1.943952
ORB.ENERGY 22.802601 13.579292 8.809854 6.077659 4.026293
0.276291 0.088304
4.983160
-0.000319 0.000108 AND EXPECTATION -352092 0.247550
0.071998 4.856325 29.238790 227.916602 0.168742 0.820949 0.077092 -0.021417 0.004909
-0.1::701 5.057456 28.996738 0.242623 0.428295
0.000539 0.047234 0.066138 -0.215317 -0.129212 0.476819 -0.405112 -0.225291
-0.000169
0.580253 0.573057 0.028503
-0.004418 0.001075
-0.012443
-0.017928 0.057488 0.034522 -y;m;t 0:064630 -0.197907
-0.129998 0.293338 0.574056 0.288370
-0.9::473 1.820583 3.753991 0.705756 1 a660520 35.063530
6.779547 4.349600
-46.3ii651
0.010631
-1.6::483 1.611799 2.913707 0.801687 5.593996
VALUES
-221.1;!552 0.093571
D BASIS.ORBITALS
3D 30 40 4D 4D
AND EXPECTATION
KINETIC
6 0
0.01995759572
KFM=
ORB.ENERGY
2P 2P 3P 3P 4P 4P 5P 5P 5P
ENERGY
-17842.29654787
-0.03157112247
KFF4=
S
li
-E%f . VALUES
283.619033
-%E -0: 002324 F BASIS,ORBITALS ORB.ENERGY CR,
-E!E 01613447
1.804581 5.801523 38.886709 -0.074633
-0.391560 0.345838 0.643817 0.161272
AND EXPECTATION -0.5::582 0.987941
1.230813 1.302744
2.214496 4.969858
4F 4F 4F
226
VALUES
11.370861
0.156045 0.583359 0.457928
5.827042 2.801680
Atomic
Data and Nuclear
Data Tables,
Vol. 26, Nos. 3/4, May/July
lQB1
A. D. MCLEAN
Roothaan-Hartree-Fock
and R. S. MCLEAN
Atomic
Wave
Functions,
Z = 55-92
TABLES. Basis-Set Expansions See page 207 for Explanations of Tables
TABLE 59-3 PRASEODYMIUM
O*lF*2
QUARTET J.
DOUBLE
ZETA
NUCLEAR CHARGE = 59.000000 NO.OF ELECTRONS= 59 VECTOR KDDD= KFFO= JDFO= KDF3=
COUPLING COEFFICIENTS -1.BOOOOOODODO KDD2= 0.05714285714 -0.85714285714 KFFP= -0.07301587302 0.0 JDFP- -0.04761904762 -0.05714285714 KDW= 0.03935458489 TOTAL ENERGY -8920.98865562
S BASIS,ORBITALS ORB.ENERGY CR>