A COMPARISON OF SPIN-ORBIT PARAMETERS

1967 ◽  
Vol 45 (4) ◽  
pp. 1501-1505 ◽  
Author(s):  
Charlotte Froese

Hartree–Fock results for some spin-orbit parameters are presented. The calculations are based on the Blume and Watson (1962) expression for the spin-orbit parameter, derived on the assumption that the atomic wave function is antisymmetric.The results are compared with experimental values and it is shown that the earlier conclusions concerning the accuracy of the spin-orbit parameter for 3p and 3d electrons are not valid. The results are also compared with Hartree–Fock–Slater values based on a simplified definition.

1995 ◽  
Vol 74 (8) ◽  
pp. 1331-1334
Author(s):  
C. Schnurr ◽  
T. A. Savard ◽  
L. J. Wang ◽  
J. E. Thomas

Author(s):  
Sylvester A. Ekong ◽  
David A. Oyegoke

This paper aims at determining the total energy and bond lengths of some polyatomic organic molecules, using quantum Monte Carlo (QMC) CASINO-code. The QMC code employed the VMC and DMC methods in the computations with emphasis on DMC, and using Slater-Jastrow trial wave-function formed from Hartree-Fock orbitals. The calculated results show that our reported values are in good agreement with the experimental values of both Hehre et al., and Linus Pauling. The total energies obtained in this study are 6 significant figures more accurate than those of previous studies.


2000 ◽  
Vol 17 (3) ◽  
pp. 165-167 ◽  
Author(s):  
Zheng-Dong Liu ◽  
Shi-Yao Zhu ◽  
Yu Lin ◽  
Liang Zeng ◽  
Qin-Min Pan

1960 ◽  
Vol 15 (10) ◽  
pp. 909-926 ◽  
Author(s):  
Levente Szász

To calculate the correlation energy of an atom with N electrons we suggest the wave functionwhere à is the antisymmetrizer operator, φ1, φ2, ..., φN are one electron wave functions, and Wjk are correlation functions of the following form:where the constants c j km, n, l are variational parameters. The function (a) is a generalization of thewave function of Hylleraas for He. After a discussion of the properties of our function, an energy expression is derived. Numerical calculation is made for the ground state of the Be atom with the functionwhere φ1 and φ2 are ls wave functions, φ3 and φ4 are 2s wave functions, r1, r2, r3 and r4 are the radial coordinates of the four electrons, r12 and r34 are the distances between the corresponding electrons, and C1 and c2 are variational parameters. Using the one electron wave functions calculated by Roothaan and coll. with the Roothaan procedure, we got the energy value E= -14.624 a. u. while the Hartree-Fock and experimental values are EH,F= -14.570 a. u. and Eexp= -14.668 a. u. respectively. Thus the function (c) gives about one-half of the correlation energy of the Be atom.


Author(s):  
S. A. Alexander ◽  
R. L. Coldwell

2005 ◽  
Vol 03 (02) ◽  
pp. 339-350 ◽  
Author(s):  
K. I. OSMAN

This paper deals with the system of a two-level atom interacting with a quantized single-mode standing-wave cavity field, which is entangled with the centre-of-mass motion of the atom under the coexistence of the Kerr nonlinearity. We investigate the effect of the spread of the initial atomic wave function on some quantum statistical properties (such as Q distribution function, entropy and phase distribution) with or without the Kerr-like medium. Numerical computations and a discussion of the results are presented.


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