Finite-field many-body perturbation theory II. SD-MBPT study of the nuclear charge dependence of the electron correlation contribution to the dipole polarizability of 10-electron atomic systems

1982 ◽  
Vol 61 (5) ◽  
pp. 485-504 ◽  
Author(s):  
Geerd H. F. Diercksen ◽  
Andrzej J. Sadlej

1990 ◽  
Vol 193 ◽  
Author(s):  
C. Sosa ◽  
K. F. Ferris

ABSTRACTThe static dipole polarizability for the ground state of C(3Π ), N(4∑+), O(3Π ) and F(2∑+ ) have been calculated using ab initio molecular orbital techniques. The polarizabilities are obtained from unrestricted Hartree-Fock and Many-Body Perturbation Theory wave functions with and without spin projection, which are computed by finite-field differentiation. The effect of spin contamination is shown to be important on the calculation of static dipole polarizabilities for the ground state of C, N, O and F.







1986 ◽  
Vol 33 (2) ◽  
pp. 814-823 ◽  
Author(s):  
Ivan Cernusak ◽  
Geerd H. F. Diercksen ◽  
Andrzej J. Sadlej


2007 ◽  
Vol 16 (04) ◽  
pp. 1221-1231 ◽  
Author(s):  
INGVAR LINDGREN ◽  
STEN SALOMONSON ◽  
DANIEL HEDENDAHL

A rigorous procedure for energy-dependent many-body perturbation theory (MBPT) is presented. This can be applied for numerical evaluation of many-body-QED effects by combining QED with electron correlation to arbitrary order. So far, it has been used only for the exchange of a single retarded photon together with an arbitrary number of instantaneous Coulomb interactions. For heliumlike neon this represents more than 99% of the nonradiative effect on the energy beyond standard MBPT.



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