1974
DOI: 10.1088/0022-3700/7/18/010
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The Rayleigh-Schrodinger perturbation and the linked-diagram theorem for a multi-configurational model space

Abstract: The Rayleigh-Schrodinger perturbation formalism is extended to the case of a model space, which is not necessarily degenerate. The model space defines the zero-order or model wavefunction, and the new formalism makes it possible to use a model wavefunction of multi-configurational type. The effect of the states outside the model space are as usual taken into account by means of a perturbation expansion and expressed in terms of an 'effective' Hamiltonian, operating only within the model space. The extended Ray… Show more

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Cited by 449 publications
(272 citation statements)
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References 25 publications
(20 reference statements)
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“…The theoretical basis of the RMBPT method, as implemented in the FAC code, is based on the Rayleigh-Schrödinger perturbation theory [47] and allows for a combination of configuration interaction and second-order many-body perturbation theory (Gu [33]). The approach is built on the H DCB , which is split up into a zero-order, model Hamiltonian, H 0 , and a perturbation, V , defined as,…”
Section: The Fac Relativistic Many-body Perturbation Theory Methodsmentioning
confidence: 99%
“…The theoretical basis of the RMBPT method, as implemented in the FAC code, is based on the Rayleigh-Schrödinger perturbation theory [47] and allows for a combination of configuration interaction and second-order many-body perturbation theory (Gu [33]). The approach is built on the H DCB , which is split up into a zero-order, model Hamiltonian, H 0 , and a perturbation, V , defined as,…”
Section: The Fac Relativistic Many-body Perturbation Theory Methodsmentioning
confidence: 99%
“…The second-order MBPT approach (Lindgren 1974;Safronova et al 1996), implemented by Gu (2005Gu ( , 2006 in FAC has been used successfully to calculate atomic parameters with high accuracy (Gu 2007;Gu et al 2011;Wang et al 2014;Fei et al 2014;Guo et al 2015;Wang et al 2015;Si et al 2015a,b). Here we briefly describe the theory.…”
Section: Mbptmentioning
confidence: 99%
“…To determine S < σ (3), we draw a horizontal dashed line just above 3 and we gather the segments of L crossing the dashed line from above. In our case the segments are (1, 0), (2,4) , (3,1), (4,3) and (5, 2), (6,5) . S < σ (3) is the set of abscissae of the first point of each segment:…”
Section: Lemma 7 (I) S < σ (K) Cannot Be Empty and (Ii) S < σ (K) Andmentioning
confidence: 73%