2016
DOI: 10.1103/physrevb.94.125124
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Partial self-consistency and analyticity in many-body perturbation theory: Particle number conservation and a generalized sum rule

Abstract: We consider a general class of approximations which guarantees the conservation of particle number in many-body perturbation theory. To do this we extend the concept of Φ-derivability for the self-energy Σ to a larger class of diagrammatic terms in which only some of the Green's function lines contain the fully dressed Green's function G. We call the corresponding approximations for Σ partially Φ-derivable. A special subclass of such approximations, which are gauge-invariant, is obtained by dressing loops in t… Show more

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Cited by 17 publications
(15 citation statements)
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References 69 publications
(179 reference statements)
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“…Let us now examine analytical properties of the determinant of the single-particle Green's function, already analyzed to a certain extent in Refs. [5], [24] and [26]. Here, we shall show that the determinant of the single-particle Green's function can be expressed as a simple rational polynomial function as in Eq.…”
Section: Determinant Of Single-particle Green's Functionmentioning
confidence: 91%
“…Let us now examine analytical properties of the determinant of the single-particle Green's function, already analyzed to a certain extent in Refs. [5], [24] and [26]. Here, we shall show that the determinant of the single-particle Green's function can be expressed as a simple rational polynomial function as in Eq.…”
Section: Determinant Of Single-particle Green's Functionmentioning
confidence: 91%
“…Its straightforward inclusion, however, yields negative spectra in some frequency regions. This prohibits the usual probability interpretation and, even worse, it jeopardizes SC calculations since the resulting Green's function (GF) has the wrong analytic structure [53]. The key idea of the PSD scheme [51,52] consists in (1) writing a SE diagram as the sum of its partitions, i.e., diagrams with particle and hole propagators, (2) bisecting each partition into two half diagrams, (3) adding the missing half diagrams to form a perfect square, and (4) gluing the half diagrams back.…”
mentioning
confidence: 99%
“…The zeroth-order approximations for the SEs c (1, 2) can be obtained by using the relations given by Eqs. (52) and (83). After the Hedin equations are solved, we calculate the nuclear SE, see for example Sec.…”
Section: Choice Of Reference Positionsmentioning
confidence: 99%