Diagrammatic self-energy approximations and the total particle number
arXiv:cond-mat/0110435 · doi:10.1103/PhysRevB.64.235106
Abstract
There is increasing interest in many-body perturbation theory as a practical tool for the calculation of ground-state properties. As a consequence, unambiguous sum rules such as the conservation of particle number under the influence of the Coulomb interaction have acquired an importance that did not exist for calculations of excited-state properties. In this paper we obtain a rigorous, simple relation whose fulfilment guarantees particle-number conservation in a given diagrammatic self-energy approximation. Hedin's G_0W_0 approximation does not satisfy this relation and hence violates the particle-number sum rule. Very precise calculations for the homogeneous electron gas and a model inhomogeneous electron system allow the extent of the nonconservation to be estimated.
arXiv comment6 pages including 3 figures, RevTeX
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- Hedin's equations and enumeration of Feynman's diagrams
- Analytic evaluation of the electronic self-energy in the GW approximation for two electrons on a sphere
- Partial self-consistency and analyticity in many-body perturbation theory: particle number conservation and a generalized sum rule
- A unified Green's function approach for spectral and thermodynamic properties from algorithmic inversion of dynamical potentials
- Quasiparticle Calculations for Point Defects on Semiconductor Surfaces
- Two-time quantum transport and quantum diffusion
- Condensation energy of the homogeneous electron gas from the density functional theory for superconductors