2011
DOI: 10.1002/andp.201100043
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Superperturbation theory on the real axis

Abstract: In this article we formulate the superperturbation theory for the Anderson impurity model on the real axis. The resulting impurity solver allows to evaluate dynamical quantities without numerical analytical continuation by the maximum entropy method or Padé approximants. This makes the solver well suited to study multiplet effects in solids within the dynamical mean field theory. First examples including multi-orbital problems are discussed.

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Cited by 2 publications
(2 citation statements)
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“…For ∆ (N ) ν ≡ 0 and in the limit of small hybridization ∆ ν , it reproduces the noninteracting limit and the result of a first-order expansion of the Green's function in the hybridization: (Dai et al, 2005). The one-and two-particle Green's functions g 12 and χ 1234 of the reference system can be expressed in terms of the ED eigenvalues and matrix elements and can be analytically continued to the real axis (Jung et al, 2011). The naive expansion exhibits a causality problem, which can however be cured (Jung, 2010) by introducing a renormalization parameter (Krivenko et al, 2010).…”
Section: Df As a Cluster Solvermentioning
confidence: 67%
“…For ∆ (N ) ν ≡ 0 and in the limit of small hybridization ∆ ν , it reproduces the noninteracting limit and the result of a first-order expansion of the Green's function in the hybridization: (Dai et al, 2005). The one-and two-particle Green's functions g 12 and χ 1234 of the reference system can be expressed in terms of the ED eigenvalues and matrix elements and can be analytically continued to the real axis (Jung et al, 2011). The naive expansion exhibits a causality problem, which can however be cured (Jung, 2010) by introducing a renormalization parameter (Krivenko et al, 2010).…”
Section: Df As a Cluster Solvermentioning
confidence: 67%
“…12. A common feature of all diagrammatic extensions is that they build upon the local (two-and more-particle) vertex and use it to construct non-local correlations in one-and two-particle quantities. These approaches allow for describing physical phenomena beyond the realm of DMFT, such as formation of a pseudogap [13][14][15][16][17][18] and (quantum) critical exponents [19][20][21][22] .…”
Section: Introductionmentioning
confidence: 99%