2018
DOI: 10.1103/physrevb.97.125141
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Practical consequences of the Luttinger-Ward functional multivaluedness for cluster DMFT methods

Abstract: The Luttinger-Ward functional (LWF) has been a starting point for conserving approximations in many-body physics for 50 years. The recent discoveries of its multivaluedness and the associated divergence of the two-particle irreducible vertex function Γ have revealed an inherent limitation of this approach. Here we demonstrate how these undesirable properties of the LWF can lead to a failure of computational methods based on an approximation of the LWF. We apply the Nested Cluster Scheme (NCS) to the Hubbard mo… Show more

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Cited by 60 publications
(59 citation statements)
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References 90 publications
(110 reference statements)
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“…Depending on the interaction strength and doping level, the generalized impurity susceptibility may have egivenvalues with negative real part but their zero-crossing occurs at finite imaginary part, leading to a smooth irreducible charge vertex. For small U , the eigenvalues remain real for a small range of doping 88 .…”
Section: Dynamical Vertexmentioning
confidence: 96%
“…Depending on the interaction strength and doping level, the generalized impurity susceptibility may have egivenvalues with negative real part but their zero-crossing occurs at finite imaginary part, leading to a smooth irreducible charge vertex. For small U , the eigenvalues remain real for a small range of doping 88 .…”
Section: Dynamical Vertexmentioning
confidence: 96%
“…Furthermore, the two-particle self-energy γ (irreducible vertex) also shows divergences, sometimes located in the vicinity of the Mott insulator [46], but they also arise in systems without Mott localization [49] and even in the atomic limit [50]. Divergences of the two-particle self-energy have been related to the multivaluedness of the Luttinger-Ward functional [51][52][53].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, a lot of attention has been directed towards the properties of the generalized susceptibilities as they, unexpectedly, can become singular 11,[19][20][21][22][23][24] in the intermediately-to-strongly correlated or disordered regime. The singular points are directly linked to eigenvalues of χ νν ω r , for a fixed bosonic frequency ω, that go from positive to negative when the interaction or disorder increases, and thus cross zero 11,22 .…”
Section: Introductionmentioning
confidence: 99%