Algorithm for computing perturbation series of dynamical mean field theory

We show how to use diagrammatic techniques to compute the weak-coupling perturbation series of the self-consistent solution to a dynamical mean field theory (DMFT) problem. This approach constitutes an alternative to using diagrammatic techniques directly as an impurity solver. It allows one to bypass the need of multiple perturbative series resummations within the DMFT self-consistency loop. It can be applied at or out of equilibrium, with any diagrammatic formalism, such as real times, imaginary times, or Matsubara frequencies formalisms. As a proof of principle, we illustrate our method with the half-filled Hubbard model on the Bethe lattice in the DMFT approximation, using quantum quasi Monte Carlo (QQMC) to obtain the impurity perturbation series on the real time axis.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2025-04-14
DOI
https://doi.org/10.1103/physrevb.111.165120
Primary Topic
Quantum chaos and dynamical systems
Type
article
Field-Weighted Citation Impact
0.00

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article

Algorithm for computing perturbation series of dynamical mean field theory

Corentin Bertrand, Olivier Parcollet, Michel Ferrero
Physical review. B./Physical review. B
Quantum chaos and dynamical systems
article

Algorithm for computing perturbation series of dynamical mean field theory

Corentin Bertrand, Olivier Parcollet, Michel Ferrero
article en

Abstract

We show how to use diagrammatic techniques to compute the weak-coupling perturbation series of the self-consistent solution to a dynamical mean field theory (DMFT) problem. This approach constitutes an alternative to using diagrammatic techniques directly as an impurity solver. It allows one to bypass the need of multiple perturbative series resummations within the DMFT self-consistency loop. It can be applied at or out of equilibrium, with any diagrammatic formalism, such as real times, imaginary times, or Matsubara frequencies formalisms. As a proof of principle, we illustrate our method with the half-filled Hubbard model on the Bethe lattice in the DMFT approximation, using quantum quasi Monte Carlo (QQMC) to obtain the impurity perturbation series on the real time axis.

Physical review. B./Physical review. BVol. 111(16)
Collège de France (FR), Centre de Physique Théorique (FR), Flatiron Health (United States) (US), Institut de Physique Théorique (FR), Flatiron Institute (US)
Grand Équipement National De Calcul Intensif
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Openalex Percentile: Top 94%
Quantum chaos and dynamical systems
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