Abstract

In this work we introduce the Dual Boson Diagrammatic Monte Carlo technique for strongly interacting electronic systems. This method combines the strength of dynamical mean-filed theory for non-perturbative description of local correlations with the systematic account of non-local corrections in the Dual Boson theory by the diagrammatic Monte Carlo approach. It allows us to get a numerically exact solution of the dual boson theory at the two-particle local vertex level for the extended Hubbard model. We show that it can be efficiently applied to description of single particle observables in a wide range of interaction strengths. We compare our exact results for the self-energy with the ladder Dual Boson approach and determine a physical regime, where description of collective electronic effects requires more accurate consideration beyond the ladder approximation. Additionally, we find that the order-by-order analysis of the perturbative diagrammatic series for the single-particle Green's function allows to estimate the transition point to the charge density wave phase.

Highlights

  • Correlated systems represent a formidable challenge in condensed matter physics

  • Divergencies of the diagrammatic series are often related to physical instabilities, as we show in Sec

  • We start from the description of the output of the calculation, namely the dual self-energykν obtained within the bare diagrammatic Monte Carlo scheme

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Summary

Introduction

Correlated systems represent a formidable challenge in condensed matter physics For this reason, the study of model systems can allow us to investigate the effects of strong interactions and analyze the effects of different approximations. Many real materials exhibit interesting physical effects, such as a charge density wave (CDW) phase, that cannot be described by a local Hubbard interaction term alone.

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