# Improved treatment of fermion-boson vertices and Bethe-Salpeter equations in non-local extensions of dynamical mean field theory

## TL;DR

This paper introduces an analytical method to handle high-frequency contributions of fermion-boson vertices in non-local dynamical mean-field theory, simplifying calculations of Bethe-Salpeter equations.

## Contribution

We derive formulas that analytically account for vertex contributions outside a chosen frequency box, reducing numerical complexity in non-local DMFT calculations.

## Key findings

- Method tested on the Hubbard model shows accurate results.
- Reduces computational effort by avoiding numerical treatment of high-frequency vertices.
- Applicable to a broad range of non-local DMFT applications.

## Abstract

We reconsider the procedure of calculation of fermion-boson vertices and numerical solution of Bethe-Salpeter equations, used in non-local extensions of dynamical mean-field theory. Because of the frequency dependence of vertices, finite frequency box for matrix inversions is typically used, which often requires some treatment of asymptotic behaviour of vertices. Recently [Phys. Rev. B 83, 085102 (2011); 97, 235140 (2018)] it was proposed to split the considered frequency box into smaller and larger one; in the smaller frequency box the numerically exact vertices are used, while beyond this box asymptotics of vertices are applied. Yet, this method requires numerical treatment of vertex asymptotics (including corresponding matrix manipulations) in the larger frequency box and/or knowing fermion-boson vertices, which may be not convenient for numerical calculations. In the present paper we derive the formulae which treat analytically contribution of vertices beyond chosen frequency box, such that only numerical operations with vertices in the chosen small frequency box are required. The method is tested on the Hubbard model and can be used in a broad range of applications of non-local extensions of dynamical mean-field theory.