Partition function zeros of quantum many-body systems

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1. Verfasser: Shastry, B Sriram
Format: Preprint
Veröffentlicht: 2025
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author Shastry, B Sriram
author_facet Shastry, B Sriram
contents We present a new method for calculating the Yang-Lee partition function zeros of a translationally invariant model of lattice fermions, exemplified by the Hubbard model. The method rests on a theorem involving the single electron self-energy $Σ_σ(k, i ω_n)$ in the imaginary time Matsubara formulation. The theorem maps the Yang-Lee zeros to a set of wavevector and spin labeled virtual energies $ξ_{k σ}$. These, thermodynamically derived virtual energies, are solutions of equations involving the self-energy at corresponding $kσ$'s. Examples of the method in simplified situations are provided.
format Preprint
id arxiv_https___arxiv_org_abs_2504_01880
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Partition function zeros of quantum many-body systems
Shastry, B Sriram
Statistical Mechanics
Strongly Correlated Electrons
We present a new method for calculating the Yang-Lee partition function zeros of a translationally invariant model of lattice fermions, exemplified by the Hubbard model. The method rests on a theorem involving the single electron self-energy $Σ_σ(k, i ω_n)$ in the imaginary time Matsubara formulation. The theorem maps the Yang-Lee zeros to a set of wavevector and spin labeled virtual energies $ξ_{k σ}$. These, thermodynamically derived virtual energies, are solutions of equations involving the self-energy at corresponding $kσ$'s. Examples of the method in simplified situations are provided.
title Partition function zeros of quantum many-body systems
topic Statistical Mechanics
Strongly Correlated Electrons
url https://arxiv.org/abs/2504.01880