Strong decay of correlations for Gibbs states in any dimension

Fuente: arXiv
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Autori principali: Bluhm, Andreas, Capel, Ángela, Pérez-Hernández, Antonio
Natura: Preprint
Pubblicazione: 2024
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author Bluhm, Andreas
Capel, Ángela
Pérez-Hernández, Antonio
author_facet Bluhm, Andreas
Capel, Ángela
Pérez-Hernández, Antonio
contents Quantum systems in thermal equilibrium are described using Gibbs states. The correlations in such states determine how difficult it is to describe or simulate them. In this article, we show that if the Gibbs state of a quantum system satisfies that each of its marginals admits a local effective Hamiltonian with short-range interactions, then it satisfies a mixing condition, that is, for any regions $A$, $C$ the distance of the reduced state $ρ_{AC}$ on these regions to the product of its marginals, $$\| ρ_{AC} ρ_A^{-1} \otimes ρ_C^{-1} - 1_{AC}\|\, ,$$ decays exponentially with the distance between regions $A$ and $C$. This mixing condition is stronger than other commonly studied measures of correlation. In particular, it implies the exponential decay of the mutual information between distant regions. The mixing condition has been used, for example, to prove positive log-Sobolev constants. On the way, we prove that the the condition regarding local effective Hamiltonian is satisfied if the Hamiltonian of the system is commuting and also commutes with every marginal of the Gibbs state. The proof of these results employs a variety of tools such as Araki's expansionals, quantum belief propagation and cluster expansions.
format Preprint
id arxiv_https___arxiv_org_abs_2401_10147
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Strong decay of correlations for Gibbs states in any dimension
Bluhm, Andreas
Capel, Ángela
Pérez-Hernández, Antonio
Quantum Physics
Mathematical Physics
Quantum systems in thermal equilibrium are described using Gibbs states. The correlations in such states determine how difficult it is to describe or simulate them. In this article, we show that if the Gibbs state of a quantum system satisfies that each of its marginals admits a local effective Hamiltonian with short-range interactions, then it satisfies a mixing condition, that is, for any regions $A$, $C$ the distance of the reduced state $ρ_{AC}$ on these regions to the product of its marginals, $$\| ρ_{AC} ρ_A^{-1} \otimes ρ_C^{-1} - 1_{AC}\|\, ,$$ decays exponentially with the distance between regions $A$ and $C$. This mixing condition is stronger than other commonly studied measures of correlation. In particular, it implies the exponential decay of the mutual information between distant regions. The mixing condition has been used, for example, to prove positive log-Sobolev constants. On the way, we prove that the the condition regarding local effective Hamiltonian is satisfied if the Hamiltonian of the system is commuting and also commutes with every marginal of the Gibbs state. The proof of these results employs a variety of tools such as Araki's expansionals, quantum belief propagation and cluster expansions.
title Strong decay of correlations for Gibbs states in any dimension
topic Quantum Physics
Mathematical Physics
url https://arxiv.org/abs/2401.10147