Fading ergodicity

Fuente: arXiv
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Auteurs principaux: Kliczkowski, Maksymilian, Świętek, Rafał, Hopjan, Miroslav, Vidmar, Lev
Format: Preprint
Publié: 2024
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author Kliczkowski, Maksymilian
Świętek, Rafał
Hopjan, Miroslav
Vidmar, Lev
author_facet Kliczkowski, Maksymilian
Świętek, Rafał
Hopjan, Miroslav
Vidmar, Lev
contents Eigenstate thermalization hypothesis (ETH) represents a breakthrough in many-body physics since it allows to link thermalization of physical observables with the applicability of random matrix theory (RMT). Recent years were also extremely fruitful in exploring possible counterexamples to thermalization, ranging, among others, from integrability, single-particle chaos, many-body localization, many-body scars, to Hilbert-space fragmentation. In all these cases the conventional ETH is violated. However, it remains elusive how the conventional ETH breaks down when one approaches the boundaries of ergodicity, and whether the range of validity of the conventional ETH coincides with the validity of RMT-like spectral statistics. Here we bridge this gap and we introduce a scenario of the ETH breakdown in many-body quantum systems, dubbed fading ergodicity regime, which establishes a link between the conventional ETH and non-ergodic behavior. We conjecture this scenario to be relevant for the description of finite many-body systems at the boundaries of ergodicity, and we provide numerical and analytical arguments for its validity in the quantum sun model of ergodicity breaking phase transition. For the latter, we provide evidence that the breakdown of the conventional ETH is not associated with the breakdown of the RMT-like spectral statistics.
format Preprint
id arxiv_https___arxiv_org_abs_2407_16773
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Fading ergodicity
Kliczkowski, Maksymilian
Świętek, Rafał
Hopjan, Miroslav
Vidmar, Lev
Statistical Mechanics
Disordered Systems and Neural Networks
Strongly Correlated Electrons
High Energy Physics - Theory
Quantum Physics
Eigenstate thermalization hypothesis (ETH) represents a breakthrough in many-body physics since it allows to link thermalization of physical observables with the applicability of random matrix theory (RMT). Recent years were also extremely fruitful in exploring possible counterexamples to thermalization, ranging, among others, from integrability, single-particle chaos, many-body localization, many-body scars, to Hilbert-space fragmentation. In all these cases the conventional ETH is violated. However, it remains elusive how the conventional ETH breaks down when one approaches the boundaries of ergodicity, and whether the range of validity of the conventional ETH coincides with the validity of RMT-like spectral statistics. Here we bridge this gap and we introduce a scenario of the ETH breakdown in many-body quantum systems, dubbed fading ergodicity regime, which establishes a link between the conventional ETH and non-ergodic behavior. We conjecture this scenario to be relevant for the description of finite many-body systems at the boundaries of ergodicity, and we provide numerical and analytical arguments for its validity in the quantum sun model of ergodicity breaking phase transition. For the latter, we provide evidence that the breakdown of the conventional ETH is not associated with the breakdown of the RMT-like spectral statistics.
title Fading ergodicity
topic Statistical Mechanics
Disordered Systems and Neural Networks
Strongly Correlated Electrons
High Energy Physics - Theory
Quantum Physics
url https://arxiv.org/abs/2407.16773