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Main Authors: Pal, Soumya Kanti, Santos, Lea F
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2508.00077
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author Pal, Soumya Kanti
Santos, Lea F
author_facet Pal, Soumya Kanti
Santos, Lea F
contents Understanding the stability of integrability in many-body quantum systems is key to controlling dynamics and predicting thermalization. While the breakdown of integrability in short-range interacting systems is well understood, the role of long-range couplings -- ubiquitous and experimentally realizable -- remains unclear. We show that in fully connected models, integrability is either robust or extremely fragile, depending on whether perturbations are non-extensive, extensive one-body, or extensive two-body. In contrast to finite short-range systems, where any of these perturbations can induce chaos at finite strength, in fully connected finite models, chaos is triggered by extensive two-body perturbations and even at infinitesimal strength. Chaos develops within energy bands defined by symmetries, leading to a fragmented realization of the eigenstate thermalization hypothesis and clarifying how microcanonical shells can be constructed in such systems. We also introduce a general symmetry-based framework that explains the stability of integrability.
format Preprint
id arxiv_https___arxiv_org_abs_2508_00077
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Fragmented eigenstate thermalization versus robust integrability in long-range models
Pal, Soumya Kanti
Santos, Lea F
Statistical Mechanics
Quantum Physics
Understanding the stability of integrability in many-body quantum systems is key to controlling dynamics and predicting thermalization. While the breakdown of integrability in short-range interacting systems is well understood, the role of long-range couplings -- ubiquitous and experimentally realizable -- remains unclear. We show that in fully connected models, integrability is either robust or extremely fragile, depending on whether perturbations are non-extensive, extensive one-body, or extensive two-body. In contrast to finite short-range systems, where any of these perturbations can induce chaos at finite strength, in fully connected finite models, chaos is triggered by extensive two-body perturbations and even at infinitesimal strength. Chaos develops within energy bands defined by symmetries, leading to a fragmented realization of the eigenstate thermalization hypothesis and clarifying how microcanonical shells can be constructed in such systems. We also introduce a general symmetry-based framework that explains the stability of integrability.
title Fragmented eigenstate thermalization versus robust integrability in long-range models
topic Statistical Mechanics
Quantum Physics
url https://arxiv.org/abs/2508.00077