Strong-to-Weak Spontaneous Symmetry Breaking in Mixed Quantum States

Fuente: arXiv
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Main Authors: Lessa, Leonardo A., Ma, Ruochen, Zhang, Jian-Hao, Bi, Zhen, Cheng, Meng, Wang, Chong
Format: Preprint
Published: 2024
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author Lessa, Leonardo A.
Ma, Ruochen
Zhang, Jian-Hao
Bi, Zhen
Cheng, Meng
Wang, Chong
author_facet Lessa, Leonardo A.
Ma, Ruochen
Zhang, Jian-Hao
Bi, Zhen
Cheng, Meng
Wang, Chong
contents Symmetry in mixed quantum states can manifest in two distinct forms: strong symmetry, where each individual pure state in the quantum ensemble is symmetric with the same charge, and weak symmetry, which applies only to the entire ensemble. This paper explores a novel type of spontaneous symmetry breaking (SSB) where a strong symmetry is broken to a weak one. While the SSB of a weak symmetry is measured by the long-ranged two-point correlation function, the strong-to-weak SSB (SW-SSB) is measured by the fidelity correlator. We prove that SW-SSB is a universal property of mixed-state quantum phases, in the sense that the phenomenon of SW-SSB is robust against symmetric low-depth local quantum channels. We also show that the symmetry breaking is "spontaneous" in the sense that the effect of a local symmetry-breaking measurement cannot be recovered locally. We argue that a thermal state at a nonzero temperature in the canonical ensemble (with fixed symmetry charge) should have spontaneously broken strong symmetry. Additionally, we study non-thermal scenarios where decoherence induces SW-SSB, leading to phase transitions described by classical statistical models with bond randomness. In particular, the SW-SSB transition of a decohered Ising model can be viewed as the "ungauged" version of the celebrated toric code decodability transition. We confirm that, in the decohered Ising model, the SW-SSB transition defined by the fidelity correlator is the only physical transition in terms of channel recoverability. We also comment on other (inequivalent) definitions of SW-SSB, through correlation functions with higher Renyi indices.
format Preprint
id arxiv_https___arxiv_org_abs_2405_03639
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Strong-to-Weak Spontaneous Symmetry Breaking in Mixed Quantum States
Lessa, Leonardo A.
Ma, Ruochen
Zhang, Jian-Hao
Bi, Zhen
Cheng, Meng
Wang, Chong
Quantum Physics
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
Symmetry in mixed quantum states can manifest in two distinct forms: strong symmetry, where each individual pure state in the quantum ensemble is symmetric with the same charge, and weak symmetry, which applies only to the entire ensemble. This paper explores a novel type of spontaneous symmetry breaking (SSB) where a strong symmetry is broken to a weak one. While the SSB of a weak symmetry is measured by the long-ranged two-point correlation function, the strong-to-weak SSB (SW-SSB) is measured by the fidelity correlator. We prove that SW-SSB is a universal property of mixed-state quantum phases, in the sense that the phenomenon of SW-SSB is robust against symmetric low-depth local quantum channels. We also show that the symmetry breaking is "spontaneous" in the sense that the effect of a local symmetry-breaking measurement cannot be recovered locally. We argue that a thermal state at a nonzero temperature in the canonical ensemble (with fixed symmetry charge) should have spontaneously broken strong symmetry. Additionally, we study non-thermal scenarios where decoherence induces SW-SSB, leading to phase transitions described by classical statistical models with bond randomness. In particular, the SW-SSB transition of a decohered Ising model can be viewed as the "ungauged" version of the celebrated toric code decodability transition. We confirm that, in the decohered Ising model, the SW-SSB transition defined by the fidelity correlator is the only physical transition in terms of channel recoverability. We also comment on other (inequivalent) definitions of SW-SSB, through correlation functions with higher Renyi indices.
title Strong-to-Weak Spontaneous Symmetry Breaking in Mixed Quantum States
topic Quantum Physics
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
url https://arxiv.org/abs/2405.03639