Exhaustive Characterization of Quantum Many-Body Scars Using Commutant Algebras

We study quantum many-body scars (QMBS) in the language of commutant algebras, which are defined as symmetry algebras of of local Hamiltonians. This framework explains the origin of dynamically disconnected subspaces seen in models with exact QMBS, i.e., the large “thermal” subspace and the small “nonthermal” subspace, which are attributed to the existence of unconventional nonlocal conserved quantities in the commutant; hence, it unifies the study of conventional symmetries and weak ergodicity-breaking phenomena into a single framework. Furthermore, this language enables us to use the von Neumann double commutant theorem to formally write down the exhaustive algebra of Hamiltonians with a desired set of QMBS, which demonstrates that QMBS survive under large classes of local perturbations. We illustrate this using several standard examples of QMBS, including the spin-<a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mn>1</a:mn><a:mo>/</a:mo><a:mn>2</a:mn></a:mrow></a:math> ferromagnetic, AKLT, spin-1 XY <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>π</c:mi></c:math>-bimagnon, and the electronic <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>η</e:mi></e:math>-pairing towers of states; in each of these cases, we explicitly write down a set of generators for the full algebra of Hamiltonians with these QMBS. Understanding this hidden structure in QMBS Hamiltonians also allows us to recover results of previous “brute-force” numerical searches for such Hamiltonians. In addition, this language clearly demonstrates the equivalence of several unified formalisms for QMBS proposed in the literature and also illustrates the connection between two apparently distinct classes of QMBS Hamiltonians—those that are captured by the so-called Shiraishi-Mori construction and those that lie beyond. Finally, we show that this framework motivates a precise definition for QMBS that automatically implies that they violate the conventional eigenstate thermalization hypothesis, and we discuss its implications to dynamics. Published by the American Physical Society 2024

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Publication Details

Journal
Physical Review X
Published
2024-12-26
DOI
https://doi.org/10.1103/physrevx.14.041069
Citations
26
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
8.78

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article

Exhaustive Characterization of Quantum Many-Body Scars Using Commutant Algebras

Olexei I. Motrunich, Sanjay Moudgalya
26 citations
Physical Review X
Quantum many-body systems
8.78
article

Exhaustive Characterization of Quantum Many-Body Scars Using Commutant Algebras

Olexei I. Motrunich, Sanjay Moudgalya
article en
26 citations

Abstract

We study quantum many-body scars (QMBS) in the language of commutant algebras, which are defined as symmetry algebras of of local Hamiltonians. This framework explains the origin of dynamically disconnected subspaces seen in models with exact QMBS, i.e., the large “thermal” subspace and the small “nonthermal” subspace, which are attributed to the existence of unconventional nonlocal conserved quantities in the commutant; hence, it unifies the study of conventional symmetries and weak ergodicity-breaking phenomena into a single framework. Furthermore, this language enables us to use the von Neumann double commutant theorem to formally write down the exhaustive algebra of Hamiltonians with a desired set of QMBS, which demonstrates that QMBS survive under large classes of local perturbations. We illustrate this using several standard examples of QMBS, including the spin-<a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mn>1</a:mn><a:mo>/</a:mo><a:mn>2</a:mn></a:mrow></a:math> ferromagnetic, AKLT, spin-1 XY <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>π</c:mi></c:math>-bimagnon, and the electronic <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>η</e:mi></e:math>-pairing towers of states; in each of these cases, we explicitly write down a set of generators for the full algebra of Hamiltonians with these QMBS. Understanding this hidden structure in QMBS Hamiltonians also allows us to recover results of previous “brute-force” numerical searches for such Hamiltonians. In addition, this language clearly demonstrates the equivalence of several unified formalisms for QMBS proposed in the literature and also illustrates the connection between two apparently distinct classes of QMBS Hamiltonians—those that are captured by the so-called Shiraishi-Mori construction and those that lie beyond. Finally, we show that this framework motivates a precise definition for QMBS that automatically implies that they violate the conventional eigenstate thermalization hypothesis, and we discuss its implications to dynamics. Published by the American Physical Society 2024

Physical Review XVol. 14(4)
California Institute of Technology (US), Munich Center for Quantum Science and Technology (DE), Technical University of Munich (DE)
National Science Foundation, Simons Foundation, California Institute of Technology, Aspen Center for Physics, Munich Center for Quantum Science and Technology, Walter Burke Institute for Theoretical Physics, Institute for Quantum Information and Matter, California Institute of Technology, Division of Materials Research
Openalex Percentile: Top 1%
Quantum many-body systems
8.78
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