Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality

Abstract We study a 3d lattice gauge theory with gauge group U(1) N−1 ⋊ S N , which is obtained by gauging the S N global symmetry of a pure U(1) N−1 gauge theory, and we call it the semi-Abelian gauge theory. We compute mass gaps and string tensions for both theories using the monopole-gas descript...

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Main Authors: Mendel Nguyen, Yuya Tanizaki, Mithat Ünsal
Format: Article
Language:English
Published: SpringerOpen 2021-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP03(2021)238
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spelling doaj-8ac239cadc9946978f0a57720db70ebc2021-03-28T11:06:55ZengSpringerOpenJournal of High Energy Physics1029-84792021-03-012021313210.1007/JHEP03(2021)238Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-alityMendel Nguyen0Yuya Tanizaki1Mithat Ünsal2Department of Physics, North Carolina State UniversityYukawa Institute for Theoretical Physics, Kyoto UniversityDepartment of Physics, North Carolina State UniversityAbstract We study a 3d lattice gauge theory with gauge group U(1) N−1 ⋊ S N , which is obtained by gauging the S N global symmetry of a pure U(1) N−1 gauge theory, and we call it the semi-Abelian gauge theory. We compute mass gaps and string tensions for both theories using the monopole-gas description. We find that the effective potential receives equal contributions at leading order from monopoles associated with the entire SU(N) root system. Even though the center symmetry of the semi-Abelian gauge theory is given by ℤ N , we observe that the string tensions do not obey the N-ality rule and carry more detailed information on the representations of the gauge group. We find that this refinement is due to the presence of non-invertible topological lines as a remnant of U(1) N−1 one-form symmetry in the original Abelian lattice theory. Upon adding charged particles corresponding to W-bosons, such non-invertible symmetries are explicitly broken so that the N-ality rule should emerge in the deep infrared regime.https://doi.org/10.1007/JHEP03(2021)238ConfinementDiscrete SymmetriesGlobal SymmetriesWilson, ’t Hooft and Polyakov loops
collection DOAJ
language English
format Article
sources DOAJ
author Mendel Nguyen
Yuya Tanizaki
Mithat Ünsal
spellingShingle Mendel Nguyen
Yuya Tanizaki
Mithat Ünsal
Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
Journal of High Energy Physics
Confinement
Discrete Symmetries
Global Symmetries
Wilson, ’t Hooft and Polyakov loops
author_facet Mendel Nguyen
Yuya Tanizaki
Mithat Ünsal
author_sort Mendel Nguyen
title Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
title_short Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
title_full Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
title_fullStr Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
title_full_unstemmed Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
title_sort semi-abelian gauge theories, non-invertible symmetries, and string tensions beyond n-ality
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-03-01
description Abstract We study a 3d lattice gauge theory with gauge group U(1) N−1 ⋊ S N , which is obtained by gauging the S N global symmetry of a pure U(1) N−1 gauge theory, and we call it the semi-Abelian gauge theory. We compute mass gaps and string tensions for both theories using the monopole-gas description. We find that the effective potential receives equal contributions at leading order from monopoles associated with the entire SU(N) root system. Even though the center symmetry of the semi-Abelian gauge theory is given by ℤ N , we observe that the string tensions do not obey the N-ality rule and carry more detailed information on the representations of the gauge group. We find that this refinement is due to the presence of non-invertible topological lines as a remnant of U(1) N−1 one-form symmetry in the original Abelian lattice theory. Upon adding charged particles corresponding to W-bosons, such non-invertible symmetries are explicitly broken so that the N-ality rule should emerge in the deep infrared regime.
topic Confinement
Discrete Symmetries
Global Symmetries
Wilson, ’t Hooft and Polyakov loops
url https://doi.org/10.1007/JHEP03(2021)238
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AT yuyatanizaki semiabeliangaugetheoriesnoninvertiblesymmetriesandstringtensionsbeyondnality
AT mithatunsal semiabeliangaugetheoriesnoninvertiblesymmetriesandstringtensionsbeyondnality
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