Lattice realization of the axial $U(1)$ noninvertible symmetry

Fuente: arXiv
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Main Authors: Honda, Yamato, Morikawa, Okuto, Onoda, Soma, Suzuki, Hiroshi
Format: Preprint
Published: 2024
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author Honda, Yamato
Morikawa, Okuto
Onoda, Soma
Suzuki, Hiroshi
author_facet Honda, Yamato
Morikawa, Okuto
Onoda, Soma
Suzuki, Hiroshi
contents In $U(1)$ lattice gauge theory with compact $U(1)$ variables, we construct the symmetry operator, i.e.\ the topological defect, for the axial $U(1)$ noninvertible symmetry. This requires a lattice formulation of chiral gauge theory with an anomalous matter content and we employ the lattice formulation on the basis of the Ginsparg--Wilson relation. The invariance of the symmetry operator under the gauge transformation of the gauge field on the defect is realized, imitating the prescription by Karasik in continuum theory, by integrating the lattice Chern--Simons term on the defect over \emph{smooth\/} lattice gauge transformations. The projection operator for allowed magnetic fluxes on the defect then emerges with lattice regularization. The resulting symmetry operator is manifestly invariant under lattice gauge transformations. In an appendix, we give another way of constructing the symmetry operator on the basis of a 3D $\mathbb{Z}_N$ topological quantum field theory, the level-$N$ BF theory on the lattice.
format Preprint
id arxiv_https___arxiv_org_abs_2401_01331
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Lattice realization of the axial $U(1)$ noninvertible symmetry
Honda, Yamato
Morikawa, Okuto
Onoda, Soma
Suzuki, Hiroshi
High Energy Physics - Lattice
High Energy Physics - Theory
In $U(1)$ lattice gauge theory with compact $U(1)$ variables, we construct the symmetry operator, i.e.\ the topological defect, for the axial $U(1)$ noninvertible symmetry. This requires a lattice formulation of chiral gauge theory with an anomalous matter content and we employ the lattice formulation on the basis of the Ginsparg--Wilson relation. The invariance of the symmetry operator under the gauge transformation of the gauge field on the defect is realized, imitating the prescription by Karasik in continuum theory, by integrating the lattice Chern--Simons term on the defect over \emph{smooth\/} lattice gauge transformations. The projection operator for allowed magnetic fluxes on the defect then emerges with lattice regularization. The resulting symmetry operator is manifestly invariant under lattice gauge transformations. In an appendix, we give another way of constructing the symmetry operator on the basis of a 3D $\mathbb{Z}_N$ topological quantum field theory, the level-$N$ BF theory on the lattice.
title Lattice realization of the axial $U(1)$ noninvertible symmetry
topic High Energy Physics - Lattice
High Energy Physics - Theory
url https://arxiv.org/abs/2401.01331