θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories

Abstract In SU(N ) gauge theory, it is argued recently that there exists a “mixed anomaly” between the CP symmetry and the 1-form ℤ N $$ {\mathbb{Z}}_N $$ symmetry at θ = π, and the anomaly matching requires CP to be spontaneously broken at θ = π if the system is in the confining phase. In this pape...

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Main Authors: Ryuichiro Kitano, Takao Suyama, Norikazu Yamada
Format: Article
Language:English
Published: SpringerOpen 2017-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2017)137
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spelling doaj-f99f33b91c6840ebab8aa37de24fcac12020-11-24T21:54:54ZengSpringerOpenJournal of High Energy Physics1029-84792017-09-012017911510.1007/JHEP09(2017)137θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theoriesRyuichiro Kitano0Takao Suyama1Norikazu Yamada2KEK Theory CenterKEK Theory CenterKEK Theory CenterAbstract In SU(N ) gauge theory, it is argued recently that there exists a “mixed anomaly” between the CP symmetry and the 1-form ℤ N $$ {\mathbb{Z}}_N $$ symmetry at θ = π, and the anomaly matching requires CP to be spontaneously broken at θ = π if the system is in the confining phase. In this paper, we elaborate on this discussion by examining the large volume behavior of the partition functions of the S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ theory on T 4 à la ’t Hooft. The periodicity of the partition function in θ, which is not 2π due to fractional instanton numbers, suggests the presence of a phase transition at θ = π. We propose lattice simulations to study the distribution of the instanton number in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ theories. A characteristic shape of the distribution is predicted when the system is in the confining phase. The measurements of the distribution may be useful in understanding the phase structure of the theory.http://link.springer.com/article/10.1007/JHEP09(2017)137Discrete SymmetriesLattice Quantum Field TheoryWilson’t Hooft and Polyakov loopsConfinement
collection DOAJ
language English
format Article
sources DOAJ
author Ryuichiro Kitano
Takao Suyama
Norikazu Yamada
spellingShingle Ryuichiro Kitano
Takao Suyama
Norikazu Yamada
θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
Journal of High Energy Physics
Discrete Symmetries
Lattice Quantum Field Theory
Wilson
’t Hooft and Polyakov loops
Confinement
author_facet Ryuichiro Kitano
Takao Suyama
Norikazu Yamada
author_sort Ryuichiro Kitano
title θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
title_short θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
title_full θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
title_fullStr θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
title_full_unstemmed θ =π in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ gauge theories
title_sort θ =π in s u n / ℤ n $$ \mathrm{s}\mathrm{u}(n)/{\mathbb{z}}_n $$ gauge theories
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-09-01
description Abstract In SU(N ) gauge theory, it is argued recently that there exists a “mixed anomaly” between the CP symmetry and the 1-form ℤ N $$ {\mathbb{Z}}_N $$ symmetry at θ = π, and the anomaly matching requires CP to be spontaneously broken at θ = π if the system is in the confining phase. In this paper, we elaborate on this discussion by examining the large volume behavior of the partition functions of the S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ theory on T 4 à la ’t Hooft. The periodicity of the partition function in θ, which is not 2π due to fractional instanton numbers, suggests the presence of a phase transition at θ = π. We propose lattice simulations to study the distribution of the instanton number in S U N / ℤ N $$ \mathrm{S}\mathrm{U}(N)/{\mathbb{Z}}_N $$ theories. A characteristic shape of the distribution is predicted when the system is in the confining phase. The measurements of the distribution may be useful in understanding the phase structure of the theory.
topic Discrete Symmetries
Lattice Quantum Field Theory
Wilson
’t Hooft and Polyakov loops
Confinement
url http://link.springer.com/article/10.1007/JHEP09(2017)137
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AT takaosuyama thpinsunznmathrmsmathrmunmathbbzngaugetheories
AT norikazuyamada thpinsunznmathrmsmathrmunmathbbzngaugetheories
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