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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Online Access: | http://link.springer.com/article/10.1007/JHEP09(2017)137 |
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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 |
work_keys_str_mv |
AT ryuichirokitano thpinsunznmathrmsmathrmunmathbbzngaugetheories AT takaosuyama thpinsunznmathrmsmathrmunmathbbzngaugetheories AT norikazuyamada thpinsunznmathrmsmathrmunmathbbzngaugetheories |
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1725864903803142144 |