From 4d Yang-Mills to 2d ℂℙN − 1 model: IR problem and confinement at weak coupling

Masahito Yamazaki, Kazuya Yonekura

研究成果: ジャーナルへの寄稿記事

16 引用 (Scopus)

抄録

We study four-dimensional SU(N) Yang-Mills theory on ℝ×T3=ℝ×SA1×SB1×SC1, with a twisted boundary condition by a ℤN center symmetry imposed on SB 1 × SC 1. This setup has no IR zero modes and hence is free from IR divergences which could spoil trans-series expansion for physical observables. Moreover, we show that the center symmetry is preserved at weak coupling regime. This is shown by first reducing the theory on T2= SA× SB , to connect the model to the two-dimensional ℂℙN− 1-model. Then, we prove that the twisted boundary condition by the center symmetry for the Yang-Mills is reduced to the twisted boundary condition by the ℤN global symmetry of ℂℙN− 1. There are N classical vacua, and fractional instantons connecting those N vacua dynamically restore the center symmetry. We also point out the presence of singularities on the Borel plane which depend on the shape of the compactification manifold, and comment on its implications.

元の言語英語
記事番号88
ジャーナルJournal of High Energy Physics
2017
発行部数7
DOI
出版物ステータス出版済み - 7 1 2017

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symmetry
boundary conditions
instantons
Yang-Mills theory
series expansion
divergence

All Science Journal Classification (ASJC) codes

  • Nuclear and High Energy Physics

これを引用

From 4d Yang-Mills to 2d ℂℙN − 1 model : IR problem and confinement at weak coupling. / Yamazaki, Masahito; Yonekura, Kazuya.

:: Journal of High Energy Physics, 巻 2017, 番号 7, 88, 01.07.2017.

研究成果: ジャーナルへの寄稿記事

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AB - We study four-dimensional SU(N) Yang-Mills theory on ℝ×T3=ℝ×SA1×SB1×SC1, with a twisted boundary condition by a ℤN center symmetry imposed on SB 1 × SC 1. This setup has no IR zero modes and hence is free from IR divergences which could spoil trans-series expansion for physical observables. Moreover, we show that the center symmetry is preserved at weak coupling regime. This is shown by first reducing the theory on T2= SA× SB , to connect the model to the two-dimensional ℂℙN− 1-model. Then, we prove that the twisted boundary condition by the center symmetry for the Yang-Mills is reduced to the twisted boundary condition by the ℤN global symmetry of ℂℙN− 1. There are N classical vacua, and fractional instantons connecting those N vacua dynamically restore the center symmetry. We also point out the presence of singularities on the Borel plane which depend on the shape of the compactification manifold, and comment on its implications.

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