$Confinement in 3d $$ \mathcal{N} $$ = 2 Spin(N) gauge theories with vector and spinor matters$

Confinement in 3d $$ \mathcal{N} $$ = 2 Spin(N) gauge theories with vector and spinor matters

We present various confinement phases in three-dimensional $$ \mathcal{N} $$ N = 2 Spin( N ) gauge theories with vector and spinor matters. The quantum Coulomb branch in the moduli space of vacua is drastically modified when the rank of the gauge group and the matter contents are changed. In many ex...

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Veröffentlicht in:	The journal of high energy physics 2019-03, Vol.2019 (3), Article 113
1. Verfasser:	Nii, Keita
Format:	Artikel
Sprache:	eng
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container_title	The journal of high energy physics
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creator	Nii, Keita
description	We present various confinement phases in three-dimensional $$ \mathcal{N} $$ N = 2 Spin( N ) gauge theories with vector and spinor matters. The quantum Coulomb branch in the moduli space of vacua is drastically modified when the rank of the gauge group and the matter contents are changed. In many examples, the Coulomb branch is one- or two-dimensional but its interpretation varies. In some examples, the Coulomb branch becomes three-dimensional and we need to introduce a “dressed” Coulomb branch operator.
doi_str_mv	10.1007/JHEP03(2019)113
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title	Confinement in 3d $$ \mathcal{N} $$ = 2 Spin(N) gauge theories with vector and spinor matters
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