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Confinement in partially broken abelian Chern-Simons theories

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arxiv hep-th/9704063 v2 pith:BEUGYDC7 submitted 1997-04-08 hep-th cond-mat

classification hep-thcond-mat
keywords gaugebrokenconfinementfieldsparticlestermtheoriesunbroken
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Planar Chern-Simons (CS) theories in which a compact abelian gauge group U(1) x U(1) is spontaneously broken to U(1) x Z_N are investigated. Among other things, it is noted that the theories just featuring the mixed CS term coupling the broken to the unbroken U(1) gauge fields in general exhibits an interesting form of confinement: only particles carrying certain multiples of the fundamental vortex flux unit and certain multiples of the fundamental charge of the unbroken U(1) gauge field can appear as free particles. Adding the usual CS term for the broken U(1) gauge fields does not change much. It merely leads to additional Aharonov-Bohm interactions among these particles. Upon introducing the CS term for the unbroken U(1) gauge fields, in contrast, the confinement phenomenon completely disappears.

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  1. Non-Invertible Symmetries as Condensation Defects in Finite-Group Gauge Theories

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    Non-invertible symmetries in finite-group gauge theories are realized as condensation defects, with a complete Z_N dictionary and new automorphism symmetry expressions.

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