Non-Abelian duality from vortex moduli: a dual model of color-confinement

dc.contributor.areaPhysicsen_US
dc.contributor.authorEto, Minoruen_US
dc.contributor.authorFerretti, Lucaen_US
dc.contributor.authorKonishi, Kenichien_US
dc.contributor.authorMarmorini, Giacomoen_US
dc.contributor.authorNitta, Munetoen_US
dc.contributor.authorOhashi, Keisukeen_US
dc.contributor.authorVinci, Walteren_US
dc.contributor.departmentElementary Particle Theoryen_US
dc.date.accessioned2006-12-11T10:12:48Zen_US
dc.date.accessioned2011-09-07T20:27:06Z
dc.date.available2006-12-11T10:12:48Zen_US
dc.date.available2011-09-07T20:27:06Z
dc.date.issued2006-12-11T10:12:48Zen_US
dc.description.abstractIt is argued that the dual transformation of non-Abelian monopoles occurring in a system with gauge symmetry breaking G \longrightarrow H is to be defined by setting the low-energy H system in Higgs phase, so that the dual system is in confinement phase. The transformation law of the monopoles follows from that of monopole-vortex mixed configurations in the system (with a large hierarchy of energy scales, v_1 \gg v_2) G {\stackrel {v_1} {\longrightarrow}} H {\stackrel {v_2} {\longrightarrow}} \emptyset, under an unbroken, exact color-flavor diagonal symmetry H_{C+F} \sim {\tilde H}. The transformation property among the regular monopoles characterized by \pi_2(G/H), follows from that among the non-Abelian vortices with flux quantized according to \pi_1(H), via the isomorphism \pi_1(G) \sim {\pi_1(H) \over \pi_2(G/H)}.en_US
dc.format.extent414124 bytesen_US
dc.format.mimetypeapplication/pdfen_US
dc.identifier.citationNucl. Phys. B 780 (2007) 161-187en_US
dc.identifier.urihttps://openscience.sissa.it/handle/1963/1903en_US
dc.language.isoen_USen_US
dc.relation.ispartofseriesSISSA;76/2006/EPen_US
dc.relation.ispartofseriesarXiv.org;hep-th/0611313en_US
dc.relation.uri10.1016/j.nuclphysb.2007.03.040en_US
dc.titleNon-Abelian duality from vortex moduli: a dual model of color-confinementen_US
dc.typePreprinten_US
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