Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1842554 | Nuclear Physics B | 2007 | 27 Pages |
Abstract
It is argued that the dual transformation of non-Abelian monopoles occurring in a system with gauge symmetry breaking GâH 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, v1â«v2) Gâv1Hâv21, under an unbroken, exact color-flavor diagonal symmetry HC+Fâ¼HË. The transformation property among the regular monopoles characterized by Ï2(G/H), follows from that among the non-Abelian vortices with flux quantized according to Ï1(H), via the isomorphism Ï1(G)â¼Ï1(H)/Ï2(G/H). Our idea is tested against the concrete models-softly-broken N=2 supersymmetric SU(N), SO(N) and USp(2N) theories, with appropriate number of flavors. The results obtained in the semiclassical regime (at v1â«v2â«Î) of these models are consistent with those inferred from the fully quantum-mechanical low-energy effective action of the systems (at v1,v2â¼Î).
Related Topics
Physical Sciences and Engineering
Mathematics
Mathematical Physics
Authors
Minoru Eto, Luca Ferretti, Kenichi Konishi, Giacomo Marmorini, Muneto Nitta, Keisuke Ohashi, Walter Vinci, Naoto Yokoi,