Non-Abelian duality from vortex moduli: a dual model of color-confinement
arXiv:hep-th/0611313 · doi:10.1016/j.nuclphysb.2007.03.040
Abstract
It is argued that the dual transformation of non-Abelian monopoles occurring in a system with gauge symmetry breaking G -> 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 >> v_2) G -> H -> 0, under an unbroken, exact color-flavor diagonal symmetry H_{C+F} \sim {\tilde H}. The transformation property among the regular monopoles characterized by Ï_2(G/H), follows from that among the non-Abelian vortices with flux quantized according to Ï_1(H), via the isomorphism Ï_1(G) \sim Ï_1(H) / Ï_2(G/H). Our idea is tested against the concrete models -- softly-broken {\cal N}=2 supersymmetric SU(N), SO(N) and USp(2N) theories, with appropriate number of flavors. The results obtained in the semiclassical regime (at v_1 >> v_2 >> Î) of these models are consistent with those inferred from the fully quantum-mechanical low-energy effective action of the systems (at v_1, v_2 \sim Î).
2+27 pages, 5 figures; v3, minor changes