Two-kink bound states in the magnetically perturbed Potts field theory at T<Tc
arXiv:0907.3697 · doi:10.1088/1751-8113/43/23/235004
Abstract
The q-state Potts field theory with in the low-temperature phase is considered in presence of a weak magnetic field h. In absence of the magnetic field, the theory is integrable, but not free at q>2: its elementary excitations - the kinks - interact at small distances, and their interaction can be characterized by the factorizable scattering matrix which was found by Chim and Zamolodchikov. The magnetic field induces the long-range attraction between kinks causing their confinement into the bound-states. We calculate the masses of the two-kink bound states in the leading order in |h| -> 0 expressing them in terms of the scattering matrix of kinks at h=0.
20 pages, no figures, v2: one section and references added
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