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the fundamental representation (larger color charge), but the color charge is screened at large distances so there is no confinement (and no deconfining transition). Chiral transitions are found in these calculations at much larger energy scales than for quarks in the fundamental representation, providing more evidence that strong, short-range forces can generate chiral phase transitions independent of confinement (Kogut et al., 1982). By integrating over all degrees of freedom except the Wilson-Polyakov loop (14.41) in the partition function (14.37), we obtain from an S U ( N ) theory one that is equivalent to a ZN spin system of the same spatial dimensionality (Svetitsky and Yaffe, 1982; Satz, 1985a). The deconfining phase transition in S U ( N ) gauge theory is associated with spontaneous breaking of the global center ZN of the group (Yaffe and Svetitsky, 1982; Polonyi and Szlachanyi, 1982). The three-dimensional Ising model has symmetry 2 2 [center of SU(2)], and is known to exhibit second order transitions. The 3-state Potts models have symmetry 5 [center of SU(3)], and are known to have first order phase transitions. Therefore, the second order character of the SU(2) deconfining transition and first order character of the SU(3) transition were not a complete surprise (Kogut, 1983). More generally, it is hypothesized that for equivalent spatial dimensionalities an S U ( N ) gauge theory, a Z N gauge theory, and a ZN spin system all belong to the same universality class (see 513.1.8). rdlc gs1 128 Packages matching GS1-128 - NuGet Gallery
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