Large-N volume independence in conformal and confining gauge theories
arXiv:1006.2101 · doi:10.1007/JHEP08(2010)030
Abstract
Consequences of large volume independence are examined in conformal and confining gauge theories. In the large limit, gauge theories compactified on are independent of the radii, provided the theory has unbroken center symmetry. In particular, this implies that a large gauge theory which, on , flows to an IR fixed point, retains the infinite correlation length and other scale invariant properties of the decompactified theory even when compactified on . In other words, finite volume effects are suppressed. In lattice formulations of vector-like theories, this implies that numerical studies to determine the boundary between confined and conformal phases may be performed on one-site lattice models. In supersymmetric Yang-Mills theory, the center symmetry realization is a matter of choice: the theory on has a moduli space which contains points with all possible realizations of center symmetry. Large QCD with massive adjoint fermions and one or two compactified dimensions has a rich phase structure with an infinite number of phase transitions coalescing in the zero radius limit.
24 pages, added ref
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