Mesoscopic QCD and the Theta Vacua
arXiv:hep-th/0108166 · doi:10.1016/S0550-3213(01)00635-6
Abstract
The partition function of QCD is analyzed for an arbitrary number of flavors, N_f, and arbitrary quark masses including the contributions from all topological sectors in the Leutwyler--Smilga regime. For given N_f and arbitrary vacuum angle, θ, the partition function can be reduced to N_f-2 angular integrations of single Bessel functions. For two and three flavors, the θdependence of the QCD vacuum is studied in detail. For N_f= 2 and 3, the chiral condensate decreases monotonically as θincreases from zero to πand the chiral condensate develops a cusp at θ=πfor degenerate quark masses in the macroscopic limit. We find a discontinuity at θ=πin the first derivative of the energy density with respect to θfor degenerate quark masses. This corresponds to the first--order phase transition in which CP is spontaneously broken, known as Dashen's phenomena.
31 pages, revtex, 10 figures, final version to appear in Nucl. Phys. B
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Cited by in corpus (15)
- SU(N) gauge theories at large N
- Theta dependence of SU(N) gauge theories in the presence of a topological term
- Deconfining Phase Transition as a Matrix Model of Renormalized Polyakov Loops
- Singular values of the Dirac operator in dense QCD-like theories
- Deconfinement in Matrix Models about the Gross--Witten Point
- The Chiral Condensate in a Finite Volume
- Cumulants of the QCD topological charge distribution
- Chiral perturbation theory in a theta vacuum
- Dashen's Phenomenon in Gauge Theories with Spontaneously Broken Chiral Symmetries
- The Heisenberg XX spin chain and low-energy QCD
- Chiral symmetry breaking with no bilinear condensate revisited
- Interpolation between the epsilon and p regimes
- Dirac spectrum of one-flavor QCD at θ=0 and continuity of the chiral condensate
- Chiral condensate and Dirac spectrum of one- and two-flavor QCD at nonzero -angle
- Phase structure with nonzero and twisted mass fermions