Topology in the SU(N_f) chiral symmetry restored phase of unquenched QCD and axion cosmology II
arXiv:1704.04906 · doi:10.1103/PhysRevD.96.014505
Abstract
We investigate the physical consequences of the survival of the effects of the U(1)_A anomaly in the chiral symmetric phase of QCD, and show that the free energy density is a singular function of the quark mass m, in the chiral limit, and that the and susceptibilities diverge in this limit at any . We also show that the difference between the and susceptibilities diverges in the chiral limit at any , a result which seems to be excluded by recent results of Tomiya et al. from numerical simulations of two-flavor QCD. We also discuss on the generalization of these results to the model.
9 pages, no figures, new references added
References in corpus (5)
- Microscopic Origin of \boldmath{} Symmetry Violation in the High Temperature Phase of QCD
- Lattice QCD for Cosmology
- On the strength of the anomaly at the chiral phase transition in QCD
- Topology in the SU(Nf) chiral symmetry restored phase of unquenched QCD and axion cosmology
- Lattice QCD at nonzero temperature and density
Cited by in corpus (5)
- Axions, Instantons, and the Lattice
- Massive Schwinger model at finite
- Axial U(1) symmetry, topology, and Dirac spectra at high temperature in lattice QCD
- Interplay between chiral symmetry, axial anomaly and massless bosons
- Spectral density of the Dirac-Ginsparg-Wilson operator, chiral anomaly, and analyticity in the high temperature phase of