On an Nτ=8 MDWF lattice, the non-singlet chiral symmetry restores at Tpc=158.7 MeV, while the UA(1) singlet symmetry remains effectively broken up to 186 MeV, as inferred from the temperature dependence of the topological susceptibility.
Staggered fermions, zero modes, and flavor-singlet mesons
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abstract
We examine the taste structure of eigenvectors of the staggered-fermion Dirac operator. We derive a set of conditions on the eigenvectors of modes with small eigenvalues (near-zero modes), such that staggered fermions reproduce the 't Hooft vertex in the continuum limit. We also show that, assuming these conditions, the correlators of flavor-singlet mesons are free of contributions singular in $1/m$, where $m$ is the quark mass. This conclusion holds also when a single flavor of sea quark is represented by the fourth root of the staggered-fermion determinant. We then test numerically, using the HISQ action, whether these conditions hold on realistic lattice gauge fields. We find that the needed structure does indeed emerge.
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Aspects of the chiral crossover transition in (2+1)-flavor QCD with M\"{o}bius domain-wall fermions
On an Nτ=8 MDWF lattice, the non-singlet chiral symmetry restores at Tpc=158.7 MeV, while the UA(1) singlet symmetry remains effectively broken up to 186 MeV, as inferred from the temperature dependence of the topological susceptibility.