Abstract

We analyze the pseudo-critical behavior of three-flavor QCD using highly improved staggered quarks (HISQ) on lattices with temporal extent Nτ=8N_τ=8 and for quark masses corresponding to a pseudoscalar Goldstone mass in the range 80 MeV ≲ mπ ≲ 140 MeV80 ~ {\rm MeV} ~ \lesssim ~ m_π~ \lesssim ~ 140 ~ {\rm MeV}. Our findings are consistent with the occurrence of a second order chiral phase transition at vanishing values of the quark masses. The chiral phase transition temperature at this finite value of the lattice spacing is determined to be Tc=98−6+3 MeVT_c = 98_{-6}^{+3}~{\rm MeV}. A comparison with a corresponding analysis performed in (2+1)-flavor QCD suggests that the continuum limit extrapolated chiral phase transition temperature in 3-flavor QCD will turn out to be below 90 MeV90 ~ {\rm MeV}.

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