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Chiral phase transition of $N_f$=2+1 and 3 QCD at vanishing baryon chemical potential

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arxiv 1511.00553 v1 pith:B7TBPCOQ submitted 2015-11-02 hep-lat nucl-th

classification hep-latnucl-th
keywords chiralmassesphasephysicalpionquarkquarkssimulations
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We present updated results on chiral phase structure in (2+1)-flavor ($N_f$=2+1) and 3-flavor ($N_f=3$) QCD based on the simulations using Highly Improved Staggered Quarks on lattices with temporal extent $N_\tau$ =6 at vanishing baryon chemical potential. In $N_f$=2+1 QCD we have performed simulations with a strange quark fixed to its physical value and two degenerate light quarks whose values are adjusted to have 5 values of Goldstone pion masses in the region of 160 - 80 MeV in the continuum limit. The universal scaling behavior of chiral condensates as well as chiral susceptibilities is discussed and the tri-critical point is suggested to be located below the physical point, i.e. at smaller than physical strange quark mass. In $N_f$=3 QCD simulations with 6 different masses of 3 degenerate quarks corresponding to the Goldstone pion masses in the region of 230 - 80 MeV have also been performed. Our results suggest that the QCD transition with these values of quark masses is of crossover type and an upper bound of the critical pion mass where the first order phase transition starts is estimated to be about 50 MeV.

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  1. Effects of Born-Infeld Electrodynamics on Chiral Symmetry Restoration and Meson Susceptibilities in Holographic QCD

    hep-ph 2026-08 conditional novelty 5.0 of 10

    In a soft-wall holographic QCD model on a Born-Infeld black hole, stronger bulk nonlinearity shifts the chiral phase boundary to higher temperatures without changing the transition order.

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