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000874414 037__ $$aFZJ-2020-01424
000874414 041__ $$aEnglish
000874414 1001_ $$0P:(DE-HGF)0$$aKaczmarek, Olaf$$b0
000874414 1112_ $$aNIC Symposium 2020$$cJülich$$d2020-02-27 - 2020-02-28$$wGermany
000874414 245__ $$aQCD Phase Transition in the Chiral Limit
000874414 260__ $$aJülich$$bForschungszentrum Jülich GmbH Zentralbibliothek, Verlag$$c2020
000874414 29510 $$aNIC Symposium 2020
000874414 300__ $$a193 - 202
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000874414 4900_ $$aPublication Series of the John von Neumann Institute for Computing (NIC) NIC Series$$v50
000874414 520__ $$aWe present a lattice QCD based determination of the chiral phase transition temperature in QCD with two massless (up and down) and one strange quark having its physical mass. We propose and calculate two novel estimators for the chiral transition temperature for several values of the light quark masses, corresponding to Goldstone pion masses in the range of 58 MeV<~m$\pi$<~163 MeV. The chiral phase transition temperature is determined by extrapolating to vanishing pion mass using universal scaling analysis. After thermodynamic, continuum and chiral extrapolations we find the chiral phase transition temperature $T^0_c$ = $132^{+3}_{-6}$ MeV. We also present some preliminary calculations on interplay of effective UA(1) restoration and chiral phase transition towards chiral limit.
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000874414 7001_ $$0P:(DE-HGF)0$$aKarsch, Frithjof$$b1$$eCorresponding author
000874414 7001_ $$0P:(DE-HGF)0$$aLahiri, Anirban$$b2
000874414 7001_ $$0P:(DE-HGF)0$$aMazur, Lukas$$b3
000874414 7001_ $$0P:(DE-HGF)0$$aSchmidt, Christian$$b4
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000874414 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aUniversität Bielefeld$$b0
000874414 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aUniversität Bielefeld$$b1
000874414 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aUniversität Bielefeld$$b2
000874414 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aUniversität Bielefeld$$b3
000874414 9101_ $$0I:(DE-HGF)0$$6P:(DE-HGF)0$$aUniversität Bielefeld$$b4
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000874414 9141_ $$y2020
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000874414 9201_ $$0I:(DE-Juel1)NIC-20090406$$kNIC$$lJohn von Neumann - Institut für Computing$$x0
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