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The finite temperature QCD transition for physical quark masses is a crossover.
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Z. Fodor and S.D. Katz, Lattice determination of the critical point of QCD at finite T and mu , JHEP
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S. Holtmann, J. Engels and T. Schulze, Specific heat and energy for the three-dimensional O(2) model , Nuclear Physics B - Proceedings Supplements
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Z. Fodor and S.D. Katz, Critical point of QCD at finite T and mu, lattice results for physical quark masses , JHEP
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Y. Aoki, G. Endrődi, Z. Fodor, S.D. Katz and K.K. Szabó, The order of the quantum chromodynamics phase transition predicted by the standard model of particle physics , Nature
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Y. Aoki, Z. Fodor, S.D. Katz and K.K. Szabó, The QCD transition temperature: Results with physical masses in the continuum limit , Phys. Lett
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Cited alongside, same era.
Y. Aoki, Z. Fodor, S.D. Katz and K.K. Szabó, The equation of state in lattice QCD: With physical quark masses towards the continuum limit , JHEP
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P. de Forcrand and O. Philipsen, The chiral critical line of N(f) = 2+1 QCD at zero and non-zero baryon density , JHEP
2007
Closest in time.
P. de Forcrand and O. Philipsen, The chiral critical point of N f = 3 N_{f}=3 QCD: towards the continuum , In proceedings of XXV International Symposium on Lattice Field Theory (2007) \pos
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Closest in time.
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