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We determine the curvature of the phase transition line in the mu-T plane through an analysis of various observables, including the Polyakov loop, the quark number susceptibilities and the susceptibility of the chiral condensate.
Z. Fodor and S. D. Katz, Lattice determination of the critical point of QCD at finite T and mu JHEP
2002
Earlier work this paper cites.
C. R. Allton et al
2002
Earlier work this paper cites.
P. de Forcrand and O. Philipsen, The QCD phase diagram for small densities from imaginary chemical potential , Nucl. Phys. B
2002
Earlier work this paper cites.
M. D’Elia and M. P. Lombardo, Finite density QCD via imaginary chemical potential , Phys. Rev. D
2003
Earlier work this paper cites.
P. de Forcrand and O. Philipsen, The QCD phase diagram for three degenerate flavors and small baryon density , Nucl. Phys. B
2003
Cited alongside, same era.
Z. Fodor and S. D. Katz, Critical point of QCD at finite T and mu, lattice results for physical quark masses , JHEP
2004
Cited alongside, same era.
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
2006
Cited alongside, same era.
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
2006
Later among the works it cites.
2006
Later among the works it cites.
2007
Later among the works it cites.
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