Abstract

We determine the curvature of the (pseudo)critical line of QCD with nfn_f=2+1 staggered fermions at nonzero temperature and quark density, by analytic continuation from imaginary chemical potentials. Monte Carlo simulations are performed adopting the HISQ/tree action discretization, as implemented in the code by the MILC collaboration, suitably modified to include a nonzero imaginary baryon chemical potential. We work on a line of constant physics, as determined in Ref.\cite{Bazavov:2011nk}, adjusting the couplings so as to keep the strange quark mass msm_s fixed at its physical value, with a light to strange mass ratio ml/ms=1/20m_l/m_s=1/20. In the present investigation we set the chemical potential at the same value for the three quark species, μl=μs≡μμ_l=μ_s\equiv μ. We explore lattices of different spatial extensions, 163×616^3\times 6 and 243×624^3\times 6, to check for finite size effects, and present results on a 323×832^3 \times 8 lattice, to check for finite cut-off effects. We discuss our results for the curvature κκ of the critical line at μ=0μ= 0, which indicate κ=0.018(4)κ=0.018(4), and compare them with previous lattice determinations by alternative methods and with experimental determinations of the freeze-out curve.

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