Finite density QCD with a canonical approach
Philippe de Forcrand (ETH & CERN), Slavo Kratochvila (ETH)

TL;DR
This paper introduces a canonical approach to study QCD directly as a function of baryon density, revealing detailed phase diagram features and interface tensions for four-flavor QCD at finite density.
Contribution
The paper develops a canonical method for QCD that directly relates properties to baryon density, providing new insights into the phase diagram and phase transitions at finite density.
Findings
Identified a first-order transition and coexistence region in the T-rho plane.
Obtained accurate results for systems with up to 30 baryons and mu up to 2 T.
Observed a bending down of the phase boundary at high chemical potential.
Abstract
We present a canonical method where the properties of QCD are directly obtained as a function of the baryon density rho, rather than the chemical potential mu. We apply this method to the determination of the phase diagram of four-flavor QCD. For a pion mass m_pi \sim 350 MeV, the first-order transition between the hadronic and the plasma phase gives rise to a co-existence region in the T-rho plane, which we study in detail, including the associated interface tension. We obtain accurate results for systems containing up to 30 baryons and quark chemical potentials mu up to 2 T. Our T-mu phase diagram agrees with the literature when mu/T \lesssim 1. At larger chemical potential, we observe a ``bending down'' of the phase boundary. We compare the free energy in the confined and deconfined phase with predictions from a hadron resonance gas and from a free massless quark gas respectively.
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