Abstract

In the absence of a genuine solution to the sign problem, lattice studies at imaginary quark chemical potential are an important tool to constrain the QCD phase diagram. We calculate the values of the tricritical quark masses in the Roberge-Weiss plane, $\mu=\imath\pi T/3$, which separate mass regions with chiral and deconfinement phase transitions from the intermediate region, for QCD with $N_\text{f}=2$ unimproved staggered quarks on $N_\tau=6$ lattices. A quantitative measure for the quality of finite size scaling plots is developed, which significantly reduces the subjective judgement required for fitting. We observe that larger aspect ratios are necessary to unambiguously determine the order of the transition than at $\mu=0$. Comparing with previous results from $N_\tau=4$ we find a $\sim50$% reduction in the light tricritical pion mass. The heavy tricritical pion mass stays roughly the same, but is too heavy to be resolved on $N_\tau=6$ lattices and thus equally afflicted with cut-off effects. Further comparison with other discretizations suggests that current cut-off effects on the light critical masses are likely to be larger than $\sim100$%, implying a drastic shrinking of the chiral first-order region to possibly zero.

Highlights

  • The theoretical prediction of the QCD phase diagram as a function of temperature T and baryon chemical potential μB has proved to be a difficult challenge for several decades

  • The results obtained in Ref. [26] with Wilson fermions on Nτ 1⁄4 6 lattices, i.e., with similar lattice spacing, appear to have considerably larger cut-off effects

  • It is interesting to compare the position of the tricritical points in physical units, mtπr;ilci;gWhtilson 1⁄4 669þ−8915 MeV mtπr;ilci;gShttaggered 1⁄4 328þ−8414 MeV

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Summary

Introduction

The theoretical prediction of the QCD phase diagram as a function of temperature T and baryon chemical potential μB has proved to be a difficult challenge for several decades. Because of the nonperturbative nature of the strong interactions on hadronic scales, a first principles approach such as lattice QCD is required. Because of the severe sign problem of lattice QCD at finite μB, standard Monte Carlo simulations are limited to addressing small densities, μB < 3T, only [1,2]. Even at zero baryon density, there remain open questions.

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