Abstract

We propose a novel Bayesian method to analytically continue observables to real baryochemical potential $\mu_B$ in finite density QCD. Taylor coefficients at $\mu_B=0$ and data at imaginary chemical potential $\mu_B^I$ are treated on equal footing. We consider two different constructions for the Pad\'e approximants, the classical multipoint Pad\'e approximation and a mixed approximation that is a slight generalization of a recent idea in Pad\'e approximation theory. Approximants with spurious poles are excluded from the analysis. As an application, we perform a joint analysis of the available continuum extrapolated lattice data for both pseudocritical temperature $T_c$ at $\mu_B^I$ from the Wuppertal-Budapest Collaboration and Taylor coefficients $\kappa_2$ and $\kappa_4$ from the HotQCD Collaboration. An apparent convergence of $[p/p]$ and $[p/p+1]$ sequences of rational functions is observed with increasing $p.$ We present our extrapolation up to $\mu_B\approx 600$ MeV.

Highlights

  • Despite considerable effort invested so far, the phase diagram of QCD in the temperature(T)-baryon chemical potential(μB) plane still awaits determination from first principles

  • These results come either from the evaluation of Taylor coefficients with lattice simulations performed at μB 1⁄4 0 or via simulations performed at imaginary μB, where the sign problem is absent, with the Taylor coefficients obtained from a subsequent fit

  • We show that the Padeapproximant knows nothing about the location of the tricritical point (TCP), as this information is not encoded in TcðμBÞ

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Summary

Introduction

Despite considerable effort invested so far, the phase diagram of QCD in the temperature(T)-baryon chemical potential(μB) plane still awaits determination from first principles. Whether the input data are the Taylor coefficients or the values of a function at several values of the imaginary chemical potential, fact is that the numerical analytic continuation needed to extrapolate the crossover to real μB is a mathematically ill-posed problem [4,5]. This means that the analytic continuation of a function

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