Abstract

The chemical-potential dependence of pi and sigma meson masses is analyzed at both real and imaginary chemical potentials, μRμ_\mathrm{R} and μIμ_\mathrm{I}, by using the Polyakov-loop extended Nambu--Jona-Lasinio (PNJL) model that possesses both the extended Z3{\mathbb Z}_3 symmetry and the chiral symmetry. In the μIμ_\mathrm{I} region, the meson masses have the Roberge-Weiss periodicity. Assuming that the meson masses will be measured at finite μIμ_\mathrm{I} by lattice QCD in future, we simulate how meson masses at finite μRμ_\mathrm{R} are extracted from those at finite μIμ_\mathrm{I}, and propose a reliable extraction method.

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