Heavy quark potential at finite imaginary chemical potential

Abstract

We investigate chemical-potential ($\mu$) dependence of the static-quark free energies in both the real and imaginary $\mu$ regions, using the clover-improved two-flavor Wilson fermion action and the renormalization-group improved Iwasaki gauge action. Static-quark potentials are evaluated from Polyakov-loop correlators in the deconfinement phase and the imaginary $\mu =i{\mu }_{\mathrm{I}}$ region and extrapolated to the real $\mu$ region with analytic continuation. As the analytic continuation, the potential calculated at imaginary $\mu =i{\mu }_{\mathrm{I}}$ is expanded into a Taylor-expansion series of $i{\mu }_{\mathrm{I}}/T$ up to 4th order and the pure imaginary variable $i{\mu }_{\mathrm{I}}/T$ is replaced by the real one ${\mu }_{\mathrm{R}}/T$. At real $\mu$, the 4th-order term weakens $\mu$ dependence of the potential sizably. Also, the color-Debye screening mass is extracted from the color-singlet potential at imaginary $\mu$, and the mass is extrapolated to real $\mu$ by analytic continuation. The screening mass thus obtained has stronger $\mu$ dependence than the prediction of the leading-order thermal perturbation theory at both real and imaginary $\mu$.

Comments: 7 pages, 8 figures, presented at the 31st International Symposium on Lattice Field Theory (Lattice 2013), 29 July - 3 August 2013, Mainz, Germany