The imaginary part of the heavy-quark potential from real-time Yang-Mills dynamics
arXiv:2102.12587 · doi:10.1007/JHEP10(2021)083
Abstract
We extract the imaginary part of the heavy-quark potential using classical-statistical simulations of real-time Yang-Mills dynamics in classical thermal equilibrium. The -dependence of the imaginary part of the potential is extracted by measuring the temporal decay of Wilson loops of spatial length . We compare our results to continuum expressions obtained using hard thermal loop theory and to semi-analytic lattice perturbation theory calculations using the hard classical loop formalism. We find that, when plotted as a function of , where is the hard classical loop Debye mass, the imaginary part of the heavy-quark potential shows little sensitivity to the lattice spacing at small and agrees well with the semi-analytic hard classical loop result. For large quark-antiquark separations, we quantify the magnitude of the non-perturbative long-range corrections to the imaginary part of the heavy-quark potential. We present our results for a wide range of temperatures, lattice spacings, and lattice volumes. This work sets the stage for extracting the imaginary part of the heavy-quark potential in an expanding non-equilibrium Yang Mills plasma.
arXiv comment25 pages, 9 figures, 1 table; v2 - major revision, published version
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