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Properties of $J/ψ$ at $T_c$: QCD second-order Stark effect

arXiv:0802.4000 · doi:10.1103/PhysRevD.79.011501

Abstract

Starting from the temperature dependence of the energy density and pressure from lattice QCD calculation, we extract the temperature dependence of the electric and magnetic condensate near $T_c$. While the magnetic condensate hardly changes across $T_c$, we find that the electric condensate increases abruptly above $T_c$. This induces a small but an equally abrupt decrease in the mass of $J/ψ$, can be calculated through the second-order Stark effect. Combining the present result with the previously determined QCD sum rule constraint, we extract the thermal width of $J/ψ$ above $T_c$, which also increases fast. These changes can be identified as the critical behavior of $J/ψ$ across $T_c$ associated with the phase transition. We find that the mass shift and with broadening of $J/ψ$ at 1.05 $T_c$ will be around -100 MeV and 100 MeV respectively.

5 pages, 4 figures, revised version to appear in Phys.Rev.D