Heavy quarkonium states with the holographic potential

The quarkonium states in a quark-gluon plasma is examined with the heavy quark potential implied by the holographic principle. Both the vanila AdS-Schwarzschild metric and the one with an infrared cutoff are considered. The dissociation temperature is calculated by solving the Schrödinger equation of the potential model. In the case of the AdS-Schwarzschild metric with a IR cutoff, the ratios of the dissociation temperatures for J/ψ and Upsilon with the U-ansatz of the potential to the deconfinement temperature are found to agree with the lattice results within a factor of two.