Quarkonia in the deconfined phase: effective potentials and lattice correlators

Abstract

The Schroedinger equation for the charmonium and bottomonium states at finite temperature is solved by employing an effective temperature dependent potential given by a linear combination of the color singlet free and internal energies obtained on the lattice from the Polyakov loop correlation functions. The melting temperatures and other properties of the quarkonium states are evaluated. The consistency of the potential model approach with the available lattice data on the quarkonium temporal correlators and spectral functions is explored.

31 pages, 12 figures

References in corpus (2)

• Quarkonium correlators and spectral functions at zero and finite temperature
• Potential Models and Lattice Gauge Current-Current Correlators

Cited by in corpus (15)

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• Dissociation of quarkonium in hot QCD medium: Modification of the inter-quark potential
• On temperature dependence of quarkonium correlators
• Potential models and lattice correlators for quarkonia at finite temperature
• The thermal width of heavy quarkonia moving in quark gluon plasma
• In-medium modification of P-wave charmonia from QCD sum rules
• Progress in finite temperature lattice QCD
• Describing Charmonium Correlation Functions in Euclidean Time
• Existence of mesons after deconfinement
• Properties of quark gluon plasma from lattice calculations
• Properties of Quarkonia at T_c