Binding Energies and Melting Temperatures of Heavy Hadrons in Quark-Gluon Plasma

We analyze the static potential of a quark-antiquark pair at $T\ge T_c$, where $T_c$ is a temperature of a deconfinement phase transition in QCD. We discuss the possibility that the non-perturbative part of this potential can be studied through the modification of the correlation functions, which define the quadratic field correlators of the nonperturbative vaccuum fields. We use the non-perturbative quark-antiquark potential derived in this way and the screened one-gluon-exchange potential with $T$-dependent Debye screening mass to calculate $J\mathrm{/}\psi$, $\mathrm{{\rm Y}}$ and ${\mathrm{\Omega }}_{bbb}$ binding energies and melting temperatures in the deconfined phase of the full 2-flavors QCD.