Abstract
We study and mesons at finite temperature using an effective field theory based on chiral and heavy-quark spin-flavor symmetries within the imaginary-time formalism. Interactions with the light degrees of freedom are unitarized via a Bethe-Salpeter approach, and the and self-energies are calculated self-consistently. We generate dynamically the and states, and study their possible identification as the chiral partners of the and ground states, respectively. We show the evolution of their masses and decay widths as functions of temperature, and provide an analysis of the chiral-symmetry restoration in the heavy-flavor sector below the transition temperature. In particular, we analyse the very special case of the -meson, for which the chiral partner is associated to the double-pole structure of the .
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