A modification to the Laplace transform of the quark propagator is introduced in a nonlocal model to align confining and deconfining regimes, allowing computation of meson screening masses over a wide temperature range and pole masses up to the transition.
Bazavov, et al., The chiral and deconfinement aspects of the QCD transition
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Mesonic modes in confining model at finite temperature
A modification to the Laplace transform of the quark propagator is introduced in a nonlocal model to align confining and deconfining regimes, allowing computation of meson screening masses over a wide temperature range and pole masses up to the transition.