Hauptseite > Publikationsdatenbank > Baryon and meson screening masses |
Journal Article | FZJ-2015-04120 |
; ; ; ;
2013
Soc.
[S.l.]
This record in other databases:
Please use a persistent id in citations: http://hdl.handle.net/2128/8869 doi:10.1103/PhysRevD.87.074038
Abstract: In a strongly coupled quark-gluon plasma, collective excitations of gluons and quarks should dominate over the excitation of individual quasifree gluon and quark modes. To explore this possibility, we computed screening masses for ground-state light-quark mesons and baryons at leading order in a symmetry-preserving truncation scheme for the Dyson-Schwinger equations using a confining formulation of a contact interaction at nonzero temperature. Meson screening masses are obtained from Bethe-Salpeter equations, and baryon analogues from a novel construction of the Faddeev equation, which employs an improved quark-exchange approximation in the kernel. Our treatment implements a deconfinement transition that is coincident with chiral symmetry restoration in the chiral limit, when both transitions are second order. Despite deconfinement, in all T=0 bound-state channels, strong correlations persist above the critical temperature, T>Tc; and, in the spectrum defined by the associated screening masses, degeneracy between parity-partner correlations is apparent for T≳1.3Tc. Notwithstanding these results, there are reasons (including Golberger-Treiman relations) to suppose that the inertial masses of light-quark bound states, when they may be defined, vanish at the deconfinement temperature, and that this is a signal of bound-state dissolution. Where a sensible comparison is possible, our predictions are consistent with results from contemporary numerical simulations of lattice-regularized QCD.
![]() |
The record appears in these collections: |