Quark spectral density and a strongly-coupled QGP
arXiv:1010.4231 · doi:10.1103/PhysRevD.84.014017
Abstract
The maximum entropy method is used to compute the dressed-quark spectral density from the self-consistent numerical solution of a rainbow truncation of QCD's gap equation at temperatures above that for which chiral symmetry is restored. In addition to the normal and plasmino modes, the spectral function also exhibits an essentially nonperturbative zero mode for temperatures extending to 1.4-1.8-times the critical temperature, T_c. In the neighbourhood of T_c, this long-wavelength mode contains the bulk of the spectral strength and so long as this mode persists, the system may fairly be described as a strongly-coupled state of matter.
4 pages, 2 figures
References in corpus (12)
- The QCD transition temperature: results with physical masses in the continuum limit II.
- Phase diagram and critical endpoint for strongly-interacting quarks
- Hadron Properties and Dyson-Schwinger Equations
- Chiral and deconfinement transition from Dyson-Schwinger equations
- Infrared properties of propagators in Landau-gauge pure Yang-Mills theory at finite temperature
- Regarding confinement and dynamical chiral symmetry breaking in QED3
- Dynamical chiral symmetry breaking and a critical mass
- condensate for light quarks beyond the chiral limit
- Quark spectral properties above Tc from Dyson-Schwinger equations
- Extraction of Spectral Functions from Dyson-Schwinger Studies via the Maximum Entropy Method
- Novel Collective Excitations and the Quasi-Particle Picture of Quarks Coupled with a Massive Boson at Finite Temperature
- Spectral properties of massless and massive quarks coupled with massive boson at finite temperature