The phase structure of the Polyakov–quark–meson model beyond mean field
By T. Herbst, Jan M. Pawlowski, B. Schaefer. 2010
205 citations recorded by the source corpus.
The Polyakov-extended quark–meson model (PQM) is investigated beyond mean-field. This represents an important step towards a fully dynamical QCD computation. Both the quantum fluctuations to the matter sector and the back-reaction of the matter fluctuations to the QCD Yang–Mills sector are included. Results on the chiral and confinement–deconfinement crossover/phase transition lines and the location of a possible critical endpoint are presented. Moreover, thermodynamic quantities such as the pressure and the quark density are discussed.
Subfields: Condensed Matter Physics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/73536e2dc708553d49d824ec21ab00f175b6e8fd
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In Condensed Matter Physics
In Nuclear and High Energy Physics
Citations in the corpus
- Polyakov loop modeling for hot QCD (2017, background): “The latter has a significant phenomenological impact especially for the size of the QCD criticality region [132, 133, 134].”
- The nonperturbative functional renormalization group and its applications (2020, background): “The phase structure of QCD and the interplay between confinement and chiral symmetry at finite temperature and density have been studied in [927–935].”
- Nonperturbative properties of Yang–Mills theories (2018, unknown): “,[124–137].”
- QCD at finite temperature and chemical potential from Dyson–Schwinger equations (2018, methodology): “The Polyakov-loop enhanced effective models such as the Polyakov-loop Nambu–Jona-Lasinio model (PNJL) [7–9] and the Polyakov-loop quark-meson model (PQM) [10–12] are excellent tools to study a range of fundamental and phenomenological questions related to the QCD phase diagram, see e.”