Polyakov–Nambu–Jona-Lasinio model

E731749

The Polyakov–Nambu–Jona-Lasinio model is an effective quantum field theory that extends the Nambu–Jona-Lasinio model by coupling quarks to the Polyakov loop to study chiral symmetry breaking and confinement in QCD-like systems.

All labels observed (1)

Label Occurrences
Polyakov–Nambu–Jona-Lasinio model canonical 1

How this entity was disambiguated

Statements (44)

Predicate Object
instanceOf QCD effective model ⓘ
effective quantum field theory ⓘ
theoretical physics model ⓘ
aimsTo unify chiral and deconfinement transitions ⓘ
appliesTo QCD-like systems ⓘ
approximates low-energy QCD ⓘ
assumes static temporal gluon background field ⓘ
belongsTo finite-temperature field theory ⓘ
category non-renormalizable model ⓘ
contains effective Polyakov-loop potential ⓘ
quark chemical potential ⓘ
couplesTo Polyakov loop ⓘ
describes chiral symmetry breaking ⓘ
confinement ⓘ
effectiveDegreesOfFreedom constituent quarks ⓘ
energyScale low to intermediate QCD scales ⓘ
extends Nambu–Jona-Lasinio model ⓘ
fieldContent quark fields ⓘ
framework mean-field approximation ⓘ
includes effective gluonic background via Polyakov loop potential ⓘ
four-fermion interactions ⓘ
possible vector interactions ⓘ
scalar-pseudoscalar quark interactions ⓘ
motivatedBy lattice QCD results for Polyakov loop ⓘ
neglects explicit gluon dynamics ⓘ
orderParameters Polyakov loop expectation value ⓘ
chiral condensate ⓘ
predicts crossover deconfinement transition at finite temperature ⓘ
crossover or first-order chiral transitions depending on parameters ⓘ
relatedTo Nambu–Jona-Lasinio model ⓘ
Polyakov loop model ⓘ
linked to: Polyakov loop
spaceTimeDimension 3+1 dimensions ⓘ
studies QCD phase diagram ⓘ
finite density QCD ⓘ
finite temperature QCD ⓘ
symmetry approximate chiral symmetry ⓘ
center symmetry via Polyakov loop ⓘ
usedFor investigating chiral phase transition ⓘ
investigating deconfinement transition ⓘ
usedIn compact star matter studies ⓘ
heavy-ion collision phenomenology ⓘ
strong interaction phenomenology ⓘ
usedToExplore critical end point in QCD phase diagram ⓘ
uses grand canonical ensemble at finite temperature and chemical potential ⓘ

How these facts were elicited

Referenced by (1)

Full triples — surface form annotated when it differs from this entity's canonical label.

Nambu–Jona-Lasinio model → hasVariant → Polyakov–Nambu–Jona-Lasinio model ⓘ