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
This entity first appeared as the object of triple T8325622 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Polyakov–Nambu–Jona-Lasinio model Context triple: [Nambu–Jona-Lasinio model, hasVariant, Polyakov–Nambu–Jona-Lasinio model]
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A.
Nambu–Jona-Lasinio model
The Nambu–Jona-Lasinio model is a theoretical framework in quantum field theory that illustrates spontaneous chiral symmetry breaking and mass generation for fermions, analogous to mechanisms in superconductivity.
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B.
Schwinger model
The Schwinger model is a two-dimensional quantum electrodynamics theory that serves as a exactly solvable toy model for studying phenomena like confinement, chiral symmetry breaking, and anomalies in quantum field theory.
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C.
Georgi–Glashow model
The Georgi–Glashow model is a grand unified theory in particle physics that unifies the strong, weak, and electromagnetic interactions within an SU(5) gauge symmetry framework.
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D.
Polyakov action
The Polyakov action is a fundamental formulation of string theory that describes the dynamics of relativistic strings via a two-dimensional worldsheet embedded in spacetime.
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E.
Polyakov
Polyakov is a common Russian surname borne by numerous notable figures in fields such as physics, mathematics, politics, and the arts.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Polyakov–Nambu–Jona-Lasinio model Target entity description: 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.
-
A.
Nambu–Jona-Lasinio model
The Nambu–Jona-Lasinio model is a theoretical framework in quantum field theory that illustrates spontaneous chiral symmetry breaking and mass generation for fermions, analogous to mechanisms in superconductivity.
-
B.
Schwinger model
The Schwinger model is a two-dimensional quantum electrodynamics theory that serves as a exactly solvable toy model for studying phenomena like confinement, chiral symmetry breaking, and anomalies in quantum field theory.
-
C.
Georgi–Glashow model
The Georgi–Glashow model is a grand unified theory in particle physics that unifies the strong, weak, and electromagnetic interactions within an SU(5) gauge symmetry framework.
-
D.
Polyakov action
The Polyakov action is a fundamental formulation of string theory that describes the dynamics of relativistic strings via a two-dimensional worldsheet embedded in spacetime.
-
E.
Polyakov
Polyakov is a common Russian surname borne by numerous notable figures in fields such as physics, mathematics, politics, and the arts.
- F. None of above. chosen
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 NERFINISHED ⓘ |
| describes |
chiral symmetry breaking
ⓘ
confinement ⓘ |
| effectiveDegreesOfFreedom | constituent quarks ⓘ |
| energyScale | low to intermediate QCD scales ⓘ |
| extends | Nambu–Jona-Lasinio model NERFINISHED ⓘ |
| 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
NERFINISHED
ⓘ
Polyakov loop model NERFINISHED ⓘ |
| 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
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You are a knowledge base construction expert. Given a subject entity and a description of it, return factual statements that you know for the subject as a JSON list of dictionaries(triples), where keys must be "subject", "predicate" and "object". The number of facts may be very high, between 25 to 50 or more, for very popular subjects. For less popular subjects, the number of facts can be very low, like 5 or 10. # Requirements - If you don't know the subject at all, return an empty list. - If the subject is not a named entity, return an empty list. - Include at least one triple where predicate is "instanceOf". - Do not get too wordy. - Separate several objects into multiple triples with one object.
Subject: Polyakov–Nambu–Jona-Lasinio model Description of subject: 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.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.