’t Hooft coupling
E415089
The ’t Hooft coupling is a rescaled gauge coupling constant, central in large-N gauge theory and string theory, that remains finite in the ’t Hooft large-N limit and controls the strength of interactions.
All labels observed (2)
| Label | Occurrences |
|---|---|
| 't Hooft large-N limit | 1 |
| ’t Hooft coupling canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T4142070 — 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: ’t Hooft coupling Context triple: [Gerard ’t Hooft, notableWork, ’t Hooft coupling]
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A.
Gauge Theory Correlators from Non-Critical String Theory
"Gauge Theory Correlators from Non-Critical String Theory" is a research paper that explores how non-critical string theory can be used to compute correlation functions in gauge theories, contributing to the development and understanding of the AdS/CFT correspondence.
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B.
AdS/CFT correspondence
The AdS/CFT correspondence is a conjectured duality in theoretical physics that equates a gravity theory in anti-de Sitter space with a conformal field theory on its boundary, providing a powerful framework for understanding quantum gravity and strongly coupled quantum field theories.
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C.
Yukawa coupling
The Yukawa coupling is a parameter in quantum field theory that quantifies the strength of interaction between a scalar field (such as the Higgs field) and a fermion, determining the fermion’s mass after symmetry breaking.
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D.
Gell-Mann–Low theorem
The Gell-Mann–Low theorem is a fundamental result in quantum field theory that rigorously connects interacting quantum fields to free fields via the adiabatic switching-on of interactions, underpinning the use of perturbation theory and the Dyson series.
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E.
Yang–Mills theory
Yang–Mills theory is a gauge field theory describing the behavior of non-abelian gauge fields, forming the mathematical foundation for modern particle physics, including the strong and electroweak interactions.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: ’t Hooft coupling Target entity description: The ’t Hooft coupling is a rescaled gauge coupling constant, central in large-N gauge theory and string theory, that remains finite in the ’t Hooft large-N limit and controls the strength of interactions.
-
A.
Gauge Theory Correlators from Non-Critical String Theory
"Gauge Theory Correlators from Non-Critical String Theory" is a research paper that explores how non-critical string theory can be used to compute correlation functions in gauge theories, contributing to the development and understanding of the AdS/CFT correspondence.
-
B.
AdS/CFT correspondence
The AdS/CFT correspondence is a conjectured duality in theoretical physics that equates a gravity theory in anti-de Sitter space with a conformal field theory on its boundary, providing a powerful framework for understanding quantum gravity and strongly coupled quantum field theories.
-
C.
Yukawa coupling
The Yukawa coupling is a parameter in quantum field theory that quantifies the strength of interaction between a scalar field (such as the Higgs field) and a fermion, determining the fermion’s mass after symmetry breaking.
-
D.
Gell-Mann–Low theorem
The Gell-Mann–Low theorem is a fundamental result in quantum field theory that rigorously connects interacting quantum fields to free fields via the adiabatic switching-on of interactions, underpinning the use of perturbation theory and the Dyson series.
-
E.
Yang–Mills theory
Yang–Mills theory is a gauge field theory describing the behavior of non-abelian gauge fields, forming the mathematical foundation for modern particle physics, including the strong and electroweak interactions.
- F. None of above. chosen
Statements (45)
| Predicate | Object |
|---|---|
| instanceOf |
coupling constant
ⓘ
physical quantity ⓘ |
| appliesTo |
gauge theory
ⓘ
surface form:
SU(N) gauge theories
|
| category | renormalized coupling ⓘ |
| controls |
convergence properties of large-N expansion
ⓘ
weight of Feynman diagrams in large-N expansion ⓘ |
| definition | λ = g^2 N ⓘ |
| dependsOn |
gauge coupling g
ⓘ
rank of gauge group N ⓘ |
| field |
gauge theory
ⓘ
quantum field theory ⓘ string theory ⓘ theoretical physics ⓘ |
| hasAspect |
strong 't Hooft coupling regime
ⓘ
weak 't Hooft coupling regime ⓘ |
| limitCondition | N → ∞ with λ fixed ⓘ |
| namedAfter |
Gerard ’t Hooft
ⓘ
surface form:
Gerard 't Hooft
|
| property |
dimensionless in four-dimensional gauge theories
ⓘ
remains finite in 't Hooft large-N limit ⓘ scale dependent in asymptotically free theories ⓘ |
| relatedTo |
Wilson loops in large-N limit
ⓘ
anomalous dimensions of operators ⓘ beta function of gauge theory ⓘ curvature radius of AdS space ⓘ double-scaling limits in matrix models ⓘ AdS/CFT correspondence ⓘ
surface form:
gauge-string duality
genus expansion in string theory ⓘ integrability in N = 4 SYM ⓘ planar diagram expansion ⓘ planar limit of QCD-like theories ⓘ string coupling g_s via large-N dualities ⓘ string tension in AdS/CFT ⓘ strong-weak coupling duality ⓘ |
| role |
connects gauge theory perturbation theory to string perturbation theory
ⓘ
controls interaction strength in large-N limit ⓘ effective coupling in AdS/CFT duality ⓘ effective expansion parameter for planar diagrams ⓘ organizes perturbative expansion in 1/N ⓘ |
| symbol | λ ⓘ |
| usedFor | matching gauge theory and string theory parameters ⓘ |
| usedIn |
’t Hooft coupling
self-linksurface differs
ⓘ
surface form:
't Hooft large-N limit
AdS/CFT correspondence ⓘ Yang–Mills theory ⓘ
surface form:
N = 4 supersymmetric Yang–Mills theory
large-N gauge theory ⓘ matrix models ⓘ |
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Subject: ’t Hooft coupling Description of subject: The ’t Hooft coupling is a rescaled gauge coupling constant, central in large-N gauge theory and string theory, that remains finite in the ’t Hooft large-N limit and controls the strength of interactions.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.