’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.

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All labels observed (2)

Label Occurrences
't Hooft large-N limit 1
’t Hooft coupling canonical 1

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

Referenced by (2)

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

Gerard ’t Hooft notableWork ’t Hooft coupling
’t Hooft coupling usedIn ’t Hooft coupling self-linksurface differs
subject surface form: 't Hooft coupling
this entity surface form: 't Hooft large-N limit