Three-point functions in N $$ \mathcalN} $$ = 4 SYM at finite N c and background independence

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Three-point functions in N $$ \mathcalN} $$ = 4 SYM at finite N c and background independence ; volume:2020 ; number:5 ; day:25 ; month:5 ; year:2020 ; pages:1-54 ; date:5.2020
Journal of high energy physics ; 2020, Heft 5 (25.5.2020), 1-54, 5.2020

Creator: Suzuki, Ryo

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2020)118

URN: urn:nbn:de:101:1-2020073019421354928966

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:45 AM CEST

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Suzuki, Ryo
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM$

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM$

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM$

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

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Three-point functions in N $$ \mathcalN} $$ = 4 SYM at finite N c and background independence

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Other Objects (12)

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Three-point functions in N = 4 $$ \mathcalN}=4 $$ SYM: the hexagon proposal at three loops

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

A high-precision result for a full-color three-loop three-point form factor in N $$ \mathcalN} $$ = 4 SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

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