Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation ; volume:2022 ; number:5 ; day:26 ; month:5 ; year:2022 ; pages:1-37 ; date:5.2022
Journal of high energy physics ; 2022, Heft 5 (26.5.2022), 1-37, 5.2022

Creator: Velizhanin, V. N.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2022)176

URN: urn:nbn:de:101:1-2022073006023730632842

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

Last update: 15.08.2025, 7:22 AM CEST

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Velizhanin, V. N.
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 $$ \mathcalN} $$

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

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

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

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

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

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

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

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

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

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

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

$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 $$ \mathcalN} $$

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

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

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

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

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

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

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

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

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

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

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

$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 $$ \mathcalN} $$

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

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

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

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

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

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

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

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

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

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

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

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

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

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Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

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Other Objects (12)

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

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

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

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

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

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

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

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

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

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

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

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

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

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

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

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

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

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

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

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

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

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

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

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

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

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

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

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

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

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

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