Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

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Alternative title: 4 SYM theory

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ ; volume:2019 ; number:4 ; day:8 ; month:4 ; year:2019 ; pages:1-31 ; date:4.2019
Journal of high energy physics ; 2019, Heft 4 (8.4.2019), 1-31, 4.2019

Creator: Banerjee, Pulak
Chakraborty, Amlan
Dhani, Prasanna K.
Ravindran, V.
Seth, Satyajit

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2019)058

URN: urn:nbn:de:101:1-2019050319101878741878

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

Last update: 14.08.2025, 10:49 AM CEST

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Banerjee, Pulak
Chakraborty, Amlan
Dhani, Prasanna K.
Ravindran, V.
Seth, Satyajit
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

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

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

$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

$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

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

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

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

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

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

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

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

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

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

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

$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

$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

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

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

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

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

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

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

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

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

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

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

$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

$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

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

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

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

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

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Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

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Other Objects (12)

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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