Correlation functions of the chiral stress-tensor multiplet in N = 4 $$ \mathcalN}=4 $$ SYM

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Correlation functions of the chiral stress-tensor multiplet in N = 4 $$ \mathcalN}=4 $$ SYM ; volume:2015 ; number:6 ; day:29 ; month:6 ; year:2015 ; pages:1-51 ; date:6.2015
Journal of high energy physics ; 2015, Heft 6 (29.6.2015), 1-51, 6.2015

Classification: Physik

Creator: Chicherin, Dmitry

Contributor: Doobary, Reza
Eden, Burkhard
Heslop, Paul
Korchemsky, Gregory P.
Mason, Lionel
Sokatchev, Emery
SpringerLink (Online service)

DOI: 10.1007/JHEP06(2015)198

URN: urn:nbn:de:1111-201708224447

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:32 AM CEST

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Associated

Chicherin, Dmitry
Doobary, Reza
Eden, Burkhard
Heslop, Paul
Korchemsky, Gregory P.
Mason, Lionel
Sokatchev, Emery
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 $$ \mathcalN} $$

$Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs$

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

$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

$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

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

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

$Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs$

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

$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

$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

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

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

$Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs$

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

$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

$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

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Correlation functions of the chiral stress-tensor multiplet in N = 4 $$ \mathcalN}=4 $$ SYM

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Other Objects (12)

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

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

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

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

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

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

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

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

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

Chiral limit of N $$ \mathcalN} $$ = 4 SYM and ABJM and integrable Feynman graphs

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

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

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