Bootstrapping correlation functions 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: Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM ; volume:2016 ; number:3 ; day:7 ; month:3 ; year:2016 ; pages:1-24 ; date:3.2016
Journal of high energy physics ; 2016, Heft 3 (7.3.2016), 1-24, 3.2016

Creator: Chicherin, Dmitry

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

DOI: 10.1007/JHEP03(2016)031

URN: urn:nbn:de:1111-2016072711384

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:50 AM CEST

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Chicherin, Dmitry
Doobary, Reza
Eden, Burkhard
Heslop, Paul
Korchemsky, Gregory P.
Sokatchev, Emery
SpringerLink (Online service)

Other Objects (12)

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

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

$Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM$

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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

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

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

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

$Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM$

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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

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

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

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

$Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM$

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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

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

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

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Other Objects (12)

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

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

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 mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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

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

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