Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization ; volume:2019 ; number:1 ; day:7 ; month:1 ; year:2019 ; pages:1-55 ; date:1.2019
Journal of high energy physics ; 2019, Heft 1 (7.1.2019), 1-55, 1.2019

Creator: Coronado, Frank

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2019)056

URN: urn:nbn:de:101:1-2019021202551905950226

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

Last update: 14.08.2025, 11:01 AM CEST

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Coronado, Frank
SpringerLink (Online service)

Other Objects (12)

$Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM$

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries$

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity$

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

$All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$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

$Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM$

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries$

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity$

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

$All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$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

$Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM$

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries$

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity$

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

$All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM$

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

$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

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Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

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Other Objects (12)

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

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

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

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

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

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

Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

A note on four-point correlators of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity

All five-loop planar four-point functions of half-BPS operators in N = 4 $$ \mathcalN}=4 $$ SYM

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

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

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