Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 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: Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM ; volume:2022 ; number:10 ; day:12 ; month:10 ; year:2022 ; pages:1-18 ; date:10.2022
Journal of high energy physics ; 2022, Heft 10 (12.10.2022), 1-18, 10.2022

Creator: Holguin, Adolfo
Wang, Shannon

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2022)078

URN: urn:nbn:de:101:1-2022123021120860010555

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

Last update: 15.08.2025, 7:23 AM CEST

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Holguin, Adolfo
Wang, Shannon
SpringerLink (Online service)

Other Objects (12)

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

$Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM$

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM

$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

$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

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

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

$Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

Non-planar data of N $$ \mathcalN} $$ = 4 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 N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

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

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

$Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM$

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM

$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

$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

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

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

$Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

Non-planar data of N $$ \mathcalN} $$ = 4 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 N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

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

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

$Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM$

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ SYM

$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

$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

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

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

$Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

Non-planar data of N $$ \mathcalN} $$ = 4 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 N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

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

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Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

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Other Objects (12)

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ 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

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

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

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

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

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ 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

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

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

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

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

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

Connected correlator of 1/2 BPS Wilson loops in N = 4 $$ \mathcalN}=4 $$ 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

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

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

Note on generating functions and connected correlators of 1/2-BPS Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

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

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