N $$ \mathcalN} $$ = 4 SYM, (super)-polynomial rings and emergent quantum mechanical symmetries

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: Online-Ressource, 1 online resource.

Language: Englisch

Bibliographic citation: N $$ \mathcalN} $$ = 4 SYM, (super)-polynomial rings and emergent quantum mechanical symmetries ; volume:2023 ; number:2 ; day:17 ; month:2 ; year:2023 ; pages:1-51 ; date:2.2023
Journal of high energy physics ; 2023, Heft 2 (17.2.2023), 1-51, 2.2023

Classification: Physik

Creator: Mello Koch, Robert de
Ramgoolam, Sanjaye

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2023)176

URN: urn:nbn:de:101:1-2023101308385393435999

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

Last update: 14.08.2025, 10:55 AM CEST

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Mello Koch, Robert de
Ramgoolam, Sanjaye
SpringerLink (Online service)

Other Objects (12)

$Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification$

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

$Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM$

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM

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

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

$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 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

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

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

$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

$Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification$

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

$Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM$

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM

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

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

$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 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

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

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

$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

$Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification$

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

$Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM$

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ SYM

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

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

$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 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

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

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

$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

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N $$ \mathcalN} $$ = 4 SYM, (super)-polynomial rings and emergent quantum mechanical symmetries

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Other Objects (12)

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ 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

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

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

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

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

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

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

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

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ 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

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

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

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

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

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

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

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

Non-invertible symmetries of N $$ \mathcalN} $$ = 4 SYM and twisted compactification

Emergent supersymmetry in the marginal deformations of N = 4 $$ \mathcalN}=4 $$ 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

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

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

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

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

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

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

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

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