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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM ; volume:2023 ; number:12 ; day:11 ; month:12 ; year:2023 ; pages:1-25 ; date:12.2023
Journal of high energy physics ; 2023, Heft 12 (11.12.2023), 1-25, 12.2023

Creator: Uhlemann, Christoph F.
Wang, Mianqi

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2023)053

URN: urn:nbn:de:101:1-2024022712453298695674

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

Last update: 14.08.2025, 10:56 AM CEST

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Uhlemann, Christoph F.
Wang, Mianqi
SpringerLink (Online service)

Other Objects (12)

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

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

$Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM$

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory$

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$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

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

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

$Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM$

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory$

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$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

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

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

$Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM$

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory$

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$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

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

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Other Objects (12)

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

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

Second order splitting functions and infrared safe cross sections in N $$ \mathcalN} $$ : = 4 SYM theory

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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