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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM ; volume:2021 ; number:3 ; day:29 ; month:3 ; year:2021 ; pages:1-53 ; date:3.2021
Journal of high energy physics ; 2021, Heft 3 (29.3.2021), 1-53, 3.2021

Creator: Delmastro, Diego
Gomis, Jaume

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2021)259

URN: urn:nbn:de:101:1-2021052518513536537927

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

Last update: 17.08.2025, 2:47 PM CEST

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Delmastro, Diego
Gomis, Jaume
SpringerLink (Online service)

Other Objects (12)

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

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

$Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM$

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

$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

$Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM$

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

$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

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

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

$Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM$

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

$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

$Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM$

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

$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

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

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

$Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM$

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

$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

$Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM$

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

$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

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

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Other Objects (12)

Splitting interfaces in 4d 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

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

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

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

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

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

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

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

Splitting interfaces in 4d 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

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

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

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

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

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

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

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

Splitting interfaces in 4d 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

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

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

Supermembranes and domain walls in N $$ \mathcalN} $$ : = 1, D = 4 SYM

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

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

Erratum to: Supermembranes and domain walls in N $$ \mathcalN} $$ = 1, D = 4 SYM

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

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