Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1434-6052

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM ; volume:82 ; number:5 ; day:12 ; month:5 ; year:2022 ; pages:1-10 ; date:5.2022
The European physical journal / C. C, Particles and fields ; 82, Heft 5 (12.5.2022), 1-10, 5.2022

Classification: Physik

Creator: Kadoh, Daisuke
Ukita, Naoya

Contributor: SpringerLink (Online service)

DOI: 10.1140/epjc/s10052-022-10404-y

URN: urn:nbn:de:101:1-2022083018545325543256

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

Last update: 15.08.2025, 7:22 AM CEST

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Kadoh, Daisuke
Ukita, Naoya
SpringerLink (Online service)

Other Objects (12)

$Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM$

Spatially modulated and supersymmetric mass deformations of 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 $$ \mathcalN} $$

$Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT$

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1$

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

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

$Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM$

Spatially modulated and supersymmetric mass deformations of 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 $$ \mathcalN} $$

$Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT$

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1$

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

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

$Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM$

Spatially modulated and supersymmetric mass deformations of 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 $$ \mathcalN} $$

$Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT$

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1$

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

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

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Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

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Other Objects (12)

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

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

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

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

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

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

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

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

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

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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

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