Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields ; volume:2022 ; number:5 ; day:16 ; month:5 ; year:2022 ; pages:1-38 ; date:5.2022
Journal of high energy physics ; 2022, Heft 5 (16.5.2022), 1-38, 5.2022

Creator: Buchbinder, Ioseph
Ivanov, Evgeny
Zaigraev, Nikita

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2022)104

URN: urn:nbn:de:101:1-2022072310015968258444

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

Last update: 15.08.2025, 7:27 AM CEST

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Buchbinder, Ioseph
Ivanov, Evgeny
Zaigraev, Nikita
SpringerLink (Online service)

Other Objects (12)

$Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions$

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

$Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops$

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

$Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins$

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings$

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

$A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations$

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine$

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

$N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell$

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

$Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

$Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Grassmannian integral for general gauge invariant off-shell amplitudes 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 $$ \mathcalN} $$

$Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions$

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

$Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops$

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

$Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins$

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings$

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

$A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations$

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine$

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

$N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell$

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

$Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

$Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Grassmannian integral for general gauge invariant off-shell amplitudes 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 $$ \mathcalN} $$

$Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions$

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

$Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops$

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

$Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins$

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

$Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines$

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

$N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings$

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

$A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations$

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine$

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

$N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell$

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

$Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

$Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM$

Grassmannian integral for general gauge invariant off-shell amplitudes 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 $$ \mathcalN} $$

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Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

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Other Objects (12)

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

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

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

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

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

Gravitational couplings in N $$ \mathcalN} $$ = 2 heterotic compactifications with Wilson lines

N $$ \mathcalN} $$ = 2 superconformal higher-spin multiplets and their hypermultiplet couplings

A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Gravitational couplings in N=2 $$ \mathcalN}=2 $$ string compactifications and Mathieu Moonshine

N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

Wilson lines, Grassmannians and gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

Grassmannian integral for general gauge invariant off-shell amplitudes in N = 4 $$ \mathcalN}=4 $$ SYM

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

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