Linearised actions for N $$ \mathcalN} $$ -extended (higher-spin) superconformal gravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Linearised actions for N $$ \mathcalN} $$ -extended (higher-spin) superconformal gravity ; volume:2019 ; number:8 ; day:13 ; month:8 ; year:2019 ; pages:1-26 ; date:8.2019
Journal of high energy physics ; 2019, Heft 8 (13.8.2019), 1-26, 8.2019

Creator: Buchbinde, Evgeny I.
Hutchings, Daniel
Hutomo, Jessica
Kuzenko, Sergei M.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2019)077

URN: urn:nbn:de:101:1-2021082520084144140940

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

Last update: 14.08.2025, 10:52 AM CEST

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Buchbinde, Evgeny I.
Hutchings, Daniel
Hutomo, Jessica
Kuzenko, Sergei M.
SpringerLink (Online service)

Other Objects (12)

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

$Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets$

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

$Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets$

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

$Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets$

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

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Linearised actions for N $$ \mathcalN} $$ -extended (higher-spin) superconformal gravity

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Other Objects (12)

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

On higher-spin N $$ \mathcalN} $$ = 2 supercurrent multiplets

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Generalised superconformal higher-spin multiplets

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

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