N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography ; volume:2024 ; number:5 ; day:31 ; month:5 ; year:2024 ; pages:1-34 ; date:5.2024
Journal of high energy physics ; 2024, Heft 5 (31.5.2024), 1-34, 5.2024

Creator: Lang, Julian
Neiman, Yasha

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2024)341

URN: urn:nbn:de:101:1-2408092107246.547955558428

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

Last update: 14.08.2025, 11:03 AM CEST

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Lang, Julian
Neiman, Yasha
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

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

$Holography for N $$ \mathcalN} $$ = 1∗ on S 4$

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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

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

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

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

$Holography for N $$ \mathcalN} $$ = 1∗ on S 4$

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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

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

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

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

$Holography for N $$ \mathcalN} $$ = 1∗ on S 4$

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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Other Objects (12)

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

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

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

Holography for N $$ \mathcalN} $$ = 1∗ on S 4

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

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