Gravitational edge mode in N $$ \mathcalN} $$ = 1 Jackiw-Teitelboim supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Gravitational edge mode in N $$ \mathcalN} $$ = 1 Jackiw-Teitelboim supergravity ; volume:2024 ; number:8 ; day:2 ; month:8 ; year:2024 ; pages:1-35 ; date:8.2024
Journal of high energy physics ; 2024, Heft 8 (2.8.2024), 1-35, 8.2024

Creator: Lee, Kyung-Sun
Sivakumar, Akhil
Yoon, Junggi

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2024)011

URN: urn:nbn:de:101:1-2410252102197.352505042800

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

Last update: 15.08.2025, 7:31 AM CEST

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Lee, Kyung-Sun
Sivakumar, Akhil
Yoon, Junggi
SpringerLink (Online service)

Other Objects (12)

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

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Gravitational edge mode in N $$ \mathcalN} $$ = 1 Jackiw-Teitelboim supergravity

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Other Objects (12)

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

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