Super-BMS3 algebras from N = 2 $$ \mathcalN}=2 $$ flat supergravities

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Super-BMS3 algebras from N = 2 $$ \mathcalN}=2 $$ flat supergravities ; volume:2016 ; number:11 ; day:24 ; month:11 ; year:2016 ; pages:1-22 ; date:11.2016
Journal of high energy physics ; 2016, Heft 11 (24.11.2016), 1-22, 11.2016

Creator: Lodato, Ivano

Contributor: Merbis, Wout
SpringerLink (Online service)

DOI: 10.1007/JHEP11(2016)150

URN: urn:nbn:de:1111-2016121411418

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:53 AM CEST

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Lodato, Ivano
Merbis, Wout
SpringerLink (Online service)

Other Objects (12)

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography$

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

$N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras$

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

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

$New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds$

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

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

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography$

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

$N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras$

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

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

$New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds$

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

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

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography$

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

$N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras$

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

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

$New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds$

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

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

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Super-BMS3 algebras from N = 2 $$ \mathcalN}=2 $$ flat supergravities

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Other Objects (12)

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

Higher spin algebras and large N $$ \mathcalN} $$ = 4 holography

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

N = 2 $$ \mathcalN}=2 $$ central charge bounds from 2d chiral algebras

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

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

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

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