Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds ; volume:2016 ; number:11 ; day:16 ; month:11 ; year:2016 ; pages:1-13 ; date:11.2016
Journal of high energy physics ; 2016, Heft 11 (16.11.2016), 1-13, 11.2016

Creator: Coimbra, André

Contributor: Strickland-Constable, Charles
SpringerLink (Online service)

DOI: 10.1007/JHEP11(2016)092

URN: urn:nbn:de:1111-201612086104

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:48 AM CEST

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Coimbra, André
Strickland-Constable, Charles
SpringerLink (Online service)

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$Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories$

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$New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics$

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$Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation$

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$N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity$

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

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

$Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes$

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

$Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions$

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Generalised structures for N=1 AdS backgrounds

$Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry$

Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry

The exceptional generalised geometry of supersymmetric AdS flux backgrounds

$Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds$

Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds

$Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions$

Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions

$Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories$

Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories

$New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics$

New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics

$Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation$

Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

$N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity$

N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity

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

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

$Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes$

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

$Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions$

Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions

Generalised structures for N=1 AdS backgrounds

$Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry$

Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry

The exceptional generalised geometry of supersymmetric AdS flux backgrounds

$Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds$

Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds

$Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions$

Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions

$Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories$

Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories

$New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics$

New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics

$Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation$

Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

$N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity$

N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity

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

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

$Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes$

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

$Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions$

Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions

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Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

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Other Objects (12)

Generalised structures for N=1 AdS backgrounds

Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry

The exceptional generalised geometry of supersymmetric AdS flux backgrounds

Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds

Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions

Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories

New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics

Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity

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

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions

Generalised structures for N=1 AdS backgrounds

Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry

The exceptional generalised geometry of supersymmetric AdS flux backgrounds

Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds

Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions

Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories

New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics

Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity

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

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions

Generalised structures for N=1 AdS backgrounds

Marginal deformations of 3d N = 2 $$ \mathcalN}=2 $$ CFTs from AdS4 backgrounds in generalised geometry

The exceptional generalised geometry of supersymmetric AdS flux backgrounds

Supersymmetric Casimir energy on N $$ \mathcalN} $$ = 1 conformal supergravity backgrounds

Rigid 4D N = 2 $$ \mathcalN}=2 $$ supersymmetric backgrounds and actions

Dessins d’enfants in N=2 $$ \mathcalN}=2 $$ generalised quiver theories

New AdS2 backgrounds and N $$ \mathcalN} $$ = 4 conformal quantum mechanics

Exact result in N $$ \mathcalN} $$ = 4 SYM theory: generalised double-logarithmic equation

N $$ \mathcalN} $$ = (8, 0) AdS vacua of three-dimensional supergravity

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

Spinning correlators in N $$ \mathcalN} $$ = 2 SCFTs: Superspace and AdS amplitudes

Embedding formalism for N $$ \mathcalN} $$ -extended AdS superspace in four dimensions

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