Perturbative solutions of N = 1 ∗ $$ \mathcalN}={1}^{\ast } $$ holography on S 4

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Perturbative solutions of N = 1 ∗ $$ \mathcalN}={1}^{\ast } $$ holography on S 4 ; volume:2019 ; number:7 ; day:29 ; month:7 ; year:2019 ; pages:1-14 ; date:7.2019
Journal of high energy physics ; 2019, Heft 7 (29.7.2019), 1-14, 7.2019

Creator: Kim, Nakwoo
Kim, Se-Jin

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2019)169

URN: urn:nbn:de:101:1-2020040609465653134487

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

Last update: 14.08.2025, 10:48 AM CEST

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Kim, Nakwoo
Kim, Se-Jin
SpringerLink (Online service)

Other Objects (12)

$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

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

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

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

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

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

$Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity$

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds$

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

$Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4$

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

$Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography$

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

$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

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

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

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

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

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

$Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity$

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds$

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

$Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4$

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

$Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography$

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

$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

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

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

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

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

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

$Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity$

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

$Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds$

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

$Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4$

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

$Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography$

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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Perturbative solutions of N = 1 ∗ $$ \mathcalN}={1}^{\ast } $$ holography on S 4

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Other Objects (12)

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

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

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

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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

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

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

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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

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

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

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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

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

Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

Holography for N $$ \mathcalN} $$ = 4 on RP $$ \mathbbmRP} $$ 4

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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