A note on the N $$ \mathcalN} $$ = 2 super- W 3 $$ \mathcal{W}}_3 $$ holographic dictionary

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: A note on the N $$ \mathcalN} $$ = 2 super- W 3 $$ \mathcal{W}}_3 $$ holographic dictionary ; volume:2020 ; number:12 ; day:28 ; month:12 ; year:2020 ; pages:1-39 ; date:12.2020
Journal of high energy physics ; 2020, Heft 12 (28.12.2020), 1-39, 12.2020

Creator: Castro, Alejandra
Faraggi, Alberto
Osorio, Israel

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2020)177

URN: urn:nbn:de:101:1-2021020119330463659409

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

Last update: 15.08.2025, 7:29 AM CEST

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Castro, Alejandra
Faraggi, Alberto
Osorio, Israel
SpringerLink (Online service)

Other Objects (12)

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK$

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

$A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model$

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds$

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK$

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

$A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model$

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds$

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK$

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

$A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model$

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds$

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

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A note on the N $$ \mathcalN} $$ = 2 super- W 3 $$ \mathcal{W}}_3 $$ holographic dictionary

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Other Objects (12)

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

Towards the holographic dual of N=2 $$ \mathcalN}=2 $$ SYK

A supersymmetric enhancement of N $$ \mathcalN} $$ = 1 holographic minimal model

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Holographic interfaces in N $$ \mathcalN} $$ = 4 SYM: Janus and J-folds

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