Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory ; volume:2017 ; number:7 ; day:5 ; month:7 ; year:2017 ; pages:1-48 ; date:7.2017
Journal of high energy physics ; 2017, Heft 7 (5.7.2017), 1-48, 7.2017

Classification: Physik

Creator: Gomes, Joao

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2017)022

URN: urn:nbn:de:1111-201710277682

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:28 AM CEST

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Gomes, Joao
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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Mathieu moonshine and $ \mathcalN}=2 $ string compactifications$

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

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

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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

$Counting all dyons in $ \mathcalN} = 4 $ string theory$

Counting all dyons in $ \mathcalN} = 4 $ string theory

$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

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

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

$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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Mathieu moonshine and $ \mathcalN}=2 $ string compactifications$

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

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

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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

$Counting all dyons in $ \mathcalN} = 4 $ string theory$

Counting all dyons in $ \mathcalN} = 4 $ string theory

$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

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

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

$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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Mathieu moonshine and $ \mathcalN}=2 $ string compactifications$

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

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

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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

$Counting all dyons in $ \mathcalN} = 4 $ string theory$

Counting all dyons in $ \mathcalN} = 4 $ string theory

$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

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

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

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Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

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Other Objects (12)

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

Counting all dyons in $ \mathcalN} = 4 $ string theory

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

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

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

Counting all dyons in $ \mathcalN} = 4 $ string theory

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

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

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Mathieu moonshine and $ \mathcalN}=2 $ string compactifications

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

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

Counting all dyons in $ \mathcalN} = 4 $ string theory

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

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

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