Logarithmic corrections to black hole entropy in matter coupled N $$ \mathcalN} $$ ≥ 1 Einstein-Maxwell supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Logarithmic corrections to black hole entropy in matter coupled N $$ \mathcalN} $$ ≥ 1 Einstein-Maxwell supergravity ; volume:2021 ; number:5 ; day:13 ; month:5 ; year:2021 ; pages:1-45 ; date:5.2021
Journal of high energy physics ; 2021, Heft 5 (13.5.2021), 1-45, 5.2021

Creator: Karan, Sudip
Panda, Binata

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2021)104

URN: urn:nbn:de:101:1-2021111520283562470856

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

Last update: 15.08.2025, 7:38 AM CEST

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Karan, Sudip
Panda, Binata
SpringerLink (Online service)

Other Objects (12)

$Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy$

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

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

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy$

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

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

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity$

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

$Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy$

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

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

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

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Logarithmic corrections to black hole entropy in matter coupled N $$ \mathcalN} $$ ≥ 1 Einstein-Maxwell supergravity

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Other Objects (12)

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

Logarithmic correction to the entropy of extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Logarithmic corrections to the entropy of non-extremal black holes in N $$ \mathcalN} $$ = 1 Einstein-Maxwell supergravity

Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy

Liberated N $$ \mathcalN} $$ = 1 supergravity

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

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

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