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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Seeley-DeWitt coefficients in N $$ \mathcalN} $$ = 2 Einstein-Maxwell supergravity theory and logarithmic corrections to N $$ \mathcalN} $$ = 2 extremal black hole entropy ; volume:2019 ; number:8 ; day:9 ; month:8 ; year:2019 ; pages:1-34 ; date:8.2019
Journal of high energy physics ; 2019, Heft 8 (9.8.2019), 1-34, 8.2019

Creator: Karan, Sudip
Banerjee, Gourav
Panda, Binata

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2019)056

URN: urn:nbn:de:101:1-2021090119301351041897

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

Last update: 15.08.2025, 7:28 AM CEST

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Karan, Sudip
Banerjee, Gourav
Panda, Binata
SpringerLink (Online service)

Other Objects (12)

$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

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

$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

$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

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

$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

$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

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

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

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Other Objects (12)

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

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

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

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

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

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

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

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

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

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

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and 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

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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