Double-logarithms in N $$ \mathcalN} $$ = 8 supergravity: impact parameter description & mapping to 1-rooted ribbon graphs

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Double-logarithms in N $$ \mathcalN} $$ = 8 supergravity: impact parameter description & mapping to 1-rooted ribbon graphs ; volume:2019 ; number:7 ; day:16 ; month:7 ; year:2019 ; pages:1-20 ; date:7.2019
Journal of high energy physics ; 2019, Heft 7 (16.7.2019), 1-20, 7.2019

Classification: Physik

Creator: Vera, Agustín Sabio

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2019)080

URN: urn:nbn:de:101:1-2019120905174316137554

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

Last update: 14.08.2025, 10:59 AM CEST

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Vera, Agustín Sabio
SpringerLink (Online service)

Other Objects (12)

$Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay$

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

Liberated N $$ \mathcalN} $$ = 1 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

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

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

$Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity$

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

$Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay$

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

Liberated N $$ \mathcalN} $$ = 1 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

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

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

$Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity$

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

$Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay$

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

Liberated N $$ \mathcalN} $$ = 1 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

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

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

$Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity$

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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Double-logarithms in N $$ \mathcalN} $$ = 8 supergravity: impact parameter description & mapping to 1-rooted ribbon graphs

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Other Objects (12)

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

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

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

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

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

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

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

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

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

Double logarithms in N $$ \mathcalN} $$ ≥ 4 supergravity: weak gravity and Shapiro’s time delay

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

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

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

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

Critical N $$ \mathcalN} $$ = (1, 1) general massive supergravity

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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