N $$ \mathcalN} $$ = 7 On-shell diagrams and supergravity amplitudes in momentum twistor space

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: N $$ \mathcalN} $$ = 7 On-shell diagrams and supergravity amplitudes in momentum twistor space ; volume:2021 ; number:1 ; day:27 ; month:1 ; year:2021 ; pages:1-47 ; date:1.2021
Journal of high energy physics ; 2021, Heft 1 (27.1.2021), 1-47, 1.2021

Urheber: Armstrong, Connor
Farrow, Joseph A.
Lipstein, Arthur E.

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2021)181

URN: urn:nbn:de:101:1-2021032120171330184275

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

Letzte Aktualisierung: 15.08.2025, 07:31 MESZ

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Beteiligte

Armstrong, Connor
Farrow, Joseph A.
Lipstein, Arthur E.
SpringerLink (Online service)

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$On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes$

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

$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

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

$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

$Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 supergravity$

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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

$On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes$

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

$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

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

$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

$Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 supergravity$

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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

$On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes$

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

$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

$All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes$

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

$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

$Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 supergravity$

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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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N $$ \mathcalN} $$ = 7 On-shell diagrams and supergravity amplitudes in momentum twistor space

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Ähnliche Objekte (12)

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

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

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

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

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

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

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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

On-shell diagrams for N $$ \mathcalN} $$ = 8 supergravity amplitudes

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

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

All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes

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

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

Multi-Regge limit of the two-loop five-point amplitudes in N $$ \mathcalN} $$ = 4 super Yang-Mills and N $$ \mathcalN} $$ = 8 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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