All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes
- Location
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Deutsche Nationalbibliothek Frankfurt am Main
- ISSN
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1029-8479
- Extent
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Online-Ressource
- Language
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Englisch
- Notes
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online resource.
- Bibliographic citation
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All-loop-orders relation between Regge limits of N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity four-point amplitudes ; volume:2021 ; number:2 ; day:4 ; month:2 ; year:2021 ; pages:1-32 ; date:2.2021
Journal of high energy physics ; 2021, Heft 2 (4.2.2021), 1-32, 2.2021
- Creator
- Contributor
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SpringerLink (Online service)
- DOI
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10.1007/JHEP02(2021)044
- URN
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urn:nbn:de:101:1-2021051614205068526947
- Rights
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Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.
- Last update
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14.08.2025, 10:55 AM CEST
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Associated
- Naculich, Stephen G.
- SpringerLink (Online service)
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Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity
Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization
Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries
Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM
Non-planar data of N $$ \mathcalN} $$ = 4 SYM
Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM
Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM
Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory
The Bethe roots of Regge cuts in strongly coupled N = 4 $$ \mathcalN}=4 $$ SYM theory
Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids
Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM
N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$
Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity
Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization
Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries
Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM
Non-planar data of N $$ \mathcalN} $$ = 4 SYM
Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM
Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM
Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory
The Bethe roots of Regge cuts in strongly coupled N = 4 $$ \mathcalN}=4 $$ SYM theory
Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids
Tessellating cushions: four-point functions in N $$ \mathcalN} $$ = 4 SYM
N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$
Proof of a three-loop relation between the Regge limits of four-point amplitudes in N $$ \mathcalN} $$ = 4 SYM and N $$ \mathcalN} $$ = 8 supergravity
Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization
Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries
Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM
Non-planar data of N $$ \mathcalN} $$ = 4 SYM
Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM
Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM
Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory
The Bethe roots of Regge cuts in strongly coupled N = 4 $$ \mathcalN}=4 $$ SYM theory