A note on one-loop cluster adjacency in N $$ \mathcalN} $$ = 4 SYM

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: A note on one-loop cluster adjacency in N $$ \mathcalN} $$ = 4 SYM ; volume:2021 ; number:1 ; day:15 ; month:1 ; year:2021 ; pages:1-13 ; date:1.2021
Journal of high energy physics ; 2021, Heft 1 (15.1.2021), 1-13, 1.2021

Creator: Mago, Jorge
Schreiber, Anders
Spradlin, Marcus
Volovich, Anastasia

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2021)084

URN: urn:nbn:de:101:1-2021030613173995153508

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

Last update: 15.08.2025, 7:37 AM CEST

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Mago, Jorge
Schreiber, Anders
Spradlin, Marcus
Volovich, Anastasia
SpringerLink (Online service)

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One-loop divergences in 6D, N $$ \mathcalN} $$ = (1, 0) SYM theory

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$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Multi-loop positivity of the planar N $$ \mathcalN} $$ = 4 SYM six-point amplitude$

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$Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM$

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$Refined counting of necklaces in one-loop N = 4 $$ \mathcalN}=4 $$ SYM$

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$Simple loop integrals and amplitudes in $ \mathcalN} = 4 $ SYM$

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$The four-loop N $$ \mathcalN} $$ = 4 SYM Sudakov form factor$

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$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

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$Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM$

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A note on one-loop cluster adjacency in N $$ \mathcalN} $$ = 4 SYM

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Other Objects (12)

All one-loop NMHV gluon amplitudes in $ \mathcalN} $ = 1 SYM

One-loop divergences in 6D, N $$ \mathcalN} $$ = (1, 0) SYM theory

Refined counting of necklaces in one-loop N = 4 $$ \mathcalN}=4 $$ SYM

One-loop amplitudes in AdS5 ×S5 supergravity from N $$ \mathcalN} $$ = 4 SYM at strong coupling

One-loop amplitudes for N $$ \mathcalN} $$ = 2 homogeneous supergravities

Simple loop integrals and amplitudes in $ \mathcalN} = 4 $ SYM

The one-loop six-dimensional hexagon integral and its relation to MHV amplitudes in $ \mathcalN} = 4 $ SYM

The four-loop N $$ \mathcalN} $$ = 4 SYM Sudakov form factor

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Multi-loop positivity of the planar N $$ \mathcalN} $$ = 4 SYM six-point amplitude

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

All one-loop NMHV gluon amplitudes in $ \mathcalN} $ = 1 SYM

One-loop divergences in 6D, N $$ \mathcalN} $$ = (1, 0) SYM theory

Refined counting of necklaces in one-loop N = 4 $$ \mathcalN}=4 $$ SYM

One-loop amplitudes in AdS5 ×S5 supergravity from N $$ \mathcalN} $$ = 4 SYM at strong coupling

One-loop amplitudes for N $$ \mathcalN} $$ = 2 homogeneous supergravities

Simple loop integrals and amplitudes in $ \mathcalN} = 4 $ SYM

The one-loop six-dimensional hexagon integral and its relation to MHV amplitudes in $ \mathcalN} = 4 $ SYM

The four-loop N $$ \mathcalN} $$ = 4 SYM Sudakov form factor

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Multi-loop positivity of the planar N $$ \mathcalN} $$ = 4 SYM six-point amplitude

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

All one-loop NMHV gluon amplitudes in $ \mathcalN} $ = 1 SYM

One-loop divergences in 6D, N $$ \mathcalN} $$ = (1, 0) SYM theory

Refined counting of necklaces in one-loop N = 4 $$ \mathcalN}=4 $$ SYM

One-loop amplitudes in AdS5 ×S5 supergravity from N $$ \mathcalN} $$ = 4 SYM at strong coupling

One-loop amplitudes for N $$ \mathcalN} $$ = 2 homogeneous supergravities

Simple loop integrals and amplitudes in $ \mathcalN} = 4 $ SYM

The one-loop six-dimensional hexagon integral and its relation to MHV amplitudes in $ \mathcalN} = 4 $ SYM

The four-loop N $$ \mathcalN} $$ = 4 SYM Sudakov form factor

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Multi-loop positivity of the planar N $$ \mathcalN} $$ = 4 SYM six-point amplitude

Bootstrapping two-loop Feynman integrals for planar N = 4 $$ \mathcalN}=4 $$ sYM

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

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