All tree-level MHV form factors in N $$ \mathcalN} $$ = 4 SYM from twistor space

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: All tree-level MHV form factors in N $$ \mathcalN} $$ = 4 SYM from twistor space ; volume:2016 ; number:6 ; day:28 ; month:6 ; year:2016 ; pages:1-26 ; date:6.2016
Journal of high energy physics ; 2016, Heft 6 (28.6.2016), 1-26, 6.2016

Creator: Koster, Laura

Contributor: Mitev, Vladimir
Staudacher, Matthias
Wilhelm, Matthias
SpringerLink (Online service)

DOI: 10.1007/JHEP06(2016)162

URN: urn:nbn:de:1111-2016070110295

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:47 AM CEST

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Koster, Laura
Mitev, Vladimir
Staudacher, Matthias
Wilhelm, Matthias
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

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

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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

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

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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$Non-planar data of N $$ \mathcalN} $$ = 4 SYM$

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory$

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids$

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

$Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects$

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM$

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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All tree-level MHV form factors in N $$ \mathcalN} $$ = 4 SYM from twistor space

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Other Objects (12)

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

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

Non-planar data of N $$ \mathcalN} $$ = 4 SYM

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

Celestial superamplitude in N $$ \mathcalN} $$ = 4 SYM theory

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Phase structure of N $$ \mathcalN} $$ = 2* SYM on ellipsoids

Bootstrap equations for N $$ \mathcalN} $$ = 4 SYM with defects

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Quark-anti-quark potential in N $$ \mathcalN} $$ = 4 SYM

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