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

zu Verbundenen Objekten

Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Non-planar data of N $$ \mathcalN} $$ = 4 SYM ; volume:2020 ; number:3 ; day:2 ; month:3 ; year:2020 ; pages:1-25 ; date:3.2020
Journal of high energy physics ; 2020, Heft 3 (2.3.2020), 1-25, 3.2020

Urheber: Fleury, Thiago
Pereira, Raul

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2020)003

URN: urn:nbn:de:101:1-2020052419150081904235

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

Letzte Aktualisierung: 14.08.2025, 10:54 MESZ

Datenpartner

Dieses Objekt wird bereitgestellt von:
Deutsche Nationalbibliothek. Bei Fragen zum Objekt wenden Sie sich bitte an den Datenpartner.

Original beim Datenpartner anzeigen

Beteiligte

Fleury, Thiago
Pereira, Raul
SpringerLink (Online service)

Ähnliche Objekte (12)

$Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections$

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

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

$Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization$

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

$Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit$

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

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$

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

$Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization$

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

$On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories$

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

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

$Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections$

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

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

$Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization$

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

$Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit$

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

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$

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

$Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization$

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

$On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories$

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

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

$Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections$

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

$Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes$

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

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

$Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization$

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

$Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit$

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

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$

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

$Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization$

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

$On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories$

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

$Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM$

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

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

Informationen zur Registrierung von Kultur- und Wissenseinrichtungen finden Sie hier.

Felder mit * müssen ausgefüllt werden.

Benutzername*

Bitte geben Sie Ihren Benutzernamen ein

E-Mail*

Bitte geben Sie Ihre E-Mail ein

Bitte füllen Sie dieses Feld nicht aus

Vorname

Nachname

Passwort*

Bitte geben Sie Ihr Passwort ein

Passwort bestätigen*

Bitte geben Sie das gleiche Passwort ein

Ich habe die Nutzungsbedingungen und die Datenschutzerklärung zur Erhebung persönlicher Daten gelesen und stimme ihnen zu. *

Dieses Feld ist ein Pflichtfeld.

Ich möchte den Newsletter der Deutschen Digitalen Bibliothek abonnieren. Siehe Informationen zum Newsletter-Abonnement.

Benutzerkonto angelegt

Ihr „Meine DDB“-Konto wurde erfolgreich angelegt. Bevor Sie sich in Ihrem Konto anmelden können, müssen Sie auf den Bestätigungslink in der Nachricht klicken, die wir gerade an die von Ihnen angegebene E-Mail-Adresse geschickt haben

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

Angaben zum Objekt

Verweise und Beziehungen

Beteiligte, Orts- und Zeitangaben

Weitere Informationen

Datenpartner

Beteiligte

Ähnliche Objekte (12)

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

Antisymmetric Wilson loops in N=4 $$ \mathcalN}=4 $$ SYM: from exact results to non-planar corrections

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

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

Non-planar corrections in orbifold/orientifold N $$ \mathcalN} $$ = 2 superconformal theories from localization

Antisymmetric Wilson loops in N $$ \mathcalN} $$ = 4 SYM beyond the planar limit

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

On-shell diagrams and the geometry of planar N < 4 $$ \mathcalN}<4 $$ SYM theories

Multi-particle amplitudes from the four-point correlator in planar N $$ \mathcalN} $$ = 4 SYM

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

Verbundene Objekte

Passwort zurücksetzen