Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM ; volume:2022 ; number:10 ; day:7 ; month:10 ; year:2022 ; pages:1-44 ; date:10.2022
Journal of high energy physics ; 2022, Heft 10 (7.10.2022), 1-44, 10.2022

Creator: Cabo-Bizet, Alejandro

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2022)052

URN: urn:nbn:de:101:1-2022122621190120070853

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

Last update: 15.08.2025, 7:34 AM CEST

Data provider

This object is provided by:
Deutsche Nationalbibliothek. If you have any questions about the object, please contact the data provider.

Show original at data provider

Associated

Cabo-Bizet, Alejandro
SpringerLink (Online service)

Other Objects (12)

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

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

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

$New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential$

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases$

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

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

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

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

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

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

$New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential$

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases$

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

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

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

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

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

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

$New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential$

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

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

$New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory$

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases$

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

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

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

Cultural heritage institutions wishing to register will find more information here.

Fields marked * need to be filled in.

Username*

Please enter your username

Email*

Please enter your email address

Please do not fill this field

First name

Last name

Password*

Please enter your password

Confirm password*

Please enter the same password

I have read the terms of use and the privacy policy for the collection of personal data and accept them. *

This field is required.

I would like to subscribe to the newsletter of the Deutsche Digitale Bibliothek. See newsletter subscription info.

Account created

Your "My DDB" account has been successfully created. Before you can log in to your account, you must click the confirmation link in the message we just sent to the email address you provided.

Quantum phases of 4d SU(N) N $$ \mathcalN} $$ = 4 SYM

Object Details

References and Relationships

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (12)

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

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

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

New phases of N $$ \mathcalN} $$ = 4 SYM at finite chemical potential

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

New bi-harmonic superspace formulation of 4D, N $$ \mathcalN} $$ = 4 SYM theory

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

Asymptotic growth of the 4d N $$ \mathcalN} $$ = 4 index and partially deconfined phases

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

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

Related objects

Reset password