Modular anomaly equation for Schur index of N $$ \mathcalN} $$ = 4 super-Yang-Mills

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Modular anomaly equation for Schur index of N $$ \mathcalN} $$ = 4 super-Yang-Mills ; volume:2022 ; number:8 ; day:3 ; month:8 ; year:2022 ; pages:1-12 ; date:8.2022
Journal of high energy physics ; 2022, Heft 8 (3.8.2022), 1-12, 8.2022

Creator: Huang, Min-xin

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2022)049

URN: urn:nbn:de:101:1-2022101920180984784997

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

Last update: 15.08.2025, 7:22 AM CEST

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Huang, Min-xin
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups$

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops$

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

$N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions$

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

$Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models$

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups$

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops$

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

$N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions$

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

$Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models$

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups$

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

$Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills$

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops$

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

$N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions$

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

$Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models$

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

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Modular anomaly equation for Schur index of N $$ \mathcalN} $$ = 4 super-Yang-Mills

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Other Objects (12)

N $$ \mathcalN} $$ = 2* Schur indices

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

N $$ \mathcalN} $$ = 2* Schur indices

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

N $$ \mathcalN} $$ = 2* Schur indices

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Schur indices for N $$ \mathcalN} $$ = 4 super-Yang-Mills with more general gauge groups

Taming defects in N $$ \mathcalN} $$ = 4 super-Yang-Mills

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops

N $$ \mathcalN} $$ = (1, 0) anomaly multiplet relations in six dimensions

Boundary Weyl anomaly of N $$ \mathcalN} $$ = (2, 2) superconformal models

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

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