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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The N = 4 $$ \mathcalN}=4 $$ Schur index with Polyakov loops ; volume:2015 ; number:12 ; day:2 ; month:12 ; year:2015 ; pages:1-15 ; date:12.2015
Journal of high energy physics ; 2015, Heft 12 (2.12.2015), 1-15, 12.2015

Classification: Physik

Creator: Drukker, Nadav

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2015)012

URN: urn:nbn:de:1111-20170822949

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:29 AM CEST

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Drukker, Nadav
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

$N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string$

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

$Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗$

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

$Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

$Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane$

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

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

$Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas$

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

$Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace$

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

$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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

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

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

$N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string$

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

$Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗$

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

$Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

$Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane$

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

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

$Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas$

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

$Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace$

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

$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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

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

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

$N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string$

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

$Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗$

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

$Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory$

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

$Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane$

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

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

$Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas$

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

$Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace$

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

$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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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Other Objects (12)

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

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

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string

Comments on higher rank Wilson loops in N $$ \mathcalN} $$ = 2∗

Combinatorics of Wilson loops in N $$ \mathcalN} $$ = 4 SYM theory

Large N Schur index of N $$ \mathcalN} $$ = 4 SYM from semiclassical D3 brane

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

Wilson loops in 3d N $$ \mathcalN} $$ = 4 SQCD from Fermi gas

Integrability of smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ superspace

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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