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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: N $$ \mathcalN} $$ = 4 SYM line defect Schur index and semiclassical string ; volume:2024 ; number:10 ; day:4 ; month:10 ; year:2024 ; pages:1-35 ; date:10.2024
Journal of high energy physics ; 2024, Heft 10 (4.10.2024), 1-35, 10.2024

Classification: Physik

Creator: Beccaria, M.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2024)046

URN: urn:nbn:de:101:1-2502182126247.706766213349

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

Last update: 15.08.2025, 7:28 AM CEST

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Beccaria, M.
SpringerLink (Online service)

Other Objects (12)

$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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

$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

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

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

$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

$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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

$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

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

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

$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

$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

$Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory$

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

$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

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

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

$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

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

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Other Objects (12)

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

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

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

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

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

Exact large charge in N $$ \mathcalN} $$ = 4 SYM and semiclassical string theory

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

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

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

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

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

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