The Bethe-Ansatz approach to the N $$ \mathcalN} $$ = 4 superconformal index at finite rank

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The Bethe-Ansatz approach to the N $$ \mathcalN} $$ = 4 superconformal index at finite rank ; volume:2021 ; number:6 ; day:21 ; month:6 ; year:2021 ; pages:1-39 ; date:6.2021
Journal of high energy physics ; 2021, Heft 6 (21.6.2021), 1-39, 6.2021

Creator: Lezcano, Alfredo González
Hong, Junho
Liu, James T.
Pando Zayas, Leopoldo A.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2021)126

URN: urn:nbn:de:101:1-2021121418494197997067

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

Last update: 11.06.2025, 1:57 PM CEST

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Lezcano, Alfredo González
Hong, Junho
Liu, James T.
Pando Zayas, Leopoldo A.
SpringerLink (Online service)

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Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory$

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

$On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories$

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

$Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index$

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory$

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

$On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories$

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

$Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index$

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory$

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

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The Bethe-Ansatz approach to the N $$ \mathcalN} $$ = 4 superconformal index at finite rank

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Other Objects (12)

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

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