S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories ; volume:2016 ; number:6 ; day:8 ; month:6 ; year:2016 ; pages:1-26 ; date:6.2016
Journal of high energy physics ; 2016, Heft 6 (8.6.2016), 1-26, 6.2016

Creator: Aharony, Ofer

Contributor: Tachikawa, Yuji
SpringerLink (Online service)

DOI: 10.1007/JHEP06(2016)044

URN: urn:nbn:de:1111-201606107126

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:48 AM CEST

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Aharony, Ofer
Tachikawa, Yuji
SpringerLink (Online service)

Other Objects (12)

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

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

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

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

$A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index$

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories$

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

$The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index$

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

$More on N $$ \mathcalN} $$ =2 S-folds$

More on N $$ \mathcalN} $$ =2 S-folds

$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

$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

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

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

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

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

$A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index$

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories$

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

$The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index$

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

$More on N $$ \mathcalN} $$ =2 S-folds$

More on N $$ \mathcalN} $$ =2 S-folds

$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

$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

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

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

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

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

$A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index$

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories$

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

$The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index$

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

$More on N $$ \mathcalN} $$ =2 S-folds$

More on N $$ \mathcalN} $$ =2 S-folds

$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

$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

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S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

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Other Objects (12)

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

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

More on N $$ \mathcalN} $$ =2 S-folds

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

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

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

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

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

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

More on N $$ \mathcalN} $$ =2 S-folds

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

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

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

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

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

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

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

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

More on N $$ \mathcalN} $$ =2 S-folds

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

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

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

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

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