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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index ; volume:2024 ; number:6 ; day:28 ; month:6 ; year:2024 ; pages:1-22 ; date:6.2024
Journal of high energy physics ; 2024, Heft 6 (28.6.2024), 1-22, 6.2024

Creator: Amariti, Antonio
Mantegazza, Fabio

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2024)206

URN: urn:nbn:de:101:1-2409230941566.436943312760

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

Last update: 15.08.2025, 7:32 AM CEST

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Amariti, Antonio
Mantegazza, Fabio
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action$

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

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

$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

$A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions$

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

$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

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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

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

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

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

$Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action$

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

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

$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

$A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions$

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

$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

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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

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

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

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

$Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action$

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

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

$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

$A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions$

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

$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

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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

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Other Objects (12)

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

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

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

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

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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

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

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

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

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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

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

Superconformal duality-invariant models and N $$ \mathcalN} $$ = 4 SYM effective action

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

A new duality between N $$ \mathcalN} $$ = 8 superconformal field theories in three dimensions

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

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

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