Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography ; volume:2024 ; number:10 ; day:16 ; month:10 ; year:2024 ; pages:1-46 ; date:10.2024
Journal of high energy physics ; 2024, Heft 10 (16.10.2024), 1-46, 10.2024

Creator: Bobev, Nikolay
Choi, Sunjin
Hong, Junho
Reys, Valentin

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2024)121

URN: urn:nbn:de:101:1-2502242136454.991725294471

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

Last update: 15.08.2025, 7:26 AM CEST

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Bobev, Nikolay
Choi, Sunjin
Hong, Junho
Reys, Valentin
SpringerLink (Online service)

Other Objects (12)

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

$Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

$From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs$

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

$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

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

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

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

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

$Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

$From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs$

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

$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

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

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

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

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

$Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

$From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs$

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

$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

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

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

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

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Superconformal indices of 3d N $$ \mathcalN} $$ = 2 SCFTs and holography

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Other Objects (12)

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

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

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

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

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

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

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

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

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

Superconformal partial waves for stress-tensor multiplet correlator in 4D N $$ \mathcalN} $$ = 2 SCFTs

From large to small N $$ \mathcalN} $$ = (4, 4) superconformal surface defects in holographic 6d SCFTs

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

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

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

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

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

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