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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: An N $$ \mathcalN} $$ = 1 Lagrangian for the rank 1 E 6 superconformal theory ; volume:2020 ; number:12 ; day:16 ; month:12 ; year:2020 ; pages:1-20 ; date:12.2020
Journal of high energy physics ; 2020, Heft 12 (16.12.2020), 1-20, 12.2020

Creator: Zafrir, Gabi

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2020)098

URN: urn:nbn:de:101:1-2021012307005922603377

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

Last update: 15.08.2025, 7:21 AM CEST

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Zafrir, Gabi
SpringerLink (Online service)

Other Objects (12)

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

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

$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 an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$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

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

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

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

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

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

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

$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

$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 an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$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

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

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

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

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

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

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

$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

$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 an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$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

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

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

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

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

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

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

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

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Other Objects (12)

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

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 an N $$ \mathcalN} $$ = 3 SCFT

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

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

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

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

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

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

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 an N $$ \mathcalN} $$ = 3 SCFT

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

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

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

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

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

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

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 an N $$ \mathcalN} $$ = 3 SCFT

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

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

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

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

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

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

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

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