The large N limit of OPEs in symmetric orbifold CFTs with N $$ \mathcalN} $$ = (4, 4) supersymmetry

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The large N limit of OPEs in symmetric orbifold CFTs with N $$ \mathcalN} $$ = (4, 4) supersymmetry ; volume:2019 ; number:8 ; day:5 ; month:8 ; year:2019 ; pages:1-39 ; date:8.2019
Journal of high energy physics ; 2019, Heft 8 (5.8.2019), 1-39, 8.2019

Creator: Beer, Thomas de
Burrington, Benjamin A.
Jardine, Ian T.
Peet, A.W

Contributor: SpringerLink (Online service)

DOI: 10.1007/s13130-019-11019-2

URN: urn:nbn:de:101:1-2021081820212170339557

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

Last update: 14.08.2025, 10:58 AM CEST

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Beer, Thomas de
Burrington, Benjamin A.
Jardine, Ian T.
Peet, A.W
SpringerLink (Online service)

Other Objects (12)

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

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

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d$

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

$Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry$

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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The large N limit of OPEs in symmetric orbifold CFTs with N $$ \mathcalN} $$ = (4, 4) supersymmetry

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Other Objects (12)

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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