4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

to related objects

Alternative title: 1 from 6d D-type N $$ \mathcalN} $$
(1, 0)

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 4d N $$ \mathcalN} $$ ; volume:2020 ; number:1 ; day:23 ; month:1 ; year:2020 ; pages:1-39 ; date:1.2020
Journal of high energy physics ; 2020, Heft 1 (23.1.2020), 1-39, 1.2020

Creator: Chen, Jin
Haghighat, Babak
Liu, Shuwei
Sperling, Marcus

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2020)152

URN: urn:nbn:de:101:1-2020041901282857172639

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

Last update: 14.08.2025, 10:57 AM CEST

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Chen, Jin
Haghighat, Babak
Liu, Shuwei
Sperling, Marcus
SpringerLink (Online service)

Other Objects (12)

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

$On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization$

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

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

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

$On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization$

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

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

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

$On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization$

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

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

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

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4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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Other Objects (12)

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

On exact correlation functions of chiral ring operators in 2d N=2,2 $$ \mathcalN}=\left(2,\ 2\right) $$ SCFTs via localization

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

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

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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