Duality walls in the 4d N $$ \mathcalN} $$ = 2 SU(N) gauge theory with 2N flavours

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Duality walls in the 4d N $$ \mathcalN} $$ = 2 SU(N) gauge theory with 2N flavours ; volume:2019 ; number:11 ; day:11 ; month:11 ; year:2019 ; pages:1-38 ; date:11.2019
Journal of high energy physics ; 2019, Heft 11 (11.11.2019), 1-38, 11.2019

Creator: Garozzo, Ivan
Mekareeya, Noppadol
Sacchi, Matteo

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2019)053

URN: urn:nbn:de:101:1-2020051723091113979353

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

Last update: 14.08.2025, 10:48 AM CEST

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Garozzo, Ivan
Mekareeya, Noppadol
Sacchi, Matteo
SpringerLink (Online service)

Other Objects (12)

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

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

$N $$ \mathcalN} $$ = 2 S-duality revisited$

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

$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

$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$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

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

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

$N $$ \mathcalN} $$ = 2 S-duality revisited$

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

$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

$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$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

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

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

$N $$ \mathcalN} $$ = 2 S-duality revisited$

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

$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

$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$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

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Duality walls in the 4d N $$ \mathcalN} $$ = 2 SU(N) gauge theory with 2N flavours

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Other Objects (12)

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

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

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

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

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

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

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

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

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

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

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

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

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

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

N $$ \mathcalN} $$ = 2 S-duality revisited

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

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

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

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

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

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