New $ \mathcalN}=1 $ dualities from orientifold transitions Part II: string theory

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: New $ \mathcalN}=1 $ dualities from orientifold transitions Part II: string theory ; volume:2013 ; number:10 ; day:1 ; month:10 ; year:2013 ; pages:1-50 ; date:10.2013
Journal of high energy physics ; 2013, Heft 10 (1.10.2013), 1-50, 10.2013

Creator: García-Etxebarria, Iñaki
Heidenreich, Ben
Wrase, Timm

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2013)006

URN: urn:nbn:de:101:1-2021080820354877510526

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

Last update: 14.08.2025, 10:49 AM CEST

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García-Etxebarria, Iñaki
Heidenreich, Ben
Wrase, Timm
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory$

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions$

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

$New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles$

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities$

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

$Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD$

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory$

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions$

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

$New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles$

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities$

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

$Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD$

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory$

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions$

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

$New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles$

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities$

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

$Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD$

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

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New $ \mathcalN}=1 $ dualities from orientifold transitions Part II: string theory

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Other Objects (12)

N $$ \mathcalN} $$ = 1 conformal dualities

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

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

N $$ \mathcalN} $$ = 1 conformal dualities

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

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

N $$ \mathcalN} $$ = 1 conformal dualities

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

New $ \mathcalN} $ = 1 dualities from orientifold transitions Part I: field theory

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Abelian dualities of N $$ \mathcalN} $$ = (0, 4) boundary conditions

New 3d N $$ \mathcalN} $$ : = 2 dualities from quadratic monopoles

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Nonrelativistic strings and the limits of N $$ \mathcalN} $$ = 2 dualities

Dualities and phases of 3d N = 1 $$ \mathcalN}=1 $$ SQCD

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