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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities ; volume:2016 ; number:6 ; day:13 ; month:6 ; year:2016 ; pages:1-44 ; date:6.2016
Journal of high energy physics ; 2016, Heft 6 (13.6.2016), 1-44, 6.2016

Creator: Lee, Jeongseog

Contributor: Yamazaki, Masahito
SpringerLink (Online service)

DOI: 10.1007/JHEP06(2016)077

URN: urn:nbn:de:1111-201606178411

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:59 AM CEST

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Lee, Jeongseog
Yamazaki, Masahito
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

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

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

$4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging$

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

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

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

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

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

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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

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

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

$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

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

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

$4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging$

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

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

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

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

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

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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

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

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

$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

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

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

$4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging$

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

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

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

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

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

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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

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

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

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

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Other Objects (12)

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

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

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

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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

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

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

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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

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

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

4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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

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

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

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

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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

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

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

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