Two dimensional N $$ \mathcalN} $$ = (0, 4) quivers dual to AdS3 solutions in massive IIA

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Two dimensional N $$ \mathcalN} $$ = (0, 4) quivers dual to AdS3 solutions in massive IIA ; volume:2020 ; number:1 ; day:22 ; month:1 ; year:2020 ; pages:1-36 ; date:1.2020
Journal of high energy physics ; 2020, Heft 1 (22.1.2020), 1-36, 1.2020

Creator: Lozano, Yolanda
Macpherson, Niall T.
Nunez, Carlos
Ramirez, Anayeli

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2020)140

URN: urn:nbn:de:101:1-2020042701161281149835

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

Last update: 14.08.2025, 10:59 AM CEST

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Lozano, Yolanda
Macpherson, Niall T.
Nunez, Carlos
Ramirez, Anayeli
SpringerLink (Online service)

Other Objects (12)

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$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

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA$

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$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

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA$

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$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

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA$

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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Two dimensional N $$ \mathcalN} $$ = (0, 4) quivers dual to AdS3 solutions in massive IIA

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Other Objects (12)

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

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