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

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

Umfang: 1 Online-Ressource.

Sprache: Englisch

Erschienen in: Spin-2 operators in two-dimensional N $$ \mathcalN} $$ = (4, 0) quivers from massive type IIA ; volume:2024 ; number:10 ; day:31 ; month:10 ; year:2024 ; pages:1-20 ; date:10.2024
Journal of high energy physics ; 2024, Heft 10 (31.10.2024), 1-20, 10.2024

Urheber: Zhang, Shuo

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2024)240

URN: urn:nbn:de:101:1-2502242140119.158528748773

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

Letzte Aktualisierung: 15.08.2025, 07:32 MESZ

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Zhang, Shuo
SpringerLink (Online service)

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

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

$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

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

Wilson loop 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

$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

$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

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

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

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

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

$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

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

Wilson loop 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

$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

$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

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

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

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

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

$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

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

Wilson loop 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

$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

$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

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

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

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

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Ähnliche Objekte (12)

Total Syntheses of Conjugation‐Ready Repeating Units of Acinetobacter baumannii AB5075 for Glycoconjugate Vaccine Development

More on spin-2 operators in holographic quantum mechanics

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

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

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

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

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

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

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

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

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

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

Total Syntheses of Conjugation‐Ready Repeating Units of Acinetobacter baumannii AB5075 for Glycoconjugate Vaccine Development

More on spin-2 operators in holographic quantum mechanics

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

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

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

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

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

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

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

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

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

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

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More on spin-2 operators in holographic quantum mechanics

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

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

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

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

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

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

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

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

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

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

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