Exploring new constraints on Kähler moduli space of 6d N $$ \mathcalN} $$ = 1 supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Exploring new constraints on Kähler moduli space of 6d N $$ \mathcalN} $$ = 1 supergravity ; volume:2024 ; number:10 ; day:29 ; month:10 ; year:2024 ; pages:1-36 ; date:10.2024
Journal of high energy physics ; 2024, Heft 10 (29.10.2024), 1-36, 10.2024

Creator: Kim, Hee-Cheol
Vafa, Cumrun

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2024)217

URN: urn:nbn:de:101:1-2502242212513.785131972863

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

Last update: 15.08.2025, 7:20 AM CEST

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Kim, Hee-Cheol
Vafa, Cumrun
SpringerLink (Online service)

Other Objects (12)

$Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity$

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity$

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity$

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

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Exploring new constraints on Kähler moduli space of 6d N $$ \mathcalN} $$ = 1 supergravity

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Other Objects (12)

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

Moduli spaces of AdS5 vacua in N $$ \mathcalN} $$ = 2 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

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