More on DBI action in 4D N $$ \mathcalN} $$ = 1 supergravity

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: More on DBI action in 4D N $$ \mathcalN} $$ = 1 supergravity ; volume:2017 ; number:1 ; day:27 ; month:1 ; year:2017 ; pages:1-23 ; date:1.2017
Journal of high energy physics ; 2017, Heft 1 (27.1.2017), 1-23, 1.2017

Classification: Physik

Creator: Aoki, Shuntaro

Contributor: Yamada, Yusuke
SpringerLink (Online service)

DOI: 10.1007/JHEP01(2017)121

URN: urn:nbn:de:1111-201702232203

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:53 AM CEST

Data provider

This object is provided by:
Deutsche Nationalbibliothek. If you have any questions about the object, please contact the data provider.

Show original at data provider

Associated

Aoki, Shuntaro
Yamada, Yusuke
SpringerLink (Online service)

Other Objects (12)

$DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

$Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

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

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

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

$Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal 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)

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

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

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

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

$DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

$Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

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

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

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

$Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal 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)

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

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

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

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

$DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

$Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

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

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

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

$Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity$

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal 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)

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

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

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

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

Cultural heritage institutions wishing to register will find more information here.

Fields marked * need to be filled in.

Username*

Please enter your username

Email*

Please enter your email address

Please do not fill this field

First name

Last name

Password*

Please enter your password

Confirm password*

Please enter the same password

I have read and agree to the privacy policy for the collection of personal data.*

This field is required.

I would like to subscribe to the newsletter of the Deutsche Digitale Bibliothek. See newsletter subscription info.

Account created

Your "My DDB" account has been successfully created. Before you can log in to your account, you must click the confirmation link in the message we just sent to the email address you provided.

More on DBI action in 4D N $$ \mathcalN} $$ = 1 supergravity

Show object

References and Relationships

Classification and Topics

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (12)

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

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

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

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

DBI action of real linear superfield in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

Abelian tensor hierarchy in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

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

Abelian tensor hierarchy and Chern-Simons actions in 4D N $$ \mathcalN} $$ = 1 conformal supergravity

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

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

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

Related objects

Reset password