Self-dual $ \mathcalN} $ = 2 Born-Infeld theory through auxiliary superfields

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Self-dual $ \mathcalN} $ = 2 Born-Infeld theory through auxiliary superfields ; volume:2014 ; number:5 ; day:15 ; month:5 ; year:2014 ; pages:1-31 ; date:5.2014
Journal of high energy physics ; 2014, Heft 5 (15.5.2014), 1-31, 5.2014

Classification: Physik

Creator: Ivanov, E.A

Contributor: Zupnik, B.M
SpringerLink (Online service)

DOI: 10.1007/JHEP05(2014)061

URN: urn:nbn:de:1111-201801196514

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:49 AM CEST

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Ivanov, E.A
Zupnik, B.M
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions$

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

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

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

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

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

Hamiltonian birefringence and Born-Infeld limits

$N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions$

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

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

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

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

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

Hamiltonian birefringence and Born-Infeld limits

$N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions$

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

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

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

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

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

Hamiltonian birefringence and Born-Infeld limits

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Self-dual $ \mathcalN} $ = 2 Born-Infeld theory through auxiliary superfields

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Other Objects (12)

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

N $$ \mathcalN} $$ = 2* Schur indices

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

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

Hamiltonian birefringence and Born-Infeld limits

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

N $$ \mathcalN} $$ = 2* Schur indices

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

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

Hamiltonian birefringence and Born-Infeld limits

N $$ \mathcalN} $$ = 2 supersymmetry deformations, electromagnetic duality and Dirac-Born-Infeld actions

Born-Infeld supermaze waves

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

N = 2 Born-Infeld attractors

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

N $$ \mathcalN} $$ = 2* Schur indices

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

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

Hamiltonian birefringence and Born-Infeld limits

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