N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity ; volume:2015 ; number:7 ; day:13 ; month:7 ; year:2015 ; pages:1-42 ; date:7.2015
Journal of high energy physics ; 2015, Heft 7 (13.7.2015), 1-42, 7.2015

Classification: Physik

Creator: Bawane, Aditya

Contributor: Bonelli, Giulio
Ronzani, Massimiliano
Tanzini, Alessandro
SpringerLink (Online service)

DOI: 10.1007/JHEP07(2015)054

URN: urn:nbn:de:1111-201802249859

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:51 AM CEST

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Bawane, Aditya
Bonelli, Giulio
Ronzani, Massimiliano
Tanzini, Alessandro
SpringerLink (Online service)

Other Objects (12)

$Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters$

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

$Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories$

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

$On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2$

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories$

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory$

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

$The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings$

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

$Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters$

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

$Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories$

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

$On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2$

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories$

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory$

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

$The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings$

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

$Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters$

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

$Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories$

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

$On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2$

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

$Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories$

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

$Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories$

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory$

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

$The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings$

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics$

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

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Other Objects (12)

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Singular BPS boundary conditions in N $$ \mathcalN} $$ = (2, 2) supersymmetric gauge theories

On N $$ \mathcalN} $$ = 2 supersymmetric gauge theories on S 2 × S 2

Effective gravitational couplings of four-dimensional N $$ \mathcalN} $$ = 2 supersymmetric gauge theories

Goldstinos, supercurrents and metastable SUSY breaking in $ \mathcalN} = 2 $ supersymmetric gauge theories

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

Low-energy dynamics of 3d N $$ \mathcalN} $$ = 2 G 2 supersymmetric gauge theory

The NSVZ relations for N $$ \mathcalN} $$ = 1 supersymmetric theories with multiple gauge couplings

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

Quaternion-Kähler N $$ \mathcalN} $$ = 4 supersymmetric mechanics

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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