Branes and 2d N $$ \mathcalN} $$ = (2, 2) gauge theories with orthogonal and symplectic groups

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Branes and 2d N $$ \mathcalN} $$ = (2, 2) gauge theories with orthogonal and symplectic groups ; volume:2018 ; number:8 ; day:7 ; month:8 ; year:2018 ; pages:1-22 ; date:8.2018
Journal of high energy physics ; 2018, Heft 8 (7.8.2018), 1-22, 8.2018

Classification: Physik

Creator: Bergman, Oren

Contributor: Avraham, Eran
SpringerLink (Online service)

DOI: 10.1007/JHEP08(2018)023

URN: urn:nbn:de:101:1-2018091408173365275828

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:24 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

Bergman, Oren
Avraham, Eran
SpringerLink (Online service)

Other Objects (12)

$Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries$

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM$

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

$Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds$

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

$N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes$

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

$3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices$

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

$Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity$

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes$

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

$Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending$

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

$On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1$

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

zweidimensionales bewegtes Bild

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

$Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries$

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM$

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

$Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds$

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

$N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes$

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

$3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices$

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

$Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity$

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes$

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

$Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending$

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

$On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1$

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

zweidimensionales bewegtes Bild

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

$Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries$

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM$

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

$Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds$

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

$N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes$

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

$3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices$

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

$Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity$

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes$

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

$Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending$

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

$On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1$

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

zweidimensionales bewegtes Bild

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

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 the terms of use and the privacy policy for the collection of personal data and accept them. *

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.

Branes and 2d N $$ \mathcalN} $$ = (2, 2) gauge theories with orthogonal and symplectic groups

Object Details

References and Relationships

Classification and Topics

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (12)

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

Seiberg-like dualities for orthogonal and symplectic 3d N $$ \mathcalN} $$ = 2 gauge theories with boundaries

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

Giant gravitons, Harish-Chandra integrals, and BPS states in symplectic and orthogonal N $$ \mathcalN} $$ = 4 SYM

Branes and symmetries for N $$ \mathcalN} $$ = 3 S-folds

N $$ \mathcalN} $$ = 2 consistent truncations from wrapped M5-branes

3d N $$ \mathcalN} $$ = 2 brane webs and quiver matrices

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

3d N = 2 $$ \mathcalN}=2 $$ minimal SCFTs from wrapped M5-branes

Deconfining N $$ \mathcalN} $$ = 2 SCFTs or the art of brane bending

On α′-effects from D-branes in 4d N $$ \mathcalN} $$ = 1

Reflections, orthogonal and symplectic

Orthogonal and symplectic Yangians

Related objects

Reset password