N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

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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 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality ; volume:2015 ; number:8 ; day:27 ; month:8 ; year:2015 ; pages:1-27 ; date:8.2015
Journal of high energy physics ; 2015, Heft 8 (27.8.2015), 1-27, 8.2015

Classification: Physik

Creator: Bolognesi, Stefano

Contributor: Giacomelli, Simone
Konishi, Kenichi
SpringerLink (Online service)

DOI: 10.1007/JHEP08(2015)131

URN: urn:nbn:de:101:1-2018082502245080015464

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:35 AM CEST

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Bolognesi, Stefano
Giacomelli, Simone
Konishi, Kenichi
SpringerLink (Online service)

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

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N $$ \mathcalN} $$ = 2 S-duality revisited

$N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories$

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$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

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Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

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$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

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

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

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

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

$N $$ \mathcalN} $$ = 2 S-duality revisited$

N $$ \mathcalN} $$ = 2 S-duality revisited

$N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories$

N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories

$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories

$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality$

Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality

$Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories$

Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories

$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

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

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

$N $$ \mathcalN} $$ = 2 S-duality revisited$

N $$ \mathcalN} $$ = 2 S-duality revisited

$N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories$

N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories

$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories

$3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality$

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality$

Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality

$Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories$

Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories

$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

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N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

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Other Objects (12)

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

N $$ \mathcalN} $$ = 2 S-duality revisited

N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality

Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories

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

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

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

N $$ \mathcalN} $$ = 2 S-duality revisited

N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality

Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories

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

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

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

N $$ \mathcalN} $$ = 2 S-duality revisited

N $$ \mathcalN} $$ =1 Lagrangians for generalized Argyres-Douglas theories

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories

3d N $$ \mathcalN} $$ = 3 generalized Giveon-Kutasov duality

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Wilson loops in 5d N = 1 $$ \mathcalN}=1 $$ theories and S-duality

Modular anomaly equation, heat kernel and S-duality in $ \mathcalN}=2 $ theories

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

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

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