Damping of hard excitations in strongly coupled N $$ \mathcalN} $$ = 4 plasma

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Damping of hard excitations in strongly coupled N $$ \mathcalN} $$ = 4 plasma ; volume:2016 ; number:12 ; day:13 ; month:12 ; year:2016 ; pages:1-34 ; date:12.2016
Journal of high energy physics ; 2016, Heft 12 (13.12.2016), 1-34, 12.2016

Classification: Physik

Creator: Fuini, John F.

Contributor: Uhlemann, Christoph F.
Yaffe, Laurence G.
SpringerLink (Online service)

DOI: 10.1007/JHEP12(2016)042

URN: urn:nbn:de:1111-201701101722

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:44 AM CEST

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Fuini, John F.
Uhlemann, Christoph F.
Yaffe, Laurence G.
SpringerLink (Online service)

Other Objects (12)

$Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality$

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

$New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability$

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

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

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

$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

$Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills$

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

$Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills$

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

$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

$Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality$

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

$New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability$

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

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

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

$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

$Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills$

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

$Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills$

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

$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

$Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality$

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

$New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability$

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

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

$Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM$

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

$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

$Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills$

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

$Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills$

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

$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

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Damping of hard excitations in strongly coupled N $$ \mathcalN} $$ = 4 plasma

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Other Objects (12)

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

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

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

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

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

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

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

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

Strongly coupled phases of N = 1 $$ \mathcalN}=1 $$ S-duality

New approach to strongly coupled N $$ \mathcalN} $$ = 4 SYM via integrability

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

Far beyond the planar limit in strongly-coupled N $$ \mathcalN} $$ = 4 SYM

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

Regge meets collinear in strongly-coupled N = 4 $$ \mathcalN}=4 $$ super Yang-Mills

Exploring Reggeon bound states in strongly-coupled N $$ \mathcalN} $$ = 4 super Yang-Mills

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

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

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

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