Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills ; volume:2022 ; number:4 ; day:5 ; month:4 ; year:2022 ; pages:1-65 ; date:4.2022
Journal of high energy physics ; 2022, Heft 4 (5.4.2022), 1-65, 4.2022

Creator: Bissi, Agnese
Fardelli, Giulia
Manenti, Andrea

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2022)016

URN: urn:nbn:de:101:1-2022062419095488083748

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:33 AM CEST

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Bissi, Agnese
Fardelli, Giulia
Manenti, Andrea
SpringerLink (Online service)

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$BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words$

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

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$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

$On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory$

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$Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity$

Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity

$BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words$

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

$On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory$

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

$Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity$

Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity

$BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words$

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills$

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

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Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

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Other Objects (12)

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

Quarter-BPS black holes in AdS4-NUT from N = 2 $$ \mathcalN}=2 $$ gauged supergravity

BPS operators in N = 4 $$ \mathcalN}=4 $$ SO(N) super Yang-Mills theory: plethysms, dominoes and words

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

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