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Radiation by a heavy quark in N=4 SYM at strong coupling

Using the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills theory. We find that this energy is fully generated via backreaction from t...

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Autores principales: Hatta, Y., Iancu, E., Mueller, A.H., Triantafyllopoulos, D.N.
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2011.04.011
http://cds.cern.ch/record/1326249
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author Hatta, Y.
Iancu, E.
Mueller, A.H.
Triantafyllopoulos, D.N.
author_facet Hatta, Y.
Iancu, E.
Mueller, A.H.
Triantafyllopoulos, D.N.
author_sort Hatta, Y.
collection CERN
description Using the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills theory. We find that this energy is fully generated via backreaction from the near-boundary endpoint of the dual string attached to the heavy quark. Because of that, the energy distribution shows the same space-time localization as the classical radiation that would be produced by the heavy quark at weak coupling. We believe that this and some other unnatural features of our result (like its anisotropy and the presence of regions with negative energy density) are artifacts of the supergravity approximation, which will be corrected after including string fluctuations. For the case where the quark trajectory is bounded, we also compute the radiated power, by integrating the energy density over the surface of a sphere at infinity. For sufficiently large times, we find agreement with a previous calculation by Mikhailov [hep-th/0305196].
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institution Organización Europea para la Investigación Nuclear
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spelling cern-13262492023-03-14T19:13:58Zdoi:10.1016/j.nuclphysb.2011.04.011http://cds.cern.ch/record/1326249engHatta, Y.Iancu, E.Mueller, A.H.Triantafyllopoulos, D.N.Radiation by a heavy quark in N=4 SYM at strong couplingParticle Physics - TheoryUsing the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills theory. We find that this energy is fully generated via backreaction from the near-boundary endpoint of the dual string attached to the heavy quark. Because of that, the energy distribution shows the same space-time localization as the classical radiation that would be produced by the heavy quark at weak coupling. We believe that this and some other unnatural features of our result (like its anisotropy and the presence of regions with negative energy density) are artifacts of the supergravity approximation, which will be corrected after including string fluctuations. For the case where the quark trajectory is bounded, we also compute the radiated power, by integrating the energy density over the surface of a sphere at infinity. For sufficiently large times, we find agreement with a previous calculation by Mikhailov [hep-th/0305196].Using the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N = 4 supersymmetric Yang–Mills theory. We find that this energy is fully generated via backreaction from the near-boundary endpoint of the dual string attached to the heavy quark. Because of that, the energy distribution shows the same space–time localization as the classical radiation that would be produced by the heavy quark at weak coupling. We believe that this is an artifact of the supergravity approximation, which will be corrected after including string fluctuations. We discuss some other features of the result, like its anisotropy and the presence of regions with negative energy density. For the case where the quark trajectory is bounded, we also compute the radiated power, by integrating the energy density over the surface of a sphere at infinity. For sufficiently large times, we find agreement with a previous calculation by Mikhailov [ hep-th/0305196 ].Using the AdS/CFT correspondence in the supergravity approximation, we compute the energy density radiated by a heavy quark undergoing some arbitrary motion in the vacuum of the strongly coupled N=4 supersymmetric Yang-Mills theory. We find that this energy is fully generated via backreaction from the near-boundary endpoint of the dual string attached to the heavy quark. Because of that, the energy distribution shows the same space-time localization as the classical radiation that would be produced by the heavy quark at weak coupling. We believe that this and some other unnatural features of our result (like its anisotropy and the presence of regions with negative energy density) are artifacts of the supergravity approximation, which will be corrected after including string fluctuations. For the case where the quark trajectory is bounded, we also compute the radiated power, by integrating the energy density over the surface of a sphere at infinity. For sufficiently large times, we find agreement with a previous calculation by Mikhailov [hep-th/0305196].arXiv:1102.0232CERN-PH-TH-2011-021CERN-PH-TH-2011-021oai:cds.cern.ch:13262492011-02-02
spellingShingle Particle Physics - Theory
Hatta, Y.
Iancu, E.
Mueller, A.H.
Triantafyllopoulos, D.N.
Radiation by a heavy quark in N=4 SYM at strong coupling
title Radiation by a heavy quark in N=4 SYM at strong coupling
title_full Radiation by a heavy quark in N=4 SYM at strong coupling
title_fullStr Radiation by a heavy quark in N=4 SYM at strong coupling
title_full_unstemmed Radiation by a heavy quark in N=4 SYM at strong coupling
title_short Radiation by a heavy quark in N=4 SYM at strong coupling
title_sort radiation by a heavy quark in n=4 sym at strong coupling
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/j.nuclphysb.2011.04.011
http://cds.cern.ch/record/1326249
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