Shining a gluon beam through quark-gluon plasma

We compute the energy density radiated by a quark undergoing circular motion in strongly coupled N=4 supersymmetric Yang-Mills plasma. If it were in vacuum, this quark would radiate a beam of strongly coupled radiation whose angular distribution has been characterized and is very similar to that of...

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Bibliographic Details
Main Authors: Chesler, Paul Michael (Contributor), Ho, Ying-Yu (Contributor), Rajagopal, Krishna (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2012-08-15T13:22:57Z.
Subjects:
Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Chesler, Paul Michael  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Rajagopal, Krishna  |e contributor 
100 1 0 |a Chesler, Paul Michael  |e contributor 
100 1 0 |a Ho, Ying-Yu  |e contributor 
100 1 0 |a Rajagopal, Krishna  |e contributor 
700 1 0 |a Ho, Ying-Yu  |e author 
700 1 0 |a Rajagopal, Krishna  |e author 
245 0 0 |a Shining a gluon beam through quark-gluon plasma 
260 |b American Physical Society,   |c 2012-08-15T13:22:57Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/72136 
520 |a We compute the energy density radiated by a quark undergoing circular motion in strongly coupled N=4 supersymmetric Yang-Mills plasma. If it were in vacuum, this quark would radiate a beam of strongly coupled radiation whose angular distribution has been characterized and is very similar to that of synchrotron radiation produced by an electron in circular motion in electrodynamics. Here, we watch this beam of gluons getting quenched by the strongly coupled plasma. We find that a beam of gluons of momenta ∼q≫πT is attenuated rapidly, over a distance ∼q[superscript 1/3](πT)[superscript -4/3] in a plasma with temperature T. As the beam propagates through the plasma at the speed of light, it sheds trailing sound waves with momenta ≲πT. Presumably these sound waves would thermalize in the plasma if they were not hit soon after their production by the next pulse of gluons from the lighthouselike rotating quark. At larger and larger q, the trailing sound wave becomes less and less prominent. The outward-going beam of gluon radiation itself shows no tendency to spread in angle or to shift toward larger wavelengths, even as it is completely attenuated. In this regard, the behavior of the beam of gluons which we analyze is reminiscent of the behavior of jets produced in heavy ion collisions at the LHC which lose a significant fraction of their energy without appreciable change in their angular distribution or their momentum distribution as they plow through the strongly coupled quark-gluon plasma produced in these collisions. 
520 |a United States. Dept. of Energy. Office of Nuclear Physics (grant no. DE-FG02-94ER40818) 
520 |a Massachusetts Institute of Technology. Dept. of Physics (Pappalardo Program) 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review D