Heavy Quark Diffusion in Strongly Coupled $\N=4$ Yang Mills

dc.creatorCasalderrey-Solana, Jorge
dc.creatorTeaney, Derek
dc.date2006-05-17
dc.date2006-06-19
dc.date.accessioned2026-07-07T11:05:04Z
dc.date.available2026-07-07T11:05:04Z
dc.descriptionWe express the heavy quark diffusion coefficient as the temporal variation of a Wilson line along the Schwinger-Keldysh contour. This generalizes the classical formula for diffusion as a force-force correlator to a non-abelian theory. We use this formula to compute the diffusion coefficient in strongly coupled $\N=4$ Yang-Mills by studying the fluctuations of a string in $AdS_5\times S_5$. The string solution spans the full Kruskal plane and gives access to contour correlations. The diffusion coefficient is $D=2/\sqrtλ πT$ and is therefore parametrically smaller than momentum diffusion, $η/(e+p)=1/4πT$. The quark mass must be much greater than $T\sqrtλ$ in order to treat the quark as a heavy quasi-particle. The result is discussed in the context of the RHIC experiments.
dc.description17 pages + 2 figures
dc.identifierhttps://arxiv.org/abs/hep-ph/0605199
dc.identifierhttp://arxiv.org/abs/hep-ph/0605199
dc.identifierPhys.Rev.D74:085012,2006
dc.identifierdoi:10.1103/PhysRevD.74.085012
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/189100
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.subjectNuclear Theory
dc.titleHeavy Quark Diffusion in Strongly Coupled $\N=4$ Yang Mills
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