Collisional jet quenching becomes probable

dc.creatorPeshier, A.
dc.date2006-07-27
dc.date.accessioned2026-07-07T11:05:20Z
dc.date.available2026-07-07T11:05:20Z
dc.descriptionIt was argued recently that loop corrections to tree-level amplitudes are essential in the discussion of the collisional energy loss of energetic partons in the hot quark gluon plasma: Instead of $dE_{\rm coll}^B/dx \sim α^2 T^2 \ln(ET/m_D^2)$, as first derived by Bjorken (assuming a constant $α$), the mean energy loss actually behaves as $dE_{\rm coll}/dx \sim α(m_D^2)T^2$. Here we calculate, within this resummation-improved framework, the probability distribution functions (`quenching weights') of the collisional energy loss. First results from a Monte Carlo implementation of this probabilistic collisional quenching shed new light on the interpretation of jet suppression in heavy ion collisions.
dc.description5 figures
dc.identifierhttps://arxiv.org/abs/hep-ph/0607299
dc.identifierhttp://arxiv.org/abs/hep-ph/0607299
dc.identifierPhys.Rev.C75:034906,2007
dc.identifierdoi:10.1103/PhysRevC.75.034906
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/189172
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectNuclear Theory
dc.titleCollisional jet quenching becomes probable
dc.typetext

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