Momentum Broadening in Weakly Coupled Quark-Gluon Plasma (with a view to finding the quasiparticles within liquid quark-gluon plasma)
Francesco D'Eramo, Mindaugas Lekaveckas, Hong Liu, Krishna Rajagopal

TL;DR
This paper calculates the transverse momentum distribution of energetic partons in weakly coupled quark-gluon plasma, comparing it to strongly coupled models, and suggests experimental ways to identify quasiparticles within the plasma.
Contribution
It provides a detailed calculation of P(k_ot) in weakly coupled quark-gluon plasma using HTL resummation and compares it to holographic models, highlighting potential experimental signatures of quasiparticles.
Findings
P(k_ot) shape is similar at modest k_ot in weakly and strongly coupled plasmas.
P(k_ot) is parametrically larger at high k_ot in weakly coupled plasma.
Large-angle deflections can reveal quasiparticles within the quark-gluon plasma.
Abstract
We calculate P(k_\perp), the probability distribution for an energetic parton that propagates for a distance L through a medium without radiating to pick up transverse momentum k_\perp, for a medium consisting of weakly coupled quark-gluon plasma. We use full or HTL self-energies in appropriate regimes, resumming each in order to find the leading large-L behavior. The jet quenching parameter \hat q is the second moment of P(k_\perp), and we compare our results to other determinations of this quantity in the literature, although we emphasize the importance of looking at P(k_\perp) in its entirety. We compare our results for P(k_\perp) in weakly coupled quark-gluon plasma to expectations from holographic calculations that assume a plasma that is strongly coupled at all length scales. We find that the shape of P(k_\perp) at modest k_\perp may not be very different in weakly coupled and…
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