2016
DOI: 10.1007/jhep03(2016)095
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Jet-medium interactions at NLO in a weakly-coupled quark-gluon plasma

Abstract: We present an extension to next-to-leading order in the strong coupling constant g of the AMY effective kinetic approach to the energy loss of high momentum particles in the quark-gluon plasma. At leading order, the transport of jet-like particles is determined by elastic scattering with the thermal constituents, and by inelastic collinear splittings induced by the medium. We reorganize this description into collinear splittings, highmomentum-transfer scatterings, drag and diffusion, and particle conversions (… Show more

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Cited by 86 publications
(161 citation statements)
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References 119 publications
(308 reference statements)
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“…In previous implementations, C [ f ] would be divided into an elastic and an inelastic term. In the leading order reformulation [3], the collision kernel is divided into (i) hard elastic and inelastic interactions, (ii) diffusion, and (iii) conversion processes.…”
Section: Description Of the Reformulated Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…In previous implementations, C [ f ] would be divided into an elastic and an inelastic term. In the leading order reformulation [3], the collision kernel is divided into (i) hard elastic and inelastic interactions, (ii) diffusion, and (iii) conversion processes.…”
Section: Description Of the Reformulated Modelmentioning
confidence: 99%
“…[3], it was shown that the parton energy loss can be equivalently reformulated in terms of hard large-angle interactions and soft small-angle collisions. A major advantage of this reformulated approach is that it could be extended to next-to-leading order [4,3]. There are nevertheless important benefits at leading order as well.…”
Section: Introductionmentioning
confidence: 99%
“…The basic premise behind the Fokker-Planck equation is that the number density of the hard particles (integrated over momenta p T of the phase space distribution) is conserved. However, in QCD there are processes already at leading order in α s , which violate the Fokker-Planck equation [77], e.g. a collinear splitting Q → Qg where both the quark and the gluon carry a large p T ("p T /2"), or a scattering of Q with a hard medium gluon whereby its momentum is changed by a large amount.…”
Section: High-p T Jetsmentioning
confidence: 99%
“…The value ofq L remains to be determined. The un-integrated C(k ⊥ ) may also parametrize a subset of non-Fokker Planck processes [77].…”
Section: High-p T Jetsmentioning
confidence: 99%
“…The large separation of scales, related in turn to the medium length and the mean free path, can also potentially lead to significant radiative corrections to transverse momentum broadening and energy loss in the medium [50][51][52] and, in general, to medium transport coefficients [51,53]. See also [54,55] for related work in next-to-leading order corrections to the medium-induced spectrum. The emission spectrum of two gluons with comparable formation times was analysed for the case of a dense medium in [56].…”
Section: Jhep11(2016)174mentioning
confidence: 99%