Reaction operator approach to non-abelian energy loss

Abstract

A systematic expansion of the induced inclusive gluon radiation associated with jet production in a dense QCD plasma is derived using a reaction operator formalism. Analytic expressions for the transverse momentum and light-cone momentum distributions are derived to all orders in powers of the gluon opacity of the medium, N σg/A = L/λg. The reaction operator approach also leads to a simple algebraic proof of the "color triviality" of single inclusive distributions and to a solvable set of recursion relations. The analytic solution generalizes previous continuum solutions (BDMPS) for applications to mesoscopic QCD plasmas. The solution is furthermore not restricted to uncorrelated geometries and allows for evolving screening scales as well as the inclusion of finite kinematic constraints. The later is particularly important because below LHC energies the kinematic constraints significantly decrease the non-abelian energy loss. Our solution for the inclusive distribution also generalizes the finite order exclusive (tagged) distribution case studied previously (GLV1). The form of the analytic solution is well suited for numerical implementation in Monte Carlo event generators to enable more accurate calculations of jet quenching in ultra-relativistic nuclear collisions. Numerical results illustrating the constributions of the first three orders in opacity are compared to the "self-quenching" hard radiation intensity. A surprising result is that the induced gluon radiation intensity is dominated by the (quadratic in L) first order opacity contribution for realistic geometries and jet energies in nuclear collisions.

Heavy quark radiative energy loss in QCD matter

“…The main goal of this paper is (1) to generalize the GLV opacity series [16] to include massive quark kinematic effects and (2) to take into account the Ter-Mikayelian plasmon effects for gluons as described in Ref. [33].…”

“…That asymptotic mass, m g = µ/ √ 2 is somewhat larger than the long wavelength plasmon mass µ/ √ 3, where µ ≈ gT GeV is chromoelectric Debye screening mass. We concentrate here as in [16] on the case of high p T eikonal jets produced inside a finite evolving QGP at some initial point (t 0 , z 0 , x 0 ). This is in contrast to the Gunion-Bertsch problem [35] with t 0 = −∞, where the jet is prepared as a beam in the remote past.…”

“…This is in contrast to the Gunion-Bertsch problem [35] with t 0 = −∞, where the jet is prepared as a beam in the remote past. We model the interactions in the QGP as in [16,17] via random color screened potentials…”

“…The color exchange bookkeeping with the target parton n is handled by an appropriate SU (N c ) generator [16], T a (n), in the d n dimensional representation of the target (Tr T a (n) = 0 and Tr (T a …”

“…The elastic cross section of target parton i with the jet is therefore proportional to the product of Casimirs, C R C 2 (T ). As in [16], the analytic results derived below with the reaction operator approach do not depend on the actual form of v, but the Yukawa form will be used for convenience in numerical estimates.…”