Revisiting scaling properties of medium-induced gluon radiation

TL;DR

This paper explores the complex nature of medium-induced gluon radiation in high-energy processes, emphasizing the importance of a broader radiation concept over simple energy loss, with implications for understanding particle suppression in nuclear collisions.

Contribution

It introduces a generalized framework for medium-induced gluon radiation that accounts for interference effects, challenging the traditional energy loss perspective in high-energy nuclear physics.

Findings

Medium-induced radiated energy scales with incoming parton energy.

Interference effects alter the interpretation of gluon radiation.

Implications for quarkonium suppression in p-A collisions.

Abstract

Discussing the general case of a hard partonic production process, we show that the notion of parton energy loss is not always sufficient to fully address medium-induced gluon radiation. The broader notion of gluon radiation associated to a hard process has to be used, in particular when initial and final state radiation amplitudes interfere, making the medium-induced radiated energy different from the energy loss of any well-identified parton. Our arguments are first presented in an abelian QED model, and then applied to large-xF quarkonium hadroproduction. In this case, we show that the medium-induced radiated energy is qualitatively similar (but not identical) to the radiative energy loss of an "asymptotic massive parton" undergoing transverse momentum broadening when travelling through the nucleus. In particular, it scales as the incoming parton energy, which suggests to reconsider gluon radiation as a possible explanation of large-xF quarkonium suppression in p-A collisions. We expect a similar effect in open heavy-flavour and possibly light-hadron hadroproduction at large xF, depending on the precise definition of the nuclear suppression factor in the latter case.