Hard pion and prompt photon at RHIC, from single to double inclusive production
Francois Arleo
TL;DR
The paper develops a unified perturbative QCD framework to study high-$p_\perp$ pion and prompt photon production at RHIC, combining NLO calculations in $p$-$p$ with shadowing and an energy-loss model to predict Au-Au quenching. By comparing to PHENIX data, it extracts a plausible medium transport scale $\omega_c$ and estimates a RHIC energy density $\epsilon_{RHIC}$ on the order of $10$–$15$ GeV/fm$^3$, with a corresponding temperature near $0.36$ GeV. The work demonstrates that photons are less quenched than pions due to the direct contribution, and it shows that photon-pion momentum correlations are especially sensitive to medium-modified fragmentation, offering a promising tool to probe fragmentation in nuclear collisions. It also provides projected counting rates for photon-pion correlations, highlighting the potential for future experimental studies to constrain the properties of the produced medium. Overall, the study connects hard probes with medium parameters and motivates further exploration of photon-tagged observables in heavy-ion collisions at RHIC.
Abstract
Single pion and prompt photon large transverse momentum spectra in p-p and Au-Au collisions are computed in perturbative QCD at RHIC energy, s^1/2 = 200 GeV. Next-to-leading order calculations are discussed and compared with p-p scattering data. Subsequently, quenching factors are computed to leading order for both pions and photons within the same energy loss model. The good agreement with PHENIX preliminary data allows for a lower estimate of the energy density reached in central Au-Au collisions, epsilon > 10 GeV/fm^3. Double inclusive photon-pion production in p-p and Au-Au collisions is then addressed. Next-to-leading order corrections prove rather small in p-p scattering. In Au-Au collisions, the quenching of momentum-correlation spectra is seen to be sensitive to parton energy loss processes, which would help to understand how the fragmentation dynamics is modified in nuclear collisions at RHIC.
