pQCD calculations predict jet quenching suppression scaling as R_AB ≈ (√(AB))^{1/3} in small ion collisions, with ^{3}He and ^{6}Li as clean QGP probes and energy loss models giving v_2 ≈ 0 in small systems.
Charged-hadron production in pp, p+Pb, Pb+Pb, and Xe+Xe collisions at √sNN =5 TeV with the ATLAS detector at the LHC
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First measurement of the nuclear modification factor R_AA in OO collisions at 5.36 TeV shows suppression with a minimum of 0.69 at p_T around 6 GeV, favoring models with parton energy loss.
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Jet Quenching in the Smallest Hadronic Collision Systems
pQCD calculations predict jet quenching suppression scaling as R_AB ≈ (√(AB))^{1/3} in small ion collisions, with ^{3}He and ^{6}Li as clean QGP probes and energy loss models giving v_2 ≈ 0 in small systems.
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Observation of suppressed charged-particle production in ultrarelativistic oxygen-oxygen collisions
First measurement of the nuclear modification factor R_AA in OO collisions at 5.36 TeV shows suppression with a minimum of 0.69 at p_T around 6 GeV, favoring models with parton energy loss.