Mechanism behind p–Pb normalized multiplicity following INEL pp energy dependence
Ascertain the mechanism responsible for the observation that the normalized mean charged-particle multiplicity per participating nucleon pair, (2/⟨N_part⟩)⟨N_ch⟩, in non-single diffractive proton–lead collisions at 5.02 TeV aligns with the energy dependence observed in inelastic proton–proton collisions rather than central nucleus–nucleus collisions.
References
The similarity between the NSD \pPb and the INEL pp data is yet to be understood.
— Charged-particle multiplicity distributions over a wide pseudorapidity range in p-Pb collisions at $\mathbf{\sqrt{s}_{\rm NN} = 5.02}$ TeV
(2502.18081 - Collaboration, 25 Feb 2025) in Results and discussion, Subsection “System-size and energy dependence of ⟨N_ch⟩”