Onset of the jet quenching phenomenon

The aim of this study is to set a baseline for the jet quenching measurements of the Quark Gluon Plasma formed in the large system size Nucleus-Nucleus (A-A) at top central collisions, via studying simulated small system size, Nucleon-Nucleon (N-N) collisions. The proton-proton (p-p) collisions were simulated using PYTHIA, at center of mass energies
$$\sqrt {{s_{NN}}} = 200 {\rm{GeV}}$$
and
$$\sqrt {{s_{NN}}} = 13 {\rm{TeV}}$$
corresponding to the available energies at the current collider experiments; the Relativistic Heavy Ion Collider, and the Large Hadron Collider. At both energies, the two-particle azimuthal correlation functions have been considered, and the yield associated with the high transverse momentum (pT) particles were extracted at its near-side (Δϕ ≈ 0) and away-side (Δϕ ≈ π) at mid pseudo rapidity (|η| ≤ 2). The ratio between the near-side yields in the high multiplicity events to these of the low multiplicity events (I), as well as, the ratio of the away-side yields (I) were calculated at both energies as a function of the hadron fractional energy zT of the high-pT particle. At both energies, the values of I and I were less than unity, and of trivial dependence on zT. The values of I are always less than these of I at the same multiplicity and energy, and both quantities show a pattern of systematic decreases with the multiplicity. Such multiplicity dependence cannot be used neither to exclude the jet quenching nor to prove it in the high multiplicity events in p-p collisions, as the suppressions have been found at both sides, near and away of the high-pT particle.