Abstract

The PHENIX collaboration has measured high-$p_T$ dihadron correlations in $p$$+$$p$, $p$$+$Al, and $p$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. The correlations arise from inter- and intra-jet correlations and thus have sensitivity to nonperturbative effects in both the initial and final states. The distributions of $p_{\rm out}$, the transverse momentum component of the associated hadron perpendicular to the trigger hadron, are sensitive to initial and final state transverse momenta. These distributions are measured multi-differentially as a function of $x_E$, the longitudinal momentum fraction of the associated hadron with respect to the trigger hadron. The near-side $p_{\rm out}$ widths, sensitive to fragmentation transverse momentum, show no significant broadening between $p$$+$Au, $p$$+$Al, and $p$$+$$p$. The away-side nonperturbative $p_{\rm out}$ widths are found to be broadened in $p$$+$Au when compared to $p$$+$$p$; however, there is no significant broadening in $p$$+$Al compared to $p$$+$$p$ collisions. The data also suggest that the away-side $p_{\rm out}$ broadening is a function of $N_{\rm coll}$, the number of binary nucleon-nucleon collisions, in the interaction. The potential implications of these results with regard to initial and final state transverse momentum broadening and energy loss of partons in a nucleus, among other nuclear effects, are discussed.

Highlights

  • High energy collisions of protons with nuclei provide a testing ground for quantum chromodynamics (QCD)

  • Nuclear parton distribution functions (PDFs) are known to have several regions where they deviate from simple superpositions of nucleon PDFs as a function of the longitudinal momentum fraction x that the parton carries of the nucleon

  • In p + A collisions, the centrality class is determined with the forward beam-beam counters (BBCs) [29], where the centrality percentiles are defined by the multiplicity measured in the nucleus-going BBC following the procedure in Ref. [30]

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Summary

Introduction

High energy collisions of protons with nuclei provide a testing ground for quantum chromodynamics (QCD). Proton-nucleus (p + A) collisions have traditionally been used as a control to identify final-state nuclear effects in high energy nucleusnucleus collisions where a strongly interacting quark-gluon plasma (QGP) is formed [1]. Semi-inclusive deep-inelastic scattering (SIDIS) experiments have shown that high z hadrons are suppressed in electron-nucleus relative to electron-deuterium collisions [6], where z is the longitudinal momentum fraction of the outgoing hadron with respect to the fragmenting parton. This suppression was found to be dependent on the nuclear target size [7]. A particle species dependence was observed, which may reflect differences in the nuclear modification of quark and/or antiquark fragmentation functions and possible differences in meson versus baryon production from nuclei [6,7]

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