Abstract

We report measurements of the primary charged particle pseudorapidity density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV, and investigate their correlation with experimental observables sensitive to the centrality of the collision. Centrality classes are defined using different event activity estimators, i.e. charged particle multiplicities measured in three disjunct pseudorapidity regions as well as the energy measured at beam rapidity (zero-degree). The procedures to determine the centrality, quantified by the number of participants ($N_{\rm part}$), or the number of nucleon-nucleon binary collisions ($N_{\rm coll}$), are described. We show that, in contrast to Pb-Pb collisions, in p-Pb collisions large multiplicity fluctuations together with the small range of participants available, generate a dynamical bias in centrality classes based on particle multiplicity. We propose to use the zero-degree energy, which we expect not to introduce a dynamical bias, as an alternative event-centrality estimator. Based on zero-degree energy centrality classes, the $N_{\rm part}$ dependence of particle production is studied. Under the assumption that the multiplicity measured in the Pb-going rapidity region scales with the number of Pb-participants, an approximate independence of the multiplicity per participating nucleon measured at mid-rapitity of the number of participating nucleons is observed. Furthermore, at high-$p_{\rm T}$ the p-Pb spectra are found to be consistent with the pp spectra scaled by $N_{\rm coll}$ for all centrality classes. Our results represent valuable input for the study of the event activity dependence of hard probes in p-Pb collision and, hence, help to establish baselines for the interpretation of the Pb-Pb data.

Highlights

  • Proton-lead collisions are an essential component of the heavy ion program at the Large Hadron Collider (LHC) [1]

  • We measure the nuclear modification factor, which is defined as the ratio of particle or jet transverse-momentum spectra in minimum-bias (MB) p-Pb to those in pp collisions scaled by the average number of binary p-nucleon (p-N) collisions nucleon binary collisions (Ncoll) [2]

  • For each V0A ring 1 distribution selected by a ZNA centrality class, we find the Ncoll distribution that, convolved with the NBDMB, fits the data, i.e., the parameters of the fit are the relative contributions of each Ncoll bin

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Summary

INTRODUCTION

Proton-lead collisions are an essential component of the heavy ion program at the Large Hadron Collider (LHC) [1]. Of particular interest are studies of nuclear effects on parton scatterings at large momentum transfer (hard processes) To this end, we measure the nuclear modification factor, which is defined as the ratio of particle or jet transverse-momentum (pT) spectra in minimum-bias (MB) p-Pb to those in pp collisions scaled by the average number of binary p-nucleon (p-N) collisions Ncoll [2]. The use of Ncoll from the Glauber model to scale cross sections of hard processes from pp to p-A has to undergo the same scrutiny as the correlation of the centrality estimator to the collision geometry This is necessary due to the enhanced role of multiplicity fluctuations in p-A.

EXPERIMENTAL CONDITIONS
Negative binomial distribution Glauber fit
Glauber–Gribov corrections
CENTRALITY FROM ZERO-DEGREE ENERGY
Multiplicity bias
Jet-veto bias
Geometric bias
Basis and assumptions of the method
V0C ring 1
Calculation of Ncoll
Charged-particle density
Nuclear modification factors
VIII. SUMMARY
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