Abstract

Mid-rapidity production of $\pi^{\pm}$, $\rm{K}^{\pm}$ and ($\bar{\rm{p}}$)p measured by the ALICE experiment at the LHC, in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, is presented. The invariant yields are measured over a wide transverse momentum ($p_{\rm{T}}$) range from hundreds of MeV/$c$ up to 20 GeV/$c$. The results in Pb-Pb collisions are presented as a function of the collision centrality, in the range 0$-$90%. The comparison of the $p_{\rm{T}}$-integrated particle ratios, i.e. proton-to-pion (p/$\pi$) and kaon-to-pion (K/$\pi$) ratios, with similar measurements in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV show no significant energy dependence. Blast-wave fits of the $p_{\rm{T}}$ spectra indicate that in the most central collisions radial flow is slightly larger at 5.02 TeV with respect to 2.76 TeV. Particle ratios (p/$\pi$, K/$\pi$) as a function of $p_{\rm{T}}$ show pronounced maxima at $p_{\rm{T}}$ $\approx$ 3 GeV/$c$ in central Pb-Pb collisions. At high $p_{\rm{T}}$, particle ratios at 5.02 TeV are similar to those measured in pp collisions at the same energy and in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. Using the pp reference spectra measured at the same collision energy of 5.02 TeV, the nuclear modification factors for the different particle species are derived. Within uncertainties, the nuclear modification factor is particle species independent for high $p_{\rm{T}}$ and compatible with measurements at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. The results are compared to state-of-the-art model calculations, which are found to describe the observed trends satisfactorily.

Highlights

  • Previous observations at the Relativistic Heavy-Ion Collider (RHIC) and at the CERN Large Hadron Collider (LHC) demonstrated that in high-energy heavy-ion (A-A) collisions, a strongly interacting quark-gluon plasma [1,2,3,4,5] is formed

  • Ordering by pT, from lowest to highest, the results are obtained using the dE /dx measured in the inner tracking system (ITS) and the time projection chamber (TPC) [61], the time of flight measured in the time-offlight (TOF) detector [62], the Cherenkov angle measured in the high-momentum particle identification detector (HMPID) [63] and the TPC dE /dx in the relativistic rise region of the Bethe-Bloch curve

  • To obtain the pT distributions of primary π ±, K±, and (p)p, the raw spectra are corrected for PID efficiency, misidentification probability, acceptance, and tracking efficiencies, following the procedures described in Ref. [14] for the ITS, TPC and TOF, in Ref. [28] for the high momentum particle identification (HMPID) and TPC and in Ref. [59] for the kink analysis

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Summary

INTRODUCTION

Previous observations at the Relativistic Heavy-Ion Collider (RHIC) and at the CERN Large Hadron Collider (LHC) demonstrated that in high-energy heavy-ion (A-A) collisions, a strongly interacting quark-gluon plasma (sQGP) [1,2,3,4,5] is formed. The observation of a qualitatively similar enhancement of the kaon-to-pion [(K+ + K−)/(π + + π −) ≡ K/π ] ratio in central Pb-Pb collisions with respect to inelastic pp collisions [28,35] supports an interpretation based on the collective radial expansion of the system that affects heavier particles more. For high pT (pT >10 GeV/c), measurements of the production of identified particles in Pb-Pb collisions relative to inelastic pp collisions contribute to the study of hard probes propagating through the medium. This offers the possibility to determine the properties of the QGP like the transport coefficient q [36] and the space-time profile of the bulk medium in terms of local temperature and fluid velocity [37].

DATA ANALYSIS
Particle identification strategy
Correction of raw spectra
Systematic uncertainties
RESULTS AND DISCUSSION
Particle production at low transverse momentum
Intermediate transverse momentum of Figure pT for
Particle production at high transverse momentum
COMPARISON TO MODELS
CONCLUSIONS
Methods
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