Abstract

In high-energy collisions, the spatio-temporal size of the particle production region can be measured using the Bose–Einstein correlations of identical bosons at low relative momentum. The source radii are typically extracted using two-pion correlations, and characterize the system at the last stage of interaction, called kinetic freeze-out. In low-multiplicity collisions, unlike in high-multiplicity collisions, two-pion correlations are substantially altered by background correlations, e.g. mini-jets. Such correlations can be suppressed using three-pion cumulant correlations. We present the first measurements of the size of the system at freeze-out extracted from three-pion cumulant correlations in pp, p–Pb and Pb–Pb collisions at the LHC with ALICE. At similar multiplicity, the invariant radii extracted in p–Pb collisions are found to be 5–15% larger than those in pp, while those in Pb–Pb are 35–55% larger than those in p–Pb. Our measurements disfavor models which incorporate substantially stronger collective expansion in p–Pb as compared to pp collisions at similar multiplicity.

Highlights

  • The role of initial and final-state effects in interpreting differences between Pb–Pb and pp collisions is expected to be clarified with p–Pb collis√ions Pb collisions at sNN [1]

  • For pp and p–Pb, owing to the larger background present for twopion correlations, we extend the fit range to q = 1.2 GeV/c for the upper variation

  • Compared to the radii from two-pion correlations, the radii from three-pion cumulant correlations are less susceptible to non-femtoscopic background correlations due to the increased quantum statistics (QS)

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Summary

Introduction

The role of initial and final-state effects in interpreting differences between Pb–Pb and pp collisions is expected to be clarified with p–Pb collis√ions Pb collisions at sNN [1]. A CGC initial state model (IP-Glasma), without a hydrodynamic phase, predicts similar freeze-out radii in p–Pb and pp collisions [17]. The extraction of freeze-out radii can be achieved using identical boson correlations at low relative momentum, which are dominated by quantum statistics (QS) and final-state Coulomb and strong interactions (FSIs). Both FSIs and QS correlations encode information about the femtoscopic space–time structure of the particle emitting source at kinetic freeze-out [18,19,20]. The calculation of FSI correlations allows for the isolation of QS correlations

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