Abstract

Recent results from lead–lead and proton–lead collisions, measured by the ATLAS experiment at the LHC, are presented. In lead–lead collisions, electroweak bosons are found to be produced proportionally to the number of binary nucleon–nucleon collisions, and to have rapidity distributions compatible with perturbative QCD calculations, suggesting no need for large nuclear PDF effects. Conversely, the large suppression of inclusive jets, the elliptic flow of hadrons at high p T and the direct measurements of jet v 2 support the need for a path-length-dependent energy loss in the hot, dense medium. Proton–lead measurements provide new insights into particle production in small, longitudinally asymmetric systems, but require further insights into the fluctuating nature of proton–proton collisions. The modification factors for charged hadrons show a non-trivial dependence on centrality and rapidity, with a “Cronin” peak appearing only in the most central events, and in the lead-going direction. Finally the measurements of inclusive jets in proton–lead show a striking scaling in the R CP suppression variable that is only a function of the jet momentum, while the suppression factor relative to PYTHIA jet cross sections shows an enhanced yield in peripheral events, and a suppressed yield in central events.

Highlights

  • Since 2010, the ATLAS detector has taken heavy ion data at the highest available energies at the Large Hadron Collider (LHC) at CERN

  • The goal has been to elucidate the properties of the hot, dense medium formed in the collisions of heavy ions

  • The lead-lead data have been used to study the collective expansion of the medium as a function of collision geometry in great detail, as well as to investigate the energy loss of jets, by means of their suppression in central events

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Summary

Introduction

Since 2010, the ATLAS detector has taken heavy ion data at the highest available energies at the Large Hadron Collider (LHC) at CERN. The lead-lead data have been used to study the collective expansion of the medium as a function of collision geometry in great detail, as well as to investigate the energy loss of jets, by means of their suppression in central events. While jets are expected to be modified in the hot, dense medium by a combination of elastic and radiative processes, electroweak bosons are not expected to interact with the medium They should be produced as in pp collisions, except effects related to isospin (the neutron fraction in the lead-lead system), and possibly modifications to the nuclear PDFs, e.g. as implemented in the EPS09 PDF set [3]. A similar study has been performed using W bosons in lead-lead collisions, measured in the single muon channel, but with jet background suppressed by requiring a large missing-ET based on charged tracks with pT > 3 GeV. More detailed studies of these quantities, especially with the higher energy and luminosity available in the LHC run, should enable a full investigation of the path-length dependence of jet quenching

What have we learned from proton-lead collisions
Findings
Conclusions
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