Abstract

Measurements are reported for charged hadron and inclusive jet transverse momentum ( p T ) spectra in pp and PbPb collisions at a nucleon–nucleon center-of-mass energy of 2.76 TeV with the CMS detector. These measurements make use of the high-statistics jet-triggered data recorded in 2011, including the total available PbPb luminosity of 150 μ b − 1 . Charged particles are reconstructed using an iterative algorithm and spurious high- p T tracks are suppressed by requiring appropriate energy deposits in the calorimeter system. Jets are reconstructed with the anti- k T algorithm, using combined information from tracking and calorimetry. The charged particle p T distributions are measured in the pseudorapidity range of | η | < 1 , and p T up to 100 GeV/ c . The jet p T distributions are measured in the pseudorapidity range of | η | < 2 , and p T from 100 to 300 GeV/ c . The nuclear modification factors, R AA , for charged hadrons and jets are presented as a function of p T and collision centrality. In the range p T = 5 – 10 GeV / c the charged hadron production in PbPb collisions is suppressed by up to a factor of seven, compared to the pp yield scaled by the number of incoherent nucleon–nucleon collisions. The charged hadron R AA increases at higher p T and approaches a value of approximately 0.5 in the range p T = 40 – 100 GeV / c for the most central collisions.

Highlights

  • The densityCMS detector is used in collisions of PbPb to at s√tudy sNN the production of charged particles and jets at high energy = 2.76 TeV recorded at the LHC in 2010√and 2011

  • The underlying PbPb background is removed with the iterative “noise/pedestal subtraction” technique, and pp jets are evaluated without the background removal

  • Jet reconstruction performance is evaluated in the analysis of Monte Carlo (MC) simulations of dijets embedded into minimum bias PbPb

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Summary

Introduction

CMS detector is used in collisions of PbPb to at s√tudy sNN the production of charged particles and jets at high energy = 2.76 TeV recorded at the LHC in 2010√and 2011. Ncoll is the average number of nucleon-nucleon collisions in heavy-ion (AA) interactions and TAA is the nuclear overlap function. The CMS detector is described elsewhere [1] This analysis uses the standard CMS Minimum Bias trigger and heavy-ion event selection [2]. For the charged particle analysis, the statistical reach of track pT is extended with jet-triggered data from 2011, with two jet triggered thresholds of 65 and 80 GeV. Jet analysis is performed on events with jets triggered at a threshold of 80 GeV

Charged particle RAA
Jet RAA
Summary
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