Abstract

The charged particle production in proton-proton collisions is studied with the LHCb detector at a centre-of-mass energy of ${\sqrt{s} =7}$TeV in different intervals of pseudorapidity $\eta$. The charged particles are reconstructed close to the interaction region in the vertex detector, which provides high reconstruction efficiency in the $\eta$ ranges $-2.5<\eta<-2.0$ and $2.0<\eta<4.5$. The data were taken with a minimum bias trigger, only requiring one or more reconstructed tracks in the vertex detector. By selecting an event sample with at least one track with a transverse momentum greater than 1 GeV/c a hard QCD subsample is investigated. Several event generators are compared with the data; none are able to describe fully the multiplicity distributions or the charged particle density distribution as a function of $\eta$. In general, the models underestimate the charged particle production.

Highlights

  • Charged particle multiplicity is a basic observable that characterizes the hadronic final state

  • The multiplicity distribution is sensitive to the underlying QCD dynamics of the proton-proton collision

  • The distributions are compared to several Monte Carlo event generators

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Summary

Introduction

Charged particle multiplicity is a basic observable that characterizes the hadronic final state. Particles traversing from the interaction region to the downstream tracking stations experience an integrated bending-field of approximately 4 Tm. The VELO consists of silicon microstrip modules, providing a measure of the radial and azimuthal coordinates, r and φ, distributed in 23 stations arranged along the beam direction. Hard interaction events are defined by requiring at least one long track with pT > 1 GeV/c in the range 2.5 < η < 4.5 where the detector has high efficiency. The geometric acceptance is no longer independent of momentum and the distributions require an additional correction In this analysis primary charged particles are defined as all particles for which the sum of the ancestors’ mean lifetimes is shorter than 10 ps; according to this definition the decay products of beauty and charm are primary particles

Efficiency correction
Background contributions
Correction and unfolding procedure
Efficiency
Non-primary particles
Pile-up
Results
Summary
Full Text
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