The pseudorapidity density and multiplicity distribution of charged particles produced in proton–proton collisions at the LHC, at a centre-of-mass energy √s = 7 TeV, were measured in the central pseudorapidity region |η| < 1. Comparisons are made with previous measurements at √s = 0.9 TeV and 2.36 TeV. At √s = 7 TeV, for events with at least one charged particle in |η| < 1, we obtain dNch/dη = 6.01 ± 0.01(stat.) +0.20 −0.12(syst.). This corresponds to an increase of 57.6%±0.4%(stat.) +3.6 −1.8%(syst.) relative to collisions at 0.9 TeV, significantly higher than calculations from commonly used models. The multiplicity distribution at 7 TeV is described fairly well by the negative binomial distribution.
Charged-particle multiplicity measurement in proton–proton collisions at √s=7 TeV with ALICE at LHC
BARBERA, Roberto;
2010-01-01
Abstract
The pseudorapidity density and multiplicity distribution of charged particles produced in proton–proton collisions at the LHC, at a centre-of-mass energy √s = 7 TeV, were measured in the central pseudorapidity region |η| < 1. Comparisons are made with previous measurements at √s = 0.9 TeV and 2.36 TeV. At √s = 7 TeV, for events with at least one charged particle in |η| < 1, we obtain dNch/dη = 6.01 ± 0.01(stat.) +0.20 −0.12(syst.). This corresponds to an increase of 57.6%±0.4%(stat.) +3.6 −1.8%(syst.) relative to collisions at 0.9 TeV, significantly higher than calculations from commonly used models. The multiplicity distribution at 7 TeV is described fairly well by the negative binomial distribution.File | Dimensione | Formato | |
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