DATA FROM V. KHACHATRYAN AND COLLEAGUES ADVANCE KNOWLEDGE IN HIGH ENERGY PHYSICS
Physics Week
April 20, 2010
According to a study from Yerevan, Armenia, "Measurements of inclusive
charged-hadron transverse-momentum and pseudorapidity distributions
are presented for proton-proton collisions at root s = 0.9 and 2.36
TeV. The data were collected with the CMS detector during the LHC
commissioning in December 2009."
"For non-single-diffractive interactions, the average charged-hadron
transverse momentum is measured to be 0.46 +/- 0.01 (stat.) +/- 0.01
(syst.) GeV/c at 0.9 TeV and 0.50 +/- 0.01 (stat.) +/- 0.01 (syst.)
GeV/c at 2.36 TeV, for pseudorapidities between -2.4 and +2.4. At
these energies, the measured pseudorapidity densities in the central
region, dN(ch)/d eta vertical bar(vertical bar eta vertical bar
<0.5), are 3.48 +/- 0.02 (stat.) +/- 0.13 (syst.) and 4.47 +/- 0.04
(stat.) +/- 0.16 (syst.), respectively. The results at 0.9 TeV are
in agreement with previous measurements and confirm the expectation
of near equal hadron production in p<(p)over bar > and pp collisions,"
wrote V. Khachatryan and colleagues.
The researchers concluded: "The results at 2.36 TeV represent the
highest-energy measurements at a particle collider to date."
Khachatryan and colleagues published the results of their research
in the Journal of High Energy Physics (Transverse-momentum and
pseudorapidity distributions of charged hadrons in pp collisions at
root s=0.9 and 2.36 TeV. Journal of High Energy Physics, 2010;(2):41).
For additional information, contact V. Khachatryan, Yerevan Phys Inst,
Yerevan 375036, Armenia.
The publisher of the Journal of High Energy Physics can be contacted
at: Springer, 233 Spring St., New York, NY 10013, USA.
From: Emil Lazarian | Ararat NewsPress
Disclaimer: This article was contributed and translated into English by Emil Lazarian. While we strive for quality, the views and accuracy of the content remain the responsibility of the contributor. Please verify all facts independently before reposting or citing.
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