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  4. Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au+Au, Cu+Cu, d+Au, and p+p collisions at ultrarelativistic energies

Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au+Au, Cu+Cu, d+Au, and p+p collisions at ultrarelativistic energies

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Author(s)
Alver, Burak Han
•
Ballintijn, Maarten
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Busza, Wit
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Gulbrandsen, K.
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Henderson, C.
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Kane, J. L.
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Katzy, J.
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Kulinich, Piotr
•
Pernegger, H.
•
Reed, C.
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Date Issued
February 2011
Journal
Physical review C
Publisher
American Physical Society
Citation
Alver, B. et al. “Charged-particle multiplicity and pseudorapidity distributions measured with the PHOBOS detector in Au+Au, Cu+Cu, d+Au, and p+p collisions at ultrarelativistic energies.” Physical Review C 83.2 (2011) : n. pag. ©2011 American Physical Society
Version
Final published version
Abstract
Pseudorapidity distributions of charged particles emitted in Au+Au, Cu+Cu, d+Au, and p+p collisions over a wide energy range have been measured using the PHOBOS detector at the BNL Relativistic Heavy-Ion Collider (RHIC). The centrality dependence of both the charged particle distributions and the multiplicity at midrapidity were measured. Pseudorapidity distributions of charged particles emitted with |η|<5.4 [|eta|<5.4], which account for between 95% and 99% of the total charged-particle emission associated with collision participants, are presented for different collision centralities. Both the midrapidity density dNch/dη [dN subscript ch / d eta] and the total charged-particle multiplicity Nch [N subscript ch] are found to factorize into a product of independent functions of collision energy, √sNN [square root of s subscript N N prime], and centrality given in terms of the number of nucleons participating in the collision, Npart [N subscript part]. The total charged particle multiplicity, observed in these experiments and those at lower energies, assumes a linear dependence of (lnsNN)2 [(1n s subscript NN) superscript 2] over the full range of collision energy of √sNN=2.7–200 [square root of S subscript NN + 2.7-200] GeV.
MIT Department
Bates Linear Accelerator Center
Massachusetts Institute of Technology. Department of Physics
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Terms of Use
Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.
Persistent DSpace Link
http://hdl.handle.net/1721.1/63166
DOI of Published Version
https://doi.org/10.1103/PhysRevC.83.024913
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