Description of η-distributions at RHIC energies in terms of a stochastic model

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dc.creatorBiyajima, Minoru
dc.creatorIde, Masaru
dc.creatorKaneyama, Masahiro
dc.creatorMizoguchi, Takuya
dc.creatorSuzuki, Naomichi
dc.date2003-09-27
dc.date2003-12-02
dc.date.accessioned2026-07-07T10:50:56Z
dc.date.available2026-07-07T10:50:56Z
dc.descriptionTo explain η-distributions at RHIC energies we consider the Ornstein-Uhlenbeck process. To account for hadrons produced in the central region, we assume existence of third source located there (y \approx 0) in addition to two sources located at the beam and target rapidities (\pm y_{max} = \pm \ln[\sqrt{s_{NN}}/m_{N}]). This results in better χ^2/n.d.f. than those for only two sources when analysing data.
dc.description4 pages, 4 figures, PTPTEX
dc.identifierhttps://arxiv.org/abs/nucl-th/0309075
dc.identifierhttp://arxiv.org/abs/nucl-th/0309075
dc.identifierProg.Theor.Phys.Suppl.153:344-348,2004
dc.identifierdoi:10.1143/PTPS.153.344
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/184695
dc.subjectNuclear Theory
dc.titleDescription of η-distributions at RHIC energies in terms of a stochastic model
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