2002
DOI: 10.1556/aph.15.2002.3-4.6
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Results from the PHOBOS Experiment at RHIC

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Cited by 128 publications
(238 citation statements)
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“…The latter becomes large for high p ⊥ mo-menta such that the attenuation of 'secondaries' is rather low when employing high p ⊥ cuts. The system Au+Au at √ s = 62.4 GeV has recently been investigated experimentally at RHIC and first results on hadron attenuation have become available at moderate p ⊥ from the PHOBOS Collaboration [46]. We thus start with single hadron attenuation in the next subsection following exactly the studies in Ref.…”
Section: /3mentioning
confidence: 99%
See 1 more Smart Citation
“…The latter becomes large for high p ⊥ mo-menta such that the attenuation of 'secondaries' is rather low when employing high p ⊥ cuts. The system Au+Au at √ s = 62.4 GeV has recently been investigated experimentally at RHIC and first results on hadron attenuation have become available at moderate p ⊥ from the PHOBOS Collaboration [46]. We thus start with single hadron attenuation in the next subsection following exactly the studies in Ref.…”
Section: /3mentioning
confidence: 99%
“…In Section 5 we will show the results of calculations for Au+Au collisions at √ s = 62.4 GeV for different centrality classes since this system is presently under investigation experimentally. Apart from a comparison of the high p ⊥ attenuation of charged hadrons with the data from the PHOBOS collaboration [46] we will also present our predictions for the 'near-side' and 'far-side' angular correlations at this energy. Section 6 summarizes our present investigations.…”
Section: Introductionmentioning
confidence: 99%
“…In studying centrality dependence the focus was put on the calculations of < N part >, its definition and uncertainty. Both the PHENIX [2] and the PHOBOS [11] observations that the charged particle mid-pseudorapidity density per participant pair slightly increases with < N part > could be reproduced fairly well by JPCIAE. However, this study indicated that it is not suitable to use the charged particle mid-pseudorapidity density per participant pair as a function of < N part > to constrain theoretical models for particle production, because < N part > is not a well defined physical variable both experimentally and theoretically.…”
Section: Figmentioning
confidence: 99%
“…Figure 2 shows multiplicity distributions in negative rapidity region (−3.9 < η < −3.0) in p+Au, d+Au and 3 He+Au collisions at √ s NN = 200 GeV. Since we employed, for the initial conditions, [13,14]. To see the plots clearly, the result in 3 He+Au (p+Au) collisions is multiplied (divided) by ten in the right figure. PYTHIA in which multiplicities fluctuate in p+p collisions, multiplicity distributions in small colliding systems take over these fluctuations.…”
Section: Introductionmentioning
confidence: 99%