2011
DOI: 10.1103/physrevd.83.052004
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Measurement of neutral mesons inp+pcollisions ats=200GeVand scaling properties of hadron production

Abstract: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the invariant differential cross section for production of K 0 S , ω, η ′ , and φ mesons in p + p collisions at √ s = 200 GeV. Measurements of ω and φ production in different decay channels give consistent results. New results for the ω are in agreement with previously published data and extend the measured pT coverage. The spectral shapes of all hadron transverse momentum distributions measured by PHENIX are well described by a Tsallis … Show more

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Cited by 205 publications
(108 citation statements)
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“…Sibyll 2.1 generates particle p T using two approaches [20]. In soft (low p T ) interactions, quark-antiquark pairs are given a p T that follows a Gaussian distribution, with a mean of 0.3, 0.45, or 0:6 þ 0:08log 10 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi s=ð30 GeVÞ p GeV, for light quarks, strange quarks, and diquarks respectively; diquarks lead to the production of baryons. Hard interactions are simulated using lowest order pQCD, with the Glück-Reya-Vogt structure functions, including a saturation correction.…”
Section: B Zenith Angle Distributionmentioning
confidence: 99%
See 1 more Smart Citation
“…Sibyll 2.1 generates particle p T using two approaches [20]. In soft (low p T ) interactions, quark-antiquark pairs are given a p T that follows a Gaussian distribution, with a mean of 0.3, 0.45, or 0:6 þ 0:08log 10 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi s=ð30 GeVÞ p GeV, for light quarks, strange quarks, and diquarks respectively; diquarks lead to the production of baryons. Hard interactions are simulated using lowest order pQCD, with the Glück-Reya-Vogt structure functions, including a saturation correction.…”
Section: B Zenith Angle Distributionmentioning
confidence: 99%
“…At low p T the spectrum follows expðÀp T =TÞ, with T % 220 MeV=c for pions (somewhat higher for kaons and protons) [10]. At higher p T , the spectrum falls as 1=ð1 þ p T =p 0 Þ n , where one fit found n ¼ 13:0 þ1:0 À0:5 and p 0 ¼ 1:9 þ0:2 À0:1 GeV=c [11].…”
Section: Introductionmentioning
confidence: 99%
“…To calculate the contribution from the η meson and its uncertainties, we assume that the shapes of its spectra for all centrality bins as a function of transverse mass are the same as the pion spectra, using the transverse mass scaling [53], and that the η/π ratio is independent of the collision system, as observed by PHENIX [54]. We also consider a scenario where the η spectrum is assumed to have the same shape as the kaon spectrum, as would be expected if the shape of the η spectrum was determined by hydrodynamical flow.…”
Section: Correction Factors F Neutral and F Totalmentioning
confidence: 99%
“…In high-energy physics there is a plethora of applications as well ( [52][53][54][55][56][57][58][59][60][61][62][63][64][65] among many others). A remarkable recent example is shown in Fig.…”
Section: Applicationsmentioning
confidence: 99%