B-meson production at forward and backward rapidity in \(p\)+\(p\) and Cu+Au collisions at \(\sqrt{s_{_{NN}}}\)=200 GeV
The fraction of \(J/\psi\) mesons which come from B-meson decay, \(\textrm{F}_{B{\rightarrow}J/\psi}\), is measured for J/\(\psi\) rapidity \mbox{\(1.2<|y|<2.2\)} and \(p_T>0\) in \(p\)+\(p\) and Cu+Au collisions at \(\sqrt{s_{_{NN}}}\)=200 GeV with the PHENIX detector. The extracted fracti...
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Published in | arXiv.org |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
12.11.2017
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Subjects | |
Online Access | Get full text |
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Summary: | The fraction of \(J/\psi\) mesons which come from B-meson decay, \(\textrm{F}_{B{\rightarrow}J/\psi}\), is measured for J/\(\psi\) rapidity \mbox{\(1.2<|y|<2.2\)} and \(p_T>0\) in \(p\)+\(p\) and Cu+Au collisions at \(\sqrt{s_{_{NN}}}\)=200 GeV with the PHENIX detector. The extracted fraction is \(\textrm{F}_{B{\rightarrow}J/\psi}\) = 0.025 \(\pm\) 0.006(stat) \(\pm\) 0.010(syst) for \(p\)+\(p\) collisions. For Cu+Au collisions, \(\textrm{F}_{B{\rightarrow}J/\psi}\) is 0.094 \(\pm\) 0.028(stat) \(\pm\) 0.037(syst) in the Au-going direction (\(-2.2<y<-1.2\)) and 0.089 \(\pm\) 0.026(stat) \(\pm\) 0.040(syst) in the Cu-going direction (\(1.2<y<2.2\)). The nuclear modification factor, \(R_{\rm CuAu}\), of B mesons in Cu+Au collisions is consistent with binary scaling of measured yields in \(p\)+\(p\) at both forward and backward rapidity. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1702.01085 |