Measurement of [psi](2S) meson production in pp collisions at √s = 7 TeV

The differential cross-section for the inclusive production of ψ(2S) mesons in pp collisions at $\sqrt{s}=7\ \mbox{TeV}$has been measured with the LHCb detector. The data sample corresponds to an integrated luminosity of 36 pb−1. The ψ(2S) mesons are reconstructed in the decay channels ψ(2S)→μ+μ− an...

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Hauptverfasser: Aaij, Roel (VerfasserIn) , Bachmann, Sebastian (VerfasserIn) , Bien, Alexander (VerfasserIn) , Dordei, Francesca (VerfasserIn) , Eisele, Franz (VerfasserIn) , Färber, Christian (VerfasserIn) , Hansmann-Menzemer, Stephanie (VerfasserIn) , Jäger, Andreas (VerfasserIn) , Kreplin, Katharina (VerfasserIn) , Krocker, Georg Alexander (VerfasserIn) , Linn, Christian (VerfasserIn) , Marks, Jörg (VerfasserIn) , Meißner, Marco (VerfasserIn) , Seyfert, Paul (VerfasserIn) , Tilburg, Jeroen van (VerfasserIn) , Uwer, Ulrich (VerfasserIn) , Wandernoth, Sebastian (VerfasserIn) , Wiedner, Dirk (VerfasserIn) , Zhelezov, Alexey (VerfasserIn)
Körperschaft: LHCb Collaboration (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 10 August 2012
In: The European physical journal. C, Particles and fields
Year: 2012, Jahrgang: 72, Heft: 8
ISSN:1434-6052
DOI:10.1140/epjc/s10052-012-2100-4
Online-Zugang:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1140/epjc/s10052-012-2100-4
Volltext
Verfasserangaben:The LHCb Collaboration*

MARC

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520 |a The differential cross-section for the inclusive production of ψ(2S) mesons in pp collisions at $\sqrt{s}=7\ \mbox{TeV}$has been measured with the LHCb detector. The data sample corresponds to an integrated luminosity of 36 pb−1. The ψ(2S) mesons are reconstructed in the decay channels ψ(2S)→μ+μ− and ψ(2S)→J/ψπ+π−, with the J/ψ meson decaying into two muons. Results are presented both for promptly produced ψ(2S) mesons and for those originating from b-hadron decays. In the kinematic range pT(ψ(2S))≤16 GeV/c and 2<y(ψ(2S))≤4.5 we measure where the last uncertainty on the prompt cross-section is due to the unknown ψ(2S) polarization. Recent QCD calculations are found to be in good agreement with our measurements. Combining the present result with the LHCb J/ψ measurements we determine the inclusive branching fraction where the last uncertainty is due to the $\mathcal{B}(b \rightarrow J/\psi X)$, $\mathcal{B}(J/\psi\rightarrow\mu^{+} \mu^{-})$and $\mathcal{B}(\psi(2S) \rightarrow e^{+} e^{-})$branching fraction uncertainties. 
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