@article{0199e8a10b7244f596f275f3a40bd79d,
title = "Study of charmonium production in \$\{b\}\$-hadron decays and first evidence for the decay \$\{\{\{B\}\} \textasciicircum{}0\_\{\{s\}\}\} \textbackslash{}!\textbackslash{}rightarrow \textbackslash{}phi \textbackslash{}phi \textbackslash{}phi \$",
abstract = "Using decays to \$\textbackslash{}phi\$-meson pairs, the inclusive production of charmonium states in \$b\$-hadron decays is studied with \$pp\$ collision data corresponding to an integrated luminosity of \$3.0fb\textasciicircum{}\{-1\}\$, collected by the LHCb experiment at centre-of-mass energies of 7 and 8 TeV. Denoting by \$B\_C\textbackslash{}equiv B(b\textbackslash{}to CX)\textbackslash{}times B(C\textbackslash{}to\textbackslash{}phi\textbackslash{}phi)\$ the inclusive branching fraction of a \$b\$ hadron to a charmonium state \$C\$ that decays into a pair of \$\textbackslash{}phi\$ mesons, ratios \$R\textasciicircum{}\{C1\}\_\{C2\}\textbackslash{}equiv B\_\{C1\}/B\_\{C2\}\$ are determined as \$R\textasciicircum{}\{\textbackslash{}chi\_\{c0\}\}\_\{\textbackslash{}eta\_c(1S)\}=0.147\textbackslash{}pm0.023\textbackslash{}pm0.011\$, \$R\textasciicircum{}\{\textbackslash{}chi\_\{c1\}\}\_\{\textbackslash{}eta\_c (1S)\}=0.073\textbackslash{}pm0.016\textbackslash{}pm0.006\$, \$R\textasciicircum{}\{\textbackslash{}chi\_\{c2\}\}\_\{\textbackslash{}eta\_c (1S)\}=0.081\textbackslash{}pm0.013\textbackslash{}pm0.005\$, \$R\textasciicircum{}\{\textbackslash{}chi\_\{c1\}\}\_\{\textbackslash{}chi\_\{c0\}\}=0.50\textbackslash{}pm0.11\textbackslash{}pm0.01\$, \$R\textasciicircum{}\{\textbackslash{}chi\_\{c2\}\}\_\{\textbackslash{}chi\_\{c0\}\}=0.56\textbackslash{}pm0.10\textbackslash{}pm0.01\$ and \$R\textasciicircum{}\{\textbackslash{}eta\_c (2S)\}\_\{\textbackslash{}eta\_c(1S)\}=0.040\textbackslash{}pm0.011\textbackslash{}pm0.004\$. Here and below the first uncertainties are statistical and the second systematic. Upper limits at \$90\textbackslash{}\%\$ confidence level for the inclusive production of \$X(3872)\$, \$X(3915)\$ and \$\textbackslash{}chi\_\{c2\}(2P)\$ states are obtained as \$R\textasciicircum{}\{X(3872)\}\_\{\textbackslash{}chi\_\{c1\}\}",
author = "Clarke, \{P E L\} and Cowan, \{G A\} and S Eisenhardt and F Muheim and M Needham and S Playfer and LHCb Collaboration",
year = "2017",
month = sep,
day = "14",
doi = "10.1140/epjc/s10052-017-5151-8",
language = "English",
volume = "C77",
pages = "609",
journal = "The European Physical Journal C",
issn = "1434-6044",
publisher = "Springer Nature",
number = "9",
}