Differential branching fraction and angular analysis of \(\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-\) decays
The differential branching fraction of the rare decay \(\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-\) is measured as a function of \(q^{2}\), the square of the dimuon invariant mass. The analysis is performed using proton-proton collision data, corresponding to an integrated luminosity of \(3.0 \...
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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
29.05.2015
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Subjects | |
Online Access | Get full text |
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Summary: | The differential branching fraction of the rare decay \(\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-\) is measured as a function of \(q^{2}\), the square of the dimuon invariant mass. The analysis is performed using proton-proton collision data, corresponding to an integrated luminosity of \(3.0 \mbox{ fb}^{-1}\), collected by the LHCb experiment. Evidence of signal is observed in the \(q^2\) region below the square of the \(J/\psi\) mass. Integrating over \(15 < q^{2} < 20 \mbox{ GeV}^2/c^4\) the branching fraction is measured as \(d\mathcal{B}(\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-)/dq^2 = (1.18 ^{+ 0.09} _{-0.08} \pm 0.03 \pm 0.27) \times 10^{-7} ( \mbox{GeV}^{2}/c^{4})^{-1}\), where the uncertainties are statistical, systematic and due to the normalisation mode, \(\Lambda^{0}_{b} \rightarrow J/\psi \Lambda\), respectively. In the \(q^2\) intervals where the signal is observed, angular distributions are studied and the forward-backward asymmetries in the dimuon (\(A^{l}_{\rm FB}\)) and hadron (\(A^{h}_{\rm FB}\)) systems are measured for the first time. In the range \(15 < q^2 < 20 \mbox{ GeV}^2/c^4\) they are found to be \(A^{l}_{\rm FB} = -0.05 \pm 0.09 \mbox{ (stat)} \pm 0.03 \mbox{ (syst)}\) and \(A^{h}_{\rm FB} = -0.29 \pm 0.07 \mbox{ (stat)} \pm 0.03 \mbox{ (syst)}\). |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1503.07138 |