Abstract
The rare electromagnetic J/ψ → μ+μ−μ+μ− decay is observed with a significance greatly exceeding the discovery threshold, using proton-proton collision data collected by the LHCb experiment during 2016–2018 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 5.4 fb−1. The rate of this decay is measured relative to that of the J/ψ → μ+μ− mode. Using the QED model for the four-muon decay in the efficiency estimation, its branching fraction is determined to be
Β(J/ψ → μ+μ−μ+μ−) = (1.13±0.10±0.05±0.01) x 10-6,
where the uncertainties are statistical, systematic and due to the uncertainty on the branching fraction of the J/ψ → μ+μ− decay.
Β(J/ψ → μ+μ−μ+μ−) = (1.13±0.10±0.05±0.01) x 10-6,
where the uncertainties are statistical, systematic and due to the uncertainty on the branching fraction of the J/ψ → μ+μ− decay.
Original language | English |
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Article number | 62 |
Number of pages | 25 |
Journal | Journal of High Energy Physics |
Volume | 62 |
DOIs | |
Publication status | Published - 10 Dec 2024 |