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CMS-BPH-24-001 ; CERN-EP-2026-023
Observation of the rare decay $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $
Submitted to Physical Review Letters
Abstract: A first observation of the rare decay $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ is reported by the CMS Collaboration at the CERN LHC. The result is based on a proton-proton collision data sample at $ \sqrt{s} = $ 13.6 TeV corresponding to an integrated luminosity of 38.0 fb$ ^{-1} $, acquired in 2022 using a high-rate dimuon trigger. Using the $ \eta\to\mu^{+}\mu^{-}\gamma $ decay channel for normalization, the branching fraction is measured to be $ \mathcal{B}(\eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^-) = ( $ 2.4 $ \pm $ 0.8 $)\times 10^{-6} $, with the uncertainty including statistical and systematic sources as well as the $ \mathcal{B}(\eta\to\mu^{+}\mu^{-}\gamma) $ uncertainty. This result is close to two orders of magnitude smaller than the existing limit, and is consistent with recent theoretical predictions.
Figures Summary References CMS Publications
Figures

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Figure 1:
Leading order standard model Feynman diagram for the decay $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $.

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Figure 2:
Summary of expected background contributions to the yield measured in the signal channel based on a simplified MC simulation. The signal channel is shown in red squares, and is closely mimicked by the $ \eta\to\mu^{+}\mu^{-}\gamma $ channel, shown in blue stars. Uncertainties are not shown. The equivalent luminosity for the simulation is 38.0 fb$ ^{-1} $.

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Figure 3:
Fit of the four-lepton invariant mass spectra in data for the signal (upper) and reference (lower) channels. Black points denote the data, the dashed grey curve is the combinatorial background fit to a threshold function, the cyan dashed curve is the $ \eta\to\mu^{+}\mu^{-}\gamma $ component of the fit, the red dot-dashed curve (signal channel only) is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ component of the fit, and the solid blue-violet curve is the overall fit including signal and background contributions. The orange distribution is the signal MC simulation (normalized to the BF prediction of 2.4 $ \times10^{-6} $ by Ref. [11]), and the magenta distribution is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ resonant background MC simulation (normalized to the world average BF measurement of 3.1 $ \times 10^{-4} $ [1]), both also normalized using the approximate cross section derived from the $ \eta\to\mu^{+}\mu^{-} $ channel. Points in the lower panel are pulls relative to the full fit model, (data-fit)/$ \sqrt{\smash[b]{\sigma_{\textrm{data}}^2 - \sigma_{\textrm{fit}}^2}} $.

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Figure 3-a:
Fit of the four-lepton invariant mass spectra in data for the signal (upper) and reference (lower) channels. Black points denote the data, the dashed grey curve is the combinatorial background fit to a threshold function, the cyan dashed curve is the $ \eta\to\mu^{+}\mu^{-}\gamma $ component of the fit, the red dot-dashed curve (signal channel only) is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ component of the fit, and the solid blue-violet curve is the overall fit including signal and background contributions. The orange distribution is the signal MC simulation (normalized to the BF prediction of 2.4 $ \times10^{-6} $ by Ref. [11]), and the magenta distribution is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ resonant background MC simulation (normalized to the world average BF measurement of 3.1 $ \times 10^{-4} $ [1]), both also normalized using the approximate cross section derived from the $ \eta\to\mu^{+}\mu^{-} $ channel. Points in the lower panel are pulls relative to the full fit model, (data-fit)/$ \sqrt{\smash[b]{\sigma_{\textrm{data}}^2 - \sigma_{\textrm{fit}}^2}} $.

png pdf
Figure 3-b:
Fit of the four-lepton invariant mass spectra in data for the signal (upper) and reference (lower) channels. Black points denote the data, the dashed grey curve is the combinatorial background fit to a threshold function, the cyan dashed curve is the $ \eta\to\mu^{+}\mu^{-}\gamma $ component of the fit, the red dot-dashed curve (signal channel only) is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ component of the fit, and the solid blue-violet curve is the overall fit including signal and background contributions. The orange distribution is the signal MC simulation (normalized to the BF prediction of 2.4 $ \times10^{-6} $ by Ref. [11]), and the magenta distribution is the $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ resonant background MC simulation (normalized to the world average BF measurement of 3.1 $ \times 10^{-4} $ [1]), both also normalized using the approximate cross section derived from the $ \eta\to\mu^{+}\mu^{-} $ channel. Points in the lower panel are pulls relative to the full fit model, (data-fit)/$ \sqrt{\smash[b]{\sigma_{\textrm{data}}^2 - \sigma_{\textrm{fit}}^2}} $.
Summary
In summary, the decay $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ has been observed for the first time, with a significance much larger than 5 standard deviations, with data collected by the CMS experiment at the LHC in 2022. The branching fraction of this decay is measured with respect to the $ \eta\to\mu^{+}\mu^{-}\gamma $ decay mode: $ \mathcal{B}(\eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^-) = (7.3 \pm 2.2)\times 10^{-3}$.Incorporating the world-average value of $ \eta\to\mu^{+}\mu^{-}\gamma $ results in an $ \eta\to\mu^{+}\mu^{-}\mathrm{e}^+\mathrm{e}^- $ branching fraction of $(2.4 \pm 0.8) \times 10^{-6}$, which is close to two orders of magnitude below the previous upper limit and is consistent with the latest standard model predictions.This measurement provides useful information for the determination of transition form factors that are used for theoretical calculations, such as the muon anomalous magnetic moment.
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Compact Muon Solenoid
LHC, CERN