A search for the very rare $D^0 \to \mu^+\mu^-$ decay is performed using data collected by the LHCb experiment in proton-proton collisions at $\sqrt{s} = 7$, 8 and $13 \rm{TeV}$, corresponding to an integrated luminosity of $9 \rm{fb^{-1}}$. The search is optimised for $D^0$ mesons from $D^{\ast+}\to D^0\pi^+$ decays but is also sensitive to $D^0$ mesons from other sources. No evidence for an excess of events over the expected background is observed. An upper limit on the branching fraction of this decay is set at $\mathcal{B}(D^0 \to \mu^+\mu^-) < 3.1 \times 10^{-9}$ at a $90\%$ CL. This represents the world's most stringent limit, constraining models of physics beyond the Standard Model.
Distributions of $\Delta m$ for (left) $ D ^0 \rightarrow K ^- \pi ^+ $ and (right) $ D ^0 \rightarrow \pi ^+ \pi ^- $ normalisation channels candidates for (top) Run 1 and (bottom) Run 2 data. The distributions are superimposed with the fit. |
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Distribution of (left) $ m(\mu ^+\mu ^- )$ and (right) $\Delta m$ for the $ D ^0 \rightarrow \mu ^+ \mu ^- $ candidates in data from (top) Run 1 and (bottom) Run 2 , for the most sensitive BDT interval. The distribution is superimposed with the fit to data. Each of the two distributions is in the signal region of the other variable, see text for details. Untagged and tagged decays are included in a single component for signal and $ D ^0 \rightarrow \pi ^+ \pi ^- $ background. |
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Distributions of (left) $ m(\mu ^+\mu ^- )$ and (right) $\Delta m$ for the $ D ^0 \rightarrow \mu ^+ \mu ^- $ candidates for Run 1 data in, top to bottom, the three BDT intervals. The distributions are superimposed with the fit to data. Each of the two distributions is in the signal region of the other variable, see text for details. Untagged and tagged decays are included in a single component for signal and $ D ^0 \rightarrow \pi ^+ \pi ^- $ background. |
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Distributions of (left) $ m(\mu ^+\mu ^- )$ and (right) $\Delta m$ for the $ D ^0 \rightarrow \mu ^+ \mu ^- $ candidates for Run 2 data in, top to bottom, the three BDT bins. The distributions are superimposed with the fit to data. Each of the two distributions is in the signal region of the other variable, see text for details. Untagged and tagged decays are included in a single component for signal and $ D ^0 \rightarrow \pi ^+ \pi ^- $ background. |
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Distributions of (left) $ m(\mu ^+\mu ^- )$ and (right) $\Delta m$ for the $ D ^0 \rightarrow \mu ^+ \mu ^- $ candidates for Run 1 data in, top to bottom, the three BDT bins. The distributions are superimposed with the fit to data. Untagged and tagged decays are included in a single component for signal and $ D ^0 \rightarrow \pi ^+ \pi ^- $ background. Unlike the correspondent figures in the main body of the Letter, here all events are shown. |
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Distributions of (left) $ m(\mu ^+\mu ^- )$ and (right) $\Delta m$ for the $ D ^0 \rightarrow \mu ^+ \mu ^- $ candidates for Run 2 data in, top to bottom, the three BDT bins. The distributions are superimposed with the fit to data. Untagged and tagged decays are included in a single component for signal and $ D ^0 \rightarrow \pi ^+ \pi ^- $ background. Unlike the correspondent figures in the main body of the Letter, here all events are shown. |
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Two-dimensional distribution of $ m( D ^0 )$ versus $\Delta m$ for the most sensitive BDT interval in the (left) Run 1 and (right) Run 2 data. Red lines represent the signal region of each variable as defined in the text. |
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Distribution of the BDT output. The $ D ^0 \rightarrow \pi ^+ \pi ^- $ candidates in data and simulation are shown and used to weight the simulated $ D ^0 \rightarrow \mu ^+ \mu ^- $ decays distribution used for the search. |
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Efficiency for two pions to pass a requirement on the $ProbNNmu$ variable (after additional requirements on its identification as muon) in Run 2, as measured from $ D ^+ \rightarrow \pi ^+ \pi ^- \pi ^+ $ and $ D ^+_ s \rightarrow \pi ^+ \pi ^- \pi ^+ $ decays in data and $ D ^0 \rightarrow \pi ^+ \pi ^- $ decays in simulation. Same sign pions are used in data to avoid contamination for hadronic resonances decaying to two real muons. |
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Value of $\rm{CL_s}$ as a function of the $ D ^0 \rightarrow \mu ^+ \mu ^- $ branching fraction. |
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Animated gif made out of all figures. |
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Created on 27 April 2024.