The $B^+ \rightarrow D_s^+ D_s^- K^+$ decay is observed for the first time using proton-proton collision data collected by the LHCb detector at centre-of-mass energies of $7$, $8$ and $13 \text{TeV}$, corresponding to an integrated luminosity of $9 \text{fb}^{-1}$. Its branching fraction relative to that of the $B^{+} \rightarrow D^{+} D^{-} K^{+}$ decay is measured to be $$\frac{B\left(B^{+} \rightarrow D_s^{+} D_s^{-} K^{+}\right)}{B\left(B^{+} \rightarrow D^{+} D^{-} K^{+}\right)}=0.525 \pm 0.033 \pm 0.027 \pm 0.034,$$ where the first uncertainty is statistical, the second systematic, and the third is due to the uncertainties on the branching fractions of the $D_s^{\pm} \rightarrow K^{\mp} K^{\pm} \pi^{\pm}$ and $D^{\pm} \rightarrow K^{\mp} \pi^{\pm} \pi^{\pm}$ decays. This measurement fills an experimental gap in the knowledge of the family of Cabibbo$-$favoured $\bar{b} \rightarrow \bar{c} c \bar{s}$ transitions and opens the path for unique studies of spectroscopy in future.
Feynman diagrams contributing to the $ B ^+ \rightarrow D ^+_ s D ^-_ s K ^+ $ decay. |
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Invariant-mass distributions of reconstructed (left) $ D ^+_ s $ $ D ^-_ s $ $ K ^+$ and (right) $ D ^+$ $ D ^-$ $ K ^+$ candidates. The fit results are overlaid. |
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Distributions of background-subtracted invariant mass of the (top) $ D ^+_ s $ $ D ^-_ s $ , (bottom left) $ D ^-_ s $ $ K ^+$ and (bottom right) $ D ^+_ s $ $ K ^+$ systems of the $ B ^+ \rightarrow D ^+_ s D ^-_ s K ^+ $ decay. |
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Efficiency as a function of the Dalitz-plot variables for the (top) $ B ^+ \rightarrow D ^+_ s D ^-_ s K ^+ $ and (bottom) $ B ^+ \rightarrow D ^+ D ^- K ^+ $ decays, calculated separately for the (left) Run1 and (right) Run2 periods. |
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Animated gif made out of all figures. |
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Sources of systematic uncertainty on the branching-fraction ratio. The statistical uncertainty is also given. |
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Created on 19 April 2024.