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The $overline{B_s^0} rightarrow chi_{c2} K^+ K^- $ decay mode is observed and its branching fraction relative to the corresponding $chi_{c1}$ decay mode, in a $pm 15 textrm{MeV}/c^2$ window around the $phi$ mass, is found to be $frac{mathcal{B}(overline{B_s^0} rightarrow chi_{c2} K^+ K^-) }{ mathcal{B}(overline{B_s^0} rightarrow chi_{c1} K^+ K^-)} = (17.1 pm 3.1 pm 0.4 pm 0.9)%,$ where the first uncertainty is statistical, the second systematic and the third due to the knowledge of the branching fractions of radiative $chi_c$ decays. The decay mode $overline{B_s^0} rightarrow chi_{c1} K^+ K^- $ allows the $ B_s^0$ mass to be measured as $m(B_s^0) = 5366.83 pm 0.25 pm 0.27 , textrm{MeV}/c^2,$ where the first uncertainty is statistical and the second systematic. A combination of this result with other LHCb determinations of the $B_s^0$ mass is made.
The first observation of the $B_s^0 to overline{D}^0 K^+ K^-$ decay is reported, together with the most precise branching fraction measurement of the mode $B^0 to overline{D}^0 K^+ K^-$. The results are obtained from an analysis of $pp$ collision dat
The first observation of the decay $B_s^0 rightarrow phi bar{K}^{*0}$ is reported. The analysis is based on a data sample corresponding to an integrated luminosity of 1.0 fb$^{-1}$ of $pp$ collisions at $sqrt{s} = 7 TeV$, collected with the LHCb dete
We measure the decay $B_s^0rightarrow K^0overline{K}^0$ using data collected at the $Upsilon(5S)$ resonance with the Belle detector at the KEKB $e^+e^-$ collider. The data sample used corresponds to an integrated luminosity of 121.4 ${rm fb^{-1}}$. W
The first observation of the decay $B^0 rightarrow D^0 overline{D}{}^0 K^+ pi^-$ is reported using proton-proton collision data corresponding to an integrated luminosity of 4.7 $mathrm{fb}^{-1}$ collected by the LHCb experiment in 2011, 2012 and 2016
The decay $overline{B}_s^0 rightarrow psi(2S) K^+ pi^-$ is observed using a data set corresponding to an integrated luminosity of $3.0fb^{-1}$ collected by the LHCb experiment in $pp$ collisions at centre-of-mass energies of 7 and 8 TeV. The branchin