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.
Tree-level Feynman diagram for the $\overline{ B }{} {}^0_ s \rightarrow \chi_{cJ} \phi$ decay mode. |
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Invariant-mass distributions of (left) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} \gamma$ and (right) $ { J \mskip -3mu/\mskip -2mu\psi \mskip 2mu} \gamma K^+ K^-$ after the loose selection criteria. |
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MLP response for (solid yellow) the $\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 1} K^+ K^-$ simulation sample, (hashed blue) high-mass sideband and (black points) the background subtracted $\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 1} K^+ K^-$ signal in data. The histogram areas are normalized to the number of $\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 1} K^+ K^-$ candidates observed in data after the loose selection. The arrow indicates the selected threshold. |
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Invariant-mass distributions of selected candidates for (left) the $\chi _{ c 1} K^+ K^-$ fit and (right) the $\chi _{ c 2} K^+ K^-$ fit. The total fitted function is superimposed (solid red line) together with the (blue hashed area) $\chi _{ c 1} $ component, (solid yellow) $\chi _{ c 2} $ component and (dashed black line) the background component. The pull, i.e. the difference between the observed and fitted value divided by the uncertainty, is shown below each of the plots. |
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Invariant-mass distribution of the $K^+K^-$ pair for the (left) $\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 1} K^+ K^-$ decay obtained with the $\chi _{ c 1} $ mass constraint applied to the $ B ^0_ s $ candidate invariant mass and (right) $\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 2} K^+ K^-$ decay obtained with the $\chi _{ c 2} $ mass constraint applied to the $ B ^0_ s $ candidate invariant mass. The (red solid line) total fitted function is superimposed together with (blue hashed area) the S-wave component. |
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Animated gif made out of all figures. |
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Results of the $\chi _{ c 1} K^+ K^-$ and $\chi _{ c 2} K^+ K^-$ fits to the invariant-mass distributions. A Gaussian constraint is applied to the $s_f$ parameter. |
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Systematic uncertainties for the measurement of the ratio $\mathcal{B}(\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 2} K^+ K^-)/\mathcal{B}(\overline{ B }{} {}^0_ s \rightarrow \chi _{ c 1} K^+ K^-)$. |
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Systematic uncertainties on the $ B ^0_ s $ mass measurement. |
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Supplementary material full pdf |
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This ZIP file contains supplemetary material for the publication LHCb-PAPER-2018-018. The files are: Supplementary.pdf : An overview of the extra figures *.pdf, *.png, *.eps : The figures in variuous formats |
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Created on 20 April 2024.