A measurement of $C P$-violating observables in $B^{\pm} \to D^{*} K^{\pm}$ and $B^{\pm} \to D^{*} \pi^{\pm}$ decays is made where the photon or neutral pion from the $D^{*} \to D\gamma$ or $D^{*} \to D\pi^{0}$ decay is not reconstructed. The $D$ meson is reconstructed in the self-conjugate decay modes, $D \to K_{S}^{0} \pi^{+} \pi^{-}$ or $D \to K_{S}^{0} K^{+} K^{-}$. The distribution of signal yields in the $D$ decay phase space is analysed in a model-independent way. The measurement uses a data sample collected in proton-proton collisions at centre-of-mass energies of 7, 8, and 13 TeV, corresponding to a total integrated luminosity of approximately 9 fb$^{-1}$. The $B^{\pm} \to D^{*} K^{\pm}$ and $B^{\pm} \to D^{*} \pi^{\pm}$ $C P$-violating observables are interpreted in terms of hadronic parameters and the CKM angle $\gamma$, resulting in a measurement of $\gamma = (92^{+21}_{-17})^{\circ}$. The total uncertainty includes the statistical and systematic uncertainties, and the uncertainty due to external strong-phase inputs.
Mass distributions for (left) $ D K $ samples and (right) $ D \pi$ samples, with $ D \rightarrow K ^0_{\mathrm{S}} \pi ^+ \pi ^- $ decays reconstructed with a (top) downstream $ K ^0_{\mathrm{S}}$ candidate and a (bottom) long $ K ^0_{\mathrm{S}}$ candidate. The projections of the fit results are overlaid. In the legend, particles in square brackets are not reconstructed. |
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Mass distributions for (left) $ D K $ samples and (right) $ D \pi$ samples, with $ D \rightarrow K ^0_{\mathrm{S}} K ^+ K ^- $ decays reconstructed with a (top) downstream $ K ^0_{\mathrm{S}}$ candidate and a (bottom) long $ K ^0_{\mathrm{S}}$ candidate. The projections of the fit results are overlaid. In the legend, particles in square brackets are not reconstructed. |
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Contours at 68.3% and 95.5% confidence levels indicated by the darker and lighter regions, respectively, for (left, red) $(x_{-}^{ D ^* K }, y_{-}^{ D ^* K })$ which is labelled $ B ^- $ and (left, purple) $(x_{+}^{ D ^* K }, y_{+}^{ D ^* K })$ which is labelled $ B ^+ $, and (right) $(\Re(\xi^{ D ^* \pi}), \Im(\xi^{ D ^* \pi}))$, including only statistical uncertainty. The black points indicate the central values. |
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Confidence intervals at 68.3% and 95.5% for the CKM angle $\gamma $ . |
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Confidence regions at 68.3% and 95.5% indicated by the lighter and darker shades respectively, for (top, left) $\gamma $ vs. $r_{B}^{ D ^* K }$, (top, right) $\gamma $ vs. $\delta_{B}^{ D ^* K }$, (bottom left) $\gamma $ vs. $r_{B}^{ D ^* \pi}$, and (bottom, right) $\gamma $ vs. $\delta_{B}^{ D ^* \pi}$. |
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Animated gif made out of all figures. |
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Signal and background yields from the global fit over the full mass range, ${4900\textendash5600\text{ Me V /}c^2 }$. All yields and uncertainties are rounded to the nearest integer and uncertainties of 1 mean one or fewer. Backgrounds that are not written explicitly in this table are included in the `Other Backgrounds' component. |
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Summary of the systematic uncertainties. Values are expressed in units of $10 ^{-2}$. |
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Statistical correlation matrix for the $ C P$ -violating observables. |
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Correlation matrix associated with LHCb-related systematic uncertainties. |
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Correlation matrix associated with the strong-phase inputs. |
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Created on 26 April 2024.