A measurement of the $CP$-violating observables from $B^{\pm}\rightarrow D^* K^{\pm}$ and $B^{\pm}\rightarrow D^* \pi^{\pm}$ decays is presented, where $D^* (D) $ is an admixture of $D^{*0}$ and $\bar{D}^{*0}$ ($D^0$ and $\bar{D}^0$) states and is reconstructed through the decay chains $ D^* \rightarrow D\pi^0/\gamma$ and $D \to K_S^0 \pi^+\pi^-/K_S^0 K^+K^-$. The measurement is performed by analysing the signal yield variation across the $D$ decay phase space and is independent of any amplitude model. The data sample used was collected by the LHCb experiment in proton-proton collisions and corresponds to a total integrated luminosity of 9 fb$^{-1}$ at centre-of-mass energies of 7, 8 and 13 TeV. The CKM angle $\gamma$ is determined to be $(69^{+13}_{-14})^{\circ}$ using the measured $CP$-violating observables. The hadronic parameters $r^{D^* K^{\pm}}_B, r^{D^* \pi^{\pm}}_B, \delta^{D^* K^{\pm}}_B, \delta^{D^* \pi^{\pm}}_B$, which are the ratios and strong phase differences between favoured and suppressed $B^{\pm}$ decays, are also reported.
(left) "Optimal" binning scheme \cite{Ablikim:2020lpk} used for $D\rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ decays. (right) "2-bins" binning scheme \cite{Ablikim:2020cfp} used for $D\rightarrow K ^0_{\mathrm{S}} K^+K^-$ decays. They are the same as those in a previous model-independent measurement \cite{LHCb-PAPER-2020-019}. |
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Projections of (left) $m( D h ^\pm )$ invariant-mass distribution and (right) $m( D \pi ^0 )$ invariant-mass distribution for the $ B ^\pm \rightarrow D ^* K ^\pm $ channels, reconstructed with the $ D ^* \rightarrow D \pi ^0 $, (a) $ D \rightarrow K ^0_{\mathrm{S}} K ^+ K ^- $ and (b) $ D \rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ modes. The signal and in-reco $ D ^* $ contributions are shown as solid colours. |
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Projections of (left) $m( D h ^\pm )$ invariant-mass distribution and (right) $m( D \pi ^0 )$ invariant-mass distribution for the $ B ^\pm \rightarrow D ^* \pi ^\pm $ channels, reconstructed with the $ D ^* \rightarrow D \pi ^0 $, (a) $ D \rightarrow K ^0_{\mathrm{S}} K ^+ K ^- $ and (b) $ D \rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ modes. The signal and in-reco $ D ^* $ contributions are shown as solid colours. |
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Projections of (left) $m( D h ^\pm )$ invariant-mass distribution and (right) $m( D \gamma)$ invariant-mass distribution for the $ B ^\pm \rightarrow D ^* K ^\pm $ channels, reconstructed with the $ D ^* \rightarrow D \gamma$, (a) $ D \rightarrow K ^0_{\mathrm{S}} K ^+ K ^- $ and (b) $ D \rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ modes. The signal, in-reco $ D ^* $ and part-reco $ D ^*$ contributions are shown as solid colours. |
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Projections of (left) $m( D h ^\pm )$ invariant-mass distribution and (right) $m( D \gamma)$ invariant-mass distribution for the $ B ^\pm \rightarrow D ^* \pi ^\pm $ channels, reconstructed with the $ D ^* \rightarrow D \gamma$, (a) $ D \rightarrow K ^0_{\mathrm{S}} K ^+ K ^- $ and (b) $ D \rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ modes. The signal, in-reco $ D ^* $ and part-reco $ D ^*$ contributions are shown as solid colours. |
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Expected asymmetry in each bin for (left) $B^{\pm} \rightarrow D^*K^{\pm}$ and (right) $B^{\pm} \rightarrow D^* \pi^{\pm}$, calculated from the $ C P$ -violating observables measured in the default fit, are shown with the solid lines and obtained in fits with independent bin yields freely varied are shown with the error bars (data points). The vertical dashed lines separate the $ D \rightarrow K ^0_{\mathrm{S}} \pi^{+} \pi^{-}$ and $ D \rightarrow K ^0_{\mathrm{S}} K^{+} K^-$ bins on the horizontal axes. |
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Confidence level at 68.2% and 95.5% probability for (left, green) $x^{ D ^* K}_{+},y^{ D ^* K}_{+}$, (left, violet) $x^{ D ^* K}_{-},y^{ D ^* K}_{-}$ and (right, green) $x^{ D ^* \pi}_{\xi},y^{ D ^* \pi}_{\xi}$ are measured in $B^{\pm}\rightarrow D ^* h^{\pm}$ decays from a profile likelihood scan. |
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Confidence limits for the CKM angle $\gamma$, as determined from {\tt GammaCombo} \cite{GammaCombo, LHCb-PAPER-2021-033}. |
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Confidence level regions for the combination of physical parameters ($ \gamma , \delta_B^{ D ^* K}, r_B^{ D ^* K}, \delta_B^{ D ^* \pi}, r_B^{ D ^* \pi}$) of interest. The 68% (hashed blue area) and 95% (light blue area) are determined from {\tt GammaCombo} \cite{GammaCombo, LHCb-PAPER-2021-033}. |
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Animated gif made out of all figures. |
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Yields of fully reconstructed $ D ^*$ contributions obtained from datasets with $ D \rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ decays. |
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Yields of fully reconstructed $ D ^*$ contributions obtained from the datasets with $ D \rightarrow K ^0_{\mathrm{S}} K^+K^-$ decays. |
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Summary of uncertainties on the measurement of $x^{ D ^* K}_{\pm},y^{ D ^* K}_{\pm},x^{ D ^* \pi}_{\xi}$ and $y^{ D ^* \pi}_{\xi}$. All numbers have been scaled up by a factor of 100. |
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Statistical correlation matrix for $ C P$ -violating observables. |
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Systematic correlation matrix for considered LHCb related effects. |
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Systematic correlation matrix for the strong phase inputs. |
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Yields of incorrectly reconstructed and partially reconstructed $ D ^*$ contributions from datasets with $D\rightarrow K ^0_{\mathrm{S}} \pi^+\pi^-$ decays. |
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Yields of incorrectly reconstructed and partially reconstructed $ D ^*$ contributions from the datasets with $ D \rightarrow K_S^0K^+K^-$ decays. |
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Created on 26 April 2024.