A combination of measurements sensitive to the $ C P$ violation angle $\gamma $ of the Cabibbo--Kobayashi--Maskawa unitarity triangle, to the charm mixing parameters that describe oscillations between $ D ^0$ and $\overline{ D } {}^0$ mesons, and to $ C P$ asymmetries in the $ D ^0 \rightarrow K ^+ K ^- $ and $ D ^0 \rightarrow \pi ^+ \pi ^- $ decays is performed. All relevant beauty and charm results obtained with the data collected with the LHCb detector at CERN's Large Hadron Collider to date are included. The charm mixing parameters are determined to be $ x = (0.398^{ +0.050}_{ -0.049})\% $ and $ y = (0.636^{ +0.020}_{ -0.019})\% $, the magnitude and phase of $ C P$ violation in charm mixing to be $ |q/p| = (0.995^{ +0.015}_{ -0.016}) $ and $\phi = (2.5 \pm 1.2)^\circ $, and the $ C P$ asymmetries in decay to be $ a_{ K ^+ K ^- }^{\textnormal{d}}$ = $ (9.0 \pm 5.7) \times 10^{-4}$ and $ a_{\pi ^+ \pi ^- }^{\textnormal{d}}$ = $ (24.0 \pm 6.2) \times 10^{-4}$ , with a correlation of $\rho=0.88$. The angle $\gamma $ is found to be $ (63.8^{ +3.5}_{ -3.7})^\circ $ and is the most precise determination from a single experiment.
One dimensional profile likelihood scans of the $ 1-{\rm CL}$ distribution for $\gamma $ from the combination using inputs from $ B ^0_ s $ (light blue, dotted), $ B ^0$ (orange, dot-dashed), $ B ^+ $ mesons (red, dashed) and all species together (blue, solid). |
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Two dimensional profile likelihood contours for (left) the charm mixing parameters $ x$ and $ y$ , and (right) the $ r_{D}^{K\pi}$ and $\delta_{D}^{K\pi}$ parameters. The blue contours (dashed) show the charm only inputs, the orange (solid) contours show the result of this combination. Contours are drawn out to $5\sigma$ and contain $68.3\%$, $95.4\%$, $99.7\%$, etc. of the distribution. |
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Two dimensional profile likelihood contours for (left) the $ C P$ asymmetries in the decay of the $ D ^0 \rightarrow K ^+ K ^- $ and $ D ^0 \rightarrow \pi ^+ \pi ^- $ channels, and (right) the $ |q/p|$ and $\phi$ parameters. The orange contours show the result of this combination, contours for the charm only inputs are indistinguishable so are not shown. Contours are drawn out to $5\sigma$ and contain $68.3\%$, $95.4\%$, $99.7\%$, etc. of the distribution. |
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Profile likelihood contours for the components which contribute towards the $\gamma $ part of the combination, showing the breakdown of sensitivity amongst different sub-combinations of modes. The contours shown are the two-dimensional $1\sigma$ and $2\sigma$ contours which correspond to the areas containing 68.3% and 95.4% of the distribution. |
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Profile likelihood contours for the charm decay and mixing parameters, showing the breakdown of sensitivity amongst different sub-combinations of modes. The contours indicate the 68.3% and 95.4% confidence regions. |
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Two dimensional profile likelihood contours making a comparison between the previous combination \cite{LHCb-PAPER-2021-033} (blue) and the current one (brown). The contours shown are the two-dimensional $1\sigma$ and $2\sigma$ contours which correspond to areas containing 68.3% and 95.4% of the distribution. |
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One dimensional $ 1-{\rm CL}$ profile for $\gamma $ from all inputs used in the combination. |
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Two dimensional profile likelihood contours for the charm mixing parameters $ x$ and $ y$ . The blue (dashed) contours show the charm only inputs, the orange (solid) contours show the result of this combination. Contours are drawn out to $5\sigma$ and contain 68.3%, 95.4%, 99.7%, etc. of the distribution. |
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Evolution of published LHCb combination results for $\gamma $ , with the central values and $1\sigma$ uncertainties in black. The result presented in this note is the rightmost data point; its value and uncertainty are highlighted by the dashed blue line and band, respectively. |
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Animated gif made out of all figures. |
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Measurements used in the combination. Those that are new, or that have changed, since the previous combination \cite{LHCb-PAPER-2021-033} are highlighted in bold. The Run 1 and 2 took place from 2011 to 2012, corresponding to $1(2)\text{ fb} ^{-1} $ of integrated luminosity of proton-proton collisions at a centre-of-mass energy of $7(8)\text{ Te V} $, and from 2015 to 2018, corresponding to $6\text{ fb} ^{-1} $ at $13\text{ Te V} $, respectively. Measurements denoted by (*) include only a fraction of the Run 2 sample, corresponding to data taken in 2015 and 2016. Where multiple references are cited, measured values are taken from the most recent results, which include information from the others. |
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Auxiliary inputs used in the combination. Those highlighted in bold have changed since the previous combination \cite{LHCb-PAPER-2021-033}. |
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Confidence intervals and central values for each of the parameters of interest, computed using the Feldman-Cousins Plugin method \cite{Bodhisattva:2009uba}. Entries marked with an asterisk show where the scan has hit a physical boundary at the lower limit. |
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Confidence intervals and best-fit values for $\gamma $ when splitting the combination inputs by initial $B$ meson species, computed using the Feldman-Cousins Plugin method \cite{Bodhisattva:2009uba}. |
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Confidence intervals and best-fit values for $\gamma $ when splitting the combination inputs by time-dependent and time-integrated methods. |
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Reduced correlation matrix for the parameters of greater interest. Values smaller than $0.01$ are replaced with a - symbol. |
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Correlation matrix of the fit result. Values smaller than $0.01$ are replaced with a - symbol. |
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Correlation matrix for the $ B ^\pm \rightarrow D h^\pm $ , $ D\rightarrow K ^\pm \pi ^\mp \pi ^+ \pi ^- $ inputs. |
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Contributions to the total $\chi^2$ and the number of observables of each input measurement. |
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Created on 03 May 2024.