Abstract We present measurements of the branching fractions of eight$$ {\overline{B}}^0 $$ →D(*)+K−$$ {K}_{(S)}^{\left(\ast \right)0} $$ ,B−→D(*)0K−$$ {K}_{(S)}^{\left(\ast \right)0} $$ decay channels. The results are based on data from SuperKEKB electron-positron collisions at the Υ(4S) resonance collected with the Belle II detector, corresponding to an integrated luminosity of 362 fb−1. The event yields are extracted from fits to the distributions of the difference between expected and observedBmeson energy, and are efficiency-corrected as a function ofm(K−$$ {K}_{(S)}^{\left(\ast \right)0} $$ ) andm(D(*)$$ {K}_{(S)}^{\left(\ast \right)0} $$ ) in order to avoid dependence on the decay model. These results include the first observation of$$ {\overline{B}}^0 $$ →D+K−$$ {K}_S^0 $$ ,B−→D*0K−$$ {K}_S^0 $$ , and$$ {\overline{B}}^0 $$ →D*+K−$$ {K}_S^0 $$ decays and a significant improvement in the precision of the other channels compared to previous measurements. The helicity-angle distributions and the invariant mass distributions of theK−$$ {K}_{(S)}^{\left(\ast \right)0} $$ systems are compatible with quasi-two-body decays via a resonant transition with spin-parityJP= 1−for theK−$$ {K}_S^0 $$ systems andJP= 1+for theK−K*0systems. We also present measurements of the branching fractions of four$$ {\overline{B}}^0 $$ →D(*)+$$ {D}_s^{-} $$ ,B−→D(*)0$$ {D}_s^{-} $$ decay channels with a precision compatible to the current world averages.
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Falconer’s $(K, d)$ distance set conjecture can fail for strictly convex sets $K$ in $\mathbb R^d$
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A bstract Measurements of CP observables in B ± → D (*) K ± and B ± → D (*) π ± decays are presented, where D (∗) indicates a neutral D or D ∗ meson that is an admixture of meson and anti-meson states. Decays of the D (∗) meson to the Dπ 0 and Dγ final states are partially reconstructed without inclusion of the neutral pion or photon. Decays of the D meson are reconstructed in the K ± π ∓ , K + K − , and π + π − final states. The analysis uses a sample of charged B mesons produced in proton-proton collisions and collected with the LHCb experiment, corresponding to integrated luminosities of 2.0, 1.0, and 5.7 fb − 1 taken at centre-of-mass energies of 7, 8, and 13 TeV, respectively. The measurements of partially reconstructed B ± → D (*) K ± and B ± → D (∗) π ± with D → K ∓ π ± decays are the first of their kind, and a first observation of the B ± → $$ {\left(D{\pi}^0\right)}_{D^{\ast }}{\pi}^{\pm } $$ D π 0 D ∗ π ± decay is made with a significance of 6.1 standard deviations. All CP observables are measured with world-best precision, and in combination with other LHCb results will provide strong constraints on the CKM angle γ .more » « less
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