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Model independent measurement of the CKM angle γ using B0 → DK∗0 decays with D → KS0π+π− and KS0K+K−

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Figure 1. Feynman diagrams of the (left) B0 → D0K∗0 and (right) B0 → D0K∗0 amplitudes,which interfere in the B0 → DK∗0 decay.
Figure 2. Binning schemes for (left) D → K0Sπ+π− and (right) D → K0SK+K−. The diagonal lineseparates the positive and negative bin numbers, where the positive bins are in the region m2− ≥ m2+.
Figure 3. Invariant mass distributions of B0 → DK∗0 candidates with (top) D → K0Sπ+π− and(bottom) D → K0SK+K−
Table 1. Functional forms of the DKπ invariant mass distribution, m, in partially reconstructeddecays of B0s → (D∗0 → D0{π0, γ})K∗0, where either the π0 or γ is not reconstructed
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