Contributions of the kaon pair from ρ(770)ρ(770) for the three-body decays B→DKKˉB \to D K\bar{K}

preprint2021arXivOpen access

Abstract

We study the contributions of the kaon pair originating from the resonance ρ(770)ρ(770) for the three-body decays B→DKKˉB \to D K\bar{K} by employing the perturbative QCD approach. According to the predictions in this work, the contributions from the intermediate state ρ(770)0ρ(770)^0 are relatively small for the three-body decays such as B0→Dˉ0K+K−B^0 \to \bar{D}^0 K^+ K^-, Bs0→Dˉ0K+K−B_s^0 \to \bar{D}^0 K^+ K^-, and B+→Ds+K+K−B^+ \to D_s^+ K^+K^-, while about 20%20\% of the total three-body branching fraction for B+→Dˉ0K+Kˉ0B^+ \to \bar{D}^0 K^+ \bar{K}^0 could possibly come from the subprocess ρ(770)+→K+Kˉ0ρ(770)^+\to K^+ \bar{K}^0. We also estimate the branching fractions for ρ(770)±ρ(770)^\pm decay into the kaon pair to be about 1%1\%, and that for the neutral ρ(770)ρ(770) decay into K+K−K^+K^- or K0Kˉ0K^0\bar{K}^0 to be about 0.5%0.5\%, which will be tested by future experiments.

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