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Observation of Radiative B Meson Decays into Higher Kaonic Resonances

Abstract

We have studied radiative B meson decays into higher kaonic resonances decaying into a two-body or three-body final state, using a data sample of 21.3 fb1^{-1} recorded at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at KEKB. For the two-body final state, we extract the BK2(1430)0γB \to K_2^{*}(1430)^0 \gamma component from an analysis of the helicity angle distribution, and obtain B(B0K2(1430)0γ)=(1.26±0.66±0.10)×105{\cal B}(B^0 \to K_2^{*}(1430)^0 \gamma) = (1.26\pm 0.66\pm 0.10)\times 10^{-5}. For the three-body final state, we observe a BKππγB \to K\pi\pi\gamma signal that is consistent with a mixture of BKπγB \to K^* \pi \gamma and BKργB \to K \rho \gamma. This is the first time that BKπγB \to K^* \pi \gamma and BKργB \to K \rho \gamma have been observed separately. We find their branching fractions to be B(BKπγ;MKπ<2.0GeV/c2)=(5.6±1.1±0.9)×105{\cal B}(B \to K^* \pi \gamma; M_{K^*\pi}<2.0 GeV/c^2) = (5.6\pm 1.1\pm 0.9)\times 10^{-5} and B(BKργ;MKρ<2.0GeV/c2)=(6.5±1.71.2+1.1)×105{\cal B}(B \to K \rho \gamma; M_{K\rho} < 2.0 GeV/c^2) = (6.5\pm 1.7^{+1.1}_{1.2})\times 10^{-5}, respectively

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