Abstract

We consider hadronic transitions from the hb(2P)h_b(2P) bottomonium resonance to lower states of bottomonium with emission of either ωω meson, or two pions, or ηη meson. For the former two transitions the branching ratios are related to similar transitions from χb1(2P)χ_{b1}(2P) and the recently measured by Belle fractions of the radiative decays of hb(2P)h_b(2P). We argue that the fraction of the hb(2P)h_b(2P) total decay rate remaining for the annihilation rate is on the verge of contradiction with the `parton' picture of bottomonium annihilation resulting in similarity between the decays of hb(1,2P)h_b(1,2P) and χb1(1,2P)χ_{b1}(1,2P). The contradiction gets even stronger, if the transition hb(2P)→Υ(1S) ηh_b(2P) \to Υ(1S) \, η has branching fraction of a few percent or more. We argue that, although quite uncertain, the latter fraction may indeed be that significant.

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