Abstract

We investigate the decays of the excited (bqˉ)(b\bar q) mesons as probes of the short-distance structure of the weak ΔB=1ΔB=1 transitions. These states are unstable under the electromagnetic or strong interactions although their widths are typically suppressed by phase space. As compared to the pseudoscalar BB meson, the purely leptonic decays of the vector B∗B^* are not chirally suppressed and are sensitive to different combinations of the underlying weak effective operators. An interesting example is Bs∗→ℓ+ℓ−B^*_s\to \ell^+\ell^-, which has a rate that can be accurately predicted in the standard model. The branching fraction is B∼10−11\mathcal{B}\sim10^{-11}, irrespective of the lepton flavor and where the main uncertainty stems from the unmeasured and theoretically not-well known Bs∗B_s^* width. We discuss the prospects for producing this decay mode at the LHC and explore the possibility of measuring the Bs∗→ℓℓB_s^*\to\ell\ell amplitude, instead, through scattering experiments at the Bs∗B_s^* resonance peak. Finally we also discuss the charged-current Bu,c∗→ℓνB_{u,c}^*\to\ellν decay which can provide complementary information on the b→uℓνb\to u\ellν and b→cℓνb\to c\ellν transitions.

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