HQET and Form Factor Effects in B→K(∗)ℓ+ℓ−B\to K^{(*)}\ell^+\ell^-

preprint1995arXivOpen access

Abstract

We examine the rates for the exclusive decays B→K(∗)ℓ+ℓ−B\to K^{(*)}\ell^+\ell^-. We use the scaling predictions of the heavy quark effective theory to extract the necessary form factors from fits to various combinations of data. These data include the D→K(∗)ℓνD\to K^{(*)}\ellν semileptonic decays, as well as the nonleptonic decays B→K(∗)ψ(′)B\to K^{(*)}ψ^{(\prime)} and the rare decay B→K∗γB\to K^*γ. We use different parametrizations of form factors, and find that integrated decay rates are not very sensitive to the forms chosen. However, the decay spectra and the forward-backward asymmetry in B→K∗ℓ+ℓ−B\to K^*\ell^+\ell^- are sensitive to the forms chosen for the form factors, while the lepton polarization asymmetry in Bˉ0→Kˉ0μ+μ−\bar B^0\to \bar K^0μ^+μ^- is largely independent of the choice of form factors. Contributions from charmonium resonances dominate the spectra and integrated rates. In our `best' scenario, we find Br(Bˉ0→Kˉ0μ+μ−)=2.0±0.3×10−6Br(\bar B^0\to \bar K^0μ^+μ^-)=2.0\pm 0.3\times 10^{-6} and Br(Bˉ0→Kˉ∗0μ+μ−)=8.1±2.0×10−6Br(\bar B^0\to \bar K^{*0}μ^+μ^-)=8.1\pm 2.0\times 10^{-6}. We also make predictions for other polarization observables in these decays.

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