Extracting V bu V bc from semileptonic <mml:…

1990; American Physical Society; Volume: 42; Issue: 1 Linguagem: Inglês

10.1103/physrevd.42.85

ISSN

1538-4500

Autores

G. Krämer, William F. Palmer,

Tópico(s)

Neutrino Physics Research

Resumo

Recent CLEO and ARGUS results for charmless semileptonic decays of $B$ mesons are compared to several models for exclusive channels under the assumption that the $\ensuremath{\pi}$, $\ensuremath{\rho}$, $D$, and ${D}^{*}$ saturate the region of high electron momentum of interest in determining $\frac{{V}_{\mathrm{bu}}}{{V}_{\mathrm{bc}}}$. The effect of current-algebra-inspired $\ensuremath{\pi}\ensuremath{\pi}$ backgrounds and threshold constraints in the $\ensuremath{\rho}$ channel, as well as the error made by the narrow-width approximation, are examined with a view to estimating the model dependence inherent in extracting $\frac{{V}_{\mathrm{bu}}}{{V}_{\mathrm{bc}}}$ from the data. Total semileptonic rates to $\ensuremath{\pi}$ and $\ensuremath{\rho}$ differ widely, model to model, while rates to $D$ and ${D}^{*}$ final states have much less model dependence. Model dependence is somewhat smaller when only high lepton energies are concerned. ${V}_{\mathrm{bc}}$ calculated from exclusive semileptonic decay to $D$ and ${D}^{*}$ final states vary about 25% and 10%, respectively, model to model. The model dependence of $\frac{{V}_{\mathrm{bu}}}{{V}_{\mathrm{bc}}}$ is also considerable. The narrow-width approximation in the $\ensuremath{\rho}$ channel can be a 20% effect in the determination of this ratio because of the sensitivity of the high-energy region to the lowest mass of the final hadronic system. If current-algebra-inspired backgrounds are present, $\frac{{V}_{\mathrm{bu}}}{{V}_{\mathrm{bc}}}$ may be considerably smaller than suggested by many models. If the ${D}^{**}$ component of $b$ to $c$ is as large as recent CLEO data suggest, $\frac{{V}_{\mathrm{bu}}}{{V}_{\mathrm{bc}}}$ may be 16% larger than expected by models that ignore this contribution. Electron spectra for various models are presented, illustrating the high variation of shape features in the end-point region.

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