7 research outputs found

    Semileptonic B and D decays in the quark model

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    We predict the matrix elements and resulting electron spectra for semileptonic meson decays using the quark potential model. Particular attention is paid to the high-energy electron end-point region in B decay since it is crucial to a determination of the b→u weak mixing angle. It is argued that in this region the usual inclusive ("quark decay") calculations are unjustified and must be replaced by explicit sums over decays of the original meson into low-mass exclusive hadronic final states

    Decay constants, semi-leptonic and non-leptonic decays in a Bethe-Salpeter Model

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    We evaluate the decay constants for the B and DD mesons and the form factors for the semileptonic decays of the B meson to DD and D∗D^* mesons in a Bethe-Salpeter model. From data we extract Vcb=0.039±0.002V_{cb}=0.039 \pm 0.002 from Bˉ→D∗lνˉ{\bar B} \to D^* l {\bar{\nu}} and Vcb=0.037±0.004V_{cb}=0.037 \pm 0.004 from Bˉ→Dlνˉ{\bar B} \to D l {\bar{\nu}} decays. The form factors are then used to obtain non-leptonic decay partial widths for B→DÏ€(K) B\to D \pi (K) and B→DD(Ds)B \to D D (D_s) in the factorization approximation.Comment: 15 Pages, 3 Postscript figures (available also from [email protected]

    B --> D(D^*) Form Factors in a Bethe-Salpeter model

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    We calculate the form factors for the semileptonic decays of the BB meson to DD and D∗D^* mesons in a Bethe-Salpeter model. We show that our model is consistent with the constraints of Heavy Quark Effective Theory (HQET) and we extract the matrix elements that represent the 1/mQ1/m_Q corrections to the form factors in HQET. With available data, we obtain VcbV_{cb} =(31.9±1.4)×10−3 (31.9 \pm 1.4)\times10^{-3}.Comment: 15 pages, 5 figure

    Semileptonic Meson Decays in the Quark Model: An Update

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    We present the predictions of ISGW2, an update of the ISGW quark model for semileptonic meson decays. The updated model incorporates a number of features which should make it more reliable, including the constraints imposed by Heavy Quark Symmetry, hyperfine distortions of wavefunctions, and form factors with more realistic high recoil behaviors.Comment: All text and tables contained in the ".latex" file and all figures (14) contained in the ".uu" file

    Branching ratios for eta l(3) in the standard model

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    We compute the rates for ηl3, l=e,μ to one loop in chiral perturbation theory. The total branching ratio for all such modes is found to be 2.6×10-¹³.Daryl Scora and Kim Maltma
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