17 research outputs found

    Evidence for Factorization in Three-body BˉD()KK0\bar B\to D^{(*)} K^- K^0 Decays

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    Motivated by experimental results on BˉD()KK0\bar B\to D^{(*)}K^-K^{0}, we use a factorization approach to study these decays. Two mechanisms concerning kaon pair production arise: current-produced (from vacuum) and transition (from the BB meson). The kaon pair in the Bˉ0D()+KK0\bar B {}^0\to D^{(*)+}K^-K^0 decays can be produced only by the vector current (current-produced), whose matrix element can be extracted from e+eKKˉe^+e^-\to K\bar K processes via isospin relations. The decay rates obtained this way are in good agreement with experiment. The BD()0KK0B^-\to D^{(*)0}K^-K^0 decays involve both current-produced and transition processes. By using QCD counting rules and the measured BD()0KK0B^-\to D^{(*)0} K^- K^0 decay rates, the measured decay spectra can be understood.Comment: 3 pages, 6 figures. Talk presented at EPS2003 Conference, Aachen, Germany, July 200

    Charmed Ωc\Omega_c weak decays into Ω\Omega in the light-front quark model

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    More than ten Ωc0\Omega_c^0 weak decay modes have been measured with the branching fractions relative to that of Ωc0Ωπ+\Omega^0_c\to\Omega^-\pi^+. In order to extract the absolute branching fractions, the study of Ωc0Ωπ+\Omega^0_c\to\Omega^-\pi^+ is needed. In this work, we predict BπB(Ωc0Ωπ+)=(5.1±0.7)×103{\cal B}_\pi\equiv {\cal B}(\Omega_c^0\to\Omega^-\pi^+)=(5.1\pm 0.7)\times 10^{-3} with the Ωc0Ω\Omega_c^0\to\Omega^- transition form factors calculated in the light-front quark model. We also predict BρB(Ωc0Ωρ+)=(14.4±0.4)×103{\cal B}_\rho\equiv {\cal B}(\Omega_c^0\to\Omega^-\rho^+)=(14.4\pm 0.4)\times 10^{-3} and BeB(Ωc0Ωe+νe)=(5.4±0.2)×103{\cal B}_e\equiv{\cal B}(\Omega_c^0\to\Omega^-e^+\nu_e)=(5.4\pm 0.2)\times 10^{-3}. The previous values for Bρ/Bπ{\cal B}_\rho/{\cal B}_\pi have been found to deviate from the most recent observation. Nonetheless, our Bρ/Bπ=2.8±0.4{\cal B}_\rho/{\cal B}_\pi=2.8\pm 0.4 is able to alleviate the deviation. Moreover, we obtain Be/Bπ=1.1±0.2{\cal B}_e/{\cal B}_\pi=1.1\pm 0.2, which is consistent with the current data.Comment: 12 pages, 2 figure

    Possible Hints and Search for Glueball Production in Charmless Rare B Decays

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    Recent data on B->p pbar K, K0 pi pi and K Kbar K hint at a 2.3\sim 2.3 GeV object recoiling against a kaon. This could be the narrow state observed in J/\psi -> gamma xi. Nonobservation in p pbar annihilation implies B(ξppˉ){\cal B}(\xi \to p\bar p) \sim few ×103\times 10^{-3}, consistent with eta_c and J/\psi decays, but there are actual hints in p pbar -> phi phi and p p-> p pi^+ pi^- pi^+ pi^- p. Simple modeling shows B(BξK)B(ξppˉ)1×106{\cal B}(B \to \xi K){\cal B}(\xi \to p\bar p) \sim 1\times 10^{-6}, appearing as a spike in the ppˉp\bar p spectrum, with \sim 30 events per 100 fb1^{-1}; modes such as K K_s K_s, K phi phi, K4 pi (K f_2 pi pi) etc. should be explored. The underlying dynamics of g* -> g xi is analogous to g* -> g etaprime or gluon fragmentation. Discovery of sizable B -> xi K could be useful for CP violation studies.Comment: 4 pages, 3 figure

    Prediction of Three-body B0ρpnˉ,πpnˉB^0\to \rho^-p\bar{n}, \pi^-p\bar{n} Decay Rates

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    We predict the rates of the charmless three-body B0ρpnˉB^0\to \rho^-p\bar{n} and πpnˉ\pi^-p\bar{n} modes due to weak vector current contributions to be 4×106\sim 4\times 10^{-6} and 2×1062\times 10^{-6}, respectively. The basis is a factorization approach of current produced nucleon pairs, together with an isospin transformation that relates nucleon weak vector form factors to electromagnetic form factors. Adding the axial vector current contribution, we find B0ρpnˉB^0\to \rho^-p\bar{n} and B+ρ0pnˉB^+\to \rho^0p\bar{n} to be at 10510^{-5} order. The three-body modes appear to dominate over the two-body modes such as BppˉB\to p\bar{p}, pΛˉp\bar \Lambda.Comment: 5 pages, 4 figures. Version to appear in Phys. Lett.

    Charmless Three-Body Baryonic B Decays

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    Motivated by recent data on B-> p pbar K decay, we study various charmless three-body baryonic B decay modes, including Lambda pbar pi, Sigma0 pbar pi, p pbar pi, p pbar Kbar0, in a factorization approach. These modes have rates of order 10^{-6}. There are two mechanisms for the baryon pair production, current-produced and transition. The behavior of decay spectra from these baryon production mechanisms can be understood by using QCD counting rules. Predictions on rates and decay spectra can be checked in the near future.Comment: 26 pages, 9 figures; version to appear in Phys. Rev.

    Evidence for Factorization in Three-body B --> D(*) K- K0 Decays

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    Motivated by recent experimental results, we use a factorization approach to study the three-body B --> D(*) K- K0 decay modes. Two mechanisms are proposed for kaon pair production: current-produced (from vacuum) and transition (from B meson). The Bbar0 --> D(*)+ K- K0 decay is governed solely by the current-produced mechanism. As the kaon pair can be produced only by the vector current, the matrix element can be extracted from e+ e- --> K Kbar processes via isospin relations. The decay rates obtained this way are in good agreement with experiment. Both current-produced and transition processes contribute to B- --> D(*)0 K- K0 decays. By using QCD counting rules and the measured B- --> D(*)0 K- K0 decay rates, the measured decay spectra can be understood.Comment: 17 pages, 6 figure
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