833 research outputs found

    Weak Decays of Doubly Heavy Baryons: BccBcV{\cal B}_{cc}\to {\cal B}_c V

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    The weak decays of a spin-1/21/2 doubly charm baryon (Bcc{\cal B}_{cc}) to a spin-1/21/2 singly charm baryon (Bc{\cal B}_c) and a light vector meson (VV) are studied under a phenomenological scheme. The contributions are classified into different topological diagrams, among which the short distance ones are calculated under the factorization hypothesis, and the long distance contributions are modelled as final-state interactions (FSIs) which are estimated with the one-particle-exchange model. In calculation the topological contributions tend to fall in a hierarchy. The branching fractions or decay widths are estimated, and it indicates that Ξcc+Ξc+π+π\Xi_{cc}^+\to\Xi_c^+\pi^+\pi^- and Ωcc+Ξc+Kπ+\Omega_{cc}^{+}\rightarrow\Xi_{c}^{+}K^-\pi^+ can be used as candidate decays for searching Ξcc+\Xi_{cc}^+ and Ωcc+\Omega_{cc}^+. Some decays that are mainly activated by the long distance effects are found, observation on which in future experiments can help to understand the role of FSIs in charm baryon decays.Comment: 29 pages, 5 figures, 7 tables; version published in EPJ

    Branching Ratios, Forward-backward Asymmetry and Angular Distributions of BK1l+lB\to K_1l^+l^- Decays

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    Using the BK1B\to K_1 form factors evaluated in the perturbative QCD approach, we study semileptonic BK1(1270)l+lB\to K_1(1270)l^+l^- and BK1(1400)l+lB\to K_1(1400)l^+l^- decays, where K1(1270)K_1(1270) and K1(1400)K_1(1400) are mixtures of K1AK_{1A} and K1BK_{1B} which are 3P1^3P_1 and 1P1^1P_1 states, respectively. Using the technique of helicity amplitudes, we express the decay amplitudes in terms of several independent and Lorentz invariant pieces. We study the dilepton invariant mass distributions, branching ratios, polarizations and forward-backward asymmetries of BK1l+l B\to K_1l^+l^- decays. The ambiguity in the sign of the mixing angle will induce much large differences to branching ratios of semileptonic B decays: branching ratios without resonant contributions either have the order of 10610^{-6} or 10810^{-8}. But the polarizations and the forward-backward asymmetries are not sensitive to the mixing angles. We find that the resonant contributions will dramatically change the dilepton invariant mass distributions in the resonant region. We also provide the angular distributions of BK1l+l(Kππ)l+l B\to K_1l^+l^-\to (K\pi\pi)l^+l^- decays.Comment: 14 pages, 6 figures, version appears in PR

    BSB\to S Transition Form Factors in the PQCD approach

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    Under two different scenarios for the light scalar mesons, we investigate the transition form factors of B(Bs)B(B_s) mesons decay into a scalar meson in the perturbative QCD approach. In the large recoiling region, the form factors are dominated by the short-distance dynamics and can be calculated using perturbation theory. We adopt the dipole parametrization to recast the q2q^2 dependence of the form factors. Since the decay constants defined by the scalar current are large, our predictions on the BSB\to S form factors are much larger than the BPB\to P transitions, especially in the second scenario. Contributions from various light-cone distribution amplitudes (LCDAs) are elaborated and we find that the twist-3 LCDAs provide more than a half contributions to the form factors. The two terms of the twist-2 LCDAs give destructive contributions in the first scenario while they give constructive contributions in the second scenario. With the form factors, we also predict the decay width and branching ratios of the semileptonic BSlνˉB\to Sl\bar\nu and BSl+lB\to Sl^+l^- decays. The branching ratios of BSlνˉB\to Sl\bar\nu channels are found to have the order of 10410^{-4} while those of BSl+lB\to Sl^+l^- have the order of 10710^{-7}. These predictions can be tested by the future experiments.Comment: 20 pages, 31 figure

    Nonleptonic charmless decays of BcTP,TVB_c\to TP, TV in the perturbative QCD approach

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    Two-body charmless hadronic BcB_c decays involving a light 13 ⁣P21^3\!P_2-tensor(TT) meson are investigated for the first time within the framework of perturbative QCD(pQCD) at leading order, in which the other meson is the lightest pseudoscalar(PP) or vector(VV) state. The concerned processes can only occur through the pure weak annihilation topology in the standard model. We predict the CP-averaged branching ratios and polarization fractions of those considered decays in Cabibbo-Kobayashi-Maskawa(CKM) favored and suppressed modes. Phenomenologically, several modes-such as the BcK2(1430)KB_c \to K_2^*(1430) K and the CKM-favored BcTVB_c \to TV-have large decay rates of 10610^{-6}, which are expected to be detected at Large Hadron Collider experiments in the near future. Moreover, all of the BcTVB_c \to TV modes are governed by the longitudinal amplitudes in the pQCD calculations and the corresponding fractions vary around 78%78\%-98%98\%. A confirmation of these results could prove the reliability of the pQCD approach used here and further shed some light on the annihilation decay mechanism.Comment: 10 pages, 1 figure, 4 tables, RevTex file; Acknowledgment updated with a grant number, Matching the published versio

    Transition form factors of B decays into p-wave axial-vector mesons in the perturbative QCD approach

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    The Bu,d,sV,AB_{u,d,s}\to V,A form factors are studied in perturbative QCD approach (V,AV,A denote a vector meson and two kinds of p-wave axial-vector mesons: 3P1^3P_1 and 1P1^1P_1 states, respectively.). The form factors are directly studied in the large recoiling region and extrapolated to the whole kinematic region within the dipole parametrization. Adopting decay constants with different signs for the two kinds of axial-vectors, we find that the two kinds of BAB\to A form factors have the same sign. The two strange mesons K1AK_{1A} and K1BK_{1B} mix with each other via the SU(3) symmetry breaking effect. In order to reduce the ambiguities in the mixing angle between K1AK_{1A} and K1BK_{1B}, we propose a model-independent way that utilizes the B decay data. Most of the branching fractions of the semilteptonic BAlνˉlB\to Al\bar \nu_l decays are of the order 10410^{-4}, which still need experimental tests in the on-going and forthcoming experiments.Comment: 22 pages, 7 figure
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