1,316 research outputs found

    Final-State Phases in B→B \to Baryon-Antibaryon Decays

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    The recent observation of the decay \ob \to \Lambda_c^+ \bar p suggests that related decays may soon be visible at e+e−e^+ e^- colliders. It is shown how these decays can shed light on strong final-state phases and amplitudes involving the spectator quark, both of which are normally expected to be small in B decays.Comment: 14 pages, LaTeX, 2 figures, submitted to Phys. Rev. D, references and discussion of helicity amplitudes adde

    Partial waves of baryon-antibaryon in three-body B meson decay

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    The conspicuous threshold enhancement has been observed in the baryon-antibaryon subchannels of many three-body B decay modes. By examining the partial waves of baryon-antibaryon, we first show for B- -->pp-bar K- that the pK- angular correlation rules out dominance of a single pp-bar partial wave for the enhancement, for instance, the resonance hypothesis or the strong final-state interaction in a single channel. The measured pK- angular correlation turns out to be opposite to the naive expectation of the short-distance picture. We study the origin of this reversed angular correlation in the context of the pp-bar partial waves and argue that NN-bar bound states may be the cause of this sign reversal. Dependence of the angular correlation on the pp-bar invariant mass is very important to probe the underlying problem from the experimental side.Comment: 16 pages, 9 figures, the version for journal publicatio

    A Detailed Monte-Carlo Simulation for the Belle TOF System

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    We have developed a detailed Monte Carlo simulation program for the Belle TOF system. Based on GEANT simulation, it takes account of all physics processes in the TOF scintillation counters and readout electronics. The simulation reproduces very well the performance of the Belle TOF system, including the dE/dx response, the time walk effect, the time resolution, and the hit efficiency due to beam background. In this report, we will describe the Belle TOF simulation program in detail.Comment: To be submitted to NI

    Light-Front Approach for Heavy Pentaquark Transitions

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    Assuming the two diquark structure for the pentaquark state as advocated in the Jaffe-Wilczek model, there exist exotic parity-even anti-sextet and parity-odd triplet heavy pentaquark baryons. The theoretical estimate of charmed and bottom pentaquark masses is quite controversial and it is not clear whether the ground-state heavy pentaquark lies above or below the strong-decay threshold. We study the weak transitions of heavy pentaquark states using the light-front quark model. In the heavy quark limit, heavy-to-heavy pentaquark transition form factors can be expressed in terms of three Isgur-Wise functions: two of them are found to be normalized to unity at zero recoil, while the third one is equal to 1/2 at the maximum momentum transfer, in accordance with the prediction of the large-Nc approach or the quark model. Therefore, the light-front model calculations are consistent with the requirement of heavy quark symmetry. Numerical results for form factors and Isgur-Wise functions are presented. Decay rates of the weak decays Theta_b+ to Theta_c0 pi+ (rho+), Theta_c0 to Theta+ pi- (rho-), Sigma'_{5b}+ to Sigma'_{5c}0 pi+ (rho+) and Sigma'_{5c}0 to N_8+ pi- (rho-) with Theta_Q, Sigma'_{5Q} and N_8 being the heavy anti-sextet, heavy triplet and light octet pentaquarks, respectively, are obtained. For weakly decaying Theta_b+ and Theta_c0, the branching ratios of Theta_b+ to Theta_c0 pi+, Theta_c0 to Theta+ pi- are estimated to be at the level of 10^{-3} and a few percents, respectively.Comment: 33 pages, 3 figures, version to be published in Phys. Rev.

    Hadronic B Decays to Charmed Baryons

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    We study exclusive B decays to final states containing a charmed baryon within the pole model framework. Since the strong coupling for ΛbBˉN\Lambda_b\bar B N is larger than that for ÎŁbBˉN\Sigma_b \bar BN, the two-body charmful decay B−→Σc0pˉB^-\to\Sigma_c^0\bar p has a rate larger than Bˉ0→Λc+pˉ\bar B^0\to\Lambda_c^+\bar p as the former proceeds via the Λb\Lambda_b pole while the latter via the ÎŁb\Sigma_b pole. By the same token, the three-body decay Bˉ0→Σc++pˉπ−\bar B^0\to\Sigma_c^{++}\bar p\pi^- receives less baryon-pole contribution than B−→Λc+pˉπ−B^-\to\Lambda_c^+\bar p\pi^-. However, because the important charmed-meson pole diagrams contribute constructively to the former and destructively to the latter, ÎŁc++pˉπ−\Sigma_c^{++}\bar p\pi^- has a rate slightly larger than Λc+pˉπ−\Lambda_c^+\bar p\pi^-. It is found that one quarter of the B−→Λc+pˉπ−B^-\to \Lambda_c^+\bar p\pi^- rate comes from the resonant contributions. We discuss the decays Bˉ0→Σc0pˉπ+\bar B^0\to\Sigma_c^0\bar p\pi^+ and B−→Σc0pˉπ0B^-\to\Sigma_c^0\bar p\pi^0 and stress that they are not color suppressed even though they can only proceed via an internal W emission.Comment: 25 pages, 6 figure

    Study of B -> \rho \pi decays at Belle

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    This paper describes a study of B meson decays to the pseudoscalar-vector final state \rho\pi using 31.9\times 10^6 B\bar{B} events collected with the Belle detector at KEKB. The branching fractions B(B^+ \to \rho^0\pi^+) = (8.0^{+2.3+0.7}_{-2.0-0.7}) \times 10^{-6} and B(B^0 -> \rho^{+-} \pi^{-+}) = (20.8^{+6.0+2.8}_{-6.3-3.1}) \times 10^{-6} are obtained. In addition, a 90% confidence level upper limit of B(B^0 \to \rho^0\pi^0) < 5.3 \times 10^{-6}is reported.Comment: 14 pages, 3 figures, to be submitted to Phys. Lett.

    Charmless Two-body Baryonic B Decays

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    We study charmless two-body baryonic B decays in a diagramatic approach. Relations on decay amplitudes are obtained. In general there are more than one tree and more than one penguin amplitudes. The number of independent amplitudes can be reduced in the large m_B limit. It leads to more predictive results. Some prominent modes for experimental searches are pointed out.Comment: 15 pages, 2 figures. To appear in Phys. Rev.
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