269 research outputs found

    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.

    Phenomenological Analysis of B->PP Decays with QCD Factorization

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    In this paper, we study nonleptonic charmless B decays to two light pseudoscalar mesons within the frame of QCD factorization, including the contributions from the chirally enhanced power corrections and weak annihilation. Predictions for the CP-averaged branching ratios and CP-violating asymmetries are given. Within the reasonable range of the parameters, we find that our predictions for the branching ratios of B -> PP are consistent with the present experimental data. But because of the logarithmic divergences at the endpoints in the hard spectator scatterings and weak annihilation, there are still large uncertainties in these predictions.Comment: 34 pages, 5 figures. to appear in PR

    Low-Mass Baryon-Antibaryon Enhancements in B Decays

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    The nature of low-mass baryon-antibaryon enhancements seen in B decays is explored. Three possibilities include (i) states near threshold as found in a model by Nambu and Jona-Lasinio, (ii) isoscalar states with JPC=0±+J^{PC} = 0^{\pm +} coupled to a pair of gluons, and (iii) low-mass enhancements favored by the fragmentation process. Ways of distinguishing these mechanisms using angular distributions and flavor symmetry are proposed.Comment: 8 pages, LaTeX, no figures, to be submitted to Phys. Rev. D. One reference adde

    Semi-inclusive B Decays and Direct CP Violation in QCD Factorization

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    We have systematically investigated the semi-inclusive B decays B->MX, which are manifestations of the quark decay b->Mq, within the framework of QCD-improved factorization. These decays are theoretically clean and have distinctive experimental signatures. We focus on a class of these that do not require any form factor information and therefore may be especially suitable for extracting information on the angles α\alpha and γ\gamma of the unitarity triangle. The nonfactorizable effects, such as vertex-type and penguin-type corrections to the two-body b decay and hard spectator corrections to the 3-body decay are calculable in the heavy quark limit. QCD factorization is applicable when the emitted meson is a light meson or a charmonium. We discuss the issue of the CPT constraint on partial rate asymmetries. The strong phase coming from final-state rescattering due to hard gluon exchange between the final states can induce large rate asymmetries for tree-dominated color-suppressed modes (π0,ρ0,ω)Xsˉ(\pi^0,\rho^0,\omega)X_{\bar s}. The nonfactorizable hard spectator interactions in the 3-body decay, though phase-space suppressed, are extremely important for the tree-dominated modes (π0,ρ0,ω)Xsˉ,ϕX(\pi^0,\rho^0,\omega)X_{\bar s}, \phi X, JXs,JXJ X_s,J X and the penguin-dominated mode ωXssˉ\omega X_{s\bar s}. In fact, they are dominated by the hard spectator corrections. Our result for B(BJ/ψXs){\cal B} (B\to J/\psi X_s) is in agreement with experiment. The semi-inclusive decay modes: Bs0(π0,ρ0,ω)XsˉB^0_s\to (\pi^0,\rho^0,\omega)X_{\bar s}, ρ0Xssˉ\rho^0X_{s\bar s}, B0(KX,KX)B^0\to(K^-X,K^{*-}X) and B(K0Xs,K0Xs)B^-\to (K^0X_s,K^{*0}X_s) are the most promising ones in searching for direct CP violation. In fact, they have branching ratios of order 10610410^{-6}-10^{-4} and CP rate asymmetries of order (1040)(10-40)%.Comment: 28 page

    Charmless BˉsVV\bar{B}_s\to VV Decays in QCD Factorization

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    The two body charmless decays of BsB_s meson to light vector mesons are analyzed within the framework of QCD factorization. This approach implies that the nonfactorizable corrections to different helicity amplitudes are not the same. The effective parameters aiha_i^h for helicity h=0,+,h=0,+,- states receive different nonfactorizable contributions and hence are helicity dependent, contrary to naive factorization approach where aiha_i^h are universal and polarization independent. The branching ratios for BˉsVV\bar{B}_s\to VV decays are calculated and we find that branching ratios of some channels are of order 10510^{-5}, which are measurable at future experiments. The transverse to total decay rate ΓT/Γ\Gamma_T/\Gamma is also evaluated and found to be very small for most decay modes, so, in charmless BˉsVV\bar{B}_s\to VV decays, both light vector mesons tend to have zero helicity.Comment: 16pages. Typos and mistakes fixed. Numerical results change

    Charmless hadronic decays BPP,PV,VVB \to PP, PV, VV and new physics effects in the general two-Higgs doublet models

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    Based on the low-energy effective Hamiltonian with the generalized factorization, we calculate the new physics contributions to the branching ratios of the two-body charmless hadronic decays of BuB_u and BdB_d mesons induced by the new gluonic and electroweak charged-Higgs penguin diagrams in the general two-Higgs doublet models (models I, II and III). Within the considered parameter space, we find that: (a) the new physics effects from new gluonic penguin diagrams strongly dominate over those from the new γ\gamma- and Z0Z^0- penguin diagrams; (b) in models I and II, new physics contributions to most studied B meson decay channels are rather small in size: from -15% to 20%; (c) in model III, however, the new physics enhancements to the penguin-dominated decay modes can be significant, (30200)\sim (30 -200)%, and therefore are measurable in forthcoming high precision B experiments; (d) the new physics enhancements to ratios {\cal B}(B \to K \etap) are significant in model III, (3570)\sim (35 -70)%, and hence provide a simple and plausible new physics interpretation for the observed unexpectedly large B \to K \etap decay rates; (e) the theoretical predictions for B(BK+π){\cal B}(B \to K^+ \pi) and B(BK0π+){\cal B}(B \to K^0 \pi^+) in model III are still consistent with the data within 2σ2\sigma errors; (f) the significant new physics enhancements to the branching ratios of BK0π0,Kη,K+π,K+ϕ,K0ω,K+ϕB \to K^0 \pi^0, K^* \eta, K^{*+} \pi^-, K^+ \phi, K^{*0} \omega, K^{*+} \phi and K0ϕK^{*0} \phi decays are helpful to improve the agreement between the data and the theoretical predictions; (g) the theoretical predictions of B(BPP,PV,VV){\cal B}(B \to PP, PV, VV) in the 2HDM's are generally consistent with experimental measurements and upper limits (9090% C.L.)Comment: 55 pages, Latex file, 17 PS and EPS figures. With minor corrections, final version to be published in Phys.Rev. D. Repot-no: PKU-TH-2000-4

    The transition form factors for semi-leptonic weak decays of J/ψJ/\psi in QCD sum rules

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    Within the Standard Model, we investigate the semi-leptonic weak decays of J/ψJ/\psi. The various form factors of J/ψJ/\psi transiting to a single charmed meson (D(d,s)()D^{(*)}_{(d,s)}) are studied in the framework of the QCD sum rules. These form factors fully determine the rates of the weak semi-leptonic decays of J/ψJ/\psi and provide valuable information about the non-perturbative QCD effects. Our results indicate that the decay rate of the semi-leptonic weak decay mode J/ψDs()+e++νeJ/\psi \to D^{(*)-}_{s}+e^{+}+\nu_{e} is at order of 101010^{-10}.Comment: 28 pages, 6 figures, revised version to be published in Eur.Phys.J.

    Pair production of the heavy leptons in future high energy linear e^{+}e^{-} colliders

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    The littlest Higgs model with T-parity predicts the existence of the T-odd particles, which can only be produced in pair. We consider pair production of the T-odd leptons in future high energy linear e+ee^{+}e^{-} collider (ILCILC). Our numerical results show that, as long as the T-odd leptons are not too heavy, they can be copiously produced and their possible signals might be detected via the processes e+eLˉiLje^{+}e^{-}\to \bar{L}_{i}L_{j} in future ILCILC experiments.Comment: Discussions added, typos and references correcte

    Charming penguin contributions to charmless B decays into two pseudoscalar mesons

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    We present estimates of the charming penguin contribution to B => K pi, pi pi,K eta, K eta' decays due to intermediate charmed meson states. We find that this contribution is indeed significant for B => K pi decays, and its inclusion, together with the tree and penguin terms, produces large branching ratios in agreement with data, though the analysis is affected by large theoretical uncertainties. On the other hand, for B => pi pi, K eta, K eta' decays, the effect of the charming penguin contribution is more modest. We also compute CP asymmetries for B => K pi, pi pi decays and we obtain rather large results.Comment: 12 pages, 4 figures, LaTeX2e with epsfig. Minor changes in the text, this version will appear in Phys. Rev.

    Pulsar Timing at Urumqi Astronomical Observatory: Observing System and Results

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    A pulsar timing system has been operating in the 18-cm band at the Urumqi Astronomical Observatory 25-m telescope since mid-1999. Frequency resolution allowing dedispersion of the pulsar signals is provided by a 2X128X2.5 MHz filterbank/digitiser system. Observations of 74 pulsars over more than 12 months have resulted in updated pulsar periods and period derivatives, as well as improved positions. Comparison with previous measurements showed that the changes in period and period derivative tend to have the same sign and to be correlated in amplitude. A model based on unseen glitches gives a good explanation of the observed changes, suggesting that long-term fluctuations in period and period derivatives are dominated by glitches. In 2000 July, we detected a glitch of relative amplitude Delta_nu/nu~24X1e-9 in the Crab pulsar. The post-glitch decay appears similar to other large Crab glitches.Comment: 11 pages, 9 figures, 4 tables, accepted by MNRA
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