665 research outputs found

    Study of pure annihilation type decays B→Ds∗KB \to D_s^{*} K

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    In this work, we calculate the rare decays B0→Ds∗−K+B^0 \to D_s^{*-} K^+ and B+→Ds∗+Kˉ0B^+ \to D_s^{*+} \bar{K}^0 in perturbative QCD approach with Sudakov resummation. We give the branching ratio of 10−510^{-5} for B0→Ds∗−K+B^0 \to D_s^{*-}K^+, which will be tested soon in BB factories. The decay B+→Ds∗+Kˉ0B^+ \to D_s^{*+} \bar{K}^0 has a very small branching ratio at O(10−8){\cal O}(10^{-8}), due to the suppression from CKM matrix elements ∣Vub∗Vcd∣|V_{ub}^* V_{cd}|. It may be sensitive to new physics contributions.Comment: 14 pages, 1 figur

    Perturbative QCD analysis of B→ϕK∗B \to \phi K^* decays

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    We study the first observed charmless B→VVB\to VV modes, the B→ϕK∗B\to\phi K^* decays, in perturbative QCD formalism. The obtained branching ratios B(B→ϕK∗)∌15×10−6B(B\to\phi K^*)\sim 15 \times 10^{-6} are larger than ∌9×10−6\sim 9\times 10^{-6} from QCD factorization. The comparison of the predicted magnitudes and phases of the different helicity amplitudes, and branching ratios with experimental data can test the power counting rules, the evaluation of annihilation contributions, and the mechanism of dynamical penguin enhancement in perturbative QCD, respectively.Comment: 14 pages, 2 tables, brief disscussion on hard sacle added, version to appear in PR

    Molecular mechanisms underlying anti-tumor promoting activities of heat-processed Panax ginseng C.A. Meyer.

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    Recently, there have been considerable efforts to search for naturally occurring substances that can inhibit, reverse, or retard the multi-stage carcinogenesis. A wide array of phenolic substances derived from edible and medicinal plants have been reported to possess anticarcinogenic and antimutagenic activities and in many cases, the chemopreventive activities of phytochemicals are associated with their anti-inflammatory and/or antioxidative properties. Panax ginseng C.A. Meyer cultivated in Korea has been widely used in traditional herbal medicine for the treatment of various diseases. Certain fractions or purified ingredients of ginseng have been shown to exert anticarcinogenic and antimutagenic activities. Our previous studies have revealed that the methanol extract of heat-processed Panax ginseng C.A. Meyer attenuates the lipid peroxidation in rat brain homogenates and is also capable of scavenging superoxide generated by xanthine- xanthine oxidase or by 12-O-tetradecanoylphorbol-13-acetate (TPA) in differentiated human promyelocytic leukemia (HL-60) cells. Topical application of the same extract onto shaven backs of female ICR mice also suppressed TPA-induced skin tumor promotion. Likewise, topical application of ginsenoside Rg3, one of the constituents of heat-treated ginseng, significantly inhibited TPA-induced mouse epidermal ornithine decarboxylase activity and skin tumor promotion. Expression of cyclooxygenase-2 (COX-2) in TPA-stimulated mouse skin was markedly suppressed by Rg3 pretreatment. In addition, Rg3 inhibited TPA-stimulated activation of NF-kappaB and extracellular-regulated protein kinase (ERK), one of the mitogen-activated protein (MAP) kinase in mouse skin and also in cultured human breast epithelial cells (MCF-10A)

    B meson light-cone wavefunctions in the heavy quark limit

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    We present a systematic study of the B meson light-cone wavefunctions in QCD in the heavy-quark limit. We construct model-independent formulae for the light-cone wavefunctions in terms of independent dynamical degrees of freedom, which exactly satisfy the QCD equations of motion and constraints from heavy-quark symmetry. The results demonstrate novel behaviors of longitudinal as well as transverse momentum distribution in the B mesons.Comment: 5 pages LaTeX, 1 style file. Talk presented at RADCOR/Loops and Legs 2002, Kloster Banz, Germany, September 8-13, 200

    Study of color suppressed modes B0→Dˉ(∗)0η(â€Č)B^0 \to \bar D^{(*)0} \eta^{(\prime)}

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    The color suppressed modes B0→Dˉ(∗)0η(â€Č)B^0 \to \bar D^{(*)0} \eta^{(\prime)} are analyzed in perturbative QCD approach. We find that the dominant contribution is from the non-factorizable diagrams. The branching ratios calculated in our approach for B0→Dˉ(∗)0ηB^0 \to \bar D^{(*)0} \eta agree with current experiments. By neglecting the gluonic contribution, we predict the branching ratios of B0→Dˉ(∗)0ηâ€ČB^0 \to \bar D^{(*)0} \eta' are at the comparable size of B0→Dˉ(∗)0π0B^0 \to \bar D^{(*)0} \pi^0, but smaller than that of B0→Dˉ(∗)0ηB^0 \to \bar D^{(*)0} \eta .Comment: revtex, 5 pages, axodraw.st

    kTk_T factorization of exclusive processes

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    We prove kTk_T factorization theorem in perturbative QCD (PQCD) for exclusive processes by considering Ï€Îłâˆ—â†’Îł(π)\pi\gamma^*\to \gamma(\pi) and B→γ(π)lΜˉB\to\gamma(\pi) l\bar\nu. The relevant form factors are expressed as the convolution of hard amplitudes with two-parton meson wave functions in the impact parameter bb space, bb being conjugate to the parton transverse momenta kTk_T. The point is that on-shell valence partons carry longitudinal momenta initially, and acquire kTk_T through collinear gluon exchanges. The bb-dependent two-parton wave functions with an appropriate path for the Wilson links are gauge-invariant. The hard amplitudes, defined as the difference between the parton-level diagrams of on-shell external particles and their collinear approximation, are also gauge-invariant. We compare the predictions for two-body nonleptonic BB meson decays derived from kTk_T factorization (the PQCD approach) and from collinear factorization (the QCD factorization approach).Comment: 11 pages, REVTEX, 5 figure

    Threshold resummation for exclusive B meson decays

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    We argue that double logarithmic corrections αsln⁥2x\alpha_s\ln^2 x need to be resumed in perturbative QCD factorization theorem for exclusive BB meson decays, when the end-point region with a momentum fraction x→0x\to 0 is important. These double logarithms, being of the collinear origin, are absorbed into a quark jet function, which is defined by a matrix element of a quark field attached by a Wilson line. The factorization of the jet function from the decay B→γlΜˉB\to\gamma l\bar\nu is proved to all orders. Threshold resummation for the jet function leads to a universal, {\it i.e.}, process-independent, Sudakov factor, whose qualitative behavior is analyzed and found to smear the end-point singularities in heavy-to-light transition form factors.Comment: 10 pages, more details are include

    Possible Large Direct CP Violations in Charmless B-Decays

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    We discuss the perturbative QCD approach for the exclusive two body B-meson decays to light mesons. We briefly review its ingredients and some important theoretical issues on factorization approach. We show numerical results which are compatible with present experimantal data for the charmless B-meson decays. Specailly we predict the possibility of large direct CP violation effects in B0→π+π−B^0 \to \pi^{+}\pi^{-} (23±7(23\pm7 %) and B0→K+π−B^0\to K^{+}\pi^{-} (−17±5(-17\pm5%). In the last section we investigate two methods to determine the weak phases ϕ2\phi_2 and ϕ3\phi_3 from B→ππ,KπB \to \pi\pi,K\pi processes. We obtain bounds on ϕ2\phi_2 and ϕ3\phi_3 from present experimental measurements.Comment: 18 pages, latex, 8 figures and 8 tables, typos corrected and added more tables and references. Presented at the 3rd workshop on Higher Luminosity B Factory, 6-7 August 2002, Kanagawa, Japan; Submitted to Phys. Rev.

    QCD factorization for B -> PP

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    In this work, we give a detailed discussion for QCD factorization involved the complete chirally enhanced power corrections for B decays to two light pseudoscalar mesons, and present some detailed calculations of radiative corrections at the order of alpha_s. We point out that the infrared finiteness of the vertex corrections in the chirally enhanced power corrections requires twist-3 light-cone distribution amplitudes (LCDAs) of the light pseudoscalar symmetric. However, even in the symmetric condition, there is also logarithmic divergence from the endpoints of the twist-3 LCDAs in the hard spectator scattering. We point out that the decay amplitudes of B --> PP predicted by QCD factorization are really free of the renormalization scale dependence, at least at the order of alpha_s. At last, we briefly compare the QCD factorization with the generalized factorization and PQCD method.Comment: 31 pages, 3 eps figure

    Perturbative QCD factorization of Ï€Îłâˆ—â†’Îł(π)\pi \gamma^*\to \gamma(\pi) and B→γ(π)lΜˉB\to \gamma(\pi)l\bar \nu

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    We prove factorization theorem for the processes Ï€Îłâˆ—â†’Îł\pi\gamma^*\to\gamma and Ï€Îłâˆ—â†’Ï€\pi\gamma^*\to\pi to leading twist in the covariant gauge by means of the Ward identity. Soft divergences cancel and collinear divergences are grouped into a pion wave function defined by a nonlocal matrix element. The gauge invariance and universality of the pion wave function are confirmed. The proof is then extended to the exclusive BB meson decays B→γlΜˉB\to\gamma l\bar\nu and B→πlΜˉB\to\pi l\bar\nu in the heavy quark limit. It is shown that a light-cone BB meson wave function, though absorbing soft dynamics, can be defined in an appropriate frame. Factorization of the B→πlΜˉB\to\pi l\bar\nu decay in kTk_T space, kTk_T being parton transverse momenta, is briefly discussed. We comment on the extraction of the leading-twist pion wave function from experimental data.Comment: 21 pages in Latex file, version to appear in Phys. Rev.
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