2,285 research outputs found

    Heavy-to-Light Meson Transitions in QCD

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    I discuss QCD sum rules determinations of the form factors governing the decay Bπ(ρ)νB \to \pi (\rho) \ell \nu. For some of these form factors the computed dependence on the momentum transferred does not agree with the expectation from the nearest pole dominance hypothesis. Relations are observed among the form factors, that seem to be compatible with equations recently derived by B.Stech. The measurement of a number of color suppressed nonleptonic B decay rates could shed light on the accuracy of the calculation of these form factors and on the factorization approximation.Comment: LaTex, 7 pages, 2 figures (files included). Talk given at the 6th International Symposium on Heavy Flavours, Pisa, 6-10 June 199

    Radiative transitions of DsJ(2317)D^*_{sJ}(2317) and DsJ(2460)D_{sJ}(2460)

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    We study radiative decays of DsJ(2317)D^*_{sJ}(2317) and DsJ(2460)D_{sJ}(2460) using light-cone QCD sum rules. In particular, we consider the decay modes DsJ(2317)DsγD^*_{sJ}(2317)\to D_s^* \gamma and DsJ(2460)Ds()γ,DsJ(2317)γD_{sJ}(2460)\to D_s^{(*)} \gamma, D^*_{sJ}(2317) \gamma and evaluate the hadronic parameters in the transition amplitudes analyzing correlation functions of scalar, pseudoscalar, vector and axial-vector quark currents. In the case of DsJ(2317)DsγD^*_{sJ}(2317)\to D_s^* \gamma we also consider determinations based on two different correlation functions in HQET. The decay widths turn out to be different than previous estimates obtained by other methods; the results favour the interpretation of DsJ(2317)D^*_{sJ}(2317) and DsJ(2460)D_{sJ}(2460) as ordinary cˉs\bar c s mesons.Comment: RevTex, 23 pages, 9 eps figure

    Properties of the DsJ states

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    Recent measurements involving the newly discovered D_sJ particles are reported. The results of D_sJ production and decay branching fraction measurements are shown. Possible spin-parity and quark content assignments of D_sJ mesons are discussed. The results are based on a large data sample recorded by the Belle detector at the KEKB e^+ e^- collider.Comment: 4 pages, 3 figures, proceedings to the talk given on behalf of the Belle Collaboration at the First Meeting of the APS Topical Group on Hadron Physic

    Chiral symmetry restoration and deconfinement in QCD at finite temperature

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    The light-quark correlator in the axial-vector channel is used, in conjunction with finite energy QCD sum rules at finite temperature, in order to (a) establish a relation between chiral-symmetry restoration and deconfinement, and (b) determine the temperature behavior of the a1(1260)a_1(1260) width and coupling. Results indicate that deconfinement takes place at a slightly lower temperature than chiral-symmetry restoration, although this difference is not significant given the accuracy of the method. The behaviour of the a1(1260)a_1(1260) parameters is consistent with quark-gluon deconfinement, as the width grows and the coupling decreases with increasing temperature

    The effects of enhanced Z penguins on lepton polarizations in BXs+B \to X_s \ell^+ \ell^-

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    The sensitivity of the BπKB \to \pi K mode to electroweak penguins and the recent experimental data for the BππB \to \pi \pi, πK\pi K modes has given rise to what is known as the ``BπKB \to \pi K puzzle''. Recently it has been observed that this {\sl puzzle} can be resolved by considering the new physics which can enter via Z0Z^0 penguins. In this note we analyze the effect of this enhanced Z0Z^0 penguins on the lepton polarization asymmetries of bs+b \to s \ell^+ \ell^-.Comment: Published versio

    Rare Radiative BcDs1(2460)γB_{c}\rightarrow D_{s1}(2460)\gamma Transition in QCD

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    We investigate the radiative BcDs1γB_{c} \to D_{s1} \gamma transition in the framework of QCD sum rules. In particular, we calculate the transition form factors responsible for this decay in both weak annihilation and electromagnetic penguin channels using the quark condensate, mixed and two-gluon condensate diagrams as well as propagation of the soft quark in the electromagnetic field as non-perturbative corrections. These form factors are then used to estimate the branching ratios of the channels under consideration. The total branching ratio of the BcDs1γB_{c} \to D_{s1} \gamma transition is obtained to be in order of 10510^{-5}, and the dominant contribution comes from the weak annihilation channel.Comment: 24 Pages and 3 Figure

    J/psi couplings to charmed resonances and to pi

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    We present an evaluation of the strong couplings JD^(*)D^(*) and JD^(*)D^(*)pi by an effective field theory of quarks and mesons. These couplings are necessary to calculate pi+J/psi --> D^(*)+barD^(*) cross sections, an important background to the J/psi suppression signal in the quark-gluon plasma. We write down the general effective lagrangian and compute the relevant couplings in the soft pion limit and beyond.Comment: 11 pages, 4 figures, 2 reference added and minor comments, style changed to RevTe

    Cusps in K_L --> 3 pi decays

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    The pion mass difference generates a pronounced cusp in K --> 3 pi decays, the strength of which is related to the pi pi S-wave scattering lengths. We apply an effective field theory framework developed earlier to evaluate the amplitudes for K_L --> 3 pi decays in a systematic manner, where the strictures imposed by analyticity and unitarity are respected automatically. The amplitudes for the decay eta --> 3 pi are also given.Comment: 15 pages, 3 figures, uses Elsevier styl
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