1,011 research outputs found

    The Renormalization Group Evolution of the CKM Matrix

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    We compute the renormalization of the complete CKM matrix in the MSbar scheme and perform a renormalization group analysis of the CKM parameters. The calculation is simplified by studying only the Higgs sector, which for the \beta-function of the CKM matrix is at one loop the same as in the full Standard Model. The renormalization group flow including QCD corrections can be computed analytically using the hierarchy of the CKM parameters and the large mass differences between the quarks. While the evolution of the Cabibbo angle is tiny V_{ub} and V_{cb} increase sizably. We compare our results with the ones in the full Standard Model.Comment: Latex, 31 pages, extensions amsmath, epsfig required The complete paper, including figures, is also available via anonymous ftp at ftp://ttpux2.physik.uni-karlsruhe.de/, or via www at http://www-ttp.physik.uni-karlsruhe.de/cgi-bin/preprints

    Form Factors from Light-Cone Sum Rules with B-Meson Distribution Amplitudes

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    New sum rules for Bπ,KB\to \pi,K and Bρ,KB\to \rho,K^* form factors are derived from the correlation functions expanded near the light-cone in terms of B-meson distribution amplitudes. The contributions of quark-antiquark and quark-antiquark-gluon components in the B meson are taken into account. Models for the B-meson three-particle distribution amplitudes are suggested, based on QCD sum rules in HQET. Employing the new light-cone sum rules we calculate the form factors at small momentum transfers, including SU(3)flSU(3)_{fl} violation effects. The results agree with the predictions of the conventional light-cone sum rules.Comment: 32 pages, 7 figures, the discussion of numerical results extended, two references added, version to be published in Phys.Rev.

    Neutrino-Mass Hierarchies and Non-linear Representation of Lepton-Flavour Symmetry

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    Lepton-flavour symmetry in the Standard Model is broken by small masses for charged leptons and neutrinos. Introducing neutrino masses via dimension-5 operators associated to lepton-number violation at a very high scale, the corresponding coupling matrix may still have entries of order 1, resembling the situation in the quark sector with large top Yukawa coupling. As we have shown recently, in such a situation one may introduce the coupling matrices between lepton and Higgs fields as non-linear representations of lepton-flavour symmetry within an effective-theory framework. This allows us to separate the effects related to the large mass difference observed in atmospheric neutrino oscillations from those related to the solar mass difference. We discuss the cases of normal or inverted hierarchical and almost degenerate neutrino spectrum, give some examples to illustrate minimal lepton-flavour violation in radiative and leptonic decays, and also provide a systematic definition of next-to-minimal lepton-flavour violation within the non-linear framework.Comment: 17 pages, 1 figur

    On the Determination of Vub|V_{ub}| from Inclusive Semileptonic Decay Spectra

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    We propose a model independent method to determine Vub|V_{ub}| from the energy spectrum of the charged lepton in inclusive semileptonic BB decays. The method includes perturbative QCD corrections as well as nonperturbative ones.Comment: LaTeX, 19 pages, 8 figures appended after \end{document} as uu-encoded and compressed .eps files, uses epsf, Technion-PH-94/9, CERN-TH.7308/9

    Comparison of 1/mQ^2 Corrections in Mesons and Baryons

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    We extend our relativistic quark model to the study of the decay Lambda_b -> Lambda_c ell nu and verify that the model satisfies the heavy-quark symmetry constraints at order 1/mQ^2. We isolate a strong dependence on a parameter which measures the relative distortion in the light-quark wave functions of the Lambda_b and Lambda_c. This parameter and the 1/mQ^2 corrections turn out to be small. The dependence on a corresponding parameter in the meson case leads to large 1/mQ^2 corrections.Comment: 9 pages, LaTeX, 3 self-contained LaTeX figures in separate fil

    Higher Order 1/m1/m Corrections at Zero Recoil

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    The general structure of the 1/m1/m corrections at zero recoil is studied. The relevant matrix elements are forward matrix elements of local higher dimensional operators and their time ordered products with higher order terms from the Lagrangian. These matrix elements may be classified in a simple way and the analysis at the non recoil point for the form factor of heavy quark currents simplifies drastically. The second order recoil corrections to the form factor hA1h_{A1} of the axial vector current, relevant for the Vcb|V_{cb}| determination from BDB \to D^* decays, are estimated to be 5%<hA11<0-5\% < h_{A1} - 1 < 0.Comment: LaTeX, 25 pages, one figure, appended after \end{document} as uu-encoded and compressed eps file, uses epsf, CERN-TH.7162/9

    Semileptonic charm decays D \to \pi l \nu_{\l} and DKlνlD \to K l \nu_l from QCD Light-Cone Sum Rules

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    We present a new calculation of the DπD\to\pi and DKD \to K form factors from QCD light-cone sum rules. The MS\overline{MS} scheme for the cc-quark mass is used and the input parameters are updated. The results are fDπ+(0)=0.670.07+0.10f^+_{D\pi}(0)= 0.67^{+0.10}_{-0.07}, fDK+(0)=0.750.08+0.11f^+_{DK}(0)=0.75^{+0.11}_{-0.08} and fDπ+(0)/fDK+(0)=0.88±0.05f^+_{D\pi}(0)/f^+_{DK}(0)=0.88 \pm 0.05. Combining the calculated form factors with the latest CLEO data, we obtain Vcd=0.225±0.005±0.0030.012+0.016|V_{cd}|=0.225\pm 0.005 \pm 0.003 ^{+0.016}_{-0.012} and Vcd/Vcs=0.236±0.006±0.003±0.013|V_{cd}|/|V_{cs}|= 0.236\pm 0.006\pm 0.003\pm 0.013 where the first and second errors are of experimental origin and the third error is due to the estimated uncertainties of our calculation. We also evaluate the form factors fDπf^-_{D\pi} and fDKf^-_{DK} and predict the slope parameters at q2=0q^2=0. Furthermore, calculating the form factors from the sum rules at q2<0q^2<0, we fit them to various parameterizations. After analytic continuation, the shape of the Dπ,KD\to \pi,K form factors in the whole semileptonic region is reproduced, in a good agreement with experiment.Comment: 34 pages, 5 figure
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