140 research outputs found

    b -> d Penguins: CP Violation, General Lower Bounds on the Branching Ratios and Standard Model Tests

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    With the wealth of new data from the B-factories, b -> d penguin decays become available for study, in addition to their b -> s counterparts that have proven an indespensable tool for the exploration of new-physics effects in flavour physics. A prominent example of the b -> d penguin transitions is Bˉd0K0Kˉ0\bar B^0_d \to K^0 \bar K^0. We show that this decay can be charaterized in the Standard Model by a surface in the observable space of the direct and mixing-induced CP asymmetries and the branching ratio. The form of this surface, which is theoretically clean, implies a lower bound for the branching ratio that has recently been confirmed experimentally. If future measurements of the CP asymmetries yield a point away from the SM surface, this would be an interesting signal of new physics. We point out that the hadronic parameters in Bˉd0K0Kˉ0\bar B^0_d \to K^0 \bar K^0 that parameterize the position on the SM surface are related to hadronic parameters in the B -> pi K system. The fact that the branching ratio of Bˉd0K0Kˉ0\bar B^0_d \to K^0 \bar K^0 is very close to its lower bound yields interesting implications for B -> pi K even without knowledge of the CP asymmetries of Bˉd0K0Kˉ0\bar B^0_d \to K^0 \bar K^0. The mechanism that produces the lower bound for Bˉd0K0Kˉ0\bar B^0_d \to K^0 \bar K^0 is actually much more general; we derive lower bounds for various other b -> d penguin-induced processes, including B -> rho gamma and B±K()±K()B^\pm \to K^{(\ast)\pm} K^{(\ast)}. Some of these theoretical lower bounds are very close to the current experimental upper bounds.Comment: 4 pages, 2 figures. Contribution to the proceedings of EPS-HEP200

    Comparing the QCD potential in Perturbative QCD and Lattice QCD at large distances

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    We compare the perturbatively calculated QCD potential to that obtained from lattice calculations in the theory without light quark flavours. We examine E_tot(r) = 2 m_pole + V_QCD(r) by re-expressing it in the MSbar mass m = m^MSbar(m^MSbar) and by choosing specific prescriptions for fixing the scale mu (dependent on r and m). By adjusting m so as to maximise the range of convergence, we show that perturbative and lattice calculations agree up to 3*r_0 ~ 7.5 GeV^-1 (r_0 is the Sommer scale) within the uncertainty of order Lambda^3 r^2.Comment: Version to appear in Eur.J.Phys; 16 pages, 7 figure

    Comparing B -> X_u l nu_l to B -> X_s gamma

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    We suggest a method to determine V_ub / V_ts through a comparison of B -> X_u l nu_l and B -> X_s gamma. The relevant quantity is the spectrum of the light-cone component of the final state hadronic momentum, which in B -> X_s gamma is the photon energy while in B -> X_u l nu_l this requires a measurement of both hadronic energy and hadronic invariant mass. The non-perturbative contributions at tree level to these distributions are identical and may be cancelled by taking the ratio of the spectra. Radiative corrections to this comparison are discussed to order alpha_s and are combined with the non-perturbative contributions.Comment: 16 pages, 4 figures. One Paragraph added, Version published in Phys.Rev. D6
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