161 research outputs found

    Determining the Weak Phase γ\gamma From Charged BB Decays

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    A quadrangle relation is shown to be satisfied by the amplitudes for B+π0K+, π+K0, ηK+B^+ \to \pi^0 K^+,~\pi^+ K^0,~\eta K^+, and ηK+\eta' K^+. By comparison with the corresponding relation satisfied by BB^- decay amplitudes, it is shown that the relative phases of all the amplitudes can be determined up to discrete ambiguities. Making use of an SU(3) relation between amplitudes contributing to the above decays and those contributing to B±π±π0B^{\pm} \to \pi^{\pm} \pi^0, it is then shown that one can determine the weak phase γArg(VubVcb/VusVcs)\gamma \equiv {\rm Arg} (V_{ub}^* V_{cb}/V_{us}^* V_{cs}), where VV is the Cabibbo-Kobayashi-Maskawa matrix describing the charge-changing weak interactions between the quarks (u,c,t)(u,c,t) and (d,s,b)(d,s,b).Comment: 16 pages, latex, 7 uuencoded figure

    Annihilation, Rescattering, and CP Asymmetries in B Meson Decays

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    A number of BB meson decays may proceed only through participation of the spectator quark, whether through amplitudes proportional to fB/mBf_B/m_B or via rescattering from other less-suppressed amplitudes. An expected hierarchy of amplitudes in the absence of rescattering will be violated by rescattering corrections. Such violations could point the way toward channels in which final-state interactions could be important. Cases in which final state phases can lead to large CP asymmetries are pointed out.Comment: 9 page

    Broken SU(3) Symmetry in Two-Body B Decays

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    The decays of BB mesons to two-body hadronic final states are analyzed within the context of broken flavor SU(3) symmetry, extending a previous analysis involving pairs of light pseudoscalars to decays involving one or two charmed quarks in the final state. A systematic program is described for learning information {}from decay rates regarding (i) SU(3)-violating contributions, (ii) the magnitude of exchange and annihilation diagrams (effects involving the spectator quark), and (iii) strong final-state interactions. The implication of SU(3)-breaking effects for the extraction of weak phases is also examined. The present status of data on these questions is reviewed and suggestions for further experimental study are made.Comment: 38 pages, 8 figures, LaTeX file. The full postscript manuscript is available by anon ftp at ftp://lpsvsh.lps.umontreal.ca/theorie/hep-ph/SU3break.ps (a VAX so use the format theorie.hep-ph if you change by more than one directory at a time

    ELECTROWEAK PENGUINS AND TWO-BODY B DECAYS

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    We discuss the role of electroweak penguins in BB decays to two light pseudoscalar mesons. We confirm that the extraction of the weak phase α\alpha through the isospin analysis involving BππB\to\pi\pi decays is largely unaffected by such operators. However, the methods proposed to obtain weak and strong phases by relating BππB\to\pi\pi, BπKB\to\pi K and BKKB\to KK decays through flavor SU(3) will be invalidated if electroweak penguins are large. We show that, although the introduction of electroweak penguin contributions introduces no new amplitudes of flavor SU(3), there are a number of ways to experimentally measure the size of such effects. Finally, using SU(3) amplitude relations we present a new way of measuring the weak angle γ\gamma which holds even in the presence of electroweak penguins.Comment: 18 pages, 3 figures, LaTeX file. The full postscript manuscript is available by anonymous ftp at ftp://lpsvsh.lps.umontreal.ca/theorie/hep-ph/EWpenguins.ps (a VAX so use the format theorie.hep-ph if you change by more than one directory at a time

    New Physics in CP Asymmetries and Rare B Decays

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    We review and update the effects of physics beyond the standard model on CP asymmetries in B decays. These asymmetries can be significantly altered if there are important new-physics contributions to \bqbqbar mixing. This same new physics will therefore also contribute to rare, flavor-changing B decays. Through a study of such decays, we show that it is possible to partially distinguish the different models of new physics.Comment: 42 pages, plain TeX (macros included), 1 figure (included). A few sentences added, references updated. Present manuscript is now identical to the version accepted for publication in Phys. Rev.

    Mixing-induced CP Asymmetries in Radiative B Decays in and beyond the Standard Model

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    In the Standard Model (SM) the photon in radiative Bˉ0\bar B^0 and Bˉs\bar B_s decays is predominantly left-handed. Thus, mixing induced CP asymmetries in bsγb\to s\gamma and bdγb\to d\gamma are suppressed by ms/mbm_s/m_b and md/mbm_d/m_b, respectively, and are very small. In many extensions of the SM, such as the left-right symmetric model (LRSM), SU(2)xU(1) models with exotic fermions and SUSY, the amplitude of right-handed photons grows proportional to the virtual heavy fermion mass, which can lead to large asymmetries. As an example, in the LRSM, asymmetries larger than 50% are possible even when radiative decay rate measurements agree with SM predictions.Comment: 11 pages + 1 figure.p

    Constraints on a Massive Dirac Neutrino Model

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    We examine constraints on a simple neutrino model in which there are three massless and three massive Dirac neutrinos and in which the left handed neutrinos are linear combinations of doublet and singlet neutrinos. We examine constraints from direct decays into heavy neutrinos, indirect effects on electroweak parameters, and flavor changing processes. We combine these constraints to examine the allowed mass range for the heavy neutrinos of each of the three generations.Comment: latex, 29 pages, 7 figures (not included), MIT-CTP-221

    Weak Hyperon Decays: Quark Sea and SU(3) Symmetry Breaking

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    An explanation of the difference in the values of the apparent f/df/d ratios for the S- and P- wave amplitudes of nonleptonic hyperon decays is proposed. The argument is formulated in the framework of the standard pole model with (56,0+)(56,0^{+}) ground-state and (70,1)(70,1^{-}) excited baryons as intermediate states for the P- and S- waves respectively. Under the assumption that the dominant part of the deviation of (f/d)Pwave(f/d)_{P-wave} from 1-1 is due to large quark sea effects, SU(3)SU(3) symmetry breaking in energy denominators is shown to lead to a prediction for (f/d)Swave(f/d)_{S-wave} which is in excellent agreement with experiment. This corroborates our previous unitarity calculations which indicated that the matrix elements of the parity conserving weak Hamiltonian between the ground-state baryons are characterized by f0/d01.6f_{0}/d_{0} \approx -1.6 or more. A brief discussion of the problem of the relative size of S- and P- wave amplitudes is given. Finally, implications for weak radiative hyperon decays are also discussed.Comment: 26 pages, LATEX, 1647/PH IFJ Krako

    Electroweak and Strong Penguins in B^{\pm, 0}\to \pi\pi, \pi K and KK Decays

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    We calculate CP-violating rates and asymmetry parameters in charged and neutral Bππ,πKB\to \pi\pi, \pi K and KˉK\bar K K decays arising from the interference of tree and penguin (strong and electroweak) amplitudes with different strong and CKM phases. The perturbative strong (electroweak) phases develop at order αs\alpha_s (αem\alpha_{em}) from absorptive parts of one-loop matrix elements of the next-to-leading (leading) logarithm corrected effective Hamiltonian. The BSW model is used to estimate the hadronic matrix elements. Based on this model, we find that the effect of strong phases and penguins is substantial in most channels, drastic in many. However, a measurement of the time dependence parameter aϵ+ϵa_{\epsilon+\epsilon'} in the π+π\pi^+\pi^- channel is only influenced at the 20\% level by the complication of the penguins. Recent flavor sum rules developed for B0,±ππ,πK,KKˉB^{0,\pm} \rightarrow \pi\pi, \pi K, K \bar K amplitudes are tested in this model. Some are well satisfied, others badly violated, when electroweak penguins are included.Comment: 29 pages, latex/revtex, no figure
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