145 research outputs found

    b Physics Beyond the Standard Model

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    I review the signals for New Physics in CP-violating measurements in B and Lambda_b decays. I also discuss ways of identifying this New Physics, should such a signal be found.Comment: 10 pages, LaTeX, 1 figure, ps file included. References adde

    Precision Tests of Flavor and CP violation in B Decays

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    Isospin and flavor SU(3) set stringent bounds on penguin pollution in B0(t)→ρ+ρ−B^0(t)\to \rho^+\rho^-, providing a theoretically precise determination of Î±â‰ĄÏ•2\alpha\equiv \phi_2 , α=(91±7exp±3th)∘\alpha = (91\pm 7_{\rm exp}\pm 3_{\rm th})^\circ. Isospin breaking in a sum rule for B→KπB\to K\pi rates is shown to be suppressed. A similar sum rule holds for CP asymmetries in B→KπB\to K\pi. Violation of these sum rules would be evidence for an anomalous ΔI=1\Delta I=1 piece in Heff{\cal H}_{\rm eff}.Comment: Reference added; Invited talk presented at the First Workshop on Theory, Phenomenology and Experiments in Heavy Flavor Physics, Anacapri, Italy, 29-31 200

    Studying New Physics Amplitudes in Charmless B_s Decays

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    A method based on flavour SU(3) is proposed for identifying and extracting New Physics (NP) amplitudes in charmless ΔS=1\Delta S=1 BsB_s decays using time-dependent CP asymmetries in these decays and in flavour SU(3) related ΔS=0\Delta S=0 decays. For illustration, we assume a hierarchy, ∌1:λ:λ2\sim 1: \lambda : \lambda^2 (λ=0.2\lambda=0.2), between a dominant ΔS=1\Delta S=1 penguin amplitude, a NP amplitude and a Standard Model amplitude with weak phase Îł\gamma. An uncertainty from SU(3) breaking corrections, reduced by using ratios of hadronic amplitudes, is further suppressed by a factor λ\lambda. We discuss examples for pairs of decays into two neutral vector mesons, Bs→ϕϕ,Bs→ϕKˉ∗0B_s\to\phi\phi, B_s\to\phi \bar K^{*0} and Bs→K∗0Kˉ∗0,B0→K∗0Kˉ∗0B_s\to K^{*0}\bar K^{*0}, B^0\to K^{*0}\bar K^{*0}, where the magnitude of the NP amplitude, its weak and strong phases can be determined.Comment: typo corrected, reference added, submitted to Physics Letters

    Interpreting the time-dependent CP asymmetry in B0→π0KSB^0 \to \pi^0 K_S

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    Flavor SU(3) is used for studying the time-dependent CP asymmetry in B0→π0KSB^0 \to \pi^0 K_S by relating this process to B0→π0π0B^0\to \pi^0\pi^0 and B0→K+K−B^0 \to K^+K^-. We calculate correlated bounds on SπK−sin⁥2ÎČS_{\pi K} - \sin 2\beta and CπKC_{\pi K}, with maximal magnitudes of 0.2 and 0.3, where SπKS_{\pi K} and CπKC_{\pi K} are coefficients of sin⁡Δmt\sin\Delta mt and cos⁡Δmt\cos\Delta mt in the asymmetry. Stronger upper limits on B0→K+K−B^0 \to K^+K^- are expected to reduce these bounds and to imply nonzero lower limits on these observables. The asymmetry is studied as a function of a strong phase and the weak phase Îł\gamma.Comment: 11 pages, 2 figures, to be published in Phys. Lett. B. Some equations corrected leading to small changes in figure

    CP violation in B meson decays

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    Recent CP asymmetry measurements in tree-dominated processes, B0→π+π−,ρ+ρ−,ρ±π∓,B+→DK+B^0\to \pi^+\pi^-, \rho^+\rho^-, \rho^{\pm}\pi^{\mp}, B^+\to DK^+, and in penguin-dominated decays, B→π0KS,ηâ€ČKS,ϕKSB \to \pi^0 K_S, \eta' K_S, \phi K_S, are interpreted in the framework of the Kobayashi-Maskawa (KM) mechanism of CP violation. The KM phase emerges as the dominant source of CP violation in tree-dominated decays, which are beginning to constrain the unitarity triangle beyond other constraints. Improving precision of CP asymmetry measurements in penguin-dominated decays may indicate the need for new physics.Comment: Talk presented at the Sixth International Conference on Hyperons, Charm and Beauty Hadrons, IIT, Chicago, June 27--July 3 200

    Improving Bounds on Penguin Pollution in B -> pi pi

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    In the presence of penguin contributions, the indirect CP asymmetry in B0(t) -> pi+ pi- measures sin(2\alpha + 2\theta), where 2\theta parametrizes the size of the penguin ``pollution.'' We derive a new upper bound on |2\theta|, requiring the measurement of of BR(B+ -> pi+ pi0) and an upper bound on B00 \equiv {1\over 2} [BR(B0 -> pi0 pi0) + BR(B0bar -> pi0 pi0)]. The new bound is stronger than those previously discussed in the literature. We also present a lower bound on B00. Current data may suggest that it is not very small, in which case \theta can be determined using a complete isospin analysis.Comment: 10 pages, LaTeX, 3 figures. Abstract modified slightly. Submitted to Physics Letter

    Measuring the CP Angle \beta in Hadronic b\to s Penguin Decays

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    Asymmetric e^+e^- colliders running on the \Upsilon(4S) (B factories) will much more readily measure CP-violating asymmetries in the decays of B_d^0 and B^\pm mesons than in the decays of B_s^0 mesons. As such, they will seemingly not be able to probe new phases in Bs-Bs(bar) mixing, i.e. in b\to s transitions. However, by measuring the CP angle \beta via b \to s hadronic penguin decays such as B_d^0 \to \eta'\ks and B_d^0 \to\phi\ks, and comparing its value to that obtained in B_d^0 \to\Psi\ks, it is possible to detect the presence of new physics in the b\to s flavour-changing neutral current. Recent CLEO results are encouraging in this regard. They suggest that the branching ratio of the b\to s penguin decay B_d^0 \to \eta'\ks is anomalously large, about 4 \times 10^{-5}, which will make it much easier to search for new physics in b\to s transitions.Comment: 8 pages, LaTeX, 1 figure (included

    Patterns of New Physics in B Decays

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    We show that any new physics (NP) which affects B decays with penguin contributions can be absorbed by redefinitions of the standard-model (SM) diagrammatic amplitudes. Hence, there are no clean signals of NP in such decays unless there is an accurate theoretical estimate of parameters or a justifiable approximation can be made. In all decays with penguin contributions, NP simultaneously affects pairs of diagrams. The evidence for a large C' from fits to B-> pi K data is naturally explained if NP contributes to P_EW, since NP affects the P_EW and C' diagrams as a pair. The weak phase gamma measured in B-> pi K decays will always agree with its SM value even in the presence of NP, if the NP contributes in such a way that the amplitudes retain the SM form after suitable redefinitions.Comment: 4 pages, revtex, no figures; Several changes made to highlight results obtaine

    CKM Phases from CP Asymmetries

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    Measuring phases in the Cabibbo-Kobayashi-Maskawa matrix through CP asymmetries in B decays is a major goal of current and future experiments. Methods based on charge-conjugation and isospin symmetries involve very little theoretical uncertainties, while schemes based on flavor SU(3) involve uncertainties due to SU(3) breaking. Resolving these uncertainties requires further studies involving a dialogue between theory and experiments.Comment: minor corrections, several references added and update

    Implications for CP asymmetries of improved data on B→K0π0B \to K^0 \pi^0

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    The decay B0→K0π0B^0 \to K^0 \pi^0, dominated by a b→sb \to s penguin amplitude, holds the potential for exhibiting new physics in this amplitude. In the pure QCD penguin limit one expects \ckp = 0 and \skp = \sin 2 \beta for the coefficients of cos⁡Δmt\cos \Delta m t and sin⁡Δmt\sin \Delta m t in the time-dependent CP asymmetry. Small non-penguin contributions lead to corrections to these expressions which are calculated in terms of isospin-related B→KπB\to K\pi rates and asymmetries, using information about strong phases from experiment. We study the prospects for incisive tests of the Standard Model through examination of these corrections. We update a prediction \ckp=0.15\pm 0.04, pointing out the sensitivity of a prediction \skp\approx 1 to the measured branching ratio for B0→K0π0B^0\to K^0\pi^0 and to other observables.Comment: Note added, to be published in Physics Letters
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