325 research outputs found

    RapidRadio: A Domain-Specific Productivity Enhancing Framework

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    The RapidRadio framework for signal classification and receiver deployment is discussed. The framework is a productivity enhancing tool that reduces the required knowledge-base for implementing a receiver on an FPGA-based SDR platform. The ultimate objective of this framework is to identify unknown signals and to build FPGA-based receivers capable of receiving them. The architecture of the receiver deployed by the framework and its implementation are discussed. The framework's capacity to classify a signal and deploy a functional receiver is validated with over-the-air experiments

    Impact of D0-D0bar mixing on the experimental determination of gamma

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    Several methods have been devised to measure the weak phase gamma using decays of the type B+- --> D K+-, where it is assumed that there is no mixing in the D0-D0bar system. However, when using these methods to uncover new physics, one must entertain the real possibility that the measurements are affected by new physics effects in the D0-D0bar system. We show that even values of x_D and/or y_D around 10^{-2} can have a significant impact in the measurement of sin^2{gamma}. We discuss the errors incurred in neglecting this effect, how the effect can be checked, and how to include it in the analysis.Comment: 18 pages, Latex with epsfig, 8 figure

    Cabibbo-suppressed non-leptonic B- and D-decays involving tensor mesons

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    The Cabibbo-suppressed non-leptonic decays of B (and D) mesons to final states involving tensor mesons are computed using the non-relativistic quark model of Isgur-Scora-Grinstein-Wise with the factorization hypothesis. We find that some of these B decay modes, as B --> (K^*, D^*)D^*_2, can have branching ratios as large as 6 x 10^{-5} which seems to be at the reach of future B factories.Comment: Latex, 11 pages, to appear in Phys. Rev.

    Weak decays of 4He-Lambda

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    We measured the lifetime and the mesonic and non-mesonic decay rates of the 4He-Lambda hypernucleus. The hypernuclei were created using a 750 MeV/c momentum K- beam on a liquid 4He target by the reaction 4He(K-,pi-)4He-Lambda. The 4He-Lambda lifetime was directly measured using protons from Lambda p -> n p non-mesonic decay (also referred to as proton-stimulated decay) and was found to have a value of tau = 245 +/- 24 ps. The mesonic decay rates were determined from the observed numbers of pi-'s and pi0's as Gamma_pi-/Gamma_tot = 0.270 +/- 0.024 and Gamma_pi0/Gamma_tot = 0.564 +/- 0.036, respectively, and the values of the proton- and neutron-stimulated decay rates were extracted as Gamma_p/Gamma_tot = 0.169 +/- 0.019 and Gamma_n/Gamma_tot <= 0.032 (95% CL), respectively. The effects of final-state interactions and possible 3-body Lambda N N decay contributions were studied in the context of a simple model of nucleon-stimulated decay. Nucleon-nucleon coincidence events were observed and were used in the determination of the non-mesonic branching fractions. The implications of the results of this analysis were considered for the empirical Delta I = 1/2 rule and the decay rates of the 4H-Lambda hypernucleus.Comment: 15 pages, 11 figures, published in PRC, revised content to match published versio

    Measuring Îł\gamma in B±→K±(KK∗)DB^\pm \to K^\pm (K K^*)_D decays

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    We develop a method to measure the CKM angle Îł\gamma without hadronic uncertainties from the analysis of B±→K±D0B^\pm \to K^\pm D^0 and K^\pm \D0bar followed by singly Cabibbo-suppressed DD decays to non CP-eigenstates, such as K±K∗∓K^\pm K^{*\mp}. This method utilizes the interference between b→cuˉsb\to c\bar u s and b→ucˉsb\to u\bar c s decays, and we point out several attractive features of it. All the modes that need to be measured for this method are accessible in the present data.Comment: 8 page

    Determining Îł\gamma using B±→DK±B^\pm \to D K^\pm with multibody D decays

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    We propose a method for determining Îł\gamma using B±→DK±B^\pm\to D K^\pm decays followed by a multibody DD decay, such as D→KSπ−π+D \to K_S \pi^-\pi^+, D→KSK−K+D \to K_S K^-K^+ and D→KSπ−π+π0D \to K_S \pi^-\pi^+\pi^0. The main advantages of the method is that it uses only Cabibbo allowed DD decays, and that large strong phases are expected due to the presence of resonances. Since no knowledge about the resonance structure is needed, Îł\gamma can be extracted without any hadronic uncertainty.Comment: 17 pages, 1 figur

    Lattice QCD calculation of Bˉ→DlΜˉ\bar{B}\to Dl\bar{\nu} decay form factors at zero recoil

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    A lattice QCD calculation of the Bˉ→DlΜˉ\bar{B}\to Dl\bar{\nu} decay form factors is presented. We obtain the value of the form factor h+(w)h_+(w) at the zero-recoil limit w=1w=1 with high precision by considering a ratio of correlation functions in which the bulk of the uncertainties cancels. The other form factor h−(w)h_-(w) is calculated, for small recoil momenta, from a similar ratio. In both cases, the heavy quark mass dependence is observed through direct calculations with several combinations of initial and final heavy quark masses. Our results are h+(1)=1.007(6)(2)(3)h_+(1) = 1.007(6)(2)(3) and h−(1)=−0.107(28)(04)(3010)h_-(1)=-0.107(28)(04)(^{10}_{30}). For both the first error is statistical, the second stems from the uncertainty in adjusting the heavy quark masses, and the last from omitted radiative corrections. Combining these results, we obtain a precise determination of the physical combination FB→D(1)=1.058(1720)F_{B\to D}(1)=1.058(^{20}_{17}), where the mentioned systematic errors are added in quadrature. The dependence on lattice spacing and the effect of quenching are not yet included, but with our method they should be a fraction of FB→D−1F_{B\to D}-1.Comment: 32 pp, 10 figs; final, published versio

    Decay constants, semi-leptonic and non-leptonic decays in a Bethe-Salpeter Model

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    We evaluate the decay constants for the B and DD mesons and the form factors for the semileptonic decays of the B meson to DD and D∗D^* mesons in a Bethe-Salpeter model. From data we extract Vcb=0.039±0.002V_{cb}=0.039 \pm 0.002 from Bˉ→D∗lΜˉ{\bar B} \to D^* l {\bar{\nu}} and Vcb=0.037±0.004V_{cb}=0.037 \pm 0.004 from Bˉ→DlΜˉ{\bar B} \to D l {\bar{\nu}} decays. The form factors are then used to obtain non-leptonic decay partial widths for B→Dπ(K) B\to D \pi (K) and B→DD(Ds)B \to D D (D_s) in the factorization approximation.Comment: 15 Pages, 3 Postscript figures (available also from [email protected]

    Resummation of Running Coupling Effects in Semileptonic B Meson Decays and Extraction of ∣Vcb∣|V_{cb}|

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    We present a determination of ∣Vcb∣|V_{cb}| from semileptonic B decays that includes resummation of supposedly large perturbative corrections, originating from the running of the strong coupling. We argue that the low value of the BLM scale found previously for inclusive decays is a manifestation of the renormalon divergence of the perturbative series starting already in third order. A reliable determination of ∣Vcb∣|V_{cb}| from inclusive decays is possible if one either uses a short-distance b quark mass or eliminates all unphysical mass parameters in terms of measured observables, such that all infra-red contributions of order 1/mb1/m_b cancel explicitly. We find that using the MS‟\overline{\rm MS} running mass significantly reduces the perturbative coefficients already in low orders. For a semileptonic branching ratio of 10.9%10.9\% we obtain ∣Vcb∣(τB/1.50 ps)1/2=0.041±0.002|V_{cb}|(\tau_B/1.50\,{\rm ps})^{1/2}= 0.041\pm 0.002 from inclusive decays, in good agreement with the value extracted from exclusive decays.Comment: 37 pages + 4 figures, final version accepted for publication in Phys. Rev.

    A new method for extracting the weak phase gamma from B ---> D K(*) decays

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    A new method to extract the weak phase Îł\gamma is suggested by exploiting B ---> D K^{(*)} decay modes that are not Cabibbo suppressed, using the isospin relations, and ignoring the annihilation diagram as usual. Assuming 3×108BBˉ3 \times 10^8 B\bar{B} pair at BB factories, one can determine Îł\gamma with 3−σ3-\sigma accuracy for 80^o D K modes and for 50^o D K^* modes.Comment: 10 pages with 2 figure
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