38 research outputs found

    Search for Resonant B±K±hK±γγB^{\pm}\to K^{\pm} h \to K^{\pm} \gamma \gamma Decays at Belle

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    We report measurements and searches for resonant B±K±hK±γγB^{\pm} \to K^{\pm} h \to K^{\pm} \gamma \gamma decays where hh is a η,η,ηc,ηc(2S),χc0,χc2,J/ψ\eta,\eta^{\prime},\eta_{c},\eta_{c}(2S),\chi_{c0},\chi_{c2},J/\psi meson or the X(3872) particle.Comment: accepted by Physics Letters

    Observation of the ϕ(1680)\phi(1680) and the Y(2175) in e+eϕπ+πe^+ e^- \to \phi\pi^+\pi^-

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    The cross sections for e+eϕπ+πe^+ e^- \to \phi\pi^+\pi^- and e^+ e^- \to \phi \fzero are measured from threshold to s=3.0\sqrt{s}=3.0 GeV\hbox{GeV} using initial state radiation. The analysis is based on a data sample of 673 fb1^{-1} collected on and below the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. First measurements are reported for the resonance parameters of the ϕ(1680)\phi(1680) in the ϕπ+π\phi\pi^+\pi^- mode: m=(1689±7±10)m=(1689\pm 7\pm 10) MeV/c2c^2 and Γ=(211±14±19)\Gamma=(211\pm 14\pm 19) MeV/c2c^2. A structure at s=2.1GeV/c2\sqrt{s}=2.1 \hbox{GeV}/c^2, corresponding to the so called Y(2175), is observed; its mass and width are determined to be 2079±1328+792079\pm13^{+79}_{-28} MeV/c2c^2 and 192±2361+25MeV/c2192\pm23^{+25}_{-61} \hbox{MeV}/c^2, respectively.Comment: 11 pages, 6 figures. Add one plot. Accepted by Phys.Rev.D(RC

    Search for \bar{B}^0\to\Lambda_c^+\bar{\Lambda}_c^- decay at Belle

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    We search for the doubly charmed baryonic decay Bˉ0Λc+Λˉc\bar{B}^0\to\Lambda_c^+\bar{\Lambda}_c^-, in a data sample of 520×106520\times10^6 BBˉB{\bar B} events accumulated at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric e^+e^- collider. We find no significant signal and set an upper limit of B(Bˉ0Λc+Λˉc)<6.2×105{\cal B}(\bar{B}^0\to\Lambda_c^+\bar{\Lambda}_c^-)<6.2\times10^{-5} at 90% confidence level. The result is significantly below a naive extrapolation from B(BΞc0Λˉc){\cal B}(B^-\to\Xi_c^0\bar{\Lambda}_c^) assuming a simple Cabibbo-suppression factor of Vcd/Vcs2|V_{cd}/V_{cs}|^2. The small branching fraction could be attributed to a suppression due to the large momentum of the baryonic decay products, which has been observed in other charmed baryonic two-body B decays. trend observed in other charmed baryonic two-body B decays.Comment: 12 page, 5 figures. Contribution paper for conferences EPS2007 and Lepton Photon 2007, Belle-Conference-070

    Search for B -> h(*) nu nubar Decays at Belle

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    We present a search for the rare decays B -> h(*) nu nubar, where h(*) stands for a light meson. A data sample of 535 million BBbar pairs collected with the Belle detector at the KEKB e+e- collider is used. Signal candidates are required to have an accompanying B meson fully reconstructed in a hadronic mode and signal-side particles consistent with a single h(*) meson. No significant signal is observed and we set upper limits on the branching fractions at 90% confidence level. The limits on B0 -> K*0 nu nubar and B+ -> K+ nu nubar decays are more stringent than the previous constraints, while the first searches for B0 -> K0 nu nubar, pi0 nu nubar, rho0 nu nubar, phi nu nubar and B+ -> K*+ nu nubar, rho+ nu nubar are reported.Comment: 6 pages, 2 figures, submit to PR

    A Low-Footprint Java-to-Native Compilation Scheme Using Formal Methods

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    Ahead-of-Time and Just-in-Time compilation are common ways to improve runtime performances of restrained systems like Java Card by turning critical Java methods into native code. However, native code is much bigger than Java bytecode, which severely limits or even forbids these practices for devices with memory constraints. In this paper, we describe and evaluate a method for reducing natively-compiled code by suppressing runtime exception check sites, which are emitted when compiling bytecodes that may potentially throw runtime exceptions. This is made possible by completing the Java program with JML annotations, and using a theorem prover in order to formally prove that the compiled methods never throw runtime exceptions. Runtime exception check sites can then safely be removed from the generated native code, as it is proved they will never be entered. We have experimented our approach on several card-range and embedded Java applications, and were able to remove almost all the exception check sites. Results show memory footprints for native code that are up to 70% smaller than the non-optimized version, and sometimes as low than 115% the size of the Java bytecode when compiled for ARM thumb

    Measurement of cross sections of exclusive e+eVPe^+ e^- \to VP processes at s=10.58\sqrt{s}=10.58 GeV

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    The cross sections for the reactions e+eϕη,ϕη,ρη,ρηe^+e^- \to \phi\eta, \quad \phi\eta', \quad \rho\eta, \quad \rho\eta' have been measured using a data sample of 516 fb1^{-1} collected with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. The corresponding values of the cross sections are: 1.4±0.4±0.11.4 \pm 0.4 \pm 0.1 fb (ϕη)(\phi\eta), 5.3±1.1±0.45.3 \pm 1.1 \pm 0.4 fb (ϕη)(\phi\eta'), 3.1±0.5±0.13.1 \pm 0.5 \pm 0.1 fb (ρη)(\rho\eta) and 3.3±0.6±0.23.3 \pm 0.6 \pm 0.2 fb (ρη)(\rho\eta'). The energy dependence of the cross sections is presented using Belle measurements together with those of CLEO and BaBar.Comment: 8 pages, 8 figure

    Measurement of the Decay B_s^0 -> D_s^- pi^+ and Evidence for B_s^0 -> D_s^{+/-} K^{-/+} in e+e- Annihilation at sqrt(s)~10.87 GeV

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    We have studied Bs0 -> Ds- pi+ and Bs0 -> Ds^(-/+) K^(+/-) decays using 23.6 /fb of data collected at the Upsilon(5S) resonance with the Belle detector at the KEKB e+e- collider. This highly pure Bs0 -> Ds- pi+ sample is used to measure the branching fraction, BR(Bs0 -> Ds- pi+)=[3.67 +0.35,-0.33}(stat.) +0.43,-0.42(syst.) +-0.49(f_s)] x 10^{-3} (f_s=N(Bs(*) Bs(*)bar)/N(b\bar b)) and the fractions of Bs0 event types at the Upsilon(5S) energy, {in particular N(Bs* Bs*bar}/N(N(Bs(*) Bs(*)bar)=(90.1 +3.8,-4.0 +-0.2)%. We also determine the masses M(Bs0)=(5364.4 +-1.3 +-0.7) MeV/c^2 and M(Bs*)=(5416.4 +-0.4 +-0.5) MeV/c^2. In addition, we observe Bs0 -> Ds^(-/+) K^(+/-) decays with a significance of 3.5\sigma and measure BR(Bs0 -> Ds^(-/+) K^(+/-))=[2.4 +1.2,-1.0(stat.) +-0.3(syst.) +-0.3(f_s)] x 10^{-4}.Comment: 5 pages, 4 figures, accepted by PR

    Measurement of B(Ds -> munu)

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    We present a measurement of the branching fraction B(Ds+μ+νμ)B(D_s^+\to\mu^+\nu_\mu) using a 548 fb1^{-1} data sample collected by the Belle experiment at the KEKB e+ee^+e^- collider. The DsD_s momentum is determined by reconstruction of the system recoiling against DKγXDK\gamma X in events of the type e+eDsDKX,DsDsγe^+e^-\to D_s^\ast DKX, D_s^\ast \to D_s\gamma, where XX represents additional pions or photons from fragmentation. The full reconstruction method provides high resolution in the neutrino momentum and thus good background separation, equivalent to that reached by experiments at the tau-charm factories. We obtain the branching fraction B(Ds+μ+νμ)=(6.44±0.76(stat)±0.57(syst))103B(D_s^+\to\mu^+\nu_\mu) = (6.44 \pm 0.76({\rm stat}) \pm 0.57({\rm syst})) \cdot 10^{-3}, implying a DsD_s decay constant of fDs=(275±16(stat)±12(syst))f_{D_s} = (275 \pm 16({\rm stat}) \pm 12({\rm syst})) MeV.Comment: 6 pages, 2 figures, replaced by version subm. to Phys. Rev. Let

    Search for B0J/ψϕB^0 \to J/\psi \phi

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    We report a search for the decay B0J/ψϕB^0 \to J/\psi \phi, using a sample of 657 ×106\times 10^6 BBˉB\bar{B} pairs collected with the Belle detector at the Υ(4S)\Upsilon(4S) resonance. No statistically significant signal is found and an upper limit for the branching fraction is determined to be B(B0J/ψϕ)<9.4×107\mathcal{B}(B^0 \to J/\psi \phi) < 9.4 \times 10^{-7} at 90% confidence level.Comment: 5 pages, 2 figures, 3 tables, submitted to PRD(RC

    Evidence for Neutral B Meson Decays to wK*0

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    We present the results of a study of the charmless vector-vector decay B0->wK*0 with 657x10^6 BB(bar) pairs collected with the Belle detector at the KEKB e+e- collider. We measure the branching fraction to be B(B0->wK*0)=[1.8+/-0.7(stat)+/-0.3(syst)]x10^-6 with 3.0sigma significance. We also perform a helicity analysis of the w and K*0 vector mesons, and obtain the longitudinal polarization fraction fL(B0->wK*0)=0.56+/-0.29(stat)+0.18-0.08(syst). Finally, we measure a large non-resonant branching fraction B[B->wK+pi-; M(Kpi)\in(0.755,1.250) GeV/c^2]=[5.1+/-0.7(stat)+/-0.7(syst)]x10^-6 with a significance of 9.5sigma.Comment: 6 pages, 3 figures (7 figure files
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