3,688 research outputs found

    Measurement of CP violating asymmetries in B^0 -> K^+K^- K^0_S decays with a time-dependent Dalitz approach

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    We report a measurement of CPCP violating asymmetries in B0(B0)K+KKS0B^0(\overline{B}^0) \to K^+ K^- K^0_S decays with a time-dependent Dalitz approach. This analysis is based on a data sample of 657×106657\times 10^6 BBB\overline{B} pairs accumulated at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. As the result of an unbinned maximum likelihood fit to the selected candidates, the mixing-induced and direct CPCP violation parameters, ϕ1eff\phi^{\rm eff}_1 and ACP{\cal A}_{CP} are obtained for B0ϕ(1020)KS0B^0 \to \phi(1020) K^0_S, B0f0(980)KS0B^0 \to f_0(980) K^0_S and other B0K+KKS0B^0 \to K^+ K^- K^0_S decays. We find four solutions that describe the data. There are \{eqnarray*} \phi_1^{\rm eff}(B^0\to \phi(1020) K^0_S) & = & (32.2 \pm 9.0 \pm 2.6 \pm 1.4)^{\circ}; \phi_1^{\rm eff}(B^0\to \phi(1020) K^0_S) & = & (26.2 \pm 8.8 \pm 2.7 \pm 1.2)^{\circ};\\ \phi_1^{\rm eff}(B^0\to \phi(1020) K^0_S) & = & (27.3 \pm 8.6 \pm 2.8 \pm 1.3)^{\circ}\; {\rm and}\\ \phi_1^{\rm eff}(B^0\to \phi(1020) K^0_S) & = & (24.3 \pm 8.0 \pm 2.9 \pm 5.2)^{\circ}.{eqnarray*}\ The values for the CPCP violating phase in B0ϕ(1020)KS0B^0\to \phi(1020) K^0_S are similar but other properties of the Dalitz plot are quite different for the four solutions. These four solutions have consistent ϕ1eff\phi^{\rm eff}_1 values for all three BB meson decay channels and none of them deviates significantly from the values measured in B(ccˉ)K0B \to (c\bar{c}) K^0 decays with the currently available statistics. In addition, we find no significant direct CPCP violation.Comment: submitted to PR

    Measurement of Inclusive Radiative B-meson Decays with a Photon Energy Threshold of 1.7 GeV

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    Using 605/fb of data collected at the Upsilon(4S) resonance we present a measurement of the inclusive radiative B-meson decay channel, B to X_s gamma. For the lower photon energy thresholds of 1.7, 1.8, 1.9 and 2.0GeV, as defined in the rest frame of the B-meson, we measure the partial branching fraction and the mean and variance of the photon energy spectrum. At the 1.7GeV threshold we obtain the partial branching fraction BF(B to X_s gamma) = (3.45 +/- 0.15 +/- 0.40) x 10^-4, where the errors are statistical and systematic.Comment: 9 pages, 3 figures, 2 table

    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

    Dalitz analysis of B --> K pi psi' decays and the Z(4430)+

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    From a Dalitz plot analysis of B --> K pi psi' decays, we find a signal for Z(4430)+ --> pi+ psi' with a mass M= (4443(+15-12)(+19-13))MeV/c^2, width Gamma= (107(+86-43)(+74-56))MeV, product branching fraction BR(B0 --> K- Z(4430)+) x BR(Z(4430)+ --> pi+ psi')= (3.2(+1.8-0.9)(+5.3-1.6)) x 10^{-5}, and significance of 6.4sigma that agrees with previous Belle measurements based on the same data sample. In addition, we determine the branching fraction BR(B^0 --> K*(892)^0 psi')= (5.52(+0.35-0.32)(+0.53-0.58)) x 10^{-4} and the fraction of K*(892)^0 mesons that are longitudinally polarized f_L= 44.8(+4.0-2.7)(+4.0-5.3)%. These results are obtained from a 605fb^{-1} data sample that contains 657 million B-anti-B pairs collected near the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric energy e+e- collider.Comment: Final version published in PRD(RC

    Study of the BX(3872)(D0Dˉ0)KB\to X(3872)(\to D^{*0}\bar D^0)K decay

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    We present a study of BX(3872)KB\to X(3872)K with X(3872) decaying to D0Dˉ0D^{*0}\bar D^0 using a sample of 657 million BBˉB\bar B pairs recorded at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. Both D0D0γD^{*0}\to D^0\gamma and D0D0π0D^{*0}\to D^0\pi^0 decay modes are used. We find a peak of 50.111.1+14.850.1^{+14.8}_{-11.1} events with a mass of (3872.90.40.5+0.6+0.4)MeV/c2(3872.9^{+0.6 +0.4}_{-0.4 -0.5}){\rm MeV}/c^2, a width of (3.91.41.1+2.8+0.2)MeV/c2(3.9^{+2.8 +0.2}_{-1.4 -1.1}){\rm MeV}/c^2 and a product branching fraction B(BX(3872)K)×B(X(3872)D0Dˉ0)=(0.80±0.20±0.10)×104{\cal B}(B\to X(3872)K)\times{\cal B}(X(3872)\to D^{*0}\bar D^0)=(0.80\pm0.20\pm0.10)\times10^{-4}, where the first errors are statistical and the second ones are systematic. The significance of the signal is 6.4σ6.4\sigma. The difference between the fitted mass and the D0Dˉ0D^{*0}\bar D^0 threshold is calculated to be (1.10.40.3+0.6+0.1)MeV/c2(1.1^{+0.6 +0.1}_{-0.4 -0.3}){\rm MeV}/c^2. We also obtain an upper limit on the product of branching fractions B(BY(3940)K)×B(Y(3940)D0Dˉ0){\cal B}(B\to Y(3940)K)\times{\cal B}(Y(3940)\to D^{*0}\bar D^0) of 0.67×1040.67\times10^{-4} at 90% CL.Comment: 7 pages, 3 figures, BELLE-CONF-0832 contributed to ICHEP 2008, revised and submitted to Phys. Rev. D R

    Search for the X(1812) in B±K±ωϕB^{\pm} \to K^{\pm} \omega \phi

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    We report on a search for the X(1812) state in the decay B±K±ωϕB^{\pm} \to K^{\pm} \omega \phi with a data sample of 657×106657\times10^6 BBˉB\bar{B} pairs collected with the Belle detector at the KEKB e+ee^+e^- collider. No significant signal is observed. An upper limit B(B±K±X(1812),X(1812)ωϕ)<3.2×107{\cal B}(B^{\pm} \to K^{\pm} X(1812),X(1812) \to \omega \phi)<3.2\times 10^{-7} (90% C.L.) is determined. We also constrain the three-body decay branching fraction to be B(B±K±ωϕ){\cal B}(B^{\pm} \to K^{\pm} \omega \phi) << 1.9 ×106\times 10^{-6} (90% C.L.).Comment: 5pages,2 figures(3 figure files). submitted to PRD(RC

    Evidence for direct CP violation in the decay B->D(*)K, D->KsPi+Pi- and measurement of the CKM phase phi3

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    We present a new measurement of the unitarity triangle angle phi3 using a Dalitz plot analysis of the KsPi+Pi- decay of the neutral D meson produced in B->D(*)K decays. The method exploits the interference between D0 and D0bar to extract the angle phi3, strong phase delta and the ratio r of suppressed and allowed amplitudes. We apply this method to a 605 fb-1 data sample collected by the Belle experiment. The analysis uses three decays: B->DK, and B->D*K with D*->DPi0 and D*->Dgamma, as well as the corresponding charge-conjugate modes. From a combined maximum likelihood fit to the three modes, we obtain phi3 = 78.4^+10.8_-11.6 +- 3.6 (syst) +- 8.9 (model) degrees. CP conservation in this process is ruled out at the confidence level (1-CL)=5x10^-4, or 3.5 standard deviations.Comment: 10 pages, 5 figures, 4 tables. Replaced by version published in Phys. Rev.

    Measurement of the Branching Fraction of the Decay B+π+π+ν\boldsymbol{B^{+}\to\pi^{+}\pi^{-}\ell^{+}\nu_\ell} in Fully Reconstructed Events at Belle

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    We present an analysis of the exclusive B+π+π+νB^{+}\to\pi^{+}\pi^{-}\ell^{+}\nu_{\ell} decay, where \ell represents an electron or a muon, with the assumption of charge-conjugation symmetry and lepton universality. The analysis uses the full Υ(4S)\Upsilon(4S) data sample collected by the Belle detector, corresponding to 711 fb1^{-1} of integrated luminosity. We select the events by fully reconstructing one BB meson in hadronic decay modes, subsequently determining the properties of the other BB meson. We extract the signal yields using a binned maximum-likelihood fit to the missing-mass squared distribution in bins of the invariant mass of the two pions or the momentum transfer squared. We measure a total branching fraction of B(B+π+π+ν)=[22.71.6+1.9(stat)±3.5(syst)]×105{{\cal B}(B^{+}\to \pi^{+}\pi^{-}\ell^{+}\nu_{\ell})= [22.7 ^{+1.9}_{-1.6} (\mathrm{stat}) \pm 3.5(\mathrm{syst}) ]\times 10^{-5}}, where the uncertainties are statistical and systematic, respectively. This result is the first reported measurement of this decay.Comment: 23 pages, 19 figure

    Search for B+ -> l+ nu gamma decays with hadronic tagging using the full Belle data sample

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    We search for the decay B+ -> l+ nu gamma with l+ = e+ or mu+ using the full Belle data set of 772 x 10^6 BBbar pairs, collected at the Y(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e- collider. We reconstruct one B meson in a hadronic decay mode and search for the B+ -> l+ nu gamma decay in the remainder of the event. We observe no significant signal within the phase space of E_gamma^sig > 1 GeV and obtain upper limits of BR(B+ -> e+ nu gamma) mu+ nu gamma) l+ nu gamma) < 3.5 x 10^-6 at 90 % credibility level.Comment: Submitted to Phys. Rev.

    Measurement of B0π+ππ+πB^0\to\pi^+\pi^-\pi^+\pi^- Decays and Search for B0ρ0ρ0B^0\to\rho^0\rho^0

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    We report on a search for the decay B0ρ0ρ0B^0\to\rho^0\rho^0 and other charmless modes with a π+ππ+π\pi^+\pi^-\pi^+\pi^- final state, including B0ρ0π+πB^0\to\rho^0\pi^+\pi^-, non-resonant B04π±B^0\to 4\pi^{\pm}, B0ρ0f0(980)B^0\to\rho^0f_0(980), B0f0(980)f0(980)B^0\to f_0(980)f_0(980) and B0f0(980)π+πB^0\to f_0(980)\pi^+\pi^-. These results are obtained from a data sample containing 657 million BBB \overline B pairs collected with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. We set an upper limit on B(B0ρ0ρ0)\mathcal{B}(B^0\to\rho^0\rho^0) of 1.0×1061.0\times 10^{-6} at the 90% confidence level (C.L.). From our B0ρ0ρ0B^0\to\rho^0\rho^0 measurement and an isospin analysis, we determine the Cabibbo-Kobayashi-Maskawa phase ϕ2\phi_2 to be 91.7±14.991.7 \pm 14.9 degrees. We find excesses in B0ρ0π+πB^0\to \rho^0\pi^+\pi^- and non-resonant B04π±B^0\to 4\pi^{\pm} with 1.3σ\sigma and 2.5σ\sigma significance, respectively. The corresponding branching fractions are less than 12.0×10612.0 \times 10^{-6} and 19.3×10619.3 \times 10^{-6} at the 90% C.L. In addition, we set 90% C.L. upper limits as follows: B(B0ρ0f0(980))<0.3×106\mathcal{B}(B^0\to\rho^0f_0(980))< 0.3 \times 10^{-6}, B(B0f0(980)f0(980))<0.1×106\mathcal{B}(B^0\to f_0(980)f_0(980))< 0.1 \times 10^{-6}, and B(B0f0(980)π+π)<3.8×106\mathcal{B}(B^0\to f_0(980)\pi^+\pi^-)< 3.8 \times 10^{-6}.Comment: 6 pages, 2 figures. Submitted to PRD(RC
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