1,324 research outputs found

    Observation of B0pΛˉD()B^{0} \rightarrow p\bar{\Lambda} D^{(*)-}

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    We report the first observation of the decays B0pΛˉD()B^0 \rightarrow p\bar{\Lambda} D^{(*)-}. The data sample of 711711 fb1^{-1} used in this analysis corresponds to 772772 million BBˉB\bar{B} pairs, collected at the Υ(4S)\Upsilon(4S) resonance by the Belle detector at the KEKB asymmetric-energy e+ee^{+}e^{-} collider. We observe 19.8σ19.8\sigma and 10.8σ10.8\sigma excesses of events for the two decay modes and measure the branching fractions of B0pΛˉDB^0 \rightarrow p\bar{\Lambda} D^{-} and B0pΛˉDB^0 \rightarrow p\bar{\Lambda} D^{*-} to be (25.1±2.6±3.5)×106(25.1\pm2.6\pm3.5)\times10^{-6} and (33.6±6.3±4.4)×106(33.6\pm6.3\pm4.4)\times10^{-6}, respectively, where the first uncertainties are statistical and the second are systematic. These results are not compatible with the predictions based on the generalized factorization approach. In addition, a threshold enhancement in the di-baryon (pΛˉp\bar{\Lambda}) system is observed, consistent with that observed in similar BB decays.Comment: 16 pages, 3 figures and 3 tables, submitted to PR

    Inclusive study of bottomonium production in association with an η\eta meson in e+ee^+e^- annihilations near Υ(5S)\Upsilon(5S)

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    We study bottomonium production in association with an η\eta meson in e+ee^+e^- annihilations near the Υ(5S)\Upsilon(5S), at a center of mass energy of s=10.866\sqrt{s}=10.866\,GeV. The results are based on the 121.4121.4\,fb1^{-1} data sample collected by the Belle experiment at the asymmetric energy KEKB collider. Only the η\eta meson is reconstructed and the missing-mass spectrum of η\eta candidates is investigated. We observe the e+eηΥJ(1D)e^+e^-\to\eta\Upsilon_J(1D) process and find evidence for the e+eηΥ(2S)e^+e^-\to\eta\Upsilon(2S) process, while no significant signals of Υ(1S)\Upsilon(1S), hb(1P)h_b(1P), nor hb(2P)h_b(2P) are found. Cross sections for the studied processes are reported.Comment: Submitted to EPJ-

    Measurement of eta_c(1S), eta_c(2S) and non-resonant eta' pi+ pi- production via two-photon collisions

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    We report the measurement of gamma gamma to eta_c(1S), eta_c(2S) to eta' pi+ pi- with eta' decays to gamma rho and eta pi+ pi- using 941 fb^{-1} of data collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. The eta_c(1S) mass and width are measured to be M = [2984.6\pm0.7 (stat.)\pm2.2 (syst.)] MeV/c^{2} and \Gamma = [30.8^{+2.3}_{-2.2}~(stat.) \pm 2.5~(syst.)] MeV, respectively. First observation of eta_c(2S) to eta' pi+ pi- with a significance of 5.5sigma including systematic error is obtained, and the eta_c(2S) mass is measured to be M = [3635.1\pm3.7~(stat.)\pm2.9~(syst.)] MeV/c^{2}. The products of the two-photon decay width and branching fraction (B) of decays to eta'pi+ pi- are determined to be \Gamma_{gamma gamma}B = [65.4\pm2.6~(stat.)\pm6.9~(syst.)] eV for eta_c(1S) and [5.6^{+1.2}_{-1.1}~(stat.)\pm1.1~(syst.)] eV for eta_c(2S). A new decay mode for the eta_c(1S) to eta'f_0(2080) with f_0(2080) to pi+ pi- is observed with a statistical significance of 20sigma. The f_0(2080) mass and width are determined to be M = [2083^{+63}_{-66}~(stat.)\pm 32~(syst.)] MeV/c^{2} and \Gamma = [178^{+60}_{-178}~(stat.) \pm 55~(syst.)] MeV. The cross sections for gamma gamma to eta' pi+ pi- and eta'f_{2}(1270) are measured for the first time.Comment: 19 pages, 14 figure

    Measurement of the CKM Matrix Element Vcb|V_{cb}| from B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell at Belle

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    We present a new measurement of the CKM matrix element Vcb|V_{cb}| from B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell decays, reconstructed with the full Belle data set of 711fb1711 \, \rm fb^{-1} integrated luminosity. Two form factor parameterizations, originally conceived by the Caprini-Lellouch-Neubert (CLN) and the Boyd, Grinstein and Lebed (BGL) groups, are used to extract the product F(1)ηEWVcb\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| and the decay form factors, where F(1)\mathcal{F}(1) is the normalization factor and ηEW\eta_{\rm EW} is a small electroweak correction. In the CLN parameterization we find F(1)ηEWVcb=(35.06±0.15±0.56)×103\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| = (35.06 \pm 0.15 \pm 0.56) \times 10^{-3}, ρ2=1.106±0.031±0.007\rho^{2}=1.106 \pm 0.031 \pm 0.007, R1(1)=1.229±0.028±0.009R_{1}(1)=1.229 \pm 0.028 \pm 0.009, R2(1)=0.852±0.021±0.006R_{2}(1)=0.852 \pm 0.021 \pm 0.006. For the BGL parameterization we obtain F(1)ηEWVcb=(34.93±0.23±0.59)×103\mathcal{F}(1)\eta_{\rm EW}|V_{cb}|= (34.93 \pm 0.23 \pm 0.59)\times 10^{-3}, which is consistent with the World Average when correcting for F(1)ηEW\mathcal{F}(1)\eta_{\rm EW}. The branching fraction of B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell is measured to be B(B0D+ν)=(4.90±0.02±0.16)%\mathcal{B}(B^{0}\rightarrow D^{*-}\ell^{+}\nu_{\ell}) = (4.90 \pm 0.02 \pm 0.16)\%. We also present a new test of lepton flavor universality violation in semileptonic BB decays, B(B0De+ν)B(B0Dμ+ν)=1.01±0.01±0.03 \frac{{\cal B }(B^0 \to D^{*-} e^+ \nu)}{{\cal B }(B^0 \to D^{*-} \mu^+ \nu)} = 1.01 \pm 0.01 \pm 0.03~. The errors correspond to the statistical and systematic uncertainties respectively. This is the most precise measurement of F(1)ηEWVcb\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| and form factors to date and the first experimental study of the BGL form factor parameterization in an experimental measurement

    Study of π0\pi^0 pair production in single-tag two-photon collisions

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    We report a measurement of the differential cross section of π0\pi^0 pair production in single-tag two-photon collisions, γγπ0π0\gamma^* \gamma \to \pi^0 \pi^0, in e+ee^+ e^- scattering. The cross section is measured for Q2Q^2 up to 30 GeV2^2, where Q2Q^2 is the negative of the invariant mass squared of the tagged photon, in the kinematic range 0.5 GeV < W < 2.1 GeV and cosθ|\cos \theta^*| < 1.0 for the total energy and pion scattering angle, respectively, in the γγ\gamma^* \gamma center-of-mass system. The results are based on a data sample of 759 fb1^{-1} collected with the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider. The transition form factor of the f0(980)f_0(980) and that of the f2(1270)f_2(1270) with the helicity-0, -1, and -2 components separately are measured for the first time and are compared with theoretical calculations.Comment: 36 pages, 37 figures, 11 tables, Belle Preprint 2015-15, KEK Preprint 2015-2

    Measurement of branching fraction and direct CPCP asymmetry in charmless B+K+Kπ+B^+ \to K^+K^- \pi^+ decays at Belle

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    We report a study of the charmless hadronic decay of the charged BB meson to the three-body final state K+Kπ+K^+ K^- \pi^+. The results are based on a data sample that contains 772×106772\times10^6 BBˉB \bar{B} pairs collected at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider. The measured inclusive branching fraction and the direct CPCP asymmetry are (5.38±0.40±0.35)×106(5.38\pm0.40\pm0.35)\times 10^{-6} and 0.170±0.073±0.017-0.170\pm0.073\pm0.017, respectively, where the first uncertainties are statistical and the second are systematic. The K+KK^{+}K^{-} invariant mass distribution of the signal candidates shows an excess in the region below 1.51.5 GeV/c2c^2, which is consistent with the previous studies from BaBar and LHCb. In addition, strong evidence of a large direct CPCP asymmetry is found in the K+KK^{+}K^{-} low-invariant-mass region.Comment: 7 pages, 3 figure

    Angular analysis of B0K(892)0+B^0 \to K^\ast(892)^0 \ell^+ \ell^-

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    We present a measurement of angular observables, P4P_4', P5P_5', P6P_6', P8P_8', in the decay B0K(892)0+B^0 \to K^\ast(892)^0 \ell^+ \ell^-, where +\ell^+\ell^- is either e+ee^+e^- or μ+μ\mu^+\mu^-. The analysis is performed on a data sample corresponding to an integrated luminosity of 711 fb1711~\mathrm{fb}^{-1} containing 772×106772\times 10^{6} BBˉB\bar B pairs, collected at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the asymmetric-energy e+ee^+e^- collider KEKB. Four angular observables, P4,5,6,8P_{4,5,6,8}' are extracted in five bins of the invariant mass squared of the lepton system, q2q^2. We compare our results for P4,5,6,8P_{4,5,6,8}' with Standard Model predictions including the q2q^2 region in which the LHCb collaboration reported the so-called P5P_5' anomaly.Comment: Conference paper for LHC Ski 2016. SM prediction for P6P_{6}' corrected and reference for arXiv:1207.2753 adde

    Measurement of Branching Fractions of Hadronic Decays of the Ωc0\Omega_c^0 Baryon

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    Using a data sample of 980 fb1{\rm fb}^{-1} of e+ee^+e^- annihilation data taken with the Belle detector operating at the KEKB asymmetric-energy e+ee^+e^- collider, we report the results of a study of the decays of the Ωc0\Omega_c^0 charmed baryon into hadronic final states. We report the most precise measurements to date of the relative branching fractions of the Ωc0\Omega_c^0 into Ωπ+π0\Omega^-\pi^+\pi^0, Ωπ+ππ+\Omega^-\pi^+\pi^-\pi^+, ΞKπ+π+\Xi^-K^-\pi^+\pi^+, and Ξ0Kπ+\Xi^0K^-\pi^+, as well as the first measurements of the branching fractions of the Ωc0\Omega_c^0 into ΞKˉ0π+\Xi^-\bar{K}^0\pi^+, Ξ0Kˉ0\Xi^0\bar{K}^0, and ΛKˉ0Kˉ0\Lambda \bar{K}^0\bar{K}^0, all with respect to the Ωπ+\Omega^-\pi^+ decay. In addition, we investigate the resonant substructure of these modes. Finally, we present a limit on the branching fraction for the decay Ωc0Σ+KKπ+\Omega_c^0\to\Sigma^+K^-K^-\pi^+
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