434 research outputs found

    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

    Get PDF
    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

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

    Get PDF
    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

    Evidence for a vector charmonium-like state in e+eDs+Ds2(2573)+c.c.e^+e^- \to D^+_sD^*_{s2}(2573)^-+c.c.

    Get PDF
    We report the measurement of e+eDs+Ds2(2573)+c.c.e^+e^- \to D^+_sD^*_{s2}(2573)^-+c.c. via initial-state radiation using a data sample of an integrated luminosity of 921.9 fb1^{-1} collected with the Belle detector at the Υ(4S)\Upsilon(4S) and nearby. We find evidence for an enhancement with a 3.4σ\sigma significance in the invariant mass of Ds+Ds2(2573)+c.c.D^+_sD^*_{s2}(2573)^- +c.c. The measured mass and width are (4619.88.0+8.9(stat.)±2.3(syst.)) MeV/c2(4619.8^{+8.9}_{-8.0}({\rm stat.})\pm2.3({\rm syst.}))~{\rm MeV}/c^{2} and (47.014.8+31.3(stat.)±4.6(syst.)) MeV(47.0^{+31.3}_{-14.8}({\rm stat.})\pm4.6({\rm syst.}))~{\rm MeV}, respectively. The mass, width, and quantum numbers of this enhancement are consistent with the charmonium-like state at 4626 MeV/c2c^2 recently reported by Belle in e+eDs+Ds1(2536)+c.c.e^+e^-\to D^+_sD_{s1}(2536)^-+c.c. The product of the e+eDs+Ds2(2573)+c.c.e^+e^-\to D^+_sD^*_{s2}(2573)^-+c.c. cross section and the branching fraction of Ds2(2573)Dˉ0KD^*_{s2}(2573)^-\to{\bar D}^0K^- is measured from Ds+Ds2(2573)D^+_sD^*_{s2}(2573)^- threshold to 5.6 GeV.Comment: 9 pages, 4 figure

    Observation of a vector charmoniumlike state in e+^{+}e^{-}\rightarrowD+^{+}s_{s}Ds1_{s1}(2536)^{-}+c.c

    Get PDF

    Measurements of the branching fractions B(B⁻ → Λˉ\bar{Λ}c_{c}^{-}Ξc´0_{c}^{´0}), B(B⁻ → Λˉ\bar{Λ}c_{c}^{-} Ξc_{c}(2645)0^{0}) and B(B⁻ → Λˉ\bar{Λ}c_{c}^{-} Ξc_{c}(2790)0^{0})

    Get PDF

    Belle II Executive Summary

    Full text link
    Belle II is a Super BB Factory experiment, expected to record 50 ab1^{-1} of e+ee^+e^- collisions at the SuperKEKB accelerator over the next decade. The large samples of BB mesons, charm hadrons, and tau leptons produced in the clean experimental environment of e+ee^+e^- collisions will provide the basis of a broad and unique flavor-physics program. Belle II will pursue physics beyond the Standard Model in many ways, for example: improving the precision of weak interaction parameters, particularly Cabibbo-Kobayashi-Maskawa (CKM) matrix elements and phases, and thus more rigorously test the CKM paradigm, measuring lepton-flavor-violating parameters, and performing unique searches for missing-mass dark matter events. Many key measurements will be made with world-leading precision.Comment: 7 pages, to be submitted to the "Rare and Precision Measurements Frontier" of the APS DPF Community Planning Exercise Snowmass 202

    Search for transitions from Υ(4S) and V(5S) to ηb(1S) and ηb(2S) with emission of an ω meson

    Get PDF
    Using data collected in the Belle experiment at the KEKB asymmetric-energy e+e− collider we search for transitions Υ(4S)→ ηb_{b}(1S)ω, Υ(5S)→ηb_{b}(1S)ω and Υ(5S)→ηb_{b}(2S)ω. No significant signals are observed and we set 90% confidence level upper limits on the corresponding visible cross sections: 0.2 pb, 0.4 pb and 1.9 pb, respectively

    Search for transitions from Υ(4S)\Upsilon(4S) and Υ(5S)\Upsilon(5S) to ηb(1S)\eta_b(1S) and ηb(2S)\eta_b(2S) with emission of an ω\omega meson

    Full text link
    Using data collected in the Belle experiment at the KEKB asymmetric-energy e+ee^+e^- collider we search for transitions Υ(4S)ηb(1S)ω\Upsilon(4S) \rightarrow \eta_b(1S)\omega, Υ(5S)ηb(1S)ω\Upsilon(5S) \rightarrow \eta_b(1S)\omega and Υ(5S)ηb(2S)ω\Upsilon(5S) \rightarrow \eta_b(2S)\omega. No significant signals are observed and we set 90\% confidence level upper limits on the corresponding visible cross sections: 0.2 pb,0.4 pb0.2 ~\textrm{pb}, 0.4 ~\textrm{pb} and 1.9 pb1.9 ~\textrm{pb}, respectively.Comment: 7 pages, 5 figure

    Search for B0^{0} decays to invisible final states ( +γ) at Belle

    Get PDF
    We report searches for B0invisibleB^0\to\rm{invisible} and B0invisible+γB^0\to\rm{invisible}+\gamma decays, where the energy of the photon is required to be larger than 0.5 GeV. These results are obtained from a 711fb1711\,{\rm fb}^{-1} data sample that contains 772×106BBˉ772 \times 10^6 B\bar{B} pairs and was collected near the Υ(4S)\Upsilon\,(4S) resonance with the Belle detector at the KEKB e+ee^+ e^- collider. We observe no significant signal for either decay and set upper limits on their branching fractions at 90%90\% confidence level of B(B0invisible)<7.8×105\mathcal{B}\,(B^0\to\rm{invisible}) < 7.8\times10^{-5} and B(B0invisible+γ)<1.6×105\mathcal{B}\,(B^0\to\rm{invisible}+\gamma) < 1.6\times10^{-5}
    corecore