262 research outputs found

    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

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

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    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

    Search for lepton-flavor-violating τ\tau decays into a lepton and a vector meson using the full Belle data sample

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    Charged-lepton-flavor-violation is predicted in several new physics scenarios. We update the analysis of τ\tau lepton decays into a light charged lepton (\ell = e±e^{\pm} or μ±\mu^{\pm}) and a vector meson (V0V^0 = ρ0\rho^0, ϕ\phi, ω\omega, K0K^{\ast0}, or K0\overline{K}{}^{\ast0}) using 980 fb1^{-1} of data collected with the Belle detector at the KEKB collider. No significant excess of such signal events is observed, and thus 90% credibility level upper limits are set on the τV0\tau \rightarrow \ell V^0 branching fractions in the range of (1.7--4.3)×1084.3) \times 10^{-8}. These limits are improved by 30% on average from the previous results.Comment: 19 pages, 5 figures; added one sentence in Acknowledgments; added a systematic uncertainty about the number of background estimation, and corrected some sentence

    First measurement of the Michel parameter ξ\xi^\prime in the τμνˉμντ\tau^-\to\mu^-\bar{\nu}_\mu\nu_\tau decay at Belle

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    We report the first measurement of the Michel parameter ξ\xi^\prime in the τμνˉμντ\tau^-\to\mu^-\bar{\nu}_\mu\nu_\tau decay with a new method proposed just recently. The measurement is based on the reconstruction of the τμνˉμντ\tau^-\to\mu^-\bar{\nu}_\mu\nu_\tau events with subsequent muon decay-in-flight in the Belle central drift chamber. The analyzed data sample of 988fb1988\,\text{fb}^{-1} collected by the Belle detector corresponds to approximately 912×106912\times10^6 τ+τ\tau^+ \tau^- pairs. We measure ξ=0.22±0.94(stat)±0.42(syst)\xi^\prime=0.22\pm0.94(\text{stat})\pm0.42(\text{syst}), which is in agreement with the Standard Model prediction of ξ=1\xi^\prime=1. Statistical uncertainty dominates in this study, being a limiting factor, while systematic uncertainty is well under control. Our analysis proved the practicability of this promising method and its prospects for further precise measurement in future experiments.Comment: 6 pages, 4 figures, submitted to Phys. Rev. Let

    Measurement of Angular Coefficients of BˉDνˉ\bar{B} \to D^* \ell \bar{\nu}_\ell: Implications for Vcb|V_{cb}| and Tests of Lepton Flavor Universality

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    We measure the complete set of angular coefficients JiJ_i for exclusive BˉDνˉ\bar{B} \to D^* \ell \bar{\nu}_\ell decays (=e,μ\ell = e, \mu). Our analysis uses the full 711fb1711\,\mathrm{fb}^{-1} Belle data set with hadronic tag-side reconstruction. The results allow us to extract the form factors describing the BDB \to D^* transition and the Cabibbo-Kobayashi-Maskawa matrix element Vcb|V_{\rm cb}|. Using recent lattice QCD calculations for the hadronic form factors, we find Vcb=(41.0±0.7)×103|V_{\rm cb}| = (41.0 \pm 0.7) \times 10^3 using the BGL parameterization, compatible with determinations from inclusive semileptonic decays. We search for lepton flavor universality violation as a function of the hadronic recoil parameter ww, and investigate the differences of the electron and muon angular distributions. We find no deviation from Standard Model expectations

    Search for charged-lepton flavor violation in Υ(2S)τ±\Upsilon(2S) \to \ell^\mp\tau^\pm (=e,μ\ell=e,\mu) decays at Belle

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    We report a search for the charged-lepton flavor violation in Υ(2S)τ±\Upsilon(2S) \to \ell^\mp\tau^\pm (=e,μ\ell=e,\mu) decays using a 25 fb125~\mathrm{fb}^{-1} Υ(2S)\Upsilon(2S) sample collected by the Belle detector at the KEKB e+ee^{+}e^{-} asymmetric-energy collider. We find no evidence for a signal and set upper limits on the branching fractions (B\mathcal{B}) at 90%\% confidence level. We obtain the most stringent upper limits: B(Υ(2S)μτ±)<0.26×106\mathcal{B}(\Upsilon(2S) \to \mu^{\mp}\tau^{\pm}) < 0.26 \times 10^{-6} and B(Υ(2S)eτ±)<1.02×106\mathcal{B}(\Upsilon(2S) \to e^{\mp}\tau^{\pm}) < 1.02 \times 10^{-6}.Comment: 11 pages, 3 figures, Submitted to JHE

    Observation of charmed strange meson pair production in Υ(2S)\Upsilon(2S) decays and in e+ee^{+}e^{-} annihilation at s=10.52 GeV\sqrt{s} = 10.52~ \rm{GeV}

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    We observe the process Υ(2S)Ds()+DsJ\Upsilon(2S)\to D_s^{(*)+} D_{sJ}^{-} and continuum production e+eDs()+DsJe^+e^- \to D_s^{(*)+} D_{sJ}^- at s=10.52\sqrt{s} = 10.52 GeV (and their charge conjugates) using the data samples collected by the Belle detector at KEKB, where DsJD_{sJ}^- is Ds1(2536)D_{s1}(2536)^- or Ds2(2573)D^{*}_{s2}(2573)^-. Both DsJD_{sJ}^- states are identified through their decay into KˉDˉ()\bar{K}\bar{D}^{(*)}. We measure the products of branching fractions B(Υ(2S)Ds()+DsJ)B(DsJKˉDˉ()){\cal B}(\Upsilon(2S) \to D_{s}^{(*)+} D_{sJ}^-) {\cal B}(D_{sJ}^-\to \bar{K} \bar{D}^{(*)}) and the Born cross sections σBorn(e+eDs()+DsJ)B(DsJKˉDˉ())\sigma^{\rm Born}(e^+e^- \to D_{s}^{(*)+} D_{sJ}^-) {\cal B}(D_{sJ}^-\to \bar{K} \bar{D}^{(*)}), and then compare the ratios R1B(Υ(2S)Ds()+DsJ)/B(Υ(2S)μ+μ)R_1 \equiv {\cal B}(\Upsilon(2S)\to D_{s}^{(*)+} D_{sJ}^-)/{\cal B}(\Upsilon(2S)\to\mu^{+}\mu^-) for Υ(2S)\Upsilon(2S) decays and R2σBorn(e+eDs()+DsJ)/σBorn(e+eμ+μ)R_2 \equiv \sigma^{\rm Born}(e^+e^-\to D_{s}^{(*)+}D_{sJ}^-)/\sigma^{\rm Born}(e^+e^-\to \mu^{+}\mu^-) for continuum production. We obtain R1/R2=9.7±2.3±1.1R_1/R_2 = 9.7\pm 2.3 \pm 1.1, 6.8±2.1±0.86.8 \pm 2.1 \pm 0.8, 10.2±3.3±2.510.2 \pm 3.3 \pm 2.5, and 3.4±2.1±0.53.4 \pm 2.1 \pm 0.5 for the Ds+Ds1(2536)D_s^+ D_{s1}(2536)^-, Ds+Ds1(2536)D_s^{*+} D_{s1}(2536)^-, Ds+Ds2(2573)D_s^+ D_{s2}^{*}(2573)^{-}, and Ds+Ds2(2573)D_s^{*+} D_{s2}^{*}(2573)^{-} final states in the DsJKDˉ()0D_{sJ}^-\to K^{-} \bar{D}^{(*)0} modes, respectively. Therefore, the strong decay is expected to dominate in the Υ(2S)Ds()+DsJ\Upsilon(2S)\to D_{s}^{(*)+}D_{sJ}^- processes. We also measure the ratios of branching fractions B(Ds1(2536)KS0D(2010))/B(Ds1(2536)KD(2007)0)=0.48±0.07±0.02{\cal B}(D_{s1}(2536)^-\to K_S^0 D^{*}(2010)^{-})/{\cal B}(D_{s1}(2536)^-\to K^{-} D^{*}(2007)^0) = 0.48 \pm 0.07 \pm 0.02 and B(Ds2(2573)KS0D)/B(Ds2(2573)KD0)=0.49±0.10±0.02{\cal B}(D_{s2}^{*}(2573)^- \to K_S^0 D^-)/{\cal B}(D_{s2}^{*}(2573)^- \to K^{-}D^0) = 0.49 \pm 0.10 \pm 0.02, which are consistent with isospin symmetry. The second ratio is the first measurement of this quantity. Here, the first uncertainties are statistical and the second are systematic

    Search for the lepton flavour violating decays B+K+τ±B^{+} \to K^{+} \tau^\pm \ell^\mp (=e,μ\ell = e, \mu) at Belle

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    We present a search for the lepton-flavour-violating decays B+K+τ±B^+ \to K^+ \tau^\pm \ell^\mp, with =(e,μ)\ell = (e, \mu), using the full data sample of 772×106772 \times 10^6 BBB\overline{B} pairs recorded by the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider. We use events in which one BB meson is fully reconstructed in a hadronic decay mode. We find no evidence for B±K±τB^\pm \to K^\pm \tau \ell decays and set upper limits on their branching fractions at the 90% confidence level in the (1(1-3)×1053) \times 10^{-5} range. The obtained limits are the world's best results.Comment: 14 pages, 6 figure

    Search for the double-charmonium state with ηcJ/ψ\eta_c J/\psi at Belle

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    We measure the cross section of e+eηcJ/ψe^+e^-\rightarrow\eta_c J/\psi at the Υ(nS)(n=1\Upsilon(nS) (n=1 -- 5)5) on-resonance and 10.52 GeV off-resonance energy points using the full data sample collected by the Belle detector with an integrated luminosity of 955 fb1955~\rm fb^{-1}. We also search for double charmonium production in e+eηcJ/ψe^+e^-\rightarrow\eta_c J/\psi via initial state radiation near the ηcJ/ψ\eta_c J/\psi threshold. No evident signal of the double charmonium state is found, but evidence for the e+eηcJ/ψe^+e^-\rightarrow\eta_c J/\psi process is found with a statistical significance greater than 3.3σ3.3\sigma near the ηcJ/ψ\eta_c J/\psi threshold. The average cross section near the threshold is measured and upper limits of cross sections are set for other regions

    Measurement of the e+eBs0Bˉs0Xe^+e^- \to B_s^0 \bar{B}_s^0 X cross section in the energy range from 10.6310.63 to 11.0211.02 GeV using inclusive Ds±D_s^{\pm} and D0D^0 production

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    We report the first measurement of the inclusive e+ebbˉDs±Xe^+e^- \to b\bar{b} \to D_s^{\pm}X and e+ebbˉD0/Dˉ0Xe^+e^- \to b\bar{b} \to D^0/\bar{D}^0X cross sections in the energy range from 10.6310.63 to 11.0211.02. Based on these results, we determine σ(e+eBs0Bˉs0X)\sigma(e^+ e^- \to B_s^0 \bar{B}_s^0 X) and σ(e+eBBˉX)\sigma(e^+ e^- \to B\bar{B}X) in the same energy range. We measure the fraction of Bs0B_s^0 events at Υ(10860)\Upsilon(10860) to be fs=(22.02.1+2.0)%f_{\rm s}=(22.0^{+2.0}_{-2.1})\%. We determine also the ratio of the Bs0B_s^0 inclusive branching fractions B(Bs0D0/Dˉ0X)/B(Bs0Ds±X)=0.416±0.018±0.092\mathcal{B}(B_s^0 \to D^0/\bar{D}^0X)/\mathcal{B}(B_s^0 \to D_s^{\pm} X)=0.416 \pm 0.018 \pm 0.092. The results are obtained using the data collected with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider
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