604 research outputs found

    Search for a dark vector gauge boson decaying to π+π\pi^+ \pi^- using ηπ+πγ\eta \rightarrow \pi^+\pi^- \gamma decays

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    We report a search for a dark vector gauge boson UU^\prime that couples to quarks in the decay chain D+D0π+,D0KS0η,ηUγD^{*+} \to D^0 \pi^+, D^0 \to K^0_S \eta, \eta \to U^\prime \gamma, Uπ+πU^\prime \to \pi^+ \pi^-. No signal is found and we set a mass-dependent limit on the baryonic fine structure constant of 10310210^{-3} - 10^{-2} in the UU^\prime mass range of 290 to 520 MeV/c2c^2. This analysis is based on a data sample of 976 fb1^{-1} collected by the Belle experiment at the KEKB asymmetric-energy e+ee^+e^- collider.Comment: 6 pages, 4 figure

    Observation of D0ρ0γD^0\to \rho^0\gamma and search for CPCP violation in radiative charm decays

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    We report the first observation of the radiative charm decay D0ρ0γD^0 \to \rho^0 \gamma and the first search for CPCP violation in decays D0ρ0γD^0 \to \rho^0 \gamma, ϕγ\phi\gamma, and K0γ\overline{K}{}^{*0} \gamma, using a data sample of 943 fb1^{-1} collected with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. The branching fraction is measured to be B(D0ρ0γ)=(1.77±0.30±0.07)×105\mathcal{B}(D^0 \to \rho^0 \gamma)=(1.77 \pm 0.30 \pm 0.07) \times 10^{-5}, where the first uncertainty is statistical and the second is systematic. The obtained CPCP asymmetries, ACP(D0ρ0γ)=+0.056±0.152±0.006\mathcal{A}_{CP}(D^0 \to \rho^0 \gamma)=+0.056 \pm 0.152 \pm 0.006, ACP(D0ϕγ)=0.094±0.066±0.001\mathcal{A}_{CP}(D^0 \to \phi \gamma)=-0.094 \pm 0.066 \pm 0.001, and ACP(D0K0γ)=0.003±0.020±0.000\mathcal{A}_{CP}(D^0 \to \overline{K}{}^{*0} \gamma)=-0.003 \pm 0.020 \pm 0.000, are consistent with no CPCP violation. We also present an improved measurement of the branching fractions B(D0ϕγ)=(2.76±0.19±0.10)×105\mathcal{B}(D^0 \to \phi \gamma)=(2.76 \pm 0.19 \pm 0.10) \times 10^{-5} and B(D0K0γ)=(4.66±0.21±0.21)×104\mathcal{B}(D^0 \to \overline{K}{}^{*0} \gamma)=(4.66 \pm 0.21 \pm 0.21) \times 10^{-4}

    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 Λc+ϕpπ0\Lambda_c^+\to\phi p \pi^0 and branching fraction measurement of Λc+Kπ+pπ0\Lambda_c^+\to K^-\pi^+ p \pi^0

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    We have searched for the Cabibbo-suppressed decay Λc+ϕpπ0\Lambda_c^+\to\phi p\pi^0 in e+ee^+e^- collisions using a data sample corresponding to an integrated luminosity of 915 fb1\rm fb^{-1}. The data were collected by the Belle experiment at the KEKB e+ee^+e^- asymmetric-energy collider running at or near the Υ(4S)\Upsilon(4S) and Υ(5S)\Upsilon(5S) resonances. No significant signal is observed, and we set an upper limit on the branching fraction of B(Λc+ϕpπ0)<15.3×105\mathcal{B}(\Lambda_c^+\to \phi p\pi^0) <15.3\times10^{-5} at 90% confidence level. The contribution for nonresonant Λc+K+Kpπ0\Lambda_c^+\to K^+K^- p\pi^0 decays is found to be consistent with zero and the corresponding upper limit on its branching fraction is set to be B(Λc+K+Kpπ0)NR<6.3×105\mathcal{B}(\Lambda_c^+\to K^+K^-p\pi^0)_{\rm NR} <6.3\times10^{-5} at 90% confidence level. We also measure the branching fraction for the Cabibbo-favored decay Λc+Kπ+pπ0\Lambda_c^+\to K^-\pi^+p\pi^0; the result is B(Λc+Kπ+pπ0)=(4.42±0.05(stat.)±0.12(syst.)±0.16(BNorm))%\mathcal{B}(\Lambda_c^+\to K^-\pi^+p\pi^0)= (4.42\pm0.05\, (\rm stat.) \pm 0.12\, (\rm syst.) \pm 0.16\, (\mathcal{B}_{\rm Norm}))\%, which is the most precise measurement to date. Finally, we have searched for an intermediate hidden-strangeness pentaquark decay Ps+ϕpP^+_s\to\phi p. We see no evidence for this intermediate decay and set an upper limit on the product branching fraction of B(Λc+Ps+π0)×B(Ps+ϕp)<8.3×105{\cal B}(\Lambda_c^+\to P^+_s \pi^0)\times {\cal B}(P^+_s\to\phi p) <8.3\times 10^{-5} at 90% confidence level.Comment: 8 pages, 5 figures, 1 table, minor text change in version

    Search for D0D^{0} decays to invisible final states at Belle

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    We report the result from the first search for D0D^0 decays to invisible final states. The analysis is performed on a data sample of 924 fb1\rm{fb}^{-1} collected at and near the Υ(4S)\Upsilon(4S) and Υ(5S)\Upsilon(5S) resonances with the Belle detector at the KEKB asymmetric-energy e+ee^{+}e^{-} collider. The absolute branching fraction is determined using an inclusive D0D^0 sample, obtained by fully reconstructing the rest of the particle system including the other charmed particle. No significant signal yield is observed and an upper limit of 9.4×1059.4\times 10^{-5} is set on the branching fraction of D0D^0 to invisible final states at 90\% confidence level.Comment: 17 pages, 4 figures, submitted to PRD(RC

    Measurement of the τ\tau lepton polarization and R(D)R(D^*) in the decay BˉDτνˉτ\bar{B} \rightarrow D^* \tau^- \bar{\nu}_\tau with one-prong hadronic τ\tau decays at Belle

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    With the full data sample of 772×106772 \times 10^6 BBˉB{\bar B} pairs recorded by the Belle detector at the KEKB electron-positron collider, the decay BˉDτνˉτ\bar{B} \rightarrow D^* \tau^- \bar{\nu}_\tau is studied with the hadronic τ\tau decays τπντ\tau^- \rightarrow \pi^- \nu_\tau and τρντ\tau^- \rightarrow \rho^- \nu_\tau. The τ\tau polarization Pτ(D)P_\tau(D^*) in two-body hadronic τ\tau decays is measured, as well as the ratio of the branching fractions R(D)=B(BˉDτνˉτ)/B(BˉDνˉ)R(D^{*}) = \mathcal{B}(\bar {B} \rightarrow D^* \tau^- \bar{\nu}_\tau) / \mathcal{B}(\bar{B} \rightarrow D^* \ell^- \bar{\nu}_\ell), where \ell^- denotes an electron or a muon. Our results, Pτ(D)=0.38±0.51(stat)0.16+0.21(syst)P_\tau(D^*) = -0.38 \pm 0.51 {\rm (stat)} ^{+0.21}_{-0.16} {\rm (syst)} and R(D)=0.270±0.035(stat)0.025+0.028(syst)R(D^*) = 0.270 \pm 0.035{\rm (stat)} ^{+0.028}_{-0.025}{\rm (syst)}, are consistent with the theoretical predictions of the Standard Model. The polarization values of Pτ(D)>+0.5P_\tau(D^*) > +0.5 are excluded at the 90\% confidence level.Comment: 17 pages, 11 figures, submitted to Physical Review

    Invariant-mass and fractional-energy dependence of inclusive production of di-hadrons in e+ee^+e^- annihilation at s=\sqrt{s}= 10.58 GeV

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    The inclusive cross sections for di-hadrons of charged pions and kaons (e+ehhXe^+e^- \rightarrow hhX) in electron-positron annihilation are reported. They are obtained as a function of the total fractional energy and invariant mass for any di-hadron combination in the same hemisphere as defined by the thrust event-shape variable and its axis. Since same-hemisphere di-hadrons can be assumed to originate predominantly from the same initial parton, di-hadron fragmentation functions are probed. These di-hadron fragmentation functions are needed as an unpolarized baseline in order to quantitatively understand related spin-dependent measurements in other processes and to apply them to the extraction of quark transversity distribution functions in the nucleon. The di-hadron cross sections are obtained from a 655fb1655\,{\rm fb}^{-1} data sample collected at or near the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider.Comment: 21 pages, 18 figures plus 25 figures in supplemental material, submitted to PR

    Study of Excited Ξc\Xi_c States Decaying into Ξc0\Xi_c^0 and Ξc+\Xi_c^+ Baryons

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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 excited Ξc\Xi_c states that decay, via the emission of photons and/or charged pions, into Ξc0\Xi_c^0 or Ξc+\Xi_c^+ ground state charmed-strange baryons. We present new measurements of the masses of all members of the Ξc\Xi_c^{\prime}, Ξc(2645)\Xi_c(2645), Ξc(2790)\Xi_c(2790), Ξc(2815)\Xi_c(2815), and Ξc(2980)\Xi_c(2980) isodoublets, measurements of the intrinsic widths of those that decay strongly, and evidence of previously unknown transitions.Comment: Submitted to PR

    Search for CPCP violation in the D+π+π0D^{+}\to\pi^{+}\pi^{0} decay at Belle

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    We search for CPCP violation in the charged charm meson decay D+π+π0D^{+}\to\pi^{+}\pi^{0}, based on a data sample corresponding to an integrated luminosity of 921 fb1\rm 921~fb^{-1} collected by the Belle experiment at the KEKB e+ee^{+}e^{-} asymmetric-energy collider. The measured CPCP violating asymmetry is [+2.31±1.24(stat)±0.23(syst)]%[+2.31\pm1.24({\rm stat})\pm0.23({\rm syst})]\%, which is consistent with the standard model prediction and has a significantly improved precision compared to previous results.Comment: 8 pages, 3 figure

    Evidence for Isospin Violation and Measurement of CPCP Asymmetries in BK(892)γB \to K^{\ast}(892) \gamma

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    We report the first evidence for isospin violation in BKγB \to K^* \gamma and the first measurement of difference of CPCP asymmetries between B+K+γB^+ \to K^{*+} \gamma and B0K0γB^0 \to K^{*0} \gamma. This analysis is based on the data sample containing 772×106BBˉ772 \times 10^6 B\bar{B} pairs that was collected with the Belle detector at the KEKB energy-asymmetric e+ee^+ e^- collider. We find evidence for the isospin violation with a significance of 3.1σ\sigma, Δ0+=(+6.2±1.5(stat.)±0.6(syst.)±1.2(f+/f00))\Delta_{0+} = (+6.2 \pm 1.5 ({\rm stat.}) \pm 0.6 ({\rm syst.}) \pm 1.2 (f_{+-}/f_{00}))\%, where the third uncertainty is due to the uncertainty on the fraction of B+BB^+B^- to B0Bˉ0B^0\bar{B}^0 production in Υ(4S)\Upsilon(4S) decays. The measured value is consistent with predictions of the SM. The result for the difference of CPCP asymmetries is ΔACP=(+2.4±2.8(stat.)±0.5(syst.))\Delta A_{CP} = (+2.4 \pm 2.8({\rm stat.}) \pm 0.5({\rm syst.}))\%, consistent with zero. The measured branching fractions and CPCP asymmetries for charged and neutral BB meson decays are the most precise to date. We also calculate the ratio of branching fractions of B0K0γB^0 \to K^{*0} \gamma to Bs0ϕγB_s^0 \to \phi \gamma.Comment: 11 pages, 7 figures. shown at FPCP2017. accepted by PR
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