6 research outputs found

    Geodetic data analysis of VGOS experiments

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    Very Long Baseline Interferometry (VLBI) serves as one of the common geodetic methods to define the global reference frames and monitor Earth\u27s orientation variations. The technical upgrade of the VLBI method known as the VLBI Global Observing System (VGOS) includes a critical re-design of the observed frequencies from the dual band mode (S and X band, i.e. 2 GHz and 8 GHz) to observations in a broadband (2-14 GHz). Since 2019 the first VGOS experiments are available for the geodetic analysis in free access at the International VLBI service for Geodesy and Astrometry (IVS). Also regional-only subnetworks such as European VLBI stations have succeeded already in VGOS mode. Based on these brand-new observations we review the current geodetic data analysis workflow to build a bridge between geodetic observed delays derived from different bands

    Measurement of branching fractions of Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 and Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta at Belle

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    We present a study of a singly Cabibbo-suppressed decay Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 and a Cabibbo-favored decay Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta based on 980 fb1\rm fb^{-1} of data collected by the Belle detector, operating at the KEKB energy-asymmetric e+ee^+e^- collider. We measure their branching fractions relative to Λc+pKS0\Lambda_c^+\to{}pK_S^0: B(Λc+pKS0KS0)/B(Λc+pKS0)=(1.48±0.08±0.04)×102\mathcal{B}(\Lambda_c^+\to{}pK_S^0K_S^0)/\mathcal{B}(\Lambda_c^+\to{}pK_S^0)={(1.48 \pm 0.08 \pm 0.04)\times 10^{-2}} and B(Λc+pKS0η)/B(Λc+pKS0)=(2.73±0.06±0.13)×101\mathcal{B}(\Lambda_c^+\to{}pK_S^0\eta)/\mathcal{B}(\Lambda_c^+\to{}pK_S^0)={(2.73\pm 0.06\pm 0.13)\times 10^{-1}}. Combining with the world average B(Λc+pKS0)\mathcal{B}(\Lambda_c^+\to{}pK_S^0), we have the absolute branching fractions: B(Λc+pKS0KS0)=(2.35±0.12±0.07±0.12)×104\mathcal{B}(\Lambda_c^+\to{}pK_S^0K_S^0) = {(2.35\pm 0.12\pm 0.07 \pm 0.12 )\times 10^{-4}} and B(Λc+pKS0η)=(4.35±0.10±0.20±0.22)×103\mathcal{B}(\Lambda_c^+\to{}pK_S^0\eta) = {(4.35\pm 0.10\pm 0.20 \pm 0.22 )\times 10^{-3}}. The first and second uncertainties are statistical and systematic, respectively, while the third ones arise from the uncertainty on B(Λc+pKS0)\mathcal{B}(\Lambda_c^+\to{}pK_S^0). The mode Λc+pKS0KS0\Lambda_c^+\to{}pK_S^0K_S^0 is observed for the first time and has a statistical significance of > ⁣10σ>\!10\sigma. The branching fraction of Λc+pKS0η\Lambda_c^+\to{}pK_S^0\eta has been measured with a threefold improvement in precision over previous results and is found to be consistent with the world average

    Measurement of the Ωc0\Omega_c^0 lifetime at Belle II

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    We report on a measurement of the Ωc0\Omega_c^0 lifetime using Ωc0Ωπ+\Omega_c^0 \to \Omega^-\pi^+ decays reconstructed in e+eccˉe^+e^-\to c\bar{c} data collected by the Belle II experiment and corresponding to 207 fb1207~{\rm fb^{-1}} of integrated luminosity. The result, τ(Ωc0)=243±48(stat)±11(syst) fs\rm\tau(\Omega_c^0)=243\pm48( stat)\pm11(syst)~fs, agrees with recent measurements indicating that the Ωc0\Omega_c^0 is not the shortest-lived weakly decaying charmed baryon

    Measurement of the Ωc0\Omega_c^0 lifetime at Belle II

    No full text
    We report on a measurement of the Ωc0\Omega_c^0 lifetime using Ωc0Ωπ+\Omega_c^0 \to \Omega^-\pi^+ decays reconstructed in e+eccˉe^+e^-\to c\bar{c} data collected by the Belle II experiment and corresponding to 207 fb1207~{\rm fb^{-1}} of integrated luminosity. The result, τ(Ωc0)=243±48(stat)±11(syst) fs\rm\tau(\Omega_c^0)=243\pm48( stat)\pm11(syst)~fs, agrees with recent measurements indicating that the Ωc0\Omega_c^0 is not the shortest-lived weakly decaying charmed baryon

    Measurement of the Ωc0\Omega_c^0 lifetime at Belle II

    No full text
    We report on a measurement of the Ωc0\Omega_c^0 lifetime using Ωc0Ωπ+\Omega_c^0 \to \Omega^-\pi^+ decays reconstructed in e+eccˉe^+e^-\to c\bar{c} data collected by the Belle II experiment and corresponding to 207 fb1207~{\rm fb^{-1}} of integrated luminosity. The result, τ(Ωc0)=243±48(stat)±11(syst) fs\rm\tau(\Omega_c^0)=243\pm48( stat)\pm11(syst)~fs, agrees with recent measurements indicating that the Ωc0\Omega_c^0 is not the shortest-lived weakly decaying charmed baryon
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