127 research outputs found

    Study of PANDA Barrel DIRC design options

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    Study of PANDA Barrel DIRC design options

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    Time-based simulation of the PANDA barrel DIRC

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    Development of a New Clusterization Method for the GEM-TPC Detector

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    The Facility for Antiproton and Ion Research FAIR, in Darmstadt Germany, will be one of the largest accelerator laboratories worldwide. The Superconducting FRagment Separator (Super-FRS)* is one of its main components. The Super-FRS can produce, separate and deliver high-energy radioactive beams with intensities up to 1e11 ions/s, covering projectiles from protons up to uranium and it can be used as an independent experimental device. The Gas Electron Multiplier-based Time Projection Chambers (GEM-TPC) in twin configuration is a newly developed beam tracking detector capable of providing spatial resolution of less than 1 mm with a tracking efficiency close to 100% at 1 MHz counting rate. The GEM-TPC (HGB4) was tested at the FRagment Separator (FRS), with 238U beam at 850 MeV/u. A new clusterization method was developed, for the first time and used for an analysis. This method allowed to access to waveforms of each strip signal within a single trigger in an event-by-event basis. The procedures involved in this method will be shown in details.Peer reviewe

    Feasibility studies of time-like proton electromagnetic form factors at PANDA at FAIR

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    Simulation results for future measurements of electromagnetic proton form factors at \PANDA (FAIR) within the PandaRoot software framework are reported. The statistical precision with which the proton form factors can be determined is estimated. The signal channel pˉpe+e\bar p p \to e^+ e^- is studied on the basis of two different but consistent procedures. The suppression of the main background channel, i.e.\textit{i.e.} pˉpπ+π\bar p p \to \pi^+ \pi^-, is studied. Furthermore, the background versus signal efficiency, statistical and systematical uncertainties on the extracted proton form factors are evaluated using two different procedures. The results are consistent with those of a previous simulation study using an older, simplified framework. However, a slightly better precision is achieved in the PandaRoot study in a large range of momentum transfer, assuming the nominal beam conditions and detector performance

    Measurements of h_c(^1P_1) in psi' Decays

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    We present measurements of the charmonium state hc(1P1)h_c(^1P_1) made with 106M ψ\psi' events collected by BESIII at BEPCII. Clear signals are observed for ψπ0hc\psi'\to\pi^0 h_c with and without the subsequent radiative decay hcγηch_c\to\gamma\eta_c. First measurements of the absolute branching ratios B(ψπ0hc)=(8.4±1.3±1.0)×104\mathcal{B}(\psi' \to\pi^0 h_c) = (8.4 \pm 1.3 \pm 1.0) \times 10^{-4} and B(hcγηc)=(54.3±6.7±5.2)\mathcal{B}(h_c \to \gamma \eta_c) = (54.3 \pm 6.7 \pm5.2)% are presented. A statistics-limited determination of the previously unmeasured hch_c width leads to an upper limit Γ(hc)<1.44\Gamma(h_c)<1.44 MeV (90% confidence). Measurements of M(hc)=3525.40±0.13±0.18M(h_c) = 3525.40 \pm 0.13 \pm 0.18 MeV/c2c^2 and B(ψπ0hc)×B(hcγηc)=(4.58±0.40±0.50)×104\mathcal{B}(\psi'\to \pi^0 h_c) \times \mathcal{B}(h_c \to \gamma\eta_c) = (4.58 \pm 0.40 \pm 0.50) \times 10^{-4} are consistent with previous results.Comment: 5 pages, 1 figure, accepted for publication in Physical Review Letter

    First observation of J/\psi and \psi(2S) decaying to n K^0_S\bar\Lambda +c.c

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    The decays of \jpsi and \psip to nKS0Λˉ+c.c.{n}{K^0_S}\bar{\Lambda}+c.c. are observed and measured for the first time, and the perturbative QCD ``12%'' rule is tested, based on 5.8×1075.8 \times 10^7 \jpsi and 1.4×1071.4 \times 10^7 \psip events collected with BESII detector at the Beijing Electron-Positron Collider. No obvious enhancement near nΛˉn\bar{\Lambda} threshold in \jpsi \to {n}{K^0_S}\bar{\Lambda}+c.c. is observed, and the upper limit on the branching ratio of \jpsi \to {K^0_S} X, X \to n \bar \Lambda is determined.Comment: 10 pages, 10 figure
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