270 research outputs found

    Neutron Detection in the A2 Collaboration Experiment on Neutral Pion Photo-production on Neutron

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    Neutron detection is of crucial importance for the neutral pion photo-production study on a neutron target that now is in progress at MAMI. Two electro-magnetic calorimeters, based on NaI and BaF2 crystals, are used in the A2 experiment. While these calorimeters are optimized for pion decay photon detection, they have a reason able efficiency for neutron detection also. The paper describes the method, which has been used to measure this efficiency using the same data taken for pion photo-production study on deuterium target with tagged photon been of 800 MeV maximal energy. The detection efficiency is a rising function of neutron momentum that reaches 40% near 1 GeV/c

    SiPM technology applied to radiation sensor development

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    The Silicon Photo-Multiplier (SiPM) being yet in its infancy, a full protocol for the sensor characterization has been developed and implemented at the Physics Department of Universita\u2019 dell\u2019Insubria. Sensors from different producers have been analyzed and compared, in view of the integration in the instruments for radiation detection. Exemplary illustrations are reported here, together with the first results on real-time dosimetry in mammography

    Measurement of pi^0 photoproduction on the proton at MAMI C

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    Differential cross sections for the gamma p -> pi^0 p reaction have been measured with the A2 tagged-photon facilities at the Mainz Microtron, MAMI C, up to the center-of-mass energy W=1.9 GeV. The new results, obtained with a fine energy and angular binning, increase the existing quantity of pi^0 photoproduction data by ~47%. Owing to the unprecedented statistical accuracy and the full angular coverage, the results are sensitive to high partial-wave amplitudes. This is demonstrated by the decomposition of the differential cross sections in terms of Legendre polynomials and by further comparison to model predictions. A new solution of the SAID partial-wave analysis obtained after adding the new data into the fit is presented.Comment: 13 pages, 12 figures, 1 tabl

    Measurement of hadronic cross section and preliminary results on the pion form factor using the radiative return at DAPHNE

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    In the fixed energy environment of the e+ee^{+}e^{-} collider DAΦ\PhiNE, KLOE can measure the cross section of the process e+ee^{+}e^{-} \to hadrons as a function of the hadronic system energy using the radiative return. At energies below 1 GeV, e+eρπ+πe^{+}e^{-} \to \rho \to \pi^{+}\pi^{-} is the dominating hadronic process. We report here on the status of the analysis for the e^{+}e^{-} \to \ppg channel, which allows to obtain a preliminary measurement of the pion form factor using an integrated luminosity of 73pb1\sim73 pb^{-1}.Comment: Invited talk at the Seventh International Workshop on Tau Lepton Physics (TAU02-WE07), Santa Cruz, Ca, USA, Sept 2002, 9 pages, LaTeX, 9 eps figure

    Precision measurement of σ(e+eπ+πγ)/σ(e+eμ+μγ)\sigma(e^+e^-\rightarrow\pi^+\pi^-\gamma)/\sigma(e^+e^-\rightarrow \mu^+\mu^-\gamma) and determination of the π+π\pi^+\pi^- contribution to the muon anomaly with the KLOE detector

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    We have measured the ratio σ(e+eπ+πγ)/σ(e+eμ+μγ)\sigma(e^+e^-\rightarrow\pi^+\pi^-\gamma)/\sigma(e^+e^-\rightarrow \mu^+\mu^-\gamma), with the KLOE detector at DAΦ\PhiNE for a total integrated luminosity of \sim 240 pb1^{-1}. From this ratio we obtain the cross section σ(e+eπ+π)\sigma(e^+e^-\rightarrow\pi^+\pi^-). From the cross section we determine the pion form factor Fπ2|F_\pi|^2 and the two-pion contribution to the muon anomaly aμa_\mu for 0.592<Mππ<0.9750.592<M_{\pi\pi}<0.975 GeV, Δππaμ\Delta^{\pi\pi} a_\mu= (385.1±1.1stat±2.7sys+theo)×1010({\rm 385.1\pm1.1_{stat}\pm2.7_{sys+theo}})\times10^{-10}. This result confirms the current discrepancy between the Standard Model calculation and the experimental measurement of the muon anomaly.Comment: 18 pages, 8 figures, minor text corrections, one table added, version to appear on Physics Letters
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