304 research outputs found

    Evaluation of two thermal neutron detection units consisting of ZnS/6{}^6LiF scintillating layers with embedded WLS fibers read out with a SiPM

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    Two single channel detection units for thermal neutron detection are investigated in a neutron beam. They consist of two ZnS/6{}^6LiF scintillating layers sandwiching an array of WLS fibers. The pattern of this units can be repeated laterally and vertically in order to build up a one dimensional position sensitive multi-channel detector with the needed sensitive surface and with the required neutron absorption probability. The originality of this work arises from the fact that the WLS fibers are read out with SiPMs instead of the traditionally used PMTs or MaPMTs. The signal processing system is based on a photon counting approach. For SiPMs with a dark count rate as high as 0.7 MHz, a trigger efficiency of 80% is achieved together with a system background rate lower than 10−3{10}^{-3} Hz and a dead time of 30 μ\mus. No change of performance is observed for neutron count rates of up to 3.6 kHz.Comment: Submitted to Nuclear Instruments and Methods

    Magnetic Moments of the Baryon Decuplet in a Relativistic Quark Model

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    The magnetic moments of the baryon decuplet are calculated in a relativistic constituent quark model using the light-front formalism. Of particular interest are the magnetic moments of the Ω−\Omega^- and Δ++\Delta^{++} for which new recent experimental measurements are available. Our calculation for the magnetic moment ratio μ(Δ++)/μ(p)\mu(\Delta^{++})/\mu(p) is in excellent agreement with the experimental ratio, while our ratio μ(Ω−)/μ(Λ0)\mu(\Omega^-)/\mu(\Lambda^0) is slightly higher than the experimental ratio.Comment: 10 pages ReVTeX, SLAC-PUB-621

    Semileptonic Hyperon Decays on the Lattice: an Exploratory Study

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    We present preliminary results of an exploratory lattice study of the vector form factor f1(q2=0)f_1(q^2 = 0) relevant for the semileptonic hyperon decay Σ−−−>nlν\Sigma^{-} --> n l \nu. This study is based on the same method used for the extraction of f+(0)f^+(0) for the decay K0−−>π−lνK^0 --> \pi^{-} l \nu. The main purpose of this study is to test the method for hyperon form factors in order to estimate the precision that can be reached and the importance of SU(3)-breaking effects.Comment: 3 pages, 5 figures, talk presented at Lattice2004(weak), Fermilab, Batavia, Illinois, 21-26 June 200

    Charge form factor of π\pi and KK mesons

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    The charge form factor of π\pi and KK mesons is evaluated adopting a relativistic constituent quark model based on the light-front formalism. The relevance of the high-momentum components of the meson wave function, for values of the momentum transfer accessible to CEBAFCEBAF energies, is illustrated. The predictions for the elastic form factor of π\pi and KK mesons are compared with the results of different relativistic approaches, showing that the measurements of the pion and kaon form factors planned at CEBAFCEBAF could provide information for discriminating among various models of the meson structure.Comment: 8 pages, latex, 4 figures available as separate .uu fil

    Sivers and Boer-Mulders functions in Light-Cone Quark Models

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    Results for the naive-time-reversal-odd quark distributions in a light-cone quark model are presented. The final-state interaction effects are generated via single-gluon exchange mechanism. The formalism of light-cone wave functions is used to derive general expressions in terms of overlap of wave-function amplitudes describing the different orbital angular momentum components of the nucleon. In particular, the model predictions show a dominant contribution from S- and P-wave interference in the Sivers function and a significant contribution also from the interference of P and D waves in the Boer-Mulders function. The favourable comparison with existing phenomenological parametrizations motivates further applications to describe azimuthal asymmetries in hadronic reactions.Comment: references and explanations added; version to appear in Phys. Rev.
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