221 research outputs found

    2D fluid approaches of DC magnetron discharge

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    A two dimensional (r,z) time-dependent fluid model was developed and used to describe a DC planar magnetron discharge with cylindrical symmetry. The transport description of the charged species uses the corresponding first three moments of Boltzmann equation: continuity, momentum transfer and mean energy transfer (the latter one only for electrons), coupled with Poisson equation. An original way is proposed to treat the transport equations. Electron and ion momentum transport equations are reduced to the classical drift-diffusion expression of the fluxes since the presence of the magnetic field is introduced as an additional part in the electron flux, while for ions an effective electric field was considered. Thus, both continuity and mean energy transfer equations are solved in a classical manner. Numerical simulations were performed considering Argon as buffer gas, with a neutral pressure varying between 5 and 30 mtorr, a gas temperature from 300 to 350 K and cathode voltages lying from -200 up to -600 V. Results obtained for densities of the charged particle, fluxes and plasma potential are in good agreement with previous works.Laboratoire de Physique des Gaz el des Plasmas (LPGP).Consiliul National al Cercetarii Stiintifice din Invatamantul Superior (CNCSIS) - A/1344/40213/2003

    DC magnetron discharge fluid model using a new numerical scheme

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    Numerical modelling of an electrical discharge by fluid model can be accomplished through different procedures and approaches. A 2D time-dependent one was applied in order to describe a cylindrical symmetry Argon DC planar magnetron discharge. All transport equations, which means continuity and momentum transfer equations for electrons and ions and electron mean energy transport equation are solved in the same manner, using corrected classical drift-diffusion expressions for fluxes. For the validity of this last approach, the presence of magnetic field has been introduced as a correction in the electronic flux expression, while for ions an effective electric field has been considered. Plasma potential is given by Poisson equation

    Two-dimensional fluid approach to the dc magnetron discharge

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    A two-dimensional (r, z) time-dependent fluid model was developed and used to describe a dc planar magnetron discharge with cylindrical symmetry. The transport description of the charged species uses the corresponding first three moments of the Boltzmann equation: continuity, momentum transfer and mean energy transfer (the last one only for electrons), coupled with the Poisson equation. An original method is proposed to treat the transport equations. Electron and ion momentum transport equations are reduced to the classical drift-diffusion expression for the fluxes since the presence of the magnetic field is introduced as an additional part in the electron flux, while for ions an effective electric field was considered. Thus, both continuity and mean energy transfer equations are solved in a classical manner. Numerical simulations were performed considering argon as a buffer gas, with a neutral pressure varying between 5 and 30 mTorr, for different voltages applied on the cathode. Results obtained for densities of the charged particle, fluxes and plasma potential are in good agreement with those obtained in previous studies.C Costin would like to thank the French Government for his PhD fellowship at Laboratoire de Physique des Gaz et des Plasmas. We are also grateful to Dr T Minea for very helpful discussions. This work was partly supported by CNCSIS Romania, grant A/1344/2003

    Radio Detection of Cosmic Ray Air Shower by the CODALEMA Experiment

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    The possibilities of measuring Extremely High Energy Cosmic Rays (EHECR) by radio detection of electromagnetic pulses radiated during the development of extensive air showers in the atmosphere are investigated. We present the demonstrative CODALEMA experiment, set up at Nancay Radio-Observatory (France). The radio-decametric array has been adapted to measure radio transients in time coincidence between antennas.Comment: 4 pages, 4 figures, Proceedings of the 9th Pisa Meeting on Advanced Detectors, Isola d'Elba 2003, to be published in NIM

    Charmonium suppression in p-A collisions

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    The new high precision data on charmonium production in proton-nucleus collisions by the E866/NuSea collaboration at Fermilab allow - together with older data at lower energies - to fix a unique set of parameters for the standard production and absorption scenario of charmonium in a proton-nucleus reaction. In this scenario the c-cbar pair is formed in an octet state, emits a gluon and continues its radial expansion in a singlet state until it has reached the charmonium radius. In all three phases it can interact with the nuclear environment. We find that the lifetime of the octet state is much shorter than acceptable on physical grounds. This challenges the physical reality of the first phase in the standard scenario.Comment: 8 pages, 10 figure

    Modeling the Pion and Kaon Form Factors in the Timelike Region

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    New, accurate measurements of the pion and kaon electromagnetic form factors are expected in the near future from experiments at electron-positron colliders,using the radiative return method. We construct a model for the timelike pion electromagnetic form factor, that is valid also at momentum transfers far above the ρ\rho resonance. The ansatz is based on vector dominance and includes a pattern of radial excitations expected from dual resonance models.The form factor is fitted to the existing data in the timelike region, continued to the spacelike region and compared with the measurements there and with the QCD predictions. Furthermore, the model is extended to the kaon electromagnetic form factor. Using isospin and SU(3)-flavour symmetry relations we extract the isospin-one contribution and predict the kaon weak form factor accessible in semileptonic τ\tau decays.Comment: 31 pages, 7 figures,latex, one reference changed, version to appear in Eur.Phys.J

    Nuclear effects in g1A(x,Q2)g_{1A}(x,Q^2) at small xx in deep inelastic scattering on 7^7Li and 3^3He

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    We suggest to use polarized nuclear targets of 7^7Li and 3^3He to study nuclear effects in the spin dependent structure functions g1A(x,Q2)g_{1A}(x,Q^2). These effects are expected to be enhanced by a factor of two as compared to the unpolarized targets. We predict a significant xx dependence at 104÷103x0.210^{-4} \div 10^{-3} \leq x \leq 0.2 of g1A(x,Q2)/g1N(x,Q2)g_{1A}(x,Q^2)/g_{1N}(x,Q^2) due to nuclear shadowing and nuclear enhancement. The effect of nuclear shadowing at x103x \approx 10^{-3} is of an order of 16% for g1A=7n.s.3/2(x,Q2)/g1Nn.s.(x,Q2)g_{1A=7}^{n.s. 3/2}(x,Q^2)/g_{1N}^{n.s.}(x,Q^2) and 10% for g1A=3n.s(x,Q2)/g1Nn.s.(x,Q2)g_{1A=3}^{n.s}(x,Q^2)/g_{1N}^{n.s.}(x,Q^2). By imposing the requirement that the Bjorken sum rule is satisfied we model the effect of enhancement. We find the effect of enhancement at x0.125(0.15)x \approx 0.125 (0.15) to be of an order of 20(55)20 (55)% for g1A=7n.s.3/2(x,Q2)/g1Nn.s.(x,Q2)g_{1A=7}^{n.s. 3/2}(x,Q^2)/g_{1N}^{n.s.}(x,Q^2) and 14(40)14 (40)% for g1A=3n.s(x,Q2)/g1Nn.s.(x,Q2)g_{1A=3}^{n.s}(x,Q^2)/g_{1N}^{n.s.}(x,Q^2), if enhancement occupies the region 0.05x0.20.05 \leq x \leq 0.2 (0.1x0.20.1 \leq x \leq 0.2). We predict a 2% effect in the difference of the scattering cross sections of deep inelastic scattering of an unpolarized projectile off 7^7Li with MJM_{J}=3/2 and MJM_{J}=1/2. We also show explicitly that the many-nucleon description of deep inelastic scattering off 7^7Li becomes invalid in the enhancement region 0.05<x0.20.05 < x \leq 0.2.Comment: 29 pages, 5 figures, RevTe

    Radio emission of extensive air shower at CODALEMA: Polarization of the radio emission along the v*B vector

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    Cosmic rays extensive air showers (EAS) are associated with transient radio emission, which could provide an efficient new detection method of high energy cosmic rays, combining a calorimetric measurement with a high duty cycle. The CODALEMA experiment, installed at the Radio Observatory in Nancay, France, is investigating this phenomenon in the 10^17 eV region. One challenging point is the understanding of the radio emission mechanism. A first observation indicating a linear relation between the electric field produced and the cross product of the shower axis with the geomagnetic field direction has been presented (B. Revenu, this conference). We will present here other strong evidences for this linear relationship, and some hints on its physical origin.Comment: Contribution to the 31st International Cosmic Ray Conference, Lodz, Poland, July 2009. 4 pages, 8 figures. v2: Typo fixed, arxiv references adde

    Lambda polarization and single-spin left-right asymmetry in diffractive hadron-hadron collisions

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    We discuss Lambda polarization and single-spin left-right asymmetry in diffractive hadron-hadron scattering at high energies. We show that the physical picture proposed in a recent Letter is consistent with the experimental observation that Λ\Lambda polarization in the diffractive process, ppΛK+ppp\to \Lambda K^+p, is much higher than that in the inclusive reaction, ppΛXpp\to \Lambda X. We make predictions for the left-right asymmetry, A_N, and for the spin transfer, DNNΛD_{NN}^\Lambda, in the single-spin process p()pΛK+pp(\uparrow)p\to \Lambda K^+p and suggest further experimental tests of the proposed picture.Comment: 14 pages, 3 ps-figures. Phys. Rev. D (in press

    Probing partonic structure in gamma* gamma -> pi pi near threshold

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    Hadron pair production gamma* gamma -> h hbar in the region where the c.m. energy is much smaller than the photon virtuality can be described in a factorized form, as the convolution of a partonic handbag diagram and generalized distribution amplitudes which are new non-perturbative functions describing the exclusive fragmentation of a quark-antiquark pair into two hadrons. Scaling behavior and a selection rule on photon helicity are signatures of this mechanism. The case where h is a pion is emphasized.Comment: 8 pages, 1 figure, LaTeX2
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