8,776 research outputs found

    A study of a collision avoidance system mounted on a curved ground plane

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    Research conducted on a traffic advisory and collision avoidance system (TCAS 2) mounted on a curved ground plane is described. It is found that a curved finite ground plane can be used as a good simulation model for the fuselage of an aircraft but may not be good enough to model a whole aircraft due to the shadowing of the vertical stabilizer, wings, etc. The surface curvature of this curved disc significantly affects the monopulse characteristics in the azimuth plane but not as much in the elevation plane. These variations of the monopulse characteristics verify the need of a lookup table for the 64 azimuth beam positions. The best location of a TCAS 2 array on a Boeing 737 is to move it as far from the vertical stabilizer as possible

    Impact of noise on a dynamical system: prediction and uncertainties from a swarm-optimized neural network

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    In this study, an artificial neural network (ANN) based on particle swarm optimization (PSO) was developed for the time series prediction. The hybrid ANN+PSO algorithm was applied on Mackey--Glass chaotic time series in the short-term x(t+6)x(t+6). The performance prediction was evaluated and compared with another studies available in the literature. Also, we presented properties of the dynamical system via the study of chaotic behaviour obtained from the predicted time series. Next, the hybrid ANN+PSO algorithm was complemented with a Gaussian stochastic procedure (called {\it stochastic} hybrid ANN+PSO) in order to obtain a new estimator of the predictions, which also allowed us to compute uncertainties of predictions for noisy Mackey--Glass chaotic time series. Thus, we studied the impact of noise for several cases with a white noise level (σN\sigma_{N}) from 0.01 to 0.1.Comment: 11 pages, 8 figure

    Influence of the photon - neutrino processes on magnetar cooling

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    The photon-neutrino processes γe±→e±ννˉ\gamma e^{\pm} \to e^{\pm} \nu \bar \nu, γ→ννˉ\gamma \to \nu \bar \nu and γγ→ννˉ\gamma \gamma \to \nu \bar \nu are investigated in the presence of a strongly magnetized and dense electron-positron plasma. The amplitudes of the reactions γe±→e±ννˉ\gamma e^{\pm} \to e^{\pm} \nu \bar \nu and γγ→ννˉ\gamma \gamma \to \nu \bar \nu are obtained. In the case of a cold degenerate plasma contributions of the considering processes to neutrino emissivity are calculated. It is shown that contribution of the process γγ→ννˉ\gamma \gamma \to \nu \bar \nu to neutrino emissivity is supressed in comparision with the contributions of the processes γe±→e±ννˉ\gamma e^{\pm} \to e^{\pm} \nu \bar \nu and γ→ννˉ\gamma \to \nu \bar \nu. The constraint on the magnetic field strength in the magnetar outer crust is obtained.Comment: 8 pages, LaTeX, 2 PS figures, based on the talk presented by D.A. Rumyantsev at the XV International Seminar Quarks'2008, Sergiev Posad, Moscow Region, May 23-29, 2008, to appear in the Proceeding

    Division Algebras and Extended N=2,4,8 SuperKdVs

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    The first example of an N=8 supersymmetric extension of the KdV equation is here explicitly constructed. It involves 8 bosonic and 8 fermionic fields. It corresponds to the unique N=8 solution based on a generalized hamiltonian dynamics with (generalized) Poisson brackets given by the Non-associative N=8 Superconformal Algebra. The complete list of inequivalent classes of parametric-dependent N=3 and N=4 superKdVs obtained from the ``Non-associative N=8 SCA" is also furnished. Furthermore, a fundamental domain characterizing the class of inequivalent N=4 superKdVs based on the "minimal N=4 SCA" is given.Comment: 14 pages, LaTe

    Spin Pumping and Inverse Spin Hall Effect in Platinum: The Essential Role of Spin-Memory Loss at Metallic Interfaces

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    Through combined ferromagnetic resonance, spin-pumping and inverse spin Hall effect experiments in Co|Pt bilayers and Co|Cu|Pt trilayers, we demonstrate consistent values of spin diffusion length ℓsfPt=3.4±0.4\ell_{\rm sf}^{\rm Pt}=3.4\pm0.4 nm and of spin Hall angle θSHEPt=0.051±0.004\theta_{\rm SHE}^{\rm Pt}=0.051\pm0.004 for Pt. Our data and model emphasize on the partial depolarization of the spin current at each interface due to spin-memory loss. Our model reconciles the previously published spin Hall angle values and explains the different scaling lengths for the ferromagnetic damping and the spin Hall effect induced voltage.Comment: 6 pages, 3 figures (main text) and 8 pages supplementary. Published with small modifications in Phys. Rev. Let

    Ultralow-Dissipation Superfluid Micromechanical Resonator

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    Micro and nanomechanical resonators with ultra-low dissipation have great potential as useful quantum resources. The superfluid micromechanical resonators presented here possess several advantageous characteristics: straightforward thermalization, dissipationless flow, and in situ tunability. We identify and quantitatively model the various dissipation mechanisms in two resonators, one fabricated from borosilicate glass and one from single crystal quartz. As the resonators are cryogenically cooled into the superfluid state, the damping from thermal effects and from the normal fluid component are strongly suppressed. At our lowest temperatures, damping is limited solely by internal dissipation in the substrate materials, and reach quality factors up to 913,000 at 13 mK. By lifting this limitation through substrate material choice and resonator design, modelling suggests that the resonators should reach quality factors as high as 108^8 at 100 mK, putting this architecture in an ideal position to harness mechanical quantum effects.Comment: 25 pages, 12 figures, 3 table
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