24,994 research outputs found

    Wave Mechanics of Two Hard Core Quantum Particles in 1-D Box

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    The wave mechanics of two impenetrable hard core particles in 1-D box is analyzed. Each particle in the box behaves like an independent entity represented by a {\it macro-orbital} (a kind of pair waveform). While the expectation value of their interaction, ,vanishesforeverystateoftwoparticles,theexpectationvalueoftheirrelativeseparation,, vanishes for every state of two particles, the expectation value of their relative separation, , satisfies λ/2 \ge \lambda/2 (or qπ/dq \ge \pi/d, with 2d=L2d = L being the size of the box). The particles in their ground state define a close-packed arrangement of their wave packets (with =λ/2 = \lambda/2, phase position separation Δϕ=2π\Delta\phi = 2\pi and momentum qo=π/d|q_o| = \pi/d) and experience a mutual repulsive force ({\it zero point repulsion}) fo=h2/2md3f_o = h^2/2md^3 which also tries to expand the box. While the relative dynamics of two particles in their excited states represents usual collisional motion, the same in their ground state becomes collisionless. These results have great significance in determining the correct microscopic understanding of widely different many body systems.Comment: 12 pages, no figur

    CVD of solid oxides in porous substrates for ceramic membrane modification

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    The deposition of yttria-doped zirconia has been experimented systematically in various types of porous ceramic substrates by a modified chemical vapor deposition (CVD) process operating in an opposing reactant geometry using water vapor and corresponding metal chloride vapors as reactants. The effects of substrate pore dimension and structure, bulk-phase reactant concentration, reactant diffusivity in substrate pores and deposition temperature are experimentally studied and explained qualitatively by a theoretical modeling analysis. The experimental and theoretical results suggest a reaction mechanism which depends on water vapor and chloride vapor concentrations. Consequently, the diffusivity, bulk-phase reactant concentration, and substrate pore dimension are important in the CVD process. Effects of deposition temperature on the deposition results and narrow deposition zone compared to the substrate thickness also suggest a Langmuir-Hinshelwood reaction mechanism involved in the CVD process with a very fast CVD reaction rate. Gas permeation data indicate that whether deposition of solid in substrate pores could result in the pore-size reduction depends strongly on the initial pore-size distribution of the substrate

    A comparative reliability analysis of ETCS train radio communications

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    StoCharts have been proposed as a UML statechart extension for performance and dependability evaluation, and were applied in the context of train radio reliability assessment to show the principal tractability of realistic cases with this approach. In this paper, we extend on this bare feasibility result in two important directions. First, we sketch the cornerstones of a mechanizable translation of StoCharts to MoDeST. The latter is a process algebra-based formalism supported by the Motor/Möbius tool tandem. Second, we exploit this translation for a detailed analysis of the train radio case study

    Calculation of d- and q-axis inductances of PM brushless ac machines accounting for Skew

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    A hybrid two-dimensional (2-D) finite-element/analytical technique is described for predicting the d-axis and q-axis inductances of permanent magnet (PM) brushless ac machines, with due account for the influence of skew. Predicted inductances are compared with measured values for two machines having identical stators, which are skewed by one slot-pitch, but which have different rotor topologies, one having surface-mounted magnets and the other having interior magnets

    Generation of electric fields and currents by neutral flows in weakly ionized plasmas through collisional dynamos

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    In weakly ionized plasmas neutral flows drag plasma across magnetic field lines generating intense electric fields and currents. An example occurs in the Earth's ionosphere near the geomagnetic equator. Similar processes take place in the Solar chromosphere and magnetohydrodynamic generators. This paper argues that not all convective neutral flows generate electric fields and currents and it introduces the corresponding universal criterion for their formation, ∇×(U×B)≠∂B/∂t, where U is the neutral flow velocity, B is the magnetic field, and t is time. This criterion does not depend on the conductivity tensor, σˆ. For many systems, the displacement current, ∂B/∂t, is negligible making the criterion even simpler. This theory also shows that the neutral-dynamo driver that generates E-fields and currents plays the same role as the DC electric current plays for the generation of the magnetic field in the Biot-Savart law.This work was supported by NSF/DOE Grant No. PHY-1500439, NASA Grant Nos. NNX11A096G and NNX14AI13G, and NSF-AGS Postdoctoral Research Fellowship Award No. 1433536. (PHY-1500439 - NSF/DOE; NNX11A096G - NASA; NNX14AI13G - NASA; 1433536 - NSF-AGS

    Iron loss in permanent-magnet brushless AC machines under maximum torque per ampere and flux weakening control

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    The airgap flux density distribution, flux density loci in the stator core, and the associated iron loss in two topologies of brushless AC motor, having a surface-mounted magnet rotor and an interior-mounted magnet rotor, respectively, are investigated when operated under maximum torque per ampere control in the constant torque mode and maximum power control in the flux-weakening mode. It is shown that whilst the interior magnet topology is known to be eminently suitable for flux-weakening operation, due to its high demagnetization withstand capability, its iron loss can be significantly higher than for a surface-mounted magnet machine

    No Ghost State in the Brane World

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    We discuss the role of the trace part of metric fluctuations hMNh_{MN} in the Randall-Sundrum scenario of gravity. Without the matter, this field (h=ηMNhMNh=\eta^{MN}h_{MN}) is a gauge-dependent term, and thus it can be gauged away. But, including the uniform source T~MN\tilde{T}_{MN}, this field satisfies the linearized equation 4h=16πG5Tμμ\Box_4 h =16\pi G_5 T^{\mu}_{\mu}. This may correspond to the scalar ξ5\xi^5 in the bending of the brane due to the localized source. Considering the case of longitudinal perturbations (h5μ=h55=0h_{5\mu} =h_{55}=0), one finds the source relation T~μμ=2T~55\tilde{T}^{\mu}_{\mu}=2\tilde{T}_{55}, which leads to the ghost states in the massive modes. In addition, if one requires T44=2(T22+T33)T_{44}=2(T_{22}+T_{33}), it is found that in the limit of mh20m^2_h \to 0 we have the massless spin-2 propagation without the ghost state. This exactly corresponds to the same situation as in the intermediate scales of Gregory-Rubakov-Sibiryakov (GRS) model.Comment: 7 pages, no figure, the version to appear in PLB, comments on the matter source and references added, main results unchange

    Nonlinear states and nonlinear tunneling in a potential well

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    A nonlinear Schroedinger model in a square well and managed nonlinearity is shown to possess nonlinear states as continuous extensions of the linear levels. The solutions are remarkably stable up to a threshold amplitude where a soliton is emitted and propagates outside the well. The analytic expression of the threshold is given in terms of the well size for each level. This process of nonlinear tunneling results from an instability of the evanescent wave inside the walls and can find experimental realization in a proposed nonlinear fiber Bragg gratings resonator.Comment: RevTex file, augmented references and related text revisio

    Wigner's Spins, Feynman's Partons, and Their Common Ground

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    The connection between spin and symmetry was established by Wigner in his 1939 paper on the Poincar\'e group. For a massive particle at rest, the little group is O(3) from which the concept of spin emerges. The little group for a massless particle is isomorphic to the two-dimensional Euclidean group with one rotational and two translational degrees of freedom. The rotational degree corresponds to the helicity, and the translational degrees to the gauge degree of freedom. The question then is whether these two different symmetries can be united. Another hard-pressing problem is Feynman's parton picture which is valid only for hadrons moving with speed close to that of light. While the hadron at rest is believed to be a bound state of quarks, the question arises whether the parton picture is a Lorentz-boosted bound state of quarks. We study these problems within Einstein's framework in which the energy-momentum relations for slow particles and fast particles are two different manifestations one covariant entity.Comment: LaTex 12 pages, 3 figs, based on the lectures delivered at the Advanced Study Institute on Symmetries and Spin (Prague, Czech Republic, July 2001
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