6,641 research outputs found

    Stationary wave patterns generated by an impurity moving with supersonic velocity through a Bose-Einstein condensate

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    Formation of stationary 3D wave patterns generated by a small point-like impurity moving through a Bose-Einstein condensate with supersonic velocity is studied. Asymptotic formulae for a stationary far-field density distribution are obtained. Comparison with three-dimensional numerical simulations demonstrates that these formulae are accurate enough already at distances from the obstacle equal to a few wavelengths.Comment: 7 pages, 3 figure

    Complete Sets of Orthogonal F-Squares of Prime Power Order with Differing Numbers of Symbols

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    This issue was undated. The date given is an estimate.21 pages, 1 article*Complete Sets of Orthogonal F-Squares of Prime Power Order with Differing Numbers of Symbols* (Mandeli, John P.; Federer, Walter T.) 21 page

    Loss Functions for Set Estimations

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    23 pages, 1 article*Loss Functions for Set Estimations* (Casella, George; Hwang, J. T.-Gene; Robert, Christian P.) 23 page

    Exact Solution of Two-Species Ballistic Annihilation with General Pair-Reaction Probability

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    The reaction process A+B>CA+B->C is modelled for ballistic reactants on an infinite line with particle velocities vA=cv_A=c and vB=cv_B=-c and initially segregated conditions, i.e. all A particles to the left and all B particles to the right of the origin. Previous, models of ballistic annihilation have particles that always react on contact, i.e. pair-reaction probability p=1p=1. The evolution of such systems are wholly determined by the initial distribution of particles and therefore do not have a stochastic dynamics. However, in this paper the generalisation is made to p<1p<1, allowing particles to pass through each other without necessarily reacting. In this way, the A and B particle domains overlap to form a fluctuating, finite-sized reaction zone where the product C is created. Fluctuations are also included in the currents of A and B particles entering the overlap region, thereby inducing a stochastic motion of the reaction zone as a whole. These two types of fluctuations, in the reactions and particle currents, are characterised by the `intrinsic reaction rate', seen in a single system, and the `extrinsic reaction rate', seen in an average over many systems. The intrinsic and extrinsic behaviours are examined and compared to the case of isotropically diffusing reactants.Comment: 22 pages, 2 figures, typos correcte

    All-optical formation of a Bose-Einstein condensate for applications in scanning electron microscopy

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    We report on the production of a F=1 spinor condensate of 87Rb atoms in a single beam optical dipole trap formed by a focused CO2 laser. The condensate is produced 13mm below the tip of a scanning electron microscope employing standard all-optical techniques. The condensate fraction contains up to 100,000 atoms and we achieve a duty cycle of less than 10s.Comment: 5 pages, 4 figure

    Asymptotic expansion for reversible A + B <-> C reaction-diffusion process

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    We study long-time properties of reversible reaction-diffusion systems of type A + B C by means of perturbation expansion in powers of 1/t (inverse of time). For the case of equal diffusion coefficients we present exact formulas for the asymptotic forms of reactant concentrations and a complete, recursive expression for an arbitrary term of the expansions. Taking an appropriate limit we show that by studying reversible reactions one can obtain "singular" solutions typical of irreversible reactions.Comment: 6 pages, no figures, to appear in PR

    Diffusion-Limited Annihilation with Initially Separated Reactants

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    A diffusion-limited annihilation process, A+B->0, with species initially separated in space is investigated. A heuristic argument suggests the form of the reaction rate in dimensions less or equal to the upper critical dimension dc=2d_c=2. Using this reaction rate we find that the width of the reaction front grows as t1/4t^{1/4} in one dimension and as t1/6(lnt)1/3t^{1/6}(\ln t)^{1/3} in two dimensions.Comment: 9 pages, Plain Te

    Fast-diffusion mean-field theory for k-body reactions in one dimension

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    We derive an improved mean-field approximation for k-body annihilation reactions kA --> inert, for hard-core diffusing particles on a line, annihilating in groups of k neighbors with probability 0 < q <= 1. The hopping and annihilation processes are correlated to mimic chemical reactions. Our new mean-field theory accounts for hard-core particle properties and has a larger region of applicability than the standard chemical rate equation especially for large k values. Criteria for validity of the mean-field theory and its use in phenomenological data fits are derived. Numerical tests are reported for k=3,4,5,6.Comment: 16 pages, TeX (plain

    Mode-hop-free tuning over 135 GHz of external cavity diode lasers without anti-reflection coating

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    We report an external cavity diode laser (ECDL), using a diode whose front facet is not antireflection (AR) coated, that has a mode-hop-free (MHF) tuning range greater than 135 GHz. We achieved this using a short external cavity and by simultaneously tuning the internal and external modes of the laser. We find that the precise location of the pivot point of the grating in our laser is less critical than commonly believed. The general applicability of the method, combined with the compact portable mechanical and electronic design, makes it well suited for both research and industrial applications.Comment: 5 pages, 5 figure

    Nontrivial Exponent for Simple Diffusion

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    The diffusion equation \partial_t\phi = \nabla^2\phi is considered, with initial condition \phi( _x_ ,0) a gaussian random variable with zero mean. Using a simple approximate theory we show that the probability p_n(t_1,t_2) that \phi( _x_ ,t) [for a given space point _x_ ] changes sign n times between t_1 and t_2 has the asymptotic form p_n(t_1,t_2) \sim [\ln(t_2/t_1)]^n(t_1/t_2)^{-\theta}. The exponent \theta has predicted values 0.1203, 0.1862, 0.2358 in dimensions d=1,2,3, in remarkably good agreement with simulation results.Comment: Minor typos corrected, affecting table of exponents. 4 pages, REVTEX, 1 eps figure. Uses epsf.sty and multicol.st
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