1,746 research outputs found

    Universality in escape from a modulated potential well

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    We show that the rate of activated escape WW from a periodically modulated potential displays scaling behavior versus modulation amplitude AA. For adiabatic modulation of an optically trapped Brownian particle, measurements yield ln⁥W∝(Ac−A)ÎŒ\ln W\propto (A_{\rm c} - A)^{\mu} with ÎŒ=1.5\mu = 1.5. The theory gives ÎŒ=3/2\mu=3/2 in the adiabatic limit and predicts a crossover to ÎŒ=2\mu=2 scaling as AA approaches the bifurcation point where the metastable state disappears.Comment: 4 pages, 3 figure

    Scaling and crossovers in activated escape near a bifurcation point

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    Near a bifurcation point a system experiences critical slowing down. This leads to scaling behavior of fluctuations. We find that a periodically driven system may display three scaling regimes and scaling crossovers near a saddle-node bifurcation where a metastable state disappears. The rate of activated escape WW scales with the driving field amplitude AA as ln⁥W∝(Ac−A)Ο\ln W \propto (A_c-A)^{\xi}, where AcA_c is the bifurcational value of AA. With increasing field frequency the critical exponent Ο\xi changes from Ο=3/2\xi = 3/2 for stationary systems to a dynamical value Ο=2\xi=2 and then again to Ο=3/2\xi=3/2. The analytical results are in agreement with the results of asymptotic calculations in the scaling region. Numerical calculations and simulations for a model system support the theory.Comment: 18 page

    Dynamics of a tunneling magnetic impurity: Kondo effect induced incoherence

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    We study how the formation of the Kondo compensation cloud influences the dynamical properties of a magnetic impurity that tunnels between two positions in a metal. The Kondo effect dynamically generates a strong tunneling impurity-conduction electron coupling, changes the temperature dependence of the tunneling rate, and may ultimately result in the destruction of the coherent motion of the particle at zero temperature. We find an interesting two-channel Kondo fixed point as well for a vanishing overlap between the electronic states that screen the magnetic impurity. We propose a number of systems where the predicted features could be observed.Comment: 4 pages, 3 figures, ReVTe

    Sequence randomness and polymer collapse transitions

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    Contrary to expectations based on Harris' criterion, chain disorder with frustration can modify the universality class of scaling at the theta transition of heteropolymers. This is shown for a model with random two-body potentials in 2D on the basis of exact enumeration and accurate Monte Carlo results. When frustration grows beyond a certain finite threshold, the temperature below which disorder becomes relevant coincides with the theta one and scaling exponents definitely start deviating from those valid for homopolymers.Comment: 4 pages, 4 eps figure

    Frequency Characteristics of Visually Induced Motion Sickness

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    This article was published in the journal, Human Factors [Sage Publications / © Human Factors and Ergonomics Society.]. The definitive version is available at: http://dx.doi.org/10.1177/0018720812469046Objective: The aim of this study was to explore the frequency response of visually induced motion sickness (VIMS) for oscillating linear motion in the foreand- aft axis. Background: Simulators, virtual environments, and commercially available video games that create an illusion of self-motion are often reported to induce the symptoms seen in response to true motion. Often this human response can be the limiting factor in the acceptability and usability of such systems. Whereas motion sickness in physically moving environments is known to peak at an oscillation frequency around 0.2 Hz, it has recently been suggested that VIMS peaks at around 0.06 Hz following the proposal that the summed response of the visual and vestibular selfmotion systems is maximized at this frequency. Methods: We exposed 24 participants to random dot optical flow patterns simulating oscillating foreand- aft motion within the frequency range of 0.025 to 1.6 Hz. Before and after each 20-min exposure, VIMS was assessed with the Simulator Sickness Questionnaire. Also, a standard motion sickness scale was used to rate symptoms at 1-min intervals during each trial. Results: VIMS peaked between 0.2 and 0.4 Hz with a reducing effect at lower and higher frequencies. Conclusion: The numerical prediction of the “crossover frequency” hypothesis, and the design guidance curve previously proposed, cannot be accepted when the symptoms are purely visually induced. Application: In conditions in which stationary observers are exposed to optical flow that simulates oscillating fore-and-aft motion, frequencies around 0.2 to 0.4 Hz should be avoided

    Scaling and universality in the anisotropic Kondo model and the dissipative two-state system

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    Scaling and universality in the Ohmic two-state system is investigated by exploiting the equivalence of this model to the anisotropic Kondo model. For the Ohmic two-state system, we find universal scaling functions for the specific heat, Cα(T)C_{\alpha}(T), static susceptibility, χα(T)\chi_{\alpha}(T), and spin relaxation function Sα(ω)S_{\alpha}(\omega) depending on the reduced temperature T/ΔrT/\Delta_{r} (frequency ω/Δr\omega/\Delta_{r}), with Δr\Delta_{r} the renormalized tunneling frequency, and uniquely specified by the dissipation strength α\alpha (0<α<10<\alpha<1). The scaling functions can be used to extract α\alpha and Δr\Delta_{r} in experimental realizations.Comment: 5 pages (LaTeX), 4 EPS figures. Minor changes, typos corrected, journal reference adde

    Evidence of Electromagnetic Absorption by Collective Modes in the Heavy Fermion Superconductor UBe13

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    We present results of a microwave surface impedance study of the heavy fermion superconductor UBe13. We clearly observe an absorption peak whose frequency- and temperature-dependence scales with the BCS gap function. Resonant absorption into a collective mode, with energy approximately proportional to the superconducting gap, is proposed as a possible explantation
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