20,726 research outputs found

    Dust-acoustic waves and stability in the permeating dusty plasma: II. Power-law distributions

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    The dust-acoustic waves and their stability driven by a flowing dusty plasma when it cross through a static (target) dusty plasma (the so-called permeating dusty plasma) are investigated when the components of the dusty plasma obey the power-law q-distributions in nonextensive statistics. The frequency, the growth rate and the stability condition of the dust-acoustic waves are derived under this physical situation, which express the effects of the nonextensivity as well as the flowing dusty plasma velocity on the dust-acoustic waves in this dusty plasma. The numerical results illustrate some new characteristics of the dust-acoustic waves, which are different from those in the permeating dusty plasma when the plasma components are the Maxwellian distribution. In addition, we show that the flowing dusty plasma velocity has a significant effect on the dust-acoustic waves in the permeating dusty plasma with the power-law q-distribution.Comment: 20 pages, 10 figures, 41 reference

    Improved cosmological constraints on the curvature and equation of state of dark energy

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    We apply the Constitution compilation of 397 supernova Ia, the baryon acoustic oscillation measurements including the AA parameter, the distance ratio and the radial data, the five-year Wilkinson microwave anisotropy probe and the Hubble parameter data to study the geometry of the universe and the property of dark energy by using the popular Chevallier-Polarski-Linder and Jassal-Bagla-Padmanabhan parameterizations. We compare the simple χ2\chi^2 method of joined contour estimation and the Monte Carlo Markov chain method, and find that it is necessary to make the marginalized analysis on the error estimation. The probabilities of Ωk\Omega_k and waw_a in the Chevallier-Polarski-Linder model are skew distributions, and the marginalized 1σ1\sigma errors are Ωm=0.279−0.008+0.015\Omega_m=0.279^{+0.015}_{-0.008}, Ωk=0.005−0.011+0.006\Omega_k=0.005^{+0.006}_{-0.011}, w0=−1.05−0.06+0.23w_0=-1.05^{+0.23}_{-0.06}, and wa=0.5−1.5+0.3w_a=0.5^{+0.3}_{-1.5}. For the Jassal-Bagla-Padmanabhan model, the marginalized 1σ1\sigma errors are Ωm=0.281−0.01+0.015\Omega_m=0.281^{+0.015}_{-0.01}, Ωk=0.000−0.006+0.007\Omega_k=0.000^{+0.007}_{-0.006}, w0=−0.96−0.18+0.25w_0=-0.96^{+0.25}_{-0.18}, and wa=−0.6−1.6+1.9w_a=-0.6^{+1.9}_{-1.6}. The equation of state parameter w(z)w(z) of dark energy is negative in the redshift range 0≤z≤20\le z\le 2 at more than 3σ3\sigma level. The flat Λ\LambdaCDM model is consistent with the current observational data at the 1σ1\sigma level.Comment: 10 figures, 12 pages, Classical and Quantum Gravity in press; v2 to match the pulished versio

    Temperature driven structural phase transition for trapped ions and its experimental detection

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    A Wigner crystal formed with trapped ion can undergo structural phase transition, which is determined only by the mechanical conditions on a classical level. Instead of this classical result, we show that through consideration of quantum and thermal fluctuation, a structural phase transition can be solely driven by change of the system's temperature. We determine a finite-temperature phase diagram for trapped ions using the renormalization group method and the path integral formalism, and propose an experimental scheme to observe the predicted temperature-driven structural phase transition, which is well within the reach of the current ion trap technology.Comment: 4 pages, 5 figure

    Control of Dynamical Localization

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    Control over the quantum dynamics of chaotic kicked rotor systems is demonstrated. Specifically, control over a number of quantum coherent phenomena is achieved by a simple modification of the kicking field. These include the enhancement of the dynamical localization length, the introduction of classical anomalous diffusion assisted control for systems far from the semiclassical regime, and the observation of a variety of strongly nonexponential lineshapes for dynamical localization. The results provide excellent examples of controlled quantum dynamics in a system that is classically chaotic and offer new opportunities to explore quantum fluctuations and correlations in quantum chaos.Comment: 9 pages, 7 figures, to appear in Physical Review

    Non-existence of Extended Holographic Dark Energy with Hubble Horizon

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    The extended holographic dark energy model with the Hubble horizon as the infrared cutoff avoids the problem of the circular reasoning of the holographic dark energy model. We show that the infrared cutoff of the extended holographic dark energy model cannot be the Hubble horizon provided that the Brans-Dicke parameter ω\omega satisfies the experimental constraint ω>104\omega> 10^4, and this is proved as a no-go theorem. The no-go theorem also applies to the case in which the dark matter interacts with the dark energy.Comment: 12 pages with revtex, 4 figures, v2: minor corrections to match the version appeared in JCA

    Superconductivity and Phase Diagram in (Li0.8_{0.8}Fe0.2_{0.2})OHFeSe1−x_{1-x}Sx_x

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    A series of (Li0.8_{0.8}Fe0.2_{0.2})OHFeSe1−x_{1-x}Sx_x (0 ≤\leq x ≤\leq 1) samples were successfully synthesized via hydrothermal reaction method and the phase diagram is established. Magnetic susceptibility suggests that an antiferromagnetism arising from (Li0.8_{0.8}Fe0.2_{0.2})OH layers coexists with superconductivity, and the antiferromagnetic transition temperature nearly remains constant for various S doping levels. In addition, the lattice parameters of the both a and c axes decrease and the superconducting transition temperature Tc_c is gradually suppressed with the substitution of S for Se, and eventually superconductivity vanishes at xx = 0.90. The decrease of Tc_c could be attributed to the effect of chemical pressure induced by the smaller ionic size of S relative to that of Se, being consistent with the effect of hydrostatic pressure on (Li0.8_{0.8}Fe0.2_{0.2})OHFeSe. But the detailed investigation on the relationships between TcT_{\rm c} and the crystallographic facts suggests a very different dependence of TcT_{\rm c} on anion height from the Fe2 layer or ChCh-Fe2-ChCh angle from those in FeAs-based superconductors.Comment: 6 pages, 6 figure

    Coherent Manipulation of Quantum Delta-kicked Dynamics: Faster-than-classical Anomalous Diffusion

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    Large transporting regular islands are found in the classical phase space of a modified kicked rotor system in which the kicking potential is reversed after every two kicks. The corresponding quantum system, for a variety of system parameters and over long time scales, is shown to display energy absorption that is significantly faster than that associated with the underlying classical anomalous diffusion. The results are of interest to both areas of quantum chaos and quantum control.Comment: 6 pages, 4 figures, to appear in Physical Review
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