49,667 research outputs found

    Weak-localization and rectification current in non-diffusive quantum wires

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    We show that electron transport in disordered quantum wires can be described by a modified Cooperon equation, which coincides in form with the Dirac equation for the massive fermions in a 1+1 dimensional system. In this new formalism, we calculate the DC electric current induced by electromagnetic fields in quasi-one-dimensional rings. This current changes sign, from diamagnetic to paramagnetic, depending on the amplitude and frequency of the time-dependent external electromagnetic field.Comment: changed title, added more detail, to appear in J. Phys.: Condens. Matte

    Continuous Multipartite Entangled State in Wigner Representation and the Violation of Zukowski-Brukner Inequality

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    We construct an explicit Wigner function for N-mode squeezed state. Based on a previous observation that the Wigner function describes correlations in the joint measurement of the phase-space displaced parity operator, we investigate the non-locality of multipartite entangled state by the violation of Zukowski-Brukner N-qubit Bell inequality. We find that quantum predictions for such squeezed state violate these inequalities by an amount that grows with the number N.Comment: 5 pages, rewritten version, accepted by Phys. Rev.

    Diffusion-Limited Aggregation Processes with 3-Particle Elementary Reactions

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    A diffusion-limited aggregation process, in which clusters coalesce by means of 3-particle reaction, A+A+A->A, is investigated. In one dimension we give a heuristic argument that predicts logarithmic corrections to the mean-field asymptotic behavior for the concentration of clusters of mass mm at time tt, c(m,t) m1/2(log(t)/t)3/4c(m,t)~m^{-1/2}(log(t)/t)^{3/4}, for 1<<m<<t/log(t)1 << m << \sqrt{t/log(t)}. The total concentration of clusters, c(t)c(t), decays as c(t) log(t)/tc(t)~\sqrt{log(t)/t} at t>t --> \infty. We also investigate the problem with a localized steady source of monomers and find that the steady-state concentration c(r)c(r) scales as r1(log(r))1/2r^{-1}(log(r))^{1/2}, r1r^{-1}, and r1(log(r))1/2r^{-1}(log(r))^{-1/2}, respectively, for the spatial dimension dd equal to 1, 2, and 3. The total number of clusters, N(t)N(t), grows with time as (log(t))3/2(log(t))^{3/2}, t1/2t^{1/2}, and t(log(t))1/2t(log(t))^{-1/2} for dd = 1, 2, and 3. Furthermore, in three dimensions we obtain an asymptotic solution for the steady state cluster-mass distribution: c(m,r)r1(log(r))1Φ(z)c(m,r) \sim r^{-1}(log(r))^{-1}\Phi(z), with the scaling function Φ(z)=z1/2exp(z)\Phi(z)=z^{-1/2}\exp(-z) and the scaling variable z m/log(r)z ~ m/\sqrt{log(r)}.Comment: 12 pages, plain Te

    Efficiency of Nonlinear Particle Acceleration at Cosmic Structure Shocks

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    We have calculated the evolution of cosmic ray (CR) modified astrophysical shocks for a wide range of shock Mach numbers and shock speeds through numerical simulations of diffusive shock acceleration (DSA) in 1D quasi- parallel plane shocks. The simulations include thermal leakage injection of seed CRs, as well as pre-existing, upstream CR populations. Bohm-like diffusion is assumed. We model shocks similar to those expected around cosmic structure pancakes as well as other accretion shocks driven by flows with upstream gas temperatures in the range T0=104107.6T_0=10^4-10^{7.6}K and shock Mach numbers spanning Ms=2.4133M_s=2.4-133. We show that CR modified shocks evolve to time-asymptotic states by the time injected particles are accelerated to moderately relativistic energies (p/mc \gsim 1), and that two shocks with the same Mach number, but with different shock speeds, evolve qualitatively similarly when the results are presented in terms of a characteristic diffusion length and diffusion time. For these models the time asymptotic value for the CR acceleration efficiency is controlled mainly by shock Mach number. The modeled high Mach number shocks all evolve towards efficiencies 50\sim 50%, regardless of the upstream CR pressure. On the other hand, the upstream CR pressure increases the overall CR energy in moderate strength shocks (MsafewM_s \sim {\rm a few}). (abridged)Comment: 23 pages, 12 ps figures, accepted for Astrophysical Journal (Feb. 10, 2005

    Bogoliubov Hamiltonian as Derivative of Dirac Hamiltonian via Braid Relation

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    In this paper we discuss a new type of 4-dimensional representation of the braid group. The matrices of braid operations are constructed by q-deformation of Hamiltonians. One is the Dirac Hamiltonian for free electron with mass m, the other, which we find, is related to the Bogoliubov Hamiltonian for quasiparticles in 3^3He-B with the same free energy and mass being m/2. In the process, we choose the free q-deformation parameter as a special value in order to be consistent with the anyon description for fractional quantum Hall effect with ν=1/2\nu = 1/2.Comment: 3 pages, 5 figure

    An alternative formulation of classical electromagnetic duality

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    By introducing a doublet of electromagnetic four dimensional vector potentials, we set up a manifestly Lorentz covariant and SO(2) duality invariant classical field theory of electric and magnetic charges. In our formulation one does not need to introduce the concept of Dirac string.Comment: 14 pages, no figures, Latex, minor corrections, references and acknowledgements adde

    Asymptotic behavior of A + B --> inert for particles with a drift

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    We consider the asymptotic behavior of the (one dimensional) two-species annihilation reaction A + B --> 0, where both species have a uniform drift in the same direction and like species have a hard core exclusion. Extensive numerical simulations show that starting with an initially random distribution of A's and B's at equal concentration the density decays like t^{-1/3} for long times. This process is thus in a different universality class from the cases without drift or with drift in different directions for the different species.Comment: LaTeX, 6pp including 3 figures in LaTeX picture mod
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