616 research outputs found

    Ambipolar Nernst effect in NbSe2_2

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    The first study of Nernst effect in NbSe2_2 reveals a large quasi-particle contribution with a magnitude comparable and a sign opposite to the vortex signal. Comparing the effect of the Charge Density Wave(CDW) transition on Hall and Nernst coefficients, we argue that this large Nernst signal originates from the thermally-induced counterflow of electrons and holes and indicates a drastic change in the electron scattering rate in the CDW state. The results provide new input for the debate on the origin of the anomalous Nernst signal in high-Tc_c cuprates.Comment: 5 pages including 4 figure

    Universal Scaling Behavior of Anomalous Hall Effect and Anomalous Nernst Effect in Itinerant Ferromagnets

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    Anomalous Hall effect (AHE) and anomalous Nernst effect (ANE) in a variety of ferromagnetic metals including pure metals, oxides, and chalcogenides, are studied to obtain unified understandings of their origins. We show a universal scaling behavior of anomalous Hall conductivity σxy\sigma_{xy} as a function of longitudinal conductivity σxx\sigma_{xx} over five orders of magnitude, which is well explained by a recent theory of the AHE taking into account both the intrinsic and extrinsic contributions. ANE is closely related with AHE and provides us with further information about the low-temperature electronic state of itinerant ferromagnets. Temperature dependence of transverse Peltier coefficient αxy\alpha_{xy} shows an almost similar behavior among various ferromagnets, and this behavior is in good agreement quantitatively with that expected from the Mott rule.Comment: 4pages, 4figures, 1tabl

    Electrical Resistivity of a Thin Metallic Film

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    The electrical resistivity of a pure sample of a thin metallic film is found to depend on the boundary conditions. This conclusion is supported by a free-electron model calculation and confirmed by an ab initio relativistic Korringa-Kohn-Rostoker computation. The low-temperature resistivity is found to be zero for a free-standing film (reflecting boundary conditions) but nonzero when the film is sandwiched between two semi-infinite samples of the same material (outgoing boundary conditions). In the latter case, this resistivity scales inversely with the number of monolayers and is due to the background diffusive scattering by a finite lattice.Comment: 20 pages. To be published in Physical Review B, December 15, 199

    Interaction of the Electromagnetic p-Waves with Thin Metal Films

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    For the first time it is shown that for thin metallic films thickness of which not exceed thickness of skin-layer, the problem allows analytical solution for arbitrary boundary value problems. The analysis of dependence of coefficients of transmission, reflection and absorbtion on angle incidence, thickness of films and coefficient of specular reflection is carried out.Comment: 15 pages, 9 figure

    Effects of Abscisin II on Phenylalanine Ammonia-Lyase Activity in Excised Bean Axes

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    Integral equation for inhomogeneous condensed bosons generalizing the Gross-Pitaevskii differential equation

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    We give here the derivation of a Gross-Pitaevskii--type equation for inhomogeneous condensed bosons. Instead of the original Gross-Pitaevskii differential equation, we obtain an integral equation that implies less restrictive assumptions than are made in the very recent study of Pieri and Strinati [Phys. Rev. Lett. 91 (2003) 030401]. In particular, the Thomas-Fermi approximation and the restriction to small spatial variations of the order parameter invoked in their study are avoided.Comment: Phys. Rev. A (accepted

    Path-decomposition expansion and edge effects in a confined magnetized free-electron gas

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    Path-integral methods can be used to derive a `path-decomposition expansion' for the temperature Green function of a magnetized free-electron gas confined by a hard wall. With the help of this expansion the asymptotic behaviour of the profiles for the excess particle density and the electric current density far from the edge is determined for arbitrary values of the magnetic field strength. The asymptotics are found to depend sensitively on the degree of degeneracy. For a non-degenerate electron gas the asymptotic profiles are essentially Gaussian (albeit modulated by a Bessel function), on a length scale that is a function of the magnetic field strength and the temperature. For a completely degenerate electron gas the asymptotic behaviour is again proportional to a Gaussian, with a scale that is the magnetic length in this case. The prefactors are polynomial and logarithmic functions of the distance from the wall, that depend on the number of filled Landau levels nn. As a consequence, the Gaussian asymptotic decay sets in at distances that are large compared to the magnetic length multiplied by n\sqrt{n}.Comment: 16 pages, 2 figures, submitted to J. Phys. A: Math. Gen; corrected small typ

    Where are Bridges Needed: Relationships Between Youth and Adult Services Before Strengthening the Transition System

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    Summary: This report summarizes the nature of the relationships between organizations and agencies in Clark County, WA, that could form a system of services to support youth and young adults with serious mental health conditions during the ages of the transition from adolescence to adulthood (ages 14‐25)

    Simple Analytical Particle and Kinetic Energy Densities for a Dilute Fermionic Gas in a d-Dimensional Harmonic Trap

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    We derive simple analytical expressions for the particle density ρ(r)\rho(r) and the kinetic energy density τ(r)\tau(r) for a system of noninteracting fermions in a dd-dimensional isotropic harmonic oscillator potential. We test the Thomas-Fermi (TF, or local-density) approximation for the functional relation τ[ρ]\tau[\rho] using the exact ρ(r)\rho(r) and show that it locally reproduces the exact kinetic energy density τ(r)\tau(r), {\it including the shell oscillations,} surprisingly well everywhere except near the classical turning point. For the special case of two dimensions (2D), we obtain the unexpected analytical result that the integral of τTF[ρ(r)]\tau_{TF}[\rho(r)] yields the {\it exact} total kinetic energy.Comment: 4 pages, 4 figures; corrected versio

    Solid State Physics

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    Contains reports on five research projects
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