4 research outputs found

    Longitudinal and Spin-Hall Conductance of a Two-Dimensional Rashba System with Arbitrary Disorder

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    We calculate the longitudinal and spin-Hall conductances in four-lead bridges with Rashba-Dresselhaus spin-orbit interactions. Numerical results are obtained both within the Landauer-Büttiker formalism and by the direct evaluation of the Kubo formula. The microscopic Hamiltonian is obtained in the tight-binding approxi-mation in terms of the neareast-neighbor hopping integral t, the Rashba spin-orbit coupling VR, the Dresselhaus spin-orbit coupling VD, and an Anderson-type, on-site disorder energy strength W. We reconfirm that below a critical disorder threshold, the spin-Hall effect is present. Further, we study the effect on the two conductivities of the Fermi energy, Rashba and/or Dresselhaus coefficient ratio and system size

    Positional Disorder, Spin-Orbit Coupling and Frustration in GaMnAs

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    We study the magnetic properties of metallic GaMnAs. We calculate the effective RKKY interaction between Mn spins using several realistic models for the valence band structure of GaAs. We also study the effect of positional disorder of the Mn on the magnetic properties. We find that the interaction between two Mn spins is anisotropic due to spin-orbit coupling within both the so-called spherical approximation and in the more realistic six band model. The spherical approximation strongly overestimates this anistropy, especially for short distances between Mn ions. Using the obtained effective Hamiltonian we carry out Monte Carlo simulations of finite and zero temperature magnetization and find that, due to orientational frustration of the spins, non-collinear states appear in both valence band approximations for disordered, uncorrelated Mn impurities in the small concentration regime. Introducing correlations among the substitutional Mn positions or increasing the Mn concentration leads to an increase in the remnant magnetization at zero temperature and an almost fully polarized ferromagnetic state.Comment: 17 Pages, 13 Figure

    Disorder, spin-orbit, and interaction effects in dilute Ga1xMnxAs{\rm Ga}_{1-x}{\rm Mn}_x{\rm As}

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    We derive an effective Hamiltonian for Ga1xMnxAs{\rm Ga}_{1-x}{\rm Mn}_x {\rm As} in the dilute limit, where Ga1xMnxAs{\rm Ga}_{1-x}{\rm Mn}_x {\rm As} can be described in terms of spin F=3/2F=3/2 polarons hopping between the {\rm Mn} sites and coupled to the local {\rm Mn} spins. We determine the parameters of our model from microscopic calculations using both a variational method and an exact diagonalization within the so-called spherical approximation. Our approach treats the extremely large Coulomb interaction in a non-perturbative way, and captures the effects of strong spin-orbit coupling and Mn positional disorder. We study the effective Hamiltonian in a mean field and variational calculation, including the effects of interactions between the holes at both zero and finite temperature. We study the resulting magnetic properties, such as the magnetization and spin disorder manifest in the generically non-collinear magnetic state. We find a well formed impurity band fairly well separated from the valence band up to xactive0.015x_{\rm active} \lesssim 0.015 for which finite size scaling studies of the participation ratios indicate a localization transition, even in the presence of strong on-site interactions, where xactive<xnomx_{\rm active}<x_{\rm nom} is the fraction of magnetically active Mn. We study the localization transition as a function of hole concentration, Mn positional disorder, and interaction strength between the holes.Comment: 15 pages, 12 figure

    Kondo temperature of SU(4) symmetric quantum dots

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    A path integral approach is used to derive a closed analytical expression for the Kondo temperature of the SU(4) symmetrical Anderson model. In contrast to the SU(2) case, the prefactor of the Kondo temperature is found to display a peculiar orbital-energy (gate voltage) dependence, reflecting the presence of various SU(4) mixed valence fixed points. Our analytical expressions are tested against and confirmed by numerical renormalization group computations
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