272 research outputs found

    Exact relations between multifractal exponents at the Anderson transition

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    Two exact relations between mutlifractal exponents are shown to hold at the critical point of the Anderson localization transition. The first relation implies a symmetry of the multifractal spectrum linking the multifractal exponents with indices q1/2q1/2. The second relation connects the wave function multifractality to that of Wigner delay times in a system with a lead attached.Comment: 4 pages, 3 figure

    Griffiths phase in the thermal quantum Hall effect

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    Two dimensional disordered superconductors with broken spin-rotation and time-reversal invariance, e.g. with p_x+ip_y pairing, can exhibit plateaus in the thermal Hall coefficient (the thermal quantum Hall effect). Our numerical simulations show that the Hall insulating regions of the phase diagram can support a sub-phase where the quasiparticle density of states is divergent at zero energy, \rho(E)\sim |E|^{1/z-1}, with a non-universal exponent z>1z>1, due to the effects of rare configurations of disorder (``Griffiths phase'').Comment: 4+ pages, 5 figure

    Surface criticality and multifractality at localization transitions

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    We develop the concept of surface multifractality for localization-delocalization (LD) transitions in disordered electronic systems. We point out that the critical behavior of various observables related to wave functions near a boundary at a LD transition is different from that in the bulk. We illustrate this point with a calculation of boundary critical and multifractal behavior at the 2D spin quantum Hall transition and in a 2D metal at scales below the localization length.Comment: Published versio

    Boundary multifractality in critical 1D systems with long-range hopping

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    Boundary multifractality of electronic wave functions is studied analytically and numerically for the power-law random banded matrix (PRBM) model, describing a critical one-dimensional system with long-range hopping. The peculiarity of the Anderson localization transition in this model is the existence of a line of fixed points describing the critical system in the bulk. We demonstrate that the boundary critical theory of the PRBM model is not uniquely determined by the bulk properties. Instead, the boundary criticality is controlled by an additional parameter characterizing the hopping amplitudes of particles reflected by the boundary.Comment: 7 pages, 4 figures, some typos correcte

    Multifractality at the spin quantum Hall transition

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    Statistical properties of critical wave functions at the spin quantum Hall transition are studied both numerically and analytically (via mapping onto the classical percolation). It is shown that the index η\eta characterizing the decay of wave function correlations is equal to 1/4, at variance with the r−1/2r^{-1/2} decay of the diffusion propagator. The multifractality spectra of eigenfunctions and of two-point conductances are found to be close-to-parabolic, Δq≃q(1−q)/8\Delta_q\simeq q(1-q)/8 and Xq≃q(3−q)/4X_q\simeq q(3-q)/4.Comment: 4 pages, 3 figure

    Dimensionality dependence of the wave function statistics at the Anderson transition

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    The statistics of critical wave functions at the Anderson transition in three and four dimensions are studied numerically. The distribution of the inverse participation ratios (IPR) PqP_q is shown to acquire a scale-invariant form in the limit of large system size. Multifractality spectra governing the scaling of the ensemble-averaged IPRs are determined. Conjectures concerning the IPR statistics and the multifractality at the Anderson transition in a high spatial dimensionality are formulated.Comment: 4 pages, 4 figure

    Multifractality of wavefunctions at the quantum Hall transition revisited

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    We investigate numerically the statistics of wavefunction amplitudes ψ(r)\psi({\bf r}) at the integer quantum Hall transition. It is demonstrated that in the limit of a large system size the distribution function of ∣ψ∣2|\psi|^2 is log-normal, so that the multifractal spectrum f(α)f(\alpha) is exactly parabolic. Our findings lend strong support to a recent conjecture for a critical theory of the quantum Hall transition.Comment: 4 pages Late
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