Universal Fluctuations in Spectra of Disordered Systems at the Anderson Transition
arXiv:cond-mat/9506114 · doi:10.1143/JJAP.34.4361
Abstract
Using the level--spacing distribution and the total probability function of the numbers of levels in a given energy interval we analyze the crossover of the level statistics between the delocalized and the localized regimes. By numerically calculating the electron spectra of systems of up to lattice sites described by the Anderson Hamiltonian it is shown that the distribution of neighboring spacings is {\em scale- independent} at the metal-insulator transition. For large spacings it has a Poisson-like asymptotic form , where . At the critical point we obtain a linear relationship between the variance of the number of levels and their average number within the interval . The constant of proportionality is less than unity due to the repulsion of the levels. Both and are determined by the probability density of having exactly levels in the energy interval . The distribution at the critical point is found to be size--independent and to obey a Gaussian law near its maximum, where .
9 pages of Revtex, 3 figures included (tar-compressed and uuencoded using script UUFILES), to appear in Jpn.J.Appl.Phys
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- Critical behaviour at the metal-insulator transition in 3-dimensional disordered systems in a strong magnetic field
- Real-space renormalization-group approach to the integer quantum Hall effect
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- Spectral Properties of Three Dimensional Layered Quantum Hall Systems