1995
DOI: 10.1088/0953-8984/7/28/002
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Critical level spacing distribution of two-dimensional disordered systems with spin-orbit coupling

Abstract: The energy level statistics of 2D electrons with spin-orbit scattering are considered near the disorder induced metal-insulator transition. Using the Ando model, the nearest-level-spacing distribution is calculated numerically at the critical point. It is shown that the critical spacing distribution is size independent and has a Poisson-like decay at large spacings as distinct from the Gaussian asymptotic form obtained by the random-matrix theory.

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Cited by 28 publications
(39 citation statements)
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“…For disorder strength W close to the critical value W c various new scale independent distributions have been discovered recently in several systems [10,11,13,16,17] that exhibit a metal-insulator-transition or at least a critical point. …”
Section: Model and Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…For disorder strength W close to the critical value W c various new scale independent distributions have been discovered recently in several systems [10,11,13,16,17] that exhibit a metal-insulator-transition or at least a critical point. …”
Section: Model and Methodsmentioning
confidence: 99%
“…On the other hand, using the method of energy-level statistics [10,11,12,13], system sizes of more than a factor of 10 larger are accessible. In this method, the knowledge of the eigenfunctions is not necessary, because the information about localized, critical or extended states is gained from the spectral correlations.…”
Section: Introductionmentioning
confidence: 99%
“…They are different from random matrix theory and Poisson statistics. The universality of these statistics dubbed "critical level statistics" is also classified by the symmetry of the ensemble [8][9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…[8], it has been suggested that the level spacing distribution may be described by a more generalized form P͑s͒ = As ␣ e −␤s ␥ ͑␣ , ␤ , ␥ Ͼ 0͒. Although this simple form is not valid, the power-law behavior at the origin and the exponential decay in the tail (with ␥ =1) have been observed in numerical studies and classified according to the symmetry of the system [9][10][11][12][13]. A similar rich structure of critical level statistics should be expected for quasiperiodic systems.…”
Section: Introductionmentioning
confidence: 99%
“…Another reason why a large number of numerical simulations of the LSD at the transition 8,9,10,11,12,13,14,15,16,17,18,19,20,21,22 were carried out during the past decade is the controversy that existed over the large-spacing tail of the critical LSD. Conclusive demonstration 12,13,21 that this tail is Poissonian, i.e., that there is no repulsion between the levels with spacings much larger than the mean value, 1 rather than super-Poissonian, 23 implying that repulsion is partially preserved, required a very high accuracy of the simulations.…”
Section: Introductionmentioning
confidence: 99%