Scaling of the conductance distribution near the Anderson transition
arXiv:cond-mat/0208157 · doi:10.1103/PhysRevB.67.155106
Abstract
The single parameter scaling hypothesis is the foundation of our understanding of the Anderson transition. However, the conductance of a disordered system is a fluctuating quantity which does not obey a one parameter scaling law. It is essential to investigate the scaling of the full conductance distribution to establish the scaling hypothesis. We present a clear cut numerical demonstration that the conductance distribution indeed obeys one parameter scaling near the Anderson transition.
References in corpus (3)
Cited by in corpus (30)
- Multifractal analysis of the metal-insulator transition in the 3D Anderson model I: Symmetry relation under typical averaging
- Numerical estimation of the -function in 2D systems with spin-orbit coupling
- Multifractal analysis of the metal-insulator transition in the 3D Anderson model II: Symmetry relation under ensemble averaging
- Transfer matrix study of the Anderson transition in non-Hermitian systems
- Ioffe-Regel criterion of Anderson localization in the model of resonant point scatterers
- Fluctuations of the Lyapunov exponent in 2D disordered systems
- Finite-size scaling analysis of localization transition for scalar waves in a 3D ensemble of resonant point scatterers
- Isosbestic points in the spectral function of correlated electrons
- Finite Size Scaling Analysis of the Anderson Transition
- Evolutions of helical edge states in disordered HgTe/CdTe quantum wells
- Universality of the metal-insulator transition in three-dimensional disordered systems
- Search for Anderson localization of light by cold atoms in a static electric field
- Unusual Metal to Marginal-Metal Transition in Two-Dimensional Ferromagnetic Electron Gases
- Localization of light in a three-dimensional disordered crystal of atoms
- Anomalously Localized States in the Anderson Model
- Scaling and localization lengths of a topologically disordered system
- Possible Anderson transition below two dimensions in disordered systems of noninteracting electrons
- Diffusion in the Anderson model in higher dimensions
- Intensity distribution of scalar waves propagating in random media
- Optimisation of multifractal analysis using box-size scaling
- Character of eigenstates of the 3D disordered Anderson Hamiltonian
- Conductance distribution near the Anderson transition
- Borel-Padé re-summation of the -functions describing Anderson localisation in the Wigner-Dyson symmetry classes
- Metal - Insulator Transition in 3D Quantum Percolation
- Conductance fluctuations in disordered superconductors with broken time-reversal symmetry near two dimensions
- Quantum transport phenomena in disordered electron systems with spin-orbit coupling in two dimensions and below
- Boundary hopping and the mobility edge in the Anderson model in three dimensions
- Reply to comment by P.Markos [arXiv:1205.0689]
- Localization of non-interacting electrons in thin layered disordered systems
- Critical behavior of Anderson transitions in higher dimensional Bogoliubov-de Gennes symmetry classes