Distribution of fractal dimensions at the Anderson transition
arXiv:cond-mat/9907067 · doi:10.1103/PhysRevLett.83.4590
Abstract
We investigated numerically the distribution of participation numbers in the 3d Anderson tight-binding model at the localization-delocalization threshold. These numbers in {\em one} disordered system experience strong level-to-level fluctuations in a wide energy range. The fluctuations grow substantially with increasing size of the system. We argue that the fluctuations of the correlation dimension, of the wave functions are the main reason for this. The distribution of these correlation dimensions at the transition is calculated. In the thermodynamic limit () it does not depend on the system size . An interesting feature of this limiting distribution is that it vanishes exactly at , the highest possible value of the correlation dimension at the Anderson threshold in this model.
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