Abstract
The phase diagram for the Anderson transition of a two-dimensional disordered system with variable impurity concentration and a perpendicular magnetic field is investigated. A phase boundary is found, separating localized from extended states. It is calculated by means of a finite-size-scaling approach. The shape of the phase boundary and the change in the magnetoresistance are explained in terms of quantum interference effects, i.e., weak localization. A critical exponent for the correlation length and the onset of the delocalized phase are determined.
| Original language | English |
|---|---|
| Pages (from-to) | 2919-2922 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 66 |
| Issue number | 22 |
| DOIs | |
| State | Published - 1991 |
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