Abstract
A criterion for localization of electron states in disordered materials is presented. Applications to binary alloys, made using the self-energy calculated in the coherent-potential approximation, confirm the Mott-Cohen-Fritzsche-Ovshinsky model in detail. Mobility edges occur inside the band edges. A mobility gap can appear within the band. The band can split into sub-bands, each with mobility edges. Below a critical concentration, an Anderson transition, where the minority sub-band becomes entirely localized, can occur.
| Original language | English |
|---|---|
| Pages (from-to) | 520-524 |
| Number of pages | 5 |
| Journal | Physical Review Letters |
| Volume | 25 |
| Issue number | 8 |
| DOIs | |
| State | Published - 1970 |
| Externally published | Yes |
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