Abstract
The anisotropic tight-binding model, which is defined by a disordered tight-binding Hamiltonian with a transfer-energy-matrix element in the z direction, t, different than the one in the x-y plane is studied using finite-size scaling methods. The dependence of the mobility edge on the strength of anisotropy t (0t1) is obtained for the center of the band, E=0. Even for very low-t values an appreciable amount of disorder is needed to localize the E=0 state. These results are found to be in satisfactory agreement with the predictions of the potential-well analogy, coupled with the coherent-potential approximation. © 1989 The American Physical Society.
| Original language | English |
|---|---|
| Pages (from-to) | 2825-2830 |
| Number of pages | 6 |
| Journal | Physical Review B |
| Volume | 40 |
| Issue number | 5 |
| DOIs | |
| State | Published - Jan 1 1989 |
| Externally published | Yes |
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