Abstract
Performing a two-cutoff scaling in 2+μ dimensions, we find that an Anderson transition does take place in the presence of the spin-orbit interaction. The mobility edge is shifted to lower values and the conductivity in the metallic phase has the form f=(e22)3/4-(d-2)g*f(Ls.o.3/4), where f(Ls.o.3/4) is a crossover function, 1+32 (3/4Ls.o.)d-2, 3/4 is the localization length, Ls.o. is the spin-orbit diffusion length, and g* is the Anderson critical conductance.
| Original language | English |
|---|---|
| Pages (from-to) | 6698-6700 |
| Number of pages | 3 |
| Journal | Physical Review B-Condensed Matter |
| Volume | 36 |
| Issue number | 12 |
| DOIs | |
| State | Published - 1987 |
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