Abstract
The conductance of a disordered system of finite volume ( spatial dimensions) is calculated by making use of a recently developed self-consistent theory. Scaling equations are derived for the dimensionless conductance and the scaling function is explicitly calculated for arbitrary dimension . It is shown that the theory obeys scaling in the sense of Wegner, Thouless, and Abrahams et al.
- Received 6 November 1981
DOI:https://doi.org/10.1103/PhysRevLett.48.699
©1982 American Physical Society