Abstract
The diffusive behavior of the number-heat correlation function for an interacting electronic disordered system is determined at first order in the disorder strength. Singular corrections are found for the coefficient of the thermopower. The resulting scaling behavior in the various universality classes differs from that obtained in the noninteracting case.
- Received 24 July 1990
DOI:https://doi.org/10.1103/PhysRevB.43.11088
©1991 American Physical Society

