Anderson localization is a physical phenomenon in which electron transport in solid materials is inhibited by disorder. The Anderson model for this phenomenon consists of the Laplacian on a lattice perturbed by a random potential.
After briefly reviewing the mathematical theory of the Anderson model, I will explain my recent joint work with Jian Ding. We prove that, in the case of a Bernoulli potential and a two dimensional lattice, the eigenfunctions near the edge of the spectrum are exponentially localized. A key ingredient is a new unique continuation result for eigenfunctions of random Hamiltonians in dimension two.
Penn Mathematics Colloquium
Wednesday, April 24, 2019 - 3:30pm
Charles Smart
Univ. Chicago