6533b828fe1ef96bd1287c09

RESEARCH PRODUCT

Macroscopic conductivity of free fermions in disordered media

C. HertlingJean-bernard BruJean-bernard BruJean-bernard BruW. De Siqueira Pedra

subject

PhysicsQuantum PhysicsCondensed matter physics82C70 82C44 82C20FOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)FermionConductivityMacroscopic scaleLattice (order)Quantum mechanicsTrivial measureOhmQuantum Physics (quant-ph)Electrical conductorAnderson impurity modelMathematical Physics

description

We conclude our analysis of the linear response of charge transport in lattice systems of free fermions subjected to a random potential by deriving general mathematical properties of its conductivity at the macroscopic scale. The present paper belongs to a succession of studies on Ohm and Joule's laws from a thermodynamic viewpoint. We show, in particular, the existence and finiteness of the conductivity measure $\mu _{\mathbf{\Sigma }}$ for macroscopic scales. Then we prove that, similar to the conductivity measure associated to Drude's model, $\mu _{\mathbf{\Sigma }}$ converges in the weak$^{\ast } $-topology to the trivial measure in the case of perfect insulators (strong disorder, complete localization), whereas in the limit of perfect conductors (absence of disorder) it converges to an atomic measure concentrated at frequency $\nu =0$. However, the AC--conductivity $\mu _{\mathbf{\Sigma }}|_{\mathbb{R}\backslash \{0\}}$ does not vanish in general: We show that $\mu _{\mathbf{\Sigma }}(\mathbb{R}\backslash \{0\})>0$, at least for large temperatures and a certain regime of small disorder.

10.1142/s0129055x14500081http://hdl.handle.net/20.500.11824/173