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We consider a macroscopic disordered system of free $d$-dimensional latticefermions whose one-body Hamiltonian is a Schr\"{o}dinger operator $H$ withergodic potential. We assume that the Fermi energy lies in the exponentiallylocalized part of the spectrum of $H$. We prove that if $S_\Lambda$ is theentanglement entropy of a lattice cube $\Lambda$ of side length $L$ of thesystem, then for any $d \ge 1$ the expectation $\mathbf{E}\{L^{-(d-1)}S_\Lambda\}$ has a finite limit as $L \to \infty$ and we identifythe limit. Next, we prove that for $d=1$ the entanglement entropy admits a welldefined asymptotic form for all typical realizations (with probability 1) as $L \to \infty$. According to numerical results of [33] the limit is notselfaveraging even for an i.i.d. potential. On the other hand, we show that for$d \ge 2$ and an i.i.d. random potential the variance of $L^{-(d-1)}S_\Lambda$decays polynomially as $L \to \infty$, i.e., the entanglement entropy isselfaveraging.

Large Block Properties of the Entanglement Entropy of Disordered Fermions