“…When the potential is deterministic, i.e., v ε (x, ω) = v ε (x), many numerical methods have been proposed; see [4,16,39,27,15,9,8] for example. When the potential is random, few works have been done; see [40,25]. As mentioned above, the major difficulty is that the wavefunction ψ ε develops high-frequency oscillations in both the physical space and the random space, which requires tremendous computational resources.…”