We present here a model of carrier distribution and transport in
semiconductor alloys accounting for quantum localization effects in disordered
materials. This model is based on the recent development of a mathematical
theory of quantum localization which introduces for each type of carrier a
spatial function called \emph{localization landscape}. These landscapes allow
us to predict the localization regions of electron and hole quantum states,
their corresponding energies, and the local densities of states. We show how
the various outputs of these landscapes can be directly implemented into a
drift-diffusion model of carrier transport and into the calculation of
absorption/emission transitions. This creates a new computational model which
accounts for disorder localization effects while also capturing two major
effects of quantum mechanics, namely the reduction of barrier height (tunneling
effect), and the raising of energy ground states (quantum confinement effect),
without having to solve the Schr\"odinger equation. Finally, this model is
applied to several one-dimensional structures such as single quantum wells,
ordered and disordered superlattices, or multi-quantum wells, where comparisons
with exact Schr\"odinger calculations demonstrate the excellent accuracy of the
approximation provided by the landscape theory.Comment: 17 pages, 18 figures, 3 table