In this section, the two cornerstones of semi-classical device simulation are given -- Poisson's equation and Boltzmann's equation. While electrostatics is covered by Poisson's equation, Boltzmann's equation describes the propagation of the distribution function within a simulation domain. These two equations are solved in a self consistent manner for example in Monte-Carlo simulators, often used as a reference for higher-order transport models which are derived from the Boltzmann transport equation as well.
M. Wagner: Simulation of Thermoelectric Devices