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PISCES-2ET and Its Application Subsystems - Stanford Technology ...

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CHAPTER 2<br />

DUET Carrier Transport<br />

Model<br />

The DUET model, a carrier transport model in semiconductors, is developed based on the moment<br />

approach to solving Boltzmann Transport Equation (BTE). It uses six state variables to describe the<br />

status of a semiconductor device. These six variables are: electrostatic potential, ψ, carrier<br />

concentrations, n <strong>and</strong> p, carrier temperatures, T n <strong>and</strong> T p , <strong>and</strong> lattice temperature, T L , <strong>and</strong> they are<br />

functions of space <strong>and</strong> time. All other device characteristics such as terminal I-V characteristics <strong>and</strong><br />

circuit model parameters can be calculated from the knowledge of the distribution of these basic<br />

variables. To determine the distribution of these variables under applied bias, six independent<br />

equations are required together with proper boundary conditions. It is well established that with the<br />

drift-diffusion (DD) carrier transport model, Shockley semiconductor equations, i.e., Poisson’s<br />

equation <strong>and</strong> carrier continuity equations, govern the distribution of ψ, n, <strong>and</strong> p. The carrier<br />

concentrations can also be replaced, equivalently, by their respective quasi-Fermi levels, <strong>and</strong> ,<br />

in classical distribution (either Boltzmann or Fermi-Dirac) functions. With the temperatures for both<br />

carriers <strong>and</strong> lattice introduced as independent variables, three more equations are needed <strong>and</strong> they can<br />

be derived from the energy balance principle. In this chapter, we will first introduce two (kinetic)<br />

energy balance equations for carriers <strong>and</strong> one thermal diffusion equation for the lattice. Various macro<br />

quantities such as carrier <strong>and</strong> energy densities will be defined using the distribution function at the<br />

quasi-thermal equilibrium. The auxiliary expressions for transport are provided. Finally the proper<br />

boundary conditions for solving differential equations are discussed.<br />

φ n<br />

φ p<br />

<strong>PISCES</strong>-<strong>2ET</strong> – 2D Device Simulation for Si <strong>and</strong> Heterostructures 5

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