Non-parabolic band hydrodynamical model of silicon semiconductors and simulation of electron devices
β Scribed by Vittorio Romano
- Publisher
- John Wiley and Sons
- Year
- 2001
- Tongue
- English
- Weight
- 341 KB
- Volume
- 24
- Category
- Article
- ISSN
- 0170-4214
- DOI
- 10.1002/mma.220
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β¦ Synopsis
Abstract
A consistent hydrodynamical model for electron transport in silicon semiconductors, free of any fitting parameter, has been formulated in Anile and Romano (Continuum Mechanics Thermodynamics 1999; 11:307β325) and Romano (Continuum Mechanics Thermodynamics 1999; 12:31β51) on the basis of the maximum entropy principle, by considering the energy band described by the Kane dispersion relation. Explicit constitutive functions for fluxes and production terms in the macroscopic balance equations of density, crystal momentum, energy and energy flux have been obtained. Scatterings of electrons with nonβpolar optical phonons (both for intervalley and intravalley interactions), acoustic phonons and impurities have been taken into account.
In this article we show the link with other macroscopic models describing the motion of charge carriers. In particular, under suitable scaling assumptions, an energy transport model is recovered. An analysis of the formal properties is given by showing that the evolution equations form a hyperbolic system in the physically relevant region of the space of the dependent variables. At last, by using the numerical method developed in Liotta et al. (International Series of Numerical Mathematics 1999; 130:651β660) and Liotta et al. (SIAM Journal on Numerical Analysis 1999, to appear) simulations for bulk silicon and n^+^βnβn^+^ silicon diode are performed. The obtained results are in good agreement with the Monte Carlo data. Copyright Β© 2001 John Wiley & Sons, Ltd.
π SIMILAR VOLUMES
## Abstract We investigate the application of preconditioned generalized minimal residual (GMRES) algorithm to the equations of hydrodynamic model of semiconductor devices. An introduction to such a model is presented. We use finiteβelement method __P__~1~β__isoP__~2~ element to discretize the equa