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M. Mock (1986)
Basic theory of stationary numerical models
John Miller (1986)
On the inclusion of the recombination term in descretizations of the semiconductor device equationsMathematics and Computers in Simulation, 28
M. Mock (1983)
ANALYSIS OF A DISCRETIZATION ALGORITHM FOR STATIONARY CONTINUITY EQUATIONS IN SEMICONDUCTOR DEVICE MODELS, IICompel-the International Journal for Computation and Mathematics in Electrical and Electronic Engineering, 3
M. Mock (1983)
Analysis of mathematical models of semiconductors devices
D. Scharfetter, H. Gummel (1969)
Large-signal analysis of a silicon Read diode oscillatorIEEE Transactions on Electron Devices, 16
M. Mock (1976)
Time discretization of a nonlinear initial value problemJournal of Computational Physics, 21
K. Pen-Yu (1983)
NUMERICAL SOLUTION OF AN INITIAL‐VALUE PROBLEM FOR A SEMICONDUCTOR DEVICECompel-the International Journal for Computation and Mathematics in Electrical and Electronic Engineering, 2
M. Mock (1981)
A time-dependent numerical model of the insulated-gate field-effect transistorSolid-state Electronics, 24
K. Watt (1977)
Why won't anyone believe us ?Simulation, 28
M. Sever, P. Markowich (1987)
The Stationary Semiconductor Device Equations.Mathematics of Computation, 49
A new algorithm is presented for the discretization of semiconductor models in one space dimension plus time. A complete error analysis is given, showing that the discretization errors do not depend on any derivatives of illbehaved quantities such as carrier densities. In this algorithm, the electrostatic potential is updated from a discretization of the equation of total current continuity, and parabolic equations for the current densities are discretized, rather than those for the carrier densities. Projection methods, e.g. simple finiteelement methods, are used for the space discretization. The equations for the current densities are similar to the familiar ScharfetterGummel expressions in the stationary limit. However, the discrete timedependent current densities are required here to be H1 functions of x, obtained in a space with at least second order approximation property in L2. This method is fully compatible with recently developed methods for uncoupling the discrete systems to be solved at each time step, for an individual device or when a given problem involves multiple, coupled devices.
COMPEL: The International Journal for Computation and Mathematics in Electrical and Electronic Engineering – Emerald Publishing
Published: Mar 1, 1987
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