Mathematical Modelling and Simulation of Electrical Circuits and Semiconductor Devices 1990
DOI: 10.1007/978-3-0348-5698-0_10
|View full text |Cite
|
Sign up to set email alerts
|

Recent Progress in Algorithms for Semiconductor Device Simulation

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
5
0

Year Published

1991
1991
2023
2023

Publication Types

Select...
4
1
1

Relationship

1
5

Authors

Journals

citations
Cited by 6 publications
(5 citation statements)
references
References 25 publications
0
5
0
Order By: Relevance
“…( 5)). But The Gummel iteration (Gummel, 1964;Scharfetter & Gummel, 1969) was discovered decades ago by the semiconductor community (Bank et al, 1990;Bank, Rose & Fichtner, 1983;Hess, 1991;Hess, Leburton & Ravaioli, 1991;Jerome, 1995;Kerkhoven, 1988;Kerkhoven & Jerome, 1990;Kerkhoven & Saad, 1992;Lundstrom, 1992) and was discovered in my lab independently by Duan Chen, some years later (e.g., Chen & Eisenberg, 1993a). The iteration is a general method for producing a selfconsistent solution of coupled equations closely related to the self-consistent field methods used in quantum mechanics to compute orbitals.…”
mentioning
confidence: 99%
“…( 5)). But The Gummel iteration (Gummel, 1964;Scharfetter & Gummel, 1969) was discovered decades ago by the semiconductor community (Bank et al, 1990;Bank, Rose & Fichtner, 1983;Hess, 1991;Hess, Leburton & Ravaioli, 1991;Jerome, 1995;Kerkhoven, 1988;Kerkhoven & Jerome, 1990;Kerkhoven & Saad, 1992;Lundstrom, 1992) and was discovered in my lab independently by Duan Chen, some years later (e.g., Chen & Eisenberg, 1993a). The iteration is a general method for producing a selfconsistent solution of coupled equations closely related to the self-consistent field methods used in quantum mechanics to compute orbitals.…”
mentioning
confidence: 99%
“…To simplify things, let us discuss the ABF method assuming that (2) is being solved by the coupled (Newton) approach with a block Gauss-Seidel iteration being used for (12)• Hence, we are interested in solving a linear system of algebraic equations D-1 is the ABF postconditioner. We then solve (19) by block Gauss-Seidel (or block SSOR) iteration; the diagonal block system arising in the Gauss-Seidel iteration can be solved via sparse direct or preconditioned iterative methods [3,2].…”
Section: The Abf Methodmentioning
confidence: 99%
“…The work ofT. F. Chan If there are v degrees of freedom associated with the underlying discrete approximation to each PDE, then (2) represents m y nonlinear algebraic equations to be solved.…”
Section: Z)\ \ L ( Z L Zz Zm) /mentioning
confidence: 99%
“…) can be obtained, the component of the current integration Equation ( 11) can be rewritten as In the present implementation, a 1-D discretization grid is adopted for the physical model of the semiconductor device, which is fully independent of the 3-D-FDTD mesh. For the physical model, space-domain integration of the semiconductor device current equations relies on the well-known Scharfetter-Gummel scheme [21], whereas a backward-Euler algorithm [22] is adopted to accomplish time-domain integration. Based on the assumption of a quasi-stationary approximation holding for active devices; i.e., the size of device active regions is assumed to be negligible, with respect to the minimum signal wave-length, the device can therefore be regarded, when solving Maxwell's equations, as a "lumped" (i.e., zero-dimensional) element, while the dielectric constant in the device region is assumed to be that of air, and thus Maxwell's equations, including a semiconductor device, in integral form, can be described as:…”
Section: Electromagnetic-physics-based Simulationmentioning
confidence: 99%