Abstract
In this work we utilize the Finite-Difference Time Domain (FDTD) Method coupled to a full band, particle-based simulator to solve for the total Lorentz force. Replacing a traditional Poisson solver with a more robust electromagnetics (EM) solver allows us to accurately account for radiated losses and provides a useful tool for investigating the near and far-field radiation patterns inherent in modern devices.
Similar content being viewed by others
References
K.S. Yee, “Numerical solution of initial boundary value problems involving Maxwell's equations in isotropic media, ” IEEE Trans. Antennas and Propagat., 14, 302 (1966).
K.M. Connolly, S.M. El-Ghazaly, R.O. Grondin, and R.P. Joshi, “Coupling Maxwell's equation time domain solution with Monte-Carlo technique to simulate ultrafast optically controlled switches, ” IEEE MTT-S Digest, 295 (1990).
S.M. Goodnick, S.S. Pennathur, U.A. Ranawake, P.M. Lenders, and Vijai K. Tripathi, “Parallel implementation of a Monte Carlo particle simulation coupled to Maxwell's equations, ” International Journal of Numerical Modeling: Electronic Networks, Devices and Fields, 8, 208 (1995).
K.A. Remley, A. Weisshaar, S.M. Goodnick, and V.K. Tripathi, “Characterization of near-and far-field radiation from ultrafast electronic systems, ” IEEE Transactions on Microwave Theory and Techniques, 46(12) (1998).
S. Hammadi, “Time domain methods for the global simulation of millimeter-wave transistors and circuits, ” Ph.D. Thesis, Arizona State University.
A. Leitenstorfer, S. Hunsche, J. Shah, M.C. Nuss, and W.H. Knox, “Femtosecond high-field transport in compound semiconductors, ” Phys. Rev., B61, 16642 (2000).
S. Wigger, M. Saraniti, S. Goodnick, and A. Leitenstorfer, “Fullband particle-based simulation of high-field transport in III-IV semiconductors, ” J. Comp. Elect., 1, 475 (2002).
C. Jacoboni and P. Lugli, The Monte Carlo Method for Semiconductor Device Equations (Springer-Verlag, Wien, 1989).
M. Fischetti and S. Laux, “Monte Carlo analysis of electron transport in small semiconductor devices including band structures and space-charge effects, ” Phys. Rev, B38(14), 9721 (1988).
M. Saraniti and S.M. Goodnick, “Hybrid full-band cellular automaton/ Monte Carlo approach for fast simulation of charge transport in semiconductors, ” IEEE Transactions on Electron Devices, 47(10), 1909 (2000).
K. Kometer, G. Zandler, and P. Vogl, “Lattice-gas cellularautomaton method for semiclassical transport in semiconductors, ” Phys. Rev., B46(3), 1382 (1992).
R. Courant, K. Friedrichs, and H. Lewy, “On the partial difference equations of mathematial physics, ” IBM Journal, 215 (1967).
J.P. B´erenger, “Perfectly matched layer for the FDTD solution of wave-structure interaction problems, ” IEEE Trans. Antennas Propagat., 44, 110 (1996).
J.P. B´erenger, “Three-dimensional perfectly matched layer for the absorption of electromagneticwaves, ” J. Comput. Phys., 127, 363 (1996).
D.M. Sullivan, “A simplified PML for use with the FDTD method, ” IEEE Microwave and Guided Wave Letters, 6(2), 97 (1996).
D.M. Sullivan, Electromagnetic Simulation Using the FDTD Method (IEEE Press Series on RF and Microwave Technology, New York, 2000).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Ayubi-Moak, J., Goodnick, S., Aboud, S. et al. Coupling Maxwell's Equations to Full Band Particle-Based Simulators. Journal of Computational Electronics 2, 183–190 (2003). https://doi.org/10.1023/B:JCEL.0000011422.05617.f1
Issue Date:
DOI: https://doi.org/10.1023/B:JCEL.0000011422.05617.f1