TY - JOUR
T1 - Two‐dimensional simulation of quantum well lasers
AU - Song, G. Hugh
AU - Hess, Karl
AU - Kerkhoven, Thomas
AU - Ravaioli, Umberto
PY - 1990
Y1 - 1990
N2 - A versatile two‐dimensional simulator for various types of semiconductor lasers for both steady state and transients has been developed. The simulator is capable of spectral analysis of quantum‐well semiconductor lasers, such as gain‐spectrum analysis, as well as analysis of the two‐dimensional current flow and optical intensity patterns. The simulator is based on the drift‐diffusion model with full Fermi‐Dirac statistics for the transport equations as well as for the Poisson equation. Simulation of the thermionic emission current is required at the abrupt heterointerfaces of the quantum well. For the spectral analysis of quantum‐well lasers, we have used the photon rate equation for each Fabry‐Perot mode. For the optical intensity pattern, we have solved the two‐dimensional Helmholtz eigenvalue equation using the subspace iteration method. The transient simulation is done by the full backward‐Euler method in conjunction with the full Newton approach for the entire semiconductor equations. To demonstrate the simulator, a model GaAs‐AIGaAs graded‐index‐separate‐confinement‐heterostructure buried‐quantum‐well laser is analyzed.
AB - A versatile two‐dimensional simulator for various types of semiconductor lasers for both steady state and transients has been developed. The simulator is capable of spectral analysis of quantum‐well semiconductor lasers, such as gain‐spectrum analysis, as well as analysis of the two‐dimensional current flow and optical intensity patterns. The simulator is based on the drift‐diffusion model with full Fermi‐Dirac statistics for the transport equations as well as for the Poisson equation. Simulation of the thermionic emission current is required at the abrupt heterointerfaces of the quantum well. For the spectral analysis of quantum‐well lasers, we have used the photon rate equation for each Fabry‐Perot mode. For the optical intensity pattern, we have solved the two‐dimensional Helmholtz eigenvalue equation using the subspace iteration method. The transient simulation is done by the full backward‐Euler method in conjunction with the full Newton approach for the entire semiconductor equations. To demonstrate the simulator, a model GaAs‐AIGaAs graded‐index‐separate‐confinement‐heterostructure buried‐quantum‐well laser is analyzed.
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U2 - 10.1002/ett.4460010403
DO - 10.1002/ett.4460010403
M3 - Article
AN - SCOPUS:84985777321
SN - 1124-318X
VL - 1
SP - 375
EP - 381
JO - European Transactions on Telecommunications
JF - European Transactions on Telecommunications
IS - 4
ER -