TWODIMENSIONAL MODELING OF QUANTUMWELL SEMICONDUCTOR LASERSLi, Z.M.; Dzurko, K.M.; McAlister, S.P.
1991 COMPEL: The International Journal for Computation and Mathematics in Electrical and Electronic Engineering
doi: 10.1108/eb051703
We have developed a twodimensional model for quantumwell lasers which solves, selfconsistently, the semiconductor equations together with the complex scalar wave equation and the photon rate equation. To predict the threshold current accurately we have included the wavelength and positiondependence of the gain and the spontaneous emission. For the complex wave equation successive over relaxation SOR is used with two adaptive acceleration parameters for the complex wave amplitude and for the eigenvalue. Since the rate equation near threshold can be driven into divergence during iteration for a steady state solution, we have introduced a special damping technique to overcome this problem. Our model enables us to predict the characteristics of a quantumwell laser with a minimal number of empirical constants. The output of the model includes lightcurrent characteristics, and the current and optical field intensity distributions. We show the results of a calculation for a gradedindex separateconfinement heterostructure single quantumwell GRINSCH SQW laser.
SIMULATION OF BIPOLAR TRANSPORT IN SEMICONDUCTOR PN JUNCTIONS USING THE GENERALIZED HYDRODYNAMIC EQUATIONSHamza, Mohammad; Morel, H.; Chante, J.P.
1991 COMPEL: The International Journal for Computation and Mathematics in Electrical and Electronic Engineering
doi: 10.1108/eb051706
A full consistent discretization scheme of the improved carrier density, momentum and energyconservation equations is presented. The carrier heat flux as well as the convection and recombination terms are considered. The convection terms are averaged and then the differential constitutive relations of the current density and the energy flux are solved. The proposed discretization scheme generalizes the ScharfetterGummel SG difference approximation to the generalized hydrodynamic model HDM. On the basis of this scheme the hydrodynamic equations HDE's are solved for both electrons and holes. The transport of hot carriers in the pin diode is investigated over a large scale of biasing values. The electric field distribution is not severely purturbed by the hot electron effects up to the medium biasing range. However, the minority carrier distribution is significantly affected by the carrier temperaturegradients near the spacechargeregions. The minority carriers that are diffused to the edge of depleted regions are heated and if the carrier temperature gradient is sufficiently strong they diffuse back to the neutral cold region rather than to be captured by the electric field as known from the standard DDM theory.
UNIFIED FRAMEWORK FOR THERMAL, ELECTRICAL, MAGNETIC, AND OPTICAL SEMICONDUCTOR DEVICE MODELINGWachutka, Gerhard
1991 COMPEL: The International Journal for Computation and Mathematics in Electrical and Electronic Engineering
doi: 10.1108/eb051708
The thermodynamic model constitutes a unified theoretical framework for the coupled simulation of carrier and energy flow in semiconductor devices under general ambient conditions such as, e.g., the presence of a quasistatic magnetic field or the interaction with an electromagnetic radiation field light. The current relations governing particle and heat transport are derived from the principles of irreversible phenomenological thermodynamics the driving forces include drift, diffusion, thermal diffusion, and deflection by the Lorentz force. All transport coefficients may be interpreted in terms of wellknown thermodynamic effects and, hence, can be obtained from theoretical calculations as well as directly from experimental data. The thermodynamic model allows the consistent treatment of a wide variety of physical phenomena which are relevant for both the operation of electronic devices e.g., lattice heating, hot carrier and low temperature effects and the function of microsensors and actuators e.g., thermoelectricity, galvanomagnetism and thermomagnetism.