Abstract
In this work a complete simulation of single quantum well (QW) blue–green injection lasers was performed using conventional electron-hole plasma theory for the optical gain in strained quantum well lasers and classical one-dimensional transport in semiconductor heterostructures. The physical model is based on the self-consistent solution of the Poisson’s equation, the current continuity equations, including the thermionic emission theory for carrier transport across heterojunctions,1 the photon rate equation2 and the scalar wave equation for the optical field.3 The band structure of the strained ZnCd0.2Se0.8/ ZnS0.06Se0.94 QW was calculated using k.p theory.4
© 1994 Optical Society of America
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