I. Introduction
GaInP–AlGaInP high-power lasers operating in the wavelength range of 630–690 nm are required for a number of applications, including photodynamic therapy and read/write optical storage systems. Unfortunately p-doped AlGaInP has a large electrical resistivity due to incomplete activation of the dopant [1], low hole mobility [2], and a relatively poor thermal conductivity [3]. These properties exacerbate the thermal management problems associated with high power lasers. However, the reduction in penetration of the optical mode into the cladding layers which occurs in large optical cavity (LOC) structures [4] opens up the possibility of reducing the cladding-layer thickness, thereby reducing the electrical and thermal resistance. In addition to the need to maintain coupling of the optical mode to the quantum wells, there are two further factors which limit the extent to which the cladding thickness can be reduced. The first is the leakage of the mode into the absorbing GaAs contact layer and substrate, increasing the gain requirement and hence the intrinsic threshold current. The second is the thermally activated leakage current, which in GaInP-based lasers is due to drift and diffusion of electrons through the p-cladding layer. The leakage current increases as the cladding thickness is reduced, increasing the threshold current, which could cause an increase in power dissipation and increased internal temperature rise, negating the benefits of the reduced thermal impedance. In this paper, we investigate the interplay of these effects by analyzing the performance of LOC structures with three different values of cladding-layer thickness 0.3, 0.5, and 1 m.