quantum well lasers offer the prospect of devices at intermediate wavelengths between about 690mn and l5Onin with applications in areas such as photodynamic therapy. The larger thermal conductivity of A1GaAS compared to that of A1GaInP could make the A1XGa)InlAs systeni attractive for high power devices. The incorporation of indium in the quantum well also improves material quality and introduces compressive strain which enhances the intrinsic perfonnance beyond that of the phosphide system due to the larger spin orbit splitting and more similar electron and hole density ofstates in Ga,ln1.As compared with Ga,In1P.We have modelled the gain and radiative recombination of wells with AI.45Gao55M barriers at a wavelength in the region 720 to 730nm. This shows that the intrinsic gain-current characteristic is superior to that of an idealised GaInP/AIGaJnP laser at the same wavelength. Devices have been fabricated, which operate at 685nmand 75Onni at room temperature, and the length dependence of the threshold current, measured as a function of temperature between 140K and 400K, analysed. At the shorter wavelength the room temperature threshold current is dominated by thennally activated carrier loss from the well. Although this could be reduced by further opthnisation, short wavelength operation is severely resthcted by the band gap of the A1GaAS barriers and this material system will be of greatest benefit for devices at wavelengths greater than about 7lOnm.