Since the first experimental demonstration of a semiconductor laser using Stranski-Krastanow (SK) quantum dots (QDs) as gain medium [l,2], these lasers are intensely studied all over the world [3]. The predominant motivation for most authors are the theoretically predicted advantages of a gain medium with zero-dimensional density of states (DOS) , such as low threshold current density, high To [4] and high material and differential gain [5]. In QD lasers the lateral carrier diffusion is suppressed as compared to quantum well (QW) devices due to carrier localization in the QDs. Therefore, nonradiative recombination of nonequilibrium carriers at laser facets, or their spreading out of the injection region, can be significantly suppressed. Furthermore, the 3D shape of SK-QDs together with a sufficiently large volume of the narrow gap material which can be coherently incorporated in the matrix allows fabrication of light emitting devices at longer wavelemgths as compared to conventional pseudomorphic QWs on the same substrate.Clear advantages of QD lasers are evident for high power applications for h 2 1.1 pm range. These diodes are needed as pump sources for rare-earth-doped fiber lasers, which are the compact sources of blue-green light (e.g. 480 nm emission is realized from Tm-doped fiber lasers pumped at k 1 1 2 0 pm). The required wavelength is however beyond the reach of "classical" InGaAdGaAs QW-based lasers. At the same time this wavelength can be easily achieved with InGaAdGaAs QDs. Furthermore, the reduced facet overheating helps to prevent catastrophical optical damage (COD) at high output powers. The schematic representation of an Al-free InGaAdGaAs QD laser for h = 1. lpm grown by MOCVD is shown in Fig.