C oupled vertical cavity surface-emitting laser (VCSEL) arrays are an attractive means to increase the coherent output power of VCSELs. Single-mode VCSELs, with output powers greater than 10 mW, would be useful as telecommunication transmitters (λ=1.3-1.55 µm) or sources for optical interconnects. Commercially available single-mode VCSELs, even at shorter wavelengths (λ=0.85 µm), are generally limited to a few milliwatts of output power. The conventional VCSEL structure incorporates a built-in positive-index waveguide, designed to support a single fundamental mode. Promising results in the 3-5 mW range (λ=0.85 µm) have been obtained from wet-oxidized, positive-index-guided VCSELs [1], [2] with small emission apertures (less than 3.5 µm-dia). The small aperture size leads to a high electrical resistance and high current density, which can impact device reliability.A larger emitting aperture is essential to reduce thermal rollover and achieve higher output powers with reliable operation. However, poor intermodal discrimination, gain-spatial-hole burning, and thermally induced self-focusing prevent single-mode outputs from larger aperture devices. Furthermore, to minimize nonlinear above-threshold effects, a relatively large built-in index step is desirable for mode stability in active devices. Unfortunately, positive-index-guided structures posses an inherent tradeoff between aperture size and index step, due to the modal cutoff conditions for single-mode operation.By contrast, antiguided VCSEL structures have shown promise for achieving larger aperture single-mode operation. To obtain high single-mode powers with a larger emitting aperture, the use of a negative-index guide (antiguide) is beneficial.