We report the growth, fabrication and characterization of high-quality AlGaN/GaN solar-blind p-i-n and MSM photodetectors by low-pressure metalorganic chemical vapor deposition (MOCVD). The epitaxial layers were grown on double-polished c-plane (0001) sapphire substrates to allow for back-side illumination. The p-i-n photodiode structures typically consist of a 0.7 mm thick Al 0.58 Ga 0.42 N "window" layer, graded to a 0.2 mm thick Al 0.47 Ga 0.53 N n layer, a 0.15 mm thick Al 0.39 Ga 0.61 N i layer, a 0.2 mm thick Al 0.47 Ga 0.53 N p layer, and capped with a 25 nm GaN : Mg contact layer. At a 0 V bias, the processed p-i-n devices exhibit a solar-blind photoresponse having a maximum responsivity of 0.058 A/W at 279 nm, corresponding to an external quantum efficiency of $26%, uncorrected for reflections, etc. The MSM devices typically consist of an AlGaN x $ 0.58 window layer, and an undoped AlGaN x $ 0.44 absorbing layer. The MSMs exhibit an external quantum efficiency as high as $47% at a bias of 15 V with a peak response at 262 nm.Introduction Photodetectors operating in the wavelength range between 250 and 300 nm, referred to as the solar-blind regime, can be used for applications such as missile detection and tracking and for biological agent and chemical detection. The III-nitride material system is ideal for these detectors, as they can be designed to have a cutoff wavelength below 300 nm. The metal-semiconductor-metal (MSM) device is well suited for this application, as it is relatively simple to fabricate and its low capacitance can result in a fast response time. Advances in material growth have resulted in high aluminum composition and crack-free AlGaN heterostructures for use as solarblind p-i-n photodetectors [1]. The p-i-n device has the advantage of operating at zero to low bias, eliminating the requirement for a bulky power supply. We report the growth, fabrication and characterization of high-quality AlGaN/GaN heteroepitaxial back-illuminated solar-blind p-i-n and MSM photodetectors with high external quantum efficiencies.