I. Introduction
Photodetectors are key components for future optical communication systems and require high-speed, high-efficiency features [1]. In particular, to meet the new challenges of 40-Gb/s applications, photodetectors must possess several characteristics.
They must operate at high power levels. The use of an erbium-doped-fiber optical preamplifier allows the decision circuit to be driven from the photodiode [2], [3]. As the usual broad-band electrical amplifier can be eliminated, the signal-to-noise ratio can be significantly improved for 40-Gb/s transmission [4]. In this case, the photodiode must handle optical power well above +10 dBm, corresponding to about a 10-mA saturation current for high output voltage.
They must provide high-efficiency photoreceiver modules at affordable prices [5]. The cost of a module is mainly linked to the tight fiber alignment tolerances in front of the photodetector, which requires a sophisticated, costly, and time-consuming pigtailing process.