Abstract-A four-wave mixing wavelength converter with no external pump laser and very low input signal power requirements is characterized. The wavelength conversion occurs inside a high-reflection/antireflection coated semiconductor optical amplifier pigtailed with a fiber Bragg grating. The pump signal is provided by the lasing mode at the Bragg wavelength. A 1-mW optical signal modulated at 2.5 Gb/s is converted over 9 nm with error rates below 10 09 . To be technologically competitive, wave-mixing frequency converters need good conversion efficiency, high signalto-noise ratio (SNR) on the converted signal, and reduced complexity. In this letter, we present a promising four-wave mixing (FWM) technique that addresses these three criteria simultaneously.
Index Terms-CommunicationA straightforward strategy to improve the FWM performance in semiconductor optical amplifiers (SOA's) is to increase the amplifier gain-length product and/or the pump power. This has led to good converter performance, using high-power erbium-doped fiber amplifiers (EDFA's) and long . The self-pumped (lasing) and folded-path configuration proposed in this letter is a candidate to implement the gain-length optimization strategy. Folding the modulated signal path by reflection off one of the cavity mirrors doubles the interaction length, while the lasing action maintains the gain (and hence, the nonlinearity) clamped at the threshold value (as opposed to external pumping where the gain is saturated by the total input power). Furthermore, the fiber Bragg grating used at the other end of the lasing cavity can, in principle, be optimized to achieve high internal lasing power and good pump suppression at the output. Although the pump is not tunable in the present configuration, a similar scheme using a tunable DBR mirror instead of a Bragg grating could be envisioned. The converter is a small external cavity semiconductor laser, where the feedback is provided on one end of the semiconductor by a high-reflection coating, and on the other end (antireflection coated) by a pigtailed fiber Bragg grating (see Fig. 1). The cavity length and reflectivity profiles are optimized for single-mode laser oscillation. The active region is 500-m-long, temperature controlled, and biased at 170 mA. The lasing threshold is 32 mA and the pump output power at the operating point is 7.5 dBm. Modulated input signals (with wavelengths outside of the Bragg reflection bandwidth) are injected into the cavity through the Bragg grating using a bidirectional coupler. The converted signal is collected from the other input arm of the coupler. A tunable external-cavity semiconductor laser is externally modulated at 2.5 Gb/s by a pseudorandom bit stream (2 1 PRBS, no