I. Introduction
Gain-Clamped erbium-doped fiber amplifiers (EDFAs) using fiber Bragg gratings (FBGs), traditionally are used to create Fabry–Pérot resonators [1], [2] which allow for the out-of-band laser to oscillate and limit the population inversion. Two simultaneous signals propagate through the 980-nm forward pumped amplifier. Transmission spectra of the three FBGs showing −30.47-, −26.83-, and −33.51-dB loss at 1549, 1551, and 1555 nm, respectively. The signals wavelengths are located between these FBG wavelengths. Alternatively, the FBGs have also been used to reflect an externally injected out-of-band signal [3] that provides a similar population limitation as the former case. An early attempt to gain-clamp an EDFA just by passive amplification of backward amplified spontaneous emission (ASE) produced satisfactory results [4] but with a gain of 21 dB for eight channels.