I. Introduction
Optical sources that generate pulses at multiple wavelengths are important for applications including fiber optic sensing, instrumentation, and communications. Erbium-doped fiber (EDF) lasers are ideal for generating such pulses. In order to obtain stable, multiwavelength operation with narrow wavelength spacing, approaches such as cooling the fiber to 77°K, temporal multiplexing, cascaded or composite cavities, frequency-shifting, and four-wave mixing (FWM) in a length of highly nonlinear fiber (HNLF), are used to overcome the limitations associated with homogeneous broadening of the EDF gain medium [1]–[12]. For continuous-wave (CW) operation, an EDF laser emitting 24 wavelengths with a spacing of 100 GHz has been achieved based on FWM in a length of HNLF [8] and 70 wavelengths with a spacing as narrow as 25 GHz has been obtained using an inhomogenous loss mechanism [9]. A mode-locked EDF laser operating on more than 24 wavelengths with 50-GHz spacing based on frequency-shifting was reported in [4]. FWM has also been considered for mode-locked operation [10]–[12]; however, the number of wavelengths is usually limited (up to 8 in [12]).