I. Introduction
Multiwavelength erbium-doped fiber lasers (EDFLs) attract much interest due to their potential applications in fiber sensing, component testing, optical signal processing, and wavelength-division-multiplexing optical communication systems. Different techniques have been proposed to realize multiwavelength oscillations at room temperature in EDFLs. These include the introduction of polarization hole burning effect by using polarization-dependent elements in the laser cavities [1]–[3], and nonlinear optical approaches by inducing various nonlinear effects such as four-wave mixing [4] and stimulated Brillouin scattering [5] in the laser cavity. Room-temperature multiwavelength operation in an EDFL has been also reported in [6] by inserting a frequency shifter in the laser cavity to prevent steady-state oscillations. Other methods of incorporating in the laser cavity a length of multimode fiber [7] or a multimode fiber Bragg grating [8], employing specially designed erbium-doped fibers (EDFs) [9] or cavity structures [2], [10] were also reported. Recently, multiwavelength single frequency operation was also obtained by dual-pumping a distributed Fabry–Pérot (F-P) feedback structure[11].