I. Introduction
Multiwavelength fiber lasers have attracted much interest in recent years because of their potential applications in wavelength-division-multiplexed (WDM) technique, fiber sensor system, and optical instrument testing [1]–[3]. Various techniques for the reduction of wavelength competition have been used to achieve stable multiwavelength oscillations. The wavelength competition originates from the homogeneous gain broadening of erbium-doped fiber (EDF) [2]. In order to overcome this limitation, approaches such as cooling the EDF to 77 K to make the gain medium inhomogeneous or polarization hole burning have been proposed [4], [5].