“…Furthermore, the homogeneous broadening gain medium of EDF and longer fiber loop in the fiber laser would bring the unstable multi-longitudinal-mode (MLM) and mode-hopping output [6,7]. Hence, in order to attain the single-longitudinal-mode (SLM) oscillation in the EDF based lasers, a number of techniques have been proposed and demonstrated, such as exploiting a unpumped EDF or graphene based saturable absorbers (SAs) [8,9], using the multiple-ring architectures [10,11], employing optical-injection loop design [12,13], applying Mach-Zehnder interferometer (MZI) structure [14,15], and utilizing the Rayleigh backscattering (RB) method [16,17]. To accomplish the wavelength tunability in EDF lasers, different optical filters have been utilized inside the fiber cavity for selecting, such as the optical tunable bandpass filter (OTBPF), ultra-narrow filter, Fabry-Perot tunable filter (FP-TF), Silicon-micro-ring resonator (SMRR) and fiber Bragg grating (FBG) [18][19][20].…”