play a great role in the lidar, spectroscopy analysis and distributed optical fiber sensing [1][2][3]. Of these multiwavelength fiber lasers, the fiber lasers around 2 μm can achieve potential applications in atmospheric transmission, gas sensing, lidar and new wavelength-divisionmultiplexed fiber communication systems [4][5][6]. Hence, the research of switchable narrow linewidth multi-wavelength fiber ring lasers around 2 μm has significance to the above fields.Switchable multi-wavelength fiber lasers mainly employ overlap cavities or polarization hole burning (PHB) to control or adjust the properties of wavelength, and therefore to achieve wavelength switching. Corresponding to the properties, various methods have been proposed and reported, such as cascaded FBGs [7], highly birefringent (Hi-Bi) fiber loop mirrors [8], Sagnac loop mirror [9], fiber Bragg gratings (FBGs) written in Hi-Bi fibers [10,11], acoustic waves [12], spatial mode beating of multimode fiber [13] and cascaded filter structures [14]. However, multi-wavelength lasers in some special applications require the specific wavelength to be tunable or controllable, for instance, switching from one lasing line to another or two lasing lines at the same time. For example, this laser can be tuned and switched to the specific absorption wavelengths of some certain gases in multi-gases sensing application [15], or to the transmit window in atmospheric transmission application [16]. The laser topology based on the combination of the FBGs and ultra-narrow bandwidth phase-shifted FBGs using optical circulator is an effective method to achieve switchable multi-wavelengths; however, it is complex, costly and not tunable [17].In this paper, a switchable, tunable and power-controllable dual-wavelength Tm-Ho co-doped fiber laser (THCDFL) around 2 μm is proposed and experimentally Abstract We demonstrate a switchable, tunable and power-controllable dual-wavelength fiber laser in 2-μm region based on parallel cavities using a 3 × 3 coupler. The laser topology is based on the parallel connection of fiber Bragg gratings (FBGs) using 3 × 3 coupler which act as two individual cavities, so that the dual wavelengths are tunable and switchable by adjusting the center wavelengths of FBGs and the cavity losses, respectively. With suitable cavity losses and input pumping power, we can obtain a 2-μm switchable single-or dual-wavelength fiber laser. The proposed configuration has very good application prospects in the fields of atmospheric transmission, gas sensing, lidar and new wavelength-division-multiplexed fiber communication systems.