We demonstrate a single-longitudinal-mode Ho 3þ :YVO 4 unidirectional ring laser based on the acousto-optic effect, utilizing the features of the acousto-optical Q switch and half-wave plate to achieve unidirectional operation. The maximum power achieved in the single-longitudinal-mode at 2053.9 nm is 941 mW when the absorbed power is set as 4.4 W, yielding a nearly 50% slope efficiency. The M 2 factor is 1. A 2 μm single-longitudinal-mode laser has the characteristics of eye safety and good transparency in the atmosphere. It has important applications in the areas of laser lidar, high resolution spectroscopy, and achieving 3-12 μm lasers [1,2] . So far, many configurations have been applied to achieve the single-longitudinal-mode lasers near 2 μm, such as the coupled cavity laser [3] , twisted-modecavity laser [4] , the microchip laser [5] , the nonplanar ring laser, the intracavity etalons laser [6] , etc. Among them, the nonplanar ring laser [7,8] and twisted-mode-cavity laser [9] are two common ways to obtain high power singlelongitudinal-mode operation, while they are applicable to only isotropic gain medium and are difficult for achieving single-longitudinal-mode operation with a long cavity length, which result in limiting the narrower linewidth output. Instead, a unidirectional ring laser utilizing the feature that the acousto-optic (AO) device has for different diffraction losses for different polarization beams can resolve the aforementioned issue. The unidirectional ring laser realized by the AO technique has the advantage of a long cavity design and a low insertion loss, which makes it possible to achieve a narrow linewidth and high power output simultaneously. In addition, this technique also has a wide spectral operating range and can be used to produce Q-switching of the single-frequency output [10] . A 2 μm single-longitudinal-mode laser is used for the lidar system, where the improvement of these two characteristics will enhance the performance (resolution, detection range, and precision) of the whole lidar system. In earlier years, the unidirectional Nd 3þ -doped ring lasers at 1 μm were demonstrated. In 1991, Clarkson and Hanna reported an Nd:YAG laser, which has a 32 mm long resonator [11] . A travelling-wave AO Q switch is inserted in a simple standing-wave resonator, and its maximum single frequency power is 100 mW. In the same year, they used the same method to construct a unidirectional operation of an Nd:YLF ring laser [12] with a maximum output power of 340 mW. Yet, the output characteristics of single-longitudinal-mode ring lasers at 2 μm are rarely investigated. In 2004, Shen et al. reported an Ho:YAG ring laser with a short cavity length (536 mm) in which a travelling-wave TeO 2 AO modulator (AOM) is used to acquire unidirectional oscillation [13] . However, to realize a narrower linewidth output of 2 μm, the longer cavity length is needed, which leads to the increase of the longitudinal mode numbers and threshold pump power. Finally, the higher radio frequency (RF) power of the AO d...