The optical parametric oscillator (OPO) based on the periodically poled lithium tantalate (PPLT) crystal (40 mm×5 mm×1 mm) is fabricated. The OPO is pumped by a Q-switched Nd:YAG laser working at 1.064 μm. An average idler output power (around 3.8 μm) of 1.2 W and signal output power (around 1.48 μm) of 3 W are obtained when the pump power is 20 W. optical superlattice, mid-infrared laser, optical parametric oscillator (OPO), periodically poled lithium tantalate (PPLT) PACS: 42.65.Yj, 42.70.Mp, 42.72.Ai Infrared (IR) is usually divided into 3 spectral regions: near (0.75-3 μm), mid (3-20 μm) and far-infrared (20-1000 μm)[1]. Because most molecules have unique vibrational spectra in the mid-infrared region, spectroscopy in that region has many applications, from remote chemical sensing to biomedicine to trace-gas detection, etc. Reliable wavelength-tunable mid-IR lasers are required for spectroscopy in this region. The mid-infrared optical parametric oscillator (MIR-OPO) has the following features: broad tuning range, compact configuration, all-solid-state, high power output and narrow linewidth. Therefore it is currently a hot subject of research [2]. In order to achieve high conversion efficiency, birefringence-phase-matching (BPM) or the quasiphase-matching (QPM) technique must be introduced. QPM materials are sometimes referred to as the optical superlattice, including periodically poled lithium niobate (PPLN), lithium tantalate (PPLT) and potassium titanyl phosphate (PPKTP). QPM materials have been extensively used in the nonlinear optical processes (such as second harmonic generation (SHG), optical parametric amplification (OPA) and optical parametric oscillation (OPO)) due to the large effective nonlinear coefficient and the possibility that they can be engineered to suit a noncritical interaction configuration.