have been successfully commercialized. Unfortunately, these crystals are hindered for further extensive applications due to their inherent drawbacks, such as low laser damage threshold (34 MW cm -2 and 13 MW cm -2 for AgGaS 2 and AgGaSe 2 , respectively) [5] and severe optical absorption for ZnGeP 2 . In addition, nonoxide crystals such as CdGeAs 2 , LiInS 2 and CdSiP 2 are commonly grown by Bridgman method. [6] The growth process of Bridgman method cannot be observed and adjusted in real time because of the closed system, making it challenging to obtain large-size single crystals with high optical quality. Unlike chalcogenides and pnictides, oxide NLO crystals usually have wide band gap and large laser damage threshold, which are important for NLO materials. [7] Meanwhile, oxide crystals possess good growth habits and excellent physical properties, which is very beneficial to large-scale commercialization. However, considering the absorption of high-frequency phonons or their overtones from light atoms, most of the oxide crystals are difficult to completely cover the 3-5 µm atmospheric window. Therefore, it is urgent to develop novel mid-IR NLO materials with wider transmission range, larger nonlinear coefficient, and higher laser damage threshold.High-performance ferroelectric crystals are some of the important and widely used functional materials in optical fields, owing to their excellent electro-optical, acousto-optical, and second-order NLO properties. [8] For example, LiNbO 3 crystal has been considered as one of the most commercial crystals for applications in nonlinear optics owing to the extraordinary properties, such as large NLO coefficients, moderate birefringence, phase-matchability, and high crystal quality. [9] However, because of the high-density light scattering domains existing in most high-performance ferroelectrics crystals, the realization of transparent ferroelectrics crystals with giant second-harmonic generation (SHG) has long been a challenge. [10] Despite more decades of effort, ferroelectric crystals with high transparency and giant SHG have been difficult to realize. Until 2020, Qiu et al. obtained transparent Pb(Mg 1/3 Nb 2/3 )O 3 -PbTiO 3 (PMN-PT) single crystal by applying alternating current to engineer the domain structures. [8b] This crystal exhibits a good transparency, a high piezoelectric coefficient, and a large electro-optical Environment-friendly lead-free potassium-sodium niobate (KNN) has become one of the most extensively investigated ferroelectrics in the past decade, while high transparency KNN single crystal has never been realized yet. Here, a transparent KNN single crystal is successfully grown by the top seeded solution growth method. The KNN crystal possesses a very wide transmittance range of 0.37-8 µm, completely covering the important mid-infrared atmospheric transparent window (3-5 µm). Noticeably, the KNN crystal exhibits the largest second-harmonic generation efficiency (7.6× that of potassium-titanyl phosphate (KTP)) with type-I phase matchability unde...