suffering from some intrinsic demerits, e.g., the low laser damage thresholds (LDTs) (<30 MW cm −2 ) for AGX (X = S, Se), nonphase matching for AGSe and the strong two-photon absorptions for ZGP under 1 µm pumping resource, which prohibit their application in the high-power lasers. [16][17][18][19] Therefore, exploring new MIR NLO crystal is still of the current research interest.Nevertheless, rationally synthesizing a high-performance MIR NLO crystals is still faced a great challenge, because an excellent IR NLO crystal needs not only a noncentrosymmetric (NCS) structure but also a series of harsh functional properties, including i) large second harmonic generation (SHG) response (≥ 0.5 × AGS); ii) wide optical transparent range, covering two atmospheric windows, 3-5 and 8-12 µm; iii) large bandgap (>3.0 eV) and high LDT for the high-power laser system, and iv) good thermal and environmental stability. Clearly, among these required properties, some of them are intrinsically conflicting, e.g., large SHG response and wide bandgap. In order to reconcile the conflicts, an effective way is to combine multiple types of anions in the structures, for example, to introduce highly electronegative O 2and X -(X = F, Cl, Br) anions to widen bandgaps, and more polarizable chalcogenide Q 2-(Q = S, Se) anions to enhance SHG responses. [20][21][22][23][24][25][26][27][28] With this strategy, many interesting mixedanion compounds have been reported, such as Sr