“…Recently, synthetic chemists have been working on the discovery of NCS functional materials through molecular structure design, such as the rational combination of different local asymmetric units to generate macroscopic asymmetry. − The effective asymmetric units can be divided into the following categories: (1) π-conjugated planar groups such as CO 3 , BO 3 , NO 3 , etc., − (2) tetrahedral units lacking centers such as BO 4 , PO 4 , and SiO 4 tetrahedron, − (3) d 10 cation (Zn 2+ , Cd 2+ , Hg 2+ ) centered polyhedra with highly polar displacement, , (4) Jahn–Teller distortion units containing nonbonded electron pair cations Pb 2+ , Sb 3+ , and Bi 3+ and d 0 cations V 5+ , Mo 6+ , W 6+ , etc. − Among them, the BO 3 unit has been proven to be a classical excellent NLO active group on the basis of the anionic group theory, and several excellent deep or short UV NLO borates displaying a strong NLO coefficient and proper birefringence like β-BaB 2 O 4 (β-BBO), KBe 2 BO 3 F 2 (KBBF), and Pb 2 BO 3 X (X = Cl, Br, I) − have been reported. HCOO – is also an excellent planar candidate for constructing NLO materials, which have been neglected for a long time, and very recently, formates have been proven to be splendid birefringent candidates. , As we know, the combination of two or more planar π-conjugated functional groups into one compound will enhance the optical properties because the synergetic effect of these planar NLO active units is conducive for the superposition of their microscopic linear and nonlinear properties. , However, it should be noted that the introduction of asymmetric units to produce a NCS material is necessary, but there are some other factors that influence the overall centricity, such as the size of the diverse template cations and anions, hydrogen-bonding effect, and the arrangement of the functional groups. , For example, alkali metal cations with discrepant cation sizes often adjust the structures with different symmetries. − …”