Abstract Antiperovskites have been studied since the 1980s because of their rich physical and chemical properties, but their linear and second‐order nonlinear optical responses remain largely unknown. Here we report a new polar crystal, Cs 3 Cl(HC 3 N 3 S 3 ) ( I ), which features a quasi‐one‐dimensional antiperovskite structure composed of ClCs 6 polyhedra and A‐site [HC 3 N 3 S 3 ] 2− rings. To our best knowledge, this kind of antiperovskite structure is reported for the first time. Remarkably, I exhibits a very strong nonlinear optical response up to 11.4 times that of the benchmark KH 2 PO 4 and exceptionally large birefringence of 0.52. The first‐principles calculations and structural analyses reveal that [HC 3 N 3 S 3 ] 2− is the “material gene” while the antiperovskite structural feature making it in a favorable arrangement. This work provides a new structural platform for the rational design of integrated optoelectronic materials with linear and second‐order nonlinear optical responses.