Chirality‐Dependent Second‐Order Nonlinear Optical Effect in 1D Organic–Inorganic Hybrid Perovskite Bulk Single Crystal

Centimeter-Sized Piezoelectric Single Crystal of Chiral Bismuth-Based Hybrid Halide with Superior Electrostrictive Coefficient

The lead-free hybrid perovskite piezoelectrics possess advantages of easy processing, light weight, and low-toxicity over inorganic ceramics. However, the lack of understanding in structure-property relationships hinders exploration of new molecular piezoelectric crystals with excellent performances. Herein, by introducing chiral α-phenylethylammonium (α-PEA⁺ ) cations into bismuth-based hybrid halides, centimeter-sized (R-α-PEA)₄ Bi₂ I₁₀ and (S-α-PEA)₄ Bi₂ I₁₀ single crystals with a superior piezoelectric voltage coefficient g₂₂ of 309 mV m N^-1 , are obtained. Structural rigidity in crystals leads to a remarkable electrostrictive coefficient Q₂₂ of 25.8 m⁴ C^-2 , nearly 20 times higher than that of poly(vinylidene fluoride) (PVDF), which is beneficial to improve piezoelectricity with the synergistic effect of chirality. Moreover, the as-grown crystals show outstanding phase stability from 173 K to ≈470 K. This work suggests a design strategy based on rigidity and chirality to exploit novel piezoelectrics among hybrid metal halides.

Chiral Hybrid Copper(I) Halides for High Efficiency Second Harmonic Generation with a Broadband Transparency Window

Chiral hybrid organic-inorganic metal halides (HOMHs) with intrinsic noncentrosymmetry have shown great promise for applications in second-order nonlinear optics (NLO). However, established chiral HOMHs often suffer from their relatively small band gaps, which lead to negative impacts on transparent window and laser-induced damage thresholds (LDT). Here, we have synthesized two chiral HOMHs based on Cu^I halides, namely (R-/S-MBA)CuBr₂ , which feature well-balanced NLO performances with a highly efficient SHG response, outstanding optical transparency, and high LDT. The effective second-order NLO coefficient of (R-MBA)CuBr₂ has been determined to be ≈24.7 pm V^-1 , which is two orders of magnitude higher than that of their Cu^II counterparts. This work shows the promising potential of Cu^I -based chiral HOMHs for nonlinear photonic applications in wide wavelength regions.