双折射
超极化率
极化率
卤化物
各向异性
材料科学
卤素
结晶学
非线性光学
紫外线
光学材料
光学各向异性
非线性光学
光电子学
二次谐波产生
透明度(行为)
光学
化学物理
工作(物理)
极化(电化学)
晶体结构
光学透明度
Crystal(编程语言)
溴
化学
卤键
密度泛函理论
光化学
合理设计
作者
Jing Lu,Xin Liu,Shuangxiong Zhao,Xuebing Deng,Qundong Fu,Jingyu Guo,Zheng Liu,Li‐Ming Wu,Ling Chen
标识
DOI:10.1002/anie.202524953
摘要
Abstract Birefringent and nonlinear optical (NLO) crystals are crucial for advanced optical applications, yet achieving large birefringence (Δ n ), noncentrosymmetric (NCS) structures, and broad transparency from solar‐blind ultraviolet (SUV) to near‐infrared (NIR) regions remains challenging. Here, we report a 4HPX family of twelve 4‐hydroxypyridinium halides, constructed from 4‐hydroxypyridinium cations [4HPH] + and halide anions [X] − (X = F ( I , II ), Cl ( III , VII , X ), Br ( IV , VIII , XI ), I ( V , VI , IX , XII )). Solution acidity dictates the structural transformations of this family, from centrosymmetric ( I – IX ) to NCS ( X – XII ) phases, where C─O bond lengths act as definitive structural fingerprints. Their optical bandgaps exceed those of all known halogen polyanion‐based crystals due to the large HOMO–LUMO gaps of both [4HPH] + and [X] − and can be systematically tuned via hydrogen‐bond strength. The large hyperpolarizability and polarizability anisotropy of [4HPH] + endow this family with exceptional Δ n and suitable second–harmonic generation (SHG) responses. Notably, II [C 5 H 6 NO] + (HF 2 ) − exhibits the largest Δ n (0.293) within the 4HPX family and among reported water–free SUV crystals. Meanwhile, I – V (0.222–0.293) also outperform commercial birefringent materials. NLO crystals X – XII show SHG responses. This work provides valuable insights into the rational design of next‐generation birefringent and NLO crystals.
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