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锂驱动二维中心对称到三维非中心对称转变产生的非线性光学硫化物LiMGaS(M = Rb/Ba,Cs/Ba)

Nonlinear Optical Sulfides LiMGa S (M = Rb/Ba, Cs/Ba) Created by Li Driven 2D Centrosymmetric to 3D Noncentrosymmetric Transformation.

作者信息

Zhang Ming-Shu, Liu Bin-Wen, Jiang Xiao-Ming, Guo Guo-Cong

机构信息

State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Fuzhou, Fujian, 350002, P. R. China.

University of Chinese Academy of Sciences, Beijing, 100049, P. R. China.

出版信息

Small. 2023 Sep;19(37):e2302088. doi: 10.1002/smll.202302088. Epub 2023 May 5.

Abstract

Cations that can regulate the configuration of anion group are greatly important but regularly unheeded. Herein, the structural transformation from 2D CS to 3D noncentrosymmetric (NCS, which is the prerequisite for second-order NLO effect) is rationally designed to newly afford two sulfides LiMGa S (M = Rb/Ba, 1; Cs/Ba, 2) by introducing the smallest alkali metal Li cation into the interlamination of 2D centrosymmetric (CS) RbGaS . The unusual frameworks of 1 and 2 are constructed from C -type [Ga S ] supertetrahedrons in a highly parallel arrangement. 1 and 2 display distinguished NLO performances, including strong phase-matchable second-harmonic generation (SHG) intensities (0.8 and 0.9 × AgGaS at 1910 nm), wide optical band gaps (3.24 and 3.32 eV), and low coefficient of thermal expansion for favorable laser-induced damage thresholds (LIDTs, 4.7, and 7.6 × AgGaS at 1064 nm), which fulfill the criteria of superior NLO candidates (SHG intensity >0.5 × AGS and band gap >3.0 eV). Remarkably, 1 and 2 melt congruently at 873.8 and 870.5 °C, respectively, which endows them with the potential of growing bulk crystals by the Bridgeman-Stockbarge method. This investigated system provides a new avenue for the structural evolution from layered CS to 3D NCS of NLO materials.

摘要

能够调节阴离子基团构型的阳离子极为重要,但却常常被忽视。在此,通过将最小的碱金属锂离子引入二维中心对称(CS)的RbGaS层间,合理设计了从二维CS到三维非中心对称(NCS,这是二阶非线性光学效应的前提条件)的结构转变,从而新合成了两种硫化物LiMGaS(M = Rb/Ba,1;Cs/Ba,2)。1和2的独特框架由高度平行排列的C型[GaS]超四面体构成。1和2展现出卓越的非线性光学性能,包括强的可相位匹配的二次谐波产生(SHG)强度(在1910 nm处分别为0.8和0.9×AgGaS)、宽的光学带隙(3.24和3.32 eV)以及低的热膨胀系数,以获得良好的激光损伤阈值(在1064 nm处分别为4.7和7.6×AgGaS),满足了优异非线性光学候选材料的标准(SHG强度>0.5×AGS且带隙>3.0 eV)。值得注意的是,1和2分别在873.8和870.5°C下完全一致熔化,这赋予了它们通过布里奇曼 - 斯托克巴奇方法生长块状晶体的潜力。该研究体系为非线性光学材料从层状CS到三维NCS的结构演变提供了一条新途径。

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