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Na₄La₂(CO₃)₅ 和 CsNa₅Ca₅(CO₃)₈:两种新型碳酸盐作为紫外非线性光学材料

Na₄La₂(CO₃)₅ and CsNa₅Ca₅(CO₃)₈: two new carbonates as UV nonlinear optical materials.

作者信息

Luo Min, Wang GenXiang, Lin Chensheng, Ye Ning, Zhou Yuqiao, Cheng Wendan

机构信息

Key Laboratory of Optoelectronic Materials Chemistry and Physics, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences , Fuzhou, Fujian 350002, P. R. China.

出版信息

Inorg Chem. 2014 Aug 4;53(15):8098-104. doi: 10.1021/ic501089f. Epub 2014 Jul 16.

Abstract

Two nonlinear optical crystal carbonates (Na4La2(CO3)5 and CsNa5Ca5(CO3)8 were successfully synthesized by hydrothermal method, and both of them crystallized in the same noncentrosymmetric hexagonal space group P63mc (No. 186). The structure of Na4La2(CO3)5 consists of a three-dimensional network made up of [CO3] triangles as well as irregular [Na(0.67)La(0.33)O10] and [NaO8] polyhedra. The structure of CsNa5Ca5(CO3)8 can be described as the standing-on-edge [CO3] groups connect the adjacent infinite [CaCO3]∞ layers in the ab plane to construct a framework with four types of channels running parallel to [010]. The Na, Cs, and [Na(0.67)Ca(0.33)] atoms reside in these channels. The measurement of second harmonic generation (SHG) by the method adapted from Kurtz and Perry indicated that Na4La2(CO3)5 and CsNa5Ca5(CO3)8 were phase-matchable in the visible region and exhibited SHG responses of approximately 3 and 1 × KH2PO4 (KDP). Meanwhile, they exhibited wide transparent region with short UV cutoff edge at about 235 and 210 nm, respectively, suggesting that these crystals as NLO materials may have potential applications in the UV region.

摘要

通过水热法成功合成了两种非线性光学晶体碳酸盐(Na4La2(CO3)5 和 CsNa5Ca5(CO3)8),它们都结晶于相同的非中心对称六方空间群 P63mc(编号 186)。Na4La2(CO3)5 的结构由一个三维网络组成,该网络由 [CO3] 三角形以及不规则的 [Na(0.67)La(0.33)O10] 和 [NaO8] 多面体构成。CsNa5Ca5(CO3)8 的结构可描述为边缘站立的 [CO3] 基团在 ab 平面连接相邻的无限 [CaCO3]∞ 层,构建了一个具有四种平行于 [010] 的通道类型的框架。Na、Cs 和 [Na(0.67)Ca(0.33)] 原子位于这些通道中。采用改编自 Kurtz 和 Perry 的方法对二次谐波产生(SHG)进行测量表明,Na4La2(CO3)5 和 CsNa5Ca5(CO3)8 在可见光区域是相位匹配的,并且分别表现出约 3 和 1×KH2PO4(KDP)的 SHG 响应。同时,它们分别在约 235 和 210 nm 处具有短紫外截止边缘的宽透明区域,这表明这些晶体作为非线性光学材料在紫外区域可能具有潜在应用。

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