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碱金属阳离子对[B3O7]型非线性光学晶体结晶习性的影响
引用本文:王迪,张德明,张季,王小飞,张庆礼,万松明,殷绍唐.碱金属阳离子对[B3O7]型非线性光学晶体结晶习性的影响[J].物理学报,2013,62(15):154203-154203.
作者姓名:王迪  张德明  张季  王小飞  张庆礼  万松明  殷绍唐
作者单位:中国科学院安徽光学精密机械研究所, 安徽省光子器件与材料重点实验室, 合肥 230031
摘    要:本文利用高温拉曼光谱技术和从头计算的方法, 研究了LiB3O5和CsB3O5晶体高温熔融体的结构, 分析了碱金属阳离子对熔体结构的影响, 以及熔体结构的差异与LiB3O5和CsB3O5晶体结晶习性的联系. 结果表明: LiB3O5和CsB3O5晶体高温熔融体中的结构基团 主要为B3Ø7和B3Ø6两种不同类型的硼氧六元环; 环内BØ4 四面体的数量影响了六元环呼吸振动峰的拉曼频率, 随BØ4四面体数量的增加六元环呼吸振动峰向低频移动; LiB3O5晶体高温熔融体中, BØ4四面体含量相对较多; 然而, 离子半径相对较大的Cs+离子却阻碍了熔体中BØ4四面体的形成, 造成CsB3O5晶体高温熔融体中BØ4/BØ3比值的降低. 结合LiB3O5和CsB3O5晶体生长动力学过程的分析 (Wang D, Wan S M et al. 2011 Cryst. Eng. Comm. 13 5239), 阳离子的不同导致高温熔体中BØ4四面体数量的差异, 被认为是影响LiB3O5和CsB3O5晶体结晶习性的重要因素, 有效降低高温熔体中BØ4四面体的数量, 将是实现LiB3O5晶体生长的关键条件. 关键词: 硼酸盐晶体 熔体结构 拉曼光谱 结晶习性

关 键 词:硼酸盐晶体  熔体结构  拉曼光谱  结晶习性
收稿时间:2012-12-23

The influence of alkali metal ions on crystallization habits of nonlinear optical crystal containing [B3O7] groups
Wang Di,Zhang De-Ming,Zhang Ji,Wang Xiao-Fei,Zhang Qin-Li,Wan Song-Ming,Yin Shao-Tang.The influence of alkali metal ions on crystallization habits of nonlinear optical crystal containing [B3O7] groups[J].Acta Physica Sinica,2013,62(15):154203-154203.
Authors:Wang Di  Zhang De-Ming  Zhang Ji  Wang Xiao-Fei  Zhang Qin-Li  Wan Song-Ming  Yin Shao-Tang
Abstract:LiB3O5 and CsB3O5 are two excellent nonlinear optical borate crystals containing B3O7] groups. With a difference of aikali metal ions in structure, LiB3O5 and CsB3O5 exhibit different crystallization habits. The former is an incongruent compound, which cannot crystallize from its melt; however, the latter is a congruent compound obtained by cooling its melt directly. In this work, using Raman spectroscopy and ab initio calculation, the structures of LiB3O5 and CsB3O5 melts have been investigated, and then the influence of alkali metal ions on melt structures is discussed, finally, the relationship between crystallization habits of LiB3O5 and CsB3O5 and their melts is proposed. Results suggest that the boron oxide species of LiB3O5 and CsB3O5 melts are in the form of six-membered rings B3Ø7 and B3Ø6 (Ø represents a bridging oxygen); Raman frequency of the symmetric breathing vibration of six-membered rings shifts to low frequency with the addition of BØ4 tetrahedrons in rings; the relatively large amount of BØ4 tetrahedrons is found in LiB3O5 melts. However, Cs+ ions with larger ion radius hinder the formation of BØ4 tetrahedrons, and then reduc, the BØ4/BØ3 ratio of the melt. Finally, considering the growth mechanism of LiB3O5 and CsB3O5 crystals (Wang D, Wan S M et al. 2011 Cryst. Eng. Comm. 13 5239), we propose that the amount of BØ4 tetrahedrons in melts, which is influenced by aikali metal ions, determines LiB3O5 and CsB3O5 crystallization habits, therefore, and suggest the reduction of BØ4 tetrahedrons in melts is an effective way to crystallize LiB3O5.
Keywords: borate crystals melt structures Raman spectroscopy crystallization habit
Keywords:borate crystals  melt structures  Raman spectroscopy  crystallization habit
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