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1. 中国科学院激发态物理开放研究实验室, 中国科学院长春光学精密机械与物理研究所, 吉林, 长春, 130021
2. 深圳赛格集团, 广州深圳, 518028
收稿日期:2001-08-08,
修回日期:2001-07-20,
纸质出版日期:2001-11-30
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马少杰, 廖燕平, 邓文渊, 张红坡, 李玉善, 刘弦. 质子交换LiTaO<sub>3</sub>光波导特性及晶格常数变化[J]. 发光学报, 2001,22(4): 417-421
MA Shao-jie, LIAO Yan-ping, DENG Wen-yuan, ZHANG Hong-po, LI Yu-shan, LIU Xian. Lattice Constant Change and Characteristic of Proton-exchanged LiTaO<sub>3</sub> Waveguide Layer[J]. Chinese Journal of Luminescence, 2001,22(4): 417-421
马少杰, 廖燕平, 邓文渊, 张红坡, 李玉善, 刘弦. 质子交换LiTaO<sub>3</sub>光波导特性及晶格常数变化[J]. 发光学报, 2001,22(4): 417-421 DOI:
MA Shao-jie, LIAO Yan-ping, DENG Wen-yuan, ZHANG Hong-po, LI Yu-shan, LIU Xian. Lattice Constant Change and Characteristic of Proton-exchanged LiTaO<sub>3</sub> Waveguide Layer[J]. Chinese Journal of Luminescence, 2001,22(4): 417-421 DOI:
采用气相质子交换方法
在Z-切LiTaO
3
晶体表面制备平面光滑波导层.样品制备采用245℃苯甲酸气体
在LiTaO
3
晶体在-C和+C表面交换8~20小时.质子交换层在LiTaO
3
表面形成
并用棱镜耦合测量波导样品.然后在HF:HNO
3
酸中用化学方法腐蚀波导层
并用电子显微镜观测光波导层与衬底界面的形貌.用X射线衍射法
测量LiTaO
3
质子交换光波层的晶格常数变化.用双晶X射线测量质子交换(PE)和退火质子交换(APE)波导层晶格常数的变化.样品的X射线衍射曲线表明
PE和APE波导晶格常数的变化不同.实验中
还测量了有无极畴反转LiTaO
3
晶格常数的改变.
Using benzoic acid gas
we fabricated proton-exchanged planar waveguide layer in
z
-cut LiTaO
3
surface.'The preparations of the samples are as follows:First
waveguides layer was fabricated in the-c and+c face of LiTaO
3
substrates in benzoic acid gas at 245℃ for 8~20h.The proton-exchanged layers were formed in the face of LiTaO
3
.Then the samples of waveguide were measured by prism coupling method.After that
waveguide layer in the surface of LiTaO
3
was etched in HF:HNO
3
acid and then measusured by use of electronic microscope.Using chemical etch method
we observed waveguide layer and the shape and form of inner interface of waveguides.Using X-ray diffraction method
we measured the change of lattice constant of proton-exchanged waveguide.The double crystal X-ray diffraction rocking curves analysis was used to determine the lattice constants of the proton-exchanged(PE) and annealed proton-exchanged(APE) 1ayer.The X-ray diffrac-tion rocking curves of the sample show that the rate of the lattice constant changes of the PE and APE were different.The lattice constants of the LiTaO
3
substrates without and with the domain-inverted slab struc-ture were measured.The experimentaI results were reported and discussed in detail.
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