| 相干反斯托克斯拉曼散射显微镜的成像特性 |
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| 引用本文： | 袁景和,肖繁荣,王桂英,徐至展.相干反斯托克斯拉曼散射显微镜的成像特性[J].中国物理 B,2005,14(5):935-941. |
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| 作者姓名： | 袁景和 肖繁荣 王桂英 徐至展 |
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| 作者单位： | Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China;Institute of Science and technology for Opto-electron information,Yantai University, Yantai 264005, China.;Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China.;Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China.;Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China. |
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| 摘 要： | 对自身不发荧光且不便于荧光标记的化学或生物学样品，集相干反斯托克斯拉曼散射与激光共焦扫描显微镜于一身的相干反斯托克斯拉曼散射显微镜是一种好的选择。因为相干反斯托克斯拉曼散射是一种非线性过程，相干反斯托克斯拉曼散射显微镜的显微成像特性与一般的共焦显微镜非常不同。首先计算了焦点附近相干反斯托克斯拉曼散射激发场的偏振分布，然后，利用格林函数方法，得到了以赫兹偶极子为源的波动方程的精确解，发现对于不同的成像配置和样品形状，像场的相干反斯托克斯拉曼散射场分布非常不同，因此传统的显微镜成像表征方式（如点扩展函数）将不再能描述相干反斯托克斯拉曼散射显微镜的成像特性。
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| 关 键 词： | 显微镜 相干反斯托克斯拉曼散射 赫兹偶极子 格林函数 |
| 收稿时间： | 2004-05-14 |
Imaging properties of coherent anti-Stokes Raman scattering microscope |
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| Yuan Jing-He,Xiao Fan-Rong,Wang Gui-Ying and Xu Zhi-Zhan.Imaging properties of coherent anti-Stokes Raman scattering microscope[J].Chinese Physics B,2005,14(5):935-941. |
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| Authors: | Yuan Jing-He Xiao Fan-Rong Wang Gui-Ying and Xu Zhi-Zhan |
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| Institution: | Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China.; Key Laboratory for High Intensity Optics, the Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China;Institute of Science and technology for Opto-electron information,Yantai University, Yantai 264005, China. |
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| Abstract: | |
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| Keywords: | microscope coherent anti-Stokes Raman scattering Hertzian dipole Green function |
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