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Molecular Spectroscopy Workbench: Raman Images from Raman Maps - Spatial Resolution, Mapping Speed, and Multivariate Techniques for Constructing the Image

机译:分子光谱工作台:来自拉曼图的拉曼图像-空间分辨率,映射速度和用于构建图像的多变量技术

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摘要

At the end of my second column, in which I discussed the development of Raman imaging, I said that my next column would discuss the physical determinants of spatial resolution as well as developing methods to improve the mapping speeds. I know that I got sidetracked, but I have not forgotten what I promised, so this column will address these issues. The spatial resolution of any imaging tool is determined by diffraction theory. In an optical microscope, it is assumed that a microscope objective is illuminated uniformly by light and the focal area is described by the Airy disk as (omega)_(o) velence 1.22 (lambda/NA) where NA stands for the numerical aperture of the objective. When the same objective is used to focus a laser beam, the beam profile is not uniform (it is very often Gaussian), nor does it fill the objective aperture. However, the minimum beam spot is described by a similar expression: (omega)_(o) velence K (lambda/NA) with the constant K not very different from 1.
机译:在第二专栏的最后,我讨论了拉曼成像的发展,我说我的下一篇专栏将讨论空间分辨率的物理决定因素以及提高映射速度的开发方法。我知道我已经陷入困境,但是我没有忘记我的承诺,因此本专栏将解决这些问题。任何成像工具的空间分辨率均由衍射理论确定。在光学显微镜中,假设显微镜物镜被光线均匀照射,并且焦距区域由艾里斑描述为ω_(o)velence 1.22(lambda / NA),其中NA代表数值孔径目标。当使用同一物镜聚焦激光束时,光束轮廓不均匀(通常是高斯分布),也不会填充物镜孔径。但是,最小束斑用类似的表达式描述:常数K与(1)相差不大的ω_(o)velence K(λ/ NA)。

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