--> component of incident light is high, the regular reflection component is removed in apparatus (Figs. 10 and 11) by means of a beam trap BT which receives light from the specimen 21 via an angled mirror M5.;Other apparatus can measure either transmission or reflection spectral absorption characteristics in a microsized region (Figs. 12 and 13) and including Cassegrain reflection optical systems disposed confocally and having a pin-hole P at the confocal point, from which the scattered light extracted passes to a detector 2.;Modifications of the apparatus allow a microscopic absorption distribution in an opaque specimen to be measured, by changing the relation between the specimen and the beam of directional parallel light, so as to apply incident light to a very small point region corresponding to a 0-order difraction component (Figs. 15A to 17).;The spectral absorption characteristics of a specimen are thus measured with high accuracy and simply and without picking up extraneous scattered light, and the invention is especially useful for examination of specimens of animal tissue."/> Method and apparatus for measuring the spectral absorption in opaque material and method and apparatus for measuring a distribution of microscopic absorption
首页> 外国专利> Method and apparatus for measuring the spectral absorption in opaque material and method and apparatus for measuring a distribution of microscopic absorption

Method and apparatus for measuring the spectral absorption in opaque material and method and apparatus for measuring a distribution of microscopic absorption

机译:测量不透明材料中光谱吸收的方法和装置以及测量微观吸收分布的方法和装置

摘要

For measuring spectral absorption characteristics of an opaque specimen, apparatus of Fig. 4 comprises a variable wavelength laser which can continuously emit monochromatic light over a wide spectral range, a beam converter 11 positioned to convert light from the laser into parallel rays, a beam splitter BS positioned to produce from the beam (i) rectilinear light which strikes a specimen 20 which transmits light, e.g. a dilute suspension or translucent biological specimen, which scatters the light, the forward component of which is combined with the incident light by a half-mirror HM, and (ii) reflected light which passes through a shifter AO where its frequency is slightly changed before being recombined with the forward scattered light in a detector 2 which can be a highly directional detecting system or a heterodyne system, which are further described (Figs. 1 to 3).;For measurement of absorption of a specimen within a scattering medium, the final light path is modified by altering the position of the half-mirror (HM) and of the specimen 21, which is placed behind a sample of the medium NZ, so that the light passing through the medium is reflected by the specimen and again through the medium and then combines with the forward scattered light at the half-mirror and passed to the detector.;Several other arrangements of the components of the apparatus are shown, for measuring various types of specimen which absorb or scatter light, including some which use a Michelson light-receiving system for a reflecting specimen, or a highly directional optical system.;For measuring spectral absorption characteristics of a reflecting specimen when the intensity of the reflection component of incident light is high, the regular reflection component is removed in apparatus (Figs. 10 and 11) by means of a beam trap BT which receives light from the specimen 21 via an angled mirror M5.;Other apparatus can measure either transmission or reflection spectral absorption characteristics in a microsized region (Figs. 12 and 13) and including Cassegrain reflection optical systems disposed confocally and having a pin-hole P at the confocal point, from which the scattered light extracted passes to a detector 2.;Modifications of the apparatus allow a microscopic absorption distribution in an opaque specimen to be measured, by changing the relation between the specimen and the beam of directional parallel light, so as to apply incident light to a very small point region corresponding to a 0-order difraction component (Figs. 15A to 17).;The spectral absorption characteristics of a specimen are thus measured with high accuracy and simply and without picking up extraneous scattered light, and the invention is especially useful for examination of specimens of animal tissue.
机译:为了测量不透明样品的光谱吸收特性,图4的设备包括能够在宽光谱范围内连续发射单色光的可变波长激光器,定位成将来自激光器的光转换成平行光线的光束转换器11,分束器。 BS被定位成从光束(i)产生直线光,该直线光入射到透射光的样本20上,例如稀悬浮液或半透明生物样本,它会散射光,其前向分量通过半反射镜HM与入射光结合,并且(ii)反射光通过移位器AO,在此之前其频率略有变化在检测器2中与正向散射光重新组合,该检测器2可以是高度定向的检测系统或外差系统,将对其进行进一步描述(图1-3)。通过改变半反射镜(HM)和样品21的位置来修改最终的光路,该样品放置在介质NZ样品的后面,从而使穿过介质的光被样品反射,然后再次穿过介质,然后与半反射镜上的前向散射光合并,然后传递到检测器。;显示了该设备组件的其他几种布置,用于测量各种类型的标本吸收或散射光的组件,包括一些将迈克尔逊光接收系统用于反射样本或高度定向的光学系统的组件;当反射强度<!-EPO时,用于测量反射样本的光谱吸收特性->入射光的分量很高,在设备中去除了正反射分量(图5和6)。在图10和11中示出)是通过光束捕获器BT,该光束捕获器经由成角度的反射镜M5接收来自样本21的光。其他设备可以测量在微尺寸区域(图12和13)中的透射或反射光谱吸收特性,包括卡塞格林共聚焦设置的反射光学系统,在共聚焦点有针孔P,提取的散射光从针孔P传到检测器2;通过修改仪器的变型,可以测量不透明样品中的微观吸收分布样本与定向平行光束之间的关系,以便将入射光施加到与0阶衍射分量相对应的非常小的点区域(图15A至17)。因此样本的光谱吸收特性为本发明以高精度且简单且无需拾取外部散射光的方式进行测量,并且本发明特别用于检查动物组织的样本。

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