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1)  concave holographic diffraction grating
平场凹面光栅
1.
A concave holographic diffraction grating is also adopted as a polychromator system.
该系统采用平场凹面光栅为主要器件构成多色仪分光系统,测量全过程由微型计算机控制,实现快速、自动的光源颜色测量。
2)  flat-field holographic concave grating
平场全息凹面光栅
1.
Optimum design of flat-field holographic concave grating for micro-spectrometers;
微型光谱仪平场全息凹面光栅的优化设计
3)  flat field holographic concave grating
平场全息凹面光栅
1.
Design of flat field holographic concave grating;
平场全息凹面光栅的设计
2.
A method which is based on Rowland mount and use ZEMAX software to design flat field holographic concave grating is given in this article.
介绍一种从罗兰圆结构出发,利用ZEMAX光学软件设计平场全息凹面光栅的方法。
3.
A method which use ZEMAX software to design flat field holographic concave grating is given in this article.
介绍利用ZEMAX软件设计平场全息凹面光栅方法。
4)  concave holographic aberration-reduced grating
全息凹面平象场光栅
1.
The spectrophotometer for bioanalyzer was designed with concave holographic aberration-reduced grating as spectroscope and photoelectron diode array as detector.
分光光度计采用全息凹面平象场光栅为分光元件、以硅光电二极管阵列为探测器。
5)  concave grating
凹面光栅
1.
In order to rule the concave grating with a long focal length,a cutter frame with elastic thimble mode was designed and manufactured.
对大曲率半径(即长焦距)金属基底凹面光栅的机械刻划技术做了研究。
2.
Based on the principle of color measure, the mini-spectrometer uses concave grating as its light splitter, fiber as its color picker and liner CCD as its detector.
它根据分光测色的原理,使用 型凹面光栅作为其分光器件,石英光纤做测色探头,线阵CCD为探测器。
3.
This paper presents the principle, structure and aberration-corrected designing of a flat focal field concave grating spectrograph.
介绍了用于 X光能谱测量研究的平焦场凹面光栅光谱仪的原理、结构及象差校正的设计方法。
6)  Planar Waveguide Concave Diffraction Gratings(PW-CDG)
平板波导凹面衍射光栅
1.
In order to design a Planar Waveguide Concave Diffraction Gratings(PW-CDG) accurately,especially a special grating structure,a design method named Modified Recursive Definition of Facet Positions(MRD) was presented.
为了精确设计平板波导凹面衍射光栅,提出了改进的刻槽位置递推计算方法。
补充资料:凹面光栅
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性质:又称罗兰光栅(Rolland grating)。它的作用是使光既衍射又聚焦。因而凹面光栅摄谱仪只需光栅、狭缝及感光板三部分。它可减少吸收现象,只存在光栅面一次反射的光损失,且无色差。可用于远紫外及远红外光谱区域。

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