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Proceedings from the theory of geometric optics,the condition adaxial noncoherent imaging of Fizeau opticalsynthetic aperture imaging system is derived to achieve diffracion limited performance over a finite field of view,and the conclusion is that the angular magnification of the individual telescope must be equal to the linear demagnification factor.

从几何光学理论出发,详细推导了斐索型光学合成孔径成像系统的近轴非相干成像条件,即子望远系统的角放大率等于系统的线性缩放因子。对于焦平面上的像点而言,合成孔径成像系统可等效为一个带有特殊形状孔径光阑的望远系统,这要求该孔径光栏的开口形状和位置分布与合成孔径成像系统各子系统孔径大小和位置分布相一致。

Based on the propagation law of partially coherent light, the spectral changes of Gaussian Schell-model beams passing through an astigmatic aperture lens are studied.

从部分相干光的传输理论出发,研究了高斯-谢尔模型光束通过光阑像散透镜传输轴上的光谱变化规律。

In the laser engineering system,a beam expander and an annular aperture were taken as the equivalent of the Cassegrain telescope system.

在激光工程系统中,把卡塞格林望远系统等效为一个扩束器和环形光阑的组合形式,研究了激光束的光腰半径与卡塞格林望远系统的参数匹配问题。

This spectral change is not only dependent on the chromatic aberration of the lens, but also on the coherence of the partially coherent light.

而部分相干光在经过光阑透镜系统时,在近场和远场光谱都会发生变化。

Based on Collins integral formula and the expansion of the hard aperture function into a finite sum of complex Gaussian functions,the approximate analytical expression of the diffraction field of Gaussian beam by a circular disc is derived,and its characteristics are analyzed by the numerical calculation and numerical simulation.

基于圆孔光阑函数展开为复高斯函数和的方法,用Colins积分公式,导出了高斯光束照射下圆盘衍射的光场近似解析表达式,经计算机数值计算,对高斯光束照射下圆盘衍射的衍射特性进行了详细的分析

The intensity distributing and the contributing range for using the serrated aperture are analyzed based on Fresnel diffraction theory.

应用菲涅耳衍射光强分布理论以及光轴上光强分布理论对波纹光阑在一定条件下的作用范围进行了分析。

Stop Down: To decrease the diameter of the light-admitting orifice of a lens by adjustment of an iris diaphragm.

缩小光圈:镜头的焦距和光圈的有效直径之间的关系。一可调节的彩虹光阑,减少透镜光孔的直径。

Based on the expression of diffractive field distribution of the Gaussian beams restricted by a rectangular aperture and focalized by a lens,the relationship between the width of the rectangular aperture and the spot size of the restricted beam,as well as the relationship between the aperture width and the power in the bucket,was numerically calculated with MATLAB.

为了研究矩形光阑边长与透镜像方焦面处光束光斑尺寸以及光斑内所包含功率的关系,根据高斯光束经矩形光阑和透镜变换后在透镜像方焦面的衍射场分布表达式,采用MATLAB进行数值计算的方法,进行了理论分析。

For example, if your widest field eyepiece has a 40mm diameter field stop and you choose a decreasing increment diameter factor of 2 (which results in a 4x decrease in area size), you'll end up with eyepieces having field stop diameters of approximately 40mm, 20mm and 10mm.

例如,如果你的最广视野的目镜拥有40mm的视场光阑直径并且你选择间隔倍率为2,(导致4倍减少区域面积),你最终选择的这组目镜的视场光阑为40mm,20mm和10mm。

Of course, avoid duplicating focal lengths. For example, if you use a 31mm Nagler (with a 42mm field stop diameter), you would not need a 32mm Plossl (with a 27mm field stop diameter).

当然,也要避免焦距重复,例如你使用一个31mm的Nagler (42mm视场光阑),你不需要一个32mm Plossl (with a 27mm视场光阑)。

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