Diffraction-Limited Imaging衍射极限成像
If an image is made through a small aperture, there is a point at which the resolution of the image is limited by the aperture diffraction. As a matter of general practice in photographic optics, the use of a smaller aperture (larger f-number) will give greater depth of field and a generally sharper image. But if the aperture is made too small, the effects of the diffraction will be large enough to begin to reduce that sharpness, and you have reached the point of diffraction-limited imaging. 如果通过一个小孔形成图像,会出现一个点,此时图像的分辨率受孔径衍射的限制。在摄影光学中,一般实践是使用较小的孔径(较大的f值)可以获得更大的景深和通常更清晰的图像。但是,如果孔径过小,衍射效应会变得足够显著,开始减少清晰度,此时就达到了衍射受限成像的点。
If you are imaging two points of light, then the smallest separation at which you could discern that there are two could reasonably be used as the limit of resolution of the imaging process. Presuming that diffraction is the determining factor, then the generally accepted criterion for the minimum resolvable detail is the Rayleigh criterion. ![]() 如果你在观察两个光点,那么你能够分辨出这两个点的最小间距可以合理地作为成像过程的分辨率极限。假设定位因素是衍射,那么通常接受的可分辨最小细节的标准是瑞利准则。 This shows the intensity curves for the radial distribution of the diffracted light for different separations. Your eye sees the characteristic bullseye distribution of light as illustrated below. ![]() While perfect imaging of the source would be smaller perfect circles of light, this shows the smearing of the light by diffraction into the bullseye patterns. 虽然理想成像的源会形成更小的光圈,但这展示了光因衍射而被模糊成靶心图案。
这展示了不同分离距离下衍射光的径向分布的强度曲线。你的眼睛会看到如下面所示的光的典型靶心分布。 References: 参考文献: The Cambridge in Colour site has calculations and demonstrations of diffraction spreading at different f-numbers. 剑桥彩色网站提供了不同f数的衍射扩散计算和演示。 |
Index
索引 | ||
|
Go Back
返回 |