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Optimization of the complex coherence function T for diffraction based wave front transformations

机译:基于衍射波前变换的复相干函数T的优化

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Partial coherence is used in a plurality of applications, magnifying microscopic imaging, interferometric measurement, lithographic imaging, CGH based wave front shaping, interference lithography and space-bandwidth-limited wave front reconstruction, just to name a few. In some applications the primary light source is characterized by a limited coherence length and an extended angular spectrum of plane waves, which has to be narrowed, e.g. if an Excimer laser is used. Sometimes the angular spectrum of plane waves of the primary light source has to be increased in order to be practical. There are several possibilities in general, the primary light source can be used directly, the system has to be adapted or the coherence function Γ has to be tailored in order to provide the specific requirements. Almost all embodiments come with little changes of the light sources coherence properties only. For example, to use a spectral bandpass filter or to limit the size of the light source seem to be the standard solution for almost everything. However, more advanced tailoring of the complex valued coherence function Γ leads to an increased image quality, e.g. in interferometers, but is not limited to this, reduces background noise, decouples Fizeau cavities or it enables complete new illumination and imaging system designs, which provide unique features. This aspect will be discussed herein. Furthermore, the propagation of the complex coherence will be taken into account. This is done in order to provide defined conditions in defined planes of imaging devices. In other words, the usage of the Wiener-Khintchin theorem and the van Cittert-Zernike theorem is just a part of the system analysis and system optimization, which has to be done. Although generic approaches are used, discrete light source layouts are strongly related to the discrete optical devices, which make use of them. The specific tailoring of the complex coherence function, which is related to the space-bandwidth-limited reconstruction of wave front segments, which also can be referred to as space-bandwidth-limited CGH reconstruction, will be described in more detail. For this type of real time dynamic imaging two major problems - among several others - have to be solved. One problem is the huge computation power and the other one is the coherent retinal cross talk of adjacent image points, which are reconstructed in the image volume. The disclosed layouts of tailored secondary light sources are based on the Wiener-Khintchin theorem and the van Cittert-Zernike theorem. Both problems, which are mentioned above, can be solved. Tailored complex valued light sources reduce the required computation power by enabling reduced coherent overlay of sub-CGH areas. Furthermore, they reduce the coherent retinal cross talk of dynamic real time space-bandwidth-limited CGH reconstruction, which is used in advanced imaging applications, too. This results in an increased image quality of partial coherent wave field reconstruction based imaging.
机译:部分相干在多种应用中使用,例如放大显微镜成像,干涉测量,光刻成像,基于CGH的波阵面整形,干涉光刻和空间带宽受限的波阵面重建,仅举几例。在一些应用中,主光源的特征在于相干长度有限和平面波的扩展角频谱,该频谱必须变窄,例如,必须减小。如果使用准分子激光器。有时,为了实用,必须增加一次光源的平面波的角谱。通常有几种可能性,可以直接使用主光源,必须调整系统或调整相干函数Γ,以提供特定的要求。几乎所有实施例都仅具有很少的光源相干特性变化。例如,使用光谱带通滤波器或限制光源的大小似乎是几乎所有设备的标准解决方案。然而,对复数值相干函数Γ的更高级剪裁导致图像质量的提高,例如,图像质量的提高。干涉仪中的传感器,但不仅限于此,它可以减少背景噪声,使Fizeau腔分离,或者可以实现全新的照明和成像系统设计,从而提供独特的功能。这方面将在本文中讨论。此外,将考虑复杂相干的传播。这样做是为了在成像设备的限定平面中提供限定条件。换句话说,Wiener-Khintchin定理和van Cittert-Zernike定理的使用只是系统分析和系统优化的一部分,必须完成。尽管使用了通用方法,但离散光源布局与使用它们的离散光学设备密切相关。将更详细地描述与波前段的空间带宽受限的重建有关的复杂相干函数的特定剪裁,也可以将其称为空间带宽受限的CGH重建。对于这种类型的实时动态成像,必须解决两个主要问题-几个其他问题。一个问题是巨大的计算能力,另一个问题是在图像体积中重建的相邻图像点的相干视网膜串扰。量身定制的辅助光源的公开布局基于维纳-欣钦定理和范·奇特-泽尼克定理。上面提到的两个问题都可以解决。量身定制的复值光源通过减少子CGH区域的相干叠加,降低了所需的计算能力。此外,它们还减少了动态实时空间带宽受限的CGH重建的相干视网膜串扰,这也被用于高级成像应用中。这导致基于部分相干波场重构的成像的图像质量提高。

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