首页> 外文期刊>Journal of the Optical Society of America, A. Optics, image science, and vision >Angular spectrum representation of fields diffracted by spherical objects: physical properties and implementations of image field models
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Angular spectrum representation of fields diffracted by spherical objects: physical properties and implementations of image field models

机译:球形物体衍射场的角频谱表示:物理性质和图像场模型的实现

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The modal expansion of the field diffracted by a spherical object is transformed to an angular spectrum representation. Outside the object the angular spectrum representation yields the same diffracted field as that from the modal expansion. By neglecting the inhomogeneous plane waves in this representation, we also obtain the virtual, or backpropagated, fields for planes within or behind the object. These virtual fields are the fields that, to an external observer, appear to exist in free space within or behind the object. Thus these virtual fields are different from the actual fields existing in these regions. The image field model is obtained by including aperture limitations to the angular spectrum representation. These image fields could have been obtained by the more cumbersome approach of first computing the field in the entrance pupil of the imaging system by using the modal expansion and then propagating it back to a plane within or behind the object. The physical properties of images of the center plane of spheres are derived for the scalar case. The conditions for representing a sphere with an equivalent thin-object model are derived along with the criteria for directly representing this thin-object model by the modal coefficients. The usefulness of the image field model for numerical field calculations is illustrated by several examples. Diffraction effects that are present only in imaging situations are presented along with field calculations in the Fresnel region, where both the image field model and the modal expansion yield the same results.#1998 Optical Society of America [S0740-3232(98)00503-1] OCIS codes: 050.1940, 050.1970.
机译:由球形物体衍射的场的模态展开被转换为角谱表示。在物体外部,角谱表示产生的模场与模态扩展产生的衍射场相同。通过忽略此表示中的不均匀平面波,我们还获得了对象内部或后面的平面的虚拟或反向传播的场。对于外部观察者而言,这些虚拟字段是看起来似乎存在于对象内部或对象之后的自由空间中的字段。因此,这些虚拟字段与这些区域中存在的实际字段不同。通过将孔径限制包括在角谱表示中来获得像场模型。通过使用模态展开首先计算成像系统的入射光瞳中的场,然后再将其传播回对象内部或后面的平面,可以通过更麻烦的方法获得这些图像场。对于标量情况,得出球的中心平面的图像的物理属性。推导了用等效的薄对象模型表示球体的条件以及通过模态系数直接表示该薄对象模型的标准。几个示例说明了图像场模型对数值场计算的有用性。仅在成像情况下出现的衍射效应与菲涅耳区域中的场计算一起出现,在该区域中,像场模型和模态展开都产生相同的结果。#1998美国光学学会[S0740-3232(98)00503- 1] OCIS代码:050.1940,050.1970。

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