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Induced aberrations in optical systems.

机译:光学系统中引起的像差。

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摘要

The total wave aberration of an optical system can be broken down into surface contributions. These surface contributions can be further differentiated into induced and intrinsic components. The intrinsic aberration is the aberration introduced by a given surface, based on a perfect incoming wavefront. The induced component is the additional aberration introduced by the surface as a consequence of monochromatic aberrations of the incoming wavefront. This distinction is made without decomposing the aberration or its components into orders. Because no methods have previously been developed to properly analyze this induced component, there is very little known about its significance. As a result, the behavior of lenses is not well understood beyond third order, and designers must depend upon optimization to find solutions with the necessary overall higher-order correction. The first part of this investigation is concerned with developing appropriate methods for separating the surface contributions to the total wave aberration of an optical system into induced and intrinsic components. These systems are limited to rotationally symmetric optical systems with spherical or aspheric surfaces. Three different methods are developed to describe the induced aberrations. These methods emphasize the aberrations of wavefronts rather than rays; rays are simply used for calculation purposes. The first is a numerical approach that determines the true shapes of the wavefront components, without separating the aberrations into orders. A second numerical method, based on a procedure developed by G. W. Hopkins, determines aberration coefficients to seventh order describing the induced, intrinsic, and complete aberrations. Because of the choice of reference surfaces, the third-order aberrations are entirely intrinsic. Thus, the induced component is described only by fifth- and higher-order coefficients. A third method uses an algebraic approach to calculate the fifth-order induced aberration coefficients in terms of third order coefficients. The second part is an exploration of the nature and significance of the induced component. The various analysis methods are used to explore the behavior of induced aberrations in many basic optical systems.
机译:光学系统的总波像差可以分解为表面贡献。这些表面贡献可以进一步分为诱导成分和固有成分。固有像差是基于理想入射波阵面的给定表面引入的像差。感应分量是由于入射波前的单色像差而由表面引入的附加像差。进行这种区分时不会将像差或其组成分解为顺序。由于以前尚未开发出任何方法来正确分析此诱导成分,因此对其意义的了解很少。结果,除了三阶以外,人们对镜片的性能还没有很好的了解,设计人员必须依靠优化来寻找具有必要的整体高阶校正的解决方案。本研究的第一部分涉及开发适当的方法,以将对光学系统的总波像差的表面贡献分成感应分量和本征分量。这些系统仅限于具有球形或非球形表面的旋转对称光学系统。开发了三种不同的方法来描述引起的像差。这些方法强调波前的像差,而不是射线。射线仅用于计算目的。第一种是一种数值方法,可以确定波前分量的真实形状,而无需将像差分成多个等级。根据G. W. Hopkins开发的一种方法,第二种数值方法将像差系数确定为七阶,描述了像差,固有像差和完整像差。由于选择了参考面,因此三阶像差完全是固有的。因此,感应分量仅由五阶和更高阶系数来描述。第三种方法使用代数方法来根据三阶系数来计算五阶诱导像差系数。第二部分探讨了诱导成分的性质和意义。各种分析方法用于探索许多基本光学系统中的像差行为。

著录项

  • 作者

    Hoffman Jeffrey Mathew.;

  • 作者单位
  • 年度 1993
  • 总页数
  • 原文格式 PDF
  • 正文语种 en
  • 中图分类

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