Chase R C, Krieger A S, Underwood J H
Appl Opt. 1982 Dec 15;21(24):4446-52. doi: 10.1364/AO.21.004446.
The focal length of grazing incidence x-ray telescopes, in particular the type-I Wolter (1952), is fixed by the mirror diameter and the angles of grazing incidence on the surfaces. Often this focal length is too short to give adequate plate scale for imaging, the resulting low f/No. also makes it difficult to match a spectrometer to the output of the telescope, and high resolution spectroscopy is therefore impossible. Both these problems can be alleviated through the use of grazing incidence relay optics (GIRO) systems. These are analogous to secondary optical systems such as Barlow lenses used in visible light optics, serving to magnify the primary image and decrease the divergence of the beam. GIROs can be made with one or more elements; we first discuss single-element GIROS which are useful for spectroscopy. For imaging, two-element systems are required; we discuss a variety of different configurations giving analytical equations for the surfaces. The systems have been studied by ray tracing, and results on resolution and overall system collecting area are shown. Finally we show how the results for resolution can be approximated by simple empirical formulas.
掠入射X射线望远镜的焦距,特别是I型沃尔特望远镜(1952年),由镜面直径和表面的掠入射角确定。通常,这个焦距太短,无法提供足够的成像板比例尺,由此产生的低f数也使得难以将光谱仪与望远镜的输出相匹配,因此高分辨率光谱学是不可能的。通过使用掠入射中继光学系统(GIRO),这两个问题都可以得到缓解。这些类似于可见光光学中使用的诸如巴罗透镜之类的二级光学系统,用于放大原始图像并减小光束的发散。GIRO可以由一个或多个元件制成;我们首先讨论对光谱学有用的单元件GIRO。对于成像,则需要二元系统;我们讨论了各种不同的配置,并给出了表面的解析方程。通过光线追迹对这些系统进行了研究,并展示了分辨率和整个系统收集面积的结果。最后,我们展示了如何通过简单的经验公式来近似分辨率的结果。