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High Contrast Imaging with an Arbitrary Aperture: Active Correction of Aperture Discontinuities

机译:任意孔径的高对比度成像:孔径不连续性的主动校正

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We present a new method to achieve high-contrast images using segmented and/or on-axis telescopes. Our approach relies on using two sequential Deformable Mirrors to compensate for the large amplitude excursions in the telescope aperture due to secondary support structures and/or segment gaps. In this configuration the parameter landscape of Deformable Mirror Surfaces that yield high contrast Point Spread Functions is not linear, and non-linear methods are needed to find the true minimum in the optimization topology. We solve the highly non-linear Monge-Ampere equation that is the fundamental equation describing the physics of phase induced amplitude modulation. We determine the optimum configuration for our two sequential Deformable Mirror system and show that high-throughput and high contrast solutions can be achieved using realistic surface deformations that are accessible using existing technologies. We name this process Active Compensation of Aperture Discontinuities (ACAD). We show that for geometries similar to JWST, ACAD can attain at least 10-7 in contrast and an order of magnitude higher for future Extremely Large Telescopes, even when the pupil features a "missing segment". We show that the converging non-linear mappings resulting from our Deformable Mirror shapes actually damp near-field diffraction artifacts in the vicinity of the discontinuities. Thus ACAD actually lowers the chromatic ringing due to diffraction by segment gaps and strut's while not amplifying the diffraction at the aperture edges beyond the Fresnel regime and illustrate the broadband properties of ACAD in the case of the pupil configuration corresponding to the Astrophysics Focused Telescope Assets. Since details about these telescopes are not yet available to the broader astronomical community, our test case is based on a geometry mimicking the actual one, to the best of our knowledge.
机译:我们提出了一种新的方法来实现高对比度图像使用分段和/或轴上望远镜。我们的方法依赖于使用两个连续的可变形反射镜来补偿望远镜孔径中由于次级支撑结构和/或段间隙而产生的大幅度偏移。在这种结构中,产生高对比度点扩展函数的可变形镜面的参数景观不是线性的,需要非线性方法来寻找优化拓扑中的真正最小值。我们求解高度非线性的Monge-Ampere方程,这是描述相位诱导振幅调制物理的基本方程。我们确定了我们的两个连续可变形镜系统的最佳配置,并表明使用现有技术可以访问的真实表面变形可以实现高通量和高对比度解决方案。我们将此过程命名为孔径不连续性的主动补偿(ACAD)。我们表明,对于类似于JWST的几何结构,相比之下,ACAD至少可以达到10-7,对于未来的超大望远镜,甚至在瞳孔具有“缺失部分”的情况下,也可以达到一个数量级。我们表明,由我们的变形镜形状产生的收敛非线性映射实际上抑制了不连续附近的近场衍射伪影。因此,ACAD实际上降低了由于分段间隙和支柱衍射而产生的色光振铃,同时不放大菲涅耳区以外孔径边缘的衍射,并说明了在与天体物理学聚焦望远镜资产对应的瞳孔配置情况下,ACAD的宽带特性。由于更广泛的天文学界尚未获得有关这些望远镜的详细信息,我们的测试案例是基于一个尽我们所知模拟实际望远镜的几何结构。

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