Refractive Phase Plates for Aberration Correction and Wavefront Engineering

Q3 Physics and Astronomy Synchrotron Radiation News Pub Date : 2022-03-04 DOI:10.1080/08940886.2022.2066442
F. Seiboth
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引用次数: 1

Abstract

The short wavelength of X-rays allows in principle the creation of focal spot sizes down to a few nanometers and below. At the same time, this short wavelength and the resulting interaction with matter puts stringent requirements on X-ray optics manufacturing and metrol-ogy. With the transition from third-generation synchrotron sources to diffraction-limited storage rings of the fourth generation, more beamlines will operate at higher spatial coherence. Thus, more instruments will work with smaller focal spot sizes that are increasingly dominated by diffraction effects instead of a demagnification of the X-ray source. Consequently, the requirements of X-ray optics will increase to ensure best beam characteristics via diffraction-limited optics. Simultaneously, X-ray optics manufacturing strives to achieve higher numerical aper-tures to provide ever decreasing beam sizes. On the forefront of this development are highly specialized nanofocusing beamlines with X-ray optics that push focusing toward 10 nm [1–4] and have the ambi-tious goal to reach 1 nm spot sizes [5]. The fabrication of X-ray optics requires the most advanced technologies, such as lithographic nano-fabrication for diffractive [6] and refractive optics [7], surface figuring with atomic precision for total reflection and multilayer mirrors [8], and thin-film technologies for multilayer optics [9]. All of these technologies have been developed over decades and further advances are expected in the future. Minuscule fluctuations or process anisotropies can cause shape deviations of the X-ray optic with a significant impact on focusing performance. Refractive phase plates in combination with a focusing optic are one solution to overcome these technological limitations. While the weak interaction of hard X-rays with matter and the resulting refractive index decrement δ on the order of 10 6 − pose a challenge for the
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用于像差校正和波前工程的折射相位板
x射线的短波长原则上允许产生小至几纳米或更小的焦点光斑。同时,这种短波长以及由此产生的与物质的相互作用对x射线光学制造和计量学提出了严格的要求。随着第三代同步加速器源向第四代衍射限制存储环的过渡,更多的光束线将以更高的空间相干度运行。因此,更多的仪器将与更小的焦斑尺寸一起工作,这些焦斑尺寸越来越多地由衍射效应而不是x射线源的退放大所主导。因此,x射线光学的要求将增加,以确保最佳的光束特性,通过衍射限制光学。同时,x射线光学制造努力实现更高的数值孔径,以提供不断减少的光束尺寸。在这一发展的前沿是高度专业化的纳米聚焦光束线与x射线光学,推动聚焦向10纳米[1 - 4],并有雄心勃勃的目标,以达到1纳米光斑尺寸b[5]。x射线光学元件的制造需要最先进的技术,如衍射光学元件[6]和折射光学元件[7]的光刻纳米加工,全反射和多层反射镜[8]的原子精度表面加工,以及多层光学元件[9]的薄膜技术。所有这些技术已经发展了几十年,预计未来会进一步发展。微小的波动或工艺各向异性会引起x射线光学的形状偏差,对聚焦性能产生重大影响。结合聚焦光学的折射相位板是克服这些技术限制的一种解决方案。而硬x射线与物质的弱相互作用和由此产生的10 6−数量级的折射率衰减δ对光学系统提出了挑战
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来源期刊
Synchrotron Radiation News
Synchrotron Radiation News Physics and Astronomy-Nuclear and High Energy Physics
CiteScore
1.30
自引率
0.00%
发文量
46
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