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离心沉积双峰钨颗粒在高纵横比硅模板中制备 X 射线吸收光栅。

Fabrication of X-ray absorption gratings by centrifugal deposition of bimodal tungsten particles in high aspect ratio silicon templates.

机构信息

Chair of Biomedical Physics, Department of Physics, School of Natural Sciences, Technical University of Munich, 85748, Garching, Germany.

Munich Institute of Biomedical Engineering, Technical University of Munich, 85748, Garching, Germany.

出版信息

Sci Rep. 2022 Mar 30;12(1):5405. doi: 10.1038/s41598-022-08222-z.

Abstract

Grating-based X-ray imaging employs high aspect ratio absorption gratings to generate contrast induced by attenuating, phase-shifting, and small-angle scattering properties of the imaged object. The fabrication of the absorption gratings remains a crucial challenge of the method on its pathway to clinical applications. We explore a simple and fast centrifugal tungsten particle deposition process into silicon-etched grating templates, which has decisive advantages over conventional methods. For that, we use a bimodal tungsten particle suspension which is introduced into a custom designed grating holder and centrifuged at over 1000×g. Gratings with 45 µm period, 450 µm depth, and 170 mm × 38 mm active area are successfully processed reaching a homogeneous absorber filling. The effective absorbing tungsten thickness in the trenches is 207 µm resulting in a filling ratio of 46.6% compared to a voidless filling. The grating was tested in a Talbot-Lau interferometer designed for clinical X-ray dark-field computed tomography, where visibilities up to 33.6% at 60 kV were achieved.

摘要

基于光栅的 X 射线成像是利用高纵横比的吸收光栅来产生由被成像物体的衰减、相移和小角度散射特性引起的对比度。吸收光栅的制造仍然是该方法向临床应用发展的关键挑战。我们探索了一种简单而快速的离心钨颗粒沉积工艺,将其沉积到硅刻蚀光栅模板中,这相对于传统方法具有决定性的优势。为此,我们使用了一种双峰钨颗粒悬浮液,将其引入到定制设计的光栅支架中,并在超过 1000×g 的离心力下进行离心。成功地处理了具有 45 µm 周期、450 µm 深度和 170 mm×38 mm 有效面积的光栅,实现了均匀的吸收剂填充。在沟槽中的有效吸收钨厚度为 207 µm,与无空隙填充相比,填充率为 46.6%。该光栅在为临床 X 射线暗场计算机断层扫描设计的泰伯-劳干涉仪中进行了测试,在 60 kV 时实现了高达 33.6%的可见度。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3151/8968707/f189361aa192/41598_2022_8222_Fig1_HTML.jpg

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