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原位去除镀铬镜面上的碳污染:用于抑制碳 K 边区域高阶谐波的理想光学元件。

In situ removal of carbon contamination from a chromium-coated mirror: ideal optics to suppress higher-order harmonics in the carbon K-edge region.

作者信息

Toyoshima Akio, Kikuchi Takashi, Tanaka Hirokazu, Mase Kazuhiko, Amemiya Kenta

机构信息

Institute of Materials Structure Science, KEK, 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan.

出版信息

J Synchrotron Radiat. 2015 Nov;22(6):1359-63. doi: 10.1107/S1600577515015040. Epub 2015 Sep 26.

DOI:10.1107/S1600577515015040
PMID:26524299
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4629864/
Abstract

Carbon-free chromium-coated optics are ideal in the carbon K-edge region (280-330 eV) because the reflectivity of first-order light is larger than that of gold-coated optics while the second-order harmonics (560-660 eV) are significantly suppressed by chromium L-edge and oxygen K-edge absorption. Here, chromium-, gold- and nickel-coated mirrors have been adopted in the vacuum ultraviolet and soft X-ray branch beamline BL-13B at the Photon Factory in Tsukuba, Japan. Carbon contamination on the chromium-coated mirror was almost completely removed by exposure to oxygen at a pressure of 8 × 10(-2) Pa for 1 h under irradiation of non-monochromated synchrotron radiation. The pressure in the chamber recovered to the order of 10(-7) Pa within a few hours. The reflectivity of the chromium-coated mirror of the second-order harmonics in the carbon K-edge region (560-660 eV) was found to be a factor of 0.1-0.48 smaller than that of the gold-coated mirror.

摘要

无碳镀铬光学元件在碳 K 边区域(280 - 330 电子伏特)是理想的,因为一阶光的反射率大于镀金光学元件,而二阶谐波(560 - 660 电子伏特)被铬 L 边和氧 K 边吸收显著抑制。在此,日本筑波光子工厂的真空紫外和软 X 射线分支光束线 BL - 13B 采用了镀铬、镀金和镀镍的镜子。在未单色化的同步辐射照射下,将镀铬镜暴露于 8×10⁻² 帕的氧气中 1 小时,几乎完全去除了镀铬镜上的碳污染。几小时内,腔室内的压力恢复到 10⁻⁷ 帕量级。发现在碳 K 边区域(560 - 660 电子伏特),镀铬镜的二阶谐波反射率比镀金镜小 0.1 - 0.48 倍。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/7ad7d24cf66f/s-22-01359-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/6a072961b1c0/s-22-01359-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/538e8693f245/s-22-01359-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/9764386e531f/s-22-01359-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/02f53d200b06/s-22-01359-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/fcbf71fe438a/s-22-01359-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/b891f39ddc25/s-22-01359-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/7ad7d24cf66f/s-22-01359-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/6a072961b1c0/s-22-01359-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/538e8693f245/s-22-01359-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/9764386e531f/s-22-01359-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/02f53d200b06/s-22-01359-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/fcbf71fe438a/s-22-01359-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/b891f39ddc25/s-22-01359-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3bc7/4629864/7ad7d24cf66f/s-22-01359-fig8.jpg

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