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通过扫描反应离子束蚀刻制造的大尺寸且偏振无关的二维光栅。

A large-size and polarization-independent two dimensional grating fabricated by scanned reactive-ion-beam etching.

作者信息

Zhang Wei, Li Wenhao, Zhang Tong, Zheng Zhongming, Chi Zhendong, Jiang Yanxiu, Wu Na

机构信息

Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, No. 3888 Dong Nanhu Road, Changchun, Jilin, 130033, China.

出版信息

Nanophotonics. 2022 Sep 29;11(21):4649-4657. doi: 10.1515/nanoph-2022-0371. eCollection 2022 Dec.

DOI:10.1515/nanoph-2022-0371
PMID:39634730
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11501946/
Abstract

Scanned reactive-ion-beam etching method was proposed to transfer two-dimensional mask patterns into quartz substrate, which would produce a larger-size and polarization-independent two-dimensional grating. This method was realized by moving grating substrate in a unidimensional scanning manner and adjusting ion beam density in the vertical scanning direction. Graphite plates between the ion beam source and the substrate were used to correct the beam density. The original Gaussian ion beam density was changed to a uniform distribution to establish a knife-edge shape around the vertical scanning direction. Therefore, a large-area pattern with consistent depth and duty cycle would be engraved into a quartz substrate. A two-dimensional, 1200 groves/mm grating with an 85-mm × 85-mm area was fabricated under scanned reactive-ion-beam etching method and exhibited a 0.197 ( = 632.8 nm) diffraction wave front. At 780 nm, the efficiency nonuniformity was less than 9%, and the average diffraction efficiencies of transverse-magnetic and transverse-electric polarized light were 57.2 and 58.0%, respectively. The large-size two-dimensional grating with uniform diffraction efficiency and polarization independence enabled grating displacement measurement with high resolution, long measurement range, multiple degrees of freedom, and potential miniaturization.

摘要

提出了扫描反应离子束蚀刻方法,将二维掩模图案转移到石英衬底上,这将产生更大尺寸且与偏振无关的二维光栅。该方法通过以一维扫描方式移动光栅衬底并在垂直扫描方向上调整离子束密度来实现。离子束源与衬底之间的石墨板用于校正束密度。将原始的高斯离子束密度改变为均匀分布,以在垂直扫描方向周围建立刀刃形状。因此,具有一致深度和占空比的大面积图案将被刻蚀到石英衬底中。在扫描反应离子束蚀刻方法下制备了面积为85 mm×85 mm的二维、1200线/mm光栅,其衍射波前为0.197(λ = 632.8 nm)。在780 nm波长下,效率不均匀性小于9%,横向磁偏振光和横向电偏振光的平均衍射效率分别为57.2%和58.0%。这种具有均匀衍射效率和偏振无关性的大尺寸二维光栅能够实现高分辨率、长测量范围、多自由度以及潜在小型化的光栅位移测量。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/07997ae841ff/j_nanoph-2022-0371_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/847a0ed755d6/j_nanoph-2022-0371_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/a02729440aa6/j_nanoph-2022-0371_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/022e072d5a1e/j_nanoph-2022-0371_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/61a7b007dc43/j_nanoph-2022-0371_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/db8e5f6d6169/j_nanoph-2022-0371_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/2e7fe1cd1a13/j_nanoph-2022-0371_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/07997ae841ff/j_nanoph-2022-0371_fig_007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/847a0ed755d6/j_nanoph-2022-0371_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/a02729440aa6/j_nanoph-2022-0371_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/022e072d5a1e/j_nanoph-2022-0371_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/61a7b007dc43/j_nanoph-2022-0371_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/db8e5f6d6169/j_nanoph-2022-0371_fig_005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/2e7fe1cd1a13/j_nanoph-2022-0371_fig_006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3c2a/11501946/07997ae841ff/j_nanoph-2022-0371_fig_007.jpg

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