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Properties of the extreme ultraviolet emission from germanium and gallium plasmas

机译:锗和镓等离子体的极紫外发射特性

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摘要

We report on the usefulness of germanium (Ge) and gallium (Ga) plasmas as potential extreme ultraviolet (EUV) sources at both 6.x and 13.5 nm, wavelengths of interest for lithography and metrology applications. Spectra from plasmas produced using neodymium-doped yttrium-aluminum-garnet (Nd:YAG) lasers with pulse durations of 170 ps and 7 ns [full width at half-maximum] and a compact electron beam ion trap have been used to determine the charge states responsible while theoretical calculations using atomic structure Cowan and HULLAC codes enabled the identification of structure in the Ge spectrum arising from strong transitions of the type 3d - 4p and 3d - 4f. Transitions of the type 3d - 4f in Ge~(10+) and Ga~(11+) were found to lie in the 6.x nm region, while 3p - 3d transitions from a range of stages in both elements contribute in the 13.5 nm region. We also studied the emission spectra of galinstan plasmas, and the results imply that galinstan might provide a promising candidate for EUV applications that exploit the progress in the development of multilayer mirrors for operation at 6.x nm.
机译:我们报告了锗(Ge)和镓(Ga)等离子体作为潜在的极紫外(EUV)源(在6.x和13.5 nm处)的有用性,这是光刻和计量学应用所关注的波长。使用掺钕钇铝石榴石(Nd:YAG)激光器产生的等离子体光谱,其脉冲持续时间为170 ps和7 ns [半最大全宽],并且使用紧凑的电子束离子阱来确定电荷在使用原子结构Cowan和HULLAC代码进行理论计算的同时,这些状态是负责任的,从而可以识别3d-4p和3d-4f型强跃迁引起的Ge光谱中的结构。发现Ge〜(10+)和Ga〜(11+)中3d-4f型跃迁位于6.x nm区域,而这两个元素中一系列阶段的3p-3d跃迁贡献了13.5。纳米区域。我们还研究了加林斯坦等离子体的发射光谱,结果表明加林斯坦可能为EUV应用提供了有前途的候选者,这些应用利用了多层镜在6.x nm下的开发进展。

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  • 来源
    《Journal of Applied Physics》 |2015年第7期|073302.1-073302.8|共8页
  • 作者单位

    School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China;

    Department of Electrical and Electronic Engineering, Faculty of Engineering, Utsunomiya University, Yoto 7-1-2, Utsunomiya, Tochigi 321-8585, Japan;

    Department of Electrical and Electronic Engineering, Faculty of Engineering, Utsunomiya University, Yoto 7-1-2, Utsunomiya, Tochigi 321-8585, Japan;

    Department of Electrical and Electronic Engineering, Faculty of Engineering, Utsunomiya University, Yoto 7-1-2, Utsunomiya, Tochigi 321-8585, Japan;

    Department of Electrical and Electronic Engineering, Faculty of Engineering, Utsunomiya University, Yoto 7-1-2, Utsunomiya, Tochigi 321-8585, Japan,Center for Optical Research and Education (CORE), Utsunomiya University, Yoto 7-1-2, Utsunomiya, Tochigi 321-8585, Japan;

    Graduate School of Science and Engineering for Research, University of Toyama, Toyama, Toyama 930-8555, Japan;

    Department of Electrical Engineering, Nagaoka University of Technology, Kami-tomiokamachi 1603-1, Nagaoka, Niigata 940-2188, Japan;

    Institute of Applied Physics, University of Tsukuba, Tsukuba, Ibaraki 305-8573, Japan;

    National Institute for Fusion Science (NIFS), Toki, Gifu 509-5292, Japan;

    National Institute for Fusion Science (NIFS), Toki, Gifu 509-5292, Japan;

    National Institute for Fusion Science (NIFS), Toki, Gifu 509-5292, Japan,Department of Fusion Science, SOKENDAI (The Graduate University of Advanced Studies), Toki, Gifu 509-5292, Japan;

    National Institute for Fusion Science (NIFS), Toki, Gifu 509-5292, Japan,Department of Fusion Science, SOKENDAI (The Graduate University of Advanced Studies), Toki, Gifu 509-5292, Japan;

    School of Physics, University College Dublin, Belfield, Dublin 4, Ireland;

    School of Physics, University College Dublin, Belfield, Dublin 4, Ireland;

    School of Physics, University College Dublin, Belfield, Dublin 4, Ireland;

    School of Nuclear Science and Technology, Lanzhou University, Lanzhou 730000, China;

    School of Physics, University College Dublin, Belfield, Dublin 4, Ireland;

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