A Continuous Emission Source Covering the 50 to 300 Angstrom Band

S. Bowyer
{"title":"A Continuous Emission Source Covering the 50 to 300 Angstrom Band","authors":"S. Bowyer","doi":"10.1364/sxray.1992.mc4","DOIUrl":null,"url":null,"abstract":"Because of the growing importance of extreme ultraviolet radiation, there is considerable interest in high intensity laboratory sources for this spectral range. A variety of sources have been proposed for these wavelengths, and many of these are described in the classic book of Samson (1967). Most of these sources have substantial limitations, especially those that are intended for use below 1200 Å. We (Paresce et al. 1971) and others have developed continuous discharge sources which are stable and maintenance-free and which provide a large number of intense lines at wavelengths down to ~300 Å. Soft X-ray sources of the type developed and refined by Henke (1975) are capable of producing substantial amounts of soft X-ray radiation. However, these sources have severe limitations for use at wavelengths longer than ~50 Å. For example, much of the radiation produced is continuum radiation with rather low flux at any specific line. In addition, the flux is peaked at shorter wavelengths. When dispersed by a grazing incidence monochromator, wavelengths at first order and many higher orders emerge from the exit slit, rather than a true monochromatic flux which is usually desired. Essentially the only sources available that can provide reasonable flux levels at wavelengths between 50 and 300 Å are capacitive discharge sources with attendant problems of severe electromagnetic interference, and plasma discharge sources.","PeriodicalId":409291,"journal":{"name":"Soft-X-Ray Projection Lithography","volume":"22 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Soft-X-Ray Projection Lithography","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/sxray.1992.mc4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Because of the growing importance of extreme ultraviolet radiation, there is considerable interest in high intensity laboratory sources for this spectral range. A variety of sources have been proposed for these wavelengths, and many of these are described in the classic book of Samson (1967). Most of these sources have substantial limitations, especially those that are intended for use below 1200 Å. We (Paresce et al. 1971) and others have developed continuous discharge sources which are stable and maintenance-free and which provide a large number of intense lines at wavelengths down to ~300 Å. Soft X-ray sources of the type developed and refined by Henke (1975) are capable of producing substantial amounts of soft X-ray radiation. However, these sources have severe limitations for use at wavelengths longer than ~50 Å. For example, much of the radiation produced is continuum radiation with rather low flux at any specific line. In addition, the flux is peaked at shorter wavelengths. When dispersed by a grazing incidence monochromator, wavelengths at first order and many higher orders emerge from the exit slit, rather than a true monochromatic flux which is usually desired. Essentially the only sources available that can provide reasonable flux levels at wavelengths between 50 and 300 Å are capacitive discharge sources with attendant problems of severe electromagnetic interference, and plasma discharge sources.
覆盖50至300埃波段的连续发射源
由于极紫外辐射的重要性日益增加,对这一光谱范围的高强度实验室光源有相当大的兴趣。针对这些波长提出了各种各样的光源,其中许多都在Samson(1967)的经典著作中进行了描述。这些来源中的大多数都有很大的限制,特别是那些打算用于1200 Å以下的来源。我们(Paresce et al. 1971)和其他人已经开发出稳定且免维护的连续放电源,并在波长低至~300 Å的情况下提供大量强谱线。Henke(1975)开发和改进的软x射线源能够产生大量的软x射线辐射。然而,这些光源对于波长超过~50 Å的使用有严重的限制。例如,产生的大部分辐射是连续辐射,在任何特定线上的通量都相当低。此外,通量在较短波长处达到峰值。当被掠入射单色器分散时,一阶和许多更高阶的波长从出口狭缝出现,而不是通常期望的真正的单色通量。从本质上讲,唯一可用的可以在波长50到300 Å之间提供合理通量水平的源是伴随严重电磁干扰问题的电容放电源和等离子体放电源。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信