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在1600埃至300埃波长范围内,不同入射角下涂覆有MgF₂和LiF的铝的反射率。

Reflectance of Aluminum Overcoated with MgF(2) and LiF in the Wavelength Region from 1600 A to 300 A at Various Angles of Incidence.

作者信息

Hunter W R, Osantowski J F, Hass G

出版信息

Appl Opt. 1971 Mar 1;10(3):540-4. doi: 10.1364/AO.10.000540.

Abstract

Since the discovery that Al overcoated with MgF(2) or LiF produces high reflectances to wavelengths as short as 1150 A and 1000 A, respectively, these coatings have been used extensively in vacuum ultraviolet instruments in the wavelength region where their reflectance is high. If the instrument is intended to cover wavelengths shorter than the two given above, usually either Pt or Ir is used, with a loss of speed at the longer wavelengths. This paper presents reflectance data showing that fluoride-overcoated Al can be useful to wavelengths as short as 500 A. Measurements were made from 1600 A to about 300 A at normal, 35 degrees , and 85 degrees angles of incidence, angles used in normal, Seya, and grazing incidence spectrometers, respectively. These measurements show that from the boundary of the high reflectance region to 500 A, the reflectance at normal and 35 degrees depends on the thickness of the fluoride coating and can be as high as 24% at 800 A for a MgF(2) thickness of 150 A. For shorter wavelengths, the reflectance shows a decreasing thickness dependence and at 304 A is very low-about 1%. At grazing incidence, the reflectance shows some thickness dependence from 1500 A to about 1000 A, but toward shorter wavelengths the dependence disappears and the reflectance increases slowly to about 80% at 500 A. In addition to the reflectance measurements, polarization effects are discussed.

摘要

自从发现用MgF₂或LiF包覆的铝分别对短至1150 Å和1000 Å的波长产生高反射率以来,这些涂层已在其反射率较高的波长区域的真空紫外仪器中得到广泛应用。如果仪器要覆盖比上述两个波长更短的波长,通常使用Pt或Ir,但在较长波长下速度会降低。本文给出的反射率数据表明,包覆氟化物的铝在短至500 Å的波长下也可能有用。在垂直、35°和85°入射角下进行了测量,这些入射角分别用于常规、塞亚和掠入射光谱仪,测量范围从1600 Å到约300 Å。这些测量结果表明,从高反射率区域的边界到500 Å,垂直和35°入射角下的反射率取决于氟化物涂层的厚度,对于150 Å厚的MgF₂涂层,在800 Å处反射率可高达24%。对于更短的波长,反射率对厚度的依赖性降低,在304 Å处非常低,约为1%。在掠入射角下,反射率在1500 Å到约1000 Å之间显示出一定的厚度依赖性,但对于更短的波长,这种依赖性消失,反射率在500 Å处缓慢增加到约80%。除了反射率测量外,还讨论了偏振效应。

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