CN106959482A - Two-dimensional single-stage diffraction grating for extreme ultraviolet - Google Patents

Two-dimensional single-stage diffraction grating for extreme ultraviolet Download PDF

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CN106959482A
CN106959482A CN201710368980.4A CN201710368980A CN106959482A CN 106959482 A CN106959482 A CN 106959482A CN 201710368980 A CN201710368980 A CN 201710368980A CN 106959482 A CN106959482 A CN 106959482A
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grating
light
strips
diffraction
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CN106959482B (en
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刘子维
浦探超
史丽娜
谢常青
王冠亚
李海亮
牛洁斌
刘明
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings
    • G02B5/1838Diffraction gratings for use with ultraviolet radiation or X-rays
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings
    • G02B5/1866Transmission gratings characterised by their structure, e.g. step profile, contours of substrate or grooves, pitch variations, materials
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings
    • G02B2005/1804Transmission gratings

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Abstract

本发明公开了一种极紫外光的二维单级衍射光栅,包括:透明基底以及位于所述透明基底表面的栅条层;所述栅条层具有多个透光栅条以及多个不透光栅条;所述透光栅条以及所述不透光栅条在第一方向上交替分布,且所述透光栅条以及所述不透光栅条均沿第二方向延伸,所述第一方向垂直于所述第二方向;在所述第一方向上,所述透光栅条相对的两边均为锯齿形;且所述透光栅条在所述第一方向上的宽度处处相同。本发明技术方案通过锯齿形的透光栅条与不透光栅条实现衍射,透光栅条的宽度不变,并设置随机分布的透光栅条,使得不透光栅条的宽度满足预设的随机分布,可以在实现对预设波段实现衍射的同时消除高次谐波。

The invention discloses a two-dimensional single-stage diffraction grating for extreme ultraviolet light, which comprises: a transparent base and a grid layer located on the surface of the transparent base; the grid layer has a plurality of transparent grating bars and a plurality of opaque gratings strips; the light-transmitting grating strips and the light-transmitting grating strips are alternately distributed in the first direction, and the light-transmitting grating strips and the light-impermeable grating strips all extend along the second direction, and the first direction is perpendicular to the In the second direction; in the first direction, the opposite sides of the light transmission grating strips are zigzag; and the width of the light transmission grating strips in the first direction is the same everywhere. The technical solution of the present invention realizes diffraction through zigzag-shaped grating strips and opaque grating strips, the width of the grating strips remains unchanged, and randomly distributed translucent grating strips are set so that the width of the opaque grating strips meets the preset random distribution. It can eliminate high-order harmonics while achieving diffraction for preset bands.

Description

一种用于极紫外的二维单级衍射光栅A two-dimensional single-order diffraction grating for extreme ultraviolet

技术领域technical field

本发明涉及光学器件技术领域,更具体的说,涉及一种用于极紫外的二维单级衍射光栅。The invention relates to the technical field of optical devices, in particular to a two-dimensional single-stage diffraction grating for extreme ultraviolet.

背景技术Background technique

衍射光栅发展时间较长,目前用于光谱仪的光栅一般为传统的一系列的平行沟槽和线条组成的金属薄膜黑白光光栅,存在多级衍射的问题。尤其是在极紫外波段,由于此波段存在大量的原子共振线与吸收线,任何材料对此波段的辐射都存在严重的吸收,甚至空气也不例外,其吸收长度通常为微米或纳米量级。因此,极紫外波段辐射的研究具有极大的困难。Diffraction gratings have been developed for a long time. At present, the gratings used in spectrometers are generally traditional metal thin film black and white optical gratings composed of a series of parallel grooves and lines, which have the problem of multi-level diffraction. Especially in the extreme ultraviolet band, due to the existence of a large number of atomic resonance lines and absorption lines in this band, any material has serious absorption of radiation in this band, even air is no exception, and its absorption length is usually on the order of microns or nanometers. Therefore, the study of extreme ultraviolet radiation is extremely difficult.

目前,很多的衍射光栅器件已经被发明应用,有的衍射光栅器件利用光栅制造周期D在(λ,2λ)区间时会抑制特定波长λ所产生的高级衍射,然而,有效抑制的波长λ范围只被限制在了(D/2,D)区间,而对于极紫外波这样的短波长,以目前的纳米制造工艺很难将周期控制在合适区间之内;有的衍射光栅器件利用不同种类的滤片组合来抑制目标波长的高次谐波,但是在测量光谱时,一块滤片仅对某一波长区域有效,不同的区域需要不同的插入件,这不仅增加了制造成本,也使谱仪结构变得复杂,更重要的是这会对测量谱线的精度造成很大的影响。总之,在极紫外波段,这些方法都很难得到满意的效果。At present, many diffraction grating devices have been invented and applied. Some diffraction grating devices can suppress the high-order diffraction produced by a specific wavelength λ when the grating manufacturing period D is in the (λ, 2λ) interval. However, the effectively suppressed wavelength λ range is only It is limited in the (D/2, D) interval, and for short wavelengths such as extreme ultraviolet waves, it is difficult to control the period within the appropriate interval with the current nano-manufacturing process; some diffraction grating devices use different types of filters However, when measuring the spectrum, a filter is only effective for a certain wavelength region, and different regions require different inserts, which not only increases the manufacturing cost, but also makes the spectrometer structure More importantly, it will have a great impact on the accuracy of the measured spectral lines. In short, in the extreme ultraviolet band, these methods are difficult to obtain satisfactory results.

因此,设计并制作能够在极紫外波段有效地抑制高次谐波,并且易于加工的单级衍射光栅是目前光谱分析技术发展和应用领域中迫切需要解决的问题。Therefore, designing and manufacturing a single-order diffraction grating that can effectively suppress high-order harmonics in the extreme ultraviolet band and is easy to process is an urgent problem to be solved in the development and application of spectral analysis technology.

发明内容Contents of the invention

为了解决上述问题,本发明提供了一种用于极紫外的二维单级衍射光栅,可以在极紫外波段有效的抑制高次谐波,且制作工艺简单,制作成本低。In order to solve the above problems, the present invention provides a two-dimensional single-stage diffraction grating for extreme ultraviolet, which can effectively suppress high-order harmonics in the extreme ultraviolet band, and has a simple manufacturing process and low manufacturing cost.

为了实现上述目的,本发明提供如下技术方案:In order to achieve the above object, the present invention provides the following technical solutions:

一种用于极紫外光的二维单级衍射光栅,所述二维单级衍射光栅包括:透明基底以及位于所述透明基底表面的栅条层;A two-dimensional single-order diffraction grating for extreme ultraviolet light, the two-dimensional single-order diffraction grating comprising: a transparent substrate and a grid layer located on the surface of the transparent substrate;

所述栅条层具有多个透光栅条以及多个不透光栅条;The grating layer has a plurality of light-transmitting grating bars and a plurality of light-impermeable grating bars;

所述透光栅条以及所述不透光栅条在第一方向上交替分布,且所述透光栅条以及所述不透光栅条均沿第二方向延伸,所述第一方向垂直于所述第二方向;The light-transmitting grating strips and the light-transmitting grating strips are alternately distributed in a first direction, and both the light-transmitting grating strips and the light-impermeable grating strips extend along a second direction, and the first direction is perpendicular to the first direction. Two directions;

在所述第一方向上,所述透光栅条相对的两边均为锯齿形;且所述透光栅条在所述第一方向上的宽度处处相同。In the first direction, opposite sides of the light transmission grating strips are zigzag; and the width of the light transmission grating strips in the first direction is the same.

优选的,在上述二维单级衍射光栅中,在所述第一方向上,所述二维单级衍射光栅的光栅常数为P,所述透光栅条的宽度为P/2,所述不透光栅条在所述第一方向上的宽度为d;且d的取值范围满足: Preferably, in the above-mentioned two-dimensional single-stage diffraction grating, in the first direction, the grating constant of the two-dimensional single-stage diffraction grating is P, the width of the grating bars is P/2, and the non- The width of the light-transmitting grating strip in the first direction is d; and the value range of d satisfies:

优选的,在上述二维单级衍射光栅中,所述光栅常数的范围是450nm-550nm,包括端点值。Preferably, in the above-mentioned two-dimensional single-stage diffraction grating, the range of the grating constant is 450nm-550nm, including the endpoint values.

优选的,在上述二维单级衍射光栅中,在所述第一方向上,所述透光栅条一侧锯齿的宽度等于所述光栅常数的六分之一。Preferably, in the above-mentioned two-dimensional single-stage diffraction grating, in the first direction, the width of the sawtooth on one side of the grating bar is equal to one-sixth of the grating constant.

优选的,在上述二维单级衍射光栅中,所述不透光栅条为金薄膜、或银薄膜、或铝薄膜、或铬薄膜、或硅薄膜、或氮化硅薄膜、或碳化硅薄膜。Preferably, in the above two-dimensional single-order diffraction grating, the opaque grating strips are gold thin films, or silver thin films, or aluminum thin films, or chromium thin films, or silicon thin films, or silicon nitride thin films, or silicon carbide thin films.

优选的,在上述二维单级衍射光栅中,在垂直于所述透明基底的方向上,所述不透光栅条的厚度范围是100nm-300nm,包括端点值。Preferably, in the above-mentioned two-dimensional single-stage diffraction grating, in a direction perpendicular to the transparent substrate, the thickness of the opaque grating strips ranges from 100nm to 300nm, inclusive.

优选的,在上述二维单级衍射光栅中,所述透明基底为二氧化硅基底、或氮化硅基底、或碳化硅基底。Preferably, in the above-mentioned two-dimensional single-order diffraction grating, the transparent substrate is a silicon dioxide substrate, or a silicon nitride substrate, or a silicon carbide substrate.

通过上述描述可知,本发明技术方案提供的用于极紫外的二维单级衍射光栅中,设置所述透光栅条以及所述不透光栅条在第一方向上交替分布,且所述透光栅条以及所述不透光栅条均沿第二方向延伸,所述第一方向垂直于所述第二方向;在所述第一方向上,所述透光栅条相对的两边均为锯齿形;且所述透光栅条在所述第一方向上的宽度处处相同。通过调整透光栅条在之间的间距以及透光栅条的宽度,在实现对极紫外光波段的衍射的同时,使得衍射图案只具有0级和正负1级衍射图案,能够消除2n、3n、4n、5n级衍射(n为非零整数)级衍射,抑制高级衍射,降低噪点,提高分辨率。It can be seen from the above description that in the two-dimensional single-order diffraction grating for extreme ultraviolet provided by the technical solution of the present invention, the grating bars and the grating bars are arranged alternately in the first direction, and the grating Both the bars and the grating bars extend along a second direction, and the first direction is perpendicular to the second direction; in the first direction, opposite sides of the grating bars are zigzag-shaped; and The widths of the light-transmitting grating bars in the first direction are the same. By adjusting the spacing between the grating bars and the width of the grating bars, while realizing the diffraction of the extreme ultraviolet light band, the diffraction pattern only has 0-order and positive and negative 1-order diffraction patterns, which can eliminate 2n, 3n, 4n, 5n order diffraction (n is a non-zero integer) order diffraction, suppressing advanced diffraction, reducing noise and improving resolution.

附图说明Description of drawings

为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据提供的附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention or the prior art, the following will briefly introduce the drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description are only It is an embodiment of the present invention, and those skilled in the art can also obtain other drawings according to the provided drawings without creative work.

图1为本发明实施例提供的一种于极紫外光的二维单级衍射光栅的俯视图;Fig. 1 is a top view of a two-dimensional single-order diffraction grating for extreme ultraviolet light provided by an embodiment of the present invention;

图2为图1所示二维单级衍射光栅在AA’方向的切面图;Fig. 2 is the sectional view of the two-dimensional single-order diffraction grating shown in Fig. 1 in the AA' direction;

图3为图1所示二维单级衍射光栅的透光栅条的结构示意图;Fig. 3 is a structural schematic diagram of the grating bars of the two-dimensional single-stage diffraction grating shown in Fig. 1;

图4为本发明实施例提供的一种二维待机衍射光栅对极紫外光的衍射特性图;Fig. 4 is a diagram of the diffraction characteristics of a two-dimensional standby diffraction grating for extreme ultraviolet light provided by an embodiment of the present invention;

图5为本发明实施例提供的一种二维待机衍射光栅对可见光的衍射特性图;Fig. 5 is a diagram of the diffraction characteristics of a two-dimensional standby diffraction grating for visible light provided by an embodiment of the present invention;

图6为本发明实施例提供的一种衍射特性图。Fig. 6 is a diffraction characteristic diagram provided by an embodiment of the present invention.

具体实施方式detailed description

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will clearly and completely describe the technical solutions in the embodiments of the present invention with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some, not all, embodiments of the present invention. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

为使本发明的上述目的、特征和优点能够更加明显易懂,下面结合附图和具体实施方式对本发明作进一步详细的说明。In order to make the above objects, features and advantages of the present invention more comprehensible, the present invention will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.

本发明实施例提供了一种用于极紫外光的二维单级衍射光栅,如图1-图3所示,图1为本发明实施例提供的一种于极紫外光的二维单级衍射光栅的俯视图,图2为图1所示二维单级衍射光栅在AA’方向的切面图,图3为图1所示二维单级衍射光栅的透光栅条的结构示意图。An embodiment of the present invention provides a two-dimensional single-stage diffraction grating for extreme ultraviolet light, as shown in Figure 1-Figure 3, Figure 1 is a two-dimensional single-stage diffraction grating for extreme ultraviolet light provided by an embodiment of the present invention The top view of the diffraction grating, Fig. 2 is a sectional view of the two-dimensional single-stage diffraction grating shown in Fig. 1 in the AA' direction, and Fig. 3 is a schematic structural diagram of the transmission grating strips of the two-dimensional single-stage diffraction grating shown in Fig. 1 .

本发明实施例提供的二维单级衍射光栅包括:透明基底11以及位于所述透明基底表面的栅条层;所述栅条层具有多个透光栅条12以及多个不透光栅条13。The two-dimensional single-order diffraction grating provided by the embodiment of the present invention includes: a transparent substrate 11 and a grating layer located on the surface of the transparent substrate;

所述透光栅条12以及所述不透光栅条13在第一方向X上交替分布,且所述透光栅条12以及所述不透光栅条13均沿第二方向Y延伸,所述第一方向X垂直于所述第二方向Y。所述第一方向X以及所述第二方向Y均平行于所述透明基底11。第三方向Z垂直于所述透明基板11。The light-transmitting grating strips 12 and the light-transmitting grating strips 13 are distributed alternately in the first direction X, and the light-transmitting grating strips 12 and the light-impermeable grating strips 13 both extend along the second direction Y, and the first The direction X is perpendicular to said second direction Y. Both the first direction X and the second direction Y are parallel to the transparent substrate 11 . The third direction Z is perpendicular to the transparent substrate 11 .

在所述第一方向X上,所述透光栅条12相对的两边均为锯齿形;且所述透光栅条12在所述第一方向X上的宽度处处相同,均为P/2。P为所述二维单级衍射光栅的光栅常数。In the first direction X, opposite sides of the light transmission grating strip 12 are zigzag; and the width of the light transmission grating strip 12 in the first direction X is the same everywhere, which is P/2. P is the grating constant of the two-dimensional single-stage diffraction grating.

如图3所示,为了使得透光栅条12相对的两边均为锯齿形,所述透光栅条12包括:沿第二方向Y延伸的矩形条状区域21;在第一方向X上,设置在矩形条状区域21两侧的多个锯齿22。As shown in FIG. 3 , in order to make the opposite sides of the light-transmitting grating strip 12 both zigzag-shaped, the light-transmitting grating strip 12 includes: a rectangular strip-shaped region 21 extending along the second direction Y; A plurality of serrations 22 on both sides of the rectangular strip area 21 .

通过调节光栅常数、透光栅条12的宽度以及不透光栅条13的宽度可以使得该二维单级衍射光栅在目标波段实现衍射的同时,并消除该波段的高级衍射。如上述,当所述二维单级衍射光栅的光栅常数为P时,为了实现在实现衍射的同时消除高级衍射,在所述第一方向X上,设置所述透光栅条12的宽度为P/2,所述不透光栅条13在所述第一方向上的宽度为d,且d的取值范围满足:不同的不透光栅条的宽度d可以不同。不透光栅条的宽度d满足随机分布关系。By adjusting the grating constant, the width of the transparent grating strip 12 and the width of the non-transparent grating strip 13, the two-dimensional single-stage diffraction grating can achieve diffraction in the target wavelength band and eliminate high-order diffraction in the band. As mentioned above, when the grating constant of the two-dimensional single-stage diffraction grating is P, in order to achieve diffraction while eliminating high-order diffraction, in the first direction X, set the width of the grating bar 12 to be P /2, the width of the opaque grating strip 13 in the first direction is d, and the value range of d satisfies: The width d of the different grating strips can be different. The width d of the opaque grating strip satisfies Random distribution relationship.

通过设置光栅常数P以及所述不透光栅条13的宽度为d,可以使得该二维单级衍射光栅能够对不同波段的光波实现衍射的同时,并消除高阶衍射。By setting the grating constant P and the width of the opaque grating strips 13 as d, the two-dimensional single-stage diffraction grating can diffract light waves of different wavelength bands and eliminate high-order diffraction.

根据光栅的延伸原理,不透光栅条的宽度d、入射光的波长λ以及入射角θ满足:According to the extension principle of the grating, the width d of the impermeable grating strip, the wavelength λ of the incident light and the angle of incidence θ satisfy:

dsinθm=mλdsinθ m =mλ

其中,θm为入射角,m为±1、±2、±3、…。根据夫琅禾费衍射原理可知,衍射强度公式为:Wherein, θ m is the incident angle, and m is ±1, ±2, ±3, . . . According to the principle of Fraunhofer diffraction, the formula of diffraction intensity is:

其中,m为衍射级次,不同衍射级次的强度是零级衍射强度I0与三个sinc数学式的乘积。当d满足上述随机分布时,2n、3n、4n、5n级衍射的强度均为零,以消除高级衍射。Among them, m is the diffraction order, and the intensity of different diffraction orders is the product of the zero-order diffraction intensity I 0 and three sinc mathematical formulas. When d satisfies the above random distribution, the intensity of 2n, 3n, 4n, and 5n order diffractions are all zero to eliminate higher order diffractions.

本发明实施例所述二维单级衍射光栅通过锯齿形的透光栅条12以及锯齿形的不透光栅条实现光波衍射,同时通过设计不透光栅条13的宽度为关于光栅常数的预设随机分布关系,在实现衍射的同时能够消除高级衍射,降低噪点,提高分辨率。The two-dimensional single-stage diffraction grating described in the embodiment of the present invention realizes light wave diffraction through the zigzag-shaped transparent grating strip 12 and the zigzag-shaped opaque grating strip. The distribution relationship can eliminate advanced diffraction, reduce noise and improve resolution while realizing diffraction.

当用于极紫外光的衍射时,所述光栅常数P的范围是450nm-550nm,包括端点值。在所述第一方向X上,所述透光栅条13一侧锯齿22的宽度等于所述光栅常数的六分之一,即锯齿22的宽度等于P/6。When used for the diffraction of extreme ultraviolet light, the range of the grating constant P is 450nm-550nm, inclusive. In the first direction X, the width of the sawtooth 22 on one side of the light-transmitting grating strip 13 is equal to one-sixth of the grating constant, that is, the width of the sawtooth 22 is equal to P/6.

本发明实施例中,所述不透光栅条13采用吸收极紫外光的材料制备。具体的,所述不透光栅条13可以为金薄膜、或银薄膜、或铝薄膜、或铬薄膜、或硅薄膜、或氮化硅薄膜、或碳化硅薄膜。In the embodiment of the present invention, the grating bars 13 are made of materials that absorb extreme ultraviolet light. Specifically, the grating bar 13 may be a gold film, or a silver film, or an aluminum film, or a chromium film, or a silicon film, or a silicon nitride film, or a silicon carbide film.

可选的,在垂直于所述透明基底的方向Z上,所述不透光栅条13的厚度范围是100nm-300nm,包括端点值。可以设置不透光栅条13的厚度为150nm。所述透明基底11为二氧化硅基底、或氮化硅基底、或碳化硅基底。Optionally, in the direction Z perpendicular to the transparent substrate, the thickness of the grating strips 13 is in a range of 100 nm-300 nm, inclusive. The thickness of the grating bars 13 may be set to be 150 nm. The transparent substrate 11 is a silicon dioxide substrate, or a silicon nitride substrate, or a silicon carbide substrate.

本发明实施例所述的二维单级衍射光栅能够消除2n、3n、4n,5n级的衍射光栅,扩大了单极衍射光栅检测到的光谱范围,完全的抑制了噪声,有效的解决了高次谐波的污染问题,同时本发明设计的单级衍射光栅包括透光和不透光的二值化的结构,易于制作,极大的简化了工艺难度,尤其是在极紫外光学系统中,使现代的光谱分析技术应用于极紫外波段。The two-dimensional single-stage diffraction grating described in the embodiment of the present invention can eliminate 2n, 3n, 4n, and 5n-order diffraction gratings, expand the spectral range detected by the single-pole diffraction grating, completely suppress noise, and effectively solve the problem of high The problem of subharmonic pollution, and the single-order diffraction grating designed by the present invention includes a light-transmitting and opaque binary structure, which is easy to manufacture and greatly simplifies the process difficulty, especially in the extreme ultraviolet optical system. Apply modern spectroscopic analysis techniques to the extreme ultraviolet band.

本发明实施例所述的二维单级衍射光栅结构简单,可以通过图案化该薄膜可以形成预设结构的不透光栅条13以及透光栅条12,该薄膜可以通过镀膜工艺形成,图案化该薄膜的方法可以采用标准的半导体工艺制作,易于加工,制作方法简单,制作成本低。可以通过刻蚀工艺在薄膜表面形成随机分布的透光栅条12,以使得不透光栅条13的宽度成预设的随机分布。The two-dimensional single-stage diffraction grating described in the embodiment of the present invention has a simple structure, and the opaque grating bars 13 and the light-transmitting grating bars 12 of a preset structure can be formed by patterning the film. The film can be formed by a coating process, and the patterned film The method of thin film can be manufactured by standard semiconductor technology, easy to process, simple in manufacturing method and low in manufacturing cost. Randomly distributed optically transparent grating strips 12 can be formed on the surface of the film by an etching process, so that the widths of the optically non-transparent grating strips 13 have a preset random distribution.

本发明实施例所述的二维单级衍射光栅用于极紫外波段衍射时,能够有效抑制高次谐波,可以在极紫外光学系统和激光等离子体诊断软X光谱测量当中得到应用,以适应更广范围的实际应用需求。When the two-dimensional single-stage diffraction grating described in the embodiment of the present invention is used for diffraction in the extreme ultraviolet band, it can effectively suppress high-order harmonics, and can be applied in extreme ultraviolet optical systems and laser plasma diagnostic soft X-spectrum measurements to adapt to A wider range of practical application needs.

下面结合具体的实验数据说明本申请实施例中二维待机衍射光栅消除高级衍射的效果。The effect of the two-dimensional standby diffraction grating in the embodiment of the present application to eliminate high-order diffraction will be described below in combination with specific experimental data.

在透明基底表面形成不透光的薄膜。该薄膜可以完全吸收极紫外光。该薄膜可以为金属铬薄膜,厚度为150nm。刻蚀所述不透光的薄膜,被刻蚀的区域形成透光栅条,未刻蚀的区域为不透光栅条。被刻蚀的区域在第一方向上的两侧均为锯齿形,形成上述锯齿形的透光栅条。Form an opaque film on the surface of a transparent substrate. The film can completely absorb extreme ultraviolet light. The film can be a metal chromium film with a thickness of 150nm. Etching the opaque film, the etched area forms a light-transmitting grating strip, and the unetched area is an opaque grating strip. Both sides of the etched region in the first direction are zigzag-shaped, forming the above-mentioned zigzag light-transmitting grating strips.

所述透光栅条在所述不透光的薄膜上随机分布,使得不透光薄膜的宽度满足随机分布关系。The light-transmitting grating strips are randomly distributed on the opaque film, so that the width of the opaque film satisfies Random distribution relationship.

当发明实施例所述二维待机衍射光栅在极紫外光照射下,其衍射特性图如图4所示,图4为本发明实施例提供的一种二维待机衍射光栅对极紫外光的衍射特性图。When the two-dimensional standby diffraction grating described in the embodiment of the invention is irradiated by extreme ultraviolet light, its diffraction characteristic diagram is shown in Figure 4, and Figure 4 is the diffraction of extreme ultraviolet light by a two-dimensional standby diffraction grating provided by the embodiment of the present invention characteristic map.

由图4可知,当入射波长为50nm时,在横轴ξ上,只存在0级和±1级衍射。图4中在横轴ξ上依次排布的三个白色光斑中,中间亮度较大的白色光斑为0级颜色图像,其左右两侧的分别为±1级衍射图像。在横轴ξ上,不存在其他高级衍射,在纵轴η上,在0级衍射图像的上下两侧不存在衍射图案。因此,该二维待机衍射光栅可以作为单色仪或者光谱仪的分光元件使用,将排除谐波污染问题。It can be seen from Figure 4 that when the incident wavelength is 50nm, on the horizontal axis ξ, there are only 0-order and ±1-order diffractions. Among the three white spots arranged sequentially on the horizontal axis ξ in Fig. 4, the white spot with higher brightness in the middle is the 0th-order color image, and the left and right sides are respectively ±1st-order diffraction images. On the horizontal axis ξ, there is no other higher order diffraction, and on the vertical axis η, there are no diffraction patterns on the upper and lower sides of the 0th order diffraction image. Therefore, the two-dimensional standby diffraction grating can be used as a spectroscopic element of a monochromator or a spectrometer, and the problem of harmonic pollution will be eliminated.

当发明实施例所述二维待机衍射光栅在波长为500nm的可见光照射下,其横轴ξ方向上的衍射特性图如图5所示,图5为本发明实施例提供的一种二维待机衍射光栅对可见光的衍射特性图,图5中纵轴为相对衍射效率,横轴为衍射级次,可以看到,1级的相对0级的衍射效率为23.94%,可以看出本发明实施例所述二维待机衍射光栅和传统正弦衍射光栅有同样的抑制高级衍射的性质,在平行于光栅衍射的ξ轴上,只存在0级和+1/-1级衍射。不存在高级衍射。When the two-dimensional standby diffraction grating described in the embodiment of the invention is irradiated by visible light with a wavelength of 500 nm, the diffraction characteristic diagram in the direction of the horizontal axis ξ is shown in Figure 5, which is a two-dimensional standby diffraction grating provided by the embodiment of the present invention. The diffraction characteristic diagram of the diffraction grating for visible light. In Figure 5, the vertical axis is the relative diffraction efficiency, and the horizontal axis is the diffraction order. It can be seen that the diffraction efficiency of the 1st order relative to the 0th order is 23.94%. It can be seen that the embodiment of the present invention The two-dimensional standby diffraction grating and the traditional sinusoidal diffraction grating have the same property of suppressing high-order diffraction, and only 0-order and +1/-1-order diffraction exist on the ξ axis parallel to grating diffraction. No advanced diffraction exists.

如图6所示,图6为本发明实施例提供的一种衍射特性图,他图6中纵轴为相对衍射效率的对数,横轴为衍射级次,可以更加清晰地看到,单级衍射光栅能够抑制2n、3n、4n,5n(n为非零整数)级衍射。本发明扩大了单极衍射光栅检测到的光谱范围,完全的抑制了噪声,有效的解决了高次谐波的污染问题。As shown in Figure 6, Figure 6 is a diffraction characteristic diagram provided by the embodiment of the present invention. In Figure 6, the vertical axis is the logarithm of the relative diffraction efficiency, and the horizontal axis is the diffraction order, which can be seen more clearly. The order diffraction grating can suppress 2n, 3n, 4n, 5n (n is a non-zero integer) order diffraction. The invention expands the spectrum range detected by the monopole diffraction grating, completely suppresses the noise, and effectively solves the pollution problem of the high order harmonic.

通过上述描述可知,本发明实施例所述二维待机衍射光栅通过锯齿形的透光栅条与不透光栅条实现衍射,透光栅条的宽度不变,并设置随机分布的透光栅条,使得不透光栅条的宽度满足预设的随机分布,可以在实现对预设波段实现衍射的同时消除高次谐波。From the above description, it can be seen that the two-dimensional standby diffraction grating in the embodiment of the present invention realizes diffraction through zigzag transparent grating strips and opaque grating strips, the width of the transparent grating strips remains unchanged, and the randomly distributed transparent grating strips are set so that no The width of the grating strips satisfies a preset random distribution, which can eliminate high-order harmonics while achieving diffraction for preset wavelength bands.

对所公开的实施例的上述说明,使本领域专业技术人员能够实现或使用本发明。对这些实施例的多种修改对本领域的专业技术人员来说将是显而易见的,本文中所定义的一般原理可以在不脱离本发明的精神或范围的情况下,在其它实施例中实现。因此,本发明将不会被限制于本文所示的这些实施例,而是要符合与本文所公开的原理和新颖特点相一致的最宽的范围。The above description of the disclosed embodiments is provided to enable any person skilled in the art to make or use the invention. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the general principles defined herein may be implemented in other embodiments without departing from the spirit or scope of the invention. Therefore, the present invention will not be limited to the embodiments shown herein, but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.

Claims (7)

1.一种用于极紫外光的二维单级衍射光栅,其特征在于,包括:透明基底以及位于所述透明基底表面的栅条层;1. A two-dimensional single-order diffraction grating for extreme ultraviolet light, characterized in that it comprises: a transparent substrate and a grid layer located on the surface of the transparent substrate; 所述栅条层具有多个透光栅条以及多个不透光栅条;The grating layer has a plurality of light-transmitting grating bars and a plurality of light-impermeable grating bars; 所述透光栅条以及所述不透光栅条在第一方向上交替分布,且所述透光栅条以及所述不透光栅条均沿第二方向延伸,所述第一方向垂直于所述第二方向;The light-transmitting grating strips and the light-transmitting grating strips are alternately distributed in a first direction, and both the light-transmitting grating strips and the light-impermeable grating strips extend along a second direction, and the first direction is perpendicular to the first direction. Two directions; 在所述第一方向上,所述透光栅条相对的两边均为锯齿形;且所述透光栅条在所述第一方向上的宽度处处相同。In the first direction, opposite sides of the light transmission grating strips are zigzag; and the width of the light transmission grating strips in the first direction is the same. 2.根据权利要求1所述的二维单级衍射光栅,其特征在于,在所述第一方向上,所述二维单级衍射光栅的光栅常数为P,所述透光栅条的宽度为P/2,所述不透光栅条在所述第一方向上的宽度为d;且d的取值范围满足: 2. The two-dimensional single-stage diffraction grating according to claim 1, characterized in that, in the first direction, the grating constant of the two-dimensional single-stage diffraction grating is P, and the width of the grating bars is P/2, the width of the opaque grating strip in the first direction is d; and the value range of d satisfies: 3.根据权利要求2所述的二维单级衍射光栅,其特征在于,所述光栅常数的范围是450nm-550nm,包括端点值。3. The two-dimensional single-stage diffraction grating according to claim 2, characterized in that, the range of the grating constant is 450nm-550nm, inclusive. 4.根据权利要求2所述的二维单级衍射光栅,其特征在于,在所述第一方向上,所述透光栅条一侧锯齿的宽度等于所述光栅常数的六分之一。4. The two-dimensional single-stage diffraction grating according to claim 2, characterized in that, in the first direction, the width of the serrations on one side of the light-transmitting grating bar is equal to one-sixth of the grating constant. 5.根据权利要求1所述的二维单级衍射光栅,其特征在于,所述不透光栅条为金薄膜、或银薄膜、或铝薄膜、或铬薄膜、或硅薄膜、或氮化硅薄膜、或碳化硅薄膜。5. The two-dimensional single-order diffraction grating according to claim 1, wherein the opaque grating strip is a gold film, or a silver film, or an aluminum film, or a chromium film, or a silicon film, or silicon nitride film, or silicon carbide film. 6.根据权利要求1所述的二维单级衍射光栅,其特征在于,在垂直于所述透明基底的方向上,所述不透光栅条的厚度范围是100nm-300nm,包括端点值。6 . The two-dimensional single-order diffraction grating according to claim 1 , wherein, in a direction perpendicular to the transparent substrate, the thickness of the grating strips ranges from 100 nm to 300 nm, inclusive. 7.根据权利要求1所述的二维单级衍射光栅,其特征在于,所述透明基底为二氧化硅基底、或氮化硅基底、或碳化硅基底。7. The two-dimensional single-order diffraction grating according to claim 1, wherein the transparent substrate is a silicon dioxide substrate, a silicon nitride substrate, or a silicon carbide substrate.
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