JP3762987B2 - X-ray condensing element - Google Patents
X-ray condensing element Download PDFInfo
- Publication number
- JP3762987B2 JP3762987B2 JP2002162285A JP2002162285A JP3762987B2 JP 3762987 B2 JP3762987 B2 JP 3762987B2 JP 2002162285 A JP2002162285 A JP 2002162285A JP 2002162285 A JP2002162285 A JP 2002162285A JP 3762987 B2 JP3762987 B2 JP 3762987B2
- Authority
- JP
- Japan
- Prior art keywords
- rays
- ray
- condensing element
- ray condensing
- condensing
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
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- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
Description
【0001】
【発明の属する技術分野】
X線は、産業、医療等で広く用いられ、利用技術の進展に伴い、ますますその用途が広がりつつある。利用分野に最適なX線のプロファイルを得るためには、X線光学素子は、必要不可欠であり、集光素子は、その中でも基本的な素子である。
【0002】
近年、集光素子は、利用に期待が集まっているX線リソグラフィーを初めとする加工分野、蛍光X線分析に代表される分析分野、CTに代表される医療分野等、X線を利用するほとんどの機器すべてに利用されているが、従来の集光素子は、加工が困難で高価であった。安価な集光素子を組み合わせ集光機能を持たせる場合には、高度なアライメントが必要であり、多くの労力を要した。
【0003】
【従来の技術】
X線に対する物質の屈折率は、如何なる物質でも、ほとんど真空中でのX線屈折率と等しく、物質透過によるX線の伝播方向の変化は、ごく僅かであるため、可視光で多用されるレンズ、プリズム等の透過型光学素子を、X線で実現する事は困難である。フレネルゾーンプレート等、回折型の光学素子では、効率が悪く、素子として有効に働くX線の波長域が限られるため、X線全般に対応可能な光学系を構成することは困難である。
反射型光学素子では、原理的にX線全般に対して伝播方向のコントロールが可能であるが、物質による反射率も小さくなるため、実用に耐えうる反射型光学素子には、可視光と比較して、厳しい条件が要求される。
【0004】
【発明が解決しようとする課題】
X線に対し、充分な反射率を得るためには、光学材料の反射面すれすれ(角度にして0.2〜0.5度程度)の斜入射でX線を入射させる必要がある。そのため、X線の集光素子を実現する場合、単なる球面ミラーでは、斜入射での収差が大きく、十分な集光が出来ない。入射面に平行な方向と垂直な方向の曲率を変え、収差を補正したトロイダルミラーであれば、集光は可能であるが、このようなトロイダルミラーの表面形状加工は、非常に困難である。加工が容易な光学素子の組み合わせにより集光機能をもたせる手法もあるが、光学素子各々に高度なアライメントが必要であり、またアライメント治具等により、システムが大型になるため、多くの労力を要した。
【0005】
【課題を解決するための手段】
上記課題を解決するために、本発明においては、加工が容易な反射面を、素子内に一体成形する。これらの反射面は、それぞれ縦、横及び前後の集光を受け持ち、これらにより入射X線を集光する。一体化により各反射面間の複雑なアライメントは不必要になり、また、集光素子の加工が容易になると共に小型化が可能となる。
【0006】
【実施の態様】
ミラーの材料としては、比較的重い金属元素、もしくはそれら元素を、集光素子形状に加工した母材内面にメッキした物がよい。あるいはX線領域においては、元素の全電子数、及び密度が高いほど該元素/真空の屈折率の違いが大きくなり、それにより大きな反射率が期待できるため、大きな反射率が期待できる重元素と軽元素を交互に積み重ねた多層膜を、集光素子形状に加工した母材内面に積層した物がよし。具体的な材料としては、クロム、マンガン、鉄、コバルト、ニッケル、銅、亜鉛、ニオブ、モリブデン、銀、金、プラチナ、タンタル、イリジウム、レニウム、タングステン等が挙げられる。周期律表上の同じような比較的重い金属元素として、タリウム、オスミウム等も可能であるが、毒性の問題がある。イリジウム、レニウムは、希少であること、タングステンは、加工性に難点がある。実施に当たっては、上記の毒性、手に入れ易さ、加工性等を考慮して決定しなければならない。
【0007】
【実施例】
図1に本発明によるX線集光素子の概念図を示す。集光素子上に形成された円筒穴内面をミラーとし、X線を反射する。反射率を損なわぬよう、各円筒ミラーは、斜入射の条件でX線が入射する配置となっている、各ミラーがそれぞれ縦、横、前後のX線集光をするため、当該光学素子の規定の位置、方向で入射したX線を集光させる事が出来る。
【0008】
また、本光学素子を図1−1のようにアレイ化することにより、本集光素子は容易に大面積化することが出来る。
【0009】
【発明の効果】
本発明によれば、従来の集光素子で必要とされていた複雑な加工、もしくは集光素子の高度なアライメントをすることなしに、X線の集光が可能となる。また、本集光素子を集積化することにより大面積の集光システムを構成することも可能となる。
【図面の簡単な説明】
【図1】 本発明の概念図
【図2】 集積化した大面積X線集光システムの概念図[0001]
BACKGROUND OF THE INVENTION
X-rays are widely used in industry, medicine, and the like, and their uses are expanding as the use technology advances. In order to obtain an X-ray profile optimal for the application field, an X-ray optical element is indispensable, and a condensing element is a basic element among them.
[0002]
In recent years, most of the light collecting elements use X-rays such as processing fields such as X-ray lithography, which are expected to be used, analysis fields represented by fluorescent X-ray analysis, medical fields represented by CT, etc. However, the conventional light collecting element is difficult to process and expensive. In order to provide a light collecting function by combining an inexpensive light collecting element, a high degree of alignment is required, and much labor is required.
[0003]
[Prior art]
The refractive index of a substance with respect to X-rays is almost the same as the X-ray refractive index in a vacuum, and the change in the X-ray propagation direction due to substance transmission is negligible. It is difficult to realize a transmission optical element such as a prism with X-rays. Diffractive optical elements such as Fresnel zone plates are inefficient and have a limited wavelength range of X-rays that work effectively as elements, making it difficult to construct an optical system that can handle X-rays in general.
Reflective optical elements can in principle control the direction of propagation for X-rays in general, but the reflectivity of the material is also small, so reflective optical elements that can withstand practical use are in comparison with visible light. Severe conditions are required.
[0004]
[Problems to be solved by the invention]
In order to obtain a sufficient reflectivity with respect to X-rays, it is necessary to make the X-rays incident at an oblique incidence of the reflective surface of the optical material (at an angle of about 0.2 to 0.5 degrees). Therefore, when an X-ray condensing element is realized, a simple spherical mirror has a large aberration at oblique incidence, and sufficient condensing cannot be performed. A toroidal mirror in which the curvature in the direction parallel to the incident surface and the direction perpendicular to the incident surface is changed to correct the aberration can collect light, but it is very difficult to process the surface shape of such a toroidal mirror. Although there is a method of providing a light collecting function by combining optical elements that are easy to process, each optical element requires a high degree of alignment, and the system becomes large due to the alignment jig, etc., which requires a lot of labor. did.
[0005]
[Means for Solving the Problems]
In order to solve the above problem, in the present invention, a reflective surface that is easy to process is integrally formed in the element. These reflecting surfaces are respectively responsible for vertical, horizontal, and front and rear light collection, and collect incident X-rays by these. The integration eliminates the need for complicated alignment between the reflecting surfaces, facilitates the processing of the light collecting element, and enables miniaturization.
[0006]
Embodiment
As a material for the mirror, a relatively heavy metal element or a material obtained by plating these elements on the inner surface of a base material processed into a condensing element shape is preferable. Alternatively, in the X-ray region, the higher the total number of electrons and the density of the element, the larger the difference in refractive index of the element / vacuum, and thus a higher reflectance can be expected. A multilayer film with light elements stacked alternately on the inner surface of a base material processed into a condensing element shape is good. Specific examples of the material include chromium, manganese, iron, cobalt, nickel, copper, zinc, niobium, molybdenum, silver, gold, platinum, tantalum, iridium, rhenium, and tungsten. Thallium, osmium, and the like are possible as similar relatively heavy metal elements on the periodic table, but there is a problem of toxicity. Iridium and rhenium are rare, and tungsten has difficulty in workability. In implementation, it must be determined in consideration of the above-mentioned toxicity, easy availability, processability and the like.
[0007]
【Example】
FIG. 1 shows a conceptual diagram of an X-ray condensing element according to the present invention. The inner surface of the cylindrical hole formed on the condensing element is used as a mirror to reflect X-rays. In order not to impair the reflectivity, each cylindrical mirror is arranged so that X-rays are incident under oblique incidence conditions. Since each mirror collects X-rays in the vertical, horizontal, and front and rear directions, X-rays incident at a specified position and direction can be condensed.
[0008]
Further, by arranging the present optical element in an array as shown in FIG. 1-1, the present condensing element can be easily increased in area.
[0009]
【The invention's effect】
According to the present invention, X-rays can be condensed without complicated processing required for a conventional light condensing element or high-level alignment of the light condensing elements. Further, by integrating the light collecting element, a large area light collecting system can be configured.
[Brief description of the drawings]
FIG. 1 is a conceptual diagram of the present invention. FIG. 2 is a conceptual diagram of an integrated large area X-ray focusing system.
Claims (2)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2002162285A JP3762987B2 (en) | 2002-06-04 | 2002-06-04 | X-ray condensing element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2002162285A JP3762987B2 (en) | 2002-06-04 | 2002-06-04 | X-ray condensing element |
Publications (2)
Publication Number | Publication Date |
---|---|
JP2004012154A JP2004012154A (en) | 2004-01-15 |
JP3762987B2 true JP3762987B2 (en) | 2006-04-05 |
Family
ID=30431064
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2002162285A Expired - Lifetime JP3762987B2 (en) | 2002-06-04 | 2002-06-04 | X-ray condensing element |
Country Status (1)
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JP (1) | JP3762987B2 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP4602944B2 (en) * | 2006-06-22 | 2010-12-22 | 日本電信電話株式会社 | X-ray condenser lens |
JP4705606B2 (en) * | 2007-05-10 | 2011-06-22 | 日本電信電話株式会社 | X-ray condenser lens |
JP4700034B2 (en) * | 2007-08-13 | 2011-06-15 | 日本電信電話株式会社 | X-ray condenser lens |
JP4659015B2 (en) * | 2007-11-14 | 2011-03-30 | 日本電信電話株式会社 | X-ray condenser lens |
US8344339B2 (en) * | 2010-08-30 | 2013-01-01 | Media Lario S.R.L. | Source-collector module with GIC mirror and tin rod EUV LPP target system |
-
2002
- 2002-06-04 JP JP2002162285A patent/JP3762987B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
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JP2004012154A (en) | 2004-01-15 |
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