JPH02217801A - Optical element consisting of multilayered films of curved type - Google Patents
Optical element consisting of multilayered films of curved typeInfo
- Publication number
- JPH02217801A JPH02217801A JP1038667A JP3866789A JPH02217801A JP H02217801 A JPH02217801 A JP H02217801A JP 1038667 A JP1038667 A JP 1038667A JP 3866789 A JP3866789 A JP 3866789A JP H02217801 A JPH02217801 A JP H02217801A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- optical element
- curved
- recessed shape
- laminated
- 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.)
- Pending
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/44—Mechanical structures for providing tensile strength and external protection for fibres, e.g. optical transmission cables
- G02B6/4401—Optical cables
- G02B6/4415—Cables for special applications
- G02B6/4427—Pressure resistant cables, e.g. undersea cables
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Filters (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は湾曲型多層膜光学素子に関し、例えばSOR
光の集光や分光などに用いられるものに関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a curved multilayer optical element, for example, SOR.
It relates to things used for condensing and spectroscopy of light.
従来の光学素子として、雑誌(Monochrorns
torsfor X−rB 5ynchrotron
radiations Comm1ssionof t
he European C()mmunltle@+
J−R−C−1@pra*l5pra+ Italy
)に記載されているものの側面(2)を第4図(a)に
示す。As a conventional optical element, magazines (Monochrons
torsfor X-rB 5ynchrotron
radiationsComm1ssionof t
he European C()mmunltle@+
J-R-C-1@pra*l5pra+ Italy
) is shown in side view (2) of FIG. 4(a).
図において、111は結晶であり、(Im) *(lb
)−(lc)。In the figure, 111 is a crystal, (Im) * (lb
)-(lc).
(1d)はそれぞれ原子列を示している。この結晶(1
)は例えば4層の原子列を有するものである。(1d) each shows an atomic sequence. This crystal (1
) has, for example, four layers of atomic arrays.
次に動作について説明する。普通の状態における平板結
晶のある原子面を模式的に示したのが第4 IN (a
)である。第4図(b)では結晶11+に矢印Aのよう
な力を加えており、湾曲した面を有する結晶(1)を構
成している。このように湾曲した結晶11)に、ある発
散角を持つX線が入射されると、ブラック条件にあう波
だけが回折を受ける。この時、結晶tllの回折を生じ
させる面の格子間隔が一様であるならば、湾曲結晶のど
の部分に当ったX線でも、同じグランシングアングルで
回折される。ここで結晶(IIは湾曲しており、結晶の
部分によって水平面に対しである角度金持っている。従
って、グランシングアングルは同じでも、水平面に対し
てはそれぞれ異なる角度の回折波となる。矢印入方向の
加圧により結晶fi+の外部はど、水平面に対しての角
度が大きくなっているので、回折金堂けた後のX線のビ
ームはしぼられたことになる。Next, the operation will be explained. The fourth IN (a
). In FIG. 4(b), a force as indicated by arrow A is applied to the crystal 11+, forming a crystal (1) having a curved surface. When X-rays with a certain divergence angle are incident on the thus curved crystal 11), only the waves that meet the Black condition undergo diffraction. At this time, if the lattice spacing of the diffraction plane of the crystal tll is uniform, X-rays hitting any part of the curved crystal will be diffracted at the same glancing angle. Here, the crystal (II) is curved, and each part of the crystal has a certain angle with respect to the horizontal plane.Therefore, even though the glancing angle is the same, the diffracted waves are at different angles with respect to the horizontal plane.Arrows Due to the pressure applied in the input direction, the angle of the outside of the crystal fi+ with respect to the horizontal plane is increased, so the X-ray beam after passing through the diffraction ring is narrowed down.
従来の湾曲型多層膜光学素子は以上のように、湾・曲結
晶を構成するために平板結晶に加圧していた。従って絶
えず外部から圧力を加え続けなければ湾曲結晶とはなら
なかった。このため、この素子を用いるための装置が複
雑になってしまう。また、精度よく湾曲面を構成するの
は、とても困難であるなどの問題点があった。As described above, in the conventional curved multilayer optical element, a flat crystal is pressed to form a curved/bent crystal. Therefore, a curved crystal could not be formed unless pressure was constantly applied from the outside. Therefore, an apparatus for using this element becomes complicated. Further, there were other problems such as it was very difficult to form a curved surface with high precision.
この発明は上記のような問題点を解消するためになされ
たもので、外部から圧力を加え続けなくても湾曲型の光
学素子を襦成し、かつ精度も向上できる湾曲型多層膜光
学素子を得ることを目的とする。This invention was made to solve the above-mentioned problems, and it provides a curved multilayer optical element that can create a curved optical element without continuously applying pressure from the outside and that can also improve accuracy. The purpose is to obtain.
この発明に係る湾曲型多層膜光学素子は、基板に複数の
金属を、その積層面がそれぞれ凹状になるように、周期
的に積層したものである。The curved multilayer film optical element according to the present invention is one in which a plurality of metals are periodically laminated on a substrate so that the laminated surfaces of the metals each have a concave shape.
この発明にふ・ける多層膜を構成するそれぞれのSμ、
凹状であるため、外部から圧力を加えることなしに湾曲
型結晶が構成される。Each Sμ constituting the multilayer film according to this invention,
Due to the concave shape, a curved crystal can be formed without applying external pressure.
以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例による湾曲型多層膜光学素子を
示す側面図である。図において、(2)は例えば平面を
有するガラスなどの基板であり、(1m)〜(1d)は
それぞれこの基板(21に積層した金属の原子列を示し
ている。この実施例では、4層積層しており、それぞれ
の積層面は凹状を成し、全体としては周期的に構成して
いる。材質は例えば第1層(Ig)、第3@(lc)は
鉄、第211(Ib)。An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure is a side view showing a curved multilayer optical element according to an embodiment of the present invention. In the figure, (2) is a flat substrate such as glass, and (1m) to (1d) respectively indicate the atomic arrays of metal laminated on this substrate (21).In this example, there are four layers. They are laminated, and each laminated surface has a concave shape, and the overall structure is periodic.The materials are, for example, the first layer (Ig), the third @ (lc) is iron, and the second layer (Ib). .
第4層(1d)はマグネシウムであり、それぞれ第21
1 (lb) 〜第4 II (ld) HIOA程艮
ノ層厚で均一に構成している。第1層(1m)は第2層
(1b)〜第4層(1d)の積1面の凹状を構成するよ
うに、基板(21に凹状に形成されている。積層方法と
しては通常のMBE法やIFB法などで実現できる。The fourth layer (1d) is magnesium, and the 21st layer
1 (lb) to 4th II (ld) HIOA, the layer thickness is uniform. The first layer (1m) is formed in a concave shape on the substrate (21) so as to form a concave shape on one side of the stack of the second layer (1b) to the fourth layer (1d). This can be achieved using the IFB Act or the IFB Act.
また、この積層面の凹形状は、例えば入射させるX線の
波長が0.71Aの時で、シリコン101の反射を利用
するとして計算すると、曲率半径を約103〜104m
fII+程度に構成すれば好ましくなる。In addition, the concave shape of this laminated surface has a radius of curvature of about 103 to 104 m when calculated using reflection from silicon 101 when the wavelength of incident X-rays is 0.71 A, for example.
It is preferable to configure it to approximately fII+.
この光学素子に、ある発散角を有するX線が入射される
と、ブラック条件にあう波だけが回折を受ける。積層面
のそれぞれは凹状をなして湾曲しているので、回折を受
けた後のX線のビームはしぼられたことになる。When X-rays having a certain divergence angle are incident on this optical element, only waves that meet the Black condition undergo diffraction. Since each of the laminated surfaces is concave and curved, the X-ray beam after undergoing diffraction is narrowed.
この実施例では、外部から圧力を加えなくても湾曲した
光学素子が得られ、従来のような加圧装置を必要としな
い。また、湾曲面が光学素子の製造工程で形成されるの
で、各積層面の凹形状、即ち水平面に対する角度は精度
良く形成することができる。In this embodiment, a curved optical element can be obtained without applying pressure from the outside, and a conventional pressure device is not required. Moreover, since the curved surfaces are formed in the manufacturing process of the optical element, the concave shape of each laminated surface, that is, the angle with respect to the horizontal plane can be formed with high precision.
なお、上記実施例は平板形状の基板(2)に、金属を積
層したものであるが、第2図に示すように、あらかじめ
基板f21を凹状の面を有するように形成し、この上に
複数の層(1a)〜(1d)を均一の厚さで積層して、
多層膜の積層面のそれぞれを凹状にすることもできる◇
また、光学素子の使用方法により結晶の各部分で異なる
角度の回折波を得る場合には、第3図に示すように多I
I膜(1M)〜(ld)のそれぞれを異なる膜厚で形成
して8f層面が凹状となるようにしてもよい。In the above embodiment, metal is laminated on a flat plate-shaped substrate (2), but as shown in FIG. 2, the substrate f21 is formed in advance to have a concave surface, and a plurality of The layers (1a) to (1d) are laminated with a uniform thickness,
It is also possible to make each of the laminated surfaces of the multilayer film concave.◇ Also, if you want to obtain diffraction waves at different angles in each part of the crystal depending on the method of using the optical element, you can make the multilayer film concave as shown in Figure 3.
The I films (1M) to (ld) may be formed with different thicknesses so that the 8f layer surface has a concave shape.
また、上記実施例では、4〜5層の金属を積層している
が、実際には基板+21の影響をなくすためには計算で
は100層程直積層する必要がある。Further, in the above embodiment, four to five metal layers are laminated, but in reality, in order to eliminate the influence of the substrate +21, it is calculated that about 100 metal layers need to be directly laminated.
以上のように、この発明によれば、基板に複数の金属を
、その積層面がそれぞれ凹状になるように、同期的に積
層することにより、外部から力を加えることなく湾曲型
結晶ft構成でき、精度良く集光9分光することができ
る湾曲型多層膜光学素子を得ることができる効果がある
。As described above, according to the present invention, by synchronously laminating a plurality of metals on a substrate so that their respective laminated surfaces are concave, a curved crystal FT can be constructed without applying any external force. This has the effect of making it possible to obtain a curved multilayer film optical element that can accurately focus 9 light beams.
第1図はこの発明の一冥施例による湾曲型多層膜光学素
子を示す側面図、第2図、第3図はそれぞれこの発明の
他の実施例による湾曲型多1ffi1膜光学素子を示す
側面図、第4図(8) l (b)は従来の74曲型多
層膜光学素子を示す側面図である。
(1a)〜(1d)・・・金属、(2)・・・基板。
なお、図中、同一符号は同一、または相当部分を示す。
第1図
第2図
1、小i!1;の表示
平
特願叫1−38667号
発明の名称
湾曲型多層暎光学素子
3、補正をする者
代表者
第4図
(b)
5、補正の対象
明細書の発明の詳細な説明の欄及び図面。
6、補正の内容
(1)明細書第1頁第20行〜第2頁第1行の「それぞ
れ〜有するものである。」を「ある結晶面を模式的に表
したものである。」に訂正する。
(2)図面の第4図を別紙のとおり訂正する。
7、 添付書類の目録
図面(第4図) 1通以 上FIG. 1 is a side view showing a curved multilayer optical element according to one embodiment of the present invention, and FIGS. 2 and 3 are side views showing curved multilayer optical elements according to other embodiments of the invention. FIG. 4(8)l(b) is a side view showing a conventional 74-curve multilayer film optical element. (1a) to (1d)...metal, (2)...substrate. In addition, in the figures, the same reference numerals indicate the same or equivalent parts. Figure 1 Figure 2 Figure 1, Small i! 1; Indication of Patent Application No. 1-38667 Name of the invention Curved multilayer optical element 3 Representative of the person making the amendment Figure 4 (b) 5. Detailed description of the invention in the specification to be amended and drawings. 6. Contents of amendment (1) From page 1, line 20 to page 2, line 1 of the specification, "each has..." was changed to "schematically represents a certain crystal plane." correct. (2) Figure 4 of the drawings will be corrected as shown in the attached sheet. 7. Attached document catalog drawing (Figure 4) 1 copy or more
Claims (1)
ように、周期的に積層した湾曲型多層膜光学素子。A curved multilayer optical element in which a plurality of metals are periodically laminated on a substrate so that each layer has a concave surface.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1038667A JPH02217801A (en) | 1989-02-17 | 1989-02-17 | Optical element consisting of multilayered films of curved type |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1038667A JPH02217801A (en) | 1989-02-17 | 1989-02-17 | Optical element consisting of multilayered films of curved type |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02217801A true JPH02217801A (en) | 1990-08-30 |
Family
ID=12531624
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1038667A Pending JPH02217801A (en) | 1989-02-17 | 1989-02-17 | Optical element consisting of multilayered films of curved type |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02217801A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP1367605A1 (en) * | 2001-04-27 | 2003-12-03 | Nikon Corporation | Multilayer-film reflective mirrors and optical systems comprising same |
| JP2007011403A (en) * | 1999-11-29 | 2007-01-18 | X-Ray Optical Systems Inc | Doubly curved optical device with graded atomic plane |
-
1989
- 1989-02-17 JP JP1038667A patent/JPH02217801A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007011403A (en) * | 1999-11-29 | 2007-01-18 | X-Ray Optical Systems Inc | Doubly curved optical device with graded atomic plane |
| EP1367605A1 (en) * | 2001-04-27 | 2003-12-03 | Nikon Corporation | Multilayer-film reflective mirrors and optical systems comprising same |
| US6833223B2 (en) | 2001-04-27 | 2004-12-21 | Nikon Corporation | Multilayer-film reflective mirrors and optical systems comprising same |
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