JPS60104913A - Condensing device - Google Patents
Condensing deviceInfo
- Publication number
- JPS60104913A JPS60104913A JP21308983A JP21308983A JPS60104913A JP S60104913 A JPS60104913 A JP S60104913A JP 21308983 A JP21308983 A JP 21308983A JP 21308983 A JP21308983 A JP 21308983A JP S60104913 A JPS60104913 A JP S60104913A
- Authority
- JP
- Japan
- Prior art keywords
- light
- condensed
- convex
- light source
- optical axis
- 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
Abstract
Description
【発明の詳細な説明】 本発明は集光装置に関する。[Detailed description of the invention] The present invention relates to a light condensing device.
一般に、事実上点光源と見なし得る、発光表面積の小さ
い光源から所定の拡がりをもって放射される光源を、幅
の狭い平行ビーノ、に集光させるには、レンズ、反射鏡
およびスリット等、複数個の個別の光学エレメントを、
所定の幾何学的条件をホ冒こすよう配列構成した光学系
が用いられる。従っ−にのよ・)な装置では、構成が複
雑となり、また、外部要因により機械的な振動を受ける
ような場合には、光学系を構成する各構成エレメント間
の相対的位置関係に狂いが生じないような構造にしなL
Jればならない。In general, in order to condense a light source emitted with a predetermined spread from a light source with a small light emitting surface area, which can be effectively considered a point light source, onto a narrow parallel beam, it is necessary to use multiple lenses, reflectors, slits, etc. individual optical elements,
Optical systems arranged and configured to violate predetermined geometrical conditions are used. The structure of such a device is complex, and if it is subjected to mechanical vibrations due to external factors, the relative positional relationship between the constituent elements of the optical system may become distorted. Create a structure that will not cause
Must be J.
本発明の目的は、きわめて堅牢な剛体的装置であって、
所定の拡がりをもつ光源の光からきわめて細く且つエネ
ルギ密度の高いビームに集光する装置を提供することに
ある。The object of the invention is an extremely robust rigid device, which
The object of the present invention is to provide a device that condenses light from a light source with a predetermined spread into an extremely narrow beam with high energy density.
上記の目的を達成するため、本発明による集光装置は、
所定の屈折率を有する光学的媒質が、入射光に向って凸
な第1の曲率をもつ入射面と、この入射面の中央部に設
けられ、光を上記媒質内に向って反射する第2の曲率を
もつ凸面反射部と、上記入射面に対向し、第3の曲率を
もつ凹型反射面と、この凹型反射面の中央部に設けられ
、上記凸面反射部の反射光を上記媒質外に透過出力させ
る、直径が上記凸面反射部の直径より小さい光導出口と
を有してなることを特徴としている。In order to achieve the above object, the light condensing device according to the present invention comprises:
An optical medium having a predetermined refractive index is provided with an entrance surface having a first curvature convex toward the incident light, and a second entrance surface provided at the center of the entrance surface and reflecting the light toward the inside of the medium. a convex reflecting section having a curvature of , a concave reflecting surface facing the incident surface and having a third curvature; It is characterized in that it has a light guide port whose diameter is smaller than the diameter of the convex reflecting section, through which the light is transmitted and output.
以下に本発明を図面に基づいて説明する。The present invention will be explained below based on the drawings.
図において、厚内凸レンズ状の形態を有する光学ガラス
1には、一方の側の凸面の光の入射面2とし、その中央
部に、光軸6を中心として、光をガラス内に反射するよ
う鏡面処理された、反射面がガラス内に向う凸面反射部
3が設りられでおり、また、入射面2に対向する例の凸
面には光軸6を中心とし所望の径を有する先取出口5の
部分を除いて、その表面に鏡面処理が施こされてガラス
内に反射面を向りた凹面鏡4が形成されている。入射面
2は焦点距離f1の球面(曲率半径2f+)、凸面反射
部3は焦点距離r2の球面(曲率半径2f2)、凹面鏡
4は焦点能Flu f aの球面(曲率半径2f3)で
ある。また、この凹面鏡4の焦点Aと上記凸型反射部3
の焦点Δは一致し、先取出口5のガラス面は、光軸6に
直交する平面となっ°ζいる。また、凸型反射部3の直
径は凹面鏡4で反則されて焦点へに向う光がずバー0反
射される大きさに選定される。In the figure, an optical glass 1 having the shape of a convex lens has a convex light incident surface 2 on one side, and a convex light incident surface 2 at the center of the optical glass 1 to reflect light into the glass with an optical axis 6 as the center. A mirror-treated convex reflecting portion 3 whose reflecting surface faces into the glass is provided, and a pre-extraction port 5 having a desired diameter centered on the optical axis 6 is provided on the convex surface facing the incident surface 2. A concave mirror 4 is formed inside the glass, with the exception of the portion shown in FIG. The entrance surface 2 is a spherical surface with a focal length f1 (radius of curvature 2f+), the convex reflecting section 3 is a spherical surface with a focal length r2 (radius of curvature 2f2), and the concave mirror 4 is a spherical surface with a focal power Flu fa (radius of curvature 2f3). Also, the focal point A of this concave mirror 4 and the convex reflecting section 3
The focal points Δ coincide with each other, and the glass surface of the pre-extraction port 5 becomes a plane perpendicular to the optical axis 6 . Further, the diameter of the convex reflecting portion 3 is selected to be such that the light reflected by the concave mirror 4 and directed toward the focal point is reflected.
次に使用方法と作用を説明する。入射面2の焦点Pに、
例えばL E D等の光源を置く。光源■)より放射さ
れた光線は、入射面2で屈折されて、光軸6に平行な光
線としてガラス内に入射する。この平行光線は凹型反射
面4により凸型反射部3に向って反射集光される。凸型
反射部3は、そこに集光されてくる光を再び平行光線と
して光取出口5に向って反射する。このようにして面4
と面3の反射が複数回くり返されながら光は光軸に向っ
て集光される。やがて、光取出口5の直径にまで集光さ
れた光は先取出口5を透過して外部へ放出されろ。Next, how to use it and its effects will be explained. At the focal point P of the entrance plane 2,
For example, place a light source such as an LED. The light rays emitted from the light source ① are refracted at the entrance surface 2 and enter the glass as rays parallel to the optical axis 6. These parallel light rays are reflected and focused by the concave reflective surface 4 toward the convex reflective section 3 . The convex reflecting section 3 reflects the light condensed thereon toward the light extraction port 5 again as parallel rays. In this way, surface 4
The light is focused toward the optical axis while being reflected by the surface 3 a plurality of times. Eventually, the light that has been focused to the diameter of the light extraction port 5 passes through the pre-extraction port 5 and is emitted to the outside.
変形実施例として、先取出口5のガラス面を光軸6に対
して斜交する平面とするときは、凸面反射部3によって
平行化された光線束は、光軸6にff1l交する方向に
取り出される。As a modified example, when the glass surface of the pre-extraction port 5 is made into a plane obliquely intersecting the optical axis 6, the beam parallelized by the convex reflection section 3 is extracted in the direction ff1l intersecting the optical axis 6. It will be done.
本発明によれば、先取出口5を所望の形状、寸法に選ぶ
ことにより、所望の断面形状、所望の大きさに集光され
た光ビームをjηることができる。According to the present invention, by selecting the pre-extraction port 5 to have a desired shape and size, it is possible to obtain a light beam that is focused in a desired cross-sectional shape and a desired size.
しかも、全体は1個の剛体で構成されるので、堅牢かつ
安価に製作3゛ることができる。従って、LED、ラン
プ等の容易に入手できる光源を用いて、または色フィル
タの併用により、所望の波長特性をもつ強いエネルギ密
度の光束を得ることができる。Furthermore, since the entire structure is made up of one rigid body, it can be manufactured robustly and inexpensively. Therefore, by using easily available light sources such as LEDs and lamps, or by using color filters in combination, it is possible to obtain a luminous flux with a strong energy density and desired wavelength characteristics.
図面は本発明の実施例の構成図である。 1・・・厚肉凸レンズ状ガラス体 2・・・入射面 3・・・凸面反射部 4・・・凹面反射鏡 5・・・光取出口6・・・光軸 特許出願人 日本レーザ光学株式会社 代 理 人 弁理士 西1) 新 The drawings are configuration diagrams of embodiments of the present invention. 1... Thick convex lens-shaped glass body 2...Incidence surface 3...Convex reflection part 4... Concave reflector 5... Light extraction port 6... Optical axis Patent applicant: Nippon Laser Optics Co., Ltd. Representative Patent Attorney Nishi 1) New
Claims (1)
な第1の曲率をもつ入射面と、この入射面の中央部に設
けられ、光を上記媒質内に向って反射する第2の曲率も
つ凸面反射部と、上記入射面に対向し、第3の曲率をも
つ凹型反射面と、この凹型反射面の中央部に設けられ、
上記凸面反射部の反射光を上記媒質外に透過出力させる
、直径が上記凸面反射部の直径より小さい光導出口とを
有してなる集光装置。An optical medium having a predetermined refractive index is provided with an entrance surface having a first curvature convex toward the incident light, and a second entrance surface provided at the center of the entrance surface and reflecting the light toward the inside of the medium. a convex reflective part having a curvature of , a concave reflective surface facing the incident surface and having a third curvature, and a concave reflective surface provided at the center of the concave reflective surface,
and a light guide port having a diameter smaller than the diameter of the convex reflector, which transmits and outputs the reflected light from the convex reflector to the outside of the medium.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21308983A JPS60104913A (en) | 1983-11-11 | 1983-11-11 | Condensing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21308983A JPS60104913A (en) | 1983-11-11 | 1983-11-11 | Condensing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60104913A true JPS60104913A (en) | 1985-06-10 |
Family
ID=16633372
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21308983A Pending JPS60104913A (en) | 1983-11-11 | 1983-11-11 | Condensing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60104913A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63313329A (en) * | 1987-06-11 | 1988-12-21 | フィリップス エレクトロニクス ネムローゼ フェンノートシャップ | Scanner |
-
1983
- 1983-11-11 JP JP21308983A patent/JPS60104913A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63313329A (en) * | 1987-06-11 | 1988-12-21 | フィリップス エレクトロニクス ネムローゼ フェンノートシャップ | Scanner |
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