JPH0421122B2 - - Google Patents

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Publication number
JPH0421122B2
JPH0421122B2 JP19985786A JP19985786A JPH0421122B2 JP H0421122 B2 JPH0421122 B2 JP H0421122B2 JP 19985786 A JP19985786 A JP 19985786A JP 19985786 A JP19985786 A JP 19985786A JP H0421122 B2 JPH0421122 B2 JP H0421122B2
Authority
JP
Japan
Prior art keywords
light
light spot
photoelectric conversion
plate
incident position
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
Application number
JP19985786A
Other languages
Japanese (ja)
Other versions
JPS6355406A (en
Inventor
Takao Tawara
Jun Aketo
Yoshuki Iwashita
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
OPUTO EREKUTORONIKUSU KK
Original Assignee
OPUTO EREKUTORONIKUSU KK
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by OPUTO EREKUTORONIKUSU KK filed Critical OPUTO EREKUTORONIKUSU KK
Priority to JP19985786A priority Critical patent/JPS6355406A/en
Publication of JPS6355406A publication Critical patent/JPS6355406A/en
Publication of JPH0421122B2 publication Critical patent/JPH0421122B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、光スポツトが放射線の入射位置を検
出するための光スポツト等の入射位置検出装置に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an incident position detection device for a light spot or the like for detecting the incident position of radiation by a light spot.

[従来の技術] 従来から、光スポツト等の入射位置を検出する
二次元検出装置としては、撮像管やCCD(電荷結
合素子)等が知られているが、何れも価格が高価
となり処理回路が複雑である。
[Prior Art] Conventionally, image pickup tubes and CCDs (charge-coupled devices) have been known as two-dimensional detection devices for detecting the incident position of light spots, etc., but both are expensive and require processing circuits. It's complicated.

本出願人は既に特願昭60−274499号において、
二次発光体を含有する板体を用いて、その入射位
置を検出する装置を提案したが、この場合は一次
元又は多数個の光電変換素子を必要とした。
The applicant has already stated in Japanese Patent Application No. 60-274499,
We have proposed a device that detects the incident position of a plate containing a secondary light emitter, but in this case one-dimensional or multiple photoelectric conversion elements are required.

[発明の目的] 本発明の目的は、更に簡易な構成により、光ス
ポツト等の入射位置を検出し得る光スポツト等の
入射位置検出装置を提供することにある。
[Object of the Invention] An object of the present invention is to provide an incident position detection device for a light spot, etc., which can detect the incident position of a light spot, etc., with a simpler configuration.

[発明の概要] 上述の目的を達成するための本発明の要旨は、
二次発光体又は散乱材を含有する透明又は半透明
の板体の端面に密着して、同様に二次発光体又は
散乱材を含有する透明又は半透明の細条部材を配
置し、該細条部材の少なくとも一方の端部に光電
変換素子を配置し、前記板体の表面に光スポツト
又は放射線を入射させて、前記板体内で発生する
二次光又は散乱光を前記細条部材に導いて再び二
次元又は散乱光を発生させ、前記光電変換素子で
得られた光強度から前記光スポツト又は放射線の
入射位置を検出することを特徴とする光スポツト
等の入射位置検出装置である。
[Summary of the invention] The gist of the present invention for achieving the above object is as follows:
A transparent or translucent strip member also containing a secondary luminescent material or a scattering material is disposed in close contact with the end face of a transparent or translucent plate containing a secondary luminous material or a scattering material, and A photoelectric conversion element is arranged at at least one end of the strip member, a light spot or radiation is made incident on the surface of the plate member, and secondary light or scattered light generated within the plate member is guided to the strip member. This is an incident position detection device for a light spot or the like, characterized in that it generates two-dimensional or scattered light again and detects the incident position of the light spot or radiation from the light intensity obtained by the photoelectric conversion element.

[発明の実施例] 本発明を図示の実施例に基づいて詳細に説明す
る。
[Embodiments of the Invention] The present invention will be described in detail based on illustrated embodiments.

第1図において、1は蛍光剤を含有する例えば
合成樹脂から成る透明又は半透明の板体である。
この板体1の各端面1a〜1dには、同様に蛍光
剤を含有し、透明又は半透明の合成樹脂から成る
細条部材2a〜2dが密着されている。そして、
これらの細条部材2a〜2dの端部には、例えば
太陽電池等から成る光電変換素子3a,3a′,3
b,3b′,…,3d′がそれぞれ取り付けられてお
り、これらの光電変換素子3a,3a′,3b,3
b′,…,3d′の出力は図示しない演算処理回路に
入力されている。
In FIG. 1, reference numeral 1 is a transparent or translucent plate made of, for example, synthetic resin and containing a fluorescent agent.
Strip members 2a to 2d made of transparent or translucent synthetic resin and containing a fluorescent agent are closely attached to each end surface 1a to 1d of the plate 1. and,
At the ends of these strip members 2a to 2d, photoelectric conversion elements 3a, 3a', 3 made of, for example, solar cells are installed.
b, 3b',..., 3d' are attached respectively, and these photoelectric conversion elements 3a, 3a', 3b, 3
The outputs of b', . . . , 3d' are input to an arithmetic processing circuit (not shown).

ここで、板体1の表面に光スポツトSが入射す
ると、この光スポツトSにより板体1中の蛍光剤
が励起されてランダムな方向に蛍光を発し、この
蛍光は板体1中を伝播して各端面1a〜1dに到
達する。この場合に、蛍光は板体1を伝播中に減
衰され、各端面1a〜1dのそれぞれの位置の光
強度は、光スポツトSまでの距離に依存して単調
増加又は減少することになる。端面1a〜1dか
ら出射された蛍光は、細条部材2a〜2dにそれ
ぞれ入射し、細条部材2a〜2d中に含まれる蛍
光剤により再びランダムな方向に発光し、細条部
材2a〜2d中を伝播し、その両端部に配置され
た光電変換素子3a,3a′,…,3d′に入射す
る。
Here, when the light spot S is incident on the surface of the plate 1, the fluorescent agent in the plate 1 is excited by the light spot S and emits fluorescence in random directions, and this fluorescence propagates through the plate 1. and reaches each end face 1a to 1d. In this case, the fluorescence is attenuated while propagating through the plate 1, and the light intensity at each position of each end face 1a to 1d monotonically increases or decreases depending on the distance to the light spot S. The fluorescence emitted from the end faces 1a to 1d enters the strip members 2a to 2d, respectively, and is emitted again in a random direction by the fluorescent agent contained in the strip members 2a to 2d. propagates and enters the photoelectric conversion elements 3a, 3a', . . . , 3d' arranged at both ends thereof.

この場合に、蛍光剤は例えば約500nmを中心
とする波長帯域の光を吸収して、約600nmを中
心とする波長帯域の光を発光するものであり、板
体1から出射する波長帯域の光を細条部材2a〜
2dの蛍光剤が吸収する関係にあることが望まし
い。従つて、板体1に含まれる蛍光剤と細条部材
2a〜2d中に含まれる蛍光剤とは異なる種類と
することが好適である。
In this case, the fluorescent agent absorbs light in a wavelength band centered on about 500 nm and emits light in a wavelength band centered on about 600 nm, and the light in the wavelength band emitted from the plate 1 The strip member 2a~
It is desirable that the fluorescent agent 2d is in an absorbing relationship. Therefore, it is preferable that the fluorescent agent contained in the plate 1 and the fluorescent agent contained in the strip members 2a to 2d be of different types.

第1図のX方向の光スポツトSの位置を求める
ためには、X方向に配置した2つの細条部材2
a,2cの端部からの出力の割合、例えば光電変
換素子3aと3a′の出の和と、光電変換素子3c
と3c′の出力の和の比を求めることにより、板体
1の表面上における光スポツトSのX方向の位置
を入射光量に関係なく求めることができる。
In order to find the position of the light spot S in the X direction in FIG.
The ratio of output from the ends of photoelectric conversion elements 3a and 3a', for example, the sum of the outputs of photoelectric conversion elements 3a and 3a', and the output of photoelectric conversion element 3c
By determining the ratio of the sum of the outputs of and 3c', the position of the light spot S on the surface of the plate 1 in the X direction can be determined regardless of the amount of incident light.

即ち、板体1の辺の長さをD、光スポツトSか
ら端面1aまでの最短距離をxとすると、細条部
材2a,2cを介して光電変換素子3a,3a′,
3c,3c′で得られる蛍光の光強度による出力
Pa,Pcはそれぞれ、 Pa=K/f(x) Pc=K/{D−f(x)} となる。ここで、Kは光スポツトSの光強度・大
きさ、蛍光剤の光変換効率、板体1、細条部材2
中の蛍光減衰率に依存する定数である。このと
き、両光電変換素子3a,3a′,3c,3c′の出
力の和Pa+Pcと差Pa−Pcをそれぞれ演算し、差
Pa−Pcを和Pa+Pcによつて除算すれば、f(x)
=Pc・D/(Pa+Pc)となり、f(x)は予め
特性を求めておくことができるので、光スポツト
Sの光強度等によらずに距離xを求めることが可
能となる。
That is, if the length of the side of the plate 1 is D, and the shortest distance from the light spot S to the end surface 1a is x, then the photoelectric conversion elements 3a, 3a',
Output based on fluorescence light intensity obtained at 3c and 3c'
Pa and Pc are respectively Pa=K/f(x) Pc=K/{D-f(x)}. Here, K is the light intensity and size of the light spot S, the light conversion efficiency of the fluorescent agent, the plate 1, the strip member 2
is a constant that depends on the fluorescence decay rate in At this time, calculate the sum Pa + Pc and the difference Pa - Pc of the outputs of both photoelectric conversion elements 3a, 3a', 3c, 3c', and
If Pa−Pc is divided by the sum Pa+Pc, f(x)
=Pc·D/(Pa+Pc), and since the characteristics of f(x) can be determined in advance, it is possible to determine the distance x without depending on the light intensity of the light spot S, etc.

なお、この場合の板体1の端面からの出力特性
は、第2図aに示すように光スポツトSが板体1
の中央部に位置するほど出力が大きい傾向にあ
る。一方、細条部材2に同じ光量で入射した蛍光
を両端部の光電変換素子3で検出しその和をとる
と、第2図bに示すように光量の減衰のために中
央部への入射量ほど小さくなる。従つて、最終的
には両者の曲線は相殺されて、両端部の光電変換
素子3から得られる出力は第2図cに示すように
ほぼ平担となる。
Note that the output characteristics from the end face of the plate 1 in this case are as shown in FIG.
There is a tendency for the output to be larger as the position is closer to the center of the area. On the other hand, when the fluorescence incident on the strip member 2 with the same amount of light is detected by the photoelectric conversion elements 3 at both ends and the sum is calculated, as shown in Figure 2b, the amount of light incident on the center part is reduced due to the attenuation of the light amount. The smaller it becomes. Therefore, both curves eventually cancel each other out, and the outputs obtained from the photoelectric conversion elements 3 at both ends become almost flat as shown in FIG. 2c.

また、Y方向についても2つの細条部材2b,
2dの端面に設けた光電変換素子3b,3b′,3
d,3d′の出力から光スポツトSの位置を同様に
求めることができ、X方向と併せて二次元的な光
スポツトSの位置を検出することが可能である。
Also, in the Y direction, two strip members 2b,
Photoelectric conversion elements 3b, 3b', 3 provided on the end face of 2d
The position of the light spot S can be similarly determined from the outputs of d and 3d', and it is possible to detect the two-dimensional position of the light spot S together with the X direction.

なお第1図においては、板体1の光スポツトS
の位置を細条部材2a,2cに投影し、光電変換
素子3aと3a′の出力の比又は光電変換素子3c
と3c′の出力の比によつて光スポツトSのY方向
の位置を求めることができる。
In FIG. 1, the light spot S on the plate 1 is
The position of
The position of the light spot S in the Y direction can be determined by the ratio of the outputs of 3c' and 3c'.

前述したように、光スポツトSの入射光の波長
或いは蛍光剤の種類によつて、励起される蛍光の
波長は異なるが、細条部材2に含まれる蛍光材の
励起光のみを透過するフイルタを各光電変換素子
3a,3a′,…,3d′の前面に設ければ、雑音の
影響を無視して精度の良い測定を行うことができ
る。勿論、板体1の表面のみを露出して、その他
は外光から遮断することが望ましいが、完全な暗
箱を形成できない場合には光スポツトSの入射光
を変調して、この変調光に同期した光電変換素子
3a,3a′,3b,3b′,…,3d′からの出力の
みを検出して外光の影響を除去するようにしても
よい。
As mentioned above, the wavelength of the excited fluorescence varies depending on the wavelength of the incident light on the light spot S or the type of fluorescent material, but a filter that transmits only the excitation light of the fluorescent material contained in the strip member 2 is used. If it is provided in front of each photoelectric conversion element 3a, 3a', . Of course, it is desirable to expose only the surface of the plate 1 and block the rest from external light, but if it is not possible to form a complete dark box, the incident light of the light spot S is modulated and synchronized with this modulated light. The influence of external light may be removed by detecting only the outputs from the photoelectric conversion elements 3a, 3a', 3b, 3b', . . . , 3d'.

また第3図においては、板体1の直交する2つ
の端面1a,1bのみにそれぞれ細条部材2a,
2bが配置されており、その端部に設けた光電変
換素子3a,3a′,3b,3b′から光スポツトS
の位置を求めるようにしている。更には、光電変
換素子3は細条部材2の両端に設けるようにして
いるが、入射光の特性が判つていれば片端のみに
設けても測定は可能である。
Further, in FIG. 3, only the two orthogonal end surfaces 1a and 1b of the plate 1 have strip members 2a and 1b, respectively.
2b is arranged, and light spots S are emitted from photoelectric conversion elements 3a, 3a', 3b, 3b' provided at the ends
I am trying to find the position of. Furthermore, although the photoelectric conversion elements 3 are provided at both ends of the strip member 2, measurements can be made even if the photoelectric conversion elements 3 are provided only at one end if the characteristics of the incident light are known.

また、板体1は実施例のような平面ではなく曲
面であつてもよく、球面や円筒形など使用目的に
応じて使い分けることができる。更に、板体1の
表面を粗に加工することにより入射強度を減少さ
せることができるので、表面に粗さ分布を与えて
第2図に示す特性をより直線化することが可能と
なる。
Further, the plate 1 may have a curved surface instead of a flat surface as in the embodiment, and can be selectively used depending on the purpose of use, such as a spherical surface or a cylindrical shape. Furthermore, since the incident intensity can be reduced by roughening the surface of the plate 1, it is possible to give a roughness distribution to the surface and make the characteristics shown in FIG. 2 more linear.

更には、測定対象は必ずしも光スポツトとは限
らず、放射線の点状入射によつても板体1内に光
点を得ることができる。この場合には、板体1内
にはシンチレータを散在しておくことが好まし
い。また、板体1内に混入する材料は、蛍光剤、
シンチレータ以外に、光強度は小さくなるもの
の、単なるアルミニウム粉のような光拡散材を混
入してもよい。
Furthermore, the object to be measured is not necessarily a light spot, and a light spot can also be obtained in the plate 1 by point-like incidence of radiation. In this case, it is preferable that scintillators are scattered within the plate 1. In addition, the materials mixed into the plate 1 include fluorescent agents,
In addition to the scintillator, a light diffusing material such as simple aluminum powder may be mixed, although the light intensity will be reduced.

なお、この光スポツト等の入射位置検出装置の
用途としては、一般に計測装置が考えられるが、
その他には計算機等のデジタイザ入力装置等に使
用することも可能である。また、図形入力であつ
ても時系列的に光スポツトを移動するようにすれ
ば十分に認識できる。
Incidentally, the application of this incident position detection device such as a light spot is generally considered to be a measuring device.
In addition, it can also be used in digitizer input devices for computers and the like. Furthermore, even when inputting figures, it is possible to sufficiently recognize the input by moving the light spot in chronological order.

[発明の効果] 以上説明したように本発明に係る光スポツト等
の入射位置検出装置は、極めて簡素な構成によ
り、光スポツトや放射線の位置を求めることがで
き、従来装置では価格的に不可能な大型の検出装
置も安価に製作することができる。
[Effects of the Invention] As explained above, the device for detecting the incident position of a light spot, etc. according to the present invention has an extremely simple configuration and can determine the position of a light spot or radiation, which is not possible with conventional devices due to the cost. A large-sized detection device can also be manufactured at low cost.

【図面の簡単な説明】[Brief explanation of drawings]

図面は本発明に係る光スポツト等の入射位置検
出装置の実施例を示し、第1図はその斜視図、第
2図aは板体の出力特性図、bは細条部材の出力
特性図、cは総合の出力特性図、第3図は他の実
施例の斜視図である。 符号1は板体、1a〜1dは端面、2a〜2d
は細条部材、3a〜3d′は光電変換素子である。
The drawings show an embodiment of the incident position detection device such as a light spot according to the present invention, and FIG. 1 is a perspective view thereof, FIG. 2a is an output characteristic diagram of a plate, and FIG. c is an overall output characteristic diagram, and FIG. 3 is a perspective view of another embodiment. Code 1 is a plate, 1a to 1d are end faces, 2a to 2d
3 is a strip member, and 3a to 3d' are photoelectric conversion elements.

Claims (1)

【特許請求の範囲】 1 二次発光体又は散乱材を含有する透明又は半
透明の板体の端面に密着して、同様に二次発光体
又は散乱材を含有する透明又は半透明の細条部材
を配置し、該細条部材の少なくとも一方の端部に
光電変換素子を配置し、前記板体の表面に光スポ
ツト又は放射線を入射させて、前記板体内で発生
する二次光又は散乱光を前記細条部材に導いて再
び二次元又は散乱光を発生させ、前記光電変換素
子で得られた光強度から前記光スポツト又は放射
線の入射位置を検出することを特徴とする光スポ
ツト等の入射位置検出装置。 2 前記二次発光体を蛍光剤とした特許請求の範
囲第1項に記載の光スポツト等の入射位置検出装
置。 3 前記板体の相対向する端面に前記細条部材を
配置し、これらの細条部材に配置した前記光電変
換素子の出力の割合から、前記細条部材の長手方
向と直交する方向の入射位置を検出するようにし
た特許請求の範囲第1項に記載の光スポツト等の
入射位置検出装置。 4 前記細条部材の両端部に前記光電変換素子を
配置し、両光電変換素子の出力の割合から、前記
板体の入射位置を前記細条部材に投影し、前記細
条部材の長手方向の入射位置を検出するようにし
た特許請求の範囲第1項に記載の光スポツト等の
入射位置検出装置。
[Scope of Claims] 1. A transparent or translucent strip that also contains a secondary luminous material or a scattering material, in close contact with the end face of a transparent or semitransparent plate containing a secondary luminous material or a scattering material. A member is arranged, a photoelectric conversion element is arranged at at least one end of the strip member, and a light spot or radiation is incident on the surface of the plate, thereby generating secondary light or scattered light inside the plate. is introduced into the strip member to generate two-dimensional or scattered light again, and the incident position of the light spot or radiation is detected from the light intensity obtained by the photoelectric conversion element. Position detection device. 2. An incident position detection device for a light spot or the like according to claim 1, wherein the secondary light emitter is a fluorescent agent. 3. The strip members are arranged on opposite end faces of the plate, and the incidence position in the direction perpendicular to the longitudinal direction of the strip members is determined from the ratio of output of the photoelectric conversion elements arranged on these strip members. An incident position detecting device for a light spot or the like according to claim 1, which detects the incident position of a light spot. 4. Arranging the photoelectric conversion elements at both ends of the strip member, projecting the incident position of the plate onto the strip member from the ratio of the outputs of both photoelectric conversion elements, and calculating the longitudinal direction of the strip member. An incident position detection device for a light spot or the like according to claim 1, which detects an incident position.
JP19985786A 1986-08-26 1986-08-26 Detecting device for incident position of light spot or the like Granted JPS6355406A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19985786A JPS6355406A (en) 1986-08-26 1986-08-26 Detecting device for incident position of light spot or the like

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19985786A JPS6355406A (en) 1986-08-26 1986-08-26 Detecting device for incident position of light spot or the like

Publications (2)

Publication Number Publication Date
JPS6355406A JPS6355406A (en) 1988-03-09
JPH0421122B2 true JPH0421122B2 (en) 1992-04-08

Family

ID=16414805

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19985786A Granted JPS6355406A (en) 1986-08-26 1986-08-26 Detecting device for incident position of light spot or the like

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JP (1) JPS6355406A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3826067A1 (en) * 1988-07-30 1990-02-01 Dornier Gmbh DEVICE FOR FIBER-OPTICAL MEASUREMENT OF ABSOLUTE POSITIONS

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JPS6355406A (en) 1988-03-09

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