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JPH0339570B2 - - Google Patents
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JPH0339570B2 - - Google Patents

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Publication number
JPH0339570B2
JPH0339570B2 JP10325883A JP10325883A JPH0339570B2 JP H0339570 B2 JPH0339570 B2 JP H0339570B2 JP 10325883 A JP10325883 A JP 10325883A JP 10325883 A JP10325883 A JP 10325883A JP H0339570 B2 JPH0339570 B2 JP H0339570B2
Authority
JP
Japan
Prior art keywords
laser beam
incident
circuit
photodetecting
output
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
JP10325883A
Other languages
Japanese (ja)
Other versions
JPS59228131A (en
Inventor
Takahito Hiratsuka
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.)
NEC Corp
Original Assignee
Nippon Electric Co Ltd
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP10325883A priority Critical patent/JPS59228131A/en
Publication of JPS59228131A publication Critical patent/JPS59228131A/en
Publication of JPH0339570B2 publication Critical patent/JPH0339570B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/42Photometry, e.g. photographic exposure meter using electric radiation detectors

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Description

【発明の詳細な説明】 本発明は、レーザ光を検知し、かつレーザ光の
入射方向を知ることができるレーザ光警報装置に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a laser light warning device that can detect laser light and know the direction of incidence of the laser light.

従来、この種のレーザ光覆警報装置は、第1図
で示すように、集光レンズ2の焦点位置に、複数
個の光検知素子5,6,7等をアレイ状に配置し
た構成をもつ光検知素子アレイ3を配置し、個々
の光検知素子5,6,7からの光電流出力を電圧
に変換する電流・電圧変換回路8,9,10等を
もち、この電圧出力をレーザ光か否かを判別する
ためのレベルコンパレータ等から構成される判別
回路11,12,13等を備え、この出力からレ
ーザ光入射したこと及び入射方向を表示する表示
器14,15,16等により構成される。その動
作は、ある入射角θをもつ入射してくるレーザ光
1が、集光レンズ2によりレーザ光1の入射角θ
に応じて光検知素子アレイ3上の集光点4に集光
され、集光点4にある光検知素子6からレーザ光
1の強度に応じた光電流電圧変換回路9に供給さ
れ、電圧出力となるから、判別回路12により、
レーザ光かどうかを判別し、レーザ光であれば表
示器15へ電圧出力を送出し、表示器15によ
り、レーザ光1の入射したことを表示すると共
に、入射角θを表示するものである。
Conventionally, this type of laser beam cover alarm device has a configuration in which a plurality of photodetecting elements 5, 6, 7, etc. are arranged in an array at the focal point of a condensing lens 2, as shown in FIG. A photodetecting element array 3 is arranged, and current/voltage conversion circuits 8, 9, 10, etc. are provided to convert the photocurrent output from the individual photodetecting elements 5, 6, 7 into voltage, and this voltage output is converted into a laser beam. It is equipped with discriminating circuits 11, 12, 13, etc., which are composed of level comparators, etc., for discriminating whether or not the laser beam is present. Ru. The operation is such that the incident laser beam 1 with a certain incident angle θ is
According to the intensity of the laser beam 1, the light is focused on a focusing point 4 on the photodetecting element array 3, and is supplied from the photodetecting element 6 at the focusing point 4 to a photocurrent-voltage conversion circuit 9 according to the intensity of the laser beam 1, which outputs a voltage. Therefore, the discrimination circuit 12
It is determined whether it is a laser beam or not, and if it is a laser beam, a voltage output is sent to the display 15, and the display 15 indicates that the laser beam 1 has entered and also displays the incident angle θ.

上述の様に構成されたレーザ光警報装置におい
ては、過大な入射強度をもつレーザ光が入射した
場合は、集光レンズ2によつて光検知素子アレイ
3上の集光点4に高強度のレーザ光が集光され過
大な入射強度のために、集光点4にある光検知素
子6に隣接する光検知素子5及び7にクロストー
ク(漏洩)が発生し、あたかも光検知素子5及び
7にもレーザ光が入射されたと同じように、電流
電圧変換素子8及び10により、電圧出力が判別
回路11及び13に送られ、さらに表示器14及
び16によりレーザ光が入射したと表示してしま
い、実際にレーザ光が入射してきた入射角θを正
確に知ることができないという欠点があつた。
In the laser beam warning device configured as described above, when a laser beam with excessive incident intensity is incident, the condensing lens 2 emits high intensity light to the condensing point 4 on the photodetecting element array 3. Because the laser beam is focused and the incident intensity is excessive, crosstalk (leakage) occurs in the photodetecting elements 5 and 7 adjacent to the photodetecting element 6 at the condensing point 4, as if the photodetecting elements 5 and 7 In the same way as if a laser beam was incident on the sensor, the current-voltage conversion elements 8 and 10 send the voltage output to the discrimination circuits 11 and 13, and the displays 14 and 16 display that the laser beam has entered the sensor. However, there was a drawback in that it was not possible to accurately determine the incident angle θ at which the laser beam actually entered.

さらに、前記過大な入射強度をもつレーザ光が
集光レンズ2によつて光検知素子アレイ3上の集
光点4に集光され、集光された光が光検知素子の
表面上で反射し、この反射光が集光レンズ2によ
りさらに光検知素子アレイ3の方向に反射され、
再度、光検知素子アレイ3上の光検知素子に入射
し、この入射に応じて光電流出力が電流電圧変換
素子に送られ、電圧出力に変換されて判別回路に
より、レーザ光と判別され、表示器によりレーザ
光が入射してきたことと共に入射方向を表示して
しまい、実際の入射角θを正確に知ることができ
なくなるという欠点があつた。
Furthermore, the laser beam with excessive incident intensity is focused by the condenser lens 2 onto a condensing point 4 on the photodetecting element array 3, and the focused light is reflected on the surface of the photodetecting element. , this reflected light is further reflected in the direction of the photodetector array 3 by the condenser lens 2,
The light enters the photodetecting element on the photodetecting element array 3 again, and in response to this incident, the photocurrent output is sent to the current-voltage conversion element, where it is converted to voltage output, which is discriminated by the discrimination circuit as laser light, and displayed. The device displays the incident direction of the laser beam as well as the incident direction, making it impossible to accurately determine the actual incident angle θ.

本発明の目的は、前記欠点を解決し、微小な入
差強度から過大な入射強度までのレーザ光の入射
方向を正確に表示することができるレーザ光警報
装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a laser beam warning device that can solve the above-mentioned drawbacks and accurately display the incident direction of laser beams ranging from minute incident intensity to excessive incident intensity.

本発明は、複数個の光検知素子をアレイ状に配
置し、これを集光レンズと組合わせてレーザ光の
入射角に応じて、前記アレイ上に配置された光検
知素子の一つに集光させ、前記光検知素子からの
光電流出力を個々の光検知素子に個有の分配比率
によつて2つの出力に分割し、前記2つの出力か
ら、光電流出力の分配比率を求めることによつて
レーザ光の入射受強度に関係なく、レーザ光の入
射角を求めるように構成される。
The present invention involves arranging a plurality of photodetecting elements in an array, combining these with a condensing lens, and focusing the laser beam on one of the photodetecting elements arranged on the array according to the incident angle of the laser beam. emitting light, dividing the photocurrent output from the photodetecting element into two outputs according to a distribution ratio unique to each photodetecting element, and determining the distribution ratio of the photocurrent output from the two outputs. Therefore, the configuration is such that the incident angle of the laser beam is determined regardless of the incident and received intensity of the laser beam.

本発明の実施例を図面を参照しながら説明す
る。
Embodiments of the present invention will be described with reference to the drawings.

第2図は、本発明の一実施令を示す構成ブロツ
ク図である。
FIG. 2 is a block diagram showing one implementation of the present invention.

本発明のレーザ光警報装置は、集光レンズ2と
光検知素子アレイ3とインピーダンス素子17,
18,19,20,21等と、電流電圧変換回路
22及び23と判別回路24及び25と、加算回
路26と減算回路27及び30と対数増幅回路2
8及び29と表示回路31とから構成される。
The laser beam alarm device of the present invention includes a condensing lens 2, a photodetecting element array 3, an impedance element 17,
18, 19, 20, 21, etc., current-voltage conversion circuits 22 and 23, discrimination circuits 24 and 25, addition circuit 26, subtraction circuits 27 and 30, and logarithmic amplifier circuit 2
8 and 29 and a display circuit 31.

光検知素子アレイ3は、複数個の光検知素子
5,6,7等をアレイ状に配置したものであり、
インピーダンス素子17,18,19,20,2
1等は、抵抗単体又は抵抗、インダクタンス、キ
ヤパシタンスにより構成され、同一のインピーダ
ンスをもち、各光検知素子5,6,7等の出力を
結合し、個々の光検知素子に個有の分配比率によ
つて光電流出力を分割し、電流電圧変換回路22
及び23へ供給するものである。判別回路は、レ
ベルコンパレータ等から構成され、電流電圧変換
回路22及び23の電圧出力がレーザ光か否かを
判別するものである。加算回路26と減算回路2
7とは超短パルス光のときの判別回路24及び2
5の出力から和信号出力と差信号出力を計算し、
それぞれの出力を複数増幅回路28及び29に供
給する。減算回路30は、この対数増幅回路28
及び29の出力から差信号出力を和信号出力で割
算をし、レーザ光の入射した光検知素子に相当す
る電圧出力を得る。表示回路31はピークホール
ド回路を有し、この減算回路30の電圧出力によ
つて、レーザ光の入射と入射方向を表示する。
The photodetecting element array 3 is a plurality of photodetecting elements 5, 6, 7, etc. arranged in an array.
Impedance elements 17, 18, 19, 20, 2
The first element is composed of a single resistor or a resistor, inductance, and capacitance, has the same impedance, and combines the outputs of each photodetector element 5, 6, 7, etc., to a distribution ratio unique to each photodetector element. Therefore, the photocurrent output is divided and the current-voltage conversion circuit 22
and 23. The determination circuit includes a level comparator and the like, and determines whether the voltage outputs of the current-voltage conversion circuits 22 and 23 are laser beams. Addition circuit 26 and subtraction circuit 2
7 is the discrimination circuit 24 and 2 for ultra-short pulse light.
Calculate the sum signal output and difference signal output from the output of 5,
The respective outputs are supplied to multiple amplifier circuits 28 and 29. The subtraction circuit 30 is a logarithmic amplifier circuit 28
From the outputs of 29 and 29, the difference signal output is divided by the sum signal output to obtain a voltage output corresponding to the photodetector element into which the laser beam is incident. The display circuit 31 has a peak hold circuit, and uses the voltage output of the subtraction circuit 30 to display the incidence and direction of incidence of the laser beam.

いま集光レンズ2に入射角θをもつてレーザ光
が入射したとすると、集光レンズ2によつてレー
ザ光1は、光検知素子アレイ3上の集光点4に集
光される。この集光点4にある光検知素子6は、
入射したレーザ光の入射強度に応じた光電流を出
力する。ここで光検知素子の数をM個とし、イン
ピーダンス素子のインピーダンスをZとすると、
インピーダンス素子は(M+1)個で構成され、
N番目の光検知素子6にレーザ光が入射したとす
ると、インピーダンス素子17,18,19,2
0,21等により番目の光検知素子の光電流出力
が電流電圧変換回路22へはI22電流電圧変換回
路23へはI23と分割される。
Assuming that a laser beam is incident on the condenser lens 2 at an incident angle θ, the condenser lens 2 condenses the laser beam 1 onto a condensing point 4 on the photodetector array 3 . The photodetecting element 6 at this condensing point 4 is
It outputs a photocurrent according to the intensity of the incident laser light. Here, if the number of photodetecting elements is M and the impedance of the impedance element is Z, then
The impedance element is composed of (M+1) pieces,
If the laser beam is incident on the Nth photodetector element 6, the impedance elements 17, 18, 19, 2
0, 21, etc., the photocurrent output of the th photodetector element is divided into I22 to the current-voltage conversion circuit 22 and I23 to the current-voltage conversion circuit 23 .

I22=I・NZ/(M+1)Z=IN/(M+1) I23=I(M+1−N)Z/(M+1)Z =I(M+1−N)/(M+1) これら電流電圧変換回路22及び23への電流
は、電流電圧変換率αによつて電圧出力となる。
電流電圧変換回路22及び23の電圧出力をそれ
ぞれV22及びV23とすると、 V22=αIN/M+1、V23=αIM+1−N/M+
1 となる。この電圧出力が判別回路24及び25を
それぞれ通り、加算回路26及び減算回路27と
に供給される。これら加算回路26電圧出力
VADD、減算回路27の電圧回路27の電圧出力
をVSUBとすると、 VADD=V23+V22=αIM+1−N/M+1 +αIN/M+1=αISUB =V23−V22=αIM+1−N/M+1 −αIN/M+1=αI(1−2N/M+1) となる。これら電圧出力VADDとVSUBとを対数増幅
回路28及び29に通しださらに減算回路30を
通すことにより、減算回路出力は、VSUB/VADD
なる。従つて減算回路30の電圧出力V30は、 V30=VSUB/VADD=αI(1−2N/M+1)/αI=1−2
N/M+1 となる。ここでMは、光検知素子アレイ3の中の
光検知素子5,6,7等の総数であり、Nはレー
ザ光の入射した光検知素子の電流電圧変換回路2
2側から数えた番号であり1からMまで変化す
る。
I 22 = I・NZ/(M+1)Z=IN/(M+1) I 23= I(M+1-N)Z/(M+1)Z =I(M+1-N)/(M+1) These current-voltage conversion circuit 22 and The current to 23 becomes a voltage output depending on the current-voltage conversion rate α.
Assuming that the voltage outputs of the current-voltage conversion circuits 22 and 23 are V 22 and V 23 , respectively, V 22 = αIN/M+1, V 23 = αIM+1-N/M+
It becomes 1. This voltage output passes through discrimination circuits 24 and 25, respectively, and is supplied to an addition circuit 26 and a subtraction circuit 27. These adder circuits 26 voltage output
V ADD and the voltage output of the voltage circuit 27 of the subtraction circuit 27 as V SUB , V ADD = V 23 + V 22 = αIM+1-N/M+1 + αIN/M+1 = αI SUB = V 23 -V 22 = αIM+1-N/M+1 -αIN/M+1=αI(1-2N/M+1). By passing these voltage outputs V ADD and V SUB through the logarithmic amplifier circuits 28 and 29 and further through the subtraction circuit 30, the subtraction circuit output becomes V SUB /V ADD . Therefore, the voltage output V 30 of the subtraction circuit 30 is V 30 = V SUB /V ADD = αI (1-2N/M+1)/αI = 1-2
It becomes N/M+1. Here, M is the total number of photodetecting elements 5, 6, 7, etc. in the photodetecting element array 3, and N is the current-voltage conversion circuit 2 of the photodetecting element on which the laser beam is incident.
This is the number counted from the 2nd side and varies from 1 to M.

この減算回路30の電圧出力V30からレーザ光
の入射強度に関係なく、レーザ光の入射角に応じ
た出力を得ることができ、この出力を表示回路3
1によつて、レーザ光の入射したことと共に、入
射角を表示するものである。
From the voltage output V 30 of this subtraction circuit 30, an output corresponding to the incident angle of the laser beam can be obtained regardless of the incident intensity of the laser beam, and this output is sent to the display circuit 30.
1 indicates that the laser beam is incident and also indicates the angle of incidence.

この方式によれば、過大な入射強度をもつレー
ザ光によつてレーザ光の集光された光検知素子6
に隣接した光検知素子5,7へのクロストーク
(漏洩れ)の影響は、光検知素子6の電流出力の
数%以下であり、隣接する光検知素子5,7へほ
ぼ等分されるために、光検知素子5の電流出力に
よる入射角度の演算誤差と光検知素子7の電流出
力による入射角度の演算誤差とが相殺するように
はたらき、レーザ光の入射角をクロストークの影
響なく正確に知ることができる。又、光検知素子
6の表面上で反射し、集光レンズ2でさらに光検
知素子アレイ3側に反対されて再度入射する光に
ついても、光検知素子6への入射強度の数%以下
の強度となり、ほぼ一様に光検知素子アレイ3上
に入射するのでレーザ光の入射角の演算誤差は非
常に小さいものとなり、従来の方式のレーザ光警
報装置に比べ、正確にレーザ光の入射方向を知る
ことができる。
According to this method, a laser beam having an excessively high incident intensity is used to collect the laser beam on the photodetecting element 6.
The influence of crosstalk (leakage) on the adjacent photodetecting elements 5 and 7 is less than a few percent of the current output of the photodetecting element 6, and the current output is almost equally distributed between the adjacent photodetecting elements 5 and 7. In addition, the calculation error of the incident angle due to the current output of the photodetector element 5 and the calculation error of the incidence angle due to the current output of the photodetector element 7 work to cancel each other out, and the incident angle of the laser beam can be accurately determined without the influence of crosstalk. You can know. Also, regarding the light that is reflected on the surface of the photodetector element 6 and is further directed toward the photodetector array 3 side by the condenser lens 2 and enters again, the intensity is less than a few percent of the intensity that is incident on the photodetector element 6. Since the laser beam is almost uniformly incident on the photodetecting element array 3, the calculation error of the incident angle of the laser beam is very small, and compared to conventional laser beam warning devices, the incident direction of the laser beam can be determined more accurately. You can know.

以上説明したように本発明は、複数の光検知素
子をアレイ状に配置したものを集光レンズと組み
合わせ、レーザ光の入射角合に応じて光検知素子
アレイの中の一つの光検知素子上にレーザ光が集
光され、光検知素子からの光電流出力を個々の光
検知素子に個有の分配比率によつて2つの出力に
分割し、この2つの出力から分配比率を求めるこ
とにより、レーザ光の射強度に関係なく、レーザ
光の入射角を得られる効果を有する。
As explained above, the present invention combines a plurality of photodetecting elements arranged in an array with a condensing lens, and selects one photodetecting element in the photodetecting element array according to the incident angle of the laser beam. The laser beam is focused on the photodetector, the photocurrent output from the photodetector is divided into two outputs according to the distribution ratio unique to each photodetector, and the distribution ratio is determined from these two outputs. This has the effect that the incident angle of the laser beam can be obtained regardless of the intensity of the laser beam.

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

第1図は、従来のレーザ光警報装置の構成を示
すブロツク図、第2図は本発明の一実施例を示す
構成ブロツク図である。 1……レーザ光、2……集光レンズ、3……光
検知素子アレイ、4……集光点、5,6,7……
光検知素子、8,9,10……電流電圧変換回
路、11,12,13……判別回路、14,1
5,16……表示器、17,18,19,20,
21……インピーダンス素子、22,23……電
流電圧変換回路、24,25……判別回路、26
……加算回路、27……減算回路、28,29…
…対数増幅回路、30……減算回路、31……表
示回路。
FIG. 1 is a block diagram showing the structure of a conventional laser beam warning device, and FIG. 2 is a block diagram showing an embodiment of the present invention. 1... Laser light, 2... Condensing lens, 3... Photodetecting element array, 4... Focusing point, 5, 6, 7...
Photodetection element, 8, 9, 10... Current-voltage conversion circuit, 11, 12, 13... Discrimination circuit, 14, 1
5, 16... Indicator, 17, 18, 19, 20,
21... Impedance element, 22, 23... Current voltage conversion circuit, 24, 25... Discrimination circuit, 26
... Addition circuit, 27 ... Subtraction circuit, 28, 29 ...
... Logarithmic amplifier circuit, 30 ... Subtraction circuit, 31 ... Display circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 集光レンズと、複数個の光検知素子がアレイ
状に配置され、前記集光レンズの焦点位置に配置
されるとともに前記集光レンズからの光を受光す
る光検知素子アレイと、この光検知累子アレイ内
の個々の光検知素子からの光電流出力を個々の光
検知素子に固有の分配比率により2つの電流に分
割する手段と、この分割された光電流出力の分配
比率を求める手段と、この求められた比率からレ
ーザ光の到来方向を表示する表示手段とを具備す
ることを特徴としたレーザ光警報装置。
1. A condensing lens, a plurality of photodetecting elements arranged in an array, a photodetecting element array disposed at the focal position of the condensing lens and receiving light from the condensing lens, and this photodetecting element array. means for dividing the photocurrent output from each photodetector in the transducer array into two currents according to a distribution ratio specific to each photodetector; and means for determining the distribution ratio of the divided photocurrent output. , and display means for displaying the direction of arrival of the laser light from the determined ratio.
JP10325883A 1983-06-09 1983-06-09 Laser light warning device Granted JPS59228131A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10325883A JPS59228131A (en) 1983-06-09 1983-06-09 Laser light warning device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10325883A JPS59228131A (en) 1983-06-09 1983-06-09 Laser light warning device

Publications (2)

Publication Number Publication Date
JPS59228131A JPS59228131A (en) 1984-12-21
JPH0339570B2 true JPH0339570B2 (en) 1991-06-14

Family

ID=14349413

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10325883A Granted JPS59228131A (en) 1983-06-09 1983-06-09 Laser light warning device

Country Status (1)

Country Link
JP (1) JPS59228131A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2734530B2 (en) * 1988-06-24 1998-03-30 日本電気株式会社 Laser beam incident direction detector
CN112665532B (en) * 2020-12-15 2022-06-21 中北大学 High-precision laser warning device based on four-quadrant detector and two-dimensional grating

Also Published As

Publication number Publication date
JPS59228131A (en) 1984-12-21

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