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JPH0135306B2 - - Google Patents
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JPH0135306B2 - - Google Patents

Info

Publication number
JPH0135306B2
JPH0135306B2 JP58243388A JP24338883A JPH0135306B2 JP H0135306 B2 JPH0135306 B2 JP H0135306B2 JP 58243388 A JP58243388 A JP 58243388A JP 24338883 A JP24338883 A JP 24338883A JP H0135306 B2 JPH0135306 B2 JP H0135306B2
Authority
JP
Japan
Prior art keywords
light
correction
optical
measurement
modulated
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
JP58243388A
Other languages
Japanese (ja)
Other versions
JPS60133381A (en
Inventor
Koji Tsuda
Shinichi Suzuki
Atsumi Kaneko
Toshifumi Kanema
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.)
Pentax Corp
Original Assignee
Asahi Kogaku Kogyo 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 Asahi Kogaku Kogyo Co Ltd filed Critical Asahi Kogaku Kogyo Co Ltd
Priority to JP58243388A priority Critical patent/JPS60133381A/en
Publication of JPS60133381A publication Critical patent/JPS60133381A/en
Publication of JPH0135306B2 publication Critical patent/JPH0135306B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481Constructional features, e.g. arrangements of optical elements

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Description

【発明の詳細な説明】 本発明は光波を用いて距離を測定する光波測距
装置の光学的構造に関するものである。光波測距
装置は周知のように、ある規定の周波数で変調さ
れた発光ダイオード等の発光素子からの光を送光
光学系を用いて測点に置かれたコーナーキユーブ
等の反射器に向けて放射し、該反射器より返され
た光を受光光学系を用いて受光素子に結像させ、
電気信号に変換し、基準変調光に対する反射変調
光の位相遅れを検出することによつて距離を測定
する装置である。この様な光波測距装置の場合、
距離の測定誤差は重要な性能上の問題であり、そ
の誤差に起因するものに光学的原因や電気的原因
が種々存在する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical structure of a light wave distance measuring device that measures distance using light waves. As is well known, a light wave ranging device uses a light transmitting optical system to direct light from a light emitting element such as a light emitting diode that is modulated at a certain specified frequency to a reflector such as a corner cube placed at a measurement point. emit the light, and image the light returned from the reflector on a light-receiving element using a light-receiving optical system;
This is a device that measures distance by converting the reflected modulated light into an electrical signal and detecting the phase delay of the reflected modulated light with respect to the reference modulated light. In the case of such a light wave ranging device,
Distance measurement error is an important performance problem, and there are various optical and electrical causes for this error.

本発明は前記の光学的原因のうち発光部の位相
むらによる影響を除去し、測定誤差を小さくする
光学的構造に関するものである。
The present invention relates to an optical structure that eliminates the influence of phase unevenness of a light emitting section among the optical causes and reduces measurement errors.

通常、光波測距装置においては、装置内の光路
長及び電子回路部の位相ずれに基く測定誤差を補
正するために、測定光とは別に補正光を設けてい
るが、この補正光のとらえ方として発光部の光軸
付近の放射光を利用する測定光とは異なり、光軸
より大きくはなれた放射角度範囲の光を使用する
方法が機構上よくとられる。しかしこの場合放射
角度のちがいにより位相むらがあると、測定光と
補正光の位相差が、光路の機械的な設定位置の経
時変化又は発光素子の温度特性により変化するこ
とによつて、距離の測定誤差が大きくなるという
問題がある。そして、この位相むらは、光波測距
装置からの出射光が大きくとれる点で非常に有効
な高指向性形の発光素子においては、光軸付近で
位相むらは小さく許容できる範囲であるが、光軸
より大きくはなれた放射角度においては、角度に
対する位相むらが非常に大きい傾向にある。
Normally, in a light wave distance measuring device, a correction light is provided separately from the measurement light in order to correct measurement errors based on the optical path length within the device and the phase shift of the electronic circuit section, but how to capture this correction light. Unlike measurement light that uses emitted light near the optical axis of the light emitting section, a method that uses light in a range of emitted angles that are far away from the optical axis is often used mechanically. However, in this case, if there is phase unevenness due to a difference in the radiation angle, the phase difference between the measurement light and the correction light will change over time due to the mechanical setting position of the optical path or the temperature characteristics of the light emitting element, which will cause the distance to change. There is a problem that the measurement error increases. This phase unevenness is small and within an acceptable range near the optical axis in a highly directional type light emitting element, which is very effective in that a large amount of light can be emitted from a light wave ranging device. At radiation angles that are far from the axis, phase unevenness with respect to angle tends to be very large.

前記放射角度に対する位相むらの影響を減少さ
せるための従来の方法としては、発光素子とオプ
テイカルフアイバーを結合しこのオプテイカルフ
アイバーを屈曲させて光路内に配置する方法、発
光素子として放射角度に対する位相むらの少ない
ものを用いる方法などがある。
Conventional methods for reducing the influence of phase unevenness on the radiation angle include a method in which a light emitting element and an optical fiber are combined and the optical fiber is bent and placed in the optical path; There is a method of using a material with less unevenness.

しかし、オプテイカルフアイバーを屈曲させる
方法は極端に曲げてやらないと目的を達成するこ
とは困難であり、その屈曲がオプテイカルフアイ
バー破断につながり光波測距装置の経時的信頼性
を損ない、また、放射角に対する位相むらの少な
い発光素子を用いる方法は、発光素子としての光
の放射特性が無指向性に近いものを選択する必要
があり、このような発光素子は無指向性であるが
ゆえに、実際に使用する狭い放射角度範囲での光
出力が小さく、さらにオプテイカルフアイバー等
と光結合して使用する場合は、それらとの結合効
率が非常に悪く、その結合損失を補うためにより
多くの電力を発光素子に供給して放射光量を増さ
なければならないという欠点がある。
However, it is difficult to achieve the objective by bending the optical fiber unless the optical fiber is bent extremely, and the bending can lead to the optical fiber breaking, impairing the reliability of the optical distance measuring device over time. In order to use a light-emitting element with little phase unevenness with respect to the radiation angle, it is necessary to select a light-emitting element whose light radiation characteristics are close to non-directional. The optical output is small in the narrow radiation angle range that is actually used, and when used in optical coupling with optical fibers, the coupling efficiency with them is very poor, and more power is required to compensate for the coupling loss. The disadvantage is that the amount of emitted light must be increased by supplying light to the light emitting element.

本発明の目的は、前記した従来の方法の欠点を
解決し、位相むらによる不都合を除去した光波測
距装置を提供することにあり、その特徴は次のよ
うである。
An object of the present invention is to provide a light wave distance measuring device which solves the drawbacks of the conventional methods described above and eliminates the disadvantages caused by phase unevenness, and its features are as follows.

本発明においては、送光部と対物レンズの間の
光路上に受光部に入射する光を測定光と補正光で
切換えるシヤツターを設け、さらに補正光に切換
えた時のシヤツター位置においてそのシヤツター
に反射部材を取り付けその反射光を集光光学系で
集光し、送光部の光軸を含む測定光とほぼ同一の
放射角度範囲の光を補正光として用いることによ
つて、送光部の光軸に対して大きな角度の光を補
正光として用いた場合と異なり、測定誤差に結び
つく放射角度に対する位相むらの影響を受けずに
済む。そして、前記した高指向性形発光素子の使
用が可能となる。従つて前述したように、オプテ
イカルフアイバーを屈曲させたり、放射角に対す
る位相むらは少ないが、光波測距装置としては効
率が悪い無指向性形の発光素子を使用して大電力
を供給しなければならないという不都合は生じな
くなる。
In the present invention, a shutter is provided on the optical path between the light transmitting part and the objective lens to switch the light incident on the light receiving part into measurement light and correction light, and furthermore, the shutter is reflected at the position of the shutter when switching to the correction light. By attaching the member and condensing the reflected light with a condensing optical system, and using the light with a radiation angle range that is almost the same as the measurement light including the optical axis of the light transmitting section as correction light, the light of the light transmitting section can be adjusted. Unlike the case where light at a large angle with respect to the axis is used as correction light, it is not affected by phase unevenness with respect to the radiation angle that leads to measurement errors. Then, it becomes possible to use the highly directional light emitting element described above. Therefore, as mentioned above, large amounts of power must be supplied by bending the optical fiber and using omnidirectional light emitting elements, which have little phase variation with respect to the radiation angle but are inefficient as light wave ranging devices. The inconvenience of not having to do so will no longer occur.

以下、図面を参照にして本発明の実施例を詳述
する。なお、放射角度に対する位相むらとは別
に、発光素子の発光面の場所による位相むらが距
離測定誤差を増大させるという問題があり、オプ
テイカルフアイバー又は棒状の透光物質(以後、
オプテイカルロツドという。)等を使用すること
によつて発光面の場所による位相むらは混合均一
され、この問題は解決されることがすでに知られ
ている。従つて、本発明の実施例においてもこの
事を考慮し、送光部として発光素子とオプテイカ
ルフアイバー又はオプテイカルロツドの組み合わ
せたものを考える。ここで、発光面の場所による
位相むらがない発光素子では、オプテイカルフア
イバー又はオプテイカルロツドが不要であること
は明らかであり、送光部として発光素子をそのま
ま配置すればよい。
Embodiments of the present invention will be described in detail below with reference to the drawings. In addition to the phase unevenness with respect to the radiation angle, there is a problem that the phase unevenness depending on the location of the light emitting surface of the light emitting element increases the distance measurement error.
It's called an optical rod. ) etc., it is already known that the phase unevenness depending on the location of the light emitting surface can be mixed and uniformed, and this problem can be solved. Therefore, in consideration of this fact in the embodiments of the present invention, a combination of a light emitting element and an optical fiber or an optical rod is considered as a light transmitting section. Here, it is clear that an optical fiber or an optical rod is not necessary for a light emitting element that has no phase unevenness depending on the location of the light emitting surface, and the light emitting element may be placed as it is as a light transmitting section.

第1図は、光波測距装置の光学的構造に関する
本発明の一実施例を示す図であり、1は送光部、
2は測定光と補正光の切換え用のシヤツター、3
はシヤツター2の駆動装置、4はシヤツター2に
設けられた反射部材、5は送光光路透孔、6は光
ビーム分割器、6a及び6bは光ビーム分割器6
の反射面、7は対物レンズ、8はコーナーキユー
ブ、9は受光部、10及び11は補正光用集光レ
ンズ、12及び13は補正光用反射部材である。
第2図は、第1図における送光部1の一実施例を
示す図であり、14は発光素子、15はコンデン
サーレンズ、16はオプテイカルフアイバー、1
6aはオプテイカルフアイバー16の入射端面、
16dはオプテイカルフアイバー16の出射端面
である。このオプテイカルフアイバーはオプテイ
カルロツドでもさしつかえない。
FIG. 1 is a diagram showing an embodiment of the present invention regarding the optical structure of a light wave distance measuring device, in which 1 indicates a light transmitting section;
2 is a shutter for switching between measurement light and correction light, 3
4 is a driving device for the shutter 2, 4 is a reflecting member provided on the shutter 2, 5 is a light transmission optical path through hole, 6 is a light beam splitter, and 6a and 6b are light beam splitters 6.
7 is an objective lens, 8 is a corner cube, 9 is a light receiving section, 10 and 11 are condensing lenses for correction light, and 12 and 13 are reflection members for correction light.
2 is a diagram showing an embodiment of the light transmitting section 1 in FIG. 1, in which 14 is a light emitting element, 15 is a condenser lens, 16 is an optical fiber,
6a is the incident end face of the optical fiber 16;
16d is the output end face of the optical fiber 16. This optical fiber can also be an optical rod.

第2図において、発光素子14からの変調光
は、コンデンサーレンズ15を経由してオプテイ
カルフアイバー16の入射端面16aに結像す
る。入射端面16aに入射した変調光は、オプテ
イカルフアイバー16により伝達され、出射端面
16bより放射される。これが送光部1からの放
射光となる。第1図においてシヤツター2は、受
光部9に入射する光を測定光と補正光のいずれか
に切換える切換シヤツターであり、測定光と補正
光の時の両方にまたがる送光光路透孔5を有し、
測定光と補正光に応じて駆動装置3により回転さ
れ、補正光の時のシヤツター位置に反射部材4が
取り付けてあり、測定光が選択される時は送光部
1からの放射光はそのシヤツター位置に反射部材
4がないためにそのままシヤツター2を通過して
光ビーム分割器6に到達する。この時、反射部材
は送光光路内にセツトされていないため、補正光
光路へは光は入らない。又、補正光が選択される
時は、送光部1からの放射光はシヤツター2に設
けられたミラー等の反射部材4により反射され補
正光光路に導かれる。この時、反射部材が送光光
路内にセツトされて測定光光路が遮断されるた
め、測定光は存在しない。つまり、今、測定光が
選択された場合を考えると、送光部1からの放射
光は、シヤツター2の送光光路透孔5を通過した
後、光ビーム分割器6の反射面6aにより反射さ
れ、対物レンズ7を通り、平行光束となつて外部
へ放射される。この放射光は、距離測定点に設置
されたコーナーキユーブ8により反射され、その
反射光は再び対物レンズ7を通過し、光ビーム分
割器6の反射面6bにより反射され、受光部9に
入射し距離測定情報となる。又、補正光が選択さ
れた場合には送光部1からの放射光は、シヤツタ
ー2の送光光路透孔5を通過した後、反射部材4
により送光部の光軸を含む測定光とほぼ同一の放
射角範囲の光が反射され、補正光用集光レンズ1
0により平行光束となり、反射部材12及び13
により反射した後、集光レンズ11により集光さ
れて受光部9に入射し、装置内の光路長及び電子
回路部の位相ずれに基く測定誤差の補正情報とな
る。
In FIG. 2, modulated light from the light emitting element 14 passes through the condenser lens 15 and forms an image on the incident end surface 16a of the optical fiber 16. The modulated light incident on the input end face 16a is transmitted by the optical fiber 16 and is emitted from the output end face 16b. This becomes the emitted light from the light transmitting section 1. In FIG. 1, the shutter 2 is a switching shutter that switches the light incident on the light receiving section 9 into either measurement light or correction light, and has a light transmission optical path through hole 5 that spans both measurement light and correction light. death,
It is rotated by a driving device 3 according to the measurement light and the correction light, and a reflection member 4 is attached to the shutter position when the correction light is used, and when the measurement light is selected, the emitted light from the light transmitting section 1 is Since there is no reflecting member 4 in place, the light passes through the shutter 2 as it is and reaches the light beam splitter 6. At this time, since the reflecting member is not set in the light transmission optical path, no light enters the correction light optical path. Further, when the correction light is selected, the emitted light from the light transmitting section 1 is reflected by a reflecting member 4 such as a mirror provided on the shutter 2 and guided to the correction light optical path. At this time, the measuring light is not present because the reflecting member is set in the light transmission optical path and the measuring light optical path is blocked. In other words, considering the case where the measurement light is selected now, the emitted light from the light transmitting section 1 passes through the light transmitting optical path through hole 5 of the shutter 2, and then is reflected by the reflecting surface 6a of the light beam splitter 6. The light passes through the objective lens 7, becomes a parallel beam of light, and is emitted to the outside. This emitted light is reflected by a corner cube 8 installed at the distance measurement point, and the reflected light passes through the objective lens 7 again, is reflected by the reflective surface 6b of the light beam splitter 6, and enters the light receiving section 9. This becomes distance measurement information. Further, when the correction light is selected, the emitted light from the light transmitting section 1 passes through the light transmitting optical path through hole 5 of the shutter 2, and then passes through the reflecting member 4.
, the light in the radiation angle range that is almost the same as the measurement light including the optical axis of the light transmitting section is reflected, and the correction light condensing lens 1
0, it becomes a parallel light beam, and the reflecting members 12 and 13
After being reflected by, the light is focused by the condensing lens 11 and enters the light receiving section 9, and becomes correction information for measurement errors based on the optical path length within the device and the phase shift of the electronic circuit section.

本実施例においては、反射部材4をシヤツター
2に取り付け、このシヤツターを駆動装置3によ
り回転しているが、シヤツターを用いずに直接反
射部材を測定光と補正光に応じて光路に出し入れ
する構造でもなんらさしつかえない。第3図はそ
の一実施例であり、反射部材4は駆動装置3の駆
動軸17により測定光、補正光に応じて回転され
て、光路に出し入れされる。このように反射部材
4の駆動方法は、測定光と補正光が切換えられれ
ばいかなる方法でもさしつかえない。さらに本実
施例では、集光レンズ10による平行光束を反射
部材12及び13で伝達しているが、この部分に
オプテイカルフアイバーを使用して、集光レンズ
10によりオプテイカルフアイバーの入射端に反
射部材4からの反射光を集光し、オプテイカルフ
アイバーで伝達後、オプテイカルフアイバーから
の出射光を集光レンズ11で集光し、受光部9へ
入射する構造でもよい。
In this embodiment, the reflecting member 4 is attached to the shutter 2, and this shutter is rotated by the drive device 3, but the structure is such that the reflecting member is directly moved in and out of the optical path according to the measurement light and the correction light without using the shutter. But I can't blame you. FIG. 3 shows one embodiment of this, in which the reflecting member 4 is rotated by the drive shaft 17 of the drive device 3 according to the measurement light and the correction light, and is moved in and out of the optical path. As described above, the reflecting member 4 can be driven by any method as long as the measuring light and the correction light can be switched. Furthermore, in this embodiment, the parallel light beam from the condensing lens 10 is transmitted by the reflecting members 12 and 13, but an optical fiber is used for this part, and the condensing lens 10 reflects the light to the incident end of the optical fiber. A structure may also be used in which the reflected light from the member 4 is collected and transmitted by an optical fiber, and then the emitted light from the optical fiber is collected by a condensing lens 11 and enters the light receiving section 9.

以上説明したように本発明によれば、送光部と
対物レンズの間の光路内に測定光と補正光に応じ
て反射部材を出し入れし、その反射光を集光光学
系で集光し、補正光とほぼ同一の反射角度範囲の
光を使用することによつて、送光部の光軸から大
きくはなれた角度の光を利用する場合と異なり、
反射角度に対する位相むらによる影響が除去で
き、放射光量が大きくとれるために光波測距儀へ
の応用として、非常に有効な高指向性形の発光素
子を使用することが可能となる。従つて、反射角
度に対する位相むらが小さい発光素子を選択し、
その発光素子に大電力を供給してその出射効率の
悪さを補うことによつて必要な放射光量を確保す
るという不都合がなくなり、その種の発光素子に
比べ、数分の一の供給電力でそれ以上の放射光量
を得ることが可能となる。従つて、光波測距装置
の低消費電力化及び電気的誤差の減少を計る上で
も非常に有効な装置である。
As explained above, according to the present invention, a reflecting member is moved in and out of the optical path between the light transmitting unit and the objective lens according to the measurement light and the correction light, and the reflected light is focused by the focusing optical system, By using light with a reflection angle range that is almost the same as the correction light, unlike the case where light is used at an angle far away from the optical axis of the light transmitting section,
Since the influence of phase unevenness on the reflection angle can be removed and a large amount of emitted light can be obtained, it becomes possible to use a highly directional light emitting element, which is very effective in application to a light wave range finder. Therefore, a light emitting element with small phase unevenness with respect to the reflection angle is selected,
By supplying a large amount of power to the light emitting element and compensating for its poor emission efficiency, the inconvenience of securing the necessary amount of emitted light is eliminated, and it can be achieved with a fraction of the power supplied compared to that type of light emitting element. It becomes possible to obtain the above amount of emitted light. Therefore, it is a very effective device for reducing power consumption and electrical errors in a light wave distance measuring device.

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

第1図は光波測距装置の光学的構造に関する一
実施例を示す図であり、第2図は送光部の一実施
例を示す図であり、第3図は反射部材の駆動部の
一実施例を示す図である。 1……送光部、2……シヤツター、3……シヤ
ツター駆動装置、4……反射部材、5……送光光
路透孔、6……光ビーム分割器、6a,6b……
光ビーム分割器6の反射面、7……対物レンズ、
8……コーナーキユーブ、9……受光部、10,
11……補正光用集光レンズ、12,13……補
正光用反射部材、14……発光素子、15……コ
ンデンサーレンズ、16……オプテイカルフアイ
バー、16a……オプテイカルフアイバー16の
入射端面、16b……オプテイカルフアイバー1
6の出射端面、17……駆動装置3の駆動軸。
FIG. 1 is a diagram showing an example of the optical structure of a light wave distance measuring device, FIG. 2 is a diagram showing an example of the light transmitting section, and FIG. 3 is a diagram showing an example of the driving section of the reflecting member. It is a figure showing an example. DESCRIPTION OF SYMBOLS 1... Light transmission part, 2... Shutter, 3... Shutter drive device, 4... Reflection member, 5... Light transmission optical path hole, 6... Light beam splitter, 6a, 6b...
Reflection surface of the light beam splitter 6, 7...objective lens,
8... Corner cube, 9... Light receiving section, 10,
11...Condensing lens for correction light, 12, 13...Reflection member for correction light, 14...Light emitting element, 15...Condenser lens, 16...Optical fiber, 16a...Incidence end surface of optical fiber 16 , 16b...Optical fiber 1
output end face of 6, 17... drive shaft of drive device 3;

Claims (1)

【特許請求の範囲】[Claims] 1 発光部からの放射変調光を送光光学系に用い
て反射器に向けて放射し、該反射器からの反射変
調光を受光光学系を用いて受光部に結像させ、前
記放射変調光と反射変調光との位相差により距離
を測定する光波測距装置において、前記送光部と
送光光学系の間の光路上に、測定光と補正光に応
じて出し入れされる反射部材を設け、補正光光路
上に前記補正光を集光する集光光学系を配置する
ことによつて、補正光として測定光とほぼ同一の
放射角度範囲の前記放射変調光を使用して、前記
放射変調光の放射角度に対する位相むらによる影
響を除去したことを特徴とする光波測距装置。
1 Emits the modulated radiation light from the light emitting section toward a reflector using a light transmitting optical system, and focuses the modulated light reflected from the reflector on the light receiving section using a light receiving optical system, so that the modulated radiation light In a light wave distance measuring device that measures distance based on a phase difference between the light beam and the reflected modulated light, a reflecting member is provided on the optical path between the light transmitting section and the light transmitting optical system, and is moved in and out according to the measurement light and the correction light. , by arranging a condensing optical system that condenses the correction light on the correction light optical path, the radiation modulation light having substantially the same radiation angle range as the measurement light is used as the correction light; A light wave ranging device characterized in that the influence of phase unevenness on the radiation angle of light is removed.
JP58243388A 1983-12-22 1983-12-22 Light wave distance measuring apparatus Granted JPS60133381A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58243388A JPS60133381A (en) 1983-12-22 1983-12-22 Light wave distance measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58243388A JPS60133381A (en) 1983-12-22 1983-12-22 Light wave distance measuring apparatus

Publications (2)

Publication Number Publication Date
JPS60133381A JPS60133381A (en) 1985-07-16
JPH0135306B2 true JPH0135306B2 (en) 1989-07-25

Family

ID=17103109

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58243388A Granted JPS60133381A (en) 1983-12-22 1983-12-22 Light wave distance measuring apparatus

Country Status (1)

Country Link
JP (1) JPS60133381A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60149985A (en) * 1984-01-14 1985-08-07 Asahi Optical Co Ltd Optical distance measuring apparatus
JPH08292258A (en) * 1995-04-21 1996-11-05 Nikon Corp Ranging device

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2956472A (en) * 1956-10-18 1960-10-18 Askania Werke Ag Electro-optical distance meter
CH606991A5 (en) * 1976-12-03 1978-11-30 Wild Heerbrugg Ag
JPS5940274B2 (en) * 1979-04-27 1984-09-28 東京光学機械株式会社 Optical fiber device for light wave distance meter
JPS6023739Y2 (en) * 1981-07-20 1985-07-15 富士光機株式会社 light wave distance meter
DE3135392A1 (en) * 1981-09-07 1983-03-17 Bayer Ag, 5090 Leverkusen "SUBSTITUTED 6-ALKOXY-TERT.-BUTYL-1,2,4-TRIAZINE-5-ONE, METHOD FOR THE PRODUCTION THEREOF AND THEIR USE AS HERBICIDES"

Also Published As

Publication number Publication date
JPS60133381A (en) 1985-07-16

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