[go: up one dir, main page]

JP3835016B2 - Laser radar equipment - Google Patents

Laser radar equipment Download PDF

Info

Publication number
JP3835016B2
JP3835016B2 JP29478998A JP29478998A JP3835016B2 JP 3835016 B2 JP3835016 B2 JP 3835016B2 JP 29478998 A JP29478998 A JP 29478998A JP 29478998 A JP29478998 A JP 29478998A JP 3835016 B2 JP3835016 B2 JP 3835016B2
Authority
JP
Japan
Prior art keywords
semi
field stop
light
laser beam
laser
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 - Fee Related
Application number
JP29478998A
Other languages
Japanese (ja)
Other versions
JP2000121724A (en
Inventor
隆一 樋口
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP29478998A priority Critical patent/JP3835016B2/en
Publication of JP2000121724A publication Critical patent/JP2000121724A/en
Application granted granted Critical
Publication of JP3835016B2 publication Critical patent/JP3835016B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Optical Radar Systems And Details Thereof (AREA)

Description

【0001】
【発明の属する技術分野】
この発明はレーザレーダ装置の送信軸と受信軸との軸ずれ検出に関するものである。
【0002】
【従来の技術】
レーザレーダ装置は、自らレーザを発射して目標物に当て目標物からの反射光を受けて信号の大きさと発射時からの時間を測ることにより、目標物の特性や目標物までの距離を求める装置である。最近は応用分野が拡がり、人工衛星に搭載して大気の散乱特性の高度分布を測定することも可能になった。レーザレーダ装置においてはレーザ反射光を受けるので、レーザで照射された目標物が必ず受信光学系の視野内になければならない。視野内から完全に外れればそもそも信号を掴むことができないし、部分的に外れても目標物の特性を正確に測定できなくなる。したがって、レーザで照射された目標物を受信光学系の視野中心に保つこと、言い替えれば、送信と受信の軸を一致させることはレーザレーダ装置にとって不可欠の条件である。送信と受信の軸を一致させるには軸ずれ検出および軸ずれ補正が必要である。
【0003】
図5は従来の軸ずれ検出方式を示す図である。図5において、1はレーザ、2はダブルウェッジのような、レーザビームの方向を調節する調節装置、3はカセグレイン光学系のような受信望遠鏡、4はピンホールのような視野絞り、5はリレー光学系、6は狭帯域フィルタ、7は検出器、8は信号処理回路、10は半透鏡、16はレンズ、17は4象限検出器である。
【0004】
次に動作について説明する。レーザ1から発生されたレーザビームは調節装置2および半透鏡10を介して目標に向けて送出される。目標からの反射光はカセグレイン主鏡3aおよびカセグレイン副鏡3bからなる受信望遠鏡3により集光されて視野絞り4を通る。視野絞り4を通過した光はレンズ5aおよびレンズ5bからなるリレー光学系5の内部に置かれた狭帯域フィルタ6を通過して検出器7に集められる。光は検出器7で電気信号に変換され、信号処理回路8により増幅、デジタル化され目標情報が抽出される。このようなレーザレーダ装置において軸ずれ検出を次のように行う。半透鏡10によりレーザビームの一部は反射して、レンズ16を経て4象限検出器17に入る。4象限検出器17はレンズ16の焦点に置かれているので、4象限検出器17面上でレーザビームは小さなスポットになる。スポットが4象限検出器17の中心にあれば4象限検出器17の出力は0であり、中心からずれていれば、ずれに比例した出力が得られる。このようにスポットの位置を検出することによりレーザビームの方向を知ることができる。ずれが発生すれば、4象限検出器17の出力を監視しながら調節装置2により修正する。
【0005】
【発明が解決しようとする課題】
レーザレーダ装置における従来の軸ずれ検出装置は以上のように送信軸ずれを検出するものである。大きな電力を消費し従って発熱量が大きいレーザ装置に起因する送信軸ずれに比べて、発熱量が遥かに小さい受信側の軸ずれは小さいので、地上における通常環境で使う限り、送信軸ずれにより送受信の相対軸ずれを代用しても支障ない。ところが、内部発熱が無くても熱的なアンバランスが生じる人工衛星搭載機器においては受信軸ずれを無視できなくなるので、送信軸ずれの検出のみを行う従来の方法では送受信の相対軸ずれを正当に評価できないという問題点がある。
【0006】
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、送信軸ずれと同時に受信軸ずれも検出することにより送受信の相対軸ずれ検出可能な装置を得ることを目的とする。
【0007】
【課題を解決するための手段】
第1の発明に係る装置は、受信視野を決める視野絞りを照明することにより光を受信光学系から逆向きに出し、この光軸と送信レーザビームの光軸の相対軸ずれを検出するようにしたものである。軸ずれ検出は次のように行う。受信光学系から出る光の一部を反射鏡により折曲げ、また、送信レーザビームの一部を半透鏡により折曲げ、両方のビームを重ね合わせてイメージセンサに結像させる。軸が合っていれば1点で結像するが、軸ずれが起これば、スポットは分かれる。2つのスポットの距離は2つの軸の方向ずれに対応するので軸ずれが分かる。また、反射鏡と半透鏡を相対変化が起きないように一体化構造にすることにより周囲の変化により反射鏡/半透鏡の向きが変わっても、相対的な軸ずれは正確に測定可能である。
【0008】
第2の発明に係る装置は、第1の発明における反射鏡を半透鏡に置き換えて適用した場合である。
【0009】
第3の発明に係る装置は、受信光学系の中心からレーザ光が出射する形式、即ち、同軸型のレーザレーダ装置に適用した場合である。
【0010】
第4の発明に係る装置は、出射レーザビームの一部を光ファイバにより受信検出器に照射して、軸ずれだけでなく検出器のずれも検出可能にするものである。
【0011】
第5の発明に係る装置は、照明を視野絞りの裏から行って視野中心を光らすことにより観測を容易にするものである。
【0012】
【発明の実施の形態】
実施の形態1.
以下、この発明の実施の形態1を図について説明する。図1において、1はレーザ、2はダブルウェッジのような、レーザビームの方向を調節する調節装置、3はカセグレイン光学系のような受信望遠鏡、4はピンホールのような視野絞り、5はリレー光学系、6は狭帯域フィルタ、7は検出器、8は信号処理回路であり、これらは通常のレーザレーダ装置の構成要素である。9は反射鏡、10は半透鏡、11は反射鏡9と半透鏡10を一体化して支持する支持枠、12はイメージセンサ、13は照明光源である。
【0013】
次に動作について説明する。レーザ1から発生されたレーザビームは調節装置2および半透鏡10を介して目標に向けて送出される。目標からの反射光はカセグレイン主鏡3aおよびカセグレイン副鏡3bからなる受信望遠鏡3により集光されて視野絞り4を通る。視野絞り4を通過した光はレンズ5aおよびレンズ5bからなるリレー光学系5の内部に置かれた狭帯域フィルタ6を通過して検出器7に集められる。光は検出器7で電気信号に変換され、信号処理回路8により増幅、デジタル化され目標情報が抽出される。このようなレーザレーダ装置において軸ずれ検出を次のように行う。照明光源13は視野絞り4を前方から照明する。視野絞り4は通常ピンホールであり、基板に小穴が開いている。照明すると、基板から光が拡散反射される。小穴からの光は皆無ではないが基板からの拡散反射光に対して遥かに小さいので、小穴は黒く見える。基板からの拡散反射光はレーザレーダ装置の入射光とは反対方向に、カセグレイン副鏡3bおよびカセグレイン主鏡3aを経て外へ向かって出る。カセグレイン主鏡3aから外へ向かって出る光束の一部を反射鏡9により遮り、折曲げて取り出す。レーザ1からのレーザビームの一部も半透鏡10により折曲げて取り出す。折曲げて取り出した2つのビームは半透鏡10で合体し、イメージセンサ12に入る。この像の観測により、スポットが重なれば光軸は合っており、スポットが分離すれば光軸がずれていることが分かる。光軸がずれていればビーム方向調節装置2により修正することができる。周囲の変形があっても反射鏡9と半透鏡10がおのおの独立に動かないように一体化されているので、光線の方向に関しては1枚の平面鏡と同じであり、送受信軸ずれを正確に測定することができる。
【0014】
図1において、反射鏡9の代わりに半透鏡を使ってもよい。
【0015】
実施の形態2.
他の実施の形態を図2に示す。図2においてレーザ1から発生されたレーザビームは調節装置2を通り、2個の直角プリズム18aおよび18bによりカセグレイン副鏡3bの裏側に平行移動された後、半透鏡14を介して目標に向けて送出される。目標からの反射光はカセグレイン主鏡3aおよびカセグレイン副鏡3bからなる受信望遠鏡3により集光されて視野絞り4を通る。視野絞り4を通過した光はレンズ5aおよびレンズ5bからなるリレー光学系5の内部に置かれた狭帯域フィルタ6を通過して検出器7に集められる。光は検出器7で電気信号に変換され、信号処理回路8により増幅、デジタル化され目標情報が抽出される。このような同軸型のレーザレーダ装置において軸じれ検出を次のように行う。レーザビームの一部を半透鏡14により反射させて取り出す。受信望遠鏡から出る光の一部も半透鏡10により折曲げて取り出す。折曲げて取り出した2つのビームは半透鏡10で合体し、イメージセンサ12に結像される。
【0016】
実施の形態3.
他の実施の形態を図3に示す。図3において、15は一端をレーザビームの端に置き、他端を検出器近傍に置く光ファイバである。光ファイバ15によりレーザビームの一部を取り出し、検出器7に照射する。検出器面で拡散反射された光はリレー光学系5および視野絞り4を通過して受信望遠鏡3から出る。リレー光学系5内にはレーザ波長のみ通過させる狭帯域フィルタ6があるので、リレー光学系5を通すためにレーザ光そのものの一部を使用する。この構成で、視野絞り4から出る光は実施の形態1と同じように使うことができる。また、検出器7がずれれば一様な検出器面から外れた光が視野絞り4を通って受信望遠鏡3から出るのでスポットの形状を観測することにより検出器7のずれが分かる。
【0017】
実施の形態4.
他の実施の形態を図4に示す。図4において、照明は視野絞り4の裏から行う。このように照明すれば、基板からの拡散反射光でなく、基板に開けた穴を通過する光のみがイメージセンサに入るので像が観測し易い。
【0018】
【発明の効果】
このように、この発明によれば、レーザレーダ装置の送信軸と受信軸の相対軸ずれを測定可能になるので、送信軸だけでなく、受信軸の変化も無視できない人工衛星軌道上のレーザレーダ装置の測定精度を高める。
【図面の簡単な説明】
【図1】 この発明の実施の形態1によるレーザレーダ装置を示す図である。
【図2】 この発明の実施の形態2を示す図である。
【図3】 この発明の実施の形態3を示す図である。
【図4】 この発明の実施の形態4を示す図である。
【図5】 従来のレーザレーダ装置を示す図である。
【符号の説明】
1 レーザ、2 レーザビーム方向調節装置、3 受信望遠鏡、3a カセグレイン主鏡、3b カセグレイン副鏡、4 視野絞り、5 リレー光学系、5a,5b レンズ、6 狭帯域フィルタ、7 検出器、8 信号処理回路、9 反射鏡、10 半透鏡、11 支持枠、12 イメージセンサ、13 照明光源、14 半透鏡、15 光ファイバ、16 レンズ、17 4象限検出器、18a,18b 直角プリズム。
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to detection of an axial deviation between a transmission axis and a reception axis of a laser radar device.
[0002]
[Prior art]
The laser radar device emits the laser itself, hits the target, receives the reflected light from the target, measures the signal magnitude and the time from the launch, and determines the characteristics of the target and the distance to the target Device. Recently, the field of application has expanded, and it is now possible to measure the altitude distribution of atmospheric scattering characteristics onboard satellites. Since the laser radar device receives the reflected laser beam, the target irradiated with the laser must be in the field of view of the receiving optical system. If it is completely out of the field of view, the signal cannot be grasped in the first place, and even if it is partially off, the characteristics of the target cannot be measured accurately. Therefore, it is an indispensable condition for the laser radar apparatus to keep the target irradiated with the laser at the center of the field of view of the receiving optical system, in other words, to match the axes of transmission and reception. Axis deviation detection and axis deviation correction are required to match the transmission and reception axes.
[0003]
FIG. 5 is a diagram showing a conventional axis deviation detection method. In FIG. 5, 1 is a laser, 2 is an adjustment device for adjusting the direction of the laser beam, such as a double wedge, 3 is a receiving telescope such as a Cassegrain optical system, 4 is a field stop such as a pinhole, and 5 is a relay An optical system, 6 is a narrow band filter, 7 is a detector, 8 is a signal processing circuit, 10 is a semi-transparent mirror, 16 is a lens, and 17 is a quadrant detector.
[0004]
Next, the operation will be described. The laser beam generated from the laser 1 is transmitted toward the target through the adjusting device 2 and the semi-transparent mirror 10. The reflected light from the target is collected by the receiving telescope 3 including the cassegrain primary mirror 3 a and the cassegrain secondary mirror 3 b and passes through the field stop 4. The light that has passed through the field stop 4 passes through a narrow-band filter 6 placed inside a relay optical system 5 including a lens 5a and a lens 5b, and is collected by a detector 7. The light is converted into an electric signal by the detector 7, amplified and digitized by the signal processing circuit 8, and target information is extracted. In such a laser radar apparatus, the axis deviation is detected as follows. A part of the laser beam is reflected by the semi-transparent mirror 10 and enters the four-quadrant detector 17 through the lens 16. Since the 4-quadrant detector 17 is placed at the focal point of the lens 16, the laser beam becomes a small spot on the surface of the 4-quadrant detector 17. If the spot is at the center of the four-quadrant detector 17, the output of the four-quadrant detector 17 is 0. If the spot is shifted from the center, an output proportional to the shift is obtained. By detecting the spot position in this way, the direction of the laser beam can be known. If a deviation occurs, the adjustment device 2 corrects the output while monitoring the output of the four-quadrant detector 17.
[0005]
[Problems to be solved by the invention]
The conventional axis deviation detection device in the laser radar apparatus detects the transmission axis deviation as described above. Compared to the transmission axis misalignment caused by a laser device that consumes a large amount of power and therefore generates a large amount of heat, the misalignment on the receiving side is much smaller. Substituting the relative axis misalignment of can be used. However, in a satellite-equipped device in which thermal imbalance occurs even if there is no internal heat generation, the reception axis deviation cannot be ignored. Therefore, the conventional method that only detects the transmission axis deviation correctly detects the relative axis deviation of transmission and reception. There is a problem that it cannot be evaluated.
[0006]
The present invention has been made to solve the above-described problems, and an object of the present invention is to obtain an apparatus capable of detecting transmission and reception relative axis deviations by detecting reception axis deviations simultaneously with transmission axis deviations.
[0007]
[Means for Solving the Problems]
The apparatus according to the first aspect of the invention emits light from the receiving optical system in the reverse direction by illuminating the field stop that determines the receiving field of view, and detects the relative axis shift between the optical axis and the optical axis of the transmitted laser beam. It is a thing. The axis deviation is detected as follows. A part of the light emitted from the receiving optical system is bent by a reflecting mirror, and a part of the transmission laser beam is bent by a semi-transparent mirror, and both beams are superimposed to form an image on an image sensor. If the axes are aligned, the image is formed at one point, but if the axis shifts, the spots are separated. Since the distance between the two spots corresponds to the misalignment of the two axes, the misalignment is known. In addition, by integrating the reflector and the semi-transparent mirror so that relative changes do not occur, even if the orientation of the reflector / semi-transparent mirror changes due to surrounding changes, the relative axis deviation can be measured accurately. .
[0008]
The apparatus according to the second invention is a case where the reflecting mirror in the first invention is replaced with a semi-transparent mirror.
[0009]
The device according to the third invention is a case where the laser beam is emitted from the center of the receiving optical system, that is, applied to a coaxial laser radar device.
[0010]
The apparatus according to the fourth aspect of the invention irradiates a part of the outgoing laser beam to the receiving detector through an optical fiber so that not only the axis deviation but also the deviation of the detector can be detected.
[0011]
The apparatus according to the fifth aspect of the invention facilitates observation by illuminating from the back of the field stop to illuminate the center of the field of view.
[0012]
DETAILED DESCRIPTION OF THE INVENTION
Embodiment 1 FIG.
Embodiment 1 of the present invention will be described below with reference to the drawings. In FIG. 1, 1 is a laser, 2 is an adjustment device for adjusting the direction of a laser beam, such as a double wedge, 3 is a receiving telescope such as a Cassegrain optical system, 4 is a field stop such as a pinhole, and 5 is a relay. An optical system, 6 is a narrow band filter, 7 is a detector, and 8 is a signal processing circuit, which are components of a normal laser radar device. Reference numeral 9 denotes a reflecting mirror, 10 denotes a semi-transparent mirror, 11 denotes a support frame that integrally supports the reflecting mirror 9 and the semi-transparent mirror 10, 12 denotes an image sensor, and 13 denotes an illumination light source.
[0013]
Next, the operation will be described. A laser beam generated from the laser 1 is transmitted toward the target via the adjusting device 2 and the semi-transparent mirror 10. The reflected light from the target is collected by the receiving telescope 3 including the cassegrain primary mirror 3 a and the cassegrain secondary mirror 3 b and passes through the field stop 4. The light that has passed through the field stop 4 passes through a narrowband filter 6 placed inside a relay optical system 5 including a lens 5a and a lens 5b, and is collected by a detector 7. The light is converted into an electric signal by the detector 7, amplified and digitized by the signal processing circuit 8, and target information is extracted. In such a laser radar apparatus, the axis deviation is detected as follows. The illumination light source 13 illuminates the field stop 4 from the front. The field stop 4 is usually a pinhole and has a small hole in the substrate. When illuminated, light is diffusely reflected from the substrate. There is no light from the small holes, but they are much smaller than the diffusely reflected light from the substrate, so the small holes look black. Diffuse reflected light from the substrate exits in the opposite direction to the incident light of the laser radar device through the cassegrain secondary mirror 3b and the cassegrain main mirror 3a. A part of the light beam exiting from the Kasegrain main mirror 3a is blocked by the reflecting mirror 9, bent, and taken out. A part of the laser beam from the laser 1 is also bent by the semi-transparent mirror 10 and taken out. The two beams taken out by bending are merged by the semi-transparent mirror 10 and enter the image sensor 12. From the observation of this image, it can be seen that the optical axes are aligned when the spots overlap, and the optical axes are shifted when the spots are separated. If the optical axis is deviated, it can be corrected by the beam direction adjusting device 2. Since the reflecting mirror 9 and the semi-transparent mirror 10 are integrated so that they do not move independently even if there is deformation in the surroundings, the direction of the light beam is the same as that of one plane mirror, and the transmission / reception axis deviation is accurately measured. can do.
[0014]
In FIG. 1, a semi-transparent mirror may be used instead of the reflecting mirror 9.
[0015]
Embodiment 2. FIG.
Another embodiment is shown in FIG. In FIG. 2, the laser beam generated from the laser 1 passes through the adjusting device 2 and is translated by the two right-angle prisms 18 a and 18 b to the back side of the cassegrain secondary mirror 3 b, and then toward the target through the semi-transparent mirror 14. Sent out. The reflected light from the target is collected by the receiving telescope 3 including the cassegrain primary mirror 3 a and the cassegrain secondary mirror 3 b and passes through the field stop 4. The light that has passed through the field stop 4 passes through a narrowband filter 6 placed inside a relay optical system 5 including a lens 5a and a lens 5b, and is collected by a detector 7. The light is converted into an electric signal by the detector 7, amplified and digitized by the signal processing circuit 8, and target information is extracted. In such a coaxial type laser radar apparatus, the axis shift detection is performed as follows. A part of the laser beam is reflected by the semi-transparent mirror 14 and taken out. Part of the light emitted from the receiving telescope is also bent out by the semi-transparent mirror 10 and extracted. The two beams taken out by bending are merged by the semi-transparent mirror 10 and imaged on the image sensor 12.
[0016]
Embodiment 3 FIG.
Another embodiment is shown in FIG. In FIG. 3, reference numeral 15 denotes an optical fiber having one end placed at the end of the laser beam and the other end placed near the detector. A part of the laser beam is taken out by the optical fiber 15 and irradiated to the detector 7. The light diffusely reflected by the detector surface passes through the relay optical system 5 and the field stop 4 and exits from the receiving telescope 3. Since there is a narrow band filter 6 that allows only the laser wavelength to pass through in the relay optical system 5, a part of the laser light itself is used to pass through the relay optical system 5. With this configuration, the light emitted from the field stop 4 can be used as in the first embodiment. Further, if the detector 7 is displaced, the light deviating from the uniform detector surface passes through the field stop 4 and exits from the receiving telescope 3, so that the displacement of the detector 7 can be found by observing the spot shape.
[0017]
Embodiment 4 FIG.
Another embodiment is shown in FIG. In FIG. 4, illumination is performed from the back of the field stop 4. By illuminating in this way, only the light that passes through the hole formed in the substrate, not the diffusely reflected light from the substrate, enters the image sensor, so that the image can be easily observed.
[0018]
【The invention's effect】
As described above, according to the present invention, since it is possible to measure the relative axis deviation between the transmission axis and the reception axis of the laser radar apparatus, the laser radar on the artificial satellite orbit where not only the transmission axis but also the change of the reception axis cannot be ignored. Increase instrument measurement accuracy.
[Brief description of the drawings]
FIG. 1 is a diagram showing a laser radar apparatus according to Embodiment 1 of the present invention.
FIG. 2 is a diagram showing a second embodiment of the present invention.
FIG. 3 is a diagram showing a third embodiment of the present invention.
FIG. 4 is a diagram showing a fourth embodiment of the present invention.
FIG. 5 is a diagram showing a conventional laser radar device.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Laser, 2 Laser beam direction adjustment apparatus, 3 Reception telescope, 3a Cassegrain primary mirror, 3b Cassegrain secondary mirror, 4 Field stop, 5 Relay optical system, 5a, 5b Lens, 6 Narrow-band filter, 7 Detector, 8 Signal processing Circuit, 9 Reflector, 10 Semi-transparent mirror, 11 Support frame, 12 Image sensor, 13 Illumination light source, 14 Semi-transparent mirror, 15 Optical fiber, 16 Lens, 174 Quadrant detector, 18a, 18b Right angle prism.

Claims (4)

レーザビームを発生するレーザ、上記レーザビームで照射された目標からの反射光を受ける受信望遠鏡、この受信望遠鏡の視野を調節する視野絞り、この視野絞りから出た光を検出器に集めるリレー光学系、このリレー光学系で集光された光を電気信号に変換する検出器および上記電気信号から目標情報を抽出する信号処理回路とを備えたレーザレーダ装置において、
上記視野絞りを照明する光源、
上記視野絞りから上記受信望遠鏡を経て出射する上記光源からの照明光の一部を折曲げる反射鏡、
上記反射鏡で折曲げられた上記照明光に重なり、かつ、上記反射鏡と平行に配置され、上記レーザビームの一部を折曲げる半透鏡、
上記反射鏡と上記半透鏡を一体化して支える支持枠、
上記半透鏡から出る光を撮影するイメージセンサと
を備えたことを特徴とするレーザレーダ装置。
Laser that generates a laser beam, a receiving telescope that receives reflected light from a target irradiated with the laser beam, a field stop that adjusts the field of view of the receiving telescope, and a relay optical system that collects light emitted from the field stop on a detector In a laser radar apparatus comprising: a detector that converts light collected by the relay optical system into an electrical signal; and a signal processing circuit that extracts target information from the electrical signal.
A light source for illuminating the field stop,
A reflecting mirror that bends part of illumination light from the light source that is emitted from the field stop through the receiving telescope;
A semi-transparent mirror that overlaps with the illumination light bent by the reflecting mirror and is arranged in parallel with the reflecting mirror and bends a part of the laser beam;
A support frame that integrally supports the reflector and the semi-transparent mirror;
A laser radar device comprising: an image sensor for photographing light emitted from the semi-transparent mirror.
レーザビームを発生するレーザ、上記レーザビームで照射された目標からの反射光を受ける受信望遠鏡、この受信望遠鏡の視野を調節する視野絞り、この視野絞りから出た光を検出器に集めるリレー光学系、このリレー光学系で集光された光を電気信号に変換する検出器および上記電気信号から目標情報を抽出する信号処理回路とを備えたレーザレーダ装置において、
上記視野絞りを照明する光源、
上記視野絞りから上記受信望遠鏡を経て出射する上記光源からの照明光の一部を折曲げる第1の半透鏡、
上記第1の半透鏡で折曲げられた上記照明光に重なり、かつ、上記反射鏡と平行に配置され、上記レーザビームの一部を折曲げる第2の半透鏡、
上記2個の半透鏡を一体化して支える支持枠、
上記第2の半透鏡から出る光を撮影するイメージセンサ
とを備えたことを特徴とするレーザレーダ装置。
Laser that generates a laser beam, a receiving telescope that receives reflected light from a target irradiated with the laser beam, a field stop that adjusts the field of view of the receiving telescope, and a relay optical system that collects light emitted from the field stop on a detector In a laser radar apparatus comprising: a detector that converts light collected by the relay optical system into an electrical signal; and a signal processing circuit that extracts target information from the electrical signal.
A light source for illuminating the field stop,
A first semi-transparent mirror that bends part of illumination light from the light source that is emitted from the field stop through the reception telescope;
A second semi-transparent mirror that overlaps the illumination light bent by the first semi-transparent mirror and is arranged in parallel with the reflecting mirror and bends a part of the laser beam;
A support frame that integrally supports the two semi-transparent mirrors,
A laser radar device comprising: an image sensor for photographing light emitted from the second semi-transparent mirror.
レーザビームを発生するレーザ、上記レーザビームで照射された目標からの反射光を受ける受信望遠鏡、この受信望遠鏡の視野を調節する視野絞り、この視野絞りから出た光を検出器に集めるリレー光学系、このリレー光学系で集光された光を電気信号に変換する検出器および上記電気信号から目標情報を抽出する信号処理回路とを備えたレーザレーダ装置において、
上記レーザビームの一部を光ファイバで取り出し上記検出器を照明する光源、
上記視野絞りから上記受信望遠鏡を経て出射する上記光源からの照明光の一部を折曲げる反射鏡、
上記反射鏡で折曲げられた上記照明光に重なり、かつ、上記反射鏡と平行に配置され、上記レーザビームの一部を折曲げる半透鏡、
上記反射鏡と上記半透鏡を一体化して支える支持枠、
上記半透鏡から出る光を撮影するイメージセンサ
とを備えたことを特徴とするレーザレーダ装置。
Laser that generates a laser beam, a receiving telescope that receives reflected light from a target irradiated with the laser beam, a field stop that adjusts the field of view of the receiving telescope, and a relay optical system that collects light emitted from the field stop on a detector In a laser radar apparatus comprising: a detector that converts light collected by the relay optical system into an electrical signal; and a signal processing circuit that extracts target information from the electrical signal.
A light source for extracting a part of the laser beam with an optical fiber and illuminating the detector;
A reflecting mirror that bends part of illumination light from the light source that is emitted from the field stop through the receiving telescope;
A semi-transparent mirror that overlaps with the illumination light bent by the reflecting mirror and is arranged in parallel with the reflecting mirror and bends a part of the laser beam;
A support frame that integrally supports the reflector and the semi-transparent mirror;
A laser radar device comprising: an image sensor for photographing light emitted from the semi-transparent mirror.
レーザビームを発生するレーザ、上記レーザビームで照射された目標からの反射光を受ける受信望遠鏡、この受信望遠鏡の視野を調節する視野絞り、この視野絞りから出た光を検出器に集めるリレー光学系、このリレー光学系で集光された光を電気信号に変換する検出器および上記電気信号から目標情報を抽出する信号処理回路とを備えたレーザレーダ装置において、
上記視野絞りを裏側から照明する光源、
上記視野絞りから上記受信望遠鏡を経て出射する上記光源からの照明光の一部を折曲げる反射鏡、
上記反射鏡で折曲げられた上記照明光に重なり、かつ、上記反射鏡と平行に配置され、上記レーザビームの一部を折曲げる半透鏡、
上記反射鏡と上記半透鏡を一体化して支える支持枠、
上記半透鏡から出る光を撮影するイメージセンサ
とを備えたことを特徴とするレーザレーダ装置。
Laser that generates a laser beam, a receiving telescope that receives reflected light from a target irradiated with the laser beam, a field stop that adjusts the field of view of the receiving telescope, and a relay optical system that collects light emitted from the field stop on a detector In a laser radar apparatus comprising: a detector that converts light collected by the relay optical system into an electrical signal; and a signal processing circuit that extracts target information from the electrical signal.
A light source for illuminating the field stop from the back side,
A reflecting mirror that bends part of illumination light from the light source that is emitted from the field stop through the receiving telescope;
A semi-transparent mirror that overlaps with the illumination light bent by the reflecting mirror and is arranged in parallel with the reflecting mirror and bends a part of the laser beam;
A support frame that integrally supports the reflector and the semi-transparent mirror;
A laser radar device comprising: an image sensor for photographing light emitted from the semi-transparent mirror.
JP29478998A 1998-10-16 1998-10-16 Laser radar equipment Expired - Fee Related JP3835016B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29478998A JP3835016B2 (en) 1998-10-16 1998-10-16 Laser radar equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29478998A JP3835016B2 (en) 1998-10-16 1998-10-16 Laser radar equipment

Publications (2)

Publication Number Publication Date
JP2000121724A JP2000121724A (en) 2000-04-28
JP3835016B2 true JP3835016B2 (en) 2006-10-18

Family

ID=17812306

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29478998A Expired - Fee Related JP3835016B2 (en) 1998-10-16 1998-10-16 Laser radar equipment

Country Status (1)

Country Link
JP (1) JP3835016B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109407333A (en) * 2018-12-14 2019-03-01 中国科学院长春光学精密机械与物理研究所 The automated calibration system and calibration method of the acquisition and tracking optical axis and Laser emission axis

Families Citing this family (36)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102006031580A1 (en) 2006-07-03 2008-01-17 Faro Technologies, Inc., Lake Mary Method and device for the three-dimensional detection of a spatial area
WO2009041307A1 (en) 2007-09-25 2009-04-02 Nikon Corporation Alignment device and method for optical system
DE102009010465B3 (en) 2009-02-13 2010-05-27 Faro Technologies, Inc., Lake Mary laser scanner
DE102009015920B4 (en) 2009-03-25 2014-11-20 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US9551575B2 (en) 2009-03-25 2017-01-24 Faro Technologies, Inc. Laser scanner having a multi-color light source and real-time color receiver
DE102009035337A1 (en) 2009-07-22 2011-01-27 Faro Technologies, Inc., Lake Mary Method for optically scanning and measuring an object
US9529083B2 (en) 2009-11-20 2016-12-27 Faro Technologies, Inc. Three-dimensional scanner with enhanced spectroscopic energy detector
DE102009055988B3 (en) 2009-11-20 2011-03-17 Faro Technologies, Inc., Lake Mary Device, particularly laser scanner, for optical scanning and measuring surrounding area, has light transmitter that transmits transmission light ray by rotor mirror
US9210288B2 (en) 2009-11-20 2015-12-08 Faro Technologies, Inc. Three-dimensional scanner with dichroic beam splitters to capture a variety of signals
DE102009055989B4 (en) * 2009-11-20 2017-02-16 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US9113023B2 (en) 2009-11-20 2015-08-18 Faro Technologies, Inc. Three-dimensional scanner with spectroscopic energy detector
DE102009057101A1 (en) 2009-11-20 2011-05-26 Faro Technologies, Inc., Lake Mary Device for optically scanning and measuring an environment
US9879976B2 (en) 2010-01-20 2018-01-30 Faro Technologies, Inc. Articulated arm coordinate measurement machine that uses a 2D camera to determine 3D coordinates of smoothly continuous edge features
CN102725702B (en) 2010-01-20 2015-04-08 法罗技术股份有限公司 Method for evaluating mounting stability of articulated arm coordinate measurement machine using inclinometers
US9628775B2 (en) 2010-01-20 2017-04-18 Faro Technologies, Inc. Articulated arm coordinate measurement machine having a 2D camera and method of obtaining 3D representations
US9607239B2 (en) 2010-01-20 2017-03-28 Faro Technologies, Inc. Articulated arm coordinate measurement machine having a 2D camera and method of obtaining 3D representations
DE102010020925B4 (en) 2010-05-10 2014-02-27 Faro Technologies, Inc. Method for optically scanning and measuring an environment
DE102010032723B3 (en) 2010-07-26 2011-11-24 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010032726B3 (en) 2010-07-26 2011-11-24 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010032725B4 (en) 2010-07-26 2012-04-26 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010033561B3 (en) 2010-07-29 2011-12-15 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US9168654B2 (en) 2010-11-16 2015-10-27 Faro Technologies, Inc. Coordinate measuring machines with dual layer arm
DE102012100609A1 (en) 2012-01-25 2013-07-25 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US8997362B2 (en) 2012-07-17 2015-04-07 Faro Technologies, Inc. Portable articulated arm coordinate measuring machine with optical communications bus
DE102012107544B3 (en) 2012-08-17 2013-05-23 Faro Technologies, Inc. Optical scanning device i.e. laser scanner, for evaluating environment, has planetary gears driven by motor over vertical motor shaft and rotating measuring head relative to foot, where motor shaft is arranged coaxial to vertical axle
US10067231B2 (en) 2012-10-05 2018-09-04 Faro Technologies, Inc. Registration calculation of three-dimensional scanner data performed between scans based on measurements by two-dimensional scanner
US9513107B2 (en) 2012-10-05 2016-12-06 Faro Technologies, Inc. Registration calculation between three-dimensional (3D) scans based on two-dimensional (2D) scan data from a 3D scanner
DE102012109481A1 (en) 2012-10-05 2014-04-10 Faro Technologies, Inc. Device for optically scanning and measuring an environment
CN104898108A (en) * 2015-05-19 2015-09-09 浙江大学 Atmosphere remote sensing laser radar optical receiving device based on telescope arrays
DE102015122844A1 (en) 2015-12-27 2017-06-29 Faro Technologies, Inc. 3D measuring device with battery pack
WO2018011945A1 (en) * 2016-07-14 2018-01-18 三菱電機株式会社 Laser radar device
US10502830B2 (en) * 2016-10-13 2019-12-10 Waymo Llc Limitation of noise on light detectors using an aperture
JP7154230B2 (en) * 2017-05-15 2022-10-17 アウスター インコーポレイテッド Optical Imaging Transmitter with Enhanced Brightness
JP2019113377A (en) * 2017-12-22 2019-07-11 パイオニア株式会社 Detector
CN111708031B (en) * 2020-07-03 2025-02-07 山东省科学院海洋仪器仪表研究所 A laser radar
CN115754978B (en) * 2022-12-28 2023-06-06 安徽科创中光科技股份有限公司 Optical axis parallel adjustment method based on laser emission system and telescope receiving system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109407333A (en) * 2018-12-14 2019-03-01 中国科学院长春光学精密机械与物理研究所 The automated calibration system and calibration method of the acquisition and tracking optical axis and Laser emission axis
CN109407333B (en) * 2018-12-14 2020-04-10 中国科学院长春光学精密机械与物理研究所 Automatic calibration system and calibration method for capturing and tracking visual axis and laser emission axis

Also Published As

Publication number Publication date
JP2000121724A (en) 2000-04-28

Similar Documents

Publication Publication Date Title
JP3835016B2 (en) Laser radar equipment
CN101553707B (en) coordinate measuring equipment
KR101257586B1 (en) Optical axis adjusting apparatus, optical axis adjusting method, and projection type display apparatus
US7471396B2 (en) Dual polarization interferometers for measuring opposite sides of a workpiece
JP3979670B2 (en) 3D color imaging
WO2002038040A3 (en) Spectrally encoded miniature endoscopic imaging probe
JP4576664B2 (en) Optical path deviation detection device and confocal microscope
US6043891A (en) System for three-dimensional measurement of inaccessible hollow spaces
US6897421B2 (en) Optical inspection system having an internal rangefinder
RU2115878C1 (en) Device for monitoring of sight parameters of teleorientation system with radiating channels employing injection lasers
JP3688560B2 (en) Optical measuring device
JP2005017127A (en) Interferometer and shape measuring device
JP3575586B2 (en) Scratch inspection device
JP4834363B2 (en) Surface inspection device
JP3971023B2 (en) M2 measuring device
JPH0823484B2 (en) Device for orienting, inspecting and / or measuring two-dimensional objects
JPH09196630A (en) Optical constant measuring apparatus and microscope
JP2002162317A (en) Wavefront measurement device
JP7035122B2 (en) Optical interference tomographic imaging device and its adjustment method
Khanna et al. Integration of the optical sectioning microscope and heterodyne interferometer for vibration measurements
JP2010223775A (en) Interferometer
JPH11304640A (en) Optical element inspection device
JPH08166209A (en) Polygon mirror evaluating device
JPH11258058A (en) Optical heterodyne interference measuring device
JP3542171B2 (en) Microscope equipment

Legal Events

Date Code Title Description
RD01 Notification of change of attorney

Free format text: JAPANESE INTERMEDIATE CODE: A7421

Effective date: 20040622

A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20041028

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20051222

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20060117

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20060315

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20060418

A521 Written amendment

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20060609

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20060704

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20060717

LAPS Cancellation because of no payment of annual fees