JP2003172612A - Light irradiation light receiving device and light irradiation light receiving method - Google Patents
Light irradiation light receiving device and light irradiation light receiving methodInfo
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- JP2003172612A JP2003172612A JP2001375625A JP2001375625A JP2003172612A JP 2003172612 A JP2003172612 A JP 2003172612A JP 2001375625 A JP2001375625 A JP 2001375625A JP 2001375625 A JP2001375625 A JP 2001375625A JP 2003172612 A JP2003172612 A JP 2003172612A
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- light
- measured
- reflected
- irradiation
- beam splitter
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Abstract
(57)【要約】
【課題】 発光手段で発光した光を被計測物体に照射
し、前記被計測物体からの反射光を受光して撮像する光
照射受光装置において、オクルージョン領域をなくし、
かつ、撮影範囲と照射範囲の調節を容易にするととも
に、発光手段で発光した光のロスを低減する。
【解決手段】 被計測物体に照射する光を発光する発光
手段と、前記被計測物体で反射した光を受光して撮像す
る撮像手段と、前記被計測物体に照射する光の光軸と前
記撮像手段で受光する光の光軸と一致させる光軸一致手
段と、前記撮像手段で撮像する像の焦点を調節する焦点
調節手段とを備える光照射受光装置であって、前記発光
手段は、単色かつ直線偏光の光を発光する光源と、前記
光源で発光した光の照射角を調節する照射角調節手段と
を備え、前記光軸一致手段は、入射する光の偏光面の向
きに応じて、光を反射あるいは透過させる偏光ビームス
プリッタと、入射した光の偏光面を45度回転させるλ
/4波長板とを備え、前記λ/4波長板は、前記偏光ビ
ームスプリッタと前記被計測物体との間に配置されてい
る光照射受光装置である。
(57) [PROBLEMS] To provide a light irradiation and light receiving device for irradiating light emitted from a light emitting means to an object to be measured and receiving reflected light from the object to be imaged to eliminate an occlusion area;
In addition, the adjustment of the photographing range and the irradiation range is facilitated, and the loss of light emitted by the light emitting means is reduced. SOLUTION: A light emitting unit that emits light for irradiating an object to be measured, an imaging unit that receives light reflected by the object to be imaged and captures an image, an optical axis of the light that irradiates the object to be measured, and the imaging An optical axis matching unit that matches an optical axis of light received by the unit, and a light irradiation and light receiving device including a focus adjustment unit that adjusts a focus of an image captured by the imaging unit, wherein the light emitting unit is monochromatic and A light source that emits linearly polarized light; and an irradiation angle adjusting unit that adjusts an irradiation angle of the light emitted by the light source, wherein the optical axis matching unit is configured to emit light in accordance with a direction of a polarization plane of incident light. And a polarization beam splitter for reflecting or transmitting light, and a λ for rotating the polarization plane of the incident light by 45 degrees.
A λ / 4 wavelength plate, wherein the λ / 4 wavelength plate is a light irradiation light receiving device disposed between the polarization beam splitter and the object to be measured.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、被計測物体に光を
照射し、前記被計測物体からの反射光を受光する光照射
受光装置及び光照射受光方法に関し、特に、前記被計測
物体の三次元形状計測やパターン計測に適用して有効な
技術に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a light irradiation / light receiving device and a light irradiation / light receiving method for irradiating an object to be measured with light and receiving reflected light from the object to be measured. The present invention relates to a technique effectively applied to original shape measurement and pattern measurement.
【0002】[0002]
【従来の技術】従来、カメラを用いて被写体(被計測物
体)の三次元形状を入力する方法には、さまざまな方法
があり、例えば、アクティブ型計測法が多く用いられて
いる。前記アクティブ型計測法は、例えば、図11に示
すように、発光手段3から発光される人工的な光を被計
測物体2に照射し、前記被計測物体2からの反射光をカ
メラ等の撮像手段4で受光し、処理することによって、
前記被計測物体2の三次元形状を求める方法である。こ
のとき、前記被計測物体2の三次元形状は、例えば、飛
行時間法(Time of Flight法)を用いて求める。2. Description of the Related Art Conventionally, there are various methods for inputting a three-dimensional shape of a subject (object to be measured) using a camera, for example, an active measurement method is often used. In the active measurement method, for example, as shown in FIG. 11, the object to be measured 2 is irradiated with artificial light emitted from the light emitting means 3, and the reflected light from the object to be measured 2 is captured by a camera or the like. By receiving light by means 4 and processing,
This is a method for obtaining the three-dimensional shape of the measured object 2. At this time, the three-dimensional shape of the measured object 2 is obtained using, for example, the time of flight method.
【0003】前記飛行時間法を用いて三次元形状を求め
るには、例えば、前記発光手段3でパルス光を発光して
前記被計測物体2に照射し、前記撮像手段4で、シャッ
ターを高速に切りながら前記被計測物体2を撮影する。
このとき、前記発光手段3から照射された光は、前記被
計測物体2の部位毎に、前記発光手段3から被計測物体
2までの距離と、前記被計測物体2から前記撮像手段4
までの距離の和に応じて、前記撮像手段2に到達するま
で時間(走行時間)にばらつきが生じる。例えば、図1
1に示したような、L字型の被計測物体2に光を照射し
たときには、前記被計測物体2の後方、言い換えると前
記発光手段3及び撮像手段4から遠い部分で反射した光
は、前記被計測物体の前方、言い換えると前記発光手段
3及び撮像手段4に近い部分で反射した光よりも走行時
間が長くなる。そのため、前記被計測物体2の後方で反
射した光は、前記撮像手段4に到達する時間に遅れが生
じ、シャッター時間内に前記撮像手段4に届く光量が少
なくなる。In order to obtain a three-dimensional shape using the time-of-flight method, for example, the light emitting means 3 emits pulsed light to irradiate the object 2 to be measured, and the image pickup means 4 moves the shutter at high speed. The object 2 to be measured is photographed while cutting.
At this time, the light emitted from the light emitting means 3 is, for each part of the measured object 2, the distance from the light emitting means 3 to the measured object 2 and the measured object 2 to the imaging means 4.
Depending on the sum of the distances up to, the time (traveling time) varies until the image pickup unit 2 is reached. For example, in FIG.
As shown in FIG. 1, when the L-shaped object to be measured 2 is irradiated with light, the light reflected at the rear of the object to be measured 2, in other words, the part far from the light emitting means 3 and the imaging means 4, is The traveling time becomes longer than the light reflected in front of the measured object, in other words, in the portion near the light emitting means 3 and the imaging means 4. Therefore, the light reflected behind the measured object 2 has a delay in reaching the image pickup means 4, and the amount of light reaching the image pickup means 4 within the shutter time is reduced.
【0004】すなわち、前記撮像手段4で撮像された画
像は、前記発光手段3及び前記撮像手段4から遠い部分
で反射された光を受光した領域が暗くなり、被計測物体
2の形状に対応した輝度の濃淡値が得られる。そこで、
前記撮像画像の輝度の濃淡値から、前記被計測物体の各
部位と撮像手段の間の距離を算出して前記被計測物体の
形状を求める。That is, in the image picked up by the image pickup means 4, the area where the light reflected by the light emitting means 3 and the portion far from the image pickup means 4 is received becomes dark and corresponds to the shape of the object 2 to be measured. The brightness value of the brightness is obtained. Therefore,
The shape of the object to be measured is obtained by calculating the distance between each part of the object to be measured and the imaging means from the gray value of the brightness of the captured image.
【0005】前記アクティブ型計測法は、高信頼性及び
高精度であるため、実用段階に供されている技術も多
い。しかしながら、従来のアクティブ型計測法では、前
記発光手段3と前記撮像手段4が、空間的に異なる位置
にあり、前記発光手段3から照射される光の光軸と、前
記撮像手段で受光する光の光軸が空間的に異なる。その
ため、前記被計測物体2の形状によっては、図12に示
すように、前記撮像手段4で撮像する範囲θ1を照射す
るように前記発光手段3の照射角θ2を設定しても、前
記発光手段3からの光があたらない領域(オクルージョ
ン領域)S3が発生することがある。前記オクルージョ
ン領域S3には光があたらないため、前記オクルージョ
ン領域S3内の形状を計測できないという問題がある。Since the active measuring method has high reliability and high accuracy, many techniques are put into practical use. However, in the conventional active measurement method, the light emitting means 3 and the imaging means 4 are spatially different positions, and the optical axis of the light emitted from the light emitting means 3 and the light received by the imaging means. The optical axes of are spatially different. Therefore, depending on the shape of the object to be measured 2, as shown in FIG. 12, even if the irradiation angle θ2 of the light emitting means 3 is set so as to irradiate the range θ1 imaged by the imaging means 4, the light emitting means 2 is set. There may occur a region (occlusion region) S3 where the light from 3 does not reach. Since the occlusion area S3 is not exposed to light, there is a problem that the shape in the occlusion area S3 cannot be measured.
【0006】また、図12に示したような配置の場合、
前記発光手段3で、前記撮像手段4で撮影する範囲θ1
を照射するには、照射角θ2で光を照射する必要がある
が、このとき、前記被計測物体2の、前記撮像手段4で
撮影されない領域S4にも光が照射される。前記発光手
段3から照射される光の単位面積あたりの光量は、照射
面積に反比例するため、図12に示したように、前記撮
像手段4で撮影されない領域S4にも光を照射すると、
前記発光手段3で発光した光の光量に無駄が生じる。そ
のため、限られた出力の照明光を有効に利用できないと
いう問題がある。In the case of the arrangement shown in FIG. 12,
A range θ1 in which the light emitting unit 3 captures an image with the image capturing unit 4
In order to irradiate, the light needs to be irradiated at an irradiation angle θ2, and at this time, the region S4 of the measured object 2 that is not imaged by the imaging unit 4 is also irradiated with light. The amount of light emitted from the light emitting unit 3 per unit area is inversely proportional to the irradiation area. Therefore, as shown in FIG. 12, when the region S4 that is not imaged by the image capturing unit 4 is also irradiated with light,
The amount of light emitted by the light emitting means 3 is wasted. Therefore, there is a problem that the limited output illumination light cannot be effectively used.
【0007】また、前記撮像手段4は、レンズを交換す
る、あるいはズームレンズを用いることにより、撮影範
囲を変更することが可能である。このとき、前記撮像手
段4で広角の撮影をする場合には、図13に示すよう
に、照射光の光軸AX2が前記撮像手段4で受光する光
の光軸AX1と異なっていても、前記撮像手段4の撮影
範囲θ1の広さに合わせて、前記発光手段3の照射角θ
2を広くすることで、前記被計測物体2の全体に光を照
射することができる。Further, the image pickup means 4 can change the photographing range by exchanging the lens or using a zoom lens. At this time, when a wide-angle image is taken by the image pickup means 4, even if the optical axis AX2 of the irradiation light is different from the optical axis AX1 of the light received by the image pickup means 4 as shown in FIG. The irradiation angle θ of the light emitting means 3 is adjusted according to the width of the photographing range θ1 of the image pickup means 4.
By making 2 wide, it is possible to irradiate the entire measured object 2 with light.
【0008】しかしながら、図13に示した状態で、例
えば、前記撮像手段4の撮影範囲θ1を狭くして、図1
4に示すように、被計測物体2の一部S5を拡大して撮
影する場合、前記発光手段3の照射角θ2も狭くして、
光量を増大し、無駄な光を少なくすることが考えられる
が、前記照射光の光軸AX2が受光する光の光軸AX1
とずれている場合には、図14に示したように、照射範
囲と撮影範囲にずれが出て、撮影範囲内に光のあたらな
い領域S5‘ができてしまうという問題がある。However, in the state shown in FIG. 13, for example, by narrowing the photographing range θ1 of the image pickup means 4,
4, when enlarging and photographing a part S5 of the measured object 2, the irradiation angle θ2 of the light emitting means 3 is also narrowed,
It is conceivable to increase the amount of light and reduce unnecessary light, but the optical axis AX1 of the light received by the optical axis AX2 of the irradiation light is considered.
If there is a deviation, as shown in FIG. 14, there is a problem that there is a deviation between the irradiation range and the shooting range, and a region S5 'where no light is shining is created within the shooting range.
【0009】また、図14に示したような、照射範囲と
撮影範囲のずれをなくすためには、前記撮影範囲の変更
に合わせて、前記発光手段3の光軸も調整する必要があ
り、作業の手間がかかるという問題がある。また、前記
発光手段3で発光する光が赤外光などの不可視光の場合
には、調節作業が困難であるという問題がある。前記ア
クティブ型計測方法における各問題は、前記発光手段3
から照射される光の光軸と前記撮像手段4で受光する光
の光軸が異なるために生じる問題であるため、前記照射
する光の光軸と受光する光の光軸を一致させることで解
決できる。Further, in order to eliminate the deviation between the irradiation range and the photographing range as shown in FIG. 14, it is necessary to adjust the optical axis of the light emitting means 3 in accordance with the change of the photographing range. There is a problem that it takes time. Further, when the light emitted from the light emitting means 3 is invisible light such as infrared light, there is a problem that adjustment work is difficult. Each problem in the active measuring method is caused by the light emitting means 3
This is a problem that occurs because the optical axis of the light emitted from the optical axis and the optical axis of the light received by the imaging unit 4 are different. Therefore, it is solved by making the optical axis of the emitted light and the optical axis of the received light coincide with each other. it can.
【0010】前記照射する光の光軸と受光する光の光軸
を一致させる方法としては、図15に示すように、ハー
フミラー10を用いる方法が提案されている。前記ハー
フミラー10を用いる場合、例えば、前記発光手段3で
発光した光をハーフミラー10に入射し、前記ハーフミ
ラー10で反射した光を前記被計測物体2に照射する。
また、前記被計測物体2で反射した光は、前記被計測物
体2に照射される光と同じ光軸を通り再び前記ハーフミ
ラー10に入射されるので、前記ハーフミラー8を透過
した光を前記撮像装置4で受光し、撮像することで、前
記各問題を解決することができる。As a method of making the optical axis of the radiated light and the optical axis of the received light coincide with each other, a method using a half mirror 10 has been proposed as shown in FIG. When the half mirror 10 is used, for example, the light emitted by the light emitting unit 3 is incident on the half mirror 10 and the light reflected by the half mirror 10 is applied to the measured object 2.
Further, since the light reflected by the measured object 2 passes through the same optical axis as the light irradiated on the measured object 2 and is incident on the half mirror 10 again, the light transmitted through the half mirror 8 is Each of the above problems can be solved by receiving light by the image pickup device 4 and picking up an image.
【0011】しかしながら、前記ハーフミラー10は、
入射した光の光量の半分が透過し、残りの半分が反射す
るため、前記発光手段3で発光した光の光量Pの半分だ
けが前記被計測物体2に照射されることになる。また、
前記被計測物体2で反射した光も、光量の半分だけが前
記ハーフミラー10を透過して前記撮像手段4で受光さ
れる。そのため、前記被計測物体2に照射した光の光量
の100%が反射したとしても、前記撮像手段4で受光
する光の光量は、前記発光手段3で発光した光の光量P
の4分の1になり、ロスが多いという問題があった。However, the half mirror 10 is
Since half of the light amount of the incident light is transmitted and the other half is reflected, only the half of the light amount P of the light emitted by the light emitting means 3 is applied to the measured object 2. Also,
Only half of the light reflected by the measured object 2 passes through the half mirror 10 and is received by the imaging unit 4. Therefore, even if 100% of the light amount of the light irradiated to the measured object 2 is reflected, the light amount of the light received by the imaging unit 4 is the light amount P of the light emitted by the light emitting unit 3.
There was a problem that there was a lot of loss.
【0012】[0012]
【発明が解決しようとする課題】前記従来の技術で説明
したように、照射する光の光軸と受光する光の光軸が異
なる場合には、図12及び図14に示したように、オク
ルージョン領域が発生するという問題や、撮影領域外に
照射される無駄な光があるという問題があった。また、
図15に示したようなハーフミラー10を用いた方法で
は、光のロスが多いという問題があった。As described in the above-mentioned prior art, when the optical axis of the emitted light and the optical axis of the received light are different from each other, as shown in FIGS. 12 and 14, occlusion occurs. There is a problem that a region is generated, and there is a problem that there is useless light that is emitted outside the photographing region. Also,
The method using the half mirror 10 as shown in FIG. 15 has a problem that a lot of light is lost.
【0013】本発明の目的は、発光手段で発光した光を
被計測物体に照射し、前記被計測物体からの反射光を受
光して撮像する光照射受光装置において、オクルージョ
ン領域をなくすことが可能な技術を提供することにあ
る。本発明の他の目的は、発光手段で発光した光を被計
測物体に照射し、前記被計測物体からの反射光を受光し
て撮像する光照射受光装置において、撮像範囲と照射範
囲の調節を容易にすることが可能な技術を提供すること
にある。本発明の他の目的は、発光手段で発光した光を
被計測物体に照射し、前記被計測物体からの反射光を受
光して撮像する光照射受光装置において、発光手段で発
光した光のロスを低減することが可能な技術を提供する
ことにある。本発明の他の目的は、発光手段で発光した
光を被計測物体に照射し、前記被計測物体からの反射光
を受光して撮像する光照射受光装置において、オクルー
ジョン領域をなくし、かつ、撮影範囲と照射範囲の調節
を容易にするとともに、発光手段で発光した光のロスを
低減することが可能な技術を提供することにある。本発
明の前記ならびにその他の目的と新規な特徴は、本明細
書の記述及び添付図面によって明らかする。An object of the present invention is to eliminate an occlusion area in a light irradiation / light receiving device that irradiates light to be measured by a light emitting means onto an object to be measured and receives reflected light from the object to be measured to capture an image. To provide various technologies. Another object of the present invention is to adjust an imaging range and an irradiation range in a light irradiation and reception device that irradiates light to be measured by a light emitting means to an object to be measured and receives reflected light from the object to be measured to capture an image. It is to provide a technology that can be facilitated. Another object of the present invention is to provide a light irradiation and reception device which irradiates light to be measured by the light emitting means onto a measured object, receives reflected light from the measured object, and picks up an image. It is to provide a technology capable of reducing the above. Another object of the present invention is to eliminate the occlusion area in a light irradiation and reception device that irradiates the light to be measured by the light emitting means to the object to be measured, receives the reflected light from the object to be measured, and captures the image. It is an object of the present invention to provide a technique capable of easily adjusting the range and the irradiation range and reducing the loss of the light emitted by the light emitting means. The above and other objects and novel features of the present invention will be apparent from the description of this specification and the accompanying drawings.
【0014】[0014]
【課題を解決するための手段】本願において開示される
発明の概要を説明すれば、以下のとおりである。第1の
発明は、被計測物体に照射する光を発光する発光手段
と、前記被計測物体で反射した光を受光して撮像する撮
像手段と、前記被計測物体に照射する光の光軸と前記撮
像手段で受光する光の光軸と一致させる光軸一致手段
と、前記撮像手段で撮像する像の焦点を調節する焦点調
節手段とを備える光照射受光装置であって、前記発光手
段は、単色かつ直線偏光の光を発光する光源と、前記光
源で発光した光の照射角を調節する照射角調節手段とを
備え、前記光軸一致手段は、入射する光の偏光面の向き
に応じて、光を反射あるいは透過させる偏光ビームスプ
リッタと、入射した光の偏光面を45度回転させるλ/
4波長板とを備え、前記λ/4波長板は、前記偏光ビー
ムスプリッタと前記被計測物体との間に配置されている
光照射受光装置である。The outline of the invention disclosed in the present application is as follows. According to a first aspect of the present invention, a light emitting unit that emits light that irradiates an object to be measured, an imaging unit that receives and images the light reflected by the object to be measured, and an optical axis of light that irradiates the object to be measured. A light irradiation and reception device comprising: an optical axis matching means for matching the optical axis of light received by the image pickup means; and a focus adjustment means for adjusting the focus of an image picked up by the image pickup means, wherein the light emitting means comprises: A light source that emits monochromatic and linearly polarized light, and an irradiation angle adjusting means that adjusts the irradiation angle of the light emitted by the light source, the optical axis matching means, depending on the direction of the polarization plane of the incident light. , A polarizing beam splitter that reflects or transmits light, and λ / that rotates the plane of polarization of incident light by 45 degrees.
And a λ / 4 wavelength plate, which is a light irradiation and reception device disposed between the polarization beam splitter and the object to be measured.
【0015】第2の発明は、前記第1の発明において、
前記光軸一致手段及び前記焦点調節手段は、前記被計測
物体と前記撮像手段とを結ぶ直線上に、前記被計測物体
側から、前記焦点調節手段、前記光軸一致手段の順に配
置され、前記光源は、発光した光の偏光面が前記偏光ビ
ームスプリッタで反射される向きになり、かつ、前記偏
光ビームスプリッタで反射した光が前記被計測物体に照
射されるように配置されており、前記照射角調節手段
は、前記光源と前記偏光ビームスプリッタの間に配置さ
れている光照射受光装置である。A second invention is the same as the first invention,
The optical axis matching means and the focus adjusting means are arranged on the straight line connecting the object to be measured and the imaging means in the order of the focus adjusting means and the optical axis matching means from the object to be measured side, The light source is arranged such that the plane of polarization of the emitted light is in a direction to be reflected by the polarization beam splitter, and the light reflected by the polarization beam splitter is applied to the object to be measured. The angle adjusting means is a light emitting and receiving device arranged between the light source and the polarization beam splitter.
【0016】第3の発明は、前記第1の発明において、
前記光軸一致手段及び前記焦点調節手段は、前記被計測
物体と前記発光手段とを結ぶ直線上に、前記被計測物体
側から、前記焦点調節手段、前記光軸一致手段の順に配
置され、前記光源は、発光した光の偏光面が、前記偏光
ビームスプリッタを透過する向きになるように配置さ
れ、前記撮像手段は、前記被計測物体からの反射光が、
前記偏光ビームスプリッタで反射する方向に配置されて
おり、前記照射角調節手段は、前記光源と前記偏光ビー
ムスプリッタの間に配置されている光照射受光装置であ
る。A third invention is the same as the first invention,
The optical axis matching means and the focus adjusting means are arranged in this order from the object to be measured on the straight line connecting the object to be measured and the light emitting means, the focus adjusting means and the optical axis matching means, The light source is arranged so that the plane of polarization of the emitted light is in a direction of passing through the polarization beam splitter, and the image pickup means is such that the reflected light from the measured object is
The irradiation angle adjusting means is a light irradiation and reception device which is arranged in a direction of being reflected by the polarization beam splitter and is arranged between the light source and the polarization beam splitter.
【0017】前記第1の発明、前記第2の発明、及び前
記第3の発明によれば、前記光軸一致手段を設けること
により、前記発光手段で発光した光、すなわち前記被計
測物体に照射する光の光軸と、前記被計測物体で反射
し、前記撮像手段で受光される光の光軸を同一軸上にす
ることができる。そのため、前記撮像手段で撮像する範
囲内に、前記光が照射されない領域(オクルージョン領
域)が発生することを防げる。According to the first invention, the second invention, and the third invention, by providing the optical axis matching means, the light emitted by the light emitting means, that is, the object to be measured is irradiated. The optical axis of the light to be reflected and the optical axis of the light reflected by the object to be measured and received by the imaging unit can be on the same axis. Therefore, it is possible to prevent a region (occlusion region) not irradiated with the light from being generated in the range captured by the image capturing unit.
【0018】また、前記発光手段に、前記照射角調節手
段を設けることにより、前記被計測物体の光が照射され
る領域を、前記撮像手段で撮影する範囲にあわせること
ができる。そのため、前記発光手段で発光した光が前記
撮像手段で撮影する範囲外に照射されたり、前記図14
に示したように、撮影範囲と照射領域にずれが生じたり
することを防げ、前記発光手段で発光した光の光量を有
効に利用することができる。またこのとき、前記被計測
物体に照射する光の光軸と、前記被計測物体で反射し、
前記撮像手段で受光される光の光軸が同一軸上であるた
め、撮像範囲の変更をした場合に、照射する光の照射角
を調節するだけでよく、光の照射範囲の調節が容易であ
る。Further, by providing the light emitting means with the irradiation angle adjusting means, it is possible to match the area of the object to be measured, which is irradiated with the light, with the range taken by the imaging means. Therefore, the light emitted by the light emitting unit is applied to the outside of the image capturing range of the image capturing unit, or the light shown in FIG.
As described above, it is possible to prevent the occurrence of a shift between the photographing range and the irradiation region, and it is possible to effectively use the light amount of the light emitted by the light emitting means. At this time, the optical axis of the light irradiating the measured object, and reflected by the measured object,
Since the optical axes of the light received by the image pickup means are on the same axis, it is only necessary to adjust the irradiation angle of the light to be emitted when the image pickup range is changed, and it is easy to adjust the light irradiation range. is there.
【0019】また、前記光軸一致手段として、前記偏光
ビームスプリッタ及び前記λ/4波長板を用い、前記光
源で発光した光を、前記偏光ビームスプリッタで反射あ
るいは透過させて被計測物体に照射することにより、前
記光源で発光した光の光量のほぼ100%を前記被計測
物体に照射することができる。このとき、前記被計測物
体に照射される光は、前記λ/4波長板で偏光面が45
度回転し、円偏光に変わって照射される。Further, the polarization beam splitter and the λ / 4 wavelength plate are used as the optical axis matching means, and the light emitted from the light source is reflected or transmitted by the polarization beam splitter to irradiate the object to be measured. As a result, almost 100% of the amount of light emitted from the light source can be applied to the measured object. At this time, the light radiated to the object to be measured has a polarization plane of 45 with the λ / 4 wavelength plate.
It is rotated once and is changed to circularly polarized light.
【0020】また、前記被計測物体で反射した光(反射
光)は、一般に、前記被計測物体に照射したときの円偏
光のほかに、無偏光が混合した状態である。前記反射光
に含まれる円偏光は、前記λ/4波長板で、前記光源で
発光した光の偏光面と直交する偏光面の直線偏光になる
ので、前記偏光ビームスプリッタで透過あるいは反射
し、前記撮像手段で受光される。このとき、前記撮像手
段で受光される光の光量は、前記円偏光と無偏光の割合
によるが、前記被計測物体で反射した光の光量の50%
から100%になる。The light reflected by the object to be measured (reflected light) is generally a state in which unpolarized light is mixed in addition to circularly polarized light when the object to be measured is irradiated. The circularly polarized light included in the reflected light becomes linearly polarized light of the polarization plane orthogonal to the polarization plane of the light emitted from the light source in the λ / 4 wavelength plate, and thus is transmitted or reflected by the polarization beam splitter. The light is received by the imaging means. At this time, the light quantity of the light received by the imaging means depends on the ratio of the circularly polarized light and the non-polarized light, but is 50% of the light quantity of the light reflected by the measured object.
To 100%.
【0021】また、前記被計測物体では、照射した光の
ほとんどが反射するため、前記撮像手段で受光される光
の光量は、前記光源で発光した光の光量の50%から1
00%になる。そのため、従来のハーフミラーを用いた
装置に比べ、光のロスを低減することができ、光を有効
に利用することができる。また、前記光照射受光装置の
各構成要素は、例えば、前記第2の発明に示したように
配置する。Since most of the emitted light is reflected by the object to be measured, the amount of light received by the image pickup means is 50% to 1% of the amount of light emitted by the light source.
It will be 00%. Therefore, the loss of light can be reduced and the light can be effectively used as compared with the conventional device using the half mirror. Further, the respective constituent elements of the light irradiation / reception device are arranged, for example, as shown in the second invention.
【0022】前記第2の発明に示した配置の場合、前記
光源で発光した直線偏光は、前記偏光ビームスプリッタ
で反射し、前記λ/4波長板で偏光面が45度回転し円
偏光に変わり、前記被計測物体に照射される。前記被計
測物体で反射した光は、一般に、円偏光と無偏光が混合
した光であり、円偏光は前記λ/4波長板で偏光面が4
5度回転し、前記光源で発光した光の偏光面と直交する
偏光面の直線偏光に変わる。そのため、前記偏光ビーム
スプリッタを透過し、前記撮像手段で受光することがで
きる。また、前記光照射受光装置の各構成要素は、前記
第2の発明に示した配置に限らず、前記第3の発明に示
したように配置してもよい。In the case of the arrangement of the second aspect of the invention, the linearly polarized light emitted from the light source is reflected by the polarization beam splitter, and the plane of polarization is rotated by 45 ° by the λ / 4 wavelength plate to change to circularly polarized light. The object to be measured is irradiated. The light reflected by the measured object is generally a mixture of circularly polarized light and non-polarized light, and the circularly polarized light has a polarization plane of 4 with the λ / 4 wavelength plate.
The light is rotated by 5 degrees and is converted into linearly polarized light having a polarization plane orthogonal to the polarization plane of the light emitted from the light source. Therefore, the light can be transmitted through the polarization beam splitter and received by the imaging unit. Further, each component of the light irradiation / reception device is not limited to the arrangement shown in the second invention, and may be arranged as shown in the third invention.
【0023】前記第3の発明に示した配置の場合、前記
光源で発光した直線偏光は、前記偏光ビームスプリッタ
を透過し、前記λ/4波長板で偏光面が45度回転し円
偏光に変わり、前記被計測物体に照射される。前記被計
測物体で反射した光は、一般に、円偏光と無偏光が混合
した光であり、円偏光は前記λ/4波長板で偏光面が4
5度回転し、光源で発光した光の偏光面と直交する偏光
面の光に変わる。そのため、前記偏光ビームスプリッタ
で反射し、前記撮像手段で受光することができる。In the case of the arrangement shown in the third aspect, the linearly polarized light emitted from the light source passes through the polarization beam splitter, and the plane of polarization is rotated by 45 degrees by the λ / 4 wavelength plate to be changed to circularly polarized light. The object to be measured is irradiated. The light reflected by the measured object is generally a mixture of circularly polarized light and non-polarized light, and the circularly polarized light has a polarization plane of 4 with the λ / 4 wavelength plate.
It rotates 5 degrees and changes to the light of the polarization plane orthogonal to the polarization plane of the light emitted from the light source. Therefore, it can be reflected by the polarization beam splitter and received by the image pickup means.
【0024】第4の発明は、被計測物体に照射する赤外
光を発光する赤外光発光手段と、前記被計測物体で反射
した赤外光を受光して撮像する第1撮像手段と、前記被
計測物体に照射する赤外光の光軸と、前記第1撮像手段
で受光する赤外光の光軸を一致させる光軸一致手段と、
前記第1撮像手段で撮像する像の焦点を調節する焦点調
節手段と、前記被計測物体で反射した光を赤外光と可視
光に分離する光分離手段と、前記光分離手段によって分
離した可視光を受光して撮像する第2撮像手段を備える
光照射受光装置であって、前記赤外光発光手段は、直線
偏光の赤外光を発光する赤外光源と、前記赤外光源で発
光した赤外光の照射角を調節する照射角調節手段とを備
え、前記光軸一致手段は、入射する光の偏光面の向きに
応じて光を反射あるいは透過させる偏光ビームスプリッ
タと、入射した光の偏光面を45度回転させるλ/4波
長板とを備え、前記光分離手段及び前記λ/4波長板
は、前記偏光ビームスプリッタと前記被計測物体との間
に、前記被計測物体側から、前記光分離手段、前記λ/
4波長板の順に配置されている光照射受光装置である。A fourth invention is an infrared light emitting means for emitting infrared light to irradiate an object to be measured, and a first imaging means for receiving and imaging the infrared light reflected by the object to be measured, Optical axis matching means for matching the optical axis of infrared light with which the object to be measured is irradiated with the optical axis of infrared light received by the first imaging means,
Focus adjustment means for adjusting the focus of the image captured by the first imaging means, light separation means for separating the light reflected by the measured object into infrared light and visible light, and visible light separated by the light separation means. It is a light irradiation light-receiving device provided with a 2nd imaging means which light-receives and images light, Comprising: The said infrared-light emission means emitted the infrared light source which emits linearly polarized infrared light, and the said infrared light source. An irradiation angle adjusting means for adjusting an irradiation angle of infrared light is provided, and the optical axis matching means is a polarization beam splitter for reflecting or transmitting light according to a direction of a polarization plane of the incident light, and a polarization beam splitter for the incident light. A λ / 4 wavelength plate for rotating the plane of polarization by 45 degrees, wherein the light splitting means and the λ / 4 wavelength plate are located between the polarization beam splitter and the measured object from the measured object side, The light splitting means, the λ /
It is a light irradiation and reception device in which four wavelength plates are arranged in this order.
【0025】第5の発明は、前記第4の発明において、
前記光分離手段は、赤外光を透過し、可視光を反射する
コールドミラーであり、前記焦点調節手段、前記コール
ドミラー、前記λ/4波長板、及び前記偏光ビームスプ
リッタは、前記被計測物体と前記第1撮像手段とを結ぶ
直線上に、前記被計測物体側から、前記焦点調節手段、
前記コールドミラー、前記λ/4波長板、前記偏光ビー
ムスプリッタの順に配置され、前記赤外光源は、発光し
た赤外光の偏光面が前記偏光ビームスプリッタで反射す
る向きになり、かつ、前記偏光ビームスプリッタで反射
した光が前記被計測物体に照射されるように配置され、
前記第2撮像手段は、前記被計測物体からの可視光が前
記コールドミラーで反射する方向に配置されている光照
射受光装置である。A fifth aspect of the invention is the same as the fourth aspect of the invention.
The light separating unit is a cold mirror that transmits infrared light and reflects visible light, and the focus adjusting unit, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are the object to be measured. On the straight line connecting the first image pickup means and the object to be measured from the focus adjusting means,
The cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are arranged in this order, and the infrared light source is such that the polarization plane of the emitted infrared light is reflected by the polarization beam splitter, and Arranged so that the light reflected by the beam splitter irradiates the measured object,
The second image pickup means is a light irradiation and reception device which is arranged in a direction in which visible light from the measured object is reflected by the cold mirror.
【0026】第6の発明は、前記第4の発明において、
前記光分離手段は、赤外光を透過し、可視光を反射する
コールドミラーであり、前記焦点調節手段、前記コール
ドミラー、前記λ/4波長板、及び前記偏光ビームスプ
リッタは、前記被計測物体と前記赤外光発光手段とを結
ぶ直線上に、前記被計測物体側から、前記焦点調節手
段、前記コールドミラー、前記λ/4波長板、前記偏光
ビームスプリッタの順に配置され、前記赤外光源は、発
光した赤外光の偏光面が前記偏光ビームスプリッタを透
過する向きになるように配置され、前記第1撮像手段
は、前記被計測物体で反射し、前記コールドミラー及び
前記λ/4波長板を通った赤外光が前記偏光ビームスプ
リッタで反射する方向に配置され、前記第2撮像手段
は、前記被計測物体からの可視光が前記コールドミラー
で反射する方向に配置されている光照射受光装置であ
る。A sixth invention is the same as the fourth invention,
The light separating unit is a cold mirror that transmits infrared light and reflects visible light, and the focus adjusting unit, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are the object to be measured. The focus adjustment means, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are arranged in this order from the object to be measured on a straight line connecting the infrared light emitting means and the infrared light source. Is arranged such that the plane of polarization of the emitted infrared light is oriented to pass through the polarization beam splitter, and the first imaging means reflects the object to be measured, and the cold mirror and the λ / 4 wavelength The infrared light that has passed through the plate is arranged in a direction that is reflected by the polarization beam splitter, and the second imaging unit is arranged in a direction that visible light from the measured object is reflected by the cold mirror. A light irradiating the light receiving device are.
【0027】第7の発明は、前記第4の発明において、
前記光分離手段は、赤外光を反射し、可視光を透過する
ホットミラーであり、前記ホットミラーと前記焦点調節
手段は、前記被計測物体と前記第2撮像手段とを結ぶ直
線上に、前記被計測物体側から前記焦点調節手段、前記
ホットミラーの順に配置され、前記λ/4波長板及び前
記偏光ビームスプリッタは、前記被計測物体からの赤外
光が前記ホットミラーで反射する方向であり、かつ、前
記ホットミラーと前記第1撮像手段とを結ぶ直線上に、
前記λ/4波長板、前記偏光ビームスプリッタの順に配
置され、前記赤外光源は、発光した赤外光の偏光面が前
記偏光ビームスプリッタで反射する向きになり、かつ、
前記被計測物体に照射されるように配置されている光照
射受光装置である。A seventh invention is the same as the fourth invention,
The light separating means is a hot mirror that reflects infrared light and transmits visible light, and the hot mirror and the focus adjusting means are on a straight line connecting the measured object and the second imaging means. The focus adjusting means and the hot mirror are arranged in this order from the measured object side, and the λ / 4 wavelength plate and the polarization beam splitter are arranged in a direction in which infrared light from the measured object is reflected by the hot mirror. And on a straight line connecting the hot mirror and the first imaging means,
The λ / 4 wavelength plate and the polarization beam splitter are arranged in this order, and the infrared light source has a polarization plane of the emitted infrared light reflected by the polarization beam splitter, and
It is a light irradiation and reception device arranged so as to irradiate the object to be measured.
【0028】第8の発明は、前記第4の発明において、
前記光分離手段は、赤外光を反射し、可視光を透過する
ホットミラーであり、前記ホットミラーと前記焦点調節
手段は、前記被計測物体と前記第2撮像手段とを結ぶ直
線上に、前記被計測物体側から、前記焦点調節手段、前
記ホットミラーの順に配置され、前記偏光ビームスプリ
ッタ及び前記λ/4波長板は、前記ホットミラーと前記
赤外光発光手段との間に、前記ホットミラー側から、前
記λ/4波長板、前記偏光ビームスプリッタの順に配置
され、前記赤外光源は、発光した赤外光の偏光面が前記
偏光ビームスプリッタを透過するような向きに配置さ
れ、前記第1撮像手段は、前記被計測物体で反射し、前
記ホットミラー及び前記λ/4波長板を通った赤外光
が、前記偏光ビームスプリッタで反射する方向に配置さ
れている光照射受光装置である。An eighth aspect of the invention is the same as the fourth aspect of the invention.
The light separating means is a hot mirror that reflects infrared light and transmits visible light, and the hot mirror and the focus adjusting means are on a straight line connecting the measured object and the second imaging means. From the object side to be measured, the focus adjusting means and the hot mirror are arranged in this order, and the polarization beam splitter and the λ / 4 wave plate are provided between the hot mirror and the infrared light emitting means. The λ / 4 wavelength plate and the polarization beam splitter are arranged in this order from the mirror side, and the infrared light source is arranged so that the polarization plane of the emitted infrared light passes through the polarization beam splitter. The first imaging means is a light irradiation and reception device arranged in a direction in which infrared light reflected by the object to be measured and passing through the hot mirror and the λ / 4 wavelength plate is reflected by the polarization beam splitter. A.
【0029】前記第4の発明、前記第5の発明、前記第
6の発明、前記第7の発明、及び前記第8の発明によれ
ば、前記赤外光源で発光した赤外光、すなわち前記被計
測物体に照射する赤外光の光軸と、前記被計測物体で反
射し、前記撮像手段で受光される赤外光の光軸を同一軸
上にすることができる。そのため、前記撮像手段で撮像
する範囲内に、前記赤外光が照射されない領域(オクル
ージョン領域)が発生することを防げる。According to the fourth invention, the fifth invention, the sixth invention, the seventh invention, and the eighth invention, the infrared light emitted from the infrared light source, that is, the The optical axis of infrared light that irradiates the object to be measured and the optical axis of infrared light that is reflected by the object to be measured and received by the imaging unit can be on the same axis. Therefore, it is possible to prevent a region (occlusion region) where the infrared light is not emitted from occurring in the range captured by the image capturing unit.
【0030】また、前記赤外光発光手段に、前記照射角
調節手段を設けることにより、前記被計測物体の赤外光
が照射される領域を、前記撮像手段で撮影する範囲にあ
わせることができる。そのため、前記赤外光源で発光し
た赤外光が前記撮像手段で撮影する範囲外に照射された
り、前記図14に示したように、撮影範囲と照射領域に
ずれが生じたりすることを防げ、前記赤外光源で発光し
た赤外光の光量を有効に利用することができる。またこ
のとき、前記被計測物体に照射する赤外光の光軸と、前
記被計測物体で反射し、前記撮像手段で受光される赤外
光の光軸が同一軸上であるため、撮像範囲の変更をした
場合に、照射する赤外光の照射角を調節するだけでよ
く、赤外光の照射範囲の調節が容易である。Further, by providing the irradiation angle adjusting means to the infrared light emitting means, it is possible to match the area of the object to be measured, which is irradiated with infrared light, with the range taken by the imaging means. . Therefore, it is possible to prevent the infrared light emitted from the infrared light source from being emitted to the outside of the range to be captured by the image capturing means, or the displacement between the capturing range and the irradiation region as shown in FIG. The amount of infrared light emitted from the infrared light source can be effectively used. At this time, since the optical axis of the infrared light that irradiates the measured object and the optical axis of the infrared light that is reflected by the measured object and received by the imaging unit are on the same axis, the imaging range When the above is changed, it is only necessary to adjust the irradiation angle of the infrared light to be irradiated, and it is easy to adjust the irradiation range of the infrared light.
【0031】また、前記光軸一致手段として、前記偏光
ビームスプリッタ及び前記λ/4波長板を用い、前記赤
外光源で発光した赤外光を、前記偏光ビームスプリッタ
で反射あるいは透過させて被計測物体に照射することに
より、前記赤外光源で発光した赤外光の光量のほぼ10
0%を前記被計測物体に照射することができる。このと
き、前記被計測物体に照射される赤外光は、前記λ/4
波長板で偏光面が45度回転し、円偏光に変わって照射
される。The polarization beam splitter and the λ / 4 wavelength plate are used as the optical axis matching means, and the infrared light emitted from the infrared light source is reflected or transmitted by the polarization beam splitter to be measured. By irradiating the object, the amount of infrared light emitted from the infrared light source is about 10
The measured object can be irradiated with 0%. At this time, the infrared light radiated to the measured object is the λ / 4.
The plane of polarization is rotated by 45 degrees by the wave plate, and the light is changed to circularly polarized light for irradiation.
【0032】また、前記被計測物体で反射した赤外光
(反射光)は、一般に、前記被計測物体に照射したとき
の円偏光のほかに、無偏光が混合した状態である。前記
反射光に含まれる円偏光は、前記λ/4波長板で、前記
赤外光源で発光した赤外光の偏光面と直交する偏光面の
直線偏光になるので、前記偏光ビームスプリッタで透過
あるいは反射し、前記撮像手段で受光される。このと
き、前記撮像手段で受光される赤外光の光量は、前記円
偏光と無偏光の割合によるが、前記被計測物体で反射し
た赤外光の光量の50%から100%になる。The infrared light (reflected light) reflected by the object to be measured is generally a state in which non-polarized light is mixed in addition to circularly polarized light when the object to be measured is irradiated. The circularly polarized light contained in the reflected light is linearly polarized in a polarization plane orthogonal to the polarization plane of the infrared light emitted from the infrared light source in the λ / 4 wavelength plate, and therefore is transmitted by the polarization beam splitter or It is reflected and received by the imaging means. At this time, the amount of infrared light received by the image pickup means is 50% to 100% of the amount of infrared light reflected by the object to be measured, although it depends on the ratio of circularly polarized light to non-polarized light.
【0033】また、前記被計測物体では、照射した赤外
光のほとんどが反射するため、前記撮像手段で受光され
る赤外光の光量は、前記赤外光源で発光した赤外光の光
量の50%から100%になる。そのため、従来のハー
フミラーを用いた装置に比べ、光のロスを低減すること
ができ、光を有効に利用することができる。また、前記
被計測物体に前記赤外光を照射する場合には、前記被計
測物体で反射する光に、前記被計測物体が存在する空間
の可視光(外光)も含まれているため、前記光分離手段
を設けて赤外光と可視光を分離することにより、前記第
1撮像手段では、赤外光だけの像を撮像することができ
る。Further, most of the irradiated infrared light is reflected by the object to be measured, so the amount of infrared light received by the imaging means is the amount of infrared light emitted by the infrared light source. From 50% to 100%. Therefore, the loss of light can be reduced and the light can be effectively used as compared with the conventional device using the half mirror. Further, when irradiating the measured object with the infrared light, the light reflected by the measured object also includes visible light (external light) in the space where the measured object exists, By providing the light separation means to separate infrared light and visible light, the first imaging means can capture an image of only infrared light.
【0034】またこのとき、前記光分離手段で分離され
た可視光の像を前記第2撮像手段で撮像することによ
り、前記被計測物体の色情報を取得できる。そのため、
前記第2撮像手段で撮影する範囲を前記第1撮像手段で
撮影する範囲と一致させておくことにより、前記被計測
物体の形状及び色を測定することができ、前記被計測物
体を認識しやすくなる。また、前記光分離手段として、
赤外光を透過し、可視光を反射するコールドミラーを用
いることができる。このとき、前記光照射受光装置の各
構成要素は、前記第5の発明に示したように配置する。At this time, the color information of the object to be measured can be obtained by capturing the image of the visible light separated by the light separating unit by the second image capturing unit. for that reason,
By making the range photographed by the second image pickup unit coincide with the range photographed by the first image pickup unit, the shape and color of the measured object can be measured, and the measured object can be easily recognized. Become. Further, as the light separating means,
A cold mirror that transmits infrared light and reflects visible light can be used. At this time, the respective constituent elements of the light irradiation / reception device are arranged as shown in the fifth invention.
【0035】前記第5の発明に示した配置の場合、前記
赤外光源で発光した赤外光は、前記偏光ビームスプリッ
タで反射し、前記λ/4波長板で偏光面を45度回転し
て円偏光に変わり、前記コールドミラーを透過して前記
被計測物体に照射される。前記被計測物体で反射した円
偏光の赤外光は、前記コールドミラーを透過し、前記λ
/4波長板で偏光面をさらに45度回転し、前記赤外光
源で発光した赤外光の偏光面と直交する偏光面の直線偏
光に変わる。そのため、前記偏光ビームスプリッタを透
過し、前記第1撮像手段で受光される。一方、前記被計
測物体で反射した可視光は、前記コールドミラーで反射
し、前記第2撮像手段で受光される。また、前記光分離
手段として、前記コールドミラーを用いた場合、前記光
照射受光装置の各構成要素は、前記第5の発明に示した
配置に限らず、第6の発明に示したような配置でもよ
い。In the case of the arrangement of the fifth invention, the infrared light emitted from the infrared light source is reflected by the polarization beam splitter, and the polarization plane is rotated by 45 degrees by the λ / 4 wavelength plate. It changes to circularly polarized light, passes through the cold mirror, and is irradiated onto the measured object. The circularly polarized infrared light reflected by the object to be measured passes through the cold mirror,
The polarization plane is further rotated by 45 degrees by the / 4 wavelength plate, and the polarization plane of the infrared light emitted from the infrared light source is changed to linear polarization. Therefore, the light passes through the polarization beam splitter and is received by the first imaging unit. On the other hand, the visible light reflected by the measured object is reflected by the cold mirror and is received by the second image pickup means. Further, when the cold mirror is used as the light separating means, each component of the light emitting and receiving device is not limited to the arrangement shown in the fifth invention, but the arrangement shown in the sixth invention. But it is okay.
【0036】前記第6の発明に示した配置の場合、前記
赤外光源で発光した赤外光は、前記偏光ビームスプリッ
タを透過し、前記λ/4波長板で偏光面を45度回転し
て円偏光に変わり、前記コールドミラーを透過して前記
被計測物体に照射される。前記被計測物体で反射した円
偏光の赤外光は、前記コールドミラーを透過し、前記λ
/4波長板で偏光面をさらに45度回転し、前記赤外光
源で発光した赤外光の偏光面と直交した偏光面の直線偏
光に変わる。そのため、前記偏光ビームスプリッタで反
射し、前記第1撮像手段で受光される。一方、前記被計
測物体で反射した可視光は、前記コールドミラーで反射
し、前記第2撮像手段で受光される。また、前記光分離
手段は、前記コールドミラーに限らず、赤外光を反射
し、可視光を透過するホットミラーを用いることもでき
る。前記ホットミラーを用いるときには、前記光照射受
光装置の各構成要素は、前記第7の発明に示したように
配置する。In the case of the arrangement shown in the sixth aspect, the infrared light emitted from the infrared light source passes through the polarization beam splitter, and the polarization plane is rotated by 45 degrees by the λ / 4 wavelength plate. It changes to circularly polarized light, passes through the cold mirror, and is irradiated onto the measured object. The circularly polarized infrared light reflected by the object to be measured passes through the cold mirror,
The polarization plane is further rotated by 45 degrees by the / 4 wavelength plate, and the polarization plane of the infrared light emitted from the infrared light source is changed to the linear polarization plane orthogonal to the polarization plane. Therefore, the light is reflected by the polarization beam splitter and received by the first image pickup means. On the other hand, the visible light reflected by the measured object is reflected by the cold mirror and is received by the second image pickup means. Further, the light separating means is not limited to the cold mirror, and a hot mirror that reflects infrared light and transmits visible light may be used. When the hot mirror is used, the respective constituent elements of the light irradiation / reception device are arranged as shown in the seventh invention.
【0037】前記第7の発明に示した配置の場合、前記
赤外光源で発光した赤外光は、前記偏光ビームスプリッ
タで反射し、前記λ/4波長板で偏光面を45度回転し
て円偏光に変わり、前記ホットミラーで反射した後、前
記被計測物体に照射される。前記被計測物体で反射した
円偏光の赤外光は、前記ホットミラーで反射し、前記λ
/4波長板で偏光面をさらに45度回転して、前記赤外
光源で発光した赤外光の偏光面と直交する偏光面の直線
偏光に変わる。そのため、前記偏光ビームスプリッタを
透過し、前記第1撮像手段で受光される。一方、前記被
計測物体で反射した可視光は、前記ホットミラーを透過
し、前記第2撮像手段で受光される。また、前記光分離
手段として、前記ホットミラーを用いる場合、前記光照
射受光装置の各構成要素は、前記第7の発明に示した配
置に限らず、前記第8の発明に示したような配置であっ
てもよい。In the case of the arrangement of the seventh invention, the infrared light emitted from the infrared light source is reflected by the polarization beam splitter, and the polarization plane is rotated by 45 degrees by the λ / 4 wavelength plate. After being changed to circularly polarized light and reflected by the hot mirror, the object to be measured is irradiated. The circularly polarized infrared light reflected by the measured object is reflected by the hot mirror,
The polarization plane is further rotated by 45 degrees by the / 4 wavelength plate, and the polarization plane of the infrared light emitted from the infrared light source is changed to linear polarization. Therefore, the light passes through the polarization beam splitter and is received by the first imaging unit. On the other hand, the visible light reflected by the measured object passes through the hot mirror and is received by the second imaging means. Further, when the hot mirror is used as the light separating means, each component of the light emitting and receiving device is not limited to the arrangement shown in the seventh invention, but the arrangement as shown in the eighth invention. May be
【0038】前記第8の発明に示した配置の場合、前記
赤外光源で発光した赤外光は、前記偏光ビームスプリッ
タを透過し、前記λ/4波長板で偏光面を45度回転し
て円偏光に変わり、前記ホットミラーで反射した後、前
記被計測物体に照射される。前記被計測物体で反射した
円偏光の赤外光は、前記ホットミラーで反射し、前記λ
/4波長板で偏光面をさらに45度回転して、前記赤外
光源で発光した赤外光の偏光面と直交する偏光面の直線
偏光に変わる。そのため、前記偏光ビームスプリッタで
反射し、前記第1撮像手段で受光される。一方、前記被
計測物体で反射した可視光は、前記ホットミラーを透過
し、前記第2撮像手段で受光される。In the case of the arrangement of the eighth invention, the infrared light emitted from the infrared light source passes through the polarization beam splitter and the polarization plane is rotated by 45 degrees by the λ / 4 wavelength plate. After being changed to circularly polarized light and reflected by the hot mirror, the object to be measured is irradiated. The circularly polarized infrared light reflected by the measured object is reflected by the hot mirror,
The polarization plane is further rotated by 45 degrees by the / 4 wavelength plate, and the polarization plane of the infrared light emitted from the infrared light source is changed to linear polarization. Therefore, the light is reflected by the polarization beam splitter and received by the first image pickup means. On the other hand, the visible light reflected by the measured object passes through the hot mirror and is received by the second imaging means.
【0039】第9の発明は、被計測物体に照射する照射
光を発光し、前記照射光の照射角を調節し、前記照射角
を調節した照射光を被計測物体に照射し、前記被計測物
体で反射した反射光を受光する光照射受光方法におい
て、単色かつ直線偏光の照射光を発光し、前記照射角を
調節した照射光を偏光ビームスプリッタで反射させ、前
記偏光ビームスプリッタで反射させた照射光の偏光面を
45度回転させてから前記被計測物体に照射し、前記被
計測物体で反射した反射光の偏光面をさらに45度回転
させ、前記偏光ビームスプリッタを透過させて受光する
光照射受光方法である。A ninth aspect of the present invention emits irradiation light for irradiating an object to be measured, adjusts an irradiation angle of the irradiation light, irradiates the object with the irradiation light with the irradiation angle adjusted, and measures the object to be measured. In the light irradiation / reception method of receiving reflected light reflected by an object, monochromatic and linearly polarized irradiation light is emitted, and the irradiation light whose irradiation angle is adjusted is reflected by a polarizing beam splitter and reflected by the polarizing beam splitter. Light received by irradiating the object to be measured after rotating the plane of polarization of the irradiation light by 45 degrees, further rotating the plane of polarization of the reflected light reflected by the object to be measured by 45 degrees, and transmitting through the polarization beam splitter. This is an irradiation / light reception method.
【0040】前記第9の発明によれば、前記偏光ビーム
スプリッタで反射した光の偏光面を45度回転して前記
被計測物体に照射し、前記被計測物体で反射した光の偏
光面をさらに45度回転させることで、前記被計測物体
で反射した光は、前記偏光ビームスプリッタで反射する
光の偏光面と直交する偏光面の光になり、前記偏光ビー
ムスプリッタを透過する。そのため、前記照射する光
を、受光する反射光と同じ方向から照射することがで
き、前記被計測物体で反射した光を受光し、撮像したと
きに、前記被計測物体に光があたっていない領域(オク
ルージョン領域)が発生することを防ぐことができる。According to the ninth aspect, the polarization plane of the light reflected by the polarization beam splitter is rotated by 45 degrees to irradiate the measured object, and the polarization plane of the light reflected by the measured object is further changed. By rotating it by 45 degrees, the light reflected by the measured object becomes a light having a polarization plane orthogonal to the polarization plane of the light reflected by the polarization beam splitter, and passes through the polarization beam splitter. Therefore, the irradiated light can be irradiated from the same direction as the received reflected light, and the light reflected by the measured object is received, and when the image is captured, the measured object is not exposed to light. (Occlusion area) can be prevented from occurring.
【0041】また、前記照射光の照射角を調節して前記
被計測物体に照射することにより、前記被計測物体で反
射した光を受光し、撮像する際の撮像範囲にあわせて光
を照射することができ、光を有効利用することができ
る。また、前記発光した光を反射して被計測物体に照射
することにより、発光した光の光量のほぼ100%を被
計測物体に照射できる。また、前記偏光ビームスプリッ
タでは、前記被計測物体で反射した光の光量の50%か
ら100%の光量の光が透過する。そのため、前記偏光
ビームスプリッタを透過した光の光量は、発光した光の
光量の50%から100%の光量であり、光のロスが少
なくなる。Further, by adjusting the irradiation angle of the irradiation light and irradiating the object to be measured, the light reflected by the object to be measured is received and the light is irradiated in accordance with the imaging range at the time of imaging. Therefore, the light can be effectively used. Further, by reflecting the emitted light and irradiating the measured object with the measured object, it is possible to irradiate the measured object with almost 100% of the amount of the emitted light. Further, the polarization beam splitter transmits 50% to 100% of the amount of light reflected by the object to be measured. Therefore, the amount of light transmitted through the polarization beam splitter is 50% to 100% of the amount of emitted light, and the loss of light is reduced.
【0042】第10の発明は、被計測物体に照射する照
射光を発光し、前記照射光の照射角を調節し、前記照射
角を調節した照射光を被計測物体に照射し、前記被計測
物体で反射した反射光を受光する光照射受光方法におい
て、単色かつ直線偏光の照射光を発光し、前記照射角を
調節した照射光を偏光ビームスプリッタで透過させ、前
記偏光ビームスプリッタを透過した照射光の偏光面を4
5度回転させてから前記被計測物体に照射し、前記被計
測物体で反射した反射光の偏光面をさらに45度回転さ
せ、前記偏光ビームスプリッタで反射させて受光する光
照射受光方法である。A tenth aspect of the present invention emits irradiation light for irradiating an object to be measured, adjusts an irradiation angle of the irradiation light, irradiates the object to be measured with the irradiation light having the adjusted irradiation angle, and measures the object to be measured. In a light irradiation / reception method of receiving reflected light reflected by an object, a monochromatic and linearly polarized irradiation light is emitted, the irradiation light with the adjusted irradiation angle is transmitted through a polarization beam splitter, and the irradiation is transmitted through the polarization beam splitter. Set the polarization plane of light to 4
It is a light irradiation and light receiving method in which the object to be measured is irradiated with the light after being rotated by 5 degrees, the polarization plane of the reflected light reflected by the object to be measured is further rotated by 45 degrees, and is reflected by the polarization beam splitter to receive light.
【0043】前記第10の発明によれば、前記偏光ビー
ムスプリッタを透過した光の偏光面を45度回転して前
記被計測物体に照射し、前記被計測物体で反射した光の
偏光面をさらに45度回転させることで、前記被計測物
体で反射した光は、前記偏光ビームスプリッタを透過す
る光の偏光面と直交する偏光面の直線偏光になり、前記
偏光ビームスプリッタで反射する。そのため、前記照射
光と同じ方向に反射した光を受光することができ、前記
被計測物体で反射した光を受光し、撮像したときに、前
記被計測物体に光があたっていない領域(オクルージョ
ン領域)が発生することを防ぐことができる。According to the tenth aspect, the polarization plane of the light transmitted through the polarization beam splitter is rotated by 45 degrees to irradiate the measured object, and the polarization plane of the light reflected by the measured object is further changed. By rotating it by 45 degrees, the light reflected by the measured object becomes linearly polarized light having a polarization plane orthogonal to the polarization plane of the light passing through the polarization beam splitter, and is reflected by the polarization beam splitter. Therefore, the light reflected in the same direction as the irradiation light can be received, and the light reflected by the measured object is received, and when the image is captured, the area where the measured object is not exposed to light (occlusion area) ) Can be prevented.
【0044】また、前記照射光の照射角を調節して前記
被計測物体に照射することにより、前記被計測物体で反
射した光を受光し、撮像する際の撮像範囲にあわせて光
を照射することができ、光を有効利用することができ
る。また、前記発光した光を透過して被計測物体に照射
することにより、発光した光の光量のほぼ100%を被
計測物体に照射できる。また、前記偏光ビームスプリッ
タでは、前記被計測物体で反射した光の光量の50%か
ら100%の光量の光が反射する。そのため、前記偏光
ビームスプリッタを反射した光の光量は、発光した光の
光量の50%から100%の光量であり、光のロスが少
なくなる。By adjusting the irradiation angle of the irradiation light and irradiating the object to be measured, the light reflected by the object to be measured is received, and the light is irradiated in accordance with the imaging range at the time of imaging. Therefore, the light can be effectively used. Further, by transmitting the emitted light and irradiating the measured object, the measured object can be irradiated with almost 100% of the amount of the emitted light. Further, the polarization beam splitter reflects 50% to 100% of the amount of light reflected by the object to be measured. Therefore, the light amount of the light reflected by the polarization beam splitter is 50% to 100% of the light amount of the emitted light, and the light loss is reduced.
【0045】第11の発明は、直線偏光の赤外光を発光
し、前記赤外光の照射角を調節し、前記照射角を調節し
た赤外光を被計測物体に照射し、前記被計測物体で反射
した赤外光及び可視光を受光する光照射受光方法におい
て、前記照射角を調節した赤外光を偏光ビームスプリッ
タで反射させ、前記偏光ビームスプリッタで反射させた
赤外光の偏光面を45度回転させてから前記被計測物体
に照射し、前記被計測物体で反射した光を赤外光と可視
光に分離し、前記分離した赤外光の偏光面をさらに45
度回転させ、前記偏光ビームスプリッタを透過させて受
光する光照射受光方法である。An eleventh aspect of the present invention emits linearly polarized infrared light, adjusts the irradiation angle of the infrared light, irradiates the measured object with the infrared light having the adjusted irradiation angle, and measures the measured object. In a light irradiation / reception method of receiving infrared light and visible light reflected by an object, the infrared light having the irradiation angle adjusted is reflected by a polarization beam splitter, and the polarization plane of the infrared light reflected by the polarization beam splitter Is rotated by 45 degrees and then irradiates the object to be measured, the light reflected by the object to be measured is separated into infrared light and visible light, and the polarization plane of the separated infrared light is further increased by 45 degrees.
It is a light irradiation and light receiving method in which the light beam is rotated by a degree and transmitted through the polarization beam splitter to receive light.
【0046】前記第11の発明によれば、前記偏光ビー
ムスプリッタで反射した赤外光の偏光面を45度回転し
て前記被計測物体に照射し、前記被計測物体で反射した
赤外光の偏光面をさらに45度回転させることで、前記
被計測物体で反射した赤外光は、前記偏光ビームスプリ
ッタで反射する赤外光の偏光面と直交する偏光面の直線
偏光になり、前記偏光ビームスプリッタを透過する。そ
のため、前記照射する赤外光を、受光する赤外光と同じ
方向から照射することができ、前記被計測物体で反射し
た赤外光を受光し、撮像したときに、前記被計測物体に
赤外光があたっていない領域(オクルージョン領域)が
発生することを防ぐことができる。According to the eleventh aspect, the plane of polarization of the infrared light reflected by the polarization beam splitter is rotated by 45 degrees to irradiate the measured object, and the infrared light reflected by the measured object is rotated. By further rotating the polarization plane by 45 degrees, the infrared light reflected by the measured object becomes a linear polarization of a polarization plane orthogonal to the polarization plane of the infrared light reflected by the polarization beam splitter, and the polarization beam Transmit through the splitter. Therefore, the emitted infrared light can be emitted from the same direction as the received infrared light, and when the infrared light reflected by the measured object is received and imaged, the measured object is red It is possible to prevent the generation of an area (occlusion area) that is not exposed to external light.
【0047】また、前記照射光の照射角を調節して前記
被計測物体に照射することにより、前記被計測物体で反
射した赤外光を受光し、撮像する際の撮像範囲にあわせ
て光を照射することができ、撮影範囲外の無駄な領域に
照射される光の量を低減し、光を有効利用することがで
きる。また、前記発光した赤外光を反射して被計測物体
に照射することにより、発光した赤外光の光量のほぼ1
00%を被計測物体に照射できる。また、前記偏光ビー
ムスプリッタでは、前記被計測物体で反射した赤外光の
光量の50%から100%の光量の光が透過する。その
ため、前記偏光ビームスプリッタを透過した赤外光の光
量は、発光した赤外光の光量の50%から100%の光
量であり、光のロスが少なくなる。また、前記被計測物
体で反射した光には、赤外光のほかに、可視光が含まれ
ているため、前記被計測物体で反射した光を赤外光と可
視光に分離することで、赤外光と可視光を別々に受光で
き、前記赤外光のみの像と前記可視光の像を撮像するこ
とができ、被計測物体の形状及び色の情報を得ることが
できる。Further, by adjusting the irradiation angle of the irradiation light and irradiating the object to be measured, the infrared light reflected by the object to be measured is received and the light is adjusted in accordance with the imaging range at the time of imaging. It is possible to irradiate, reduce the amount of light that is irradiated to a useless area outside the photographing range, and use the light effectively. Further, by reflecting the emitted infrared light and irradiating the measured object with the infrared light, the amount of the emitted infrared light is almost 1%.
The object to be measured can be irradiated with 00%. Further, the polarizing beam splitter transmits 50% to 100% of the amount of infrared light reflected by the measured object. Therefore, the amount of infrared light transmitted through the polarization beam splitter is 50% to 100% of the amount of emitted infrared light, and light loss is reduced. Further, in addition to infrared light, visible light is included in the light reflected by the measured object, so that by separating the light reflected by the measured object into infrared light and visible light, Infrared light and visible light can be received separately, an image of only the infrared light and an image of the visible light can be captured, and information on the shape and color of the measured object can be obtained.
【0048】第12の発明は、直線偏光の赤外光を発光
し、前記赤外光の照射角を調節し、前記照射角を調節し
た赤外光を被計測物体に照射し、前記被計測物体で反射
した赤外光及び可視光を受光する光照射受光方法におい
て、前記照射角を調節した赤外光を偏光ビームスプリッ
タで透過し、前記偏光ビームスプリッタで反射させた赤
外光の偏光面を45度回転させてから前記被計測物体に
照射し、前記被計測物体で反射した光を赤外光と可視光
に分離し、前記分離した赤外光の偏光面をさらに45度
回転させ、前記偏光ビームスプリッタで反射して受光す
る光照射受光方法である。A twelfth aspect of the present invention emits linearly polarized infrared light, adjusts the irradiation angle of the infrared light, irradiates the measured object with the infrared light having the adjusted irradiation angle, and measures the measured object. In a light irradiation / reception method of receiving infrared light and visible light reflected by an object, a polarization plane of infrared light transmitted through a polarization beam splitter and adjusted by the polarization beam splitter, the infrared light having the irradiation angle adjusted. Irradiate the object to be measured after rotating it by 45 degrees, separate the light reflected by the object to be measured into infrared light and visible light, and further rotate the polarization plane of the separated infrared light by 45 degrees, It is a light irradiation / reception method in which light is reflected and received by the polarization beam splitter.
【0049】前記第12の発明によれば、前記偏光ビー
ムスプリッタを透過した赤外光の偏光面を45度回転し
て前記被計測物体に照射し、前記被計測物体で反射した
赤外光の偏光面をさらに45度回転させることで、前記
被計測物体で反射した赤外光は、前記偏光ビームスプリ
ッタを透過する赤外光の偏光面と直交する偏光面の直線
偏光になり、前記偏光ビームスプリッタで反射する。そ
のため、前記赤外光を照射した方向と同じ方向に反射し
た赤外光を受光することができ、前記被計測物体で反射
した赤外光を受光し、撮像したときに、前記被計測物体
に赤外光があたっていない領域(オクルージョン領域)
が発生することを防ぐことができる。According to the twelfth aspect of the invention, the plane of polarization of the infrared light transmitted through the polarization beam splitter is rotated by 45 degrees to irradiate the measured object, and the infrared light reflected by the measured object is changed. By further rotating the plane of polarization by 45 degrees, the infrared light reflected by the object to be measured becomes a linear polarization of a plane of polarization orthogonal to the plane of polarization of the infrared light transmitted through the polarization beam splitter, and the polarization beam Reflect on the splitter. Therefore, it is possible to receive infrared light reflected in the same direction as the direction in which the infrared light is emitted, receive the infrared light reflected by the measured object, and when the image is taken, the measured object is Area not exposed to infrared light (occlusion area)
Can be prevented.
【0050】また、前記照射光の照射角を調節して前記
被計測物体に照射することにより、前記被計測物体で反
射した赤外光を受光し、撮像する際の撮像範囲にあわせ
て光を照射することができ、撮影範囲外の無駄な領域に
照射される光の量を低減し、光を有効利用することがで
きる。また、前記発光した赤外光を透過して被計測物体
に照射することにより、発光した赤外光の光量のほぼ1
00%を被計測物体に照射できる。また、前記偏光ビー
ムスプリッタでは、前記被計測物体で反射した赤外光の
光量の50%から100%の光量の光が反射する。その
ため、前記偏光ビームスプリッタを反射して受光される
赤外光の光量は、発光した赤外光の光量の50%から1
00%の光量であり、光のロスが少なくなる。また、前
記被計測物体で反射した光には、赤外光のほかに、可視
光が含まれているため、前記被計測物体で反射した光を
赤外光と可視光に分離することで、赤外光と可視光を別
々に受光でき、前記赤外光のみの像と前記可視光の像を
撮像することができ、被計測物体の形状及び色の情報を
得ることができる。By adjusting the irradiation angle of the irradiation light to irradiate the object to be measured, the infrared light reflected by the object to be measured is received and the light is adjusted according to the imaging range at the time of imaging. It is possible to irradiate, reduce the amount of light that is irradiated to a useless area outside the photographing range, and use the light effectively. In addition, by transmitting the emitted infrared light and irradiating the object to be measured, the amount of the emitted infrared light is about 1
The object to be measured can be irradiated with 00%. Further, the polarization beam splitter reflects 50% to 100% of the amount of infrared light reflected by the measured object. Therefore, the amount of infrared light reflected and received by the polarization beam splitter is 50% to 1 of the amount of emitted infrared light.
The amount of light is 00%, and the loss of light is small. Further, in addition to infrared light, visible light is included in the light reflected by the measured object, so that by separating the light reflected by the measured object into infrared light and visible light, Infrared light and visible light can be received separately, an image of only the infrared light and an image of the visible light can be captured, and information on the shape and color of the measured object can be obtained.
【0051】第13の発明は、前記第11の発明または
前記第12の発明において、前記被計測物体で反射した
光は、コールドミラーを用い、赤外光を透過させ、可視
光を反射させて分離する光照射受光方法である。前記第
13の発明によれば、前記コールドミラーを用いて赤外
光を透過し、可視光を反射させることにより、前記コー
ルドミラーを通ることによる赤外光及び可視光のロスが
ほとんどなく、光を有効利用することができる。In a thirteenth aspect of the present invention according to the eleventh aspect or the twelfth aspect, the light reflected by the object to be measured uses a cold mirror to transmit infrared light and reflect visible light. This is a light irradiation / reception method of separating. According to the thirteenth invention, infrared light is transmitted through the cold mirror and visible light is reflected, so that there is almost no loss of infrared light and visible light due to passing through the cold mirror. Can be effectively used.
【0052】第14の発明は、前記第11の発明または
前記第12の発明において、前記被計測物体で反射した
光は、ホットミラーを用い、赤外光を反射させ、可視光
を透過させて分離する光照射受光方法である。前記第1
4の発明によれば、前記ホットミラーを用いて赤外光を
反射させ、可視光を透過することにより、前記ホットミ
ラーを通ることによる赤外光及び可視光のロスがほとん
どなく、光を有効に利用することができる。In a fourteenth aspect of the invention according to the eleventh aspect or the twelfth aspect of the invention, the light reflected by the object to be measured uses a hot mirror to reflect infrared light and transmit visible light. This is a light irradiation / reception method of separating. The first
According to the invention of 4, the infrared light is reflected using the hot mirror and the visible light is transmitted, so that there is almost no loss of infrared light and visible light due to passing through the hot mirror, and the light is effective. Can be used for.
【0053】以下、本発明について、図面を参照して実
施の形態(実施例)とともに詳細に説明する。なお、実
施例を説明するための全図において、同一機能を有する
ものは、同一符号をつけ、その繰り返しの説明は省略す
る。Hereinafter, the present invention will be described in detail with reference to the drawings together with the embodiments (embodiments). In all the drawings for explaining the embodiments, those having the same function are designated by the same reference numerals, and the repeated description thereof will be omitted.
【0054】[0054]
【発明の実施の形態】(実施形態1)図1は、本発明に
よる実施形態1の光照射受光装置の概略構成を示す模式
図である。図1において、1Aは光照射受光装置、2は
被計測物体、3は発光手段、301は光源、302は照
射角調節手段、4は撮像手段、5は光軸一致手段、50
1は偏光ビームスプリッタ、502はλ/4波長板、6
は焦点調節手段である。また、図1に示した矢印のう
ち、実線の矢印は被計測物体に照射する光の進路を示
し、破線の矢印は受光する光の進路を示す。また、実線
の矢印に添えたsはs偏光であることを示し、破線の矢
印に添えたpはp偏光であることを示す。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS (Embodiment 1) FIG. 1 is a schematic diagram showing a schematic configuration of a light irradiation / reception device of Embodiment 1 according to the present invention. In FIG. 1, 1A is a light irradiation / reception device, 2 is an object to be measured, 3 is a light emitting means, 301 is a light source, 302 is an irradiation angle adjusting means, 4 is an imaging means, 5 is an optical axis matching means, 50.
1 is a polarization beam splitter, 502 is a λ / 4 wave plate, 6
Is a focus adjusting means. In addition, among the arrows shown in FIG. 1, solid arrows indicate the paths of the light that irradiates the object to be measured, and broken arrows indicate the paths of the light that is received. Further, s attached to the arrow of the solid line indicates that it is s-polarized light, and p attached to the arrow of the broken line indicates that it is p-polarized light.
【0055】本実施形態1の光照射受光装置1Aは、図
1に示すように、被計測物体2に照射する光を発光する
発光手段3と、前記被計測物体2で反射した光を受光し
て撮像する撮像手段4と、前記被計測物体2に照射する
光の光軸と前記撮像手段4で受光する光の光軸とを一致
させる光軸一致手段5と、前記撮像手段4で撮像する像
の焦点を調節する焦点調節手段6とにより構成されてい
る。また、前記発光手段3は、単色かつ直線偏光の光を
発光する光源301と、前記光源301で発光した光の
照射角を調節する照射角調節手段302とを備える。As shown in FIG. 1, the light irradiation / reception device 1A according to the first embodiment receives a light emitting means 3 for emitting light to be irradiated onto the object to be measured 2 and a light reflected by the object to be measured 2. The image pickup means 4 for picking up an image, the optical axis matching means 5 for matching the optical axis of the light radiated to the object to be measured 2 with the optical axis of the light received by the image pickup means 4, and the image pickup means 4. The focus adjusting means 6 adjusts the focus of the image. The light emitting means 3 includes a light source 301 which emits monochromatic and linearly polarized light, and an irradiation angle adjusting means 302 which adjusts the irradiation angle of the light emitted by the light source 301.
【0056】また、前記光軸一致手段5は、入射する光
の偏光面の向きに応じて、光を反射あるいは透過させる
偏光ビームスプリッタ501と、入射した光の偏光面を
45度回転させるλ/4波長板502とを備え、前記λ
/4波長板502は、前記偏光ビームスプリッタ501
と前記被計測物体2との間に配置されている。Further, the optical axis matching means 5 has a polarization beam splitter 501 which reflects or transmits light depending on the direction of the polarization plane of the incident light, and λ / which rotates the polarization plane of the incident light by 45 degrees. A four-wave plate 502, and
The quarter wave plate 502 is the polarization beam splitter 501.
And the object 2 to be measured.
【0057】また、本実施形態1の光照射受光装置1A
では、図1に示したように、前記光軸一致手段5及び前
記焦点調節手段6は、前記被計測物体2と前記撮像手段
4とを結ぶ直線上に、前記被計測物体2側から、前記焦
点調節手段6、前記光軸一致手段5の順に配置されてい
る。Further, the light irradiation / reception device 1A of the first embodiment
Then, as shown in FIG. 1, the optical axis matching means 5 and the focus adjusting means 6 are arranged on a straight line connecting the measured object 2 and the image pickup means 4 from the measured object 2 side, The focus adjusting means 6 and the optical axis matching means 5 are arranged in this order.
【0058】また、前記光源301は、発光した光の偏
光面が前記偏光ビームスプリッタ501で反射される向
きになり、かつ、前記偏光ビームスプリッタ501で反
射した光が前記被計測物体2に照射されるように配置さ
れ、前記照射角調節手段302は、前記光源301と前
記偏光ビームスプリッタ501の間に配置されている。Further, in the light source 301, the plane of polarization of the emitted light is oriented so as to be reflected by the polarization beam splitter 501, and the light reflected by the polarization beam splitter 501 is applied to the object to be measured 2. The irradiation angle adjusting means 302 is arranged between the light source 301 and the polarization beam splitter 501.
【0059】本実施形態1の光照射受光装置では、前記
光源301で発光した単色かつ直線偏光の光は、前記照
射角調節手段302で照射角を調節した後、前記偏光ビ
ームスプリッタ501に入射される。このとき、前記偏
光ビームスプリッタ501に入射する光はs偏光である
ため、前記偏光ビームスプリッタ501で反射する。前
記偏光ビームスプリッタ501で反射した照射光は、前
記λ/4波長板で偏光面を45度回転させて円偏光にし
た後、前記焦点調節手段6を通して前記被計測物体2に
照射される。In the light irradiation and reception device of the first embodiment, the monochromatic and linearly polarized light emitted from the light source 301 is incident on the polarization beam splitter 501 after the irradiation angle adjusting means 302 adjusts the irradiation angle. It At this time, the light incident on the polarization beam splitter 501 is s-polarized light, and thus is reflected by the polarization beam splitter 501. The irradiation light reflected by the polarization beam splitter 501 is rotated by the λ / 4 wavelength plate by 45 degrees so as to be circularly polarized light, and then is irradiated onto the measured object 2 through the focus adjusting means 6.
【0060】このとき、前記光源301で発光する光は
直線偏光であり、前記偏光ビームスプリッタ501でほ
ぼ100%反射するため、前記光源301で発光した光
の光量のほぼ100%を前記被計測物体2に照射するこ
とができる。前記被計測物体2に光を照射する場合、少
なくとも、前記撮像手段4で撮影する範囲(撮影画角)
の全域に照射する必要があるが、前記光を照射する領域
が広すぎる場合は、単位面積あたりの光量が低下して光
の利用効率が低下するとともに、撮影した画像の精度が
低下する。そのため、前記照射角調節手段により、前記
被計測物体2の光が照射される領域が、前記撮影画角と
同等あるいは撮影画角よりもやや広くなるように調節す
る。At this time, since the light emitted from the light source 301 is linearly polarized and reflected by the polarization beam splitter 501 by almost 100%, almost 100% of the light amount of the light emitted by the light source 301 is measured by the object to be measured. 2 can be irradiated. When irradiating the object to be measured 2 with light, at least the range to be photographed by the image pickup means 4 (photographing field angle)
However, if the area irradiated with the light is too wide, the light amount per unit area decreases, the light utilization efficiency decreases, and the accuracy of the captured image decreases. Therefore, the irradiation angle adjusting means adjusts the region of the measured object 2 to be irradiated with light so as to be equal to or slightly wider than the photographing field angle.
【0061】図2及び図3は、本実施形態1の光照射受
光装置1Aの動作を説明するための模式図であり、それ
ぞれ、前記被計測物体に照射する光の照射角の調節方法
を説明するための模式図である。前記光照射受光装置1
Aを用いて、例えば、図2に示すように、前記焦点調節
手段6により、前記撮像手段4で撮影する範囲を、前記
被計測物体2の一部の狭い領域S1に設定した場合、前
記光源301で発光した光が、前記狭い領域S1内全体
を照射していればよい。そのため、前記照射角調節手段
302により、前記狭い領域S1と同じ領域、あるいは
前記狭い領域S1よりもやや広い領域を照射するように
照射角を調節する。FIGS. 2 and 3 are schematic diagrams for explaining the operation of the light irradiation / reception device 1A of the first embodiment, and respectively explain the method of adjusting the irradiation angle of the light irradiated to the object to be measured. It is a schematic diagram for doing. The light irradiation / light receiving device 1
As shown in FIG. 2, using A, for example, when the focus adjustment unit 6 sets the range to be captured by the image capturing unit 4 in a narrow region S1 of a part of the measured object 2, It is sufficient that the light emitted in 301 illuminates the entire inside of the narrow region S1. Therefore, the irradiation angle adjusting means 302 adjusts the irradiation angle so as to irradiate the same region as the narrow region S1 or a region slightly wider than the narrow region S1.
【0062】また、前記光照射受光装置1Aを用いて、
例えば、図3に示すように、前記焦点調節手段6によ
り、前記撮像手段4で撮影する範囲を、前記被計測物体
2の広い領域S2に設定した場合は、前記光源301で
発光した光で、前記広い領域S2内全体を照射しなけれ
ばならない。そのため、前記照射角調節手段302によ
り、前記広い領域S2と同じ領域、あるいは前記広い領
域S2よりもやや広い領域を照射するように照射角を調
節する。また、前記撮像手段4の撮影範囲は、前記焦点
調節手段6の調節により、図2及び図3に示した場合以
外も考えられるが、その場合も、前記撮像手段4の撮影
範囲に合わせて、前記照射角調節手段302により光の
照射範囲を調節する。Further, by using the light irradiation / reception device 1A,
For example, as shown in FIG. 3, when the focus adjusting unit 6 sets the range to be captured by the image capturing unit 4 to the wide region S2 of the measured object 2, the light emitted from the light source 301 The entire large area S2 must be illuminated. Therefore, the irradiation angle adjusting means 302 adjusts the irradiation angle so as to irradiate the same region as the wide region S2 or a region slightly wider than the wide region S2. Further, the image pickup range of the image pickup means 4 may be adjusted by the focus adjustment means 6 other than the cases shown in FIGS. 2 and 3, but in that case, according to the image pickup range of the image pickup means 4, The irradiation angle adjusting means 302 adjusts the irradiation range of light.
【0063】このように、前記焦点調節手段6の焦点距
離を変化させて、前記撮像手段4の撮影範囲(撮影画
角)を変更したときに、その変化に合わせて、前記照射
角調節手段302により光の照射角(照射領域)を変更
することにより、前記光照射受光装置1Aから照射する
光のほとんどを前記撮影画角内に照射でき、照射した光
の光量をほぼ100%利用することができる。そのた
め、前記発光手段3で発光した光を有効に利用すること
ができる。As described above, when the focal length of the focus adjusting means 6 is changed and the photographing range (photographing angle of view) of the image pickup means 4 is changed, the irradiation angle adjusting means 302 is adjusted according to the change. By changing the irradiation angle (irradiation area) of light, most of the light irradiated from the light irradiation and reception device 1A can be irradiated within the photographing field angle, and the light amount of the irradiated light can be used almost 100%. it can. Therefore, the light emitted by the light emitting means 3 can be effectively used.
【0064】また、前記被計測物体2に照射した光と、
前記被計測物体2で反射した光が同じ光路を通るため、
前記撮像手段4で撮影する範囲を変更するときに、前記
照射角調節手段302で照射角を調節するだけでよい。
そのため、撮影範囲を効率よく照射するための制御が容
易になる。またこのとき、前記照射角調節手段302
を、前記焦点調節手段6と連動させることにより、前記
撮像手段4で撮影する範囲に照射することができ、光量
を有効に利用することができる。The light applied to the object to be measured 2 is
Since the light reflected by the measured object 2 passes through the same optical path,
When changing the range to be photographed by the image pickup means 4, it is only necessary to adjust the irradiation angle by the irradiation angle adjusting means 302.
Therefore, control for efficiently irradiating the photographing range becomes easy. At this time, the irradiation angle adjusting means 302
By linking with the focus adjusting means 6, it is possible to irradiate the range to be photographed by the image pickup means 4, and to effectively use the light amount.
【0065】一方、前記被計測物体2に照射した光は反
射し、図1に示したように、再び前記焦点調節手段6を
通して前記λ/4波長板502に入射し、再び偏光面が
45度回転する。前記被計測物体2からの反射光は、一
般に、円偏光と無偏光が混合した状態であり、前記円偏
光は前記λ/4波長板502で直線偏光に戻る。このと
きの偏光面は、前記光源301で発光した光の偏光面に
対して90度回転した状態、すなわちp偏光であるた
め、前記偏光ビームスプリッタ501を透過し、前記撮
像手段4で受光される。On the other hand, the light applied to the object to be measured 2 is reflected and again enters the λ / 4 wave plate 502 through the focus adjusting means 6 as shown in FIG. Rotate. The reflected light from the measured object 2 is generally in a mixed state of circularly polarized light and non-polarized light, and the circularly polarized light returns to linearly polarized light at the λ / 4 wavelength plate 502. Since the polarization plane at this time is 90 ° rotated with respect to the polarization plane of the light emitted from the light source 301, that is, p-polarized light, the polarization plane is transmitted through the polarization beam splitter 501 and is received by the imaging unit 4. .
【0066】一方、前記無偏光は偏光面がランダムな光
であり、前記λ/4波長板502により各偏光面が均一
に回転するだけなので、無偏光のまま前記偏光ビームス
プリッタ501に入射される。このとき、前記無偏光の
一部、すなわち偏光面が前記偏光ビームスプリッタ50
1を透過する向きの成分だけが透過し、残りの成分は反
射する。そのため、前記撮像手段4で受光する光の光量
は、前記被計測物体2で反射した光の円偏光と無偏光の
混合比に依存するが、前記被計測物体2で反射した光の
光量の、おおよそ50%から100%となる。On the other hand, the non-polarized light is a light whose polarization plane is random, and since each polarization plane is uniformly rotated by the λ / 4 wavelength plate 502, it is incident on the polarization beam splitter 501 without being polarized. . At this time, a part of the non-polarized light, that is, the plane of polarization is the polarization beam splitter 50.
Only the component in the direction of transmitting 1 is transmitted, and the remaining components are reflected. Therefore, the light amount of the light received by the imaging unit 4 depends on the mixing ratio of the circularly polarized light and the non-polarized light of the light reflected by the measured object 2, but the amount of the light reflected by the measured object 2 is: It will be approximately 50% to 100%.
【0067】本実施形態1の光照射受光装置1Aでは、
前記被計測物体2に照射する光の光軸を、前記撮像手段
4で受光する光の光軸と一致させているため、前記撮像
手段4で撮影する領域内に光があたらない領域(オクル
ージョン領域)が発生しない。また、前記光源301で
発光した光の光量のほぼ100%を前記被計測物体2に
照射でき、前記被計測物体2で反射した光の光量の50
%から100%を前記撮像手段4で受光することができ
るので、従来のハーフミラーを用いた装置に比べ、撮像
に利用できる光量を増加することができる。In the light irradiation / reception device 1A of the first embodiment,
Since the optical axis of the light applied to the object to be measured 2 is made coincident with the optical axis of the light received by the image pickup means 4, an area (occlusion area) where light does not fall within the area taken by the image pickup means 4 ) Does not occur. Further, almost 100% of the amount of light emitted from the light source 301 can be applied to the measured object 2, and 50% of the amount of light reflected by the measured object 2 can be applied.
Since 100% to 100% can be received by the image pickup means 4, the amount of light that can be used for image pickup can be increased as compared with a device using a conventional half mirror.
【0068】図4は、本実施形態1の光照射受光装置の
具体的な構成例を示す模式図である。本実施形態1の光
照射受光装置1Aは、主に、前記被計測物体2の三次元
形状を測定したり、パターン認識をしたりするのに用い
られる三次元形状測定装置として用いられ、前記光源3
01として、図4に示すように、パルスレーザ光を発光
する半導体レーザ発振器301を用いる。FIG. 4 is a schematic view showing a concrete example of the structure of the light irradiation / reception device of the first embodiment. The light irradiation / reception device 1A of the first embodiment is mainly used as a three-dimensional shape measuring device used for measuring the three-dimensional shape of the measured object 2 and for pattern recognition. Three
As 01, a semiconductor laser oscillator 301 that emits pulsed laser light is used as shown in FIG.
【0069】また、前記撮像手段4は、高速のシャッタ
ー動作及び光を増幅するゲート付きMCP401及びリ
レーレンズ402が設けられた撮像カメラ403を用い
る。また、必要に応じて前記λ/4波長板502と前記
撮像カメラ403の間に、前記半導体レーザ発振器30
1で発光したレーザパルス光の波長以外の波長の光を除
去するバンドパスフィルタ404を設ける。また、前記
焦点調節手段6は、例えば、焦点距離の短いCマウント
レンズ601と、焦点距離延長レンズ602を組み合わ
せて用いる。The image pickup means 4 uses an image pickup camera 403 provided with a gated MCP 401 and a relay lens 402 for high-speed shutter operation and light amplification. The semiconductor laser oscillator 30 may be provided between the λ / 4 wave plate 502 and the image pickup camera 403 as needed.
A bandpass filter 404 for removing light having a wavelength other than the wavelength of the laser pulse light emitted in 1 is provided. The focus adjusting means 6 uses, for example, a C-mount lens 601 having a short focal length and a focal length extending lens 602 in combination.
【0070】図4に示した三次元形状測定装置の動作を
簡単に説明すると、まず、前記半導体レーザ発振器30
1でレーザパルス光を発光する。前記レーザパルス光
は、前記照射角調節手段302で、前記レーザパルス光
の照射角が前記撮像カメラで撮影する範囲(撮像画角)
と同等あるいはやや広くなるように調節して前記偏光ビ
ームスプリッタ501に入射する。The operation of the three-dimensional shape measuring apparatus shown in FIG. 4 will be briefly described. First, the semiconductor laser oscillator 30
At 1, the laser pulse light is emitted. The range of the irradiation angle of the laser pulse light captured by the imaging camera by the irradiation angle adjusting unit 302 (the imaging angle of view).
And is made to be slightly wider than the above, and enters the polarization beam splitter 501.
【0071】このとき、前記半導体レーザ発振器301
は、前記レーザパルス光がs偏光になるように配置され
ており、前記偏光ビームスプリッタ501で反射し、前
記λ/4波長板502で円偏光になり、前記焦点延長レ
ンズ602及び前記Cマウントレンズ601を通って前
記被計測物体2に照射される。前記被計測物体2に照射
され、反射したレーザパルス光は、再び前記Cマウント
レンズ601及び焦点距離延長レンズ602を通り、前
記λ/4波長板502に入射する。At this time, the semiconductor laser oscillator 301
Are arranged so that the laser pulse light is s-polarized light, reflected by the polarization beam splitter 501, circularly polarized by the λ / 4 wavelength plate 502, the focus extension lens 602 and the C-mount lens. The object 2 to be measured is irradiated through 601. The laser pulse light that is irradiated and reflected on the measured object 2 passes through the C mount lens 601 and the focal length extension lens 602 again and is incident on the λ / 4 wavelength plate 502.
【0072】このとき、反射した前記レーザパルス光の
うち円偏光の光は、前記半導体レーザ発振器301で発
光したレーザパルス光の偏光面と直交する偏光面のパル
ス光になるため、前記偏光ビームスプリッタ501を透
過する。また、前記反射したレーザパルス光の無偏光成
分は、前記偏光ビームスプリッタ501が透過する偏光
面に近い成分が透過する。At this time, circularly polarized light of the reflected laser pulse light becomes pulsed light having a polarization plane orthogonal to the polarization plane of the laser pulse light emitted from the semiconductor laser oscillator 301, so that the polarization beam splitter is used. 501 is transmitted. Further, as the non-polarized component of the reflected laser pulse light, a component close to the polarization plane transmitted by the polarization beam splitter 501 is transmitted.
【0073】前記偏光ビームスプリッタ501を透過し
た光は、前記バンドパスフィルタ404に入射され、前
記半導体レーザ光源301で発光したレーザパルス光の
波長以外の外光成分が除去される。なお、前記三次元形
状測定装置を用いた計測を暗室で行う場合や、前記レー
ザパルス光の強度が前記外光の強度よりも十分に大きい
場合には、前記バンドパスフィルタ404を設けなくて
もよい。前記バンドパスフィルタ404を通過した光
は、前記ゲート付きMCP401を用いて高速のシャッ
ター動作をさせながら、前記リレーレンズ402を通し
て前記撮像カメラ403で光の像を撮影する。The light transmitted through the polarization beam splitter 501 is incident on the bandpass filter 404 and external light components other than the wavelength of the laser pulse light emitted from the semiconductor laser light source 301 are removed. In addition, when the measurement using the three-dimensional shape measuring apparatus is performed in a dark room, or when the intensity of the laser pulse light is sufficiently higher than the intensity of the outside light, the bandpass filter 404 may not be provided. Good. The light that has passed through the bandpass filter 404 is captured by the imaging camera 403 through the relay lens 402 while performing a high-speed shutter operation using the gated MCP 401.
【0074】このとき、前記被計測物体2の各部位で反
射した光には、前記半導体レーザ発振器301から前記
被計測物体2までの距離と、前記被計測物体2から前記
撮像カメラ403までの距離の和に応じた時間差があ
る。そのため、高速のシャッター動作をさせながら像を
撮影することにより、撮影された画像には、単位時間内
に到達した光の光量に応じた濃淡が現われる。そこで、
前記撮像した画像の濃淡値にもとづき、飛行時間法を用
いて、撮影した画像の各点に対する前記被計測物体まで
の距離を求めることにより、前記被計測物体の形状を求
めることができる。At this time, in the light reflected by each part of the measured object 2, the distance from the semiconductor laser oscillator 301 to the measured object 2 and the distance from the measured object 2 to the imaging camera 403. There is a time difference according to the sum of. Therefore, when an image is captured while a high-speed shutter operation is performed, the captured image shows shades corresponding to the amount of light reaching within a unit time. Therefore,
The shape of the measured object can be obtained by calculating the distance to the measured object with respect to each point of the captured image using the time-of-flight method based on the gray value of the captured image.
【0075】以上説明したように、本実施形態1の光照
射受光装置によれば、前記被計測物体2に照射する光の
光軸を、前記撮像手段4で受光する光の光軸と一致させ
ることにより、前記被計測物体2にオクルージョン領域
が発生するのを防ぐことができる。またこのとき、前記
照射角調節手段302を用いることにより、前記被計測
物体2の撮影領域(撮像画角)と同等あるいはやや広い
領域のみに光を照射することができ、光量を有効に利用
することができる。また、前記偏光ビームスプリッタ5
01及びλ/4波長板502を用いることにより、前記
撮像手段4で受光する光の光量が、前記光源301で発
光した光の光量の50%から100%になるため、従来
のハーフミラーを用いた装置に比べ、光の利用効率を高
くすることができる。As described above, according to the light irradiation / reception device of the first embodiment, the optical axis of the light with which the measured object 2 is irradiated is made to coincide with the optical axis of the light received by the image pickup means 4. As a result, it is possible to prevent an occlusion area from being generated in the measured object 2. Further, at this time, by using the irradiation angle adjusting means 302, it is possible to irradiate light only on an area equal to or slightly wider than the imaging area (imaging angle of view) of the measured object 2, and the light quantity is effectively utilized. be able to. In addition, the polarization beam splitter 5
01 and the λ / 4 wave plate 502, the amount of light received by the image pickup unit 4 is 50% to 100% of the amount of light emitted by the light source 301, so that the conventional half mirror is used. The efficiency of light utilization can be increased as compared with the conventional device.
【0076】(実施形態2)図5は、本発明による実施
形態2の光照射受光装置の概略構成を示す模式図であ
る。図5において、1Bは光照射受光装置、2は被計測
物体、3は発光手段、301は光源、302は照射角調
節手段、4は撮像手段、5は光軸一致手段、501は偏
光ビームスプリッタ、502はλ/4波長板、6は焦点
調節手段である。また、図5に示した矢印のうち、実線
の矢印は被計測物体に照射する光の進路を示し、破線の
矢印は受光する光の進路を示す。また、実線の矢印に添
えたpはp偏光であることを示し、破線の矢印に添えた
sはs偏光であることを示す。(Embodiment 2) FIG. 5 is a schematic diagram showing a schematic structure of a light irradiation / light receiving device of Embodiment 2 according to the present invention. In FIG. 5, 1B is a light irradiation / reception device, 2 is an object to be measured, 3 is a light emitting means, 301 is a light source, 302 is an irradiation angle adjusting means, 4 is an imaging means, 5 is an optical axis matching means, and 501 is a polarization beam splitter. 502 is a λ / 4 wave plate, and 6 is a focus adjusting means. In addition, among the arrows shown in FIG. 5, solid arrows indicate the paths of the light that illuminates the measured object, and broken arrows indicate the paths of the light that is received. Further, p attached to the solid arrow indicates p-polarized light, and s attached to the dashed arrow indicates s-polarized light.
【0077】本実施形態2の光照射受光装置1Bは、前
記実施形態1の光照射受光装置1Aと同様の構成であ
り、図5に示すように、前記光源301及び照射角調節
手段302を備える発光手段3と、前記撮像手段4と、
前記偏光ビームスプリッタ501及び前記λ/4波長板
502を備える光軸一致手段5と、前記焦点調節手段6
とにより構成されている。そのため、前記各構成要素の
説明は省略する。The light irradiation / reception device 1B of the second embodiment has the same structure as the light irradiation / reception device 1A of the first embodiment, and includes the light source 301 and the irradiation angle adjusting means 302 as shown in FIG. The light emitting means 3, the imaging means 4,
An optical axis matching unit 5 including the polarization beam splitter 501 and the λ / 4 wavelength plate 502, and the focus adjusting unit 6
It is composed of and. Therefore, the description of each component is omitted.
【0078】本実施形態2の光照射受光装置1Bにおい
て、前記実施形態1の光照射受光装置1Aと異なる点
は、前記発光手段3と前記撮像手段4の配置である。本
実施形態2の光照射受光装置1Bでは、前記発光手段3
の前記光源301は、発光した光の偏光面が、前記偏光
ビームスプリッタ501を透過する向きになるように配
置されている。また、前記撮像手段4は、前記被計測物
体からの反射光が、前記偏光ビームスプリッタ501で
反射する方向に配置されている。また、前記光源301
は、発光した光の偏光面が前記偏光ビームスプリッタ5
01で反射される向きになり、かつ、前記偏光ビームス
プリッタ501で反射した光が前記被計測物体2に照射
されるように配置され、前記照射角調節手段302は、
前記光源301と前記偏光ビームスプリッタ501の間
に配置されている。The light irradiation / reception device 1B of the second embodiment differs from the light irradiation / reception device 1A of the first embodiment in the arrangement of the light emitting means 3 and the image pickup means 4. In the light irradiation and reception device 1B of the second embodiment, the light emitting means 3
The light source 301 is arranged so that the plane of polarization of the emitted light is oriented to pass through the polarization beam splitter 501. Further, the image pickup means 4 is arranged in a direction in which the reflected light from the measured object is reflected by the polarization beam splitter 501. In addition, the light source 301
Means that the polarization plane of the emitted light is the polarization beam splitter 5
The irradiation angle adjusting means 302 is arranged so that the light reflected by 01 and reflected by the polarization beam splitter 501 is irradiated on the measured object 2.
It is arranged between the light source 301 and the polarization beam splitter 501.
【0079】本実施形態2の光照射受光装置1Bでは、
前記光源301で発光した単色かつ直線偏光の光は、前
記照射角調節手段302で照射角を調節した後、前記偏
光ビームスプリッタ501に入射される。このとき、前
記偏光ビームスプリッタ501に入射する光はp偏光で
あるため、前記偏光ビームスプリッタ501を透過す
る。前記偏光ビームスプリッタ501を透過した照射光
は、前記λ/4波長板502で偏光面を45度回転させ
て円偏光にした後、前記焦点調節手段6を通して前記被
計測物体2に照射される。In the light irradiation / reception device 1B of the second embodiment,
The monochromatic and linearly polarized light emitted from the light source 301 is incident on the polarization beam splitter 501 after the irradiation angle is adjusted by the irradiation angle adjusting means 302. At this time, since the light incident on the polarization beam splitter 501 is p-polarized light, it passes through the polarization beam splitter 501. The irradiation light transmitted through the polarization beam splitter 501 is rotated by the λ / 4 wavelength plate 502 by 45 degrees to form circularly polarized light, and then is irradiated onto the measured object 2 through the focus adjusting means 6.
【0080】このとき、前記光源301で発光する光は
直線偏光であり、前記偏光ビームスプリッタ501でほ
ぼ100%反射するため、前記光源301で発光した光
の光量のほぼ100%を前記被計測物体2に照射するこ
とができる。また、前記被計測物体2に光を照射する場
合には、前記実施形態1で説明したように、前記照射角
調節手段302により、前記被計測物体2の光が照射さ
れる領域が、前記撮影画角と同等あるいは撮影画角より
もやや広くなるように調節する。At this time, since the light emitted from the light source 301 is linearly polarized and reflected by the polarization beam splitter 501 by almost 100%, almost 100% of the light amount emitted by the light source 301 is measured by the object to be measured. 2 can be irradiated. Further, when irradiating the measured object 2 with light, as described in the first embodiment, the area of the measured object 2 irradiated with light by the irradiation angle adjusting unit 302 is the image capturing area. Adjust so that it is equal to or slightly wider than the shooting angle of view.
【0081】前記被計測物体2に照射した光は反射し、
図5に示したように、再び前記焦点調節手段6を通して
前記λ/4波長板502に入射し、再び偏光面が45度
回転する。前記被計測物体2からの反射光は、一般に、
円偏光と無偏光が混合した状態であり、前記円偏光は前
記λ/4波長板502で直線偏光に戻る。このときの偏
光面は、前記光源301で発光した光の偏光面に対して
90度回転した状態、すなわちs偏光であるため、前記
偏光ビームスプリッタ501で反射し、前記撮像手段4
で受光される。The light applied to the measured object 2 is reflected,
As shown in FIG. 5, it again enters the λ / 4 wave plate 502 through the focus adjusting means 6, and the plane of polarization is again rotated by 45 degrees. The reflected light from the measured object 2 is generally
This is a state in which circularly polarized light and non-polarized light are mixed, and the circularly polarized light returns to linearly polarized light at the λ / 4 wavelength plate 502. Since the polarization plane at this time is rotated by 90 degrees with respect to the polarization plane of the light emitted from the light source 301, that is, s-polarized light, the polarization plane is reflected by the polarization beam splitter 501 and the imaging unit 4
Is received by.
【0082】一方、前記無偏光は偏光面がランダムな光
であり、前記λ/4波長板502により各偏光面が均一
に回転するだけなので、無偏光のまま前記偏光ビームス
プリッタ501に入射される。このとき、前記無偏光の
一部、すなわち偏光面が前記偏光ビームスプリッタ50
1で反射する向きの成分だけが反射し、残りの成分は透
過する。そのため、前記撮像手段4で受光する光の光量
は、前記被計測物体2で反射した光の円偏光と無偏光の
混合比に依存するが、前記被計測物体2で反射した光の
光量の、おおよそ50%から100%となる。On the other hand, the non-polarized light is a light whose polarization plane is random, and since each polarization plane is uniformly rotated by the λ / 4 wavelength plate 502, it is incident on the polarization beam splitter 501 without polarization. . At this time, a part of the non-polarized light, that is, the plane of polarization is the polarization beam splitter 50.
Only the component in the direction of reflection at 1 is reflected, and the remaining components are transmitted. Therefore, the light amount of the light received by the imaging unit 4 depends on the mixing ratio of the circularly polarized light and the non-polarized light of the light reflected by the measured object 2, but the amount of the light reflected by the measured object 2 is: It will be approximately 50% to 100%.
【0083】本実施形態2の光照射受光装置1Bでは、
前記被計測物体2に照射する光の光軸を、前記撮像手段
4で受光する光の光軸と一致させているため、前記撮像
手段4で撮影する領域内に光があたらない領域(オクル
ージョン領域)が発生しない。また、前記光源301で
発光した光の光量のほぼ100%を前記被計測物体2に
照射でき、前記被計測物体2で反射した光の光量の50
%から100%を前記撮像手段4で受光することができ
るので、従来のハーフミラーを用いた装置に比べ、撮像
に利用できる光量を増加することができる。本実施形態
2の光照射受光装置1Bも、前記実施形態1の光照射受
光装置1Aと同様に、主に、前記被計測物体の三次元形
状を測定したり、パターン認識をしたりするのに用いら
れる三次元形状測定装置として用いられるが、その具体
的な構成及び動作の説明については省略する。In the light irradiation / reception device 1B of the second embodiment,
Since the optical axis of the light applied to the object to be measured 2 is made coincident with the optical axis of the light received by the image pickup means 4, an area (occlusion area) where light does not fall within the area taken by the image pickup means 4 ) Does not occur. Further, almost 100% of the amount of light emitted from the light source 301 can be applied to the measured object 2, and 50% of the amount of light reflected by the measured object 2 can be applied.
Since 100% to 100% can be received by the image pickup means 4, the amount of light that can be used for image pickup can be increased as compared with a device using a conventional half mirror. Similarly to the light irradiation / reception device 1A of the first embodiment, the light irradiation / reception device 1B of the second embodiment is mainly used for measuring the three-dimensional shape of the measured object or for pattern recognition. Although it is used as a three-dimensional shape measuring apparatus used, a description of its specific configuration and operation will be omitted.
【0084】以上説明したように、本実施形態2の光照
射受光装置によれば、前記光軸一致手段5を用い、前記
被計測物体2に照射する光の方向と同じ方向に反射した
光を前記撮像手段4で受光することにより、前記被計測
物体2にオクルージョン領域が発生するのを防ぐことが
できる。またこのとき、前記照射角調節手段302を用
いることにより、前記被計測物体2の撮影領域(撮像画
角)と同等あるいはやや広い領域のみに光を照射するこ
とができ、光量を有効に利用することができる。また、
前記偏光ビームスプリッタ501及びλ/4波長板50
2を用いることにより、前記撮像手段4で受光する光の
光量が、前記光源301で発光した光の光量の50%か
ら100%になるため、従来のハーフミラーを用いた装
置に比べ、光の利用効率を高くすることができる。As described above, according to the light irradiation / reception device of the second embodiment, the light reflected by the optical axis matching means 5 is reflected in the same direction as the direction of the light with which the measured object 2 is irradiated. By receiving the light by the imaging unit 4, it is possible to prevent an occlusion region from being generated in the measured object 2. Further, at this time, by using the irradiation angle adjusting means 302, it is possible to irradiate light only on an area equal to or slightly wider than the imaging area (imaging angle of view) of the measured object 2, and the light quantity is effectively utilized. be able to. Also,
The polarization beam splitter 501 and the λ / 4 wave plate 50
By using 2, the light quantity of the light received by the image pickup means 4 becomes 50% to 100% of the light quantity of the light emitted by the light source 301, so that the light quantity of the light is smaller than that of the apparatus using the conventional half mirror. Utilization efficiency can be increased.
【0085】(実施形態3)図6は、本発明による実施
形態3の光照射受光装置の概略構成を示す模式図であ
る。図6において、1Cは光照射受光装置、2は被計測
物体、3は発光手段、302は照射角調節手段、303
は赤外光源、4は第1撮像手段、5は光軸一致手段、5
01は偏光ビームスプリッタ、502はλ/4波長板、
6は焦点調節手段、7Aは光分離手段(コールドミラ
ー)、8は第2撮像手段である。また、図6に示した矢
印のうち、実線の矢印は被計測物体に照射する光の進路
を示し、破線の矢印は受光する光の進路を示す。また、
実線の矢印に添えたsはs偏光であることを示し、破線
の矢印に添えたpはp偏光であることを示す。(Embodiment 3) FIG. 6 is a schematic diagram showing a schematic structure of a light irradiation / reception device of Embodiment 3 according to the present invention. In FIG. 6, 1C is a light irradiation / receiving device, 2 is an object to be measured, 3 is a light emitting means, 302 is an irradiation angle adjusting means, and 303.
Is an infrared light source, 4 is a first imaging means, 5 is an optical axis matching means, 5
01 is a polarization beam splitter, 502 is a λ / 4 wave plate,
Reference numeral 6 is a focus adjusting means, 7A is a light separating means (cold mirror), and 8 is a second imaging means. Further, among the arrows shown in FIG. 6, the solid line arrow indicates the path of the light that illuminates the measured object, and the broken line arrow indicates the path of the light that is received. Also,
The s attached to the solid arrow indicates s-polarized light, and the p attached to the dashed arrow indicates p-polarized light.
【0086】本実施形態3の光照射受光装置1Cは、図
6に示すように、被計測物体2に照射する赤外光を発光
する発光手段3と、前記被計測物体2で反射した赤外光
を受光して撮像する第1撮像手段4と、前記被計測物体
2に照射する赤外光の光軸と、前記第1撮像手段4で受
光する赤外光の光軸を一致させる光軸一致手段5と、前
記第1撮像手段4で撮像する像の焦点を調節する焦点調
節手段6と、前記被計測物体2で反射した光を赤外光と
可視光に分離する光分離手段7Aと、前記光分離手段7
Aによって分離した可視光を受光して撮像する第2撮像
手段8とにより構成されている。As shown in FIG. 6, the light irradiation / reception device 1C of the third embodiment emits infrared light that irradiates the object 2 to be measured, and infrared light reflected by the object 2 to be measured. An optical axis that matches the optical axis of infrared light received by the first imaging unit 4 with the first imaging unit 4 that receives light and images Matching means 5, focus adjusting means 6 for adjusting the focus of the image captured by the first imaging means 4, and light separating means 7A for separating the light reflected by the measured object 2 into infrared light and visible light. , The light separating means 7
The second image pickup means 8 receives the visible light separated by A and picks up an image.
【0087】また、前記発光手段3は、直線偏光の赤外
光を発光する赤外光源303と、前記赤外光源303で
発光した赤外光の照射角を調節する照射角調節手段30
2とを備える。また、前記光軸一致手段5は、入射する
光の偏光面の向きに応じて光を反射あるいは透過させる
偏光ビームスプリッタ501と、入射した光の偏光面を
45度回転させるλ/4波長板502とを備える。ま
た、前記光分離手段7A、前記λ/4波長板502は、
前記偏光ビームスプリッタ501と前記被計測物体2と
の間に、前記被計測物体2側から、前記光分離手段7、
前記λ/4波長板502の順に配置されている。The light emitting means 3 includes an infrared light source 303 for emitting linearly polarized infrared light and an irradiation angle adjusting means 30 for adjusting the irradiation angle of the infrared light emitted by the infrared light source 303.
2 and. The optical axis matching means 5 includes a polarization beam splitter 501 that reflects or transmits light depending on the direction of the polarization plane of incident light, and a λ / 4 wavelength plate 502 that rotates the polarization plane of incident light by 45 degrees. With. Further, the light separating means 7A and the λ / 4 wave plate 502 are
Between the polarization beam splitter 501 and the measured object 2, from the measured object 2 side, the light splitting means 7,
The λ / 4 wave plate 502 is arranged in this order.
【0088】また、本実施形態3の光照射受光装置1C
において、前記光分離手段7Aは、赤外光を透過し、可
視光を反射するコールドミラーであり、前記焦点調節手
段6、前記コールドミラー7A、前記λ/4波長板50
2、前記偏光ビームスプリッタ501は、図6に示した
ように、前記被計測物体2と前記第1撮像手段4とを結
ぶ直線上に、前記被計測物体2側から、前記焦点調節手
段6、前記コールドミラー7A、前記λ/4波長板50
2、前記偏光ビームスプリッタ501の順に配置されて
いる。Further, the light irradiation / reception device 1C of the third embodiment.
In the above, the light separating means 7A is a cold mirror that transmits infrared light and reflects visible light, and the focus adjusting means 6, the cold mirror 7A, and the λ / 4 wavelength plate 50.
2. The polarization beam splitter 501 is, as shown in FIG. 6, on the straight line connecting the measured object 2 and the first imaging means 4, from the measured object 2 side, the focus adjusting means 6, The cold mirror 7A and the λ / 4 wave plate 50
2. The polarization beam splitter 501 is arranged in this order.
【0089】また、前記赤外光源303は、発光した赤
外光の偏光面が前記偏光ビームスプリッタ501で反射
する向きになり、かつ、前記偏光ビームスプリッタ50
1で反射した赤外光が前記被計測物体2に照射されるよ
うに配置されている。また、前記第2撮像手段8は、前
記被計測物体2からの可視光が前記コールドミラー7A
で反射する方向に配置されている。In the infrared light source 303, the polarization plane of the emitted infrared light is oriented so as to be reflected by the polarization beam splitter 501, and the polarization beam splitter 50
It is arranged so that the infrared light reflected at 1 is irradiated onto the measured object 2. In addition, the second imaging unit 8 causes the visible light from the measured object 2 to be reflected by the cold mirror 7A.
It is arranged in the direction of reflection.
【0090】本実施形態3の光照射受光装置1Cでは、
前記赤外光源303で発光した直線偏光の赤外光は、前
記照射角調節手段302で照射角を調節した後、前記偏
光ビームスプリッタ501に入射される。このとき、前
記偏光ビームスプリッタ501に入射する赤外光はs偏
光であるため、前記偏光ビームスプリッタ501で反射
する。前記偏光ビームスプリッタ501で反射した赤外
照射光は、前記λ/4波長板502で偏光面を45度回
転させて円偏光にした後、前記コールドミラー7Aを透
過し、前記焦点調節手段6を通して前記被計測物体2に
照射される。In the light irradiation / reception device 1C of the third embodiment,
The linearly polarized infrared light emitted from the infrared light source 303 is incident on the polarization beam splitter 501 after the irradiation angle is adjusted by the irradiation angle adjusting means 302. At this time, since the infrared light incident on the polarization beam splitter 501 is s-polarized light, it is reflected by the polarization beam splitter 501. The infrared irradiation light reflected by the polarization beam splitter 501 is rotated by the λ / 4 wavelength plate 502 by 45 degrees to form circularly polarized light, and then transmitted through the cold mirror 7A and passed through the focus adjusting means 6. The object to be measured 2 is irradiated.
【0091】このとき、前記赤外光源303で発光する
赤外光は直線偏光であり、前記偏光ビームスプリッタ5
01でほぼ100%反射する。また、前記赤外光は前記
コールドミラー7Aもほぼ100%透過するため、前記
赤外光源301で発光した赤外光の光量のほぼ100%
を前記被計測物体2に照射することができる。また、前
記被計測物体2に光を照射する場合には、前記実施形態
1で説明したように、前記照射角調節手段302によ
り、前記被計測物体2の光が照射される領域が、前記撮
影画角と同等あるいは撮影画角よりもやや広くなるよう
に調節する。At this time, the infrared light emitted from the infrared light source 303 is linearly polarized light, and the polarization beam splitter 5
01 reflects almost 100%. Further, since the infrared light passes through the cold mirror 7A by almost 100%, almost 100% of the amount of infrared light emitted by the infrared light source 301 is transmitted.
Can be applied to the measured object 2. Further, when irradiating the measured object 2 with light, as described in the first embodiment, the area of the measured object 2 irradiated with light by the irradiation angle adjusting unit 302 is the image capturing area. Adjust so that it is equal to or slightly wider than the shooting angle of view.
【0092】前記被計測物体2に照射した光は反射し、
図6に示したように、再び前記焦点調節手段6を通して
前記コールドミラー7Aに入射する。このとき、前記被
計測物体2で反射した光は、前記赤外光と外光(可視
光)が含まれているが、赤外光は前記コールドミラー7
Aを透過し、可視光は前記コールドミラー7Aで反射す
る。前記コールドミラー7Aを透過した赤外光は、再び
前記λ/4波長板502に入射し、再び偏光面が45度
回転する。The light applied to the measured object 2 is reflected,
As shown in FIG. 6, the light enters the cold mirror 7A through the focus adjusting means 6 again. At this time, the light reflected by the measured object 2 includes the infrared light and external light (visible light), but the infrared light is the cold mirror 7.
Visible light passes through A and is reflected by the cold mirror 7A. The infrared light transmitted through the cold mirror 7A again enters the λ / 4 wave plate 502, and the polarization plane is rotated by 45 degrees again.
【0093】前記被計測物体2で反射した赤外光は、一
般に、円偏光と無偏光が混合した状態であり、前記円偏
光は前記λ/4波長板502で直線偏光に戻る。このと
きの偏光面は、前記光源301で発光した光の偏光面に
対して90度回転した状態、すなわちp偏光であるた
め、前記偏光ビームスプリッタ501で反射し、前記撮
像手段4で受光される。The infrared light reflected by the object to be measured 2 is generally in a mixed state of circularly polarized light and non-polarized light, and the circularly polarized light returns to linearly polarized light at the λ / 4 wavelength plate 502. The polarization plane at this time is 90 ° rotated with respect to the polarization plane of the light emitted from the light source 301, that is, it is p-polarized light, so it is reflected by the polarization beam splitter 501 and received by the imaging means 4. .
【0094】一方、前記無偏光は偏光面がランダムな光
であり、前記λ/4波長板502により各偏光面が均一
に回転するだけなので、無偏光のまま前記偏光ビームス
プリッタ501に入射される。このとき、前記無偏光の
一部、すなわち偏光面が前記偏光ビームスプリッタ50
1で反射する向きの成分だけが反射し、残りの成分は透
過する。また、前記コールドミラー7Aは赤外光をほぼ
100%透過するため、前記撮像手段4で受光する光の
光量は、前記被計測物体2で反射した光の円偏光と無偏
光の混合比に依存するが、前記被計測物体2で反射した
光の光量の、おおよそ50%から100%となる。On the other hand, the non-polarized light is a light whose polarization plane is random, and since each polarization plane is uniformly rotated by the λ / 4 wavelength plate 502, it is incident on the polarization beam splitter 501 without polarization. . At this time, a part of the non-polarized light, that is, the plane of polarization is the polarization beam splitter 50.
Only the component in the direction of reflection at 1 is reflected, and the remaining components are transmitted. Further, since the cold mirror 7A transmits almost 100% of infrared light, the amount of light received by the image pickup means 4 depends on the mixing ratio of circularly polarized light and unpolarized light of the light reflected by the measured object 2. However, the light amount of the light reflected by the measured object 2 is about 50% to 100%.
【0095】また、前記コールドミラー7Aで反射した
可視光は、図6に示したように、第2撮像手段8で受光
し、撮像される。このとき、前記第2撮像手段8は、前
記第1撮像手段4で撮影する範囲と同じ範囲を撮影でき
るように光学的距離を調整しておく。The visible light reflected by the cold mirror 7A is received by the second image pickup means 8 and picked up as shown in FIG. At this time, the second image pickup means 8 adjusts the optical distance so that the same range as the range photographed by the first image pickup means 4 can be photographed.
【0096】本実施形態3の光照射受光装置1Cでは、
前記被計測物体2に照射する赤外光の光軸を、前記第1
撮像手段4で受光する赤外光の光軸と一致させているた
め、前記第1撮像手段4で撮影する領域内に赤外光があ
たらない領域(オクルージョン領域)が発生しない。In the light irradiation / reception device 1C of the third embodiment,
The optical axis of the infrared light irradiating the measured object 2 is set to the first
Since the optical axis of the infrared light received by the image pickup means 4 is matched, there is no area (occlusion area) where the infrared light does not fall within the area taken by the first image pickup means 4.
【0097】また、前記赤外光源301で発光した光の
光量のほぼ100%を前記被計測物体2に照射でき、前
記被計測物体2で反射した赤外光の光量の50%から1
00%を前記撮像手段4で受光することができるので、
従来のハーフミラーを用いた装置に比べ、撮像に利用で
きる光量を増加することができる。Almost 100% of the amount of light emitted from the infrared light source 301 can be applied to the measured object 2, and 50% to 1% of the amount of infrared light reflected by the measured object 2 can be applied.
Since 00% can be received by the image pickup means 4,
It is possible to increase the amount of light that can be used for imaging, as compared with a device using a conventional half mirror.
【0098】また、前記コールドミラー7Aを用いて、
前記被計測物体2で反射した光から可視光を分離し、前
記第2撮像手段8で受光し、撮像することにより、前記
第1撮像手段4で撮影した範囲の色情報を取得すること
ができる。そのため、前記被計測物体2の形状及び色情
報を測定でき、前記被計測物体2を認識しやすくなる。Using the cold mirror 7A,
By separating visible light from the light reflected by the object 2 to be measured, receiving the light by the second image pickup means 8, and picking up an image, it is possible to obtain the color information of the range picked up by the first image pickup means 4. . Therefore, the shape and color information of the measured object 2 can be measured, and the measured object 2 can be easily recognized.
【0099】図7は、本実施形態3の光照射受光装置の
具体的な構成例を示す模式図である。本実施形態3の光
照射受光装置1Cは、主に、前記被計測物体の三次元形
状を測定したり、パターン認識をしたりするのに用いら
れる三次元形状測定装置として用いられ、前記赤外光源
303として、図4に示すように、パルスレーザ光を発
光する半導体レーザ発振器303を用いる。FIG. 7 is a schematic diagram showing a specific structural example of the light irradiation / reception device of the third embodiment. The light irradiation / reception device 1C of the third embodiment is mainly used as a three-dimensional shape measuring device used for measuring the three-dimensional shape of the object to be measured and for pattern recognition. As the light source 303, as shown in FIG. 4, a semiconductor laser oscillator 303 that emits pulsed laser light is used.
【0100】また、前記撮像手段4は、赤外光に感度を
有し、高速のシャッター動作及び増幅をするゲート付き
MCP401及びリレーレンズ402が設けられた撮像
カメラ403を用いる。また、必要に応じて前記λ/4
波長板502と前記撮像カメラ403の間に、前記赤外
半導体レーザ発振器303で発光したレーザパルス光の
波長以外の波長の光を除去するバンドパスフィルタ40
4を設ける。また、前記焦点調節手段6は、例えば、焦
点距離の短いCマウントレンズ601と、焦点距離延長
レンズ602を組み合わせて用いる。The image pickup means 4 uses an image pickup camera 403 which is sensitive to infrared light and is provided with a gated MCP 401 and a relay lens 402 for performing high-speed shutter operation and amplification. If necessary, the λ / 4
Between the wave plate 502 and the imaging camera 403, the bandpass filter 40 for removing light having a wavelength other than the wavelength of the laser pulse light emitted from the infrared semiconductor laser oscillator 303.
4 is provided. The focus adjusting means 6 uses, for example, a C-mount lens 601 having a short focal length and a focal length extending lens 602 in combination.
【0101】図7に示した三次元形状測定装置の動作を
簡単に説明すると、まず、前記赤外半導体レーザ発振器
303でレーザパルス光を発光する。前記レーザパルス
光は、前記照射角調節手段302で、前記レーザパルス
光の照射角が前記撮像カメラで撮影する範囲(撮像画
角)と同等あるいはやや広くなるように調節して前記偏
光ビームスプリッタ501に入射する。The operation of the three-dimensional shape measuring apparatus shown in FIG. 7 will be briefly described. First, the infrared semiconductor laser oscillator 303 emits laser pulse light. The polarization beam splitter 501 adjusts the laser pulse light by the irradiation angle adjusting means 302 so that the irradiation angle of the laser pulse light becomes equal to or slightly wider than the range (image pickup angle of view) captured by the image pickup camera. Incident on.
【0102】このとき、前記赤外半導体レーザ発振器3
03は、前記レーザパルス光がs偏光になるように配置
されており、前記偏光ビームスプリッタ501で反射
し、前記λ/4波長板502で円偏光になり、前記コー
ルドミラー7Aを透過し、前記焦点延長レンズ602及
び前記Cマウントレンズ601を通って前記被計測物体
2に照射される。At this time, the infrared semiconductor laser oscillator 3
03 is arranged so that the laser pulse light is s-polarized light, reflected by the polarization beam splitter 501, circularly polarized by the λ / 4 wave plate 502, transmitted through the cold mirror 7A, and The object to be measured 2 is irradiated through the focus extension lens 602 and the C-mount lens 601.
【0103】前記被計測物体2に照射され、反射したレ
ーザパルス光は、再び前記Cマウントレンズ601及び
焦点距離延長レンズ602を通り、前記コールドミラー
7Aに入射する。このとき、反射した前記レーザパルス
光のうち円偏光の赤外光は、前記コールドミラー7Aを
透過し、前記λ/4波長板502で、前記赤外半導体レ
ーザ発振器303で発光したレーザパルス光の偏光面と
直交する偏光面のパルス光、すなわちp偏光になる。そ
のため、前記偏光ビームスプリッタ501を透過する。
また、前記反射したレーザパルス光の無偏光成分は、前
記偏光ビームスプリッタ501が透過する偏光面に近い
成分が透過する。The laser pulse light which is irradiated to and reflected from the object to be measured 2 passes through the C-mount lens 601 and the focal length extension lens 602 again and is incident on the cold mirror 7A. At this time, the circularly polarized infrared light of the reflected laser pulse light is transmitted through the cold mirror 7A, and the laser pulse light emitted by the infrared semiconductor laser oscillator 303 is emitted by the λ / 4 wavelength plate 502. It becomes pulsed light of a polarization plane orthogonal to the polarization plane, that is, p-polarized light. Therefore, the light passes through the polarization beam splitter 501.
Further, as the non-polarized component of the reflected laser pulse light, a component close to the polarization plane transmitted by the polarization beam splitter 501 is transmitted.
【0104】前記偏光ビームスプリッタ501を透過し
た光は、前記バンドパスフィルタ404に入射され、前
記赤外半導体レーザ光源303で発光したレーザパルス
光の波長以外の外光成分が除去される。前記バンドパス
フィルタ404を通過した光は、前記ゲート付きMCP
401を用いて高速のシャッター動作をさせながら、前
記リレーレンズ402を通して前記撮像カメラ403で
光の像を撮影する。The light transmitted through the polarization beam splitter 501 is incident on the bandpass filter 404 and external light components other than the wavelength of the laser pulse light emitted from the infrared semiconductor laser light source 303 are removed. The light passing through the bandpass filter 404 is converted into the MCP with gate.
A high-speed shutter operation is performed using 401, and a light image is captured by the imaging camera 403 through the relay lens 402.
【0105】このとき、前記被計測物体2の各部位で反
射した光には、前記半導体レーザ発振器から前記被計測
物体までの距離と、前記被計測物体から前記撮像カメラ
までの距離の和に応じた時間差がある。そのため、高速
のシャッター動作をさせながら像を撮影することによ
り、撮影された画像には、単位時間内に到達した光の光
量に応じた濃淡が現われる。そこで、前記撮像した画像
の濃淡値にもとづき、飛行時間法を用いて、撮影した画
像の各点に対する前記被計測物体までの距離を求めるこ
とにより、前記被計測物体の形状を求めることができ
る。At this time, the light reflected by each part of the object 2 to be measured depends on the sum of the distance from the semiconductor laser oscillator to the object to be measured and the distance from the object to be measured to the imaging camera. There is a time difference. Therefore, when an image is captured while a high-speed shutter operation is performed, the captured image shows shades corresponding to the amount of light reaching within a unit time. Therefore, the shape of the measured object can be obtained by calculating the distance to the measured object with respect to each point of the captured image using the time-of-flight method based on the gray value of the captured image.
【0106】一方、前記コールドミラー7Aに入射した
可視光は、前記コールドミラー7Aで反射するが、その
ままでは撮影した像の左右が入れ替わるため、ミラー9
でもう一度反射させ、像の左右を元に戻したあと、前記
第2撮像手段8で受光し、撮像する。On the other hand, the visible light incident on the cold mirror 7A is reflected by the cold mirror 7A, but since the left and right of the captured image are interchanged as it is, the mirror 9
After that, the image is reflected again and the left and right of the image are returned to the original state, and then the second image pickup means 8 receives the light and picks up the image.
【0107】以上説明したように、本実施形態3の光照
射受光装置によれば、前記光軸一致手段5を用い、前記
被計測物体2に照射する光の光軸を前記第1撮像手段4
で受光する光の光軸と一致させることにより、前記被計
測物体2にオクルージョン領域が発生するのを防ぐこと
ができる。またこのとき、前記照射角調節手段302を
用いることにより、前記被計測物体2の撮影領域(撮像
画角)と同等あるいはやや広い領域のみに光を照射する
ことができ、光量を有効に利用することができる。ま
た、前記偏光ビームスプリッタ501及びλ/4波長板
502を用いることにより、前記撮像手段4で受光する
光の光量が、前記光源301で発光した光の光量の50
%から100%になるため、従来のハーフミラーを用い
た装置に比べ、光の利用効率を高くすることができる。
また、前記光分離手段(コールドミラー)7Aを用いる
ことにより、前記被計測物体で反射した可視光を前記第
2撮像手段8で撮影することができ、前記被計測物体2
を認識するための情報量が増え、認識しやすくなる。As described above, according to the light irradiation / reception device of the third embodiment, the optical axis coincidence means 5 is used, and the optical axis of the light irradiated to the measured object 2 is measured by the first image pickup means 4.
By making it coincide with the optical axis of the light received by, it is possible to prevent an occlusion region from occurring in the measured object 2. Further, at this time, by using the irradiation angle adjusting means 302, it is possible to irradiate light only on an area equal to or slightly wider than the imaging area (imaging angle of view) of the measured object 2, and the light quantity is effectively utilized. be able to. Further, by using the polarization beam splitter 501 and the λ / 4 wavelength plate 502, the light amount of the light received by the imaging unit 4 is 50 times the light amount of the light emitted by the light source 301.
% To 100%, the light utilization efficiency can be improved as compared with the conventional device using the half mirror.
Further, by using the light separating means (cold mirror) 7A, the visible light reflected by the measured object can be photographed by the second imaging means 8, and the measured object 2
The amount of information for recognizing is increased, which makes it easier to recognize.
【0108】図8は、前記実施形態3の光照射受光装置
の変形例を示す模式図である。前記実施形態3の光照射
受光装置1Cでは、図6に示したように、前記焦点調節
手段6、前記コールドミラー7A、前記λ/4波長板5
02、前記偏光ビームスプリッタ501を、前記被計測
物体2と前記第1撮像手段4とを結ぶ直線上に、前記被
計測物体2側から、前記焦点調節手段6、前記コールド
ミラー7A、前記λ/4波長板502、前記偏光ビーム
スプリッタ501の順に配置しているが、これに限ら
ず、図8に示したように、前記被計測物体2と前記赤外
光発光手段3とを結ぶ直線上に、前記被計測物体2側か
ら、前記焦点調節手段6、前記コールドミラー7A、前
記λ/4波長板502、前記偏光ビームスプリッタ50
1の順に配置してもよい。FIG. 8 is a schematic diagram showing a modification of the light irradiation / reception device of the third embodiment. In the light irradiation / reception device 1C of the third embodiment, as shown in FIG. 6, the focus adjusting means 6, the cold mirror 7A, and the λ / 4 wave plate 5 are provided.
02, the polarization beam splitter 501 on the straight line connecting the measured object 2 and the first imaging means 4, from the measured object 2 side, the focus adjusting means 6, the cold mirror 7A, the λ / Although the four-wave plate 502 and the polarization beam splitter 501 are arranged in this order, the present invention is not limited to this, and as shown in FIG. 8, on a straight line connecting the measured object 2 and the infrared light emitting means 3. From the side of the measured object 2, the focus adjusting means 6, the cold mirror 7A, the λ / 4 wave plate 502, and the polarization beam splitter 50.
You may arrange in the order of 1.
【0109】このとき、前記赤外光源303は、発光し
た赤外光の偏光面が前記偏光ビームスプリッタ501を
透過する向きになるように配置する。また、前記第1撮
像手段4は、前記被計測物体2で反射され、前記コール
ドミラー7A及び前記λ/4波長板502を通った赤外
光が前記偏光ビームスプリッタ501で反射する方向に
配置する。図8に示したような構成の場合、前記第1撮
像手段4で受光する光の光軸が前記被計測物体2に照射
する赤外光の光軸と一致するため、前記実施形態3の光
照射受光装置1Cと同じ効果を得ることができる。At this time, the infrared light source 303 is arranged so that the plane of polarization of the emitted infrared light is oriented to pass through the polarization beam splitter 501. Further, the first imaging means 4 is arranged in a direction in which the infrared light reflected by the measured object 2 and passing through the cold mirror 7A and the λ / 4 wave plate 502 is reflected by the polarization beam splitter 501. . In the case of the configuration as shown in FIG. 8, the optical axis of the light received by the first image pickup means 4 coincides with the optical axis of the infrared light with which the object to be measured 2 is irradiated. The same effect as that of the irradiation / light receiving device 1C can be obtained.
【0110】(実施形態4)図9は、本発明による実施
形態4の光照射受光装置の概略構成を示す模式図であ
る。図9において、1Dは光照射受光装置、2は被計測
物体、3は発光手段、302は照射角調節手段、303
は赤外光源、4は第1撮像手段、5は光軸一致手段、5
01は偏光ビームスプリッタ、502はλ/4波長板、
6は焦点調節手段、7Bは光分離手段(ホットミラ
ー)、8は第2撮像手段である。また、図9に示した矢
印のうち、実線の矢印は被計測物体に照射する光の進路
を示し、破線の矢印は受光する光の進路を示す。また、
実線の矢印に添えたsはs偏光であることを示し、破線
の矢印に添えたpはp偏光であることを示す。(Embodiment 4) FIG. 9 is a schematic diagram showing a schematic structure of a light irradiation / reception device of Embodiment 4 according to the present invention. In FIG. 9, 1D is a light irradiation / reception device, 2 is an object to be measured, 3 is a light emitting means, 302 is an irradiation angle adjusting means, and 303.
Is an infrared light source, 4 is a first imaging means, 5 is an optical axis matching means, 5
01 is a polarization beam splitter, 502 is a λ / 4 wave plate,
6 is a focus adjusting means, 7B is a light separating means (hot mirror), and 8 is a second imaging means. In addition, among the arrows shown in FIG. 9, solid arrows indicate the paths of the light that illuminates the measured object, and broken arrows indicate the paths of the light that is received. Also,
The s attached to the solid arrow indicates s-polarized light, and the p attached to the dashed arrow indicates p-polarized light.
【0111】本実施形態4の光照射受光装置1Dは、前
記実施形態3の光照射受光装置と同様の構成であり、図
9に示すように、赤外光源303と照射角調節手段30
2を備える発光手段3と、前記第1撮像手段4と、前記
偏光ビームスプリッタ501と前記λ/4波長板502
を備える前記光軸一致手段5と、前記焦点調節手段6
と、前記光分離手段7Bと、前記第2撮像手段8とによ
り構成されている。そのため、各構成要素の説明は省略
する。The light irradiation / reception device 1D of the fourth embodiment has the same structure as the light irradiation / reception device of the third embodiment, and as shown in FIG. 9, the infrared light source 303 and the irradiation angle adjusting means 30.
2, the first image pickup unit 4, the polarization beam splitter 501, and the λ / 4 wave plate 502.
The optical axis matching means 5 and the focus adjusting means 6
And the light separation means 7B and the second image pickup means 8. Therefore, description of each component is omitted.
【0112】本実施形態4の光照射受光装置1Dにおい
て、前記実施形態3の光照射受光装置1Cと異なる点
は、前記光分離手段7Bとして、赤外光を反射し、可視
光を透過するホットミラーを用いる点と、前記各構成要
素の配置である。本実施形態4の光照射受光装置1Dで
は、前記ホットミラー7Bと前記焦点調節手段6は、図
9に示したように、前記被計測物体2と前記第2撮像手
段8とを結ぶ直線上に、前記被計測物体2側から前記焦
点調節手段6、前記ホットミラー7Bの順に配置され
る。The light irradiation / reception device 1D of the fourth embodiment is different from the light irradiation / reception device 1C of the third embodiment in that the light separating means 7B is a hot light reflecting infrared light and transmitting visible light. The point of using a mirror and the arrangement of each of the above-mentioned components. In the light irradiation / reception device 1D of the fourth embodiment, the hot mirror 7B and the focus adjustment means 6 are arranged on a straight line connecting the measured object 2 and the second imaging means 8 as shown in FIG. The focus adjusting means 6 and the hot mirror 7B are arranged in this order from the measured object 2 side.
【0113】また、前記λ/4波長板502及び前記偏
光ビームスプリッタ501は、前記被計測物体2からの
赤外光が前記ホットミラー7Bで反射する方向であり、
かつ、前記ホットミラー7Bと前記第1撮像手段4とを
結ぶ直線上に、前記λ/4波長板502、前記偏光ビー
ムスプリッタ501の順に配置される。また、前記赤外
光源303は、発光した赤外光の偏光面が前記偏光ビー
ムスプリッタ501で反射する向きになり、かつ、前記
被計測物体2に照射されるように配置されている。Further, the λ / 4 wave plate 502 and the polarization beam splitter 501 are in a direction in which infrared light from the measured object 2 is reflected by the hot mirror 7B,
Further, the λ / 4 wave plate 502 and the polarization beam splitter 501 are arranged in this order on a straight line connecting the hot mirror 7B and the first image pickup means 4. Further, the infrared light source 303 is arranged so that the plane of polarization of the emitted infrared light is oriented to be reflected by the polarization beam splitter 501 and is irradiated onto the measured object 2.
【0114】本実施形態4の光照射受光装置1Dでは、
前記赤外光源303で発光した直線偏光の赤外光は、前
記照射角調節手段302で照射角を調節した後、前記偏
光ビームスプリッタ501に入射される。このとき、前
記偏光ビームスプリッタ501に入射する赤外光はs偏
光であるため、前記偏光ビームスプリッタ501で反射
する。前記偏光ビームスプリッタ501で反射した赤外
照射光は、前記λ/4波長板502で偏光面を45度回
転させて円偏光にした後、前記ホットミラー7Bで反射
し、前記焦点調節手段6を通して前記被計測物体2に照
射される。In the light irradiation / reception device 1D of the fourth embodiment,
The linearly polarized infrared light emitted from the infrared light source 303 is incident on the polarization beam splitter 501 after the irradiation angle is adjusted by the irradiation angle adjusting means 302. At this time, since the infrared light incident on the polarization beam splitter 501 is s-polarized light, it is reflected by the polarization beam splitter 501. The infrared irradiation light reflected by the polarization beam splitter 501 is rotated by 45 ° in the λ / 4 wavelength plate 502 into circularly polarized light, reflected by the hot mirror 7B, and passed through the focus adjusting means 6. The object to be measured 2 is irradiated.
【0115】このとき、前記赤外光源303で発光する
赤外光は直線偏光であり、前記偏光ビームスプリッタ5
01でほぼ100%反射する。また、前記ホットミラー
7Bもほぼ100%反射するため、前記赤外光源303
で発光した赤外光の光量のほぼ100%を前記被計測物
体2に照射することができる。また、前記被計測物体2
に光を照射する場合には、前記実施形態1で説明したよ
うに、前記照射角調節手段302により、前記被計測物
体2の光が照射される領域が、前記撮影画角と同等ある
いは撮影画角よりもやや広くなるように調節する。At this time, the infrared light emitted from the infrared light source 303 is linearly polarized light, and the polarization beam splitter 5
01 reflects almost 100%. Further, since the hot mirror 7B also reflects almost 100%, the infrared light source 303
It is possible to irradiate the measured object 2 with almost 100% of the amount of infrared light emitted in step 1. In addition, the measured object 2
In the case of irradiating light on the object, as described in the first embodiment, the area of the object to be measured 2 irradiated by the light by the irradiation angle adjusting means 302 is equal to or equal to the photographic field angle. Adjust so that it is slightly wider than the corner.
【0116】前記被計測物体2に照射した光は反射し、
図6に示したように、再び前記焦点調節手段6を通して
前記ホットミラー7Bに入射する。このとき、前記被計
測物体2で反射した光は、前記赤外光と外光(可視光)
が含まれているが、赤外光は前記ホットミラー7Bで反
射し、可視光は前記ホットミラー7Bを透過する。前記
ホットミラー7Bで反射した赤外光は、再び前記λ/4
波長板502に入射し、再び偏光面が45度回転する。The light applied to the measured object 2 is reflected,
As shown in FIG. 6, the light enters the hot mirror 7B through the focus adjusting means 6 again. At this time, the light reflected by the measured object 2 is the infrared light and the external light (visible light).
However, infrared light is reflected by the hot mirror 7B and visible light is transmitted through the hot mirror 7B. The infrared light reflected by the hot mirror 7B is again reflected by the λ / 4.
It is incident on the wave plate 502, and the plane of polarization is again rotated by 45 degrees.
【0117】前記被計測物体2で反射した赤外光は、一
般に、円偏光と無偏光が混合した状態であり、前記円偏
光は前記λ/4波長板502で直線偏光に戻る。このと
きの偏光面は、前記赤外光源303で発光した光の偏光
面に対して90度回転した状態、すなわちp偏光である
ため、前記偏光ビームスプリッタ501で反射し、前記
撮像手段4で受光される。The infrared light reflected by the object to be measured 2 is generally in a mixed state of circularly polarized light and non-polarized light, and the circularly polarized light is returned to the linearly polarized light by the λ / 4 wavelength plate 502. Since the polarization plane at this time is 90 ° rotated with respect to the polarization plane of the light emitted from the infrared light source 303, that is, p-polarized light, the polarization plane is reflected by the polarization beam splitter 501 and received by the imaging unit 4. To be done.
【0118】一方、前記無偏光は偏光面がランダムな光
であり、前記λ/4波長板502により各偏光面が均一
に回転するだけなので、無偏光のまま前記偏光ビームス
プリッタ501に入射される。このとき、前記無偏光の
一部、すなわち偏光面が前記偏光ビームスプリッタ50
1で反射する向きの成分だけが反射し、残りの成分は透
過する。また、前記ホットミラー7は赤外光をほぼ10
0%反射するため、前記撮像手段4で受光する光の光量
は、前記被計測物体2で反射した光の円偏光と無偏光の
混合比に依存するが、前記被計測物体2で反射した光の
光量の、おおよそ50%から100%となる。On the other hand, the non-polarized light is a light whose polarization plane is random, and since each polarization plane is uniformly rotated by the λ / 4 wavelength plate 502, it is incident on the polarization beam splitter 501 without polarization. . At this time, a part of the non-polarized light, that is, the plane of polarization is the polarization beam splitter 50.
Only the component in the direction of reflection at 1 is reflected, and the remaining components are transmitted. Further, the hot mirror 7 emits almost 10 infrared rays.
Since it reflects 0%, the amount of light received by the imaging unit 4 depends on the mixing ratio of the circularly polarized light and the non-polarized light of the light reflected by the measured object 2, but the light reflected by the measured object 2 The light amount is about 50% to 100%.
【0119】また、前記ホットミラー7Bを透過した可
視光は、図9に示したように、第2撮像手段8で受光
し、撮像される。このとき、前記第2撮像手段8は、前
記第1撮像手段4で撮影する範囲と同じ範囲を撮影でき
るように光学的距離を調整しておく。The visible light transmitted through the hot mirror 7B is received and imaged by the second image pickup means 8 as shown in FIG. At this time, the second image pickup means 8 adjusts the optical distance so that the same range as the range photographed by the first image pickup means 4 can be photographed.
【0120】本実施形態4の光照射受光装置1Dでは、
前記被計測物体2に照射する赤外光の光軸を、前記第1
撮像手段4で受光する赤外光の光軸と一致させているた
め、前記第1撮像手段4で撮影する領域内に赤外光があ
たらない領域(オクルージョン領域)が発生しない。In the light irradiation / reception device 1D of the fourth embodiment,
The optical axis of the infrared light irradiating the measured object 2 is set to the first
Since the optical axis of the infrared light received by the image pickup means 4 is matched, there is no area (occlusion area) where the infrared light does not fall within the area taken by the first image pickup means 4.
【0121】また、前記赤外光源301で発光した光の
光量のほぼ100%を前記被計測物体2に照射でき、前
記被計測物体2で反射した赤外光の光量の50%から1
00%を前記撮像手段4で受光することができるので、
従来のハーフミラーを用いた装置に比べ、撮像に利用で
きる光量を増加することができる。Further, almost 100% of the amount of light emitted from the infrared light source 301 can be applied to the measured object 2, and 50% to 1% of the amount of infrared light reflected by the measured object 2 can be applied.
Since 00% can be received by the image pickup means 4,
It is possible to increase the amount of light that can be used for imaging, as compared with a device using a conventional half mirror.
【0122】また、前記ホットミラー7Bを用いて、前
記被計測物体2で反射した光から可視光を分離し、前記
第2撮像手段8で受光し、撮像することにより、前記第
1撮像手段4で撮影した範囲の色情報を取得することが
できる。そのため、前記被計測物体2の形状及び色情報
を測定でき、前記被計測物体2を認識しやすくなる。Further, the visible light is separated from the light reflected by the object to be measured 2 by using the hot mirror 7B, the second image pickup means 8 receives the light, and the image is picked up, whereby the first image pickup means 4 is obtained. It is possible to acquire the color information of the range photographed in. Therefore, the shape and color information of the measured object 2 can be measured, and the measured object 2 can be easily recognized.
【0123】本実施形態4の光照射受光装置1Dも、主
に、前記被計測物体の三次元形状を測定したり、パター
ン認識をしたりするのに用いられる三次元形状測定装置
として用いられるが、その具体的な構成及び動作は、前
記実施形態3の装置と同様であるため、その説明は省略
する。The light irradiation / reception device 1D of the fourth embodiment is mainly used as a three-dimensional shape measuring device used for measuring the three-dimensional shape of the object to be measured and for pattern recognition. Since its specific configuration and operation are the same as those of the device of the third embodiment, description thereof will be omitted.
【0124】以上説明したように、本実施形態4の光照
射受光装置によれば、前記光軸一致手段5を用い、前記
被計測物体2に照射する光の光軸を前記第1撮像手段4
で受光する光の光軸と一致させることにより、前記被計
測物体2にオクルージョン領域が発生するのを防ぐこと
ができる。またこのとき、前記照射角調節手段302を
用いることにより、前記被計測物体2の撮影領域(撮像
画角)と同等あるいはやや広い領域のみに光を照射する
ことができ、光量を有効に利用することができる。As described above, according to the light irradiation / reception device of the fourth embodiment, the optical axis coincidence means 5 is used, and the optical axis of the light irradiated to the measured object 2 is measured by the first image pickup means 4.
By making it coincide with the optical axis of the light received by, it is possible to prevent an occlusion region from occurring in the measured object 2. Further, at this time, by using the irradiation angle adjusting means 302, it is possible to irradiate light only on an area equal to or slightly wider than the imaging area (imaging angle of view) of the measured object 2, and the light quantity is effectively utilized. be able to.
【0125】また、前記偏光ビームスプリッタ501及
びλ/4波長板502を用いることにより、前記撮像手
段4で受光する光の光量が、前記光源301で発光した
光の光量の50%から100%になるため、従来のハー
フミラーを用いた装置に比べ、光の利用効率を高くする
ことができる。また、前記光分離手段(ホットミラー)
7Bを用いることにより、前記被計測物体で反射した可
視光を前記第2撮像手段8で撮影することができ、前記
被計測物体2を認識するための情報量が増え、認識しや
すくなる。By using the polarization beam splitter 501 and the λ / 4 wavelength plate 502, the amount of light received by the image pickup means 4 is changed from 50% to 100% of the amount of light emitted by the light source 301. Therefore, the light utilization efficiency can be increased as compared with the conventional device using the half mirror. Also, the light separating means (hot mirror)
By using 7B, the visible light reflected by the measured object can be photographed by the second imaging means 8, the amount of information for recognizing the measured object 2 increases, and it becomes easy to recognize.
【0126】図10は、前記実施形態4の光照射受光装
置の変形例を示す模式図である。前記実施形態4の光照
射受光装置1Dでは、図9に示したように、前記λ/4
波長板502及び前記偏光ビームスプリッタ501を、
前記被計測物体2からの赤外光が前記ホットミラー7B
で反射する方向であり、かつ、前記ホットミラー7Bと
前記第1撮像手段4とを結ぶ直線上に、前記λ/4波長
板502、前記偏光ビームスプリッタ501の順に配置
しているが、これに限らず、図10に示すように、前記
ホットミラー7Bと前記発光手段3との間に、前記ホッ
トミラー7B側から、前記λ/4波長板502、前記偏
光ビームスプリッタ501の順に配置してもよい。FIG. 10 is a schematic diagram showing a modification of the light irradiation / reception device of the fourth embodiment. In the light irradiation / reception device 1D of the fourth embodiment, as shown in FIG.
The wave plate 502 and the polarization beam splitter 501 are
The infrared light from the measured object 2 is the hot mirror 7B.
The λ / 4 wavelength plate 502 and the polarization beam splitter 501 are arranged in this order on a straight line which is in the direction of reflection at and which connects the hot mirror 7B and the first image pickup means 4. Without being limited to this, as shown in FIG. 10, the λ / 4 wavelength plate 502 and the polarization beam splitter 501 may be arranged between the hot mirror 7B and the light emitting means 3 in this order from the hot mirror 7B side. Good.
【0127】図10に示したような配置の場合は、前記
赤外光源303は、発光した赤外光の偏光面が前記偏光
ビームスプリッタ501を透過するような向きに配置
し、前記第1撮像手段4は、前記被計測物体2で反射さ
れ、前記ホットミラー7B及び前記λ/4波長板502
を通った赤外光が、前記偏光ビームスプリッタ501で
反射する方向に配置することで、前記実施形態4の光照
射受光装置1Dと同じ効果を得ることができる。In the case of the arrangement shown in FIG. 10, the infrared light source 303 is arranged so that the plane of polarization of the emitted infrared light passes through the polarization beam splitter 501, and the first image pickup is performed. The means 4 is reflected by the measured object 2, and the hot mirror 7B and the λ / 4 wave plate 502 are included.
By arranging the infrared light that has passed through the polarization beam splitter 501 in a direction in which the infrared light is reflected, the same effect as that of the light irradiation and reception device 1D of the fourth embodiment can be obtained.
【0128】以上、本発明を、前記実施形態に基づき具
体的に説明したが、本発明は、前記実施形態に限定され
るものではなく、その要旨を逸脱しない範囲において種
々変更可能であることはもちろんである。Although the present invention has been specifically described based on the above embodiment, the present invention is not limited to the above embodiment, and various modifications can be made without departing from the scope of the invention. Of course.
【0129】[0129]
【発明の効果】本願において開示される発明の効果は、
以下のとおりである。
(1)発光手段で発光した光を被計測物体に照射し、前
記被計測物体からの反射光を受光して撮像する光照射受
光装置において、オクルージョン領域をなくすことがで
きる。
(2)発光手段で発光した光を被計測物体に照射し、前
記被計測物体からの反射光を受光して撮像する光照射受
光装置において、撮像範囲と照射範囲の調節を容易にす
ることができる。
(3)発光手段で発光した光を被計測物体に照射し、前
記被計測物体からの反射光を受光して撮像する光照射受
光装置において、発光手段で発光した光のロスを低減す
ることができる。
(4)発光手段で発光した光を被計測物体に照射し、前
記被計測物体からの反射光を受光して撮像する光照射受
光装置において、オクルージョン領域をなくし、かつ、
撮影範囲と照射範囲の調節を容易にするとともに、発光
手段で発光した光のロスを低減することができる。The effects of the invention disclosed in the present application are as follows.
It is as follows. (1) The occlusion area can be eliminated in the light irradiation and reception device that irradiates the object to be measured with the light emitted by the light emitting means, receives the reflected light from the object to be measured, and captures the image. (2) In the light irradiation and reception device that irradiates the light to be measured by the light emitting means to the object to be measured and receives the reflected light from the object to be measured to capture an image, it is possible to easily adjust the imaging range and the irradiation range. it can. (3) In a light irradiation and reception device that irradiates the light to be measured by the light emitting means onto the object to be measured and receives and reflects the reflected light from the object to be measured, it is possible to reduce the loss of the light emitted from the light emitting means. it can. (4) In a light irradiation / light receiving device that irradiates light to be measured by the light emitting means to an object to be measured and receives reflected light from the object to be measured to capture an image, eliminating an occlusion area, and
It is possible to easily adjust the shooting range and the irradiation range and reduce the loss of the light emitted by the light emitting means.
【図1】本発明による実施形態1の光照射受光装置の概
略構成を示す模式図である。FIG. 1 is a schematic diagram showing a schematic configuration of a light irradiation / reception device according to a first embodiment of the present invention.
【図2】本実施形態1の光照射受光装置の動作を説明す
るための模式図である。FIG. 2 is a schematic diagram for explaining the operation of the light irradiation / reception device of the first embodiment.
【図3】本実施形態1の光照射受光装置の動作を説明す
るための模式図である。FIG. 3 is a schematic diagram for explaining the operation of the light irradiation / reception device of the first embodiment.
【図4】本実施形態1の光照射受光装置の具体的な構成
例を示す模式図である。FIG. 4 is a schematic diagram showing a specific configuration example of the light irradiation / reception device of the first embodiment.
【図5】本発明による実施形態2の光照射受光装置の概
略構成を示す模式図である。FIG. 5 is a schematic diagram showing a schematic configuration of a light irradiation / reception device according to a second embodiment of the present invention.
【図6】本発明による実施形態3の光照射受光装置の概
略構成を示す模式図である。FIG. 6 is a schematic diagram showing a schematic configuration of a light irradiation / reception device of a third embodiment according to the present invention.
【図7】本実施形態3の光照射受光装置の具体的な構成
例を示す模式図である。FIG. 7 is a schematic diagram showing a specific configuration example of the light irradiation / reception device of the third embodiment.
【図8】前記実施形態3の光照射受光装置の変形例を示
す模式図である。FIG. 8 is a schematic diagram showing a modified example of the light irradiation / reception device of the third embodiment.
【図9】本発明による実施形態4の光照射受光装置の概
略構成を示す模式図である。FIG. 9 is a schematic diagram showing a schematic configuration of a light irradiation / reception device of a fourth embodiment according to the present invention.
【図10】前記実施形態4の光照射受光装置の変形例を
示す模式図である。FIG. 10 is a schematic diagram showing a modified example of the light irradiation / reception device of the fourth embodiment.
【図11】従来のアクティブ型計測方法を説明するため
の模式図である。FIG. 11 is a schematic diagram for explaining a conventional active measurement method.
【図12】従来のアクティブ型計測方法の課題を説明す
るための模式図である。FIG. 12 is a schematic diagram for explaining the problems of the conventional active measurement method.
【図13】従来のアクティブ型計測方法の課題を説明す
るための模式図である。FIG. 13 is a schematic diagram for explaining a problem of a conventional active measurement method.
【図14】従来のアクティブ型計測方法の課題を説明す
るための模式図である。FIG. 14 is a schematic diagram for explaining a problem of a conventional active measurement method.
【図15】従来のアクティブ型計測方法の課題を説明す
るための模式図である。FIG. 15 is a schematic diagram for explaining the problems of the conventional active measurement method.
1A,1B,1C,1D…光照射受光装置、2…被計測
物体、3…発光手段、301…光源、302…照射角調
節手段、303…赤外光源、4…撮像手段(第1撮像手
段)、401…ゲート付きMCP、402…リレーレン
ズ、403…撮像カメラ、404…バンドパスフィル
タ、5…光軸一致手段、501…変更ビームスプリッ
タ、502…λ/4波長板、6…焦点調節手段、7A…
コールドミラー、7B…ホットミラー、8…第2撮像手
段、9…ミラー、10…ハーフミラー。1A, 1B, 1C, 1D ... Light irradiation / receiving device, 2 ... Object to be measured, 3 ... Light emitting means, 301 ... Light source, 302 ... Irradiation angle adjusting means, 303 ... Infrared light source, 4 ... Imaging means (first imaging means) ), 401 ... MCP with gate, 402 ... Relay lens, 403 ... Imaging camera, 404 ... Bandpass filter, 5 ... Optical axis matching means, 501 ... Change beam splitter, 502 ... λ / 4 wavelength plate, 6 ... Focus adjusting means , 7A ...
Cold mirror, 7B ... Hot mirror, 8 ... Second imaging means, 9 ... Mirror, 10 ... Half mirror.
───────────────────────────────────────────────────── フロントページの続き Fターム(参考) 2F065 AA53 BB05 DD00 DD05 FF04 FF32 FF49 GG06 GG22 HH02 HH09 HH12 JJ03 JJ05 JJ26 LL04 LL20 LL22 LL30 LL33 LL36 LL37 MM22 PP22 QQ24 QQ25 UU01 UU02 UU07 2H099 AA00 BA09 BA17 CA07 ─────────────────────────────────────────────────── ─── Continued front page F term (reference) 2F065 AA53 BB05 DD00 DD05 FF04 FF32 FF49 GG06 GG22 HH02 HH09 HH12 JJ03 JJ05 JJ26 LL04 LL20 LL22 LL30 LL33 LL36 LL37 MM22 PP22 QQ24 QQ25 UU01 UU02 UU07 2H099 AA00 BA09 BA17 CA07
Claims (14)
手段と、前記被計測物体で反射した光を受光して撮像す
る撮像手段と、前記被計測物体に照射する光の光軸と前
記撮像手段で受光する光の光軸とを一致させる光軸一致
手段と、前記撮像手段で撮像する像の焦点を調節する焦
点調節手段とを備える光照射受光装置であって、前記発
光手段は、単色かつ直線偏光の光を発光する光源と、前
記光源で発光した光の照射角を調節する照射角調節手段
とを備え、前記光軸一致手段は、入射する光の偏光面の
向きに応じて、光を反射あるいは透過させる偏光ビーム
スプリッタと、入射した光の偏光面を45度回転させる
λ/4波長板とを備え、前記λ/4波長板は、前記偏光
ビームスプリッタと前記被計測物体との間に配置されて
いることを特徴とする光照射受光装置。1. A light emitting means for emitting light for irradiating an object to be measured, an image pickup means for receiving and imaging light reflected by the object to be measured, an optical axis of light applied to the object to be measured, and the A light irradiation and light receiving device comprising: an optical axis matching means for matching an optical axis of light received by the image pickup means; and a focus adjustment means for adjusting the focus of an image picked up by the image pickup means, wherein the light emitting means comprises: A light source that emits monochromatic and linearly polarized light, and an irradiation angle adjusting means that adjusts the irradiation angle of the light emitted by the light source, the optical axis matching means, depending on the direction of the polarization plane of the incident light. A polarization beam splitter that reflects or transmits light, and a λ / 4 wavelength plate that rotates a polarization plane of incident light by 45 degrees, and the λ / 4 wavelength plate includes the polarization beam splitter and the object to be measured. Characterized by being placed between Light irradiating the light-receiving device.
は、前記被計測物体と前記撮像手段とを結ぶ直線上に、
前記被計測物体側から、前記焦点調節手段、前記光軸一
致手段の順に配置され、前記光源は、発光した光の偏光
面が前記偏光ビームスプリッタで反射される向きにな
り、かつ、前記偏光ビームスプリッタで反射した光が前
記被計測物体に照射されるように配置され、前記照射角
調節手段は、前記光源と前記偏光ビームスプリッタの間
に配置されていることを特徴とする請求項1に記載の光
照射受光装置。2. The optical axis matching means and the focus adjusting means are on a straight line connecting the object to be measured and the imaging means,
The focus adjusting means and the optical axis matching means are arranged in this order from the measured object side, and the light source is oriented such that the polarization plane of the emitted light is reflected by the polarization beam splitter, and the polarization beam. The light reflected by the splitter is arranged so as to be irradiated onto the object to be measured, and the irradiation angle adjusting means is arranged between the light source and the polarization beam splitter. Light irradiation and light receiving device.
は、前記被計測物体と前記発光手段とを結ぶ直線上に、
前記被計測物体側から、前記焦点調節手段、前記光軸一
致手段の順に配置され、前記光源は、発光した光の偏光
面が、前記偏光ビームスプリッタを透過する向きになる
ように配置され、前記撮像手段は、前記被計測物体から
の反射光が、前記偏光ビームスプリッタで反射する方向
に配置されており、前記照射角調節手段は、前記光源と
前記偏光ビームスプリッタの間に配置されていることを
特徴とする請求項1に記載の光照射受光装置。3. The optical axis matching means and the focus adjusting means are on a straight line connecting the object to be measured and the light emitting means,
The focus adjusting unit and the optical axis matching unit are arranged in this order from the measured object side, and the light source is arranged such that the polarization plane of the emitted light is in a direction of passing through the polarization beam splitter. The imaging means is arranged in a direction in which the reflected light from the object to be measured is reflected by the polarization beam splitter, and the irradiation angle adjusting means is arranged between the light source and the polarization beam splitter. The light irradiation / reception device according to claim 1.
赤外光発光手段と、前記被計測物体で反射した赤外光を
受光して撮像する第1撮像手段と、前記被計測物体に照
射する赤外光の光軸と、前記第1撮像手段で受光する赤
外光の光軸を一致させる光軸一致手段と、前記第1撮像
手段で撮像する像の焦点を調節する焦点調節手段と、前
記被計測物体で反射した光を赤外光と可視光に分離する
光分離手段と、前記光分離手段によって分離した可視光
を受光して撮像する第2撮像手段を備える光照射受光装
置であって、前記赤外光発光手段は、直線偏光の赤外光
を発光する赤外光源と、前記赤外光源で発光した赤外光
の照射角を調節する照射角調節手段とを備え、前記光軸
一致手段は、入射する光の偏光面の向きに応じて光を反
射あるいは透過させる偏光ビームスプリッタと、入射し
た光の偏光面を45度回転させるλ/4波長板とを備
え、前記光分離手段及び前記λ/4波長板は、前記偏光
ビームスプリッタと前記被計測物体との間に、前記被計
測物体側から、前記光分離手段、前記λ/4波長板の順
に配置されていることを特徴とする光照射受光装置。4. An infrared light emitting means for emitting infrared light for irradiating an object to be measured, a first image pickup means for receiving and imaging infrared light reflected by the object to be measured, and the object to be measured. Optical axis matching means for matching the optical axis of infrared light irradiating the same with the optical axis of infrared light received by the first imaging means, and focus adjustment for adjusting the focus of the image captured by the first imaging means. Light irradiation / reception including: a light separation unit that separates the light reflected by the object to be measured into infrared light and visible light; and a second imaging unit that receives and images the visible light separated by the light separation unit. In the device, the infrared light emitting means includes an infrared light source for emitting linearly polarized infrared light, and an irradiation angle adjusting means for adjusting an irradiation angle of the infrared light emitted by the infrared light source. , The optical axis matching means reflects or transmits light depending on the direction of the plane of polarization of the incident light. And a λ / 4 wavelength plate for rotating the plane of polarization of incident light by 45 degrees, wherein the light splitting means and the λ / 4 wavelength plate are provided between the polarization beam splitter and the object to be measured. A light irradiation / reception device characterized in that the light separating means and the λ / 4 wavelength plate are arranged in this order from the side of the measured object.
視光を反射するコールドミラーであり、前記焦点調節手
段、前記コールドミラー、前記λ/4波長板、及び前記
偏光ビームスプリッタは、前記被計測物体と前記第1撮
像手段とを結ぶ直線上に、前記被計測物体側から、前記
焦点調節手段、前記コールドミラー、前記λ/4波長
板、前記偏光ビームスプリッタの順に配置され、前記赤
外光源は、発光した赤外光の偏光面が前記偏光ビームス
プリッタで反射する向きになり、かつ、前記偏光ビーム
スプリッタで反射した赤外光が前記被計測物体に照射さ
れるように配置され、前記第2撮像手段は、前記被計測
物体からの可視光が前記コールドミラーで反射する方向
に配置されていることを特徴とする請求項4に記載の光
照射受光装置。5. The light splitting means is a cold mirror that transmits infrared light and reflects visible light, and the focus adjusting means, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are A focus adjustment means, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are arranged in this order from the measured object side on a straight line connecting the measured object and the first imaging means, The infrared light source is arranged such that the plane of polarization of the emitted infrared light is oriented to be reflected by the polarization beam splitter, and the infrared light reflected by the polarization beam splitter is applied to the measured object. The light irradiation / reception device according to claim 4, wherein the second imaging unit is arranged in a direction in which visible light from the measured object is reflected by the cold mirror.
視光を反射するコールドミラーであり、前記焦点調節手
段、前記コールドミラー、前記λ/4波長板、及び前記
偏光ビームスプリッタは、前記被計測物体と前記赤外光
発光手段とを結ぶ直線上に、前記被計測物体側から、前
記焦点調節手段、前記コールドミラー、前記λ/4波長
板、前記偏光ビームスプリッタの順に配置され、前記赤
外光源は、発光した赤外光の偏光面が前記偏光ビームス
プリッタを透過する向きになるように配置され、前記第
1撮像手段は、前記被計測物体で反射され、前記コール
ドミラー及び前記λ/4波長板を通った赤外光が前記偏
光ビームスプリッタで反射する方向に配置され、前記第
2撮像手段は、前記被計測物体からの可視光が前記コー
ルドミラーで反射する方向に配置されていることを特徴
とする請求項4に記載の光照射受光装置。6. The light separating means is a cold mirror that transmits infrared light and reflects visible light, and the focus adjusting means, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are The focus adjustment means, the cold mirror, the λ / 4 wavelength plate, and the polarization beam splitter are arranged in this order from the measured object side on a straight line connecting the measured object and the infrared light emitting means. The infrared light source is arranged such that the plane of polarization of the emitted infrared light is oriented to pass through the polarization beam splitter, the first imaging means is reflected by the measured object, and the cold mirror and The infrared light that has passed through the λ / 4 wave plate is arranged in a direction in which it is reflected by the polarization beam splitter, and the second imaging unit reflects visible light from the measured object by the cold mirror. The light irradiation and reception device according to claim 4, wherein the light irradiation and reception device is arranged in a direction.
視光を透過するホットミラーであり、前記ホットミラー
と前記焦点調節手段は、前記被計測物体と前記第2撮像
手段とを結ぶ直線上に、前記被計測物体側から前記焦点
調節手段、前記ホットミラーの順に配置され、前記λ/
4波長板及び前記偏光ビームスプリッタは、前記被計測
物体からの赤外光が前記ホットミラーで反射する方向で
あり、かつ、前記ホットミラーと前記第1撮像手段とを
結ぶ直線上に、前記λ/4波長板、前記偏光ビームスプ
リッタの順に配置され、前記赤外光源は、発光した赤外
光の偏光面が前記偏光ビームスプリッタで反射する向き
になり、かつ、前記被計測物体に照射されるように配置
されていることを特徴とする請求項4に記載の光照射受
光装置。7. The light separating means is a hot mirror that reflects infrared light and transmits visible light, and the hot mirror and the focus adjusting means connect the measured object and the second imaging means. On the connecting straight line, the focus adjusting means and the hot mirror are arranged in this order from the measured object side, and the λ /
The four-wave plate and the polarization beam splitter are in a direction in which infrared light from the object to be measured is reflected by the hot mirror, and on the straight line connecting the hot mirror and the first imaging means, the λ The / 4 wavelength plate and the polarization beam splitter are arranged in this order, and the infrared light source is oriented such that the polarization plane of the emitted infrared light is reflected by the polarization beam splitter and is irradiated to the object to be measured. The light irradiation / reception device according to claim 4, wherein the light irradiation / reception device is arranged as follows.
視光を透過するホットミラーであり、前記ホットミラー
と前記焦点調節手段は、前記被計測物体と前記第2撮像
手段とを結ぶ直線上に、前記被計測物体側から、前記焦
点調節手段、前記ホットミラーの順に配置され、前記偏
光ビームスプリッタ及び前記λ/4波長板は、前記ホッ
トミラーと前記赤外光発光手段との間に、前記ホットミ
ラー側から、前記λ/4波長板、前記偏光ビームスプリ
ッタの順に配置され、前記赤外光源は、発光した赤外光
の偏光面が前記偏光ビームスプリッタを透過するような
向きに配置され、前記第1撮像手段は、前記被計測物体
で反射され、前記ホットミラー及び前記λ/4波長板を
通った赤外光が、前記偏光ビームスプリッタで反射する
方向に配置されていることを特徴とする請求項4に記載
の光照射受光装置。8. The light separating means is a hot mirror that reflects infrared light and transmits visible light, and the hot mirror and the focus adjusting means connect the measured object and the second imaging means. The focus adjusting means and the hot mirror are arranged in this order on the connecting straight line from the side of the object to be measured, and the polarization beam splitter and the λ / 4 wavelength plate are arranged between the hot mirror and the infrared light emitting means. The λ / 4 wavelength plate and the polarization beam splitter are arranged in this order from the hot mirror side, and the infrared light source is oriented so that the polarization plane of the emitted infrared light passes through the polarization beam splitter. And the first imaging means is arranged in a direction in which the infrared light reflected by the object to be measured and passing through the hot mirror and the λ / 4 wavelength plate is reflected by the polarization beam splitter. The light irradiation / reception device according to claim 4, wherein
前記照射光の照射角を調節し、前記照射角を調節した照
射光を被計測物体に照射し、前記被計測物体で反射した
反射光を受光する光照射受光方法において、単色かつ直
線偏光の照射光を発光し、前記照射角を調節した照射光
を偏光ビームスプリッタで反射させ、前記偏光ビームス
プリッタで反射させた照射光の偏光面を45度回転させ
てから前記被計測物体に照射し、前記被計測物体で反射
した反射光の偏光面をさらに45度回転させ、前記偏光
ビームスプリッタを透過させて受光することを特徴とす
る光照射受光方法。9. An irradiation light for irradiating an object to be measured is emitted,
In the light irradiation and receiving method of adjusting the irradiation angle of the irradiation light, irradiating the irradiation light with the irradiation angle adjusted to the object to be measured, and receiving the reflected light reflected by the object to be measured, irradiation of monochromatic and linearly polarized light Light is emitted, the irradiation light whose irradiation angle is adjusted is reflected by a polarization beam splitter, the polarization plane of the irradiation light reflected by the polarization beam splitter is rotated by 45 degrees, and then the object to be measured is irradiated, A light irradiation / reception method characterized in that the plane of polarization of the reflected light reflected by the object to be measured is further rotated by 45 degrees, and is transmitted through the polarization beam splitter to receive light.
し、前記照射光の照射角を調節し、前記照射角を調節し
た照射光を被計測物体に照射し、前記被計測物体で反射
した反射光を受光する光照射受光方法において、単色か
つ直線偏光の照射光を発光し、前記照射角を調節した照
射光を偏光ビームスプリッタで透過させ、前記偏光ビー
ムスプリッタを透過した照射光の偏光面を45度回転さ
せてから前記被計測物体に照射し、前記被計測物体で反
射した反射光の偏光面をさらに45度回転させ、前記偏
光ビームスプリッタで反射させて受光することを特徴と
する光照射受光方法。10. Irradiation light for irradiating an object to be measured is emitted, the irradiation angle of the irradiation light is adjusted, and the irradiation light with the adjusted irradiation angle is applied to the object to be measured and reflected by the object to be measured. In the light irradiation / reception method of receiving reflected light, a monochromatic and linearly polarized irradiation light is emitted, the irradiation light whose irradiation angle is adjusted is transmitted by a polarization beam splitter, and the polarization plane of the irradiation light transmitted by the polarization beam splitter is transmitted. Is rotated by 45 degrees and then irradiates the measured object, the polarization plane of the reflected light reflected by the measured object is further rotated by 45 degrees, and is reflected by the polarization beam splitter to receive light. Irradiation method.
光の照射角を調節し、前記照射角を調節した赤外光を被
計測物体に照射し、前記被計測物体で反射した赤外光及
び可視光を受光する光照射受光方法において、前記照射
角を調節した赤外光を偏光ビームスプリッタで反射さ
せ、前記偏光ビームスプリッタで反射させた赤外光の偏
光面を45度回転させてから前記被計測物体に照射し、
前記被計測物体で反射した光を赤外光と可視光に分離
し、前記分離した赤外光の偏光面をさらに45度回転さ
せ、前記偏光ビームスプリッタを透過させて受光するこ
とを特徴とする光照射受光方法。11. The linearly polarized infrared light is emitted, the irradiation angle of the infrared light is adjusted, the infrared light with the adjusted irradiation angle is irradiated to the object to be measured, and reflected by the object to be measured. In a light irradiation / reception method of receiving infrared light and visible light, the infrared light whose irradiation angle is adjusted is reflected by a polarization beam splitter, and the polarization plane of the infrared light reflected by the polarization beam splitter is rotated by 45 degrees. After irradiating the measured object,
The light reflected by the measured object is separated into infrared light and visible light, the polarization plane of the separated infrared light is further rotated by 45 degrees, and the light is transmitted through the polarization beam splitter and received. Light irradiation and light receiving method.
光の照射角を調節し、前記照射角を調節した赤外光を被
計測物体に照射し、前記被計測物体で反射した赤外光及
び可視光を受光する光照射受光方法において、前記照射
角を調節した赤外光を偏光ビームスプリッタで透過し、
前記偏光ビームスプリッタで反射させた赤外光の偏光面
を45度回転させてから前記被計測物体に照射し、前記
被計測物体で反射した光を赤外光と可視光に分離し、前
記分離した赤外光の偏光面をさらに45度回転させ、前
記偏光ビームスプリッタで反射して受光することを特徴
とする光照射受光方法。12. Linearly polarized infrared light is emitted, the irradiation angle of the infrared light is adjusted, the infrared light with the adjusted irradiation angle is irradiated to the object to be measured, and reflected by the object to be measured. In the light irradiation receiving method of receiving infrared light and visible light, the infrared light adjusted the irradiation angle is transmitted by a polarization beam splitter,
The polarization plane of the infrared light reflected by the polarization beam splitter is rotated by 45 degrees, and then the measured object is irradiated with the light, and the light reflected by the measured object is separated into infrared light and visible light. The method for irradiating and receiving light, characterized in that the polarization plane of the infrared light is further rotated by 45 degrees, and the infrared light is reflected and received by the polarization beam splitter.
ルドミラーを用い、赤外光を透過させ、可視光を反射さ
せて分離することを特徴とする請求項11または請求項
12に記載の光照射受光方法。13. The light reflected by the object to be measured is transmitted through infrared light using a cold mirror, and is reflected by visible light to be separated. Light irradiation and light receiving method.
トミラーを用い、赤外光を反射させ、可視光を透過させ
て分離することを特徴とする請求項11または請求項1
2に記載の光照射受光方法。14. The light reflected by the object to be measured is separated by separating it by reflecting infrared light and transmitting visible light using a hot mirror.
2. The light irradiation / reception method described in 2.
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|---|---|---|---|
| JP2001375625A JP3766326B2 (en) | 2001-12-10 | 2001-12-10 | Light irradiation receiver |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2001375625A JP3766326B2 (en) | 2001-12-10 | 2001-12-10 | Light irradiation receiver |
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| Publication Number | Publication Date |
|---|---|
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| JP3766326B2 JP3766326B2 (en) | 2006-04-12 |
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|---|---|---|---|
| JP2001375625A Expired - Fee Related JP3766326B2 (en) | 2001-12-10 | 2001-12-10 | Light irradiation receiver |
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| Country | Link |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JP2007526453A (en) * | 2004-01-28 | 2007-09-13 | カネスタ インコーポレイテッド | Single chip red, green, blue, distance (RGB-Z) sensor |
| JP2008126984A (en) * | 2006-11-27 | 2008-06-05 | Nippon Seiki Co Ltd | Head-up display device |
| JP2011530097A (en) * | 2008-08-03 | 2011-12-15 | マイクロソフト インターナショナル ホールディングス ビイ.ヴイ. | Rolling camera system |
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