Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0563773B2 - - Google Patents
[go: Go Back, main page]

JPH0563773B2 - - Google Patents

Info

Publication number
JPH0563773B2
JPH0563773B2 JP30803186A JP30803186A JPH0563773B2 JP H0563773 B2 JPH0563773 B2 JP H0563773B2 JP 30803186 A JP30803186 A JP 30803186A JP 30803186 A JP30803186 A JP 30803186A JP H0563773 B2 JPH0563773 B2 JP H0563773B2
Authority
JP
Japan
Prior art keywords
measurement light
light beam
reflected
objective lens
optical
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP30803186A
Other languages
Japanese (ja)
Other versions
JPS63163315A (en
Inventor
Katsushige Nakamura
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitaka Kohki Co Ltd
Original Assignee
Mitaka Kohki Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitaka Kohki Co Ltd filed Critical Mitaka Kohki Co Ltd
Priority to JP30803186A priority Critical patent/JPS63163315A/en
Publication of JPS63163315A publication Critical patent/JPS63163315A/en
Publication of JPH0563773B2 publication Critical patent/JPH0563773B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Measurement Of Optical Distance (AREA)
  • Automatic Focus Adjustment (AREA)

Description

【発明の詳細な説明】 〈産業上の利用分野〉 この発明は透明体の表面への焦点位置合わせに
好適な非接触自動焦点位置合わせ方法に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a non-contact automatic focusing method suitable for focusing on the surface of a transparent body.

〈従来の技術〉 様々なサイズ、形状、物性を有する対象物へ、
光学的に非接触で焦点位置合わせすることは、技
述的に難しい問題である。しかし、その非接触に
よる焦点位置合わせ技術の用途が非常に多くある
ことから、今でも多くの学者が研究を重ねている
課題である。
<Conventional technology> For objects with various sizes, shapes, and physical properties,
Optically contactless focusing is a technically difficult problem. However, because there are so many uses for this non-contact focusing technology, it is still a subject that many scholars are researching.

そして、従来行われてきた一般的な焦点位置合
わせ技術として、コンピユータを利用した画像処
理技術があるが、この画像処理技術にあつては、
装置が大掛かりになること、また画像走査を行う
ので焦点位置合わせ速度が遅いこと等の問題点が
多くあり、あまり実用的であるとは言えなかつ
た。
As a conventional focus positioning technique, there is an image processing technique using a computer.
There are many problems such as the large size of the device and the slow focus positioning speed due to image scanning, so it cannot be said to be very practical.

そこで、本発明者は上記の如き要請に応じるた
め、長年にわたる鋭意研究をしてきた結果とし
て、先に非接触自動位置合わせ装置(特願昭60−
214773号参照)を提案した。
Therefore, in order to meet the above-mentioned demands, the present inventor has conducted intensive research over many years and has developed a non-contact automatic positioning device (patent application filed in 1983-
214773)).

〈発明が解決しようとする問題点〉 しかしながら、昨今の技術進歩の速さに応じ
て、光学的感知の難しい透明体にも光学的に焦点
位置合わせを行わなければならない場合が多くな
つてきた。しかも、透明体はその表面に画像が存
在しないので、前記の画像処理技術で透明体に対
応することは不可能である。
<Problems to be Solved by the Invention> However, with the recent speed of technological progress, it has become increasingly necessary to perform optical focus positioning even on transparent objects that are difficult to detect optically. Moreover, since a transparent body does not have an image on its surface, it is impossible to deal with transparent bodies using the image processing techniques described above.

そこで、本発明者は先の提案に基づいて研究を
重ね、そのような光学的に感知の難しい透明体で
も、正確且つ瞬時に焦点位置合わせできる方法を
開発したものである。
Therefore, the inventor of the present invention conducted extensive research based on the above proposal and developed a method that enables accurate and instantaneous focus positioning even for such transparent objects that are optically difficult to detect.

〈問題点を解決するための手段〉 この発明に係る非接触自動焦点位置合わせ方法
は、上記の目的を達成するために、光学機構の光
軸と平行に発せられた測定光束としての偏光He
−Neレーザ光線を、光軸に対して45度の傾斜角
度を保ちつつ平行移動自在な可動ミラーにて反射
し、該可動ミラーにて反射された測定光束を、光
軸と45度の傾斜角度で配された固定ミラーにて反
射し、該固定ミラーにて反射された測定光束を、
対物レンズで屈折せしめてから透明体て向けて照
射し、該透明体の表面で反射された測定光束を、
再度対物レンズに屈折せしめてから光位置検出器
にて受光し、該光位置検出器からの位置信号に対
応する焦点位置合わせ機構にて、少なくとも透明
体と対物レンズとの間の距離を調整することによ
り、測定光束を透明体の表面へ自動的に焦点位置
合わせするものであつて、 前記可動ミラーを反透明体側へ平行移動させる
ことにより固定ミラーにて反射された測定光束を
対物レンズの外周部側で屈折せしめ、測定光束を
大きい照射角度でもつて透明体へ照射し、そして
透明体の表面以外で反射する測定光束を対物レン
ズに入射不能な方向に反射させるものである。
<Means for Solving the Problems> In order to achieve the above object, the non-contact automatic focusing method according to the present invention uses polarized He as a measurement light beam emitted parallel to the optical axis of an optical mechanism.
-The Ne laser beam is reflected by a movable mirror that can be moved in parallel while maintaining an inclination angle of 45 degrees with respect to the optical axis, and the measurement light beam reflected by the movable mirror is reflected at an inclination angle of 45 degrees with respect to the optical axis. The measurement light beam reflected by the fixed mirror is reflected by the fixed mirror arranged at
After being refracted by an objective lens, it is irradiated onto a transparent body, and the measurement light beam reflected on the surface of the transparent body is
After being refracted by the objective lens, the light is received by an optical position detector, and at least the distance between the transparent body and the objective lens is adjusted by a focus positioning mechanism corresponding to the position signal from the optical position detector. By this, the measurement light beam is automatically focused on the surface of the transparent body, and by moving the movable mirror in parallel to the side opposite to the transparent body, the measurement light beam reflected by the fixed mirror is focused on the outer periphery of the objective lens. The measurement light beam is refracted on the transparent body side, and the measurement light beam is irradiated onto the transparent body at a large irradiation angle, and the measurement light beam that is reflected on a surface other than the surface of the transparent body is reflected in a direction that cannot be incident on the objective lens.

〈作用〉 可動ミラーを反透明体側へ平行移動させること
により、固定ミラーにおける測定光束の反射点を
反光軸側へ変化させ、測定光束を光軸から離反さ
せる。測定光束が光軸から離反すると、測定光束
は対物レンズの外周部側で屈折し、光軸に対する
大きい照射角度でもつて透明体に照射される。す
ると透明体の表面以外(例えば透明体の裏面、透
明体の裏面側に接合された不透明体、透明体の内
部に設けられた不透明体、透明体の裏面側に離間
配置された不透明体)にて反射された測定光束
は、対物レンズに入射不能な方向に反射される。
<Operation> By moving the movable mirror in parallel toward the opposite side of the transparent body, the reflection point of the measurement light beam on the fixed mirror is changed to the side opposite to the optical axis, and the measurement light beam is separated from the optical axis. When the measurement light beam moves away from the optical axis, the measurement light beam is refracted at the outer peripheral side of the objective lens and is irradiated onto the transparent body at a large irradiation angle with respect to the optical axis. Then, other than the surface of the transparent body (for example, the back of the transparent body, the opaque body bonded to the back side of the transparent body, the opaque body provided inside the transparent body, the opaque body spaced apart on the back side of the transparent body) The measurement light beam reflected by the object lens is reflected in a direction in which it cannot enter the objective lens.

<実施例> 以下この発明の好適な実施例を図面に基づいて
説明する。
<Embodiments> Preferred embodiments of the present invention will be described below based on the drawings.

第1実施例 第1図〜第5図はこの発明の第1実施例を示す
図である。
First Embodiment FIGS. 1 to 5 are diagrams showing a first embodiment of the present invention.

まず最初に本発明を実施するための装置の基本
構造を第1図〜第3図に基づいて説明する。
First, the basic structure of an apparatus for carrying out the present invention will be explained based on FIGS. 1 to 3.

1はレーザ機構、2は光学機構〔図中二点鎖線
で囲んだ部分〕、3は焦点位置合わせ機構、4は
対象物、をそれぞれ示している。
Reference numeral 1 indicates a laser mechanism, 2 an optical mechanism (encircled by a two-dot chain line in the figure), 3 a focus positioning mechanism, and 4 an object.

レーザ機構1は、測定光束aとしての偏光He
−Neレーザ光線、つまり偏光されたHe−Neレ
ーザ光線を、後述する光学機構2の光軸5と平行
に発するものである。
The laser mechanism 1 emits polarized light He as the measurement light flux a.
-Ne laser beam, that is, a polarized He--Ne laser beam, is emitted parallel to the optical axis 5 of optical mechanism 2, which will be described later.

光学機構2は、可動ミラー6、固定ミラー7、
対物レンズ8、結像レンズ9、拡大レンズ10、
光位置検出器11、とを備えている。可動ミラー
6は、レーザ機構1から発せられた測定光束a
を、光軸5に対して平行移動しつつ直角方向へ反
射できるようになつている。固定ミラー7はハー
フミラーで、前記可動ミラー6にて反射された測
定光束bを再度直角に反射し、光軸5と平行な測
定光束cとするものである。固定ミラー7におけ
る反射点12は、可動ミラー6の平行移動位置に
応じて変化するものであり、またこの固定ミラー
7における反射点12の位置に応じて、固定ミラ
ー7から反射される測定光束cは光軸5に対して
接近・離反自在となる。
The optical mechanism 2 includes a movable mirror 6, a fixed mirror 7,
Objective lens 8, imaging lens 9, magnifying lens 10,
An optical position detector 11 is provided. The movable mirror 6 receives the measurement light beam a emitted from the laser mechanism 1.
can be reflected in a perpendicular direction while moving parallel to the optical axis 5. The fixed mirror 7 is a half mirror that reflects the measurement light beam b reflected by the movable mirror 6 at right angles again to form a measurement light beam c parallel to the optical axis 5. The reflection point 12 on the fixed mirror 7 changes depending on the parallel movement position of the movable mirror 6, and the measurement light beam c reflected from the fixed mirror 7 changes depending on the position of the reflection point 12 on the fixed mirror 7. can approach and move away from the optical axis 5.

次に、固定ミラー7にて反射された測定光束c
は、対物レンズ8にて屈折せしめられた後に対象
物4へ照射され、測定光束dとなつて焦点p1が
表面4aに合致する。対象物4への測定光束dの
照射角度θは、測定光束cの光軸5との距離に応
じて決定される。つまり、固定ミラー7で反射さ
れた測定光束cが光軸5から離反している場合
は、測定光束cは対物レンズ8の外周部側で屈折
するので大きい照射角度θでもつて対象物4へ照
射される。逆に、測定光束cが光軸5に接近して
いる場合は、測定光束cは対物レンズ8の中心部
側で屈折するので小さい照射角度θでもつて対象
物4へ照射されるものである。
Next, the measurement light beam c reflected by the fixed mirror 7
is refracted by the objective lens 8 and then irradiated onto the object 4, becoming a measuring light beam d whose focal point p1 coincides with the surface 4a. The irradiation angle θ of the measurement light beam d onto the object 4 is determined according to the distance of the measurement light beam c from the optical axis 5. In other words, when the measurement light beam c reflected by the fixed mirror 7 is away from the optical axis 5, the measurement light beam c is refracted at the outer peripheral side of the objective lens 8, so that it is irradiated onto the object 4 even at a large irradiation angle θ. be done. On the other hand, when the measurement light beam c is close to the optical axis 5, the measurement light beam c is refracted toward the center of the objective lens 8, so that it is irradiated onto the object 4 even at a small irradiation angle θ.

対象物4の表面4aにおいて照射角度θと同じ
反射角度でもつて反射した測定光束eは、対物レ
ンズ8にて再度屈折せしめられて光軸5と平行な
測定光束fとなる。この測定光束fは結像レンズ
9にて更に屈折されて測定光束gとなり、光軸5
上の再結像点p2を経て拡大レンズ10へと導か
れる。そして、測定光束gはこの拡大レンズ10
にて屈折され、測定光束hとなつて光位置検出器
11の2分割ホトセンサー11a,11bで受光
される。
The measurement light beam e reflected at the same reflection angle as the irradiation angle θ on the surface 4a of the object 4 is refracted by the objective lens 8 to become a measurement light beam f parallel to the optical axis 5. This measurement light flux f is further refracted by the imaging lens 9 to become a measurement light flux g, and the optical axis 5
It is guided to the magnifying lens 10 via the upper reimaging point p2. Then, the measurement light flux g is this magnifying lens 10
The light beam is refracted at , becomes a measurement light beam h, and is received by the two-split photosensors 11a and 11b of the optical position detector 11.

そして、この光位置検出器11としては、半導
体光位置検出器(PSD)を採用した。この半導
体光位置検出器(PSD)は、画像上で走査を行
わず入射光の位置情報を含んだ位置信号を得るこ
とができ、CCD,MOS等の固体撮像素子に比べ
て、より高い分解能を持ち高いサンプリンググレ
ードを得ることができる。そして、この光位置検
出器11は焦点位置合わせ機構3と電気的に接続
されており、光位置検出器11において測定光束
hがどちらのホトセンサー11a,11bにて受
光されたかを示す位置信号が焦点位置合わせ機構
3へ送られるようになつている。ホトセンサー1
1aは対象物4と対物レンズ8との距離を小さく
する信号を焦点位置合わせ機構3へ伝え、ホトセ
ンサー11bはその距離を大きくする位置信号を
伝えるようになつている。
As this optical position detector 11, a semiconductor optical position detector (PSD) was adopted. This semiconductor optical position detector (PSD) can obtain a position signal that includes position information of incident light without scanning the image, and has higher resolution than solid-state imaging devices such as CCD and MOS. A high sampling grade can be obtained. The optical position detector 11 is electrically connected to the focus alignment mechanism 3, and the optical position detector 11 receives a position signal indicating which photosensor 11a or 11b receives the measurement luminous flux h. It is designed to be sent to the focus positioning mechanism 3. Photo sensor 1
1a transmits a signal for reducing the distance between the object 4 and the objective lens 8 to the focus positioning mechanism 3, and the photosensor 11b transmits a position signal for increasing the distance.

焦点位置合わせ機構3としては、サーボ回路に
よつてモータを駆動させる非常に動作スピードの
速い「サーボ機構」を採用した。そして、この焦
点位置合わせ機構3は対象物4に接続してあり、
光位置検出器11からの位置信号に応じて、対象
物4と対物レンズ8との距離を調整し、対象物4
の表面4aで測定光束dの焦点p1が合致するよ
うにされている。尚、この焦点位置合わせ機構3
は、対物レンズ8(或いは光学機構2全体)の方
を移動させることもできるし、対象物4と対物レ
ンズ8(或いは光学機構2全体)の両方を移動さ
せることもできる。
As the focus positioning mechanism 3, a ``servo mechanism'' with an extremely fast operating speed, in which a motor is driven by a servo circuit, is employed. This focus positioning mechanism 3 is connected to the object 4,
The distance between the object 4 and the objective lens 8 is adjusted according to the position signal from the optical position detector 11, and the distance between the object 4 and the objective lens 8 is adjusted.
The focal point p1 of the measurement light beam d is made to coincide with the surface 4a. In addition, this focus positioning mechanism 3
The objective lens 8 (or the entire optical mechanism 2) can be moved, or both the object 4 and the objective lens 8 (or the entire optical mechanism 2) can be moved.

焦点が合つている状態〔第1図参照〕 測定光束dの焦点p1が対象物4の表面4aに
合致している状態が、焦点位置合わせされている
状態であり、この状態において、対象物4から反
射された測定光束hは、ホトセンサー11a,1
1bの中立位置p3(即ち、バランスがとれてい
る位置)で受光され、焦点位置合わせ機構3を作
動させないようになつている。
A focused state [see Fig. 1] A state in which the focal point p1 of the measurement light beam d matches the surface 4a of the object 4 is a focused state, and in this state, the object 4 The measurement luminous flux h reflected from the photosensors 11a, 1
The light is received at a neutral position p3 (that is, a balanced position) of 1b, and the focus positioning mechanism 3 is not activated.

対象物が光学機構側に近づいている状態〔第2図
参照〕 対象物4が光学機構2側へ外れて、焦点がズレ
ている場合には、対物レンズ8で屈折された測定
光束dが、対象物4表面4aにおける光軸5より
下方の反射点14にて反射され、そのまま対物レ
ンズ8、結像レンズ9を経て、先の再結像点p2
よりも先の再結像点15を通過し、拡大レンズ1
0の外周部側を通過して下側のホトセンサー11
bにて受光される。すると、その位置信号が焦点
位置合わせ機構3へ送られ、対象物4を光学機構
2から遠ざけるように移動させ、測定光束hがホ
トセンサー11a,11bの中立位置p3に来た
時に焦点位置合わせ機構3の作動は停止する。従
つて、前記第1図の如く測定光束dの焦点p1対
象物4の表面4aへ合うこととなる。
A state in which the object is approaching the optical mechanism (see Figure 2). When the object 4 has moved toward the optical mechanism 2 and is out of focus, the measurement light beam d refracted by the objective lens 8 becomes It is reflected at a reflection point 14 below the optical axis 5 on the surface 4a of the object 4, passes through the objective lens 8 and the imaging lens 9, and then returns to the previous re-imaging point p2.
It passes through the re-imaging point 15 which is further ahead than the magnifying lens 1.
0 passing through the outer peripheral side of the lower photo sensor 11
The light is received at b. Then, the position signal is sent to the focus alignment mechanism 3, which moves the object 4 away from the optical mechanism 2, and when the measurement light beam h reaches the neutral position p3 of the photosensors 11a and 11b, the focus alignment mechanism 3 moves the object 4 away from the optical mechanism 2. 3 stops. Therefore, as shown in FIG. 1, the focal point p1 of the measurement light beam d is focused on the surface 4a of the object 4.

対象物が光学機構側から遠ざかつている状態〔第
3図参照〕 先とは逆に、対象物4が光学機構2から遠ざか
つて、表面4aが焦点p1からズレている場合に
は、対物レンズ8で屈折された測定光束dが、対
象物4の表面4aにおける光軸5より上方の反射
点16にて反射され、そのまま対物レンズ8、結
像レンズ9、拡大レンズ10、手前の再結像点1
7を経て、上側のホトセンサー11aに受光され
る。すると、その位置信号が焦点位置合わせ機構
3へ送られ、焦点位置合わせ機構3が対象物4を
光学機構2側へ近づけるように移動させ、前記1
図の如く測定光束dの焦点位置合わせを行えるよ
うになつている。
A state in which the object is moving away from the optical mechanism (see Figure 3).Contrary to the above, when the object 4 is moving away from the optical mechanism 2 and the surface 4a is deviated from the focal point p1, the objective lens 8 The measurement light beam d refracted at 1
7, and is received by the upper photosensor 11a. Then, the position signal is sent to the focus positioning mechanism 3, and the focus positioning mechanism 3 moves the object 4 closer to the optical mechanism 2 side.
As shown in the figure, the focal position of the measurement light beam d can be adjusted.

このように、対象物4が対物レンズ8の焦点p
1から外れていたとしても、それを自動的に是
正・調整し、測定光束dの焦点p1を対象物4の
表面4aにピタリと合わせることができる。更
に、対象物4が、仮に光軸5に対して傾斜状態で
あつたとしても、その対象物4の表面4aからの
乱反射光にて光位置検出器11及び焦点位置合わ
せ機構3を作動することが出来るので問題はな
い。尚、以上の基本構造において、固定ミラー7
として、ハーフミラーを採用したが、ダイクロツ
クミラー、レーザミラーその他のミラーであつて
も構わない。また、光位置検出器11として半導
体光位置検出器(PSD)を採用したが、その他
の光位置検出器、例えばフオトダイオード(PD)
などを採用しても同程度の効果を期待できる。そ
して、焦点位置合わせ機構3として、サーボ機構
を採用したが、サーボ機構と同程度の動作スピー
ドを有する機構であれば他のものでも同じ効果を
得ることができる。更に、光位置検出器11の直
前位置に偏向フイルターを配し、偏光He−Neレ
ーザ光線と同波長(6328Å)付近の入射光を遮断
し、耐ノイズ性を向上させることも可能である。
In this way, the object 4 is at the focal point p of the objective lens 8.
Even if it deviates from 1, it can be automatically corrected and adjusted, and the focal point p1 of the measurement light beam d can be perfectly aligned with the surface 4a of the object 4. Furthermore, even if the object 4 is tilted with respect to the optical axis 5, the optical position detector 11 and the focus positioning mechanism 3 can be operated by the diffusely reflected light from the surface 4a of the object 4. There is no problem because it can be done. In addition, in the above basic structure, the fixed mirror 7
Although a half mirror is used as the mirror, a dichroic mirror, laser mirror, or other mirror may also be used. In addition, although a semiconductor optical position detector (PSD) was adopted as the optical position detector 11, other optical position detectors, such as a photodiode (PD)
Similar effects can be expected even if other methods are adopted. Although a servo mechanism is used as the focus positioning mechanism 3, the same effect can be obtained with other mechanisms as long as they have the same operating speed as the servo mechanism. Furthermore, it is also possible to arrange a polarizing filter immediately in front of the optical position detector 11 to block incident light around the same wavelength (6328 Å) as the polarized He-Ne laser beam, thereby improving noise resistance.

上記の装置を使用した本発明の実施例を第4図
及び第5図に基づいて更に説明する。尚、先の基
本構造に説明と共通する部分については同一の符
号を付し、また光学機構2の対物レンズ8と対象
物4近辺だけを図示するものとし、その他の図示
は省略する。
An embodiment of the present invention using the above-mentioned apparatus will be further explained based on FIGS. 4 and 5. In addition, the same reference numerals are given to the parts common to the above-mentioned basic structure and the explanation, and only the objective lens 8 of the optical mechanism 2 and the vicinity of the object 4 are illustrated, and the illustration of the other parts is omitted.

透明体(対象物)4は、その表面4aを裏面4
bとでそれぞれ反射が行われる。つまり、ある照
射角度θでもつて照射された測定光束dは、その
まま透明体4内へ屈折して透過していく測定光束
iと、表面4aで反射される測定光束eとに一旦
分かれる。一方、透明体4内へ透過していつた測
定光束iは、更に裏面4b側へ抜けていく測定光
束jと、裏面4bで反射される測定光束kとに分
かれる。従つて、表面4aで反射された測定光束
eと、裏面4bで反射された測定光束kの両方
が、再度対物レンズ8にて屈折されて、光位置検
出器11にて感知される〔第4図参照〕。表面4
aからの測定光束eの方が強い場合には、表面4
aに焦点が合うが、裏面4bの状況によつては、
裏面4bからの測定光束kの方が強い場合があ
り、その際はその裏面4bから反射されたこの測
定光束kにて光位置検出器11及び焦点位置合わ
せ機構3が支配され、裏面4bに焦点が合つてし
まうおそれがある。
The transparent body (object) 4 has its front surface 4a as its back surface 4.
Reflection is performed at both b and b. In other words, the measurement light beam d irradiated at a certain irradiation angle θ is once divided into a measurement light beam i, which is refracted and transmitted into the transparent body 4, and a measurement light beam e, which is reflected by the surface 4a. On the other hand, the measurement light beam i that has passed through the transparent body 4 is further divided into a measurement light beam j that passes toward the back surface 4b and a measurement light beam k that is reflected by the back surface 4b. Therefore, both the measurement light flux e reflected on the front surface 4a and the measurement light flux k reflected on the back surface 4b are refracted by the objective lens 8 and sensed by the optical position detector 11. See figure]. surface 4
If the measuring luminous flux e from a is stronger, then the surface 4
A is in focus, but depending on the situation on the back side 4b,
The measurement light flux k from the back surface 4b may be stronger, and in that case, the optical position detector 11 and the focus alignment mechanism 3 are controlled by the measurement light flux k reflected from the back surface 4b, and the focus is focused on the back surface 4b. There is a risk that they will match.

そこで、そのような場合には、可動ミラー6を
反透明体側Aへ平行移動させることにより、固定
ミラー7にて反射された測定光束cを対物レンズ
8の外周部側で屈折せしめ、測定光束dを大きい
照射角度θ1でもつて透明体4へ照射すればよ
い。そうすると、表面4a及び裏面4bで反射す
る測定光束e,kも共に反射角度が大きくなり、
裏面4bから反射された測定光束kは、対物レン
ズ8に入射不能な方向へ反射されることとなる。
従つて、表面4aで反射された測定光束eだけが
対物レンズ8にて屈折され、この測定光束eによ
り焦点位置合わせ機構3を作動させることが可能
となる。尚、表面4aからの測定光束eは、透明
体4の表面4aからの反射光なので、その光量は
少ないが光位置検出器11にて電気的に増幅すれ
ば問題ない。
Therefore, in such a case, by moving the movable mirror 6 in parallel to the side A opposite to the transparent body, the measurement light beam c reflected by the fixed mirror 7 is refracted on the outer peripheral side of the objective lens 8, and the measurement light beam d is It is sufficient to irradiate the transparent body 4 with a large irradiation angle θ1. Then, the reflection angles of both the measurement light beams e and k reflected on the front surface 4a and the back surface 4b become large,
The measurement light beam k reflected from the back surface 4b is reflected in a direction in which it cannot enter the objective lens 8.
Therefore, only the measurement light beam e reflected by the surface 4a is refracted by the objective lens 8, and it becomes possible to operate the focus positioning mechanism 3 by this measurement light beam e. Incidentally, since the measurement light flux e from the surface 4a is reflected light from the surface 4a of the transparent body 4, the amount of light is small, but if it is electrically amplified by the optical position detector 11, there will be no problem.

つまりこの実施例は実際に焦点合わせしたい透
明体4の表面4a以外で反射する測定光束kを、
対物レンズ8に入射不能な方向へ反射させるべく
測定光束の照射角度θを調整するものであり、透
明体4の裏面4b側に不透明体などが接合又は離
間配置されている場合にも同様に適用できる。
In other words, in this embodiment, the measurement light flux k that is reflected off a surface other than the surface 4a of the transparent body 4 that is actually desired to be focused is
This is to adjust the irradiation angle θ of the measurement light beam so as to reflect it in a direction where it cannot enter the objective lens 8, and it is also applied when an opaque body or the like is attached or separated from the back surface 4b of the transparent body 4. can.

第2実施例 第6図及び第7図はこの発明の第2実施例を示
す図である。この実施例では、透明体4の内部に
不透明体18が存在する場合について説明する。
この場合は不透明体18で反射される測定光束l
の方が、表面4aで反射される測定光束eよりも
強いので、光位置検出器11及び焦点位置合わせ
機構3は必ず不透明体18の表面へ焦点位置合わ
せをしてしまう〔第6図参照〕。そうすると、実
際に焦点位置合わせを行いたい透明体4の表面4
aに焦点が合わなくなつてしまう。このような場
合にも、可動ミラー6を反対象物側Aへ平行移動
させ、測定光束dを大きい照射角度θ1とするこ
とにより、測定光束dの不透明体18での反射を
回避することができる〔第7図参照〕。従つて、
透明体4の表面4aで反射された測定光束eだけ
により焦点位置合わせ機構3を作動させ、透明体
4の表面4aに焦点を合わせることが可能とな
る。この実施例の適用例としては、例えば透明基
板内に電子回路(半導体等)を封入した場合など
に最適である。更に、不透明体18が透明体4の
内部に存在する場合だけでなく、前述の如く透明
体4の裏面4b側に不透明体18などが接合又は
離間配置されている場合も、不透明体18と測定
光束dとの干渉(照射)を回避すれば、本実施例
と同様に、透明体4の表面4aにだけ焦点を合わ
せることができる。
Second Embodiment FIGS. 6 and 7 are diagrams showing a second embodiment of the present invention. In this embodiment, a case where an opaque body 18 exists inside a transparent body 4 will be described.
In this case, the measurement light flux l reflected by the opaque body 18
is stronger than the measurement light beam e reflected by the surface 4a, so the optical position detector 11 and the focus positioning mechanism 3 always focus on the surface of the opaque body 18 (see FIG. 6). . Then, the surface 4 of the transparent body 4 where you want to actually focus
I can no longer focus on a. Even in such a case, by moving the movable mirror 6 in parallel to the side A away from the object and setting the measurement light beam d at a large irradiation angle θ1, reflection of the measurement light beam d on the opaque body 18 can be avoided. [See Figure 7]. Therefore,
It becomes possible to operate the focus positioning mechanism 3 only by the measurement light beam e reflected on the surface 4a of the transparent body 4, and to focus on the surface 4a of the transparent body 4. As an example of application of this embodiment, it is most suitable, for example, when an electronic circuit (semiconductor, etc.) is enclosed within a transparent substrate. Furthermore, not only when the opaque body 18 exists inside the transparent body 4, but also when the opaque body 18 or the like is bonded to or placed apart from the back surface 4b of the transparent body 4 as described above, the opaque body 18 can be measured. If interference (irradiation) with the light beam d is avoided, it is possible to focus only on the surface 4a of the transparent body 4, as in the present embodiment.

〈効果〉 この発明に係る非接触自動焦点位置合わせ方法
は、以上説明してきた如き内容のものであつて、
可動ミラーを反透明体側へ平行移動させることに
より、測定光束の照射角度を大きくするので、透
明体の表面以外で反射された測定光束を、対物レ
ンズに入射不能な方向へ反射し、透明体の表面だ
けに焦点を合わせることができるという効果があ
る。
<Effects> The non-contact automatic focus positioning method according to the present invention has the contents as described above, and has the following features:
By moving the movable mirror in parallel toward the opposite side of the transparent object, the irradiation angle of the measurement light beam is increased, so that the measurement light beam reflected off the surface of the transparent object is reflected in a direction that cannot be incident on the objective lens, and This has the effect of allowing you to focus only on the surface.

測定光束として偏光He−Neレーザ光線を採用
したので、他のレーザ光線に比べて光束が細いう
えに集光スポツトが非常に小さく広がらないの
で、その分、光位置検出器での位置検出を高精度
(高分解能)で行えるものである。この偏光He−
Neレーザ光線の集光スポツトの径は対物レンズ
の倍率にもよるが、大体1μ〜100μと非常に小さ
いものである(つまり、焦点位置合わせ精度が高
い)。
Since a polarized He-Ne laser beam is used as the measurement light beam, the light beam is narrower than other laser beams, and the focal spot is very small and does not spread out, so the position detection with the optical position detector is improved accordingly. This can be done with high precision (high resolution). This polarized light He−
Although the diameter of the condensing spot of the Ne laser beam depends on the magnification of the objective lens, it is very small, approximately 1 μ to 100 μ (that is, the focus positioning accuracy is high).

また、この発明の実施例によれば、 測定光束の変位を拡大レンズで拡大するので、
小さな変位も見逃さずに正確に拡大し、その後光
位置検出器にて位置検出するので、高精度の位置
検出を実現することができる。従つて、対物レン
ズと対象物との間隔が大きく焦点精度が低下しや
すい状況であつても、高精度の焦点位置合わせを
実現することができる(つまり、焦点位置合わせ
精度が高い)。
Further, according to the embodiment of the present invention, since the displacement of the measurement light beam is magnified by the magnifying lens,
Since even small displacements are accurately magnified without being overlooked, and the position is then detected by an optical position detector, highly accurate position detection can be achieved. Therefore, even in a situation where the distance between the objective lens and the object is large and the focus accuracy tends to decrease, highly accurate focus positioning can be achieved (that is, the focus positioning accuracy is high).

光位置検出器としての半導体光位置検出器
(PSD)は、検出した測定光束のスポツトの重心
位置を出力するだけなので、輝度分布が変化して
も影響を受けず、対象物の表面における輝度分布
(コントラスト)によつて焦点位置合わせ精度が
影響を受けない(つまり、耐ノイズ性、測定の確
実性が高い)。
The semiconductor optical position detector (PSD) as an optical position detector only outputs the position of the center of gravity of the spot of the detected measurement light beam, so it is not affected by changes in the brightness distribution, and the brightness distribution on the surface of the object Focus positioning accuracy is not affected by (contrast) (that is, noise resistance and measurement reliability are high).

光位置検出器として半導体光位置検出器
(PSD)を採用し、且つ焦点位置合わせ機構とし
てサーボ機構を採用したので、平均10mmsecの素
早い動作で、光学機構と対象物との間の距離を調
整することができる(つまり、焦点位置合わせ速
度が速い)。
A semiconductor optical position detector (PSD) is used as the optical position detector, and a servo mechanism is used as the focus positioning mechanism, so the distance between the optical mechanism and the object can be adjusted with a quick movement of 10 mmsec on average. (that is, the focus positioning speed is fast).

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

第1図は本発明の第1実施例を実施する装置の
基本構造を示す概略説明図、第2図は対象物が光
学機構側へズレている状態を示す第1図相当の概
略説明図、第3図は対象物が反光学機構側へズレ
ている状態を示す第1図相当の概略説明図、第4
図及び第5図は、各々この発明の第1実施例を示
す拡大説明図、そして第6図及び第7図は、各々
この発明の第2実施例を示す拡大説明図である。 1…レーザ機構、2…光学機構、3…焦点位置
合わせ機構、4…対象物、5…光軸、6…可動ミ
ラー、7…固定ミラー、8…対物レンズ、9…結
像レンズ、11…光位置検出器、p1…焦点、
θ,θ1…照射角度、a〜l…測定光束。
FIG. 1 is a schematic explanatory diagram showing the basic structure of an apparatus implementing the first embodiment of the present invention, FIG. 2 is a schematic explanatory diagram corresponding to FIG. 1 showing a state in which the object is shifted toward the optical mechanism, Figure 3 is a schematic explanatory diagram equivalent to Figure 1 showing a state in which the object is shifted toward the opposite side of the optical mechanism;
5 and 5 are enlarged explanatory views showing a first embodiment of the present invention, and FIGS. 6 and 7 are enlarged explanatory views showing a second embodiment of the invention, respectively. DESCRIPTION OF SYMBOLS 1... Laser mechanism, 2... Optical mechanism, 3... Focus alignment mechanism, 4... Target, 5... Optical axis, 6... Movable mirror, 7... Fixed mirror, 8... Objective lens, 9... Imaging lens, 11... Optical position detector, p1...focal point,
θ, θ1...Irradiation angle, a-l...Measurement light flux.

Claims (1)

【特許請求の範囲】 1 光学機構の光軸と平行に発せられた測定光束
としての偏光He−Neレーザ光線を、光軸に対し
て45度の傾斜角度を保ちつつ平行移動自在な可動
ミラーにて反射し、 該可動ミラーにて反射された測定光束を、光軸
と45度の傾斜角度で配された固定ミラーにて反射
し、 該固定ミラーにて反射された測定光束を、対物
レンズで屈折せしめてから透明体へ向けて照射
し、 該透明体の表面で反射された測定光束を、再度
対物レンズで屈折せしめてから光位置検出器にて
受光し、 該光位置検出器からの位置信号に対応する焦点
位置合わせ機構にて、少なくとも透明体と対物レ
ンズとの間の距離を調整することにより、測定光
束を透明体の表面へ自動的に焦点位置合わせする
ものであつて、 前記可動ミラーを反透明体側へ平行移動させる
ことにより、固定ミラーにて反射された測定光束
を対物レンズの外周部側で屈折せしめ、測定光束
を大きい照射角度でもつて透明体へ照射し、そし
て透明体の表面以外で反射する測定光束を対物レ
ンズに入射不能な方向に反射させることを特徴と
する非接触自動焦点位置合わせ方法。
[Claims] 1. A polarized He-Ne laser beam as a measurement light beam emitted parallel to the optical axis of an optical mechanism is applied to a movable mirror that can be moved in parallel while maintaining an inclination angle of 45 degrees with respect to the optical axis. The measuring beam reflected by the movable mirror is reflected by a fixed mirror arranged at an angle of 45 degrees with respect to the optical axis, and the measuring beam reflected by the fixed mirror is reflected by an objective lens. After being refracted, it is irradiated towards a transparent body, and the measurement light beam reflected on the surface of the transparent body is refracted by an objective lens and then received by an optical position detector, and the position from the optical position detector is determined. The focus positioning mechanism corresponding to the signal automatically focuses the measurement light beam onto the surface of the transparent body by adjusting at least the distance between the transparent body and the objective lens, the movable By moving the mirror in parallel toward the opposite side of the transparent object, the measurement light beam reflected by the fixed mirror is refracted at the outer circumferential side of the objective lens, and the measurement light beam is irradiated onto the transparent object at a large irradiation angle. A non-contact automatic focus positioning method characterized by reflecting a measurement light beam reflected off a surface other than the surface in a direction where it cannot enter an objective lens.
JP30803186A 1986-12-25 1986-12-25 Noncontact automatic focus positioning method Granted JPS63163315A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30803186A JPS63163315A (en) 1986-12-25 1986-12-25 Noncontact automatic focus positioning method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30803186A JPS63163315A (en) 1986-12-25 1986-12-25 Noncontact automatic focus positioning method

Publications (2)

Publication Number Publication Date
JPS63163315A JPS63163315A (en) 1988-07-06
JPH0563773B2 true JPH0563773B2 (en) 1993-09-13

Family

ID=17976053

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30803186A Granted JPS63163315A (en) 1986-12-25 1986-12-25 Noncontact automatic focus positioning method

Country Status (1)

Country Link
JP (1) JPS63163315A (en)

Also Published As

Publication number Publication date
JPS63163315A (en) 1988-07-06

Similar Documents

Publication Publication Date Title
JP4255682B2 (en) Reflector automatic tracking device
JP2913984B2 (en) Tilt angle measuring device
JPH0563771B2 (en)
JPH0743251B2 (en) Optical displacement meter
EP0627610B1 (en) Two-stage detection noncontact positioning apparatus
JP2002039724A (en) Internal hole surface inspecting device
JPH11173821A (en) Optical inspecting device
JPH0563773B2 (en)
JPH0563772B2 (en)
JP2003161610A (en) Optical measurement device
JPH08261734A (en) Shape measuring device
JPH06249648A (en) Displacement gauge
JPS63199311A (en) Method and apparatus for bidirectional and contactless automatic focus positioning
JP2808713B2 (en) Optical micro displacement measuring device
JPH0617934B2 (en) Non-contact automatic alignment device
JPS62218802A (en) Optical type distance and inclination measuring apparatus
JP2989995B2 (en) Positioning device
JP2000258339A (en) Birefringence measurement device
JPH0558483B2 (en)
JPH06137827A (en) Optical step measuring device
JPH02276908A (en) Three-dimensional position recognizing device
JPS6112203B2 (en)
JPS6275309A (en) Displacement convertor
JPS6285813A (en) Distance measuring instrument
JPS60228908A (en) Inspection of surface defect

Legal Events

Date Code Title Description
R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

LAPS Cancellation because of no payment of annual fees