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JPH02134508A - Tilt detection head - Google Patents

Tilt detection head

Info

Publication number
JPH02134508A
JPH02134508A JP63287987A JP28798788A JPH02134508A JP H02134508 A JPH02134508 A JP H02134508A JP 63287987 A JP63287987 A JP 63287987A JP 28798788 A JP28798788 A JP 28798788A JP H02134508 A JPH02134508 A JP H02134508A
Authority
JP
Japan
Prior art keywords
convex lens
position detection
detection element
optical position
light
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.)
Pending
Application number
JP63287987A
Other languages
Japanese (ja)
Inventor
Masahiro Nakashiro
正裕 中城
Shinji Kaino
甲斐野 真次
Noriyuki Inagaki
典之 稲垣
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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
Priority to KR1019860007275A priority Critical patent/KR920001908B1/en
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63287987A priority patent/JPH02134508A/en
Priority to KR1019890016479A priority patent/KR920010908B1/en
Publication of JPH02134508A publication Critical patent/JPH02134508A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/02Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/16Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光ディスク、半導体ウェハ、液晶TVガラス
基板、CCDCD撮像等子平板の傾きを検査、あるいは
検査に基づいて調整を行うための傾き検出ヘッドに関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a tilt detection head for inspecting the tilt of an optical disk, semiconductor wafer, liquid crystal TV glass substrate, CCDCD imaging plate, or adjusting the tilt based on the inspection. It is something.

従来の技術 平板の傾きを非接触で検出する傾き検出ヘッドとして、
凸レンズと光位置検出素子を用いたものがある。
Conventional technology As a tilt detection head that detects the tilt of a flat plate without contact,
Some use a convex lens and an optical position detection element.

第3図において、61は半導体レーザ光源、62はコリ
メータレンズ、63はビームスプリッタ−164は被測
定物、66は凸レンズ、56は光位置検出素子で、光位
置検出素子66は凸レンズ66のほぼ焦点位置に設置さ
れている。このような構成で、コリメータレンズ62か
ら出射され、ビームスプリッタ−63を透過したほぼ平
行の光は、被測定物64に照射され、被測定物64がθ
傾いている場合は、2θ傾いた方向に反射される。反射
光は、ビームスプリッタ−63で反射し、凸レンズ66
に入射し、光位置検出素子68上で、光軸からf as
in(2θ)ずれた位置に集光する。ただしfは凸レン
ズ65の焦点距離である。また、被測定物64が紙面に
対して直角方向に傾いた場合も同等に、光位置検出素子
66上で、紙面に対して直角方向に光軸からずれた位置
に集光する。したがって、任意の方向の傾きが光位置検
出素子66上の光スポツト位置で検出できることがわか
る。
In FIG. 3, 61 is a semiconductor laser light source, 62 is a collimator lens, 63 is a beam splitter, 164 is an object to be measured, 66 is a convex lens, 56 is an optical position detection element, and the optical position detection element 66 is approximately the focal point of the convex lens 66. installed in position. With this configuration, the nearly parallel light emitted from the collimator lens 62 and transmitted through the beam splitter 63 is irradiated onto the object to be measured 64, and the object to be measured 64 is
If it is tilted, it will be reflected in a 2θ tilted direction. The reflected light is reflected by the beam splitter 63 and passed through the convex lens 66.
is incident on the optical position detection element 68 from the optical axis f as
The light is focused at a position shifted by in (2θ). However, f is the focal length of the convex lens 65. Furthermore, even when the object to be measured 64 is tilted in a direction perpendicular to the plane of the paper, the light is similarly focused on the optical position detection element 66 at a position deviated from the optical axis in the direction perpendicular to the plane of the paper. Therefore, it can be seen that the tilt in any direction can be detected by the optical spot position on the optical position detection element 66.

発明が解決しようとする課題 しかしながら、上記のよう々構成では、検出分解能を上
げかつ検出範囲を拡げようとすると、凸レンズの焦点距
離を長くする必要があり、光学系が大がかりなものとな
P・、実現が困難になるという問題点を有していた。
Problems to be Solved by the Invention However, with the above configuration, in order to increase the detection resolution and expand the detection range, it is necessary to increase the focal length of the convex lens, which requires a large-scale optical system. , which has the problem of being difficult to implement.

たとえば、10  d@gの分解能で1 digの検出
範囲をもつ光学系は、光位置検出素子の寸法をロ6喘と
すれば fφsin (2) = 5 より、f=143msとなり、凸レンズと光位置検出素
子の間隔が140籠以上となるため、非常に大きな光学
系となってしまう。
For example, in an optical system with a resolution of 10 d@g and a detection range of 1 dig, if the dimensions of the optical position detection element are 6 mm, then fφsin (2) = 5, so f = 143 ms, and the distance between the convex lens and the optical position is Since the distance between the detection elements is 140 cages or more, the optical system becomes very large.

本発明は、上記問題点に鑑み、高分解能で広い検出範囲
を有し、しかもコンパクトな傾き検出ヘッドを提供する
ものである。
In view of the above problems, the present invention provides a tilt detection head that has high resolution, a wide detection range, and is compact.

ipを解決するための手段 上記問題点を解消するために、本発明の傾き検出ヘッド
は、出射角の異なる少なくとも2本のほぼ平行光を出射
する光源と、ビームスプリッタ−と、凸レンズと、光位
置検出素子と、上記凸レンズと光位置検出素子との間に
配設された少なくとも3枚のミラーとを備え、そのミラ
ーのうちの1枚が光を2度反射するように構成したもの
である。
In order to solve the above problems, the tilt detection head of the present invention includes a light source that emits at least two substantially parallel beams with different emission angles, a beam splitter, a convex lens, and a light source that emits at least two substantially parallel beams with different emission angles. It comprises a position detection element and at least three mirrors disposed between the convex lens and the optical position detection element, and one of the mirrors is configured to reflect light twice. .

作  用 上記の構成により、まず1本の平行光のみ発光し、被測
定物に照射する。反射光は、ビームスプリッタ−で反射
し、凸レンズで収束され、光位置検出素子上に集光スポ
ットを形成する。この集光スポットが、光位置検出素子
をはずれた場合は、光源を消光し、もう1本の平行光を
発光する。こJしにより、集光スポットが、光位置検出
素子に入射すハば検出可能となる。このように、すべて
の光源を順次発光してゆくことにより、検出範囲が広が
り、かつ3枚のミラーを用いしかもその内の1枚に光を
2度反射させることにより焦点距離の長い凸レンズに対
しても検出分解能を低下させないでコンパクト化でキル
Operation With the above configuration, only one parallel light is first emitted and irradiated onto the object to be measured. The reflected light is reflected by a beam splitter, converged by a convex lens, and forms a focused spot on the optical position detection element. When this focused spot misses the optical position detection element, the light source is extinguished and another parallel beam is emitted. By doing so, it becomes possible to detect when the focused spot is incident on the optical position detection element. In this way, by sequentially emitting light from all the light sources, the detection range is expanded, and by using three mirrors and reflecting the light twice on one of them, it is possible to use a convex lens with a long focal length. It can be downsized without reducing detection resolution.

実施例 以下、本発明の実施例を第1図、第2図にもとづいて説
明する。
EXAMPLE Hereinafter, an example of the present invention will be explained based on FIGS. 1 and 2.

第1図において、1は第1の平行光源、2は第2の平行
光源、3は第1のビームスブリ、ター4は第2のビーム
スプリッタ−16は被測定物、8は凸レンズ、7,8.
9は、それぞれ第1.第2、第3のミラー、1oは光位
置検出素子である。
In FIG. 1, 1 is a first parallel light source, 2 is a second parallel light source, 3 is a first beam splitter, 4 is a second beam splitter, 16 is an object to be measured, 8 is a convex lens, 7, 8 ..
9 is the first. The second and third mirrors 1o are optical position detection elements.

このような構成で、第1.第2の平行光源1,2をたと
えば、半導体レーザとコリメータレンズを使用すれば、
被測定物6に照射されるビームは通常2 m X 6 
fi程度の楕円形状であり、この領域内の平均的な傾き
をこのヘッドでは測定する。
With such a configuration, the first. For example, if a semiconductor laser and a collimator lens are used as the second parallel light sources 1 and 2,
The beam irradiated onto the object to be measured 6 is usually 2 m x 6
It has an elliptical shape of approximately fi, and this head measures the average inclination within this area.

まず、第1の平行光源1を発光し、被測定物6が、あら
かじめ設定された基準面よりθ傾いている場合、反射光
は2θの傾きをもち、第2のビームスプリッタ−4で反
射して、凸レンズ6に入射する。入射光は凸レンズ6で
収束され、第1.第2、第3のミラー7.8.9を反射
して光位置検出素子10に集光スポットを形成する。こ
の実施例においては、3枚のミラー?、8.9を用いて
光路を折り曲げ、しかもそのうちの1枚のミラー7は光
を2度反射するので、空間を有効に利用できる。
First, when the first parallel light source 1 emits light and the object to be measured 6 is inclined by θ from a preset reference plane, the reflected light has an inclination of 2θ and is reflected by the second beam splitter 4. and enters the convex lens 6. The incident light is converged by the convex lens 6, and the first . The light is reflected by the second and third mirrors 7.8.9 to form a focused spot on the optical position detection element 10. In this example, three mirrors? , 8.9 are used to bend the optical path, and one of the mirrors 7 reflects the light twice, so space can be used effectively.

また、集光スポットが光位置検出素子1oをはずれる場
合は、第1の平行光源1を消光し、代わって、第2の平
行光源2を発光することができるので検出範囲を拡げる
ことができる。
Further, when the focused spot is off the optical position detection element 1o, the first parallel light source 1 can be extinguished and the second parallel light source 2 can be emitted instead, so that the detection range can be expanded.

このよりなI’ffi成で広がる検出範囲について、第
2図で説明する。2つの平行光101,102の出射角
の差をαとし、その出射角の2等分線方向に反射光が返
る場合の集光スポットが光位置検出素子1oの原点に位
置するように光学調整がなされているとする。このとき
、2等分線と垂直な平面を基早とすれば、第1の平行光
101はα/2゜第2の平行光102は一α/2被測定
物6がそれぞれ傾いた状態で集光スポットが原点に位置
することになる。検出範囲は、f=143amの凸レン
ズ6を使用すれば、それぞれi degとなる。2つの
平行光101,102による検出範囲に重なりをなくす
ためには、α=1dθqとすれば良く、このときの検出
範囲は、合計2 dogと2倍に広がる。
The detection range expanded by this wider I'ffi configuration will be explained with reference to FIG. Let α be the difference between the emission angles of the two parallel beams 101 and 102, and perform optical adjustment so that the focused spot when the reflected light returns in the direction of the bisector of the emission angle is located at the origin of the optical position detection element 1o. Suppose that this is done. At this time, if the plane perpendicular to the bisector is taken as the basic plane, the first parallel light 101 is α/2° and the second parallel light 102 is α/2 with the object 6 tilted. The focused spot will be located at the origin. The detection range becomes i deg if a convex lens 6 with f=143 am is used. In order to eliminate overlap between the detection ranges of the two parallel beams 101 and 102, it is sufficient to set α=1dθq, and the detection range at this time is doubled to a total of 2 dogs.

以上の説明は、−軸方向のみの検出範囲を拡大する方法
についてであるが、さらにもう−軸の検出範囲を拡大す
るためには、もう1水平行光源を追加すれば良い。
The above explanation is about a method of expanding the detection range only in the -axis direction, but in order to further expand the detection range in the -axis direction, it is sufficient to add one more horizontal light source.

また、2本の平行光を発生させるために、ビームスプリ
ッタ−で合成する方法を用いたが、2つの発光点をもつ
半導体レーザを使用すれば、ビームスプリッターなしで
2本の平行光を発生できることは言うまでもない。
Also, in order to generate two parallel beams, we used a method of combining them with a beam splitter, but if we use a semiconductor laser with two light emitting points, it is possible to generate two parallel beams without a beam splitter. Needless to say.

発明の効果 以」二のように、本発明は、少なくとも2木の平行光を
出射することができ、少なくとも3枚のミラーを有して
そのミラーのうち1枚は光を2度反射するため、コンパ
クトでかつ高分解能、広い検出範囲をもつ傾き検出ヘッ
ドを提供できる。
Effects of the Invention As described in 2., the present invention is capable of emitting at least two parallel lights, and has at least three mirrors, one of which reflects the light twice. , it is possible to provide a tilt detection head that is compact, has high resolution, and has a wide detection range.

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

2r’J ’図は本発明の実施例における傾き検出ヘッ
ドの(7?I成図、第2図はその説明図、第3図は従来
の傾き検出ヘッドの構成図である。 1・・・・・・第1の平行光源、2・・・・・・第2の
平行光源、4・・・・・・第2のビームスプリッタ−1
6・・・・・凸レンズ、7,8.9・・・・・・ミラー
 1o・・・・・・光位置検出素子。
2r'J' is a (7?I) diagram of the tilt detection head in the embodiment of the present invention, FIG. 2 is an explanatory diagram thereof, and FIG. 3 is a configuration diagram of a conventional tilt detection head. 1... ...First parallel light source, 2...Second parallel light source, 4...Second beam splitter-1
6...Convex lens, 7,8.9...Mirror 1o...Optical position detection element.

Claims (1)

【特許請求の範囲】[Claims] 出射角の異なる少なくとも2本のほぼ平行光を出射する
光源と、ビームスプリッターと、凸レンズと、光位置検
出素子と、上記凸レンズと光位置検出素子の間に少なく
とも3枚のミラーとを備え、そのミラーのうち1枚が光
を2度反射するようにした傾き検出ヘッド。
A light source that emits at least two substantially parallel beams with different emission angles, a beam splitter, a convex lens, an optical position detection element, and at least three mirrors between the convex lens and the optical position detection element, A tilt detection head in which one of the mirrors reflects light twice.
JP63287987A 1985-09-06 1988-11-15 Tilt detection head Pending JPH02134508A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
KR1019860007275A KR920001908B1 (en) 1985-09-06 1986-08-30 Slant detecting head pilot hydraulic system for operating directional control valve
JP63287987A JPH02134508A (en) 1988-11-15 1988-11-15 Tilt detection head
KR1019890016479A KR920010908B1 (en) 1988-11-15 1989-11-14 Mirror detection head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63287987A JPH02134508A (en) 1988-11-15 1988-11-15 Tilt detection head

Publications (1)

Publication Number Publication Date
JPH02134508A true JPH02134508A (en) 1990-05-23

Family

ID=17724330

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63287987A Pending JPH02134508A (en) 1985-09-06 1988-11-15 Tilt detection head

Country Status (2)

Country Link
JP (1) JPH02134508A (en)
KR (1) KR920010908B1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011196883A (en) * 2010-03-19 2011-10-06 Toshiba Corp Distance measuring apparatus

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20000058691A (en) * 2000-06-24 2000-10-05 박의석 A manufacturing method of instant kochujang
KR20040046290A (en) * 2002-11-26 2004-06-05 박영배 Manufacturing method of powdered kochujang material

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011196883A (en) * 2010-03-19 2011-10-06 Toshiba Corp Distance measuring apparatus

Also Published As

Publication number Publication date
KR900008243A (en) 1990-06-02
KR920010908B1 (en) 1992-12-21

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