JPS61196111A - Flatness measuring apparatus - Google Patents

Flatness measuring apparatus

Info

Publication number
JPS61196111A
JPS61196111A JP3808885A JP3808885A JPS61196111A JP S61196111 A JPS61196111 A JP S61196111A JP 3808885 A JP3808885 A JP 3808885A JP 3808885 A JP3808885 A JP 3808885A JP S61196111 A JPS61196111 A JP S61196111A
Authority
JP
Japan
Prior art keywords
light
lens
measured
beam splitter
incident
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
JP3808885A
Other languages
Japanese (ja)
Inventor
Tazuko Ishizuka
石塚 多津子
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Pentax Corp
Original Assignee
Asahi Kogaku Kogyo Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Asahi Kogaku Kogyo Co Ltd filed Critical Asahi Kogaku Kogyo Co Ltd
Priority to JP3808885A priority Critical patent/JPS61196111A/en
Publication of JPS61196111A publication Critical patent/JPS61196111A/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
    • G01B11/30Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces
    • G01B11/306Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces for measuring evenness

Landscapes

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

Abstract

PURPOSE:To enable the fast measurement of a 2-D shape of the entire plane while in noway damaging the surface to be measured, by providing a beam splitter, an objective lens, collimator lens, a fine lens and the like. CONSTITUTION:This apparatus is provided with a beam splitter 3, an objective lens 4, a collimator lens 6, a fine lens 7 and the like. Light from a light source 1 is expanded with a beam expander 2 and bent with the splitter 3 to be incident into the lens 4. The light from the lens 4 passes through a 1/4lambda plate 5 while being incident into the lens 6, where it is turned to a thick parallel flux to be incident into a fine lens array. In this array, a plurality of the same lenses 7 are stuck on a coverglass 8. Light introduced to the surface 9 to be measured is reflected thereon to be incident into the splitter 3 passing through the lenses 7 and 6, the plate 5 and the lens 4 again. Moreover, after the removal of noises with a spatial filter 10, the reflected light is introduced to a lens system 11, an observation surface 12 and a photoconductive element 13 to detect the intensity of light.

Description

【発明の詳細な説明】 a、技術分野 本発明は、一般的な平面特にカメラボディー内のフィル
ムの圧板平面の形状等を、光学的に且つ非接触で高精度
に測定する平面度測定器に関するものである。
Detailed Description of the Invention: a. Technical Field The present invention relates to a flatness measuring device that optically and non-contactly measures a general plane, particularly the shape of a pressure plate plane of a film inside a camera body, with high precision. It is something.

b、従来技術およびその問題点 従来、カメラボディー内のフィルムの圧板の平面形状測
定には、主に触針式の手段が用いられている。しかし、
この手段では1.針が被測定面に直接、接触するので、
被測定面に損傷を与える危険性がある。また、触針式測
定の場合、観測点が数ケ所と限られ、平面全体の2次元
的測定は困難であり、測定にも可成りの時間を要すると
いった問題がある。
b. Prior art and its problems Conventionally, stylus-type means have been mainly used to measure the planar shape of a film pressure plate in a camera body. but,
With this method, 1. Since the needle comes into direct contact with the surface to be measured,
There is a risk of damaging the surface to be measured. Furthermore, in the case of stylus measurement, there are problems in that the number of observation points is limited to a few, making it difficult to two-dimensionally measure the entire plane, and also requiring a considerable amount of time.

C1目 的 本発明は、上記の従来技術の問題点を解消すべくなされ
たもので、圧板などの平面形状を光学的に且つ非接触で
測定することによって、被測定面を傷つけることなく、
また平面全体の2次元的形状を高速に測定することを可
能とした平面度測定器を提供しようとするものである。
C1 Purpose The present invention was made to solve the problems of the above-mentioned prior art, and by optically and non-contact measuring the planar shape of a pressure plate, etc., it is possible to measure without damaging the surface to be measured.
Another object of the present invention is to provide a flatness measuring device that can measure the two-dimensional shape of an entire plane at high speed.

d、実施例の構成 第1図は本発明の一実施例を示す説明図であり、光路に
沿って構成を説明する。光源1は小さな点光源でHe−
Neレーザーである。この光源1かもの光は、ビームエ
キスパンダー2で広げられ、偏光ビームスプリッタ−3
で曲げられ、対物レンズ4に入射する。対物レンズから
の光は、1/4人板5を透過すると共にコリメーターレ
ンズ6に入射し、このコリメーターレンズ6で太い平行
光束となり、その平行光束は微小レンズ・アレイに入射
する。この微小レンズ・アレイは、同一の微小レンズ7
が多数、光軸に垂直なカバーガラス8上に並べて貼り付
けたら構成となっている。前記微小レンズ・アレイの焦
点位置附近には被測定面9が置かれ、該被測定面9上に
微小レンズ7の数だけ同形状、同じ大きさのスポット像
が表れる。
d. Configuration of Example FIG. 1 is an explanatory diagram showing an example of the present invention, and the configuration will be explained along the optical path. Light source 1 is a small point light source He-
It is a Ne laser. The light from this light source 1 is expanded by a beam expander 2, and is then expanded by a polarizing beam splitter 3.
The beam is bent by the angle , and enters the objective lens 4 . The light from the objective lens passes through the quarter plate 5 and enters the collimator lens 6, where it becomes a thick parallel beam of light, and the parallel light beam enters the microlens array. This microlens array consists of identical microlenses 7
The structure is obtained by affixing a large number of lenses side by side on a cover glass 8 perpendicular to the optical axis. A surface to be measured 9 is placed near the focal point of the microlens array, and spot images having the same shape and size as the number of microlenses 7 appear on the surface to be measured 9.

この被測定面9は、図面に矢印で示したように光軸方向
への移動が可能であり、その移動量が検出(m定)でき
るように移動量検出器(図示せず)に接続されている。
This surface to be measured 9 can be moved in the direction of the optical axis as shown by the arrow in the drawing, and is connected to a movement amount detector (not shown) so that the amount of movement can be detected (determined in m). ing.

前記被測定面9に導かれた光、即ち各スポット像はそこ
で反射され、その反射光は再び微小レンズ7、コリメー
ターレンズ6.1/4人板5.対物レンズ4を通り偏光
ビームスプリッタ−3に入射する。ここで、対物レンズ
4とコリメーターレンズ6との間に設けられた1/4入
板5は、被測定面9への入射光と被測定面9からの反射
光とを分離するためのものである。偏光ビームスプリッ
タ−3に入射した反射光(スポット像)は、偏光ビーム
スプリッタ−3を透過し、対物レンズ4の集光位置に設
けられた空間フィルタ(spatial filter
)10によりノイズを除去された後、レンズ系11を介
して微小レンズ・アレイ(微小レンズ)の瞳に対して被
測定面9と共役な位置に設けられた観測面12に導かれ
る。この観測面12上には各微小レンズ7に対応する位
置に微小レンズ7と同数の光電素子13が配置されてお
り、この光電素子13により微小レンズ7の各光強度が
検出され光電変換される。この光強度と前記移動量検出
器によって検出された被測定面9の移動量とは演算素子
(図示せず)により結びつけられている。
The light guided to the surface to be measured 9, that is, each spot image, is reflected there, and the reflected light is again passed through the microlens 7, collimator lens 6, 1/4 plate 5. The light passes through the objective lens 4 and enters the polarizing beam splitter 3. Here, the 1/4 input plate 5 provided between the objective lens 4 and the collimator lens 6 is for separating the light incident on the surface to be measured 9 and the light reflected from the surface to be measured 9. It is. The reflected light (spot image) incident on the polarizing beam splitter 3 passes through the polarizing beam splitter 3 and passes through a spatial filter provided at the condensing position of the objective lens 4.
) 10, the light is guided through a lens system 11 to an observation surface 12 provided at a position conjugate with the surface to be measured 9 with respect to the pupil of a microlens array (microlens). On this observation surface 12, the same number of photoelectric elements 13 as the microlenses 7 are arranged at positions corresponding to each microlens 7, and the light intensity of each microlens 7 is detected by the photoelectric elements 13 and photoelectrically converted. . This light intensity and the amount of movement of the surface to be measured 9 detected by the movement amount detector are linked by an arithmetic element (not shown).

尚、上記実施例では光源にHe  Noレーザーを用い
て説明したが、光源が普通のランプの場合には、1/4
人板5は不要となり、また偏光ビームスプリッタ−3は
偏光特性を有しないビームスプリッタ−ツタ−で構わな
いことは勿論である。
In the above embodiment, a He No laser is used as the light source, but if the light source is an ordinary lamp, the
The plate 5 is no longer necessary, and the polarizing beam splitter 3 may of course be a beam splitter without polarizing characteristics.

e、実施例の作用 微小レンズ・アレイに入射した平行光は、被測定面9上
に集光し、微小レンズ7の数だけ同形状。
e. Effect of Example Parallel light incident on the microlens array is condensed onto the surface to be measured 9, and has the same shape as the number of microlenses 7.

同じ大きさのスポット像が表われる。被測定面9に凹凸
がある場合、被測定面9上のスポット像の大きさ形が不
均一になる。また被測定面9が丁度。
Spot images of the same size appear. If the surface to be measured 9 has irregularities, the size and shape of the spot image on the surface to be measured 9 will be non-uniform. Also, the surface to be measured 9 is exactly.

微小レンズ7の焦点位置にあるとき、スポット像の形状
が最も小さくなり、被測定面9が前後に少しズしたとき
はスポット像が大きくなる。
When the spot image is at the focal position of the microlens 7, the shape of the spot image becomes the smallest, and when the surface to be measured 9 shifts slightly back and forth, the spot image becomes larger.

一方、被測定面9と共役な面(ai1!m面)には、各
々の微小レンズ7に対応する位置に光電素子が配置され
ているので、被測定面9からの反射光、即ちスポット像
は光強度として検出される。
On the other hand, on the plane (ai1!m plane) that is conjugate with the surface to be measured 9, photoelectric elements are arranged at positions corresponding to the respective microlenses 7, so that the reflected light from the surface to be measured 9, that is, the spot image is detected as light intensity.

従って、被測定面9を光軸方向に前後に移動させ、被測
定面9上の各点に像を結ぶときの被測定面9の移動量に
よって生ずる光強度を検出し、光電変換し演算素子で処
理することにより、被測定面9の凹凸を求めることがで
きる。
Therefore, when the surface to be measured 9 is moved back and forth in the optical axis direction and an image is focused on each point on the surface to be measured 9, the light intensity generated by the amount of movement of the surface to be measured 9 is detected, photoelectrically converted, and the arithmetic element By processing this, the unevenness of the surface to be measured 9 can be determined.

f、効 果 以上説明したように本発明の平面度測定器によれば、光
学的手段を用いたことによって、非接触に被測定面の平
面形状を測定できるため、被測定面を傷つけることなく
平面性を測定することが可能となり、また微小レンズを
多数並べることにより、被測定平面の形状を2次元的に
かつ高速に測定できるようになった。このように本発明
は、実際の圧板形状測定などにおいて極めて利用価値の
高いものである・
f. Effects As explained above, according to the flatness measuring device of the present invention, the planar shape of the surface to be measured can be measured non-contact by using optical means, so the flatness measurement device can measure the planar shape of the surface to be measured without damaging the surface to be measured. It has become possible to measure flatness, and by arranging a large number of microlenses, it has become possible to measure the shape of a plane to be measured two-dimensionally and at high speed. As described above, the present invention has extremely high utility value in actual pressure plate shape measurement, etc.

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

第1図は本発明の一実施例を示す説明図である。 1:レーザー光源  2:ビームエキスノ(シダー3=
偏光ビームスプリッタ−4:対物レンズ5:1/4人板
  6:コリメーターレンズ7:微小レンズ  8:カ
バーガラス 9;被測定面   10:空間フィルタ(spatia
l filter)11;微小レンズの瞳をWt測面に
共役に導くための光学系12:観測面  13:受光素
子 特許出願人   旭光学工業株式会社 躬10 手続補正書 昭和60年11月27日
FIG. 1 is an explanatory diagram showing one embodiment of the present invention. 1: Laser light source 2: Beam Exno (Cedar 3 =
Polarizing beam splitter 4: Objective lens 5: 1/4 plate 6: Collimator lens 7: Microlens 8: Cover glass 9; Surface to be measured 10: Spatial filter (spatia
l filter) 11; Optical system for guiding the pupil of the microlens to the Wt measuring surface conjugately 12: Observation surface 13: Light receiving element Patent applicant Asahi Kogaku Kogyo Co., Ltd. 10 Procedural amendment November 27, 1985

Claims (1)

【特許請求の範囲】 1、小さな点光源と、その光源からの光を太い平行光束
にする手段と、前記平行光束によって照らされる同一の
微小レンズ・アレイと、その微小レンズ・アレイの焦点
面附近におかれた光軸方向に移動可能な被測定面と、そ
の移動量を測定する移動量検出器と、前記被測定面で反
射した光が入射路をたどり微小レンズを再び通り抜けた
あと、入射光と分離するためのビームスプリッターと、
この反射光を微小レンズの瞳に対して共役な位置に導く
ための光学系と、各微小レンズに対して共役な位置での
光を光電変換する光電検出器と、この光電検出器からの
出力と前記被測定面の移動量を結びつける演算素子を有
することを特徴とする平面度測定器。 2、光源にレーザーを用いることを特徴とする特許請求
の範囲第1項記載の平面度測定器。 3、上記ビームスプリッターが偏光ビームスプリッター
であり、その後に1/4入板を配することを特徴とする
特許請求の範囲第2項記載の平面度測定器。
[Claims] 1. A small point light source, a means for converting the light from the light source into a thick parallel light beam, the same microlens array illuminated by the parallel light flux, and the vicinity of the focal plane of the microlens array. A surface to be measured that can be moved in the direction of the optical axis is placed in A beam splitter to separate the light,
An optical system that guides this reflected light to a position conjugate to the pupil of each microlens, a photoelectric detector that photoelectrically converts the light at a position conjugate to each microlens, and an output from this photoelectric detector. A flatness measuring instrument characterized by having an arithmetic element that connects the amount of movement of the surface to be measured with the amount of movement of the surface to be measured. 2. The flatness measuring instrument according to claim 1, characterized in that a laser is used as a light source. 3. The flatness measuring instrument according to claim 2, wherein the beam splitter is a polarizing beam splitter, followed by a 1/4 plate.
JP3808885A 1985-02-26 1985-02-26 Flatness measuring apparatus Pending JPS61196111A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3808885A JPS61196111A (en) 1985-02-26 1985-02-26 Flatness measuring apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3808885A JPS61196111A (en) 1985-02-26 1985-02-26 Flatness measuring apparatus

Publications (1)

Publication Number Publication Date
JPS61196111A true JPS61196111A (en) 1986-08-30

Family

ID=12515720

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3808885A Pending JPS61196111A (en) 1985-02-26 1985-02-26 Flatness measuring apparatus

Country Status (1)

Country Link
JP (1) JPS61196111A (en)

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