JPH0384403A - Device for measuring shape of plane - Google Patents
Device for measuring shape of planeInfo
- Publication number
- JPH0384403A JPH0384403A JP22125689A JP22125689A JPH0384403A JP H0384403 A JPH0384403 A JP H0384403A JP 22125689 A JP22125689 A JP 22125689A JP 22125689 A JP22125689 A JP 22125689A JP H0384403 A JPH0384403 A JP H0384403A
- Authority
- JP
- Japan
- Prior art keywords
- memory
- value
- reflectance
- plane
- optical system
- 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.)
- Granted
Links
Landscapes
- Length Measuring Devices By Optical Means (AREA)
- Automatic Focus Adjustment (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、サブミクロン程度の平面形状(表面の凹凸)
を光学式のフォーカスエラ一方式を用いて測定す、る平
面形状測定装置における測定精度の改善に関する。[Detailed Description of the Invention] <Industrial Application Field> The present invention is applicable to submicron planar shapes (surface irregularities).
This invention relates to improving measurement accuracy in a planar shape measuring device that measures by using an optical focus error method.
〈従来の技術〉
従来より、測定試料のサブミクロン程度の平面形状を光
学式フォーカスエラ一方式を用いて測定する平面形状測
定装置がある。フォーカスエラー方式には臨界角法と非
点収差法とがある。<Prior Art> Conventionally, there has been a planar shape measuring device that measures the submicron planar shape of a measurement sample using an optical focus error type. Focus error methods include a critical angle method and an astigmatism method.
第6図(イ)は臨界角法の原理構成図、同図(ロ)はそ
のil力特性を示す図である。対象物表面で反射した光
は、対物レンズlを通って臨界角プリズム2に入射し、
プリズム端面で反射した後光電検出器3a、3bに入射
する。この2分割された光電検出器は光軸を境として配
置されており、差動増幅器4はこの光電検出素子の出力
の差(Vout )を求めるようになっている。FIG. 6(a) is a diagram showing the basic configuration of the critical angle method, and FIG. 6(b) is a diagram showing its illumination force characteristics. The light reflected on the object surface passes through the objective lens l and enters the critical angle prism 2,
After being reflected by the end face of the prism, it enters the photoelectric detectors 3a and 3b. The two divided photoelectric detectors are arranged with the optical axis as a boundary, and the differential amplifier 4 is designed to determine the difference (Vout) between the outputs of the photoelectric detection elements.
図において、B点が合焦点であり、そのときは光電検出
器3a、3bに同一光量が戻り、出力Voutは零とな
る。A、0点は焦点からずれた位置であり、そのときは
プリズム2の臨界角より小さいと光電検出器に光が戻ら
ず、Voutは同図(ロ)に示すA、C点のように零以
外の値となる、第7図(イ)は非点収差法の原理構成図
、同図(ロ)はその出力特性を示す図である。測定試料
の反射光路上の、対物レンズ1の後に円筒レンズ5を設
置することにより、A(焦点内)、C(焦点外)点で非
点収差が発生する。同図(ハ)に示すように4分割され
た光電検出器a、 l)、 c、 dを反射光集束点の
近傍に配置しておき、反射光を受光した時同図(ロ)に
示すような光スポツト形状になる。In the figure, point B is the focal point, and at that time the same amount of light returns to the photoelectric detectors 3a and 3b, and the output Vout becomes zero. Point A and 0 are positions shifted from the focal point, and at that time, if the angle is smaller than the critical angle of prism 2, the light will not return to the photoelectric detector, and Vout will be zero as shown at points A and C shown in the same figure (b). FIG. 7(a) is a diagram showing the principle configuration of the astigmatism method, and FIG. 7(b) is a diagram showing its output characteristics. By installing the cylindrical lens 5 after the objective lens 1 on the reflected optical path of the measurement sample, astigmatism occurs at points A (in-focus) and C (out-of-focus). As shown in the same figure (c), photoelectric detectors a, l), c, and d, which are divided into four parts, are placed near the reflected light convergence point, and when the reflected light is received, the photoelectric detectors shown in the same figure (b) It becomes a light spot shape like this.
各光電検出器の出力より、(c十b)−(a+d)を演
算し、その値からフォーカス状態を知ることができる。(c+b)-(a+d) is calculated from the output of each photoelectric detector, and the focus state can be determined from the value.
フォーカスエラーは第7図(二〉に示すような特性とな
る。The focus error has characteristics as shown in FIG. 7 (2).
〈発明が解決しようとする課題〉
しかしながら、臨界角法においては次のような問題があ
る。第8図に示すように、合焦点にある均一表面の対象
試料における反射率が部分的に異なる(低反射率と高反
射率)ような場合、光学系が移動したとき高反射率表面
aおよび低反射率表面Cでは光電検出器3a、3bに戻
る光量は同一であり、差動増幅器4の出力voutは零
となるが、反射率の変化する境界すの近傍では同一平面
上であるにもかかわらず戻る光量が同一でなく出力vo
utは零とはならない。<Problems to be Solved by the Invention> However, the critical angle method has the following problems. As shown in Figure 8, when the reflectance of the target sample with a uniform surface at the focal point is partially different (low reflectance and high reflectance), when the optical system moves, the high reflectance surface a and On the low reflectance surface C, the amount of light returning to the photoelectric detectors 3a and 3b is the same, and the output vout of the differential amplifier 4 is zero, but near the boundary where the reflectance changes, even though they are on the same plane. The amount of light returned is not the same regardless of the output vo
ut does not become zero.
すなわち、反射率の変化によってもフォーカスエラーが
生じ、平面形状を正しく測定することができないという
問題があった。なお、非点収差法においても同様である
。That is, there is a problem in that focus errors occur due to changes in reflectance, making it impossible to accurately measure the planar shape. Note that the same applies to the astigmatism method.
゛本発明の目的は、このような点に鑑みてなされたもの
で、反射率の変化する試料でも正しく平面形状を測定す
ることのできる平面形状測定装置を提供することにある
。An object of the present invention has been made in view of the above points, and is to provide a planar shape measuring device that can accurately measure the planar shape even of a sample whose reflectance changes.
く課題を解決するための手段〉
このような目的を遠戚するために、本発明では、被測定
試料表面に光を照射し、その反射光を収束レンズの合焦
点位置からずれた位置に配置された多分割の光電検出器
で受け、各光電変換器により電気信号に変換して出力す
る測定光学系出力回路と、
この測定光学系出力回路の出力信号が記憶されるメモリ
と、
前記測定光学系出力回路より与えられる新たな測定値と
前記メモリに記憶されている以前の値とを比較し、変化
のあるときは新たな値を前記メモリに記憶すると同時に
平面形状を示す信号を出力する比較演算器
を具備したことを特徴とする。Means for Solving the Problem> In order to achieve this objective, the present invention irradiates the surface of the sample to be measured with light and places the reflected light at a position shifted from the focal point position of the converging lens. a measurement optical system output circuit that receives the signal from the multi-divided photoelectric detector, converts it into an electrical signal by each photoelectric converter, and outputs it; a memory in which the output signal of the measurement optical system output circuit is stored; and the measurement optical system. Comparison that compares the new measured value given by the system output circuit with the previous value stored in the memory, and if there is a change, stores the new value in the memory and outputs a signal indicating the planar shape at the same time. It is characterized by being equipped with a computing unit.
く作用〉
本発明では、被測定試料からの反射光を多分割の光電検
出器で受けるが、光電検出器を焦点位置よりわずかにず
れた位置に配置しておく。Effect> In the present invention, the reflected light from the sample to be measured is received by a multi-divided photoelectric detector, and the photoelectric detector is placed at a position slightly shifted from the focal position.
比較演算器では、メモリに記憶した以前の測定値と、多
分割の充電検出器より出力される今回値を比較観察し、
変化の状態により同一反射率面か反射率境界領域である
かなどを判断し、メモリへの新たな値の書き込みおよび
平面形状を示す信号の出力を行う。The comparison calculator compares and observes the previous measured value stored in memory and the current value output from the multi-divided charge detector.
Depending on the state of change, it is determined whether the surface has the same reflectance or a reflectance boundary area, and a new value is written into the memory and a signal indicating the planar shape is output.
〈実施例〉 以下図面を参照して本発明の詳細な説明する。<Example> The present invention will be described in detail below with reference to the drawings.
第1図は本発明に係る平面形状測定装置の一実施例を示
す構成図である0図において、10は対象試料、20は
測定光学系出力回路、30はメモリ、40は比較演算器
である。FIG. 1 is a block diagram showing an embodiment of a planar shape measuring device according to the present invention. In FIG. 0, 10 is a target sample, 20 is a measurement optical system output circuit, 30 is a memory, and 40 is a comparison calculator. .
測定光学系出力口′#I20は後述するように多分割の
光電検出器を備えており、その光電検出器の出力値は測
定の初期においてはそのままメモリ30に格納される。The measurement optical system output port '#I20 is equipped with a multi-divided photoelectric detector as will be described later, and the output value of the photoelectric detector is stored as is in the memory 30 at the initial stage of measurement.
比較演算器40はその後の測定値(光電検出器の出力f
R)をメモリ30に格納された以前のデータと比較し、
差異のあった場合のみその新たな測定値を格納する。The comparator 40 calculates the subsequent measured value (output f of the photoelectric detector)
R) with previous data stored in memory 30;
Only if there is a difference, the new measured value is stored.
第2図は測定光学系出力回路20の詳細を示す構成図で
ある。レーザダイオード等の光源(図示せず〉からの光
ビームはプリズム22で面内した後対物レンズ21によ
り試料10上に集束される。FIG. 2 is a block diagram showing details of the measurement optical system output circuit 20. A light beam from a light source (not shown) such as a laser diode is focused on the sample 10 by an objective lens 21 after being reflected in the plane by a prism 22 .
試料で反射した光は対物レンズ21およびプリズム22
を通過して収束レンズ23により絞られ、焦点より少し
ずれた位置に配置された光電検出器24に入射する。The light reflected by the sample passes through the objective lens 21 and the prism 22.
The light passes through, is condensed by a converging lens 23, and enters a photodetector 24 located at a position slightly shifted from the focal point.
光電検出器24は第3図(イ)に示すような8分割され
たフォトダイオードセンサアレイである。The photoelectric detector 24 is a photodiode sensor array divided into eight parts as shown in FIG. 3(A).
すなわち、四角形をまず4つの四角形に等分割し、更に
分割の中心を中心とする円で分割する。これにより、図
示のように外側にa〜d、内側に1〜4の分割光電検出
素子が形成される。That is, the quadrilateral is first divided into four equal squares, and then further divided into circles centered at the center of the division. As a result, as shown in the figure, divided photoelectric detection elements a to d are formed on the outside and 1 to 4 on the inside.
なお、合焦時に光電検出器の出力(a十り+c十a)−
(1+2+3+4)が零になる位置に光電検出器を設置
し、試料の平面形状(凹凸)により焦点がずれるとその
信号は第4図に示すように+−に変化する。In addition, when focusing, the output of the photoelectric detector (a + c + a) -
A photoelectric detector is installed at a position where (1+2+3+4) becomes zero, and when the focus shifts due to the planar shape (unevenness) of the sample, the signal changes to +- as shown in FIG.
変換口#t25は、分割光電検出素子の各出力(電流出
力〉を電気信号(電圧信号)に変換し、更にこれをディ
ジタル変換して出力するものである。The conversion port #t25 converts each output (current output) of the divided photoelectric detection element into an electric signal (voltage signal), and further converts this into a digital signal and outputs it.
このような構成における測定動作を第5図の動作フロー
を参照して次に説明する。The measurement operation in such a configuration will be explained next with reference to the operation flow shown in FIG.
■::定光学系出力回路20で試料10表面からの反射
光を光電検出器24で受光し、変換回路25で変換され
た各検出素子a〜d、1〜4の各出力値をメモリ30に
格納する。■:: In the constant optical system output circuit 20, the photoelectric detector 24 receives the reflected light from the surface of the sample 10, and the conversion circuit 25 converts the output values of the detection elements a to d and 1 to 4 into the memory 30. Store in.
■::較演算器40において光電検出器の出力(a+b
十c+d) (1+2+3+4)を演算する。■こ
の演算結果によりフォーカスエラー信号(平面形状信号
)を出力しホールドする。■::The output of the photoelectric detector (a+b
10c+d) Calculate (1+2+3+4). (2) Based on this calculation result, a focus error signal (planar shape signal) is output and held.
■::定終了なら、メモリ30をリセットする。■:: If the process ends, the memory 30 is reset.
■:時時間後後サンプリングして光電検出器出力の総和
(a+b+c+d+1+2+3+4)とメモリの値を比
較する。一致すれば(変化がなければ)同−反射率面で
あり、そのまま演算を行う。(2): Sampling is performed after an hour and the sum of the photoelectric detector outputs (a+b+c+d+1+2+3+4) is compared with the value in the memory. If they match (if there is no change), the reflectance surfaces are the same, and the calculation is performed as is.
光電検出器出力の総和が変化すると反射率が変化してい
る領域になる。A change in the sum total of the photoelectric detector output results in a region where the reflectance is changing.
■〜■:
光電検出器出力のすべてが変化すれば新しい反射率面に
完全に移動したことになるので、メモリ30に新たな値
を記録する。一部の値のみの変化は反射率変化の境界領
域にいることになるので、変化した値はメモリの値を使
用してフォーカスエラー信号を演算する。■~■: If all of the photodetector outputs change, it means that the reflectance surface has been completely moved to a new reflectance surface, so new values are recorded in the memory 30. Since a change in only a part of the values means that the reflectance changes in the boundary region, the changed value is used to calculate a focus error signal using the value in the memory.
〈発明の効果〉
以上詳細に説明したように、本発明では、フォーカスエ
ラー検出光学系として収束レンズと8分割の光電検出器
より構成され、光学系からの信号を電気信号に変換し、
メモリに記録する。そして、時分割で順次測定した信号
とメモリの信号の値を比較することにより、被測定物の
面が反射率の変化している領域にあるのかどうか判断す
ることが可能になる。その結果反射率の変化している領
域の場合には、メモリの値を用いて演算することにより
反射率変化に伴う平面形状(粗度)の測定でも正しい値
を得ることができる。<Effects of the Invention> As explained in detail above, in the present invention, the focus error detection optical system is composed of a converging lens and an 8-divided photoelectric detector, and the signal from the optical system is converted into an electric signal.
Record in memory. By comparing the values of the signals sequentially measured in a time-division manner with the values of the signals in the memory, it becomes possible to determine whether the surface of the object to be measured is in a region where the reflectance is changing. As a result, in the case of a region where the reflectance is changing, correct values can be obtained even when measuring the planar shape (roughness) due to the change in reflectance by performing calculations using the values in the memory.
第1図は本発明に係る平面形状測定装置の一実施例を示
す構成図、第2図は測定光学系出力回路の詳細を示す構
成図、第3図は光電検出器の詳細を示す構成図、第4図
は光電検出器の出力の特性を示す図、第5図は動作フロ
ーを示す図、第6図は臨界角法の原理構成図、第7図は
非点収差法の原理構成図、第8図は反射率の変化が出力
に及ぼす影響を説明するための図である。
10・・・被測定試料、20・・・測定光学系出力回路
、30・・・メモリ、
40・・・比較演算器。
第3図
第4図
第5図
第6図
(イ)
(ロ)
第7図
[c+bl−(a十dl
(ニ)Fig. 1 is a block diagram showing an embodiment of the planar shape measuring device according to the present invention, Fig. 2 is a block diagram showing details of the measurement optical system output circuit, and Fig. 3 is a block diagram showing details of the photoelectric detector. , Figure 4 is a diagram showing the output characteristics of the photoelectric detector, Figure 5 is a diagram showing the operation flow, Figure 6 is a diagram showing the principle of the critical angle method, and Figure 7 is a diagram of the principle of the astigmatism method. , FIG. 8 is a diagram for explaining the influence that a change in reflectance has on output. DESCRIPTION OF SYMBOLS 10... Sample to be measured, 20... Measurement optical system output circuit, 30... Memory, 40... Comparison calculator. Figure 3 Figure 4 Figure 5 Figure 6 (A) (B) Figure 7 [c+bl-(a0dl (d)
Claims (1)
電検出器で受け、各光電変換器により電気信号に変換し
て出力する測定光学系出力回路と、この測定光学系出力
回路の出力信号が記憶されるメモリと、 前記測定光学系出力回路より与えられる新たな測定値と
前記メモリに記憶されている以前の値とを比較し、変化
のあるときは新たな値を前記メモリに記憶すると同時に
平面形状を示す信号を出力する比較演算器 を具備したことを特徴とする平面形状測定装置。[Scope of Claims] A measurement optical system output circuit that irradiates light onto the surface of a sample to be measured, receives the reflected light with a multi-divided photoelectric detector, converts it into an electrical signal by each photoelectric converter, and outputs it; A memory in which the output signal of the measurement optical system output circuit is stored, and a new measured value given from the measurement optical system output circuit is compared with the previous value stored in the memory, and if there is a change, the new measurement value is 1. A planar shape measuring device comprising: a comparator that stores a value in the memory and outputs a signal indicating a planar shape at the same time.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22125689A JP2517406B2 (en) | 1989-08-28 | 1989-08-28 | T-plane shape measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22125689A JP2517406B2 (en) | 1989-08-28 | 1989-08-28 | T-plane shape measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0384403A true JPH0384403A (en) | 1991-04-10 |
| JP2517406B2 JP2517406B2 (en) | 1996-07-24 |
Family
ID=16763920
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22125689A Expired - Lifetime JP2517406B2 (en) | 1989-08-28 | 1989-08-28 | T-plane shape measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2517406B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2017107201A (en) * | 2015-12-09 | 2017-06-15 | 由田新技股▲ふん▼有限公司 | Dynamic autofocus system |
-
1989
- 1989-08-28 JP JP22125689A patent/JP2517406B2/en not_active Expired - Lifetime
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2017107201A (en) * | 2015-12-09 | 2017-06-15 | 由田新技股▲ふん▼有限公司 | Dynamic autofocus system |
| US10521895B2 (en) | 2015-12-09 | 2019-12-31 | Utechzone Co., Ltd. | Dynamic automatic focus tracking system |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2517406B2 (en) | 1996-07-24 |
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