JPH0458884B2 - - Google Patents
Info
- Publication number
- JPH0458884B2 JPH0458884B2 JP9012885A JP9012885A JPH0458884B2 JP H0458884 B2 JPH0458884 B2 JP H0458884B2 JP 9012885 A JP9012885 A JP 9012885A JP 9012885 A JP9012885 A JP 9012885A JP H0458884 B2 JPH0458884 B2 JP H0458884B2
- Authority
- JP
- Japan
- Prior art keywords
- measured
- focusing
- output
- signal
- sensor
- 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
Links
- 238000005259 measurement Methods 0.000 claims description 36
- 238000000034 method Methods 0.000 claims description 20
- 238000001514 detection method Methods 0.000 claims description 14
- 230000003287 optical effect Effects 0.000 claims description 11
- 238000000691 measurement method Methods 0.000 claims description 2
- 238000010586 diagram Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F9/00—Registration or positioning of originals, masks, frames, photographic sheets or textured or patterned surfaces, e.g. automatically
- G03F9/70—Registration or positioning of originals, masks, frames, photographic sheets or textured or patterned surfaces, e.g. automatically for microlithography
- G03F9/7003—Alignment type or strategy, e.g. leveling, global alignment
- G03F9/7023—Aligning or positioning in direction perpendicular to substrate surface
- G03F9/7026—Focusing
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Measurement Of Optical Distance (AREA)
Description
【発明の詳細な説明】
(1) 技術分野
本発明は、円環状光束を用いた距離測定装置に
於る測定方法に関する。DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field The present invention relates to a measuring method in a distance measuring device using an annular light beam.
(2) 従来技術
従来、光学的距離測定装置として本件出願人よ
る特願昭59−242490が有る。ここで提案されてい
る距離測定装置を第1図に示す。図中、1はレー
ザ光源、2はコリメータレンズ、3は第1の円錐
形ミラー、4は第2の円錐形ミラー、5は焦点距
離可変レンズ、6は偏光ビームスプリツター、7
は1/4波長板、8は集光レンズ、9は被測定物、
10は合焦検知手段、11は処理装置である。(2) Prior Art Conventionally, there is a Japanese Patent Application No. 59-242490 filed by the present applicant regarding an optical distance measuring device. The distance measuring device proposed here is shown in FIG. In the figure, 1 is a laser light source, 2 is a collimator lens, 3 is a first conical mirror, 4 is a second conical mirror, 5 is a variable focal length lens, 6 is a polarizing beam splitter, and 7
is a 1/4 wavelength plate, 8 is a condenser lens, 9 is an object to be measured,
10 is a focus detection means, and 11 is a processing device.
レーザ光源1から出射したレーザ光は、コリメ
ータレンズ2により平光光束となつて第1の円錐
形ミラー3、第2の円錐形ミラー4を介して中心
部分が暗い円環状光束(以下、リングビームと記
す)となる。このリングビームは焦点距離可変レ
ンズ5、偏光ビームスプリツター6を通り、直線
偏光を円偏光に変換された後集光レンズ8を介し
て被測定物9上に投射される。被測定物9の上面
で反射されたリングビームは、集光レンズ8を通
り1/4波長板7により円偏向を入射時と直交する
直線偏光に変換され、偏光ビームスプリツタ6で
反射して偏向され合焦検知手段10に投射され
る。 The laser beam emitted from the laser light source 1 is turned into a flat beam by a collimator lens 2, and then passes through a first conical mirror 3 and a second conical mirror 4 into an annular beam with a dark center (hereinafter referred to as a ring beam). ). This ring beam passes through a variable focal length lens 5 and a polarizing beam splitter 6, converts linearly polarized light into circularly polarized light, and then projects it onto an object to be measured 9 via a condenser lens 8. The ring beam reflected on the top surface of the object to be measured 9 passes through a condensing lens 8 and is converted from circular polarization by a quarter-wave plate 7 into linearly polarized light perpendicular to the incident light, and then reflected by a polarizing beam splitter 6. It is deflected and projected onto the focus detection means 10.
第2図は合焦検知手段10の受光面を示してお
り、円環状のリングセンサ12,13により同心
円を形成している。 FIG. 2 shows the light receiving surface of the focus detection means 10, in which annular ring sensors 12 and 13 form concentric circles.
合焦検知手段10に投射されるリングビーム
は、リングビームの焦点位置と被測定物9との位
置関係に応じてそのビーム径を変化させる為、リ
ングビームの焦点位置が被測定物9の上面と一致
する時にリングセンサ12と13の各々から得ら
れる出力が等しくなる様、ビーム径及びリングセ
ンサ12,13の径を設定しておけば、被測定物
9の位置に応じた合焦状態の変化をリングセンサ
12,13の出力差によつて検出する事が出来
る。尚、第3図に示す如く被測定物9の位置と合
焦状態を示す合焦信号(通常リングセンサ12,
13の出力差をその出力和で規格化したもの)と
は所定の測定範囲に於て良好な線型関係を保つて
いる。 The ring beam projected onto the focus detection means 10 changes its beam diameter according to the positional relationship between the focal position of the ring beam and the object to be measured 9, so that the focal position of the ring beam is on the upper surface of the object to be measured 9. If the beam diameter and the diameter of the ring sensors 12 and 13 are set so that the outputs obtained from each of the ring sensors 12 and 13 are equal when the Changes can be detected by the difference in output between ring sensors 12 and 13. Incidentally, as shown in FIG. 3, a focus signal (usually a ring sensor 12,
13, which is normalized by the output sum), maintains a good linear relationship within a predetermined measurement range.
従つて、この様な装置を用いて測定を行なう場
合、予め被測定物の略々の位置を知つておくか、
被測定物自体を所定の測定範囲内に配置する必要
が有り、測定時間を短縮できず、自動化も困難で
あつた。又、測定時に最も検出感度の良いリング
ビームの焦点位置が解らない為、事実上、最良の
状態で測定できず、測定精度も十分に信頼できる
ものではなかつた。 Therefore, when performing measurements using such a device, it is necessary to know the approximate location of the object to be measured in advance, or
The object to be measured itself must be placed within a predetermined measurement range, making it impossible to shorten the measurement time and making automation difficult. Furthermore, since the focal position of the ring beam with the best detection sensitivity is not known during measurement, it is virtually impossible to measure under the best conditions, and the measurement accuracy is not sufficiently reliable.
(3) 発明の概要
本発明の目的は、上記従来の欠点に鑑み、測定
の自動化及び高速化を達成し得る距離測定方法を
提供する事にある。(3) Summary of the Invention In view of the above-mentioned conventional drawbacks, an object of the present invention is to provide a distance measuring method that can automate and speed up measurement.
上述目的を達成する為に、本発明に係わる距離
測定方法は、光軸方向の一点に集光する測定用光
束の集光位置を光軸方向の複数位置に順次変化さ
せ、被測定面で反射された前記測定用光束を、被
測定面の光軸方向位置に応じて前記測定用光束の
変位する方向に配列された2つのセンサ部を有す
る合焦検知手段で検知する第一過程と、該合焦検
知手段の前記2つのセンサ部の各出力に基づく差
分の関数として得られる合焦信号の極性が変化す
る前後の2つの集光位置を得る第二過程と、前記
2つの集光位置から、前記被測定面の位置と前記
合焦信号とがほぼ線形な関係を備えた測定範囲内
に前記被測定面を有する集光位置を選別する第三
過程とを有し、該選別された集光位置で得られる
合焦信号から前記被測定面までの距離を測定する
ことを特徴とする。 In order to achieve the above-mentioned object, the distance measuring method according to the present invention sequentially changes the focusing position of the measurement light beam focused at one point in the optical axis direction to a plurality of positions in the optical axis direction, and reflects it on the surface to be measured. a first step of detecting the measured light beam with a focus detection means having two sensor sections arranged in a direction in which the measurement light beam is displaced according to the position of the surface to be measured in the optical axis direction; a second process of obtaining two light focusing positions before and after the polarity of the focusing signal obtained as a function of the difference based on the respective outputs of the two sensor sections of the focus detection means changes; and from the two light focusing positions; a third step of selecting a light focusing position having the surface to be measured within a measurement range in which the position of the surface to be measured and the focusing signal have a substantially linear relationship; The method is characterized in that the distance from the focusing signal obtained at the optical position to the surface to be measured is measured.
好ましくは、前記測定用光束はリングビームで
あり、前記合焦検知手段は、通常内側と外側の2
つに分割されたリングセンサを有し、該リングセ
ンサの外側と内側の出力差、もしくは該出力差を
前記リングセンサの外側と内側の出力和で規格化
した値を合焦信号として用いる。前記リングビー
ムの集光位置の変化に伴ない、前記合焦信号の極
性が変化した時の前記リングセンサの内側の出力
と前記合焦信号の極性が変化する前の前記リング
センサの外側の出力とを比較するか、もしくは、
前記合焦信号の極性が変化した時の前記リングセ
ンサの外側の出力と前記合焦信号の極性が変化す
る前の前記リングセンサの内側の出力とを比較
し、該出力の大きい方の合焦信号により前記被測
定面までの距離を測定する事が出来る。 Preferably, the measurement light beam is a ring beam, and the focus detection means usually includes two inner and outer beams.
It has a ring sensor divided into two parts, and uses the difference in output between the outside and inside of the ring sensor, or a value obtained by normalizing the output difference by the sum of the outputs of the outside and inside of the ring sensor, as a focusing signal. An output from the inside of the ring sensor when the polarity of the focusing signal changes with a change in the focusing position of the ring beam, and an output from the outside of the ring sensor before the polarity of the focusing signal changes. or,
The output from the outside of the ring sensor when the polarity of the focus signal changes is compared with the output from the inside of the ring sensor before the polarity of the focus signal changes, and the one with the larger output is focused. The distance to the surface to be measured can be measured by the signal.
上記方法に従い測定を行なえば、自動的に最適
な集光位置を検出し、該集光位置で被測定面まで
の距離を測定出来る。 If the measurement is performed according to the above method, the optimum light focusing position can be automatically detected and the distance to the surface to be measured can be measured at the light focusing position.
以下、本発明に係る距離測定方法の基本原理を
説明する。 The basic principle of the distance measuring method according to the present invention will be explained below.
第4図は本発明の基本原理説明図で、第1図と
同じ部材には同番号を符す。尚、14は集光レン
ズ8により集光されたリングビーム、P1,P2,
P3は光学系の焦点距離を変化させた時のリング
ビーム14の各集光位置、A1,A2,A3は各集光
位置P1,P2,P3に於る測定範囲を示す。 FIG. 4 is a diagram illustrating the basic principle of the present invention, and the same members as in FIG. 1 are designated by the same numbers. In addition, 14 is a ring beam condensed by the condensing lens 8, P 1 , P 2 ,
P 3 is each focusing position of the ring beam 14 when the focal length of the optical system is changed, and A 1 , A 2 , A 3 is the measurement range at each focusing position P 1 , P 2 , P 3 . show.
第1図に示す如き装置に於いては、前述の様に
リングビーム14の所定の集光位置に対応して、
位置と合焦信号が良好な線型関係にある。従つ
て、焦点距離可変レンズ等を用い集光位置をP1,
P2,P3……と変化させ、前記測定範囲をA1,
A2,A3……とシフトする事により、被測定物9
の位置を検出し得る測定範囲を有する集光位置へ
リングビーム14を集光させる事が出来る。 In the device as shown in FIG.
The position and focus signal have a good linear relationship. Therefore, using a variable focal length lens, etc., the focusing position is set to P 1 ,
P 2 , P 3 ..., and the measurement range is changed to A 1 , P 3 ...
By shifting A 2 , A 3 ..., the object to be measured 9
The ring beam 14 can be focused on a focusing position that has a measurement range that can detect the position of the ring beam.
例えば、第2図で示す如きリングセンサ12,
13からの出力を各々D1,D2とすると、合焦信
号は差信号D2−D1を強度信号D2+D1で規格化し
た値F、即ち
F=D2−D1/D2+D1 …(1)
で表わす事が出来る。この時、第4図に示す様に
リングビーム14の集光位置を集光レンズ8側か
ら順次変化させる場合、被測定物9で反射された
リングビーム14は、集光位置がP1,P2の如く
集光レンズ8と被測定物9の間にある時は、ビー
ム径が拡げられて集光レンズ8へ入射し、集光レ
ンズ8により収斂光となる為、リングセンサ1
2,13へは合焦時より径が小さくなり投射され
る。従つて、合焦信号Fの値は(1)式よりF<0と
なる。次に集光位置がP3の如く被測定物9の集
光レンズ8とは逆側にある時は、ビーム径が小さ
くなつて集光レンズ8へ入射し、集光レンズ8に
より発散光となる為、リングセンサ12,13へ
は合焦時より径が大きくなり投射される。従つ
て、合焦信号Fの値は(1)式よりF>0となる。即
ち、リングビーム14の集光位置を順次変化させ
て合焦信号Fの極性を判別していけば、被測定物
9を介して集光レンズ8側とその反対側の最も被
測定物9に近接した2つの集光位置の間で極性が
変化する為、該2つの集光位置の少なくとも一方
が測定に於る最適集光位置となる。 For example, a ring sensor 12 as shown in FIG.
If the outputs from 13 are D 1 and D 2 respectively, the focusing signal is the value F which is the difference signal D 2 - D 1 normalized by the intensity signal D 2 + D 1 , that is, F = D 2 - D 1 /D 2 +D 1 ...(1) It can be expressed as: At this time, when the condensing position of the ring beam 14 is sequentially changed from the condensing lens 8 side as shown in FIG. When the beam is between the condenser lens 8 and the object to be measured 9 as shown in 2 , the beam diameter is expanded and enters the condenser lens 8, and becomes converged light by the condenser lens 8, so the ring sensor 1
2 and 13 are projected with a smaller diameter than when in focus. Therefore, the value of the focus signal F becomes F<0 from equation (1). Next, when the condensing position is on the opposite side of the object to be measured 9 from the condensing lens 8, as shown in P3 , the beam diameter becomes smaller and enters the condensing lens 8, and the condensing lens 8 converts the beam into a diverging beam. Therefore, the beam is projected onto the ring sensors 12 and 13 with a larger diameter than when in focus. Therefore, the value of the focus signal F is F>0 from equation (1). That is, by sequentially changing the focusing position of the ring beam 14 and determining the polarity of the focusing signal F, it is possible to determine the polarity of the focusing signal F by sequentially changing the focusing position of the ring beam 14. Since the polarity changes between two adjacent light focusing positions, at least one of the two light focusing positions becomes the optimum light focusing position for measurement.
尚、上述の説明では、集光レンズ8側から集光
位置を順次変化させているが、被測定物9を介し
て集光レンズ8とは反対側から順次変化させても
良い。又、集光位置の変化量は各集光位置を中心
にして定まる測定範囲が連続しているのが好まし
く、当然隣接する測定範囲の一部が重複しても構
わない。更に、上述の説明では合焦信号として規
格化した値を使用しているが、単に差信号D2−
D1を合焦信号として用いても良く、差信号とし
てD1−D2の値を用いても当然構わない。但し差
信号としてD1−D2の値を用いる場合、被測定物
と合焦信号との線型関係は、第3図に示すものと
は逆に左上がりの直線となり、又被測定物の前後
に於る合焦信号の変化の仕方も逆になる。 In the above description, the condensing position is sequentially changed from the condenser lens 8 side, but it may be sequentially changed from the side opposite to the condenser lens 8 via the object to be measured 9. Further, it is preferable that the measurement ranges determined by the amount of change in the light focusing position are continuous, with each light focusing position being the center, and it is of course possible for adjacent measurement ranges to partially overlap. Furthermore, although the above explanation uses a standardized value as the focus signal, it is simply the difference signal D 2 −
Of course, D 1 may be used as the focusing signal, and the value of D 1 −D 2 may be used as the difference signal. However, when using the value of D 1 - D 2 as the difference signal, the linear relationship between the object to be measured and the focusing signal will be a straight line sloping upward to the left, contrary to what is shown in Fig. The manner in which the focusing signal changes is also reversed.
以下、実施例により本発明を詳述する。 Hereinafter, the present invention will be explained in detail with reference to Examples.
(4) 実施例
第5図は本発明に係る距離測定方法のフローチ
ヤート図を示す。(4) Embodiment FIG. 5 shows a flowchart of the distance measuring method according to the present invention.
本実施例に示す距離測定方法を適用し、被測定
面までの距離を測定する装置として第1図、第2
図に示した装置を考える。ここで、焦点距離可変
レンズ5により距離Nのステツプで集光位置を変
化させる事が出来るものとし、被測定面に最も近
接した2つの集光位置の内、集光レンズ8側の集
光位置に於るリング状センサの内側12、外側1
3の出力を各々D′1,D′2、又、集光レンズ8とは
反対側の焦点位置に於るリングセンサの内側1
2、外側13の出力を各々D1,D2とする。更に
合焦信号は前述の様にF=D2−D1/D2+D1で表わすもの
とする。 Figures 1 and 2 show an apparatus for measuring the distance to a surface to be measured by applying the distance measuring method shown in this example.
Consider the device shown in the figure. Here, it is assumed that the focal length variable lens 5 can change the focusing position in steps of distance N, and the focusing position on the focusing lens 8 side is of the two focusing positions closest to the surface to be measured. Inside 12 and outside 1 of the ring-shaped sensor in
The outputs of 3 are respectively D' 1 and D' 2 , and the outputs of the ring sensor 1 at the focal position opposite to the condenser lens 8 are
2. Let the outputs of the outside 13 be D 1 and D 2 respectively. Furthermore, the focusing signal is expressed as F=D 2 -D 1 /D 2 +D 1 as described above.
まず、最も集光レンズ8に近い焦点距離にリン
グビームを集光させて合焦信号Fの検出を開始す
る。F>0、即ちリングビームの集光位置が被測
定面の集光レンズ8とは逆側になるまで、焦点距
離可変レンズ5により、焦点距離を+Nづつ増加
していき、その都度合焦信号Fの極性を判別し、
F>0になつた時の集光位置に於るリングセンサ
12の出力信号D1を記憶する。 First, the ring beam is focused at the focal length closest to the condenser lens 8, and detection of the focus signal F is started. The focal length is increased by +N by the variable focal length lens 5 until F>0, that is, the focal position of the ring beam is on the opposite side of the surface to be measured from the condensing lens 8, and each time the focus signal is Determine the polarity of F,
The output signal D1 of the ring sensor 12 at the light focusing position when F>0 is stored.
次に、F>0になつた時の集光位置から−N離
れた(Nだけ集光レンズに近い)位置、即ち被測
定面に最も近接し且つ集光レンズ8側の集光位置
へ再びリングビームを集光させ、この時のリング
センサ13の出力信号D′2を記憶する。 Next, return to the position -N away from the focusing position when F>0 (closer to the focusing lens by N), that is, the focusing position closest to the surface to be measured and on the side of the focusing lens 8. The ring beam is focused, and the output signal D' 2 of the ring sensor 13 at this time is stored.
ここで、記憶された出力信号D1とD′2の大小比
較を行ない、D1≦D′2であれば現在のF<0であ
る集光位置に於る合焦信号Fと焦点距離から得ら
れる被測定面までの距離を測定値とする。又D1
>D′2であれば再び現在のF<0である集光位置
より+Nだけ離れた位置へリングビームを集光さ
せ、この集光位置に於る合焦信号Fと焦点距離か
ら得られる被測定面までの距離を測定値とする。
尚、この様なD1とD′2との比較は、被測定面を介
した2つの集光位置の内、更に被測定面に近接し
ており且つ該集光位置を中心とする測定範囲(第
3図参照)に被測定面を含んでいる最適集光位置
を検知する為に行なう。 Here, the stored output signals D 1 and D' 2 are compared in magnitude, and if D 1 ≦ D' 2 , it is determined from the in-focus signal F and focal length at the current focusing position where F < 0. The resulting distance to the surface to be measured is taken as the measured value. Also D 1
>D′ 2 , the ring beam is again focused at a position +N away from the current focusing position where F<0, and the focus signal F at this focusing position and the focal length obtained from the focal length are The distance to the measurement surface is taken as the measured value.
Note that this comparison of D 1 and D' 2 is based on the measurement range that is closer to the surface to be measured and centered on the focal point of the two focal points via the surface to be measured. This is done in order to detect the optimum light focusing position that includes the surface to be measured (see Fig. 3).
第6図は本発明に係る距離測定方法の別のフロ
ーチヤート図を示す。本方法を適用する装置とし
ては前記実施例同様第1図、第2図に示した装置
を考え、集光位置変化量N、リングセンサ12,
13の出力信号D1,D2,D′1,D′2、及び合焦信
号F等全て前記実施例同様として取り扱う。 FIG. 6 shows another flow chart of the distance measuring method according to the present invention. As the apparatus to which this method is applied, the apparatus shown in FIGS.
No. 13 output signals D 1 , D 2 , D' 1 , D' 2 , focus signal F, etc. are all handled as in the previous embodiment.
最初に装置を始動させ、任意の集光位置に於る
リングセンサ12,13での合焦信号Fを検出す
る。ここで、Fの、極性を検出し現在のリングビ
ームの集光位置が、被測定面から見て集光レンズ
8側にあるのか、又は反対側にあるのかを判別す
る。 First, the apparatus is started and a focus signal F from the ring sensors 12 and 13 at an arbitrary light focusing position is detected. Here, the polarity of F is detected to determine whether the current focusing position of the ring beam is on the condensing lens 8 side or on the opposite side when viewed from the surface to be measured.
合焦信号F>0の時は、リングビームの集光位
置が被測定面から見て集光レンズ8と反対側にあ
る為、現在位置から−Nづつ集光位置を変化さ
せ、徐々に集光レンズ8に近づける。この時各集
光位置毎に合焦信号Fの極性を判別する。F>0
であればこの判別を繰り返し、F<0になつた時
の集光位置に於るリングセンサ13の出力信号
D′2を記憶する。次に、F<0である現在位置か
ら再度+N離れた集光位置へリングビームを集光
させ、この集光位置に於るリングセンサ12の出
力信号D1を記憶する。記憶された出力信号D′2,
D1を大小比較し、D1≧D′2であればこの集光位置
に於る合焦信号Fと焦点距離から得られる測定値
を被測定面までの距離とする。又、D′2>D1であ
ればF<0である現在位置から−N離れた位置へ
リングビームを集光させ、この集光位置に於る合
焦信号Fと焦点距離から得られる測定値を被測定
面までの距離とする。 When the focus signal F>0, the condensing position of the ring beam is on the opposite side of the condenser lens 8 when viewed from the surface to be measured, so the condensing position is changed by -N from the current position, and the condensing position is gradually focused. Bring it closer to the optical lens 8. At this time, the polarity of the focusing signal F is determined for each focusing position. F>0
If so, repeat this determination and obtain the output signal of the ring sensor 13 at the condensing position when F<0.
Remember D′ 2 . Next, the ring beam is again focused at a focusing position that is +N away from the current position where F<0, and the output signal D 1 of the ring sensor 12 at this focusing position is stored. Stored output signal D′ 2 ,
The magnitude of D 1 is compared, and if D 1 ≧D′ 2 , the measured value obtained from the focus signal F and the focal length at this focusing position is taken as the distance to the surface to be measured. Also, if D' 2 > D 1 , the ring beam is focused at a position -N away from the current position where F < 0, and the measurement obtained from the focusing signal F and focal length at this focusing position is Let the value be the distance to the surface to be measured.
次に、装置作動直後の合焦信号Fの極性がF<
0の場合、リングビームの集光位置は被測定面か
ら見て集光レンズ8側にある為、現在位置から+
Nづつ集光位置を変化させ、徐々に集光レンズ8
から遠ざける。この時各集光位置毎に合焦信号F
の極性を判別する。 Next, the polarity of the focusing signal F immediately after the device is activated is F<
In the case of 0, the condensing position of the ring beam is on the condensing lens 8 side when viewed from the surface to be measured, so it is + from the current position.
The condensing position is changed by N, and the condensing lens 8 is gradually
keep away from At this time, the focus signal F for each focus position
Determine the polarity of
F<0であればこの判別を繰り返し、F>0に
なつた時の集光位置に於るリングセンサ12の出
力信号D1を記憶する。続いて、F>0である現
在位置から再度−N離れた集光位置へリングビー
ムを集させ、この集光位置に於るリングセンサ1
3の出力信号D′2、を記憶する。記憶された出力
信号D1,D′2を大小比較し、D′2≧D1であればこ
の集光位置に於る合焦信号Fと焦点距離から得ら
れる測定値を被測定面までの距離とする。又、
D1>D′2であれば現在位置から+N離れた位置へ
リングビームを集光させ、この集光位置に於る合
焦信号Fと焦点距離から得られる測定値を被測定
面までの距離とする。 If F<0, this determination is repeated, and the output signal D1 of the ring sensor 12 at the condensing position when F>0 is stored. Next, the ring beam is again focused at a focusing position that is −N away from the current position where F>0, and the ring sensor 1 at this focusing position is
3, the output signal D' 2 is stored. The stored output signals D 1 and D′ 2 are compared in magnitude, and if D′ 2 ≧D 1 , the measurement value obtained from the focal signal F and focal length at this condensing position is used as the distance to the surface to be measured. Distance. or,
If D 1 >D' 2 , the ring beam is focused at a position +N away from the current position, and the measured value obtained from the focusing signal F and focal length at this focusing position is calculated as the distance to the surface to be measured. shall be.
尚、測定中、合焦信号FがF=0となつた場合
は、リングビームの集光位置に被測定面が存在し
ている為、即、被測定面位置が検出された事にな
る。 If the focus signal F becomes F=0 during the measurement, the surface to be measured exists at the condensing position of the ring beam, and this means that the position of the surface to be measured has been detected immediately.
又、距離N毎の集光位置変化に従い連続して得
られる各測定範囲に重複部分があり、その重複部
分に被測定面が存在する場合、各々の測定範囲を
有する集光位置のどちらに於る合焦信号Fを用い
て被測定面までの距離を検出しても構わない。 In addition, if there is an overlapping part in each measurement range that is continuously obtained according to the change in the focusing position for each distance N, and the surface to be measured exists in the overlapping part, which of the focusing positions with each measurement range is located? The distance to the surface to be measured may be detected using the focusing signal F.
以上の如き方法を用いた測定は、例えば第1図
に示される装置に於る処理装置11等に組み込ま
れたマイコンにより自動的に制御される為、高速
処理が可能で測定結果はすぐに得る事が出来る。 Measurement using the above method is automatically controlled by a microcomputer built into the processing device 11 of the apparatus shown in FIG. 1, for example, so high-speed processing is possible and measurement results can be obtained immediately. I can do things.
上記2つの実施例では、被測定面に最も近接し
た2つの集光位置を検出し、リングセンサの出力
D1とD′2を比較する事により最適集光位置を検出
した後、合焦信号Fから被測定面までの距離を測
定しているが、各集光位置に於る合焦信号Fもし
くは測定値を記憶しておき、最適集光位置検出
後、その位置に対応する記憶していた合焦信号F
もしくは測定値を呼び出す方法もある。従つて、
上記実施例以外にも本発明の思想を逸脱しない限
り各種応用が可能である。 In the above two embodiments, the two light focusing positions closest to the surface to be measured are detected, and the output of the ring sensor is
After detecting the optimal focusing position by comparing D 1 and D′ 2 , the distance from the focusing signal F to the surface to be measured is measured. After memorizing the measured values and detecting the optimal focusing position, the stored focusing signal F corresponding to that position is
Alternatively, there is also a method of calling the measured value. Therefore,
Various applications other than the above-mentioned embodiments are possible as long as they do not depart from the spirit of the present invention.
又、本実施例では被測定面までの距離を測定す
る方法に関して述べたが、例えば半導体装置に於
るマスクとウエハーの間隔を測定するギヤツプ測
定装置等に応用可能で、この場合、マスク及びウ
エハー各々の距離を測定しその差を取る事で両者
の間隔を測定出来る。 Furthermore, although this embodiment has described a method for measuring the distance to the surface to be measured, it can also be applied to, for example, a gap measuring device that measures the distance between a mask and a wafer in a semiconductor device. By measuring each distance and taking the difference, you can measure the distance between them.
(5) 発明の効果
以上説明した様に、本発明に係る距離測定方法
は自動的に測定時に最適集光位置を検出する事が
可能で、且つ高速に最適集光位置を検出し被測定
面までの距離を測定し得る測定方法である。(5) Effects of the Invention As explained above, the distance measuring method according to the present invention can automatically detect the optimum light focusing position during measurement, and can detect the optimum light focusing position at high speed to This is a measurement method that can measure the distance to.
第1図は光学的距離測定装置の一例を示す図。
第2図はリング状センサを示す図。第3図は合焦
信号と被測定位置との関係を示す図。第4図は本
発明に係る距離測定方法の基本原理説明図。第5
図、第6は本発明に係る距離測定方法の一例を示
すフローチヤート図。
1……レーザ光源、2……コリメータレンズ、
3……第1の円錐形ミラー、4……第2の円錐形
ミラー、5……焦点距離可変レンズ、6……偏光
ビームスプリツター、7……1/4波長板、8……
集光レンズ、9……被測定物、10……合焦検知
手段、11……処理装置、12,13……リング
状センサ、A1,A2,A3……測定範囲、P1,P2,
P3……集光位置。
FIG. 1 is a diagram showing an example of an optical distance measuring device.
FIG. 2 is a diagram showing a ring-shaped sensor. FIG. 3 is a diagram showing the relationship between the focus signal and the measured position. FIG. 4 is a diagram explaining the basic principle of the distance measuring method according to the present invention. Fifth
FIG. 6 is a flowchart showing an example of the distance measuring method according to the present invention. 1... Laser light source, 2... Collimator lens,
3...First conical mirror, 4...Second conical mirror, 5...Variable focal length lens, 6...Polarizing beam splitter, 7...1/4 wavelength plate, 8...
Condensing lens, 9...Object to be measured, 10...Focus detection means, 11...Processing device, 12, 13...Ring sensor, A1 , A2 , A3 ...Measurement range, P1 , P2 ,
P 3 ……Focusing position.
Claims (1)
位置を光軸方向の複数位置に順次変化させ、被測
定面で反射された前記測定用光束を、被測定面の
光軸方向位置に応じて前記測定用光束の変位する
方向に配列された2つのセンサ部を有する合焦検
知手段で検知する第一過程と、該合焦検知手段の
前記2つのセンサ部の各出力に基づく差分の関数
として得られる合焦信号の極性が変化する前後の
2つの集光位置を得る第二過程と、前記2つの集
光位置から、前記被測定面の位置と前記合焦信号
とがほぼ線形な関係を備えた測定範囲内に前記被
測定面を有する集光位置を選別する第三過程とを
有し、該選別された集光位置で得られる合焦信号
から前記被測定面までの距離を測定することを特
徴とする距離測定方法。 2 前記測定用光束は円環状であり、前記合焦検
知手段が前記2つのセンサ部として内側と外側の
2つに分割された円環状センサを有し、該円環状
センサの外側と内側の出力差、もしくは該出力差
を前記円環状センサの外側と内側の出力和で規格
化した値を前記合焦信号とし、該合焦信号の極性
が変化した時の前記円環状センサの内側の出力
と、該合焦信号の極性が変化する前の前記円環状
センサの外側の出力とを比較し、該出力が大きい
方の合焦信号から前記被測定面までの距離を測定
することを特徴とする特許請求の範囲第1項記載
の距離測定方法。 3 前記測定用光束は円環状であり、前記合焦検
知手段が、前記2つのセンサ部として内側と外側
の2つに分割された円環状センサを有し、該円環
状センサの外側と内側の出力差、もしくは該出力
差を前記円環状センサの外側と内側の出力和で規
格化した値を前記合焦信号とし、該合焦信号の極
性が変化した時の前記円環状センサの外側の出力
と、該合焦信号の極性が変化する前の前記円環状
センサの内側の出力とを比較し、該出力が大きい
方の合焦信号から前記被測定面までの距離を測定
することを特徴とする特許請求の範囲第1項記載
の距離測定方法。[Scope of Claims] 1. Sequentially changing the convergence position of the measurement light beam condensed at one point in the optical axis direction to a plurality of positions in the optical axis direction, and directing the measurement light beam reflected from the surface to be measured to the measurement object. a first step of detecting with a focus detection means having two sensor sections arranged in a direction in which the measurement light beam is displaced according to the position of the surface in the optical axis direction, and the two sensor sections of the focus detection means; A second process of obtaining two light focusing positions before and after the polarity of the focusing signal obtained as a function of the difference based on each output of a third step of selecting a focusing position having the surface to be measured within a measurement range having a substantially linear relationship with the focusing signal; A distance measurement method characterized by measuring the distance to a surface to be measured. 2. The measurement light beam is annular, and the focus detection means has an annular sensor divided into an inner and an outer part as the two sensor parts, and the output of the outer and inner parts of the annular sensor is The difference or the value obtained by normalizing the output difference by the sum of the outputs of the outside and inside of the annular sensor is the focus signal, and the output of the inside of the annular sensor when the polarity of the focus signal changes. , the focus signal is compared with the output from the outside of the annular sensor before the polarity changes, and the distance from the focus signal with the larger output to the surface to be measured is measured. A distance measuring method according to claim 1. 3. The measurement light beam is annular, and the focus detection means has an annular sensor divided into two, an inner and an outer part, as the two sensor parts, and an outer and an inner part of the annular sensor. The output difference or the value obtained by normalizing the output difference by the sum of the outputs of the outside and inside of the annular sensor is the focus signal, and the output of the outside of the annular sensor when the polarity of the focus signal changes. and an output from the inner side of the annular sensor before the polarity of the focusing signal changes, and the distance from the focusing signal with the larger output to the surface to be measured is measured. A distance measuring method according to claim 1.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9012885A JPS61247910A (en) | 1985-04-26 | 1985-04-26 | Distance measuring method |
| FR8515821A FR2572515B1 (en) | 1984-10-25 | 1985-10-24 | POSITION DETECTION DEVICE |
| DE3538062A DE3538062C2 (en) | 1984-10-25 | 1985-10-25 | Position detection device |
| GB08526374A GB2167262B (en) | 1984-10-25 | 1985-10-25 | A position detecting device |
| US07/218,447 US4830498A (en) | 1984-10-25 | 1988-07-12 | Position detecting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9012885A JPS61247910A (en) | 1985-04-26 | 1985-04-26 | Distance measuring method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61247910A JPS61247910A (en) | 1986-11-05 |
| JPH0458884B2 true JPH0458884B2 (en) | 1992-09-18 |
Family
ID=13989867
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9012885A Granted JPS61247910A (en) | 1984-10-25 | 1985-04-26 | Distance measuring method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61247910A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0654231B2 (en) * | 1986-12-18 | 1994-07-20 | 株式会社ミツトヨ | Non-contact displacement meter |
-
1985
- 1985-04-26 JP JP9012885A patent/JPS61247910A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61247910A (en) | 1986-11-05 |
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