JPH05223533A - Height measuring apparatus - Google Patents

Height measuring apparatus

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Publication number
JPH05223533A
JPH05223533A JP963392A JP963392A JPH05223533A JP H05223533 A JPH05223533 A JP H05223533A JP 963392 A JP963392 A JP 963392A JP 963392 A JP963392 A JP 963392A JP H05223533 A JPH05223533 A JP H05223533A
Authority
JP
Japan
Prior art keywords
light
height
measured
glass substrate
laser
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
Application number
JP963392A
Other languages
Japanese (ja)
Other versions
JP2701639B2 (en
Inventor
Masao Kinoshita
雅夫 木下
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP963392A priority Critical patent/JP2701639B2/en
Publication of JPH05223533A publication Critical patent/JPH05223533A/en
Application granted granted Critical
Publication of JP2701639B2 publication Critical patent/JP2701639B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)
  • Measurement Of Optical Distance (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To obtain a height measuring apparatus which can measure the height of a lead correctly in the actual using state while a semiconductor device is mounted on a glass substrate. CONSTITUTION:Laser beams are scanned and condensed onto leads 21 of a semiconductor device 20 mounted on a glass substrate 25. The light reflected at each lead is condensed on a first-dimensional sensor 7 by a first and a second cylindrical lenses 6, 8, with forming an image at a position corresponding to the height of the lead. Nearly the whole of the regularly reflected light from the surface of the glass substrate 25 is cast onto a shielding plate 9. However, the regularly reflected light from an end part of scanning passes aside the shielding plate 9 and forms an image on the first-dimensional sensor 7 corresponding to the height of the upper surface of the glass substrate. The height of each lead from the glass substrate can be correctly measured by a detecting circuit 11 which obtains the height from signals corresponding to the position on the sensor 7 where the image is formed and a correcting circuit 12 which corrects the height using the height signal from the upper surface of the glass substrate as a reference.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、高さ測定装置に関し、
特に複数本のリードを有する半導体素子のリード高さ、
すなわち基準面からのリードの浮き量を測定する高さ測
定装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a height measuring device,
Especially, the lead height of a semiconductor device having a plurality of leads,
That is, the present invention relates to a height measuring device that measures the amount of lead floating from a reference surface.

【0002】[0002]

【従来の技術】図6は従来の高さ測定装置の一例を示す
斜視図であり、図7は図6に示す装置の動作説明図であ
る。
2. Description of the Related Art FIG. 6 is a perspective view showing an example of a conventional height measuring apparatus, and FIG. 7 is an operation explanatory view of the apparatus shown in FIG.

【0003】図6に示す高さ測定装置36は、レーザ3
1と、レーザ光32を半導体素子20のリード21に集
光する投光レンズ33と、リード21からの反射光を集
光する受光レンズ34と、受光レンズ34の結像点に配
置された1次元センサ35とを備えている。
The height measuring device 36 shown in FIG.
1, a light projecting lens 33 that collects the laser light 32 on the lead 21 of the semiconductor element 20, a light receiving lens 34 that collects the reflected light from the lead 21, and a light receiving lens 34 that is arranged at the image forming point of the light receiving lens 34. And a dimension sensor 35.

【0004】図7に示すようにリード21の高さが変化
すると、レーザ光32の反射点がA,B,Cと変化し、
また反射点A,B,Cの像は、受光レンズ34により1
次元センサ上にそれぞれA’,B’,C’の位置に結像
される。したがって、1次元センサ35上の結像点のず
れから、1本のリードの高さを求めることができる。
As shown in FIG. 7, when the height of the lead 21 changes, the reflection points of the laser light 32 change to A, B and C,
Also, the images of the reflection points A, B, and C are
Images are formed on the dimensional sensor at positions A ', B', and C ', respectively. Therefore, the height of one lead can be obtained from the deviation of the image formation point on the one-dimensional sensor 35.

【0005】また、半導体素子は平面基板上に置かれて
使用されることを考慮し、各リードの高さから基準面を
求め、その基準面からの各リードの高さを算出してい
た。
Further, in consideration of the fact that the semiconductor element is placed on a flat substrate for use, a reference plane is obtained from the height of each lead, and the height of each lead from the reference plane is calculated.

【0006】半導体素子20、または高さ測定装置36
を移動させることにより、リード21a,21b,21
c,21dというように各リードの高さを測定していく
ことができる。
The semiconductor element 20 or the height measuring device 36
By moving the leads 21a, 21b, 21
It is possible to measure the height of each lead like c and 21d.

【0007】[0007]

【発明が解決しようとする課題】上述した従来の高さ測
定装置では、半導体素子のパッケージ部を吸着等により
保持し、各リードはまったく拘束を受けない自由な状態
で、測定される。そのため、各リードの高さから基準面
を求め、さらにその基準面から実際の高さを求めてい
た。しかしながら、各リードの高さは、実使用状態、す
なわち、平面基板上に置かれた状態での平面基板からの
高さが重要であり、測定もこの状態で行う必要がある。
In the conventional height measuring device described above, the package portion of the semiconductor element is held by suction or the like, and each lead is measured in a free state without any constraint. Therefore, the reference plane is obtained from the height of each lead, and the actual height is obtained from the reference plane. However, it is important for the height of each lead to be in actual use, that is, the height from the flat substrate when placed on the flat substrate, and the measurement needs to be performed in this state.

【0008】従来の高さ測定装置を用いて実使用状態で
リード高さを測定しようとする場合、ガラス基板上に半
導体素子を載せ、下側からガラス基板を通して測定する
ことも考えられるが、ガラス表面での正反射光も受光レ
ンズを通して、1次元センサ上に結像されるため、正確
な高さを求めることができないという欠点があった。
When it is attempted to measure the lead height in a practical use state using a conventional height measuring device, it is conceivable that a semiconductor element is placed on a glass substrate and the glass substrate is measured from below. Since the specularly reflected light on the surface is also imaged on the one-dimensional sensor through the light receiving lens, there is a drawback that an accurate height cannot be obtained.

【0009】また、多数本のリードを有する半導体素子
のリード高さを測定する場合には、半導体素子または、
リード高さ検出装置自体を機械的に移動させて、1ポイ
ントずつ測定しなければならないので、ステージのよう
な移動機構が必要となり、1ポイントずつ機械的に移動
させる時間が必要となるため、トータルの測定に時間が
かかるという欠点があった。
When measuring the lead height of a semiconductor element having a large number of leads, the semiconductor element or
Since the lead height detection device itself must be mechanically moved to measure one point at a time, a moving mechanism such as a stage is required, and time to mechanically move one point at a time is required. There was a drawback that it took time to measure.

【0010】[0010]

【課題を解決するための手段】本発明の高さ測定装置
は、被測定物を載せる透明で平らなガラス基板と、レー
ザと、このレーザのレーザ光を一方向に回転走査するミ
ラーと、このミラーにより回転走査されるレーザ光を略
平行に走査集光するレンズとからなり、前記ガラス基板
の斜め下方から前記被測定物の被測定面にレーザ光を照
射する投光光学系と、前記被測定面に一方の焦点を有
し、レーザ光の走査方向に曲率を有する第1のシリンド
リカルレンズと、前記第1のシリンドリカルレンズの他
方の焦点の直前に配置され前記レーザ光の一部走査領域
を除き、前記ガラス基板の上面からの正反射光を遮断す
る遮光板と、この遮光板の直後に配置され前記一部走査
領域のガラス基板上面からの正反射光及び前記被測定面
からのレーザ光の乱反射光の前記遮光板の外側に広がっ
た部分を受光する1次元センサと、前記第1のシリンド
リカルレンズの曲率の方向と直交する曲率を有し前記被
測定面のレーザ光の反射点の像を前記1次元センサ上に
結像する第2のシリンドリカルレンズとからなる受光光
学系と、前記1次元センサの出力から被測定面の高さを
測定する高さ測定回路と、前記ガラス基板の上面からの
正反射光が前記遮光板により遮断されない領域における
前記1次元センサの出力値を基準値とする高さの補正回
路とを備えている。
A height measuring device of the present invention comprises a transparent and flat glass substrate on which an object to be measured is placed, a laser, and a mirror for rotationally scanning a laser beam of the laser in one direction. A projection optical system for irradiating a laser beam on a surface to be measured of the object to be measured from obliquely below the glass substrate, and A first cylindrical lens having one focus on the measurement surface and having a curvature in the scanning direction of the laser light, and a partial scanning region of the laser light arranged immediately before the other focus of the first cylindrical lens. Except for the light-shielding plate that blocks the specularly reflected light from the upper surface of the glass substrate, the specularly-reflected light from the glass substrate upper surface and the laser light from the surface to be measured in the partial scanning region disposed immediately after the light-shielding plate. Rebellion A one-dimensional sensor that receives a portion of the light that spreads outside the light shielding plate, and an image of a reflection point of the laser light on the measured surface that has a curvature that is orthogonal to the direction of the curvature of the first cylindrical lens. A light receiving optical system including a second cylindrical lens that forms an image on the one-dimensional sensor, a height measuring circuit that measures the height of the surface to be measured from the output of the one-dimensional sensor, and a height measuring circuit from the upper surface of the glass substrate. And a height correction circuit that uses an output value of the one-dimensional sensor as a reference value in a region where specular reflection light is not blocked by the light shielding plate.

【0011】本発明の高さ測定装置は、上面の一部に乱
反射物質が付着され被測定物を載せる透明で平らなガラ
ス基板と、レーザと、このレーザのレーザ光を一方向に
回転走査するミラーと、このミラーにより回転走査され
るレーザ光を略平行に走査集光するレンズとからなり、
前記ガラス基板の斜め下方から前記被測定物の被測定面
にレーザ光を照射する投光光学系と、前記被測定面に一
方の焦点を有し、レーザ光の走査方向に曲率を有する第
1のシリンドリカルレンズと、前記第1のシリンドリカ
ルレンズの他方の焦点に配置され前記ガラス基板の上面
からの正反射光を遮断する遮光板と、この遮光板の直後
に配置され前記被測定面及び前記乱反射物質からのレー
ザ光の乱反射光の前記遮光板の外側に広がった部分を受
光する1次元センサと、前記第1のシリンドリカルレン
ズの曲率の方向と直交する曲率を有し前記被測定面のレ
ーザ光の反射点の像を前記1次元センサ上に結像する第
2のシリンドリカルレンズとからなる受光光学系と、前
記1次元センサの出力から被測定面の高さを測定する高
さ測定回路と、前記乱反射物質からの1次元センサの出
力値を基準値とする高さ補正回路とを備えている。
The height measuring apparatus according to the present invention has a transparent flat glass substrate on which an object to be measured is placed, on which a diffusely reflecting substance is attached on a part of the upper surface thereof, a laser, and a laser beam of the laser is rotationally scanned in one direction. A mirror and a lens that scans and condenses the laser light that is rotationally scanned by the mirror in substantially parallel,
A projecting optical system that irradiates a measured surface of the measured object with laser light obliquely from below the glass substrate; and a first projection having one focus on the measured surface and having a curvature in a scanning direction of the laser light. Cylindrical lens, a light shielding plate arranged at the other focal point of the first cylindrical lens to block specularly reflected light from the upper surface of the glass substrate, and the measured surface and the irregular reflection arranged immediately after the light shielding plate. A one-dimensional sensor that receives the diffused light of the laser light from the substance that spreads to the outside of the light shielding plate, and a laser light having a curvature that is orthogonal to the curvature direction of the first cylindrical lens. A light receiving optical system including a second cylindrical lens for forming an image of the reflection point of the image on the one-dimensional sensor, and a height measuring circuit for measuring the height of the surface to be measured from the output of the one-dimensional sensor, Previous And a height compensation circuit as a reference value an output value of the one-dimensional sensor from diffuse reflection material.

【0012】[0012]

【実施例】次に、本発明の実施例について、図面を参照
して詳細に説明する。
Embodiments of the present invention will now be described in detail with reference to the drawings.

【0013】図1は本発明の一実施例を示す斜視図であ
る。図2,図3は図1に示す実施例の動作説明図であ
る。
FIG. 1 is a perspective view showing an embodiment of the present invention. 2 and 3 are operation explanatory diagrams of the embodiment shown in FIG.

【0014】図1に示す高さ測定装置は、被測定物であ
る半導体素子20を載せる透明で平らなガラス基板25
と、レーザ1と、レーザ光2を一方向に回転走査するガ
ルバノミラー3と、レーザ光2を略平行に走査集光する
テレセントリック系の投光レンズ4とからなり、ガラス
基板25の斜め下方から被測定面である半導体素子20
のリード21に斜めからレーザ光2を照射する投光光学
系5と、レーザ光2の被測定面からの反射光を受光し被
測定面に一方の焦点を有し、レーザ光の走査方向に曲率
を有する第1のシリンドリカルレンズ6と、第1のシリ
ンドリカルレンズ6の他方の焦点の直前に配置され、レ
ーザ光2の走査領域の端の一部を除き、ガラス基板25
の上面からの正反射光15を遮断する遮光板9と、遮光
板9の直後に配置され走査領域の端の一部におけるガラ
ス基板25の上面からの正反射光15及び、リード21
からの乱反射光16の遮光板9の外側に広がった部分を
受光する1次元センサ7と、第1のシリンドリカルレン
ズ6の曲率の方向と直交する曲率を有し、リード21の
反射点の像を1次元センサ7上に結像する第2のシリン
ドリカルレンズ8とからなる受光光学系10と、1次元
センサ7の出力からリード21の高さを測定する高さ測
定回路11と、ガラス基板25の上面からの正反射光1
5を受光した時の1次元センサ7の出力値を基準値とし
て高さ測定回路11の測定結果を補正する高さ補正回路
12とで構成される。高さ補正回路12は、基準値を入
れるメモリ部と、メモリ内のデータとの比較回路よりな
る。
The height measuring apparatus shown in FIG. 1 has a transparent and flat glass substrate 25 on which a semiconductor element 20 as an object to be measured is placed.
A laser 1, a galvano mirror 3 for rotating and scanning the laser light 2 in one direction, and a telecentric projection lens 4 for scanning and condensing the laser light 2 in a substantially parallel manner. Semiconductor element 20 which is the surface to be measured
The projection optical system 5 for irradiating the lead 21 with the laser light 2 obliquely, and the reflected light from the surface to be measured of the laser light 2 is received and has one focus on the surface to be measured. The first cylindrical lens 6 having a curvature and the glass substrate 25, which is arranged immediately in front of the other focus of the first cylindrical lens 6 except for a part of the end of the scanning region of the laser beam 2.
Of the specularly reflected light 15 from the upper surface of the glass substrate 25, the specularly reflected light 15 from the upper surface of the glass substrate 25 at a part of the end of the scanning region which is arranged immediately after the shading plate 9, and the leads 21.
The one-dimensional sensor 7 for receiving the portion of the diffused reflected light 16 from the outside of the light-shielding plate 9 and the curvature of the first cylindrical lens 6 that is orthogonal to the curvature direction, and the image of the reflection point of the lead 21 is formed. The light receiving optical system 10 including the second cylindrical lens 8 that forms an image on the one-dimensional sensor 7, the height measuring circuit 11 that measures the height of the lead 21 from the output of the one-dimensional sensor 7, and the glass substrate 25 Specular reflection light from the upper surface 1
The height correction circuit 12 corrects the measurement result of the height measurement circuit 11 with the output value of the one-dimensional sensor 7 when 5 is received as a reference value. The height correction circuit 12 is composed of a memory unit for storing a reference value and a comparison circuit for comparing the data in the memory.

【0015】次に、図2,図3を用いて本実施例の動作
を説明する。
Next, the operation of this embodiment will be described with reference to FIGS.

【0016】レーザ1から出射されたレーザ光2は、ガ
ルバノミラー3により一方向に回転走査されるが、テレ
セントリック系の投光レンズ4により略平行走査される
とともに、ガラス基板25上に保持された半導体素子2
0のリード21に集光照射される。このとき、レーザ光
2の一部はガラス基板25の表面で正反射される。ガラ
ス基板25を透過したレーザ光2は、リード21の表面
で反射されるが、リード21の表面は多少荒れているこ
とから乱反射も起こすため、ガラス基板25の表面での
正反射光15に比べ、リード21での反射光16のほう
がビームの広がり角が大きくなる。
The laser beam 2 emitted from the laser 1 is rotationally scanned in one direction by the galvanometer mirror 3, but is substantially parallel scanned by the projection lens 4 of the telecentric system and is held on the glass substrate 25. Semiconductor element 2
The lead 21 of 0 is focused and irradiated. At this time, part of the laser light 2 is specularly reflected by the surface of the glass substrate 25. The laser light 2 that has passed through the glass substrate 25 is reflected by the surface of the lead 21, but since the surface of the lead 21 is somewhat rough, diffuse reflection also occurs. The divergence angle of the beam is larger for the reflected light 16 on the leads 21.

【0017】以下、反射光について走査方向と、走査と
直角方向に分けて説明する。
The reflected light will be described below separately in the scanning direction and the direction perpendicular to the scanning.

【0018】まず走査方向についてのみ考えると、図2
に示すように第2のシリンドリカルレンズ8は、単なる
ガラス板と考えることができる。各走査位置におけるガ
ラス表面での正反射光15は、各光軸は略平行であり、
またある広がり角をもって拡散していくが、第1のシリ
ンドリカルレンズ6の働きにより、各正反射光15のビ
ームは略平行光となるとともに光軸は曲げられ、焦点の
位置に集まろうとする。遮光板9は、焦点の位置より前
に配置されているので走査領域の端で正反射した光1
5’の一部は遮光板9の横を抜けて1次元センサ7に照
射されるが、それ以外の走査領域での正反射光15は遮
光板9上に集められ、1次元センサ7上に照射されな
い。
First, considering only the scanning direction, FIG.
As shown in, the second cylindrical lens 8 can be considered as a simple glass plate. The specular reflection light 15 on the glass surface at each scanning position has its optical axes substantially parallel,
Further, although it diffuses with a certain divergence angle, the beam of each specularly reflected light 15 becomes substantially parallel light and the optical axis is bent by the action of the first cylindrical lens 6, and it tries to gather at the focal position. Since the light shielding plate 9 is arranged before the focal position, the light 1 specularly reflected at the edge of the scanning region 1
A part of 5 ′ passes through the light shielding plate 9 and is applied to the one-dimensional sensor 7. However, the specularly reflected light 15 in the other scanning region is collected on the light shielding plate 9 and is then projected onto the one-dimensional sensor 7. Not irradiated.

【0019】一方、リード21での乱反射光16は、ガ
ラス表面での正反射光15に比べビーム広がり角が大き
いため、第1のシリンドリカルレンズ6を透過した後の
ビーム径も大きくなり、遮光板9で一部が遮ぎられるも
のの、残りの部分が後方に配置された1次元センサ7上
に照射される(図2)。
On the other hand, since the diffused reflection light 16 on the lead 21 has a larger beam divergence angle than the regular reflection light 15 on the glass surface, the beam diameter after passing through the first cylindrical lens 6 also becomes large, and the light shield plate Although a part is blocked by 9, the remaining part is irradiated on the one-dimensional sensor 7 arranged in the rear (FIG. 2).

【0020】次に、走査と直角方向について考えると、
第1のシリンドリカルレンズ6は単なるガラス板と考え
ることができる。したがって、リード21上に集光され
たスポットが、第2のシリンドリカルレンズ8により、
1次元センサ7上に結像される。ここでリード21の高
さが変化すると1次元センサ7上の結像位置が変化し、
この変化は1次元センサ7により検出することができ
(図3)、リード21の高さを求めることができる。
Next, considering the direction perpendicular to the scanning,
The first cylindrical lens 6 can be considered as a simple glass plate. Therefore, the spot condensed on the lead 21 is changed by the second cylindrical lens 8.
An image is formed on the one-dimensional sensor 7. Here, if the height of the lead 21 changes, the image forming position on the one-dimensional sensor 7 changes,
This change can be detected by the one-dimensional sensor 7 (FIG. 3), and the height of the lead 21 can be obtained.

【0021】また、走査領域の端の部分では、ガラス基
板25の上面からの反射光15’が遮光板9の横を抜け
て、1次元センサ7に照射され、これによりガラス基板
25の上面の高さを求めることができる。また、ガラス
基板25の下面からの正反射光15は一般に測定範囲に
比べガラス基板25が厚いため、1次元センサ7の測定
範囲外に結像されるので無視できる。走査領域の端の部
分での1次元センサ7の出力値を高さ補正回路12の基
準値として取り込み、高さ検出回路11で得られた高さ
データをこの基準値で補正する。
At the end of the scanning area, the reflected light 15 'from the upper surface of the glass substrate 25 passes through the light shielding plate 9 and is applied to the one-dimensional sensor 7, whereby the upper surface of the glass substrate 25 is exposed. You can ask for height. Further, the specularly reflected light 15 from the lower surface of the glass substrate 25 is generally outside the measurement range of the one-dimensional sensor 7 because the glass substrate 25 is thicker than the measurement range and can be ignored. The output value of the one-dimensional sensor 7 at the end of the scanning area is taken in as a reference value of the height correction circuit 12, and the height data obtained by the height detection circuit 11 is corrected by this reference value.

【0022】以上のように、1組のシリンドリカルレン
ズと遮光板の働きにより、通常走査領域では、ガラス表
面の反射光を遮光し、リードでの反射光を効率よく1次
元センサ上に集めて、リード高さを測定するとともに、
走査領域の端では、ガラス上面での正反射光を、1次元
センサ上に集め、ガラス上面の高さを測定するので、ガ
ラス上面からのリードの高さを正確に測定することがで
きる。
As described above, due to the function of the pair of cylindrical lenses and the light blocking plate, in the normal scanning area, the reflected light from the glass surface is blocked and the reflected light from the leads is efficiently collected on the one-dimensional sensor. While measuring the lead height,
At the end of the scanning region, specular reflection light on the glass upper surface is collected on the one-dimensional sensor and the height of the glass upper surface is measured, so that the height of the lead from the glass upper surface can be accurately measured.

【0023】また、ガルバノミラーでレーザ光を高速に
走査するとともに、その反射光を1次元センサ上に集め
ることができるので、各リードの高さを高速に測定する
ことができる。
Further, since the laser beam can be scanned at high speed by the galvano mirror and the reflected light can be collected on the one-dimensional sensor, the height of each lead can be measured at high speed.

【0024】図4は本発明の他の実施例を示す斜視図で
ある。図5は図4に示す実施例の動作説明図である。
FIG. 4 is a perspective view showing another embodiment of the present invention. FIG. 5 is an operation explanatory diagram of the embodiment shown in FIG.

【0025】図4において投光光学系5は図1に示すも
のと同一である。被測定物である半導体素子20を載せ
る透明で平らなガラス基板25の上面の周辺部は乱反射
物質26が付着されている。受光光学系10はレーザ光
2の被測定面からの反射光を受光し被測定面に一方の焦
点を有し、レーザ光の走査方向に曲率を有する第1のシ
リンドリカルレンズ6と、第1のシリンドリカルレンズ
6の他方の焦点に配置され、ガラス基板25の上面から
の正反射光15を遮断する遮光板9と、遮光板9の直後
に配置し、リード21及び乱反射物質26からの乱反射
光16,16’の遮光板9の外側に広がった部分を受光
する1次元センサ7と、第1のシリンドリカルレンズ6
の曲率の方向と直交する曲率を有し、リード21及び乱
反射物質26の反射点の像を1次元センサ7上に結像す
る第2のシリンドリカルレンズ8とからなる。高さ測定
回路11は1次元センサ7の出力からリードの高さ及び
乱反射物質の高さを測定する。高さ補正回路12は乱反
射物質26の高さすなわちガラス基板25の上面の高さ
を基準値としてリードの高さを補正する。高さ補正回路
12は、基準値を入れるメモリ部と、メモリ内のデータ
との比較回路よりなる。
In FIG. 4, the projection optical system 5 is the same as that shown in FIG. A diffuse reflection material 26 is attached to the peripheral portion of the upper surface of a transparent and flat glass substrate 25 on which the semiconductor element 20 as the object to be measured is placed. The light receiving optical system 10 receives the reflected light of the laser light 2 from the surface to be measured, has one focus on the surface to be measured, and has a first cylindrical lens 6 having a curvature in the scanning direction of the laser light; A light shielding plate 9 arranged at the other focal point of the cylindrical lens 6 and blocking the specularly reflected light 15 from the upper surface of the glass substrate 25, and a light shielding plate 9 arranged immediately after the light shielding plate 9 to diffusely reflect light 16 from the lead 21 and the irregular reflection substance 26. , 16 'of the one-dimensional sensor 7 for receiving the portion of the light-shielding plate 9 spread outside the light-shielding plate 9, and the first cylindrical lens 6
The second cylindrical lens 8 has a curvature that is orthogonal to the direction of the curvature of, and forms an image of the reflection point of the lead 21 and the diffuse reflection material 26 on the one-dimensional sensor 7. The height measuring circuit 11 measures the height of the lead and the height of the diffuse reflection material from the output of the one-dimensional sensor 7. The height correction circuit 12 corrects the height of the lead with the height of the diffuse reflection material 26, that is, the height of the upper surface of the glass substrate 25 as a reference value. The height correction circuit 12 is composed of a memory unit for storing a reference value and a comparison circuit for comparing the data in the memory.

【0026】次に図5を用いて本実施例の動作を説明す
る。
Next, the operation of this embodiment will be described with reference to FIG.

【0027】まず走査方向についてのみ考えると、図5
に示すように第2のシリンドリカルレンズ8は、単なる
ガラス板と考えることができる。各走査位置におけるガ
ラス表面での正反射光15は、各光軸は略平行であり、
またある広がり角をもって拡散していくが、第1のシリ
ンドリカルレンズ6の働きにより、各正反射光15のビ
ームは略平行光となるとともに光軸は曲げられ、焦点の
位置に集まる。遮光板9は、焦点の位置に配置されてい
るので正反射光15は、遮光板9上に集められ、1次元
センサ7上に照射されない。
First, considering only the scanning direction, FIG.
As shown in, the second cylindrical lens 8 can be considered as a simple glass plate. The specular reflection light 15 on the glass surface at each scanning position has its optical axes substantially parallel,
Although it diffuses with a certain divergence angle, the beam of each specularly reflected light 15 becomes substantially parallel light and the optical axis is bent by the action of the first cylindrical lens 6, and the beams are gathered at the focal position. Since the light shielding plate 9 is arranged at the focal position, the specularly reflected light 15 is collected on the light shielding plate 9 and is not irradiated onto the one-dimensional sensor 7.

【0028】一方、リード21及び乱反射物質26での
乱反射光16,16’は、ガラス表面での正反射光15
に比べビーム広がり角が大きいため、第1のシリンドリ
カルレンズ6を通過した後のビーム径も大きくなり、遮
光板9で一部が遮ぎられるものの、後方に配置された1
次元センサ7上に照射される。(図5)。
On the other hand, the diffusely reflected light 16 and 16 'from the lead 21 and the diffusely reflective material 26 are specularly reflected light 15 from the glass surface.
Since the beam divergence angle is larger than that of, the beam diameter after passing through the first cylindrical lens 6 is also large, and although part of the beam is blocked by the light blocking plate 9, it is arranged at the rear.
It is irradiated onto the dimension sensor 7. (Fig. 5).

【0029】次に、走査と直角方向について考えると、
図3に示したのと同様に第1のシリンドリカルレンズ6
は単なるガラス板と考えることができる。したがって、
リード21上に集光されたスポットが、第2のシリンド
リカルレンズ8により、1次元センサ7上に結像され
る。ここでリード21の高さが変化すると1次元センサ
7上の結像位置が変化し、この変化は1次元センサ7に
より検出することができ、リード21の高さを求めるこ
とができる。同様に、乱反射物質26の高さ、すなわち
ガラス基板25の上面の高さを検出することができる。
この時の1次元センサ7の出力値を高さ補正回路12の
基準値として取り込み、高さ検出回路11で得られた高
さデータと比較し補正する。
Next, considering the direction perpendicular to the scanning,
The first cylindrical lens 6 is the same as that shown in FIG.
Can be thought of as just a glass plate. Therefore,
The spot condensed on the lead 21 is imaged on the one-dimensional sensor 7 by the second cylindrical lens 8. Here, if the height of the lead 21 changes, the imaging position on the one-dimensional sensor 7 changes, and this change can be detected by the one-dimensional sensor 7, and the height of the lead 21 can be obtained. Similarly, the height of the diffuse reflection material 26, that is, the height of the upper surface of the glass substrate 25 can be detected.
The output value of the one-dimensional sensor 7 at this time is taken in as a reference value of the height correction circuit 12, and the height data obtained by the height detection circuit 11 is compared and corrected.

【0030】上記乱反射物質26は、ガラス基板表面に
塗料等を塗ることで簡単に設けられる。
The diffuse reflection material 26 is easily provided by applying a paint or the like on the surface of the glass substrate.

【0031】以上のように、1組のシリンドリカルレン
ズと遮光板の働きにより、ガラス表面の反射光を遮光
し、リードでの反射光を効率よく1次元センサ上に集め
てリード高さを測定するとともに、走査領域の端では、
ガラス上面に設けた乱反射物質によりガラス上面の高さ
を測定することができるので、ガラス上面からのリード
の高さを正確に測定することができる。
As described above, the function of the pair of cylindrical lenses and the light blocking plate blocks the reflected light from the glass surface, and the reflected light from the leads is efficiently collected on the one-dimensional sensor to measure the lead height. At the end of the scan area,
Since the height of the glass upper surface can be measured by the diffuse reflection material provided on the glass upper surface, the height of the lead from the glass upper surface can be accurately measured.

【0032】[0032]

【発明の効果】本発明の高さ測定装置は、多数本のリー
ド高さを測定するのに被測定物または、測定装置をステ
ージにのせ、機械的に移動させる代りに、レーザ光を高
速に走査し、各リードに照射するとともに、1組のシリ
ンドリカルレンズと遮光板の働きにより、半導体素子を
載せるガラス表面での正反射光を遮光し、かつ、各リー
ドからの反射光を効率よくセンサ上に集めることによ
り、リード高さを測定できるとともに、走査領域の端で
は、ガラス上面での正反射光または乱反射物質からの乱
反射光によりガラス上面の高さを測定できるので半導体
素子をガラス基板上に搭載した実使用状態にて、各リー
ドのガラス基板からの高さを正確にまた高速に測定でき
るという効果がある。
According to the height measuring apparatus of the present invention, instead of placing the object to be measured or the measuring apparatus on the stage and mechanically moving it in order to measure the heights of a large number of leads, the laser light is emitted at high speed. While scanning and irradiating each lead, a set of cylindrical lenses and a light blocking plate work to block the specularly reflected light from the glass surface on which the semiconductor element is mounted and to efficiently reflect the reflected light from each lead on the sensor. The lead height can be measured by collecting the light on the glass substrate at the edge of the scanning area, and the height of the glass upper surface can be measured by specular reflection light on the glass top surface or diffuse reflection light from the diffuse reflection material. The effect is that the height of each lead from the glass substrate can be measured accurately and at high speed in the mounted actual use state.

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

【図1】本発明の一実施例を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of the present invention.

【図2】図1に示す実施例の動作を説明するための走査
方向の面上の光路を示す図である。
FIG. 2 is a diagram showing an optical path on a surface in the scanning direction for explaining the operation of the embodiment shown in FIG.

【図3】図1に示す実施例の動作を説明するための走査
と直角方向の面上の光路を示す図である。
FIG. 3 is a diagram showing an optical path on a surface in a direction perpendicular to scanning for explaining the operation of the embodiment shown in FIG.

【図4】本発明の他の実施例を示す図である。FIG. 4 is a diagram showing another embodiment of the present invention.

【図5】図4に示す実施例の動作を説明する図である。FIG. 5 is a diagram for explaining the operation of the embodiment shown in FIG.

【図6】従来の高さ測定装置を示す斜視図である。FIG. 6 is a perspective view showing a conventional height measuring device.

【図7】図6に示す従来の高さ測定装置の動作を説明す
る図である。
FIG. 7 is a diagram for explaining the operation of the conventional height measuring device shown in FIG.

【符号の説明】[Explanation of symbols]

1,31 レーザ 2,32 レーザ光 3 ガルバノミラー 4,33 投光レンズ 5 投光光学系 6 第1のシリンドリカルレンズ 7,35 1次元センサ 8 第2のシリンドリカルレンズ 9 遮光板 10 受光光学系 11 高さ測定回路 12 高さ補正回路 15 ガラス表面での正反射光 16 リードでの反射光 16’ 乱反射物質での反射光 20 半導体素子 21 リード 25 ガラス基板 26 乱反射物質 1,31 laser 2,32 laser light 3 galvano mirror 4,33 light projecting lens 5 light projecting optical system 6 first cylindrical lens 7,35 one-dimensional sensor 8 second cylindrical lens 9 light shielding plate 10 light receiving optical system 11 high Measurement circuit 12 Height correction circuit 15 Regularly reflected light on the glass surface 16 Reflected light from the lead 16 'Reflected light from the diffusely-reflecting substance 20 Semiconductor element 21 Lead 25 Glass substrate 26 Diffuse-reflecting substance

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 被測定物を載せる透明で平らなガラス基
板と、 レーザと、このレーザのレーザ光を一方向に回転走査す
るミラーと、このミラーにより回転走査されるレーザ光
を略平行に走査集光するレンズとからなり、前記ガラス
基板の斜め下方から前記被測定物の被測定面にレーザ光
を照射する投光光学系と、 前記被測定面に一方の焦点を有し、レーザ光の走査方向
に曲率を有する第1のシリンドリカルレンズと、前記第
1のシリンドリカルレンズの他方の焦点の直前に配置さ
れ前記レーザ光の一部走査領域を除き、前記ガラス基板
の上面からの正反射光を遮断する遮光板と、この遮光板
の直後に配置され前記一部走査領域のガラス基板上面か
らの正反射光及び前記被測定面からのレーザ光の乱反射
光の前記遮光板の外側に広がった部分を受光する1次元
センサと、前記第1のシリンドリカルレンズの曲率の方
向と直交する曲率を有し前記被測定面のレーザ光の反射
点の像を前記1次元センサ上に結像する第2のシリンド
リカルレンズとからなる受光光学系と、 前記1次元センサの出力から被測定面の高さを測定する
高さ測定回路と、前記ガラス基板の上面からの正反射光
が前記遮光板により遮断されない領域における前記1次
元センサの出力値を基準値とする高さの補正回路とを備
えたことを特徴とする高さ測定装置。
1. A transparent and flat glass substrate on which an object to be measured is placed, a laser, a mirror for rotationally scanning a laser beam of this laser in one direction, and a laser beam rotationally scanned by this mirror is scanned substantially in parallel. A condensing lens, a projection optical system for irradiating the measured surface of the object to be measured with laser light from obliquely below the glass substrate, and the measured surface having one focus, A first cylindrical lens having a curvature in the scanning direction, and a specular reflection light from the upper surface of the glass substrate, except for a partial scanning region of the laser light, which is arranged immediately before the other focal point of the first cylindrical lens. A light-blocking plate for blocking, and a part of the specularly-reflected light from the upper surface of the glass substrate in the partial scanning region, which is arranged immediately after the light-blocking plate, and the diffused light of the laser beam from the surface to be measured, which spreads outside the light-blocking plate To A one-dimensional sensor that emits light and a second cylindrical lens that has a curvature orthogonal to the direction of curvature of the first cylindrical lens and forms an image of a reflection point of the laser light on the surface to be measured on the one-dimensional sensor. A light receiving optical system including a lens, a height measuring circuit that measures the height of the surface to be measured from the output of the one-dimensional sensor, and a region in which regular reflection light from the upper surface of the glass substrate is not blocked by the light shielding plate. A height measuring device comprising a height correction circuit using an output value of the one-dimensional sensor as a reference value.
【請求項2】 上面の一部に乱反射物質が付着され被測
定物を載せる透明で平らなガラス基板と、 レーザと、このレーザのレーザ光を一方向に回転走査す
るミラーと、このミラーにより回転走査されるレーザ光
を略平行に走査集光するレンズとからなり、前記ガラス
基板の斜め下方から前記被測定物の被測定面にレーザ光
を照射する投光光学系と、 前記被測定面に一方の焦点を有し、レーザ光の走査方向
に曲率を有する第1のシリンドリカルレンズと、前記第
1のシリンドリカルレンズの他方の焦点に配置され前記
ガラス基板の上面からの正反射光を遮断する遮光板と、
この遮光板の直後に配置され前記被測定面及び前記乱反
射物質からのレーザ光の乱反射光の前記遮光板の外側に
広がった部分を受光する1次元センサと、前記第1のシ
リンドリカルレンズの曲率の方向と直交する曲率を有し
前記被測定面のレーザ光の反射点の像を前記1次元セン
サ上に結像する第2のシリンドリカルレンズとからなる
受光光学系と、 前記1次元センサの出力から被測定面の高さを測定する
高さ測定回路と、前記乱反射物質からの1次元センサの
出力値を基準値とする高さ補正回路とを備えたことを特
徴とする高さ測定装置。
2. A transparent and flat glass substrate on which an object to be measured is placed, with a diffusely reflecting substance attached to a part of its upper surface, a laser, a mirror for rotationally scanning the laser light of this laser in one direction, and rotation by this mirror. A projection optical system configured to irradiate a laser beam onto a measured surface of the object to be measured from obliquely below the glass substrate, and a lens to condense the scanned laser light in a substantially parallel manner, and to the measured surface. A first cylindrical lens having one focus and having a curvature in the scanning direction of the laser light, and a light shield arranged at the other focus of the first cylindrical lens to block specular reflection light from the upper surface of the glass substrate. A board,
A one-dimensional sensor disposed immediately after the light shield plate for receiving the portion of the diffused reflected light of the laser light from the surface to be measured and the irregular reflection material that spreads outside the light shield plate, and the curvature of the first cylindrical lens. From the output of the one-dimensional sensor, a light receiving optical system including a second cylindrical lens that has a curvature orthogonal to the direction and forms an image of the reflection point of the laser light on the measured surface on the one-dimensional sensor. A height measuring device comprising: a height measuring circuit for measuring the height of a surface to be measured; and a height correcting circuit using an output value of a one-dimensional sensor from the diffuse reflection material as a reference value.
JP963392A 1992-01-23 1992-01-23 Height measuring device Expired - Lifetime JP2701639B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP963392A JP2701639B2 (en) 1992-01-23 1992-01-23 Height measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP963392A JP2701639B2 (en) 1992-01-23 1992-01-23 Height measuring device

Publications (2)

Publication Number Publication Date
JPH05223533A true JPH05223533A (en) 1993-08-31
JP2701639B2 JP2701639B2 (en) 1998-01-21

Family

ID=11725644

Family Applications (1)

Application Number Title Priority Date Filing Date
JP963392A Expired - Lifetime JP2701639B2 (en) 1992-01-23 1992-01-23 Height measuring device

Country Status (1)

Country Link
JP (1) JP2701639B2 (en)

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