JP3266217B2 - Liquid crystal substrate foreign matter inspection device - Google Patents

Liquid crystal substrate foreign matter inspection device

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Publication number
JP3266217B2
JP3266217B2 JP17113393A JP17113393A JP3266217B2 JP 3266217 B2 JP3266217 B2 JP 3266217B2 JP 17113393 A JP17113393 A JP 17113393A JP 17113393 A JP17113393 A JP 17113393A JP 3266217 B2 JP3266217 B2 JP 3266217B2
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JP
Japan
Prior art keywords
foreign matter
scattered light
liquid crystal
crystal substrate
substrate
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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 - Fee Related
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JP17113393A
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Japanese (ja)
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JPH075407A (en
Inventor
秀一 近松
Original Assignee
日立電子エンジニアリング株式会社
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】この発明は、液晶基板の異物検査
装置に関し、詳しくは、TFT(薄膜トランジスタ)を
有するアクディブマトリックスLCDの基板の異物検査
において、異物を有効に検出できるような異物検査装置
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a foreign substance inspection apparatus for a liquid crystal substrate, and more particularly to a foreign substance inspection apparatus capable of effectively detecting a foreign substance in a foreign substance inspection of a substrate of an active matrix LCD having a TFT (thin film transistor). .

【0002】[0002]

【従来の技術】アクディブマトリックスLCDの基板に
は、半導体ウエハと同様にTFTや透明電極の微細パタ
ーンが表面に形成される。また、カラー液晶基板(LC
D基板)の場合には、さらに微細なフィルタパターンが
形成される。これら基板の表面上に付着した異物は、品
質を劣化させたり、TFTや配向膜を破損させて画素不
良の原因になる。したがって、半導体ウエハの場合と同
様に異物が問題にされ、液晶基板の製造過程の各工程で
検査する必要になる。半導体ウエハの異物検査装置は、
種々のものあり、その技術はより微細な異物を検出する
方向にあるが、液晶基板の異物検査装置は、まだ手探り
状態であって、液晶基板専用の検査方法が技術として明
確に確立されているわけではない。
2. Description of the Related Art On a substrate of an active matrix LCD, fine patterns of TFTs and transparent electrodes are formed on the surface similarly to a semiconductor wafer. In addition, color liquid crystal substrates (LC
D substrate), a finer filter pattern is formed. Foreign matter adhering to the surface of these substrates deteriorates the quality and damages the TFT and the alignment film, causing pixel defects. Therefore, as in the case of a semiconductor wafer, foreign matter is regarded as a problem, and it is necessary to inspect each step in the process of manufacturing a liquid crystal substrate. Semiconductor wafer foreign matter inspection equipment
There are various types, and the technology is in the direction of detecting finer foreign matter, but the foreign matter inspection device for the liquid crystal substrate is still groping, and the inspection method dedicated to the liquid crystal substrate is clearly established as a technology. Do not mean.

【0003】[0003]

【発明が解決しようとする課題】そこで、ウエハ異物検
査装置の技術がそのまま液晶基板の異物検査に利用でき
ることが望ましいが、実際に形成されるパターンが相違
するのでそう簡単なものではない。ウエハ異物検査装置
の技術としては、ウエハの表面に対してレーザビームを
照射し、異物が散乱させる散乱光を受光して異物を検出
し、この検出信号を適当な処理回路により処理して得ら
れる異物データをディスプレイ装置にマップ表示する。
これを液晶基板の異物検査装置として実際に使用してみ
ると、ウエハの異物検査装置のような異物検出感度が得
られないことが分かった。
Therefore, it is desirable that the technique of the wafer foreign substance inspection apparatus can be used as it is for the foreign substance inspection of the liquid crystal substrate, but it is not so simple because the actually formed pattern is different. As a technique of a wafer foreign matter inspection apparatus, a laser beam is irradiated on the surface of a wafer, scattered light scattered by the foreign matter is received, foreign matter is detected, and the detection signal is processed by an appropriate processing circuit. Foreign matter data is displayed on a map on a display device.
When this was actually used as a foreign substance inspection apparatus for a liquid crystal substrate, it was found that foreign substance detection sensitivity could not be obtained as in a foreign substance inspection apparatus for a wafer.

【0004】その理由として考えられることは、TFT
のパターンは、ウエハに形成されるLSIのパターンに
比べて膜厚が厚く、段差が大きいこと。LSIのパター
ンに比べて形成されるパターンのエッジが粗いこと。T
FTのパターンが形成されていない透明電極膜(ITO
膜,インジュウムすず酸化電極膜)が大きな領域で存在
し、ここでの反射率が低いこと。などである。すなわ
ち、異物は、それが置かれたバックグランドの反射率が
高いほどその散乱光も大きくなるが、ITO膜の反射率
は低く、ここに存在する異物は、その散乱光のレベルが
比較的低い。これに対してTFT側は、ITO膜の30
倍以上もの反射率がある。そこで、TFT上の異物の散
乱光は大きい。また、TFTのパターンの角の部分で散
乱した場合、特に、TFTパターンのうちAl配線の角
の部分で散乱した場合、その散乱光のレベルは、異物よ
りも高くなる。ITO膜の角部分の散乱も段差が大き
く、そのレベルは、この領域にある異物より高い。異物
検出の範囲は、TFTの形成領域とITO膜の領域の双
方を含むことになるが、ITO膜に異物が存在していて
もITO膜の角部分やTFTの形成領域の角の部分から
の散乱光が大きく、特にTFTの角ではITO膜状の異
物の10倍以上もある。このようなことからITO膜上
の異物を検出する適切な感度の選択ができない。また、
TFT領域状の異物もその角部分からの散乱が大きいの
で、これも検出することが難しい。液晶基板では、高い
段差の矩形状のパターンが基本となり、それが多数配列
されることから角部分が多く存在しかつそこでの散乱が
多く、この散乱光を除く、簡単で有効な手段が現在のと
ころみい出せない。
[0004] The possible reason is that TFT
Is thicker and has a larger step than the LSI pattern formed on the wafer. The edge of a pattern formed is coarser than that of an LSI pattern. T
A transparent electrode film on which no FT pattern is formed (ITO
Film, indium tin oxide electrode film) exists in a large area, and the reflectivity is low here. And so on. That is, the higher the reflectivity of the background on which the foreign matter is placed, the higher the scattered light, but the reflectivity of the ITO film is low, and the foreign matter present here has a relatively low level of the scattered light. . On the other hand, on the TFT side, the 30
There are more than twice the reflectance. Therefore, the scattered light of the foreign matter on the TFT is large. Further, when the light is scattered at the corners of the TFT pattern, particularly when the light is scattered at the corners of the Al wiring in the TFT pattern, the level of the scattered light is higher than that of the foreign matter. The scattering at the corners of the ITO film also has a large step, and its level is higher than that of the foreign matter in this region. The range of foreign matter detection includes both the TFT formation region and the ITO film region. Even if foreign matter is present in the ITO film, the range from the corner of the ITO film or the corner of the TFT formation region is large. The scattered light is large, especially at the corner of the TFT, which is 10 times or more that of the foreign matter in the form of an ITO film. For this reason, it is not possible to select an appropriate sensitivity for detecting foreign matter on the ITO film. Also,
The foreign matter in the TFT area also has a large scattering from the corners, and thus it is difficult to detect the foreign matter. In liquid crystal substrates, a rectangular pattern with a high step is basically used, and since many patterns are arranged, there are many corners and there is a lot of scattering there, and a simple and effective means for removing this scattered light is presently available. I can't find it.

【0005】しかし、あらたに液晶基板の異物検査につ
いて装置を開発するには時間と費用がかかるので、でき
るだけ従来からあるウエハ異物検査装置の技術を利用し
て液晶基板の異物検査を行うことが望ましい。この発明
は、前記のような従来技術の欠点を解決するものであっ
て、段差の大きな矩形状のパターンを多数有し、照射光
に対して強い散乱がパターンの角部分で発生する液晶基
板について散乱光で異物を検出する液晶基板の異物検査
装置を提供することを目的とする。
However, it takes time and expense to develop a new apparatus for inspecting foreign substances on a liquid crystal substrate. Therefore, it is desirable to inspect foreign substances on a liquid crystal substrate by using a conventional technique for inspecting foreign substances on a wafer as much as possible. . The present invention solves the above-mentioned drawbacks of the prior art, and relates to a liquid crystal substrate having a large number of rectangular patterns having large steps and in which strong scattering with respect to irradiation light occurs at corners of the pattern. An object of the present invention is to provide a foreign substance inspection device for a liquid crystal substrate which detects a foreign substance by scattered light.

【0006】[0006]

【課題を解決するための手段】このような目的を達成す
るためのこの発明の液晶基板の異物検査装置の特徴は、
基板上に形成された矩形状のパターンの1つの辺に対し
て水平面に投影した照射角がほぼ45度になる状態で対
向させて互いに異なる波長の2本のレーザ光をほぼ等し
い仰角で斜めに照射して照射点の上方でそれぞれの散乱
光を受光し、それぞれの散乱光を分離してセンサで検出
し、それぞれの検出レベルがほぼ等しいときに異物と判
定するものである。
The object of the present invention for achieving the above object is as follows.
Two laser beams of different wavelengths are obliquely tilted at substantially the same elevation angle with one side of a rectangular pattern formed on the substrate facing each other in a state where the irradiation angle projected on the horizontal plane is approximately 45 degrees. Irradiation receives each scattered light above the irradiation point, separates each scattered light and detects it with a sensor. When the respective detection levels are substantially equal, it is determined that a foreign substance exists.

【0007】[0007]

【作用】このように、ほぼ45度の等しい角度で対向さ
せて2本のレーザビームを照射した場合、2本のレーザ
ビームを受けた異物の前方散乱はほぼ等しいので、照射
点上方の散乱光はほぼ等しくなるが、パターンの角の部
分では、2本のレーザビームのうち一方は、直角に当た
り、他方は、平行に近い形になるので、直角に当たった
方のレーザビームの前方散乱光は大きいが、平行に当た
った方のレーザビームの前方散乱光は小さい。したがっ
て、これらに差が生じ、これらの散乱光のレベルは等し
くはならない。ITO膜の領域とTFT領域とでは散乱
光のレベルに相違があるが、以上の関係は、ITO膜で
もTFT領域でも同じである。これによりITO膜の領
域でも、TFT領域でも異物とパターンとを分けて検出
することができる。
As described above, when two laser beams are irradiated while facing each other at an equal angle of approximately 45 degrees, the forward scattering of the foreign matter that has received the two laser beams is substantially equal, so the scattered light above the irradiation point is obtained. Are approximately equal, but at the corners of the pattern, one of the two laser beams hits a right angle and the other is nearly parallel, so the forward scattered light of the right-angled laser beam is Although it is large, the forward scattered light of the laser beam hit in parallel is small. Thus, there is a difference between them, and their scattered light levels are not equal. Although there is a difference in the level of scattered light between the ITO film region and the TFT region, the above relationship is the same for both the ITO film and the TFT region. Thus, the foreign matter and the pattern can be detected separately in both the ITO film region and the TFT region.

【0008】[0008]

【実施例】図1は、この発明の一実施例の液晶基板の異
物検査装置を適用した検査装置の構成図、図2はその検
出原理の説明図である。図1において、1は、LCD基
板であって、このLCD基板1に対して2つのレーザビ
ームの照射系2,3が斜めから対向するように設けられ
ている。照射系2は、レーザダイオード(LD)2aと
集束レンズ2b、ミラー2cからなり、LCD基板1の
表面を基準として仰角35度でかつ基板(XY平面)上
へ投影したときのX軸(正方向の軸)となす角が45度
となる波長λ1 のレーザビームをLCD基板1上の検査
点Pに照射する。照射系3は、レーザダイオード(L
D)3aと集束レンズ3b、ミラー3cからなり、同様
に仰角35度角度でかつ基板(XY平面)上へ投影した
ときのX軸(正方向の軸)となす角が135度となる波
長λ2 のレーザビームを検査点Pに照射する。したがっ
て、基板(XY平面)上へ投影したときの照射系2と3
のレーザビームは、Y軸(正方向の軸)に対して45度
の角度で両側に配置され対向する。なお、X軸,Y軸
は、LCD基板1の横の辺と縦の辺にそれぞれ対応して
いる。
FIG. 1 is a block diagram of an inspection apparatus to which a foreign substance inspection apparatus for a liquid crystal substrate according to one embodiment of the present invention is applied, and FIG. 2 is an explanatory diagram of the detection principle. In FIG. 1, reference numeral 1 denotes an LCD substrate, on which two laser beam irradiation systems 2 and 3 are provided so as to be obliquely opposed to the LCD substrate 1. The irradiation system 2 includes a laser diode (LD) 2a, a focusing lens 2b, and a mirror 2c, and has an elevation angle of 35 degrees with respect to the surface of the LCD substrate 1 and an X-axis (positive direction) when projected onto the substrate (XY plane). An inspection point P on the LCD substrate 1 is irradiated with a laser beam having a wavelength λ 1 at an angle of 45 ° to the inspection point P. The irradiation system 3 includes a laser diode (L
D) A wavelength λ that is composed of 3a, a focusing lens 3b, and a mirror 3c, and has an elevation angle of 35 degrees and an angle of 135 degrees with the X axis (positive axis) when projected onto a substrate (XY plane). The inspection point P is irradiated with the second laser beam. Therefore, irradiation systems 2 and 3 when projected onto a substrate (XY plane)
Are arranged on both sides at an angle of 45 degrees with respect to the Y axis (positive axis) and face each other. The X axis and the Y axis correspond to the horizontal side and the vertical side of the LCD substrate 1, respectively.

【0009】4は、検査点Pの上部に配置された対物光
学系であり、対物レンズ4aと集束レンズ4b、ミラー
4c、スリット4d、レンズ4e、ダイクロイックミラ
ー4f、CCD等の光電変換センサ4g,4hで構成さ
れる。ダイクロイックミラー4fは、波長λ1 とλ2
を分離し、照射系2に対応する波長λ1 の散乱光をセン
サ4gに送り、照射系3に対応する波長λ2 の散乱光を
センサ4hに送り出す。5は、顕微鏡観測光学系であ
り、点線で示すミラー5a、レンズ5b,5c、ミラー
5d,5e、観測光学器5fからなり、必要に応じて対
物光学系4の光路にミラー5aが挿入され、さらに点線
で示す光学系が挿入される。
Reference numeral 4 denotes an objective optical system disposed above the inspection point P. The objective lens 4a, the focusing lens 4b, the mirror 4c, the slit 4d, the lens 4e, the dichroic mirror 4f, a photoelectric conversion sensor 4g such as a CCD, and the like. 4h. The dichroic mirror 4f separates the wavelengths λ 1 and λ 2 , sends the scattered light of the wavelength λ 1 corresponding to the irradiation system 2 to the sensor 4g, and sends the scattered light of the wavelength λ 2 corresponding to the irradiation system 3 to the sensor 4h. Send out. Reference numeral 5 denotes a microscope observation optical system, which includes a mirror 5a indicated by a dotted line, lenses 5b and 5c, mirrors 5d and 5e, and an observation optical device 5f. The mirror 5a is inserted into the optical path of the objective optical system 4 as necessary. Further, an optical system indicated by a dotted line is inserted.

【0010】6は、検出回路であって、センサ4gから
の検出信号を受けて所定の閾値THa 以上の信号を増幅
するアンプ(AMP)6aと、センサ4hから検出信号
を受けて所定の閾値THb 以上の信号を増幅するアンプ
(AMP)6b、これらアンプの出力を受けてアンプ6
aの値をアンプ6bの値で割る割算回路6c、そして割
算回路6cの出力を受けて異物か否かを判定する異物判
定回路6dとからなる。なお、それぞれの閾値THa ,
THb のレベル調整は可能である。また、異物判定回路
6dは、アナログのレベル判定回路あるいはA/D変換
回路と判定プログラムを有するマイクロプロセッサ等で
構成されていてもよい。
Reference numeral 6 denotes a detection circuit, which is an amplifier (AMP) 6a for receiving a detection signal from the sensor 4g and amplifying a signal equal to or higher than a predetermined threshold THa, and a predetermined threshold THb for receiving a detection signal from the sensor 4h. An amplifier (AMP) 6b for amplifying the above signals, and an amplifier 6
It comprises a dividing circuit 6c for dividing the value of a by the value of the amplifier 6b, and a foreign matter determining circuit 6d which receives the output of the dividing circuit 6c and determines whether or not the foreign matter exists. Note that each of the threshold values THa,
THb level adjustment is possible. Further, the foreign matter determination circuit 6d may be constituted by an analog level determination circuit or an A / D conversion circuit and a microprocessor having a determination program.

【0011】次に図2を参照してこの発明の検出原理を
説明する。LCD基板1上に形成されたパターンは、矩
形の基板の各辺に対応して表示のための画素が配列され
る関係で、ほぼ矩形のITO膜のパターンが縦横に配列
されている。図2(a)に示すように、1画素形成のパ
ターン7には、ITO膜8の片隅にTFT形成領域9が
あり、ITO膜8がTFT領域9のソースに接続され
る。その外側周囲には、信号線とアドレス線を構成する
Al配線SL ,AL が設けられている。
Next, the detection principle of the present invention will be described with reference to FIG. The pattern formed on the LCD substrate 1 is such that pixels for display are arranged corresponding to each side of the rectangular substrate, and thus a substantially rectangular ITO film pattern is arranged vertically and horizontally. As shown in FIG. 2A, the pattern 7 for forming one pixel has a TFT forming region 9 at one corner of the ITO film 8, and the ITO film 8 is connected to the source of the TFT region 9. Al wirings SL and AL constituting signal lines and address lines are provided around the outside.

【0012】同図(b)に示すように、この画素のパタ
ーン7に対しては、波長λ1 の照射系2からレーザビー
ムA,波長λ2 の照射系3からレーザビームBがそれぞ
れ45度の角度で対向して照射される。その結果、異物
10については、レーザビームAとBの散乱光A+Bが
対物光学系4の対物レンズ4aに入射される。したがっ
て、センサ4gと4hの出力は、ほぼ等しくなり、それ
が閾値THa ,THb を越える一定値以上になると各ア
ンプ6a,6bで増幅され、割算回路6cに入力され
る。このとき、各入力信号に対して割算回路6cで割り
算した結果はほぼ1になる。異物判定回路6dは、割算
回路6cの出力が“1”あるいはほぼ“1”のときに異
物と判定する。
As shown in FIG. 1B, the laser beam A from the irradiation system 2 having the wavelength λ 1 and the laser beam B from the irradiation system 3 having the wavelength λ 2 are 45 degrees with respect to the pattern 7 of the pixel. Irradiation at opposite angles. As a result, with respect to the foreign material 10, the scattered light A + B of the laser beams A and B is incident on the objective lens 4a of the objective optical system 4. Therefore, the outputs of the sensors 4g and 4h become substantially equal, and when they become equal to or more than a certain value exceeding the threshold values THa and THb, they are amplified by the amplifiers 6a and 6b and input to the division circuit 6c. At this time, the result obtained by dividing each input signal by the division circuit 6c becomes substantially 1. The foreign matter determination circuit 6d determines that the foreign matter is present when the output of the division circuit 6c is "1" or substantially "1".

【0013】同図(c)に示すように、パターン7の角
部分については、この部分にレーザビームAとBが照射
された場合、角に直角に照射されるビームと平行に照射
されるビームとに分かれる。パターン7の角部分は、実
際には、異物と同様に多少角に丸みがあって、直角に照
射されたレーザビームAか、Bのいずれかを異物に照射
した場合と同様になる。その結果、レーザビームAの散
乱光A又はレーザビームBの散乱光Bのいずれかが対物
光学系4に多く入射する。したがって、センサ4gと4
hの出力は、いずれか一方が強くなり、他方が弱くな
る。一方の出力のみが閾値を越えたとき、割算回路6c
で割り算した結果は“0”又は“∞”になる。また、両
者が閾値THa ,THb を越えたときであっても、
“1”以外の値になる。なお、閾値THa ,THb の値
を選択すれば、その出力はいずれか一方のみにすること
ができる。これにより割算回路6cで割り算した結果
は、ほぼ“0”又は“∞”にすることができので、割算
回路6cの出力が“1”あるいはほぼ“1”のときにそ
れを異物として検出することができる。
As shown in FIG. 1C, when a laser beam A and a laser beam B are irradiated to a corner portion of the pattern 7, a beam irradiated in parallel with a beam irradiated at a right angle to the corner. Divided into The corner portion of the pattern 7 is actually slightly rounded like the foreign material, and is similar to the case where the laser beam A or B irradiated at right angles is applied to the foreign material. As a result, either the scattered light A of the laser beam A or the scattered light B of the laser beam B enters the objective optical system 4 in a large amount. Therefore, the sensors 4g and 4g
As for the output of h, one of them becomes strong and the other becomes weak. When only one output exceeds the threshold, the dividing circuit 6c
Results in "0" or "$". Further, even when both of them exceed the threshold values THa and THb,
It becomes a value other than "1". If the values of the threshold values THa and THb are selected, only one of them can be output. As a result, the result of the division by the dividing circuit 6c can be made substantially "0" or "∞", so that when the output of the dividing circuit 6c is "1" or almost "1", it is detected as a foreign substance. can do.

【0014】また、同図(d)に示すように、パターン
7の辺については、この部分にレーザビームAとBが照
射された場合、辺に対する照射角が45度であるので、
対物光学系4に入射される散乱光は少ないか、ほとんど
ない。したがって、センサ4gと4hの出力は、いずれ
も弱い。その検出信号は、閾値THa ,THb の値を選
択すれば、これ以下となる。その結果、これらの出力は
発生しない。この閾値THa ,THb の値の選択は、前
記の閾値THa ,THb の値をある値以上に設定すれば
よいので、一方の出力のみを有効とする前記の閾値の選
択と両立させることができる。その結果、割算回路6c
で割り算した結果は“1”あるいはほぼ“1”か、
“0”又は“∞”のいずれかとなる。“0”又は“∞”
のときには、パターンになるので、ほぼ“1”あるいは
“1”を異物と判定して検出することができる。
As shown in FIG. 1D, when the laser beam A and the laser beam B are irradiated on the side of the pattern 7, the irradiation angle with respect to the side is 45 degrees.
The scattered light incident on the objective optical system 4 is small or almost non-existent. Therefore, the outputs of the sensors 4g and 4h are both weak. If the values of the threshold values THa and THb are selected, the detection signal becomes less than this value. As a result, these outputs do not occur. The selection of the threshold values THa and THb can be made compatible with the selection of the threshold value that makes only one of the outputs valid, since the threshold values THa and THb need only be set to a certain value or more. As a result, the division circuit 6c
The result of dividing by "1" or almost "1"
It is either "0" or "$". “0” or “∞”
In this case, since the pattern becomes a pattern, almost "1" or "1" can be determined and detected as a foreign substance.

【0015】以上説明してきたが、実施例における照射
系のLCD基板に対する仰角は、35度に限定されな
い。また、実施例では、割算回路により受光センサによ
る散乱光の検出レベルが等しいか否かを検出している
が、これは、アナログコンパレータを始め、各種のレベ
ル比較回路を使用することができる。
As described above, the elevation angle of the irradiation system with respect to the LCD substrate in the embodiment is not limited to 35 degrees. In the embodiment, the division circuit detects whether or not the detection levels of the scattered light by the light receiving sensor are equal. For this, various level comparison circuits including an analog comparator can be used.

【0016】[0016]

【発明の効果】以上の説明のとおり、この発明による液
晶基板の異物検査装置にあっては、等しい角度で対向さ
せて2本のレーザビームを照射しているので、これらの
レーザビームを受けた異物の前方散乱はほぼ等しく、ま
た、パターンの角の部分では、2本のレーザビームのう
ち一方は、直角に当たり、他方は、平行に近い形になる
ので、直角に当たった方のレーザビームの前方散乱光は
大きく、平行に当たった方のレーザビームの前方散乱光
は小さくなる。したがって、これらに差が生じ、等しく
はならないので、ITO膜の領域でも、TFT領域でも
異物とパターンとを分けて検出することができる。
As described above, in the apparatus for inspecting foreign matter on a liquid crystal substrate according to the present invention, two laser beams are irradiated so as to face each other at an equal angle. The forward scattering of the foreign matter is almost equal, and at the corners of the pattern, one of the two laser beams hits a right angle and the other becomes nearly parallel, so that the laser beam hit at the right angle The forward scattered light is large, and the forward scattered light of the laser beam hit in parallel is small. Therefore, there is a difference between them and they are not equal, so that the foreign matter and the pattern can be detected separately in both the ITO film region and the TFT region.

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

【図1】図1は、この発明の一実施例の液晶基板の異物
検査装置を適用した検査装置の構成図である。
FIG. 1 is a configuration diagram of an inspection apparatus to which a foreign substance inspection apparatus for a liquid crystal substrate according to an embodiment of the present invention is applied.

【図2】図2はその検出原理の説明図であって、(a)
は画素パターンの説明図、(b)は異物の散乱状態の説
明図、(c)はパターンの角部分の散乱状態の説明図、
(d)はパターンの辺部分の散乱状態の説明図である。
FIG. 2 is an explanatory view of the detection principle, and (a)
Is an explanatory view of a pixel pattern, (b) is an explanatory view of a scattering state of a foreign substance, (c) is an explanatory view of a scattering state of a corner portion of the pattern,
(D) is an explanatory view of a scattering state of a side portion of the pattern.

【符号の説明】[Explanation of symbols]

1…LCD基板、2,3…照射系、4…対物光学系、5
…顕微鏡観測光学系、6…検出回路、7…1画素形成の
パターン、8…ITO膜、9…TFT形成領域、10…
異物。
1 ... LCD substrate, 2,3 ... irradiation system, 4 ... objective optical system, 5
... Microscope observation optical system, 6 ... Detection circuit, 7 ... Pattern for forming one pixel, 8 ... ITO film, 9 ... TFT formation area, 10 ...
Foreign matter.

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G02F 1/13 101 G01N 21/88 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 7 , DB name) G02F 1/13 101 G01N 21/88

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】矩形状のパターンが配列された基板の表面
に投影されたときの照射角が前記矩形状のパターンの1
つの辺に対してほぼ45度になる状態で照射点に立てた
法線を挟んで対向する互いに異なる波長の2本のレーザ
光を前記基板の表面に対してほぼ等しい仰角で斜めに照
射する第1及び第2の照射系と、前記照射点の上方でそ
れぞれの散乱光を受光し、前記異なる波長のそれぞれに
分離してこれら分離された散乱光を第1及び第2の光電
変換センサでそれぞれ受光してそれぞれの検出信号を発
生する検出光学系と、前記第1及び第2の光電変換セン
サにより得られる検出信号のレベルがほぼ等しいか否か
を検出する検出回路とを備える液晶基板の異物検査装
置。
An irradiation angle when projected on a surface of a substrate on which a rectangular pattern is arranged is one of the rectangular patterns.
The two laser beams having different wavelengths facing each other with a normal line at the irradiation point interposed therebetween at an angle of approximately 45 degrees with respect to the two sides are obliquely applied to the surface of the substrate at substantially equal elevation angles. First and second irradiation systems, each of which receives scattered light above the irradiation point, separates the scattered light into each of the different wavelengths, and separates the scattered light with the first and second photoelectric conversion sensors. Foreign matter on a liquid crystal substrate, comprising: a detection optical system that receives light to generate respective detection signals; and a detection circuit that detects whether the levels of the detection signals obtained by the first and second photoelectric conversion sensors are substantially equal. Inspection equipment.
【請求項2】前記検出回路は、第1及び第2の光電変換
センサより得られるそれぞれの検出信号を受け、この検
出信号に対して所定の閾値を有する第1及び第2の増幅
回路と、これら第1及び第2の増幅回路の出力を受けて
これら出力がほぼ等しいか否か検出する割算回路あるい
はアナログ比較回路とを備える請求項1記載の液晶基板
の異物検査装置。
2. The detection circuit receives first and second detection signals obtained from first and second photoelectric conversion sensors, and first and second amplification circuits having a predetermined threshold value for the detection signals. 2. The liquid crystal substrate foreign matter inspection apparatus according to claim 1, further comprising a division circuit or an analog comparison circuit which receives the outputs of the first and second amplifier circuits and detects whether or not these outputs are substantially equal.
JP17113393A 1993-06-17 1993-06-17 Liquid crystal substrate foreign matter inspection device Expired - Fee Related JP3266217B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17113393A JP3266217B2 (en) 1993-06-17 1993-06-17 Liquid crystal substrate foreign matter inspection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17113393A JP3266217B2 (en) 1993-06-17 1993-06-17 Liquid crystal substrate foreign matter inspection device

Publications (2)

Publication Number Publication Date
JPH075407A JPH075407A (en) 1995-01-10
JP3266217B2 true JP3266217B2 (en) 2002-03-18

Family

ID=15917599

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17113393A Expired - Fee Related JP3266217B2 (en) 1993-06-17 1993-06-17 Liquid crystal substrate foreign matter inspection device

Country Status (1)

Country Link
JP (1) JP3266217B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3130222B2 (en) 1995-02-14 2001-01-31 三菱電機株式会社 Method for analyzing minute foreign matter, analyzer, and method for producing semiconductor element or liquid crystal display element using the same
JP2813147B2 (en) * 1995-02-14 1998-10-22 三菱電機株式会社 Method for analyzing minute foreign matter, analyzer and method for producing semiconductor element or liquid crystal display element using the same
US7349082B2 (en) * 2004-10-05 2008-03-25 Asml Netherlands B.V. Particle detection device, lithographic apparatus and device manufacturing method

Also Published As

Publication number Publication date
JPH075407A (en) 1995-01-10

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