200827819 九、發明說明： 【發明所屬之^技術領域】 技術領域 ^ 本發明係有關於一種修復液晶顯示面板的技術，更詳 ， 5 而吕之’係有關於去除液晶顯示面板之瑕疯像素的方法及 用以實現該方法之裝置。 t先前技術3 背景技術 液晶顯示裝置係藉由影像信號來調節液晶之透光率， 10以顯示影像。因此，液晶顯示裝置包含有設有配置成矩陣 狀之晶胞_)的液晶顯示面板，及藉由影像信號來控制各 晶胞之透光率的驅動電路。 第1圖係簡單地顯示習知液晶顯示面板之晶胞結構的 圖式。液晶顯不面板之晶胞包含有藉由在薄膜電晶體(τρτ) • 15纟璃⑽彩色濾光片（CF)玻璃19之間控制電壓來偏光之液 晶層15 1以實現全彩之R、G、轉色據光片17;及可控 舰晶狀偏絲度，關節透光率的半㈣電路層12。 另外液晶顯示面板之晶胞還包含有像素電極13、配向膜 14、共通電極16及黑色矩陣a等。 20 調節晶胞亮度的原理如下。由背光（圖未示)提供之光通 過液晶層15並偏光，經偏光之光通過配置於tft玻璃⑽ CF玻璃19外部之偏光板（圖未示）而進入肉目艮。此時，經偏 光之光的方向越接近與偏光板之偏光方向垂直的方向，經 偏光之光就越無法順利通過偏光板，而其越接近平行的方 5 200827819 向，經偏光之光就越可以順利通過偏光板。結果，藉由透 過控制施加於兩玻璃之間的電壓，來調節液晶層之偏光程 . 度，即可調節晶胞之亮度。 - 另一方面，使用具有可使特定波長之光順利穿透，而 ’ 5 遮斷其他波長之光之特性的彩色慮光片’可實現彩色液晶 顯示面板。即，R濾光片可使紅色光順利穿透，且使其他波 長之光無法穿透，G濾光片可使綠色光順利穿透，且使其他 波長之光無法穿透，而B濾光片則可使藍色光順利穿透’且 使其他波長之光無法穿透。 10 生產液晶顯示面板的業者判斷液晶顯示面板是否有瑕 疵的基準在於液晶顯示面板所含之瑕疵晶胞數。瑕疵晶胞 可分成亮點晶胞和暗點晶胞，但通常可容許之亮點晶胞數 較暗點晶胞數嚴格。根據此種理由，將亮點晶胞暗點化可 提高液晶顯示面板的產率。例如，在完全不能容許有亮點 ‘ 15晶胞存在，而可容許1個暗點晶胞存在時，若在具有一個亮 點晶胞之液晶顯示面板將亮點晶胞替換成暗點晶胞，液晶 顯示面板即可成為正常面板。 專利文獻1揭示使亮點晶胞暗點化來修復液晶顯示面 板的技術。具體地參照該修復技術看來，為使因異物引起 2〇之亮點晶胞暗點化，係將雷射照射在黑色矩陣上，以、溶化 黑色矩陣’然後將已溶化之黑色矩陣的物質引導至異物 处、X使儿·、、、占日日胞暗點化。但是，前述方式在溶化黑色矩 陣日守，已令化之黑色矩陣的物質會移動至與瑕疵晶胞隣接 之正“曰胞，此時會有連正常晶胞都被暗點化的嚴重問題 6 200827819 【專利文獻1】韓國專利公開第2006-0067042號公報 發明揭示 5 發明所欲解決之問題 本發明者了解到，需要可使對隣接晶胞之影響最小 化，並使亮點晶胞暗點化的方案。即，藉由將雷射直接照 射在透光之晶胞區域(彩色濾光片區域），來代替熔化黑色矩 陣，而完成本發明。 10 但是，以雷射照射彩色濾光片使瑕疵像素暗點化的方 式有如第2圖所說明之問題點。 一般而言，在雷射照射時，雷射穿透的深度越大，雷 射的能量或強度就下降的越多，而某種程度之雷射能源可 傳達至比較深的層。因此，如第2圖所示，即 b點已對準彩色遽光片17’還是會有-部分的能源傳達= 晶層15。由於傳達至液晶層的能源，會有在液晶㈣產生 氣體的可能，此種氣體就會成為液晶層内產生氣泡22的原 因。 20 入液晶層，故還 就算雷射能源無法傳達至液晶層，但由於在雷射的昭 射過程中於彩色濾光片產生之氣體等會侵 、 是會有氣泡產生的可能性。 產生於液晶層之氣、泡也會對所欲修復之像素以外 致命性曙。而且，也有__面_ B曰層的氣泡而無法❹的情形，必須盡量避免氣泡現 7 200827819 象的發生。 - A了防止如上所述之氣泡現象，應減低雷射之穿透深 . f °為此’應縮短之祕波長。而縮短雷射波長最好 - 是從彩色濾光片之穿透度來看。 :5第3圖係顯示彩色濾光片之透光率特性的圖表。如該圖 所不，各彩W光片對於特定波長附近之光的透光率優 異，但對於其他波長之光的穿透性較低。例如，B渡光片^ 料46Gnm附近之波長的透光率優異，g澹光片η對於 52〇nm附近之波長的透光率優異，純據光片η對於_腿 10 以上之波長的透光率優異。 因此，在想要使用雷射來變化彩色滤光片的物理性質 時，最好是使用彩色滤光片之透光率低之波長的雷射，以 提高能源之傳達效率。參照第3圖，要使用一個雷射來變化 ' R、G、聰光片的物理性質，最好是使用具有約41Gnm以下 * 15 之波長的雷射。 但是，在使用波長非常短的雷射來變化彩色濾光片的 物理性質的過程中，會有液晶顯示面板的其他構成要素(如 偏光板)無法使用的可能。因此，最好不要持續使用短波長 的雷射。 20 在此，在將雷射直接照射在彩色濾光片來修復液晶顯 不面板的方式中，從彩色濾光片之吸光率、液晶層的氣泡 現象來看，雷射最為重要，本發明人即著眼於這一點上， 而對此進行研究，當中發現藉由以相異之雷射透過二個段 階來對包含在瑕疵像素中之彩色濾光片照射雷射，可有效 8 200827819 地修復瑕窥晶胞，而完成本發明。 本發明係有鑑於前述問題而作成者，且其目的在於提 供使對液晶顯示面板之隣接晶胞的影響最小化，並可修復 液晶顯不面板之瑕疵晶胞的方法及用以實現該方法之裝 ， 5 置。 用以解決問題之手段 為解決前述問題，本發明之一實施形態之液晶顯示面 板之修復方法包含有：照射第1雷射，使包含在喊像素中 之π色濾光片在彩色渡光片玻璃附近形成間隙的步驟；及 Η)照射第2雷射，使前述有間隙形成之彩色濾光片的物理性質 變化，以降低透光性的步驟。 此時，前述第1雷射最好是奈秒脈衝雷射。 另外，前述第1雷射最好是波長約扮肺之脈衝雷射。 此外，前述第1雷射最好是波長約53施之脈衝雷射。 • 15 $外，前述形成間_步驟最好是包含有：提供基本 波長約1064nm之脈衝雷射的步驟；提供前述基本波長約 祕碰之脈衝雷射之諸波中之其中—個來作為前述第蹭 射的步驟；及將前述第1雷射照射在前述瑕疲像素上的步 驟。 20 &外，前述形成間隙的步驟最好是更包含有：使前述 彩色慮光片在财述彩色據光片玻璃附近形成·4 ^一 左右之前述間隙的步驟。 另外，前述第2雷射最好是波長約400nm〜490nm之雷 射0 9 200827819 此外，前述第2雷射最好是波長約4〇8nm之連續雷射。 另外，前述第2雷射最好是波長約446nm之連續雷射。 此外，前述第2雷射最好是波長約45〇nm之飛秒脈衝雷 射。 5 另外，液晶顯示面板之修復裝置包含有··第1雷射產生 器，係可產生第1雷射，使包含在瑕疲像素中之彩色遽光片 在形色濾光片玻璃附近形成間隙者；及第2雷射產生器，係 可產生第2雷射，使前述有間隙形成之彩色濾光片的物理性 質變化，以降低透光性者。 10 此時，前述第1雷射產生器最好是可產生奈秒脈衝雷射 之脈衝雷射產生器。 另外，前述第！雷射產生器最好是可產生波長約355嫌 之脈衝雷射之脈衝雷射產生器。 此外，前述第！雷射產生器最好是可產生波長約532nm 15 之脈衝雷射之脈衝雷射產生器。 另外，前述第2雷射產生器最好是可產生波長約 400nm〜490nm之雷射的雷射產生器。 此外，前述第2雷射產生器最好是可產生波長約45〇nm 之飛秒脈衝雷射之脈衝雷射產生器。 2〇另外，前述第2雷射產生器最好是可產生波長約408nm 之連續雷射之光二極體雷射產生器。 而且，前述第2雷射產生器最好是可產生波長約446nm 之連續雷射之光二極體雷射產生器。 發明效果 200827819 根據本發明之液晶顯示面板之修復方法及裝置，藉由 使瑕疵晶胞之彩色濾光片的物理性質變化，可使對液晶顯 示面板之隣接晶胞的影響最小化。另外，在液晶顯示面板 之修復方法及裝置中，藉由不會對隣接晶胞產生影響地使 5 梵點暗點化’可有效地提南液晶顯示面板之產率。 t實施方式3 實施發明之最佳形態 以下參照添附圖式，詳細地說明實施本發明之實施形 態。 10 接下來會詳細地說明該等實施形態，以使發明所屬技 術領域中具有通常知識者可充分地實施本發明。而且要理 解的是，本發明之多樣化實施形態相異，沒有相互排他性 的必要。例如，此處所揭示之特定形狀、構造及特性，只 要與一實施形態有關聯，而不脫離本發明之精神及範圍， 15即可以另一實施形態實現。另外還需理解的是，所分別揭 示之實施形態内之個別構成要素的位置或配置只要不脫離 本發明之精神及範圍，皆可作變更。因此，後述之詳細說 明並非以限定意義來例示者，若要適當地說明本發明之範 圍’即其僅為和其請求項所主張者均等之所有範圍一起添 2〇附之請求項所限定。圖式中，類似的參照符號在各方面中 係表示同一或類似的機能。 第4圖係顯示本發明之一實施形態之液晶顯示面板之 修復過程的流程圖。 首先’為修復液晶顯示面板，要檢測出存在於液晶顯 11 200827819 - 5 示面板之亮點晶胞(si)。因檢測出亮點晶胞的方式係眾所周 知的技術，故省略其說明。在液晶顯示面板發現亮點晶胞， 而需要使該亮點晶胞暗點化時，即，可使亮點晶胞暗點化 來修復液晶顯示面板時，進行液晶顯示面板之修復。 首先，使用第1雷射在免點晶胞之彩色濾、光片形成間p审 (S2)。而在使彩色濾光片之物理性質變化之前在彩色濾、光片 形成間隙的理由，係可使彩色濾光片的物理性質順利產生 變化。換言之，將第1雷射照射在彩色濾光片時，彩色濾光 片會在彩色濾光片之玻璃附近形成間隙，而有間隙形成之 10 彩色濾光片具有容易藉由雷射而變化之物理性質（透光性) 的特性。 在彩色濾光片形成間隙時，使用第2雷射來降低彩色濾 光片之透光性(S3)。將第2雷射照射在有間隙形成之彩色渡 光片時，就會變化彩色遽光片之物理性質。此時，彩色濾 - 15 光片之透光性會急速地降低。 如此，為修復液晶顯示面板，需要用以使彩色濾光片 形成間隙的第1雷射，及用以使有間隙形成之彩色濾光片之 物理性質變化的第2雷射。如此，參照第5A圖來說明可產生 第1雷射及第2雷射之液晶顯示面板的修復裝置。 20 第5A圖係顯示本發明之一實施形態之液晶顯示面板之 修復裝置40的方塊圖。 液晶顯示面板之修復裝置40包含第1雷射產生器41、第 2雷射產生器42及雷射傳達路徑43。 第1雷射產生器41可產生用以使包含在液晶顯示面板 12 200827819 46之喊日日日胞47中之彩色^片在彩色心片玻璃附近形 成間隙的第1雷射44。 在使彩色滤'光片形成間隙的過程中，要使液晶顯示面 _ 板之其他部分的損傷最小化，必須要將第丨雷射之能源集中 • 5 在有間隙形成的部分。 為此’必腳短第❻射之波長。錢行使用各種波長 的雷射在彩色遽光片形成間隙的實驗後，可確認说細波長 之雷射顯不出優異之性能。另一方面，532細波長的雷射亦 可在彩色濾光片形成間隙。 10 料，從實驗結果可發現，在第！雷射使用奈秒雷射 時，可順利在彩色遽光片形成間隙。這是因為彩色滤光片 f子之晶格祕係以奈秒料來進行，制奈秒雷射時在 和色慮光片为子會產生共振，而可在彩色濾光片順利形 間隙。 為產生八此種特性之雷射，第i雷射產生器可使用 1064nm波長之奈秒脈衝雷射。 355細波長之脈衝雷射係由l〇64nm波長之奈秒脈衝雷 射之第3諧波取得。同樣地，532·波長之脈衝雷射係由 l〇64nm波長之奈秒脈衝雷射之第2譜波取得。 20 ^驗結果顯示，彩色遽光片之間隙大小在約〇·4〜〇·8μιη 左右日才，對液晶顯示面板其他部分的影響較少，且可藉由 第2雷射順利地使彩色濾光片之物理性質產生變化。 第2雷射產生器42可產生可使有間隙形成之彩色濾光 片的物理貝艾化’以降低透光性的第2雷射#。 13 200827819 第2雷射係用以使已有間隙形成之彩色濾光片的物理 性質變化，故可使用較第丨雷射長之波長的雷射。實驗結果 顯示，第2雷射之波長在約4〇〇〜49〇nm的範圍内時，有間隙 形成之彩色濾光片的物理性質較容易產生變化， 一 且對液晶 5 顯示面板其他部分的影響較少。 弟2运射可使用飛秒脈衝雷射或連續雷射。實驗時在 使用450nm之飛秒脈衝雷射時彩色濾光片之物理性^的微200827819 IX. INSTRUCTIONS: [Technical Field] Technical Field The present invention relates to a technique for repairing a liquid crystal display panel, and more specifically, and the "Lv" is related to removing a mad pixel of a liquid crystal display panel. Method and apparatus for implementing the method. BACKGROUND OF THE INVENTION A liquid crystal display device adjusts the transmittance of a liquid crystal by an image signal to display an image. Therefore, the liquid crystal display device includes a liquid crystal display panel provided with a unit cell arranged in a matrix, and a drive circuit for controlling the light transmittance of each unit cell by an image signal. Fig. 1 is a view showing a simple structure of a unit cell of a conventional liquid crystal display panel. The liquid crystal display panel unit cell includes a liquid crystal layer 15 1 which is polarized by a voltage between a thin film transistor (τρτ) • 15 glass (10) color filter (CF) glass 19 to achieve full color R, G, color-changing light film 17; and controllable ship crystal-shaped partial wire, joint light transmittance of the half (four) circuit layer 12. Further, the unit cell of the liquid crystal display panel further includes a pixel electrode 13, an alignment film 14, a common electrode 16, a black matrix a, and the like. 20 The principle of adjusting the brightness of the unit cell is as follows. Light supplied from a backlight (not shown) passes through the liquid crystal layer 15 and is polarized, and the polarized light passes through a polarizing plate (not shown) disposed outside the tft glass (10) CF glass 19 to enter the flesh. At this time, the closer the direction of the polarized light is to the direction perpendicular to the polarization direction of the polarizing plate, the more the polarized light passes through the polarizing plate, and the closer it is to the parallel side 5 200827819, the more the polarized light passes. Can pass the polarizer smoothly. As a result, the brightness of the unit cell can be adjusted by controlling the bias period of the liquid crystal layer by controlling the voltage applied between the two glasses. On the other hand, a color liquid crystal display panel can be realized by using a color filter sheet having a characteristic of allowing light of a specific wavelength to smoothly penetrate and '5 blocking light of other wavelengths'. That is, the R filter allows the red light to penetrate smoothly, and the light of other wavelengths cannot be penetrated. The G filter can smoothly penetrate the green light and make the light of other wavelengths unable to penetrate, and the B filter The film allows the blue light to penetrate smoothly and prevents other wavelengths of light from penetrating. 10 The manufacturer who produces the liquid crystal display panel determines whether the liquid crystal display panel has a flaw. The benchmark is the number of cells in the liquid crystal display panel. The germanium unit cell can be divided into a bright spot cell and a dark spot cell, but the number of bright spot cells can usually be tolerated to be stricter than the dark cell. For this reason, darkening the bright spot cells can increase the yield of the liquid crystal display panel. For example, when a bright spot '15 cell is completely unacceptable and one dark spot cell can be allowed to exist, if a liquid crystal display panel having a bright spot cell replaces the bright cell with a dark cell, the liquid crystal display The panel becomes the normal panel. Patent Document 1 discloses a technique of darkening a bright spot cell to repair a liquid crystal display panel. Referring specifically to the repair technique, in order to darken the bright spot cell caused by the foreign matter, the laser is irradiated onto the black matrix to melt the black matrix and then guide the dissolved black matrix material. To the foreign body, X makes the children, and, in the day, dark spots. However, the above-mentioned method dissolves the black matrix and keeps the material of the black matrix moving to the positive "cell" adjacent to the unit cell. At this time, there will be a serious problem that even the normal unit cell is darkened. 200827819 [Patent Document 1] Korean Patent Publication No. 2006-0067042 DISCLOSURE OF THE INVENTION PROBLEMS TO BE SOLVED BY THE INVENTION The present inventors have learned that it is necessary to minimize the influence on adjacent cells and to darken the bright spot cells. That is, the present invention is completed by directly irradiating a laser in a light-transmissive cell region (color filter region) instead of melting a black matrix. 10 However, the color filter is irradiated with laser light. The way in which the pixels are darkened is as described in Figure 2. In general, the greater the depth of laser penetration during laser illumination, the more the energy or intensity of the laser decreases. The laser energy of a certain degree can be transmitted to a deeper layer. Therefore, as shown in Fig. 2, that point b is aligned with the color calender sheet 17' or there will be a part of the energy transmission = the crystal layer 15. Energy to the liquid crystal layer, There is a possibility of generating a gas in the liquid crystal (4), and this gas causes the generation of the bubble 22 in the liquid crystal layer. 20 Entering the liquid crystal layer, even if the laser energy cannot be transmitted to the liquid crystal layer, due to the laser emission process The gas generated in the color filter will invade, and there is a possibility that bubbles will be generated. The gas and bubbles generated in the liquid crystal layer will also be fatal to the outside of the pixel to be repaired. Moreover, there are also __面_ In the case of bubbles in the B layer, it is necessary to avoid the occurrence of bubbles. - A. To prevent the bubble phenomenon as described above, the penetration depth of the laser should be reduced. f ° The wavelength is the best, and the laser wavelength is shortened best - from the transparency of the color filter. : 5 Figure 3 shows a graph of the light transmittance characteristics of the color filter. The color W light sheet is excellent in light transmittance for light near a specific wavelength, but has low transmittance to light of other wavelengths. For example, the wavelength of light near the wavelength of 46 Gnm of the B-wave film is excellent, and the light is bright. The sheet η is excellent in light transmittance at a wavelength near 52 〇 nm, The light η is excellent in light transmittance for wavelengths above _ leg 10. Therefore, when it is desired to use a laser to change the physical properties of the color filter, it is preferable to use a color filter with low light transmittance. The laser of the wavelength to improve the efficiency of energy transmission. Referring to Figure 3, a laser is used to change the physical properties of 'R, G, Congguang, preferably using a wavelength of about 41 Gnm or less* 15 Laser. However, in the process of changing the physical properties of the color filter using a laser with a very short wavelength, there is a possibility that other components of the liquid crystal display panel (such as a polarizing plate) cannot be used. Therefore, it is best not to use it. Continuous use of short-wavelength lasers. 20 Here, in the way of directly irradiating a laser to a color filter to repair a liquid crystal display panel, from the light absorption rate of the color filter and the bubble phenomenon of the liquid crystal layer, The laser is the most important, and the present inventors focused on this point and studied it, and found that the color filter included in the pixel is irradiated with laser light by transmitting two different steps with different lasers. ,may have 8200827819 repairing flaws glimpse cell, and completed the present invention. The present invention has been made in view of the foregoing problems, and an object thereof is to provide a method for minimizing the influence of adjacent cells of a liquid crystal display panel, and capable of repairing a germanium cell of a liquid crystal display panel and for implementing the method. Installed, 5 sets. Means for Solving the Problems In order to solve the above problems, a method for repairing a liquid crystal display panel according to an embodiment of the present invention includes: illuminating a first laser to cause a π color filter included in a shouting pixel to be in a color light passing sheet a step of forming a gap near the glass; and a step of irradiating the second laser to change the physical properties of the color filter formed by the gap to reduce the light transmittance. At this time, the first laser is preferably a nanosecond pulse laser. Further, the first laser is preferably a pulsed laser having a wavelength of about the lung. Further, the first laser is preferably a pulsed laser having a wavelength of about 53. • 15 Å, the aforementioned inter-formation step _ preferably includes: providing a pulse laser having a fundamental wavelength of about 1064 nm; providing one of the waves of the pulse wave of the basic wavelength of the aforementioned collision as the aforementioned a step of emitting a first shot; and a step of irradiating the first laser to the aforementioned fatigued pixel. Further, in the step of forming the gap, the step of forming the gap further includes the step of forming the color light-receiving sheet to form the gap of about 4^1 in the vicinity of the glass of the color light-receiving sheet. Further, the second laser is preferably a laser having a wavelength of about 400 nm to 490 nm. 0 9 200827819 Further, the second laser is preferably a continuous laser having a wavelength of about 4 〇 8 nm. Further, the second laser is preferably a continuous laser having a wavelength of about 446 nm. Further, the aforementioned second laser is preferably a femtosecond pulse laser having a wavelength of about 45 〇 nm. In addition, the repair device of the liquid crystal display panel includes a first laser generator that generates a first laser, so that a color filter included in the fatigued pixel forms a gap near the color filter glass. And the second laser generator is capable of generating a second laser to change the physical properties of the color filter formed by the gap to reduce the light transmittance. 10 At this time, the aforementioned first laser generator is preferably a pulsed laser generator which can generate a nanosecond pulse laser. In addition, the aforementioned! Preferably, the laser generator is a pulsed laser generator that produces a pulsed laser having a wavelength of about 355. In addition, the aforementioned first! The laser generator is preferably a pulsed laser generator that produces a pulsed laser having a wavelength of about 532 nm. Further, the second laser generator is preferably a laser generator which can generate a laser having a wavelength of about 400 nm to 490 nm. Further, the aforementioned second laser generator is preferably a pulsed laser generator capable of generating a femtosecond pulsed laser having a wavelength of about 45 〇 nm. Further, the second laser generator is preferably a photodiode laser generator capable of generating a continuous laser having a wavelength of about 408 nm. Further, the second laser generator is preferably a photodiode laser generator capable of generating a continuous laser having a wavelength of about 446 nm. EFFECT OF THE INVENTION 200827819 According to the method and apparatus for repairing a liquid crystal display panel of the present invention, the influence on the adjacent unit cell of the liquid crystal display panel can be minimized by changing the physical properties of the color filter of the unit cell. Further, in the repairing method and apparatus for a liquid crystal display panel, the yield of the south liquid crystal display panel can be effectively improved by not darkening the van Gogh point without affecting the adjacent unit cell. BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings. The embodiments will be described in detail below, so that those skilled in the art can fully implement the present invention. Moreover, it is to be understood that the various embodiments of the present invention are different and are not mutually exclusive. For example, the specific shapes, configurations, and characteristics disclosed herein may be made in a single embodiment without departing from the spirit and scope of the invention. In addition, it is to be understood that the position and arrangement of the individual components in the embodiments disclosed herein may be modified without departing from the spirit and scope of the invention. Therefore, the detailed description is not to be construed as limited to the scope of the invention, and the scope of the present invention is to be construed as being limited to the scope of the claims. In the drawings, like reference characters indicate the same or similar functions in the various aspects. Fig. 4 is a flow chart showing the repair process of the liquid crystal display panel of one embodiment of the present invention. First of all, in order to repair the liquid crystal display panel, it is necessary to detect the bright spot cell (si) present in the liquid crystal display panel of 200827819-5. Since the manner in which the bright spot cells are detected is a well-known technique, the description thereof will be omitted. When a bright spot cell is found on the liquid crystal display panel, and the bright spot cell needs to be darkened, that is, when the bright spot cell is darkened to repair the liquid crystal display panel, the liquid crystal display panel is repaired. First, the first laser is used for the color filter of the spot cell and the film formation is performed (S2). The reason why the gap between the color filter and the light sheet is formed before the physical properties of the color filter are changed is that the physical properties of the color filter can be smoothly changed. In other words, when the first laser is irradiated on the color filter, the color filter forms a gap near the glass of the color filter, and the 10 color filter formed with the gap is easily changed by the laser. Characteristics of physical properties (transparency). When a gap is formed in the color filter, the second laser is used to reduce the light transmittance of the color filter (S3). When the second laser is irradiated onto a color light-emitting sheet formed by a gap, the physical properties of the color light-emitting sheet are changed. At this time, the light transmittance of the color filter - 15 light sheet is rapidly lowered. As described above, in order to repair the liquid crystal display panel, a first laser for forming a gap between the color filters and a second laser for changing the physical properties of the color filter having the gap are required. Thus, a repairing apparatus for a liquid crystal display panel capable of generating a first laser and a second laser will be described with reference to Fig. 5A. Fig. 5A is a block diagram showing a repairing device 40 of a liquid crystal display panel according to an embodiment of the present invention. The repair device 40 for the liquid crystal display panel includes a first laser generator 41, a second laser generator 42, and a laser transmission path 43. The first laser generator 41 generates a first laser 44 for forming a gap between the color chips included in the solar cell 47 of the liquid crystal display panel 12 200827819 46 in the vicinity of the color core glass. In order to minimize the damage of other parts of the liquid crystal display panel during the process of forming the gap between the color filter 'slabs, it is necessary to concentrate the energy of the third laser to be 5 in the portion where the gap is formed. For this reason, the wavelength of the short shot is required. After using a laser of various wavelengths to form a gap in a color filter, it was confirmed that a fine-wavelength laser showed excellent performance. On the other hand, a 532 fine-wavelength laser can also form a gap in the color filter. 10 materials, from the experimental results can be found in the first! When a laser uses a nanosecond laser, it can smoothly form a gap in the color pupil. This is because the crystal lattice of the color filter f is carried out in nanoseconds. When the nanosecond laser is produced, the color and the color filter are resonated, and the color filter can be smoothly formed in the gap. To produce a laser of this nature, the i-th laser generator can use a 1064 nm wavelength nanosecond pulsed laser. The 355 fine-wavelength pulsed laser is obtained from the third harmonic of the nanosecond pulsed laser with a wavelength of l〇64nm. Similarly, a 532-wavelength pulsed laser is obtained from a second spectral wave of a nanosecond pulsed laser having a wavelength of 64 nm. 20 ^ The test results show that the gap size of the color light film is about 〇·4~〇·8μιη, which has less influence on other parts of the liquid crystal display panel, and the color filter can be smoothly filtered by the second laser. The physical properties of the light sheet change. The second laser generator 42 can generate a second laser # which can reduce the light transmittance of the color filter formed by the gap. 13 200827819 The second laser is used to change the physical properties of the color filter formed by the existing gap, so that a laser with a longer wavelength than the first laser can be used. The experimental results show that when the wavelength of the second laser is in the range of about 4 〇〇 to 49 〇 nm, the physical properties of the color filter formed by the gap are relatively easy to change, and the other parts of the liquid crystal display panel are displayed. Less impact. Brother 2 can use femtosecond pulsed lasers or continuous lasers. The physical properties of the color filter when using a 450nm femtosecond pulsed laser during the experiment
化特性優異。 θ > I 其理由係必須將第2雷射的能源集中在彩色濾光片之 10間隙形成的部分，而所集中之能源可透過分子之晶柊振動 擴散至其他部位的緣故。通常分子之晶格振動所需之時間 為奈秒單位，藉此，在使用可非常短的時間内集中能源之 飛秒雷射時’可順利顯現彩色濾光片之物理性質的^化特 性。 15 另一方面，連續雷射產生器中，在使用可產生 408(±8)nm之連續雷射的光二極體雷射產生器或可產生 446nm之連續雷射的光二極體雷射產生器時，彩色濾光片之 物理性質的變化特性優異。 第5B圖係顯不實現液晶顯示面板之修復裝置之例的立 20體圖。雷射及光學部（對應第5A圖之40)可在γ軸方向上移 動，且液晶顯示面板(對應第5A圖之46)所搭載之載台可在X 轴方向上移動。 如此，雷射、光學部與載台可互相移動，使雷射對應 所欲修復之瑕疵晶胞。 14 200827819 雷射及光學部包含可產生用以在彩色遽光片形成間隙 之雷射的第1雷射產生器（對應第5A圖之41)，可產生用以彩 色慮光片之物理H質變化之雷射的第2雷射產生器（對應第 5A圖之42)’及心使來自該等雷射產生器之雷射正球地到 5達瑕疲晶胞的雷射傳達路徑(對應第5A®之43)。 第5C圖係顯示實現第5B圖之液晶顯示面板之修復裝 置中之雷射及光學部之例的圖式。雷射及光學部包含雷射 產生态及雷射傳達路徑。 雷射傳達路經包含可提高雷射直進性之準直儀、可調 10節雷射輸出之衰減器、透鏡、稜鏡、分束器及鏡子等。 要達成本發明之目的，可設置用以使彩色渡光片之物 理性質變化的雷射產生器、及將雷射產生器所產生之雷射 傳達至瑕疫晶胞之彩色濾光片的雷射傳達路徑。 因此，第5C圖所示之雷射及光學部僅為一例，亦可變 15更衰減器、透鏡、稜鏡、分束器及鏡子等之排列。另外， 可依需要刪除或追加前述之光學元件。 第6A及6B圖係顯示藉由本發明之一實施形態使彩色 濾光片形成間隙之情形的截面圖。 第6A圖係拍攝將第1雷射照射在亮點晶胞之彩色濾光 2〇片形成46〇nm之間隙之情形的照片，而第6B圖係拍攝736nm 之間隙形成之情形的照片。如該等圖式所示，間隙並非形 成於垂直方向，而是形成於水平方向。 第7A圖、第7B圖及第7C圖係拍攝藉由本發明之一實施 形悲使物理性質變化，以降低彩色濾光片之透光性之情形 15 200827819 . 的照片。 特別是’第7A圖、第7B圖及第7C圖係拍攝將彻伽波 : *之雷射照射在有間隙形成之彩色渡光片時，物理性質在 間隙周圍變化之情形的照片。 - 5 第7A圖係顯示以82等級的強度照射雷射時，在間隙周 圍之物理性質的變化，第7B圖係顯示以84等級的強度照射 雷射時，在間隙周圍之物理性質的變化，而第7€圖係顯示 以86等級的強度照射雷射時，在間隙周圍之物理性質的變 化由此可知，當雷射能量增加時，物理性質變化之部分 1〇的厚度會增加。如此，彩色濾光片之物理性質變化之部分 可將光遮斷，故物理性質變化部位具有一定以上之厚度 時，亮點晶胞即可變成暗點晶胞。但是，因有晶胞變龐大 的可能，故將物理性質變化部位維持在適當的厚度是很重 要的。 15產業上利用之可能性 根據本發明，藉由使瑕疵晶胞之彩色濾光片的物理性 質變化，可使對液晶顯示面板之隣接晶胞的影響最小化。 另外’在液晶顯示面板之修復方法及裝置中，藉由不會對 隣接晶胞產生影響地使亮點暗點化，可有效地提高液晶顯 〇不面板之產率。因此，本發明之產業利用性可說是極高。 【圖式簡單說明】 第1圖係顯示習知液晶顯示面板之晶胞結構的截面圖。 第2圖係顯示在第1圖所示之晶胞結構中使用雷射使彩 色濾光片之透光率降低時所產生之問題點的截面圖。 16 200827819 第3圖係顯示彩色濾光片之透光率特性的圖表。 第4圖係顯示本發明之一實施形態之液晶顯示面板之 修復過程的流程圖。 第5A圖係顯示本發明之一實施形態之液晶顯示面板之 5 修復裝置的方塊圖。 第5B圖係顯示實現液晶顯示面板之修復裝置之例的立 體圖。 第5C圖係顯示實現第5B圖之液晶顯示面板之修復裝 置中之雷射及光學部之例的圖式。 10 第6A圖及第6B圖係藉由本發明之一實施形態使彩色 濾光片形成間隙之情形的截面圖， 第7A圖、第7B圖及第7C圖係顯示藉由本發明之一實施 形態使物理性質變化，以降低彩色濾光片之透光性之情形 的截面圖。 17 200827819 【主要元件符號說明】 11…薄膜電晶體玻璃 22...氣泡 12...半導體電路層 40…修復裝置 13...像素電極 41…第1雷射產生器 14...配向膜 42…第2雷射產生器 15…液晶層 43...雷射傳達路徑 16...共通電極 44…第1雷射 17...彩色濾光片 45...第2雷射 18…黑色矩陣 46...液晶顯不面板 19...彩色濾光片玻璃 47…瑕jSL晶胞 21…雷射 S1〜S3···步驟 18Excellent chemical properties. θ > I The reason is that the energy of the second laser must be concentrated in the portion formed by the gap of the color filter, and the concentrated energy can be diffused to other parts through the vibration of the crystal of the molecule. Usually, the time required for the lattice vibration of the molecule is in nanosecond units, whereby the physical properties of the color filter can be smoothly exhibited when using a femtosecond laser that concentrates energy in a very short period of time. 15 On the other hand, in a continuous laser generator, a photodiode laser generator that produces a continuous laser of 408 (±8) nm or a photodiode laser generator that produces a continuous laser of 446 nm is used. In the case of the color filter, the physical properties of the color filter are excellent. Fig. 5B is a perspective view showing an example of a repair device for a liquid crystal display panel. The laser and optical sections (corresponding to 40 of Fig. 5A) are movable in the γ-axis direction, and the stage mounted on the liquid crystal display panel (corresponding to 46 of Fig. 5A) is movable in the X-axis direction. In this way, the laser, the optics and the stage can move relative to each other so that the laser corresponds to the unit cell to be repaired. 14 200827819 The Laser and Optics section contains a first laser generator (corresponding to 41 of Figure 5A) that produces a laser for forming a gap in a color filter, which produces a physical H-quality for the color filter. The second laser generator of the changing laser (corresponding to 42 of Fig. 5A) and the laser transmitting path from the laser of the laser generator to the laser cell of the fatigue cell (corresponding to 5A® 43). Fig. 5C is a view showing an example of a laser and an optical portion in the repairing apparatus for realizing the liquid crystal display panel of Fig. 5B. The laser and optics contain laser generation and laser propagation paths. The laser transmission path includes a collimator that improves laser straightness, an attenuator with adjustable 10-section laser output, a lens, a beam, a beam splitter, and a mirror. To achieve the object of the present invention, a laser generator for changing the physical properties of the color illuminator and a ray for transmitting the laser generated by the laser generator to the color filter of the plague cell can be provided. Shoot the path. Therefore, the laser and optical portion shown in Fig. 5C is only an example, and the arrangement of the attenuator, the lens, the beam, the beam splitter, and the mirror can be changed. In addition, the aforementioned optical elements may be deleted or added as needed. Figs. 6A and 6B are cross-sectional views showing a state in which a color filter is formed into a gap by an embodiment of the present invention. Fig. 6A is a photograph showing a case where the first laser beam is irradiated to the color filter of the bright spot cell 2 to form a gap of 46 〇 nm, and Fig. 6B is a photograph of the case where the gap of 736 nm is formed. As shown in these figures, the gap is not formed in the vertical direction but in the horizontal direction. Fig. 7A, Fig. 7B and Fig. 7C are photographs showing the case where the physical properties of the sorrow are changed to reduce the light transmittance of the color filter by one of the inventions. In particular, the 7A, 7B, and 7C images are photographs of a situation in which the physical properties of the gamma wave are changed around the gap when the laser beam is irradiated on the color fascia formed by the gap. - 5 Fig. 7A shows the change in physical properties around the gap when the laser is irradiated with an intensity of 82 degrees, and Fig. 7B shows the change in the physical properties around the gap when the laser is irradiated with an intensity of 84 degrees, On the other hand, when the laser is irradiated with the intensity of 86 degrees, the physical properties around the gap are changed. As a result, as the laser energy increases, the thickness of the portion of the physical property changes increases. Thus, the portion of the physical property change of the color filter can block the light, so that when the physical property change portion has a certain thickness or more, the bright spot cell can become a dark spot cell. However, since there is a possibility that the unit cell becomes bulky, it is important to maintain the physical property change portion at an appropriate thickness. 15 Industrial Applicability According to the present invention, the influence on the adjacent unit cell of the liquid crystal display panel can be minimized by changing the physical properties of the color filter of the germanium unit cell. Further, in the method and apparatus for repairing a liquid crystal display panel, the bright spots are darkened without affecting the adjacent cells, and the yield of the liquid crystal display panel can be effectively improved. Therefore, the industrial applicability of the present invention can be said to be extremely high. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a cross-sectional view showing the cell structure of a conventional liquid crystal display panel. Fig. 2 is a cross-sectional view showing a problem occurring when a laser is used to reduce the light transmittance of the color filter in the unit cell structure shown in Fig. 1. 16 200827819 Figure 3 is a graph showing the light transmittance characteristics of a color filter. Fig. 4 is a flow chart showing the repair process of the liquid crystal display panel of one embodiment of the present invention. Fig. 5A is a block diagram showing a repairing apparatus of a liquid crystal display panel according to an embodiment of the present invention. Fig. 5B is a perspective view showing an example of a repairing device for realizing a liquid crystal display panel. Fig. 5C is a view showing an example of a laser and an optical portion in the repairing apparatus for realizing the liquid crystal display panel of Fig. 5B. 10A and 6B are cross-sectional views showing a state in which a color filter is formed into a gap by an embodiment of the present invention, and FIGS. 7A, 7B, and 7C are diagrams showing an embodiment of the present invention. A cross-sectional view of a situation in which the physical properties are changed to reduce the light transmittance of the color filter. 17 200827819 [Description of main component symbols] 11... Thin film transistor glass 22... Bubble 12... Semiconductor circuit layer 40... Repair device 13: Pixel electrode 41... First laser generator 14... Alignment film 42...second laser generator 15...liquid crystal layer 43...laser transmission path 16...common electrode 44...first laser 17...color filter 45...second laser 18... Black matrix 46... Liquid crystal display panel 19... Color filter glass 47...瑕jSL unit cell 21...Laser S1~S3···Step 18