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TW200827821A - Apparatus and method for blacking liquid crystal using laser - Google Patents

Apparatus and method for blacking liquid crystal using laser Download PDF

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Publication number
TW200827821A
TW200827821A TW096148359A TW96148359A TW200827821A TW 200827821 A TW200827821 A TW 200827821A TW 096148359 A TW096148359 A TW 096148359A TW 96148359 A TW96148359 A TW 96148359A TW 200827821 A TW200827821 A TW 200827821A
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TW
Taiwan
Prior art keywords
laser
liquid crystal
crystal display
wavelength
blackening
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TW096148359A
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Chinese (zh)
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TWI340840B (en
Inventor
Il-Ho Kim
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Cowin Dst Co Ltd
Il-Ho Kim
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Publication of TW200827821A publication Critical patent/TW200827821A/en
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/1306Details
    • G02F1/1309Repairing; Testing
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/1303Apparatus specially adapted to the manufacture of LCDs
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2201/00Constructional arrangements not provided for in groups G02F1/00 - G02F7/00
    • G02F2201/50Protective arrangements
    • G02F2201/506Repairing, e.g. with redundant arrangement against defective part
    • G02F2201/508Pseudo repairing, e.g. a defective part is brought into a condition in which it does not disturb the functioning of the device

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Optics & Photonics (AREA)
  • General Physics & Mathematics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Electromagnetism (AREA)
  • Liquid Crystal (AREA)
  • Manufacturing & Machinery (AREA)
  • Plasma & Fusion (AREA)
  • Devices For Indicating Variable Information By Combining Individual Elements (AREA)
  • Laser Beam Processing (AREA)

Abstract

The present invention relates to a blacking apparatus and method, which eliminate light leakage caused by impurities present in liquid crystal cells. The apparatus for blacking a liquid crystal panel according to the present invention includes a laser oscillation unit (100), a beam delivery unit (120), and a scan unit (130). The laser oscillation unit includes a plurality of laser oscillators, beam adjustment means for adjusting intensity of a laser beam emitted from each laser oscillator, beam formation means for converting a profile of the laser beam, and a half mirror having characteristics for selectively transmitting or reflecting the laser beam. The beam delivery unit switches a direction of the laser beam. The scan unit adjusts a direction of the laser beam so that the laser beam is radiated onto a region of the liquid crystal panel desired to be blacked.

Description

200827821 九、發明說明: 【發明所屬之技術領域】 本發明係關於一種修補液晶顯示器(LCD; Liqujd Crystal Display Device)缺陷的方法’尤其是一種消除液 晶單兀内部因雜質而發生之漏光現象的黑化裝置及方法。 【先别技術】 近來’液晶顯示器因電力消耗低、攜帶方便、技術含 里尚、且附加價值高,而被認爲是下一代尖端顯示元件。 - 這樣的液晶顯示器,係具有可切換各像素施加電壓之切換 (switching)元件的有源矩陣(actjve matrix)型液晶顯 示裝置’因其較高的清晰度及影像顯示功能而備受關注。 液晶顯示器採用上部基板(substrate )彩色濾光片及 下4基板/專膜%效應電晶體TFT(Thin Film Transistor)陣 列基板的雙向結合,在其中間形成具有介電異向性 (Dielectric Anisotropy)的液晶層構造,藉由像素選擇用的 定址佈線來切換啓動附加有數十萬個像素的薄膜場效應電 u 晶體TFT,並按照對相應之像素施加電壓的方式進行驅動。 爲製造上述液晶顯示器,則需進行薄膜場效應電晶體 T F T陣歹j基板處理、彩色遽光片基板處理、液晶單元處理 上述薄膜場效應電晶體TFT陣列基板是藉由反復的沈 積、光刻、钱刻等處理,在玻璃基板上形成門(gate )佈 線、資料佈線、薄膜場效應電晶體及像素電極的處理。 上述彩色濾光片基板處理是在形成黑矩陣(black 5 200827821 matrix )的玻璃基板上按照一定的順序排列並設置會顯示 顏色之紅-綠藍(RGB)的彩色濾色層後,用銦錫氧化物 (Indium Tin Oxide,ITO)膜形成共同電極的處理。 另外,液晶單元處理是在維持一定縫隙的狀態下結合 薄膜場效應電晶體TFT陣列基板和彩色濾光片陣列基板, 並在其縫隙間注入液晶形成液晶層的處理。 在上述液晶顯示裝置的檢查過程中,在液晶顯示器的 晝面中顯示測試圖(test pattern )來判斷有無不合袼像素, 找到不合格像素時’對此進行修補。液晶顯示器的不合格 可分爲點缺陷、線缺陷、顯示不均勻,其中TFT元件、像 素電極H慮光片佈線不合格等引發點缺陷;佈線之間 的開路、短路、靜電引起的TFT破壞、驅動電路及接觸不 良可引發線缺陷;單元厚度的不均句、液晶取向的不均句、 TFT在特定點漫射或相對較高瞬變時間常數可引發顯示不 均勻。其中’點缺陷及線缺陷—般是因爲佈線的不合格引 起的’以往如發現開路(Gpen)的佈線,將開路的部分連 接,如有短路(short)就把相關佈線進行開路。 除此之外,還有有的像素單元發出特別亮光的現象, 勺視見s s很谷易察覺到這樣特定點的漏光現象,發現 ^属光現象的液晶顯示器就被分爲不合格産品。但是,漏 佈線的開路或短路無關,以往藉由加工處理佈線 的技術無法解決此問題。 液晶顯示器的過程中會吸附包括灰塵'有機物或 以❹的雜質’這樣的雜質如被吸附在彩色渡光片附 200827821 近’"亥像素單元在被驅動時就會發出比別的正常像素單元 更党的光’即引發形成漏光現象的亮度不合格像素,在顯 示器檢查過程中可能被分爲不合格産品。而利用雷射消除 這種雜質之方法的研究工作正在進行。 日本專利2006— 72229公開了以下技術:對取向膜照 射雷射而改變液晶的排列特性,由此降低光對液晶的透過 率’而消除漏光現象。但是這些方法不能完全消除排列特 性’並且程序需要更多的時間。 另外,韓國專利2006_ 65134公開了將雷射照射到取 向膜上使之半透明的修補技術。上述雷射採用的是鉉 (Neodymium) YAG雷射、二極體、二氧化碳(c〇2)雷 射等。但是上述方式中,通常使用的是具有納秒脈衝幅度 的雷射,將其照射到要進行修補的基板時,範圍因爲熱擴 散的原因會損傷基板的其他範圍,而使液晶基板成爲不合 格叩。特別是,光澤不足(hazing)處理有機物層時,進 ’光澤不足(hazing)處理而用雷射照射的面積相比有機 物的面積小不僅需要較長的加工時間,而且不適用於大量 生産産品的工廠生產線中。 【發明内容】 、本發明的目的是爲解決上述問題,提供一種有效消除 液晶顯示器漏光現象的黑化裝置及方法。並且,本發明在 進^黑化處理時,可選擇性地使用薄膜吸收波譜較高頻帶 的雷射光束,而達到減少雷射光束能量損失的效果。另外, 本發明提供一種藉由調整雷射光束的強度及照射面積來提 200827821 ,黑化處理速度,減調整黑化處理厚度的裝置及方法。 最後,本發明提供一種雷射光束的照射方式採用範圍 (scope)或掃描方式,不僅可以提高黑化的速度,並能 調整黑化處理厚度的黑化處理裝置及方法。 本發明提供一種液晶顯示器黑化裝置,包括: 多個雷射振蕩器; 光束調整單元,用於調整上述雷射振蕩器輸出的光束 強度; 雷射振蕩單元,包括變換上述雷射光束輪廓的光束形 成單元及具有選擇性地透射或反射上述雷射光束的半透半 反鏡(half mirror); 光束傳遞單元,轉換上述雷射振蕩單元雷射光束方 向; 掃描單元,調整光束的方向使上述雷射光束照射到需 要黑化的部位。 【實施方式】 以下結合附圖對本發明的較佳實施例做詳細說明。 第一圖是本發明黑化裝置組成圖,具有雷射振蕩單元 100 ;調整上述雷射振蕩單元100照射的雷射光束路徑的 光束傳遞單元120 ;調整上述光束傳遞單元12〇的光束使 其照射到目標物的掃描單元1 30。 上述雷射振蕩單元1 〇 〇包括··多個雷射振蕩器1 〇 1、 102、103 ;調整雷射光束的強度、角度或偏光的雷射光束 調整單元104、105、1〇6;將雷射光束的輪廓變換爲平頂 200827821 狀的光束形成單元107、108、109 ;透射或反射上述雷射 振蕩器101、102、103振蕩出之雷射光束的第一、第二半 透半反鏡1 1 0、111及雷射控制器。 上述雷射振蕩器101、102、103可使用雷射二極體、 雷射二極體模組或二極體激發式固態(Di〇de Pumped Solid State,DPSS〉雷射光源。另外,上述雷射振蕩器1 〇1、ι 〇2、 1 0 3較佳的是使用紅色波長、綠色波長及近紅外線波長帶200827821 IX. Description of the Invention: [Technical Field] The present invention relates to a method for repairing defects of a liquid crystal display (LCD), in particular, a black method for eliminating light leakage caused by impurities inside a liquid crystal cell Device and method. [Previous technology] Recently, liquid crystal displays are considered to be the next generation of sophisticated display elements due to their low power consumption, convenient carrying, high technology, and high added value. - Such a liquid crystal display is an active matrix type liquid crystal display device having a switching element capable of switching a voltage applied to each pixel, and has attracted attention due to its high definition and image display function. The liquid crystal display adopts a bidirectional combination of an upper substrate color filter and a lower substrate/substrate transistor (Thin Film Transistor) array substrate, and a dielectric anisotropy is formed therebetween. In the liquid crystal layer structure, a thin film field effect electric u crystal TFT to which hundreds of thousands of pixels are added is switched by an address wiring for pixel selection, and is driven in such a manner as to apply a voltage to the corresponding pixel. In order to manufacture the above liquid crystal display, a thin film field effect transistor TFT array substrate processing, a color light beam substrate processing, and a liquid crystal cell processing are required. The thin film field effect transistor TFT array substrate is repeatedly deposited, photolithographically processed, Processing such as money etching, forming gate wiring, data wiring, thin film field effect transistor, and pixel electrode processing on a glass substrate. The color filter substrate processing is performed by placing a color filter layer of red-green-blue (RGB) which displays colors in a predetermined order on a glass substrate on which a black matrix (black 5 200827821 matrix) is formed, and then using indium tin. An oxide (Indium Tin Oxide, ITO) film forms a common electrode. Further, the liquid crystal cell processing is a process of bonding a thin film field effect transistor TFT array substrate and a color filter array substrate while maintaining a certain gap, and injecting liquid crystal between the slits to form a liquid crystal layer. During the inspection of the liquid crystal display device described above, a test pattern is displayed on the face of the liquid crystal display to determine whether or not there is a non-conforming pixel, and when the defective pixel is found, it is repaired. The failure of the liquid crystal display can be classified into point defects, line defects, and display unevenness, in which the TFT element, the pixel electrode H is inferior to the wiring of the photoreceptor, and the like; the open circuit, the short circuit, the TFT damage caused by the static electricity, Driving circuits and poor contact can cause line defects; unevenness of cell thickness, unevenness of liquid crystal orientation, diffusion of TFT at a specific point, or relatively high transient time constant can cause display unevenness. Among them, the 'point defect and the line defect are caused by the failure of the wiring. In the past, if the wiring of the open circuit (Gpen) was found, the open portion was connected, and if there was a short circuit, the relevant wiring was opened. In addition, there are some pixel units that emit special bright light. The spoon sees s s, and it is easy to detect the light leakage phenomenon at such a specific point. It is found that the liquid crystal display which is a light phenomenon is classified into a non-conforming product. However, the open circuit or the short circuit of the drain wiring is irrelevant, and the conventional technique of processing the wiring cannot solve the problem. In the process of liquid crystal display, impurities such as dust 'organic matter or impurities such as ruthenium' are adsorbed, such as being adsorbed on a color light-emitting sheet attached to 200827821. The ''pixel' unit is driven to emit more normal pixel units than when it is driven. The more party's light's brightness-inferior pixels that cause the formation of light leakage may be classified as substandard products during the display inspection process. Research work is being carried out using lasers to eliminate such impurities. Japanese Patent No. 2006-72229 discloses a technique of irradiating a laser to an alignment film to change the alignment characteristics of the liquid crystal, thereby reducing the transmittance of light to the liquid crystal, and eliminating the light leakage phenomenon. But these methods do not completely eliminate the permutation characteristics' and the program takes more time. Further, Korean Patent No. 2006_65134 discloses a repairing technique of irradiating a laser onto a facing film to make it translucent. The above-mentioned laser uses a neodymium YAG laser, a diode, a carbon dioxide (c〇2) laser, and the like. However, in the above method, a laser having a nanosecond pulse width is generally used, and when it is irradiated onto the substrate to be repaired, the range of the substrate is damaged due to thermal diffusion, and the liquid crystal substrate becomes unsatisfactory. . In particular, when the organic layer is hazing, the area subjected to laser irradiation is less than the area of the organic material, which requires a longer processing time and is not suitable for mass production. In the factory production line. SUMMARY OF THE INVENTION An object of the present invention is to provide a blackening apparatus and method for effectively eliminating light leakage from a liquid crystal display in order to solve the above problems. Moreover, in the blackening process of the present invention, the film can selectively use a laser beam having a higher frequency band of the absorption spectrum to achieve the effect of reducing the energy loss of the laser beam. In addition, the present invention provides an apparatus and method for improving the blackening processing speed and reducing the thickness of the blackening treatment by adjusting the intensity and the irradiation area of the laser beam. Finally, the present invention provides a blackening processing apparatus and method that can not only increase the speed of blackening but also adjust the thickness of the blackening treatment by using a scope or a scanning mode of the laser beam. The invention provides a liquid crystal display blackening device, comprising: a plurality of laser oscillators; a beam adjusting unit for adjusting a beam intensity output by the laser oscillator; and a laser oscillation unit comprising a beam for transforming the contour of the laser beam Forming a cell and a half mirror having a selective transmission or reflection of the laser beam; a beam transfer unit that converts a direction of the laser beam of the laser oscillation unit; and a scanning unit that adjusts a direction of the beam to make the thunder The beam is irradiated to a portion where blackening is required. [Embodiment] Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings. The first figure is a composition diagram of the blackening device of the present invention, which has a laser oscillating unit 100; a beam transmitting unit 120 for adjusting a laser beam path irradiated by the laser oscillating unit 100; and adjusting the beam of the beam transmitting unit 12 to illuminate To the scanning unit 1 30 of the target. The above-mentioned laser oscillating unit 1 〇〇 includes a plurality of laser oscillators 1 102 1, 102, 103; laser beam adjusting units 104, 105, 1 〇 6 that adjust the intensity, angle or polarization of the laser beam; The contour of the laser beam is transformed into a flat-topped 200827821 shaped beam forming unit 107, 108, 109; the first and second transflective beams that transmit or reflect the laser beam oscillated by the laser oscillators 101, 102, 103 Mirror 1 1 0, 111 and laser controller. The above laser oscillators 101, 102, and 103 may use a laser diode, a laser diode module, or a diode-excited solid state (DPSS) laser source. The oscillators 1 〇1, ι 〇2, and 1 0 3 preferably use red, green, and near-infrared wavelength bands.

域的雷射。根據需要上述近紅外線波長帶域可替代使用青 色波長雷射。 上述光束形成單元107、1〇8、1〇9包括:光束整形器 (beam shaper),其係用於擴大可進行處理的範圍,並 使光束的形狀平滑;光束狹縫(beam s|jt),根據要黑化 的範圍(即處理範圍的大小)調整照射光束大小。 … 工処尤采得遞單 V ,丨,π I _咐尤术路徑方 向勺轉換鏡1 21、1 22。本實施例中雖標有兩個方向轉換 鏡121、122 ’但根據雷射振蕩單元1〇〇及目標物140的 位置:上述方向轉換鏡⑵、122的數量及位置可 化。上述光束傳遞單元12〇反射從雷射振蕩單元_ 振“之所有波長的雷射光束,因此要設計爲可在寬範圍 使用。第六圖是光束傳遞單元方向轉換鏡' «項曲㈣。(a)設計歧射35Q〜 2 = 内所有範圍波長,rh、土 * unm乾圍波段 ^Λ 0 考慮到能夠照射到的雷射波長, 8又汁馬只反射對應波長帶域。 长 上述掃福單元130包括:2軸移動掃描單元131,用 9 200827821The laser of the domain. The above-mentioned near-infrared wavelength band can be used instead of the cyan wavelength laser as needed. The beam forming units 107, 1〇8, 1〇9 include: a beam shaper for expanding the range in which processing is possible and smoothing the shape of the beam; beam slits (beam s|jt) The size of the illumination beam is adjusted according to the range to be blackened (ie, the size of the processing range). ... The office has a special order V, 丨, π I _ 咐 咐 路径 path conversion mirror 1 21, 1 22. In the present embodiment, the two direction changing mirrors 121, 122' are marked, but the number and position of the above-described direction converting mirrors (2), 122 can be made according to the positions of the laser oscillation unit 1 and the target 140. The above-mentioned beam transfer unit 12 〇 reflects the laser beam of all wavelengths from the laser oscillating unit _ vibration, and therefore is designed to be used in a wide range. The sixth picture is the beam transfer unit direction conversion mirror' «Item (4). a) Design the astigmatism 35Q~ 2 = all wavelengths within the range, rh, soil * unm dry band ^ Λ 0 Considering the laser wavelength that can be irradiated, 8 the juice horse only reflects the corresponding wavelength band. The unit 130 includes: a 2-axis mobile scanning unit 131, with 9 200827821

於调整上述雷射光束焦點距離;電荷耦合器件(eh「胩 。响device,CCD)攝像機133,用於觀察上述雷射光 束是否照射在液晶顯示器的正確目標140上;連接裝置 W2,連接上述2軸移動掃描單元131和ccd攝像機⑶ 的攝像機;包括變換光束方向的χ軸檢流計鏡和 Y轴檢流計鏡134-2的χγ軸移動掃描單元134;掃描鏡 (scan lens),對由上述移動掃描器134來改變方向 的雷射光束進行集束;照明光源136,用於得到清晰的影 像。爲滿足光束傳遞單元及第六圖中曲線圖的特性,上述 X軸檢流計鏡134— 1和Y軸檢流計鏡134_2也進行週邊 ^鍍(coating)處理。上述掃描鏡135不僅起集束作用, 逛可以藉由CCD攝像機133觀察雷射光束照射在液晶顯 示器上形成的影像。 、 苐一圖疋吸附了雜質的液晶顯示器之剖面圖,包括: 包含丨τ〇膜210和有機物材質的彩色濾光片22〇、黑矩陣、 取向膜(圖中未示)、偏光臈280、保護膜(圖中未示)、 防反射膜(圖中未示)的第一基板240 ;液晶層250 ;包 含TFT(圖中未示)和取向膜(圖中未示)及偏光膜(圖中 未示)的第二基板260b。 製造液晶顯示器的過程中會吸附包括灰塵、有機物或 至屬在内的雜質270’這樣的雜質270如被吸附在彩色淚 光片220附近,在驅動該像素單元時就會發出比別的正常 像素單元更亮的光,即引發形成漏光現象的亮度不合格像 素’在顯示器檢查過程中可能被認爲是不合格産品。這時 10 200827821 候,利用上述黑化裝置對吸附雜質的液晶顯示器像素進行 黑化處理,調整到肉眼不能察覺的程度,就可以以合袼産 品出廢。 以下透過由上述構造組成的黑化裝置說明消除液晶顯 示器的漏光現象所進行的處理過程,即黑化處理。 首先,藉由檢測裝置檢測出液晶顯示器彳40中引發形 成漏光現象的亮度不合格像素,如果檢測出不合格像^ ^ 驅動控制單元150把液晶顯示器14Q移動到黑化裝置中。 本發明的驅動控制單元15〇包括:板台(pane|stage) (圖中未示),用於將液晶顯示器140向X、Y、z軸移 動或回轉,並裝載、卸載液晶顯示器14〇,以使將不合样 像素位置移動到雷射照射的位置上;控制臺(咖⑽ stage )(圖中未示)係用於 戰隹板口後,可使雷射照射 在不合袼像素位置上;批涂丨 , …”置上,控制“圖中未示)係用於控制上 述控制$和板台動作。利用 s§ - 4 %勒控制早兀1 50將液晶 顯不益140移動到黑化裝置中, 一 古 稭由田早70 1 30來判斷 冗度不合格像素的位置。 確定不合格像素亮度的位置後 中rrn m 積由幹描早το 130確 疋CCD攝像機133拍攝 置。此日像,來確定準確的處理位 置此盼可猎由CCD攝像機133Adjusting the focus distance of the laser beam; a charge coupled device (eh "device", CCD) camera 133 for observing whether the laser beam is irradiated on the correct target 140 of the liquid crystal display; connecting device W2, connecting the above 2 a camera that moves the scanning unit 131 and the ccd camera (3); includes a 检-axis galvanometer mirror that converts the beam direction and a χ-axis movement scanning unit 134 of the Y-axis galvanometer mirror 134-2; a scan lens The moving scanner 134 is used to change the direction of the laser beam to be bundled; the illumination source 136 is used to obtain a clear image. To satisfy the characteristics of the beam transfer unit and the graph in the sixth figure, the X-axis galvanometer mirror 134 is The 1 and Y-axis galvanometer mirrors 134_2 are also subjected to a peripheral coating process. The scanning mirrors 135 not only function as a cluster, but also can observe the image formed by the laser beam on the liquid crystal display by the CCD camera 133. A cross-sectional view of a liquid crystal display in which impurities are adsorbed, including: a color filter 22 including a 丨τ〇 film 210 and an organic material, a black matrix, an alignment film (not shown) a polarizing plate 280, a protective film (not shown), a first substrate 240 of an anti-reflection film (not shown), a liquid crystal layer 250, and a TFT (not shown) and an alignment film (not shown) and a second substrate 260b of a polarizing film (not shown). During the process of manufacturing the liquid crystal display, impurities such as impurities 270, including dust, organic matter or genus, are adsorbed, such as being adsorbed near the colored tear film 220, When the pixel unit is driven, light that is brighter than other normal pixel units is emitted, that is, the luminance defective pixel that causes the light leakage phenomenon to be formed may be regarded as a defective product during the display inspection. At this time, 10 200827821 By using the above-mentioned blackening device to blacken the pixels of the liquid crystal display that adsorb the impurities, and to adjust to the extent that the naked eye can not perceive, the combined products can be disposed of. Hereinafter, the blackout device composed of the above structure is used to eliminate the light leakage of the liquid crystal display. The processing performed by the phenomenon, that is, the blackening process. First, the brightness of the liquid crystal display 彳40 causing the light leakage phenomenon is detected by the detecting device. If the pixel is detected, the drive control unit 150 moves the liquid crystal display 14Q into the blackening device. The drive control unit 15 of the present invention includes: a pane|stage (not shown), For moving or rotating the liquid crystal display 140 to the X, Y, z axes, and loading and unloading the liquid crystal display 14 以 to move the unsuited pixel position to the position of the laser irradiation; the console (ca) The figure is not shown in the figure. After being used in the trench, the laser can be irradiated at the position of the non-aligned pixel; the batch is coated, ...", and the control "not shown" is used to control the above control and Plate action. Using s§ - 4 % 勒 兀 兀 兀 将 将 将 将 将 液晶 液晶 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动 移动After determining the position of the unacceptable pixel brightness, the rrn m product is determined by the CCD camera 133. This day image, to determine the exact processing position, this hope can be hunt by the CCD camera 133

攝像機> 進仃即蚪監控,透過CCD 攝彳冢機133確定亮度不合格 晶顯示器膜,铁後戌叙μ + ”的位置及要進行黑化的液 肤…'後啓動上述雷射振蕩單元1〇〇。 根據要進行黑化的膜種 軟體潠摆##& 不问,利用事先運算好的 軟-選擇振蕩出不同雷射的波長及輪出。 ^ 11 200827821 =振蕩單元⑽單獨顯示3種波長,這 雷射抵圍分別爲紅色波長範_ 1〇1、近紅外線波長雷 射1〇2範圍及綠色波長範圍的雷射1〇3,雷射1〇1、1〇2、 ⑽分別由雷射專用控制器112進行控制。可料色波長 ^ 軌圍也可使用紫外線或近紫外線波長範圍的雷射。 i外線或近紫外線波長不受液晶顯示器膜顏色(R,G B)The camera> is monitored immediately, and the CCD camera 133 is used to determine the brightness of the crystal display film, and the position of the iron and the liquid to be blackened... 1〇〇. According to the film type to be blackened, ##& Do not ask, use the soft-option calculated in advance to oscillate the wavelengths of different lasers and turn out. ^ 11 200827821 = Oscillation unit (10) is displayed separately Three kinds of wavelengths, the laser is bounded by red wavelength range _1〇1, near-infrared wavelength laser 1〇2 range and green wavelength range of laser 1〇3, laser 1〇1,1〇2, (10) They are controlled by the laser-specific controller 112. The color wavelength can also be used for lasers in the ultraviolet or near-ultraviolet wavelength range. i The external or near-ultraviolet wavelength is not affected by the liquid crystal display film color (R, GB).

的影響,r㈣在所有範圍内都能被吸收,可不受薄膜顏色 的影響,被選擇使用。 _以下,以具備紅色波長範圍的雷身ί 101、近紅外線波 長範圍的雷射1G2、綠色波長範圍的雷射1G3 單元100爲基準做詳細說明。 根據不合格像素的位置及要進行黑化的膜,來選擇該 膜所吸收波長⑽圍的雷射振蕩器,所選的雷射振蕩器振蕩 出的雷射光束通過光束調整單元104、105、106調整其角 度、強度及偏光,藉由光束形成單元1G7、⑽、⑽使光 束輪廓變平滑的同日夺,調整光束大小與要黑化的位置大小 一致。、另外,透過2個半透半反鏡11〇、川,各雷射光 束來成-個光束。ϋ由上述方法,使照射的光束的能量分 佈均勻的同時,可調整大小,因此可將光束以掃描的方式 知射到要黑化的部位,來進行黑化,㈣也可調大光束, 以整塊輻身“b丨〇ck shot)的方式進行照射(對要進行黑 化的部分只照射一次光束的方式)。 第一半透半反鏡110透射紅色波長範圍的雷射1〇1, 12 200827821 反射近紅外線範圍的雷射102;第二半透半反鏡彳11透射 紅色波長範圍的雷射1 01和近紅外線範圍的雷射1 02,反 射綠色波長範圍的雷射1 03。 第三圖的(a)和(b)是分別根據第一半透半反鏡11〇的 波長的透射和反射的曲線圖,第四圖的和(㈨是分別根 據第二半透半反鏡111的波長的透射和反射的曲線圖。即, 第一半透半反鏡110和第二半透半反鏡彳彳彳的透射或反射 的波長不同,因此要根據雷射波長的特性進行設計和塗鍍 (coating)。第一半透半反鏡11〇和第二半透半反鏡 的透射和反射特性可根據雷射振蕩器及上述半透半反鏡的 特性進行多樣的變化。 如前所述,上述光束調整單元1〇4、1〇5、1〇6將振蕩 的雷射光束調整到適合進行黑化處理的狀態。如果輸出的 雷射強度太大,會損傷到要進行黑化處理的膜以外的其他 指’攸而使整個液晶顯示器變成廢品。雷射被調整到適 當狀態後,藉由雷射光束形成單元1〇7、1〇8、1〇9,再藉 由半透半反鏡11G、川,^後被光束傳遞單元⑵轉^ 方向,入射到Z轴移動掃描單元131。雷射光束被掃描器 131和掃描鏡135聚光後,照射到液晶顯示器⑽上。雷 射光束照射的同時’藉由χγ軸移動掃描單元134移動所 需大小及形狀的雷射光束’來對薄膜進行黑化。 對構成液晶顯示器14 〇从1时匕 盗Μϋ的溥膜進行黑化的處理過 中’可藉由掃描鏡135看5丨|沾忐w 拉壯 看到的處理的影像反射到攝像機連 接裝置132内的影像半透半 成連 久鏡132-1上,並傳遞到ccd 13 200827821 攝像機133上,可進行即時監控。此時,可根據需要,攝 像機連接裝置1 32插入用於可擴大或縮小影像的中繼透鏡 (relay lens)(圖中未示)或爲得到清晰的影像消除一定 波段波長的載止濾光片(Cut-Offfiiter)(圖中未示)。 第五圖是掃描鏡1 35及照明光源1 36的放大圖。 如圖所示,照明光源136環設在掃描鏡135的週邊。 上述照明光源1 36包括多個LED照明1 37。上述照明光源 136在藉由掃描鏡135將處理的影像傳遞到CCD攝像機 133時,被聚成比處理範圍稍大的大小,以補充不足的光 亮。 例如,如果要黑化LED板彩色濾光片的RGB中之一 個像素,就要使用各像素吸收波譜最廣波長的雷射。爲消 除各像素,如上述構成的雷射振蕩器内部可選擇性地振蕩 輸出各個雷射,因此可高效率地黑化像素。 上述雷射振蕩單元1 〇〇根據要進行處理的彩色濾光片 玻璃(glass) 260a表面上偏光膜280的有無來選擇波長, 當黏貼偏光膜280時較佳的是使用紅色波長1〇1、綠色波 長103、近紅外線波長102範圍的雷射,當黏貼偏光膜之 前’較佳的是使用紅色波長101、綠色波長1〇3、藍色波 長1〇2—1範圍的雷射,即,可根據有無偏光膜,青色波 長102-1的雷射替代近紅外線波長1〇2的雷射。 更爲常用的是在液晶顯示器上結合使用偏光膜28〇進 行黑化處理,也適用於已完成的産品中。可在具有偏光膜 280的狀態下進行加工,也就可以在無偏光膜28〇下進行 200827821 加工。但疋波長越短,物質内的吸收度將會增加,如果沒 有偏光膜28Q _,代替近紅外線波長1 G2,使用青色波長 1 〇2_1的雷射其效果更好。 第七圖是液晶顯示器中彩色濾光片透過率曲線圖。 要黑化RGB中一個,就要參考上述曲線圖。例如, 要黑化具有530nm的波長範圍—綠色波長—如使用綠色波 長的雷射就會透射掉,所以不能進行黑化。The effect of r(iv) can be absorbed in all ranges and can be selected without being affected by the color of the film. _ Hereinafter, the laser 1G2 unit 100 having a red wavelength range, the laser 1G2 in the near-infrared wavelength range, and the laser 1G3 unit 100 in the green wavelength range will be described in detail. Selecting a laser oscillator surrounded by the wavelength (10) absorbed by the film according to the position of the defective pixel and the film to be blackened, and the laser beam oscillated by the selected laser oscillator passes through the beam adjusting unit 104, 105, 106 adjusts its angle, intensity, and polarization, and the beam forming unit 1G7, (10), and (10) smoothes the beam profile to the same day, and adjusts the beam size to coincide with the position to be blackened. In addition, through the two semi-transparent mirrors 11 and Sichuan, each of the laser beams is used to form a beam. ϋ By the above method, the energy distribution of the irradiated light beam is uniform, and the size can be adjusted. Therefore, the light beam can be scanned to the portion to be blackened to perform blackening, and (4) the large light beam can also be adjusted. Irradiation of the whole body "b丨〇ck shot" (the way in which only the primary beam is irradiated to the portion to be blackened). The first half mirror 110 transmits the laser 1红色1 in the red wavelength range, 12 200827821 Laser 102 reflecting the near-infrared range; the second half-transparent mirror 彳11 transmits the laser in the red wavelength range 1 01 and the laser in the near-infrared range 1 02, reflecting the laser in the green wavelength range 1 03. (a) and (b) of the three figures are graphs of transmission and reflection according to the wavelengths of the first half mirror 11 分别, respectively, and the sum of the fourth figure ((9) is according to the second half mirror 111, respectively. The transmission and reflection curves of the wavelengths. That is, the transmission wavelengths of the first half mirrors and the second half mirrors are different, so the design is based on the characteristics of the laser wavelengths. Coating. The first half of the mirror is 11 〇 and the second The transmission and reflection characteristics of the transflective mirror can be varied according to the characteristics of the laser oscillator and the above-mentioned half mirror. As described above, the beam adjusting units 1〇4, 1〇5, 1〇6 will The oscillating laser beam is adjusted to a state suitable for blackening. If the output laser intensity is too large, it will damage other fingers than the film to be blackened, and the entire liquid crystal display will become waste. After being adjusted to an appropriate state, the laser beam forming unit 1〇7, 1〇8, 1〇9 is further rotated by the beam transmitting unit (2) by the half mirror 11G, and then incident. Moving to the scanning unit 131 by the Z-axis. The laser beam is condensed by the scanner 131 and the scanning mirror 135, and then irradiated onto the liquid crystal display (10). While the laser beam is being irradiated, the scanning unit 134 is moved by the χ γ axis to move the required size and The shape of the laser beam 'is blackened the film. The blackening of the enamel film which constitutes the liquid crystal display 14 from 1 匕 ' ' ' ' ' ' ' ' ' ' ' 扫描 扫描 135 135 135 135 扫描 135 135 135 扫描 扫描Strongly seeing the processed image reflected to the camera The image in the machine connecting device 132 is half-transparent into the continuous lens 132-1 and transmitted to the ccd 13 200827821 camera 133 for real-time monitoring. At this time, the camera connecting device 1 32 can be inserted for use as needed. A relay lens (not shown) that enlarges or reduces the image or a Cut-Offfiiter (not shown) that eliminates a certain wavelength of wavelength for obtaining a clear image. An enlarged view of the scanning mirror 1 35 and the illumination source 136. As shown, the illumination source 136 is looped around the scanning mirror 135. The illumination source 136 includes a plurality of LED illuminations 137. When the processed light source 136 transmits the processed image to the CCD camera 133 by the scanning mirror 135, it is concentrated to a size slightly larger than the processing range to supplement the insufficient light. For example, if you want to blacken one of the RGB pixels of the LED board color filter, use the laser that absorbs the widest wavelength of the spectrum. In order to eliminate each pixel, the laser oscillator can be selectively oscillated and outputted inside the laser oscillator constructed as described above, so that the pixel can be blackened with high efficiency. The laser oscillation unit 1 选择 selects a wavelength according to the presence or absence of the polarizing film 280 on the surface of the color filter glass 260a to be processed, and when the polarizing film 280 is pasted, it is preferable to use a red wavelength of 〇1. A laser having a green wavelength of 103 or a near-infrared wavelength of 102 is preferably a laser having a red wavelength of 101, a green wavelength of 1 〇 3, and a blue wavelength of 1 〇 2 -1 before being attached to the polarizing film, that is, According to the presence or absence of a polarizing film, a laser having a cyan wavelength of 102-1 replaces a laser having a near-infrared wavelength of 1 〇 2 . More commonly used is the use of a polarizing film 28 on the liquid crystal display for blackening, and is also suitable for use in finished products. The processing can be carried out in a state in which the polarizing film 280 is provided, and the processing can be carried out under the unpolarized film 28 under the condition of 200827821. However, the shorter the wavelength of 疋, the higher the absorbance in the material. If there is no polarizing film 28Q _, instead of the near-infrared wavelength 1 G2, the laser with a cyan wavelength of 1 〇 2_1 is better. The seventh figure is a graph of the transmittance of the color filter in the liquid crystal display. To blacken one of RGB, refer to the above graph. For example, to blacken a wavelength range of 530 nm - green wavelength - if a laser using a green wavelength is transmitted, blackening cannot be performed.

第八圖是根據偏光膜波長的透射率曲線圖。 k圖可知在可見光波段具有5〇%以下的透射率,根本 不透射紫外線(UV)波段内的波長,越接近近紅外線範圍 透射率就會增大。因此如要黑化具有偏光膜的像素的rgb 中的一個時,較佳的是使用近紫外線範圍的雷射。 例如,如果黑化LCD板之彩色遽光片W RGB中的一 個像素’就要使用各像素吸收波譜最寬波長的雷射。爲消 ::像素’如上述構成的雷射振蕩器内可選擇性地振蕩輸 各個像素用的各個雷射,因此可高效率地黑化像素。例 ::如要黑化液晶顯示器中彩色濾光片的藍色⑻波段, ==波長的雷射;如要黑化紅色(…皮段,就要 用近,νί長的雷射;如要黑化綠色(G)波段,就要使 用近紅外線波長的雷射。 根據具體情況,如要愛介汸曰 时 II多、“ t黑化液晶顯不器中彩色濾光片的 -色波段,就要振蕩出黃色波 長的汝且、…、 (大於或等於黃色波 $ π Η、 $卜線波長以下波段的雷射;如要 …、、、工色波段,就要振舊屮έ年&、士 g 撖街出綠色波長以下或近紅外線波長 15 200827821 以上的雷射;如要黑化綠色波段,就要振蕩出青色波長以 下或黃色波長以上雷射。 雷射照射到薄臈中,構成薄膜的有機物就會發生分子 間的結合斷裂,釋放出包括中性原子、分子、正負離子的 等離子,自由基,離子簇(CLUSTER ),電子及光子 (PHOTON),然後被燒备(ABLA丁丨〇N)進行黑化。 燒# ( ABLATION)是構成有機物分子間的結合解離 成爲分子、離子等的現象,爲這樣的解離,有機物要吸收 能量級以上的能量。 第九圖是實施本發明的雷射光束的輪廓的曲線圖。 最初,雷射振蕩器照射的雷射以高斯( · 態能量集中在中間範圍。藉由這樣的雷射:束形成2 108 1 ( beam shaper 或 homogennizer),在 一定範圍内使雷射光束強度m,並變換成擴大的平頂 的輪廓’騎與光束輪廓一起雷射的照射面積同時也發生 變化。此時可變換爲四角平頂3〇〇或圓形平頂形態期。 …根據本發明的實施例’制光束形成單元和光束調整 調整照射的雷射光束的大小及強度,照射的雷射光 述-射Π小’黑化整個多數像素所需的時間越長。將上 束的大小變的均句,可適用於進行大量生産的生 產線中。變換成摘♦士 301 角平頂3〇0或圓形平頂形態 的雷射,經由Z軸移動掃 多個薄膜中的RGB料將、成液晶顯示器的 1豕京黑化到所需厚度。 弟十圖4明根據要黑化的薄膜的厚度,對所需厚度的 16 200827821 :膜進仃消除黑化處理而設計的焦點會聚範圍(De_ 咖s,D0F)的概略圖。即,消除所需厚度的薄模後重 新凋整焦距去除的過程。 、 利用z軸移動掃描單元131,把D〇 素厚度的㈣的範圍對齊後,制χγ軸移動掃描單:: '亍,.、、化利用CCD攝像機確認黑化程度,黑化不足時, 重新移動Ζ軸移動掃描單元131的位置,冑D〇F與相當 於像素厚度20%的範圍對齊後,利肖χγ軸移動掃描: =134進行请除。反復進行2~4次消除後,黑化達到滿意 私度,就終止黑化。爲下一步處理做準備。 第十一圖是根據上述步驟移動焦點距離進行黑化處理 的流程圖。 如圖所示,最初照射雷射光S1〇,完成1〇%的黑化 S20 ’確認黑化程度S30後,判斷是否滿足黑化程度s4〇, 如黑化達到要求就終止黑化S5〇,沒達到要求,z軸移動 S60焦距重新照射雷射進行黑化程式。 焦點會聚範圍在不超過1pm的範圍内,根據Z軸移動 掃描單元1 31和掃描鏡1 35的焦距及入射光束的直徑進行 計算。 數學式1 DOF = ^/2(NA)2 數學式2 NA = nsin0 數學式3 17 200827821 f/# = 1 / 2(NA) 衫式4 f/# = efl Ιφ 利用上述數學式3和數學式4可導出數學式5。 氩#式5 NA =0/2(efl) 上述數學式中,其中NA(numerical aperture)爲數位 光圈’又(lambda )爲雷射的波長,ef丨爲焦距。 "T知入射光束的直徑越大、雷射波長越短,焦點會聚 範圍變窄,如果鏡頭(丨ens )的焦距ef|短,數位光圈就 會變大,焦點會聚範圍(DOF)變窄。 本發明中爲製作1"m以下的焦點會聚範圍(D〇F), 使用大口徑的掃描鏡1 35,並設計與此相應的光學儀。 液晶顯示器使用的彩色渡光片24〇,其進行黑化處理 的厚度優選的是20〜40%,最好不要超過9〇%,以使在夜 :曰顯示器視野範圍内不發生漏光現象。如要以低於2〇%的 予度進行黑化處理時,就不能進行1GQ%的 :::過度的黑化可損傷其下層的膜。另外,爲以適當: 尽度黑化薄膜’雷射能量起到重要的作用。即, 恭 射的輪出能量調整黑化厚度。 田 第十二 理的方法。 a、十二 b、 十二C圖是根據本發明的黑化處 象的像素的薄膜進行黑化處理,可採用掃描(第 單f調整光束大小的雷射對發生漏光現 a圖) 18 200827821 多次整塊輻射(multi-block Sh0t)(第 射(block shot)(第十-6圖)或整塊輻 不丁一 c圖)等方 將雷射以掃描的方式照射到要 ▼掏方式是指 (block shot)方式是對要 t塊輻射 、击沾十斗、β ^ …化的部分只照射一i # 速的方式’又稱爲範圍(sc〇pe)方式; :人先 (mum-bl(5cksh()t)爲掃描方式和整塊輻 息輻射 方式的結合’在進行照射的同時,以與掃描方C shot) 式進行連續照射。 、田工相同的方 例如,具有電腦屏大小的液晶顯示器中像素的面積遠 、, 了被光束形成早疋變換成像素大小, 亚契液晶顯示器的像素面積相同時,藉由一次雷射 ⑷ock shot)可將像素的全部面積進行黑化處理(第:二 c圖)。又如’ 30英寸大型電視機用液晶顯示器的像素 爲數十萬平方微米(_2),只經由—次.雷射照射不能將對應 像素的薄膜的全部面積進行黑化。這時,藉由在薄膜的整 個表面以”Z”字型方式進行掃描(第十二3圖)或以多次整 塊輻射(mum她ck sh〇t)(第十二c圖)的方式進行雷射 照射。 第十三圖是根據本發明另一實施例的黑化裝置構成 圖’上述黑化裝置,包括: 多個雷射振蕩器; 调整上述雷射振蕩器振蕩出的光束的輸出強度的光束 調整單元; 包括i:換上述雷射光束的輪廓的光束形成單元和選擇 200827821 性地透射或反射雷射光束的半透半反鏡的雷射振择 100; ^ 70 用於控制上述雷射振蕩單元100照射的雷射光束的影 像及攝像的聚焦的光學單元400。 〜 在此’省略與第一圖重復部分的說明。 上述光學單元400包括引導從上述雷射振蕩單元1〇〇 輸出的雷射光束到要進行黑化的液晶顯示器彳4〇用的方向 轉換鏡401。本實施例中,只顯示有一個方向轉換鏡4〇1, 但是根據雷射振蕩單元1〇〇及目標物14〇的位置,上述方 向轉換鏡401的個數及位置可進行多樣的變化。上述方向 轉換鏡401要反射從雷射振蕩器振蕩出的所有波長的雷射 光束,因此要被設計爲可在較寬範圍的波長中使用。第六 圖中顯示的塗鍍可同樣適用於本實施例中。 另外,上述光學單元,還包括··用於在多個薄膜中對 要進行黑化處理的薄膜自動調焦的聚焦感測器(f〇cus sensor) 415和聚焦透鏡(f〇cus lens) 419;用於調整雷 射光束的狹縫(s I i t) 41 3;用於確定狹縫(s I i t )大小及位 置的狹缝(s丨i t )照明41 2 ;反射上述狹缝(s I i t )照明用 的狹縫(slit)半透半反鏡411 ;用於確認亮度不合格像素 的2個半透半反鏡414、417; CCD攝像機416及光源418。 確認亮度不合格像素的位置後,利用聚焦感測器和聚 焦透鏡調整雷射的焦點到多個薄膜中將要進行黑化的薄膜 上。聚焦感測器41 5及光源41 8照射到多個薄膜中的特定 薄膜後,藉由分離器(splitter)感應重新反射回來的光。 20 200827821 如對不准影像的焦點,聚焦感測胃415上下控制聚焦透鏡 419 ’以此得到清晰的影像並即時傳❹】cCD攝像機。經 'CCD攝像機確定亮度不合格像素的位置及要進行黑: 的溥膜’根據其種類啓動適合進行黑化的雷射振蕩器、 1〇2、1〇3。光束調整單元104、1〇5、1〇6將輸出的雷射 調整到適合進行黑化處理的狀態。調整到適當狀態的雷射 經過光束形成單元107, 108, 1〇9後再經由狹縫(sm)4i3 來調整其大小’透過聚焦透鏡419照射到液晶顯示器14〇。 構成液晶顯示器140的薄膜進行黑化的處理過程可藉由 CCD攝像機41 6進行即時監控。 如上所述,經由附圖和具體實施方式對本發明進行描 述,/旦並不限於上述的實施方式,在不脫離本發明範圍内, 本範圍普通技術人員可進行各種變更和修改。 發明效果 本發明可選擇地使用雷射光束的波長,可減少雷射輸 出的損失,可達到全面提高處理效率的功效。 另外,根據本發明,使用χγ軸移動掃描單元可進行 高速地黑化處理,經由z軸移動掃描單元調整焦距,可對 各種厚度的薄膜進行黑化處理。 另外,根據本發明,利用光束形成單元將照射光束的 輪廓進行變換、調整大小,藉由掃描方式或整塊輻射 shot)方式進行照射以提高處理速度。 【圖式簡單說明】 第一圖是本發明黑化裝置組成圖。 21 200827821 第二圖是吸附了雜質的液晶顯示器的剖視圖。 第三圖是在雷射振蕩器内部可選擇地透射或反射雷射 光束的半透半反鏡的波長的透射或反射曲線圖。 第四圖是在雷射振蕩器内部可選擇地透射或反射雷射 光束的半透半反鏡的波長的透射或反射曲線圖。 第五圖是掃描鏡(scan丨ens)及照明光源的擴大圖。 —时第/、圖是光束傳遞單元的方向轉換鏡及x丫-軸移動掃 口° 一内口P 的 X 軸檢流計鏡(Ga|van〇meter mirror)及 γ 軸檢流計鏡波長的反射曲線圖。 第七圖是薄臈波長的透射率曲線圖。 =八圖是偏光膜對各波長的透射率曲線圖。 第九圖是實施本發明雷射 圖。 知β田考了尤果輪廓(profile )的曲線 行黑==示根據要黑化的薄膜的厚度調整焦點距離進 第十—圖是黑化過程流程圖。The eighth graph is a graph of transmittance according to the wavelength of the polarizing film. The k-picture shows that the transmittance in the visible light band is 5% or less, and the wavelength in the ultraviolet (UV) band is not transmitted at all, and the transmittance is increased as it approaches the near-infrared range. Therefore, in order to blacken one of the rgbs of the pixel having the polarizing film, it is preferable to use a laser in the near ultraviolet range. For example, if one pixel of the color grading sheet W RGB of the blackened LCD panel is used, it is necessary to use a laser that absorbs the widest wavelength of the spectrum of each pixel. In order to eliminate the 'pixels', the lasers configured as described above can selectively oscillate the respective lasers for the respective pixels, so that the pixels can be blackened with high efficiency. Example: If you want to blacken the blue (8) band of the color filter in the liquid crystal display, == wavelength of the laser; if you want to blacken the red (... skin segment, you need to use near, νί long laser; if you want In the blackened green (G) band, it is necessary to use a laser with a near-infrared wavelength. According to the specific situation, if you want to love the media, the color band of the color filter in the black liquid crystal display device is It is necessary to oscillate the yellow wavelengths of 汝 and ..., (greater than or equal to the yellow wave $ π Η, $ wavelength below the wavelength of the laser; if you want ...,,, the color band, you must revitalize the old year &;, g, 撖 street out of the green wavelength below or near-infrared wavelength 15 200827821 or more laser; if you want to blacken the green band, it is necessary to oscillate a laser below the cyan wavelength or above the yellow wavelength. The organic matter constituting the film undergoes intermolecular bond cleavage, releasing plasma including neutral atoms, molecules, positive and negative ions, free radicals, ion clusters (CLUSTER), electrons and photons (PHOTON), and then burned (ABLA Ding)丨〇N) Blackening. Burning # (ABLATION) is The phenomenon of the dissociation between the molecules constituting the organic molecules becomes a phenomenon of molecules, ions, etc., and the organic matter absorbs energy above the energy level for such dissociation. The ninth figure is a graph of the outline of the laser beam embodying the present invention. The laser irradiated by the oscillator is Gaussian (the state energy is concentrated in the middle range. With such a laser: beam formation 2 108 1 (beam shaper or homogenizer), the intensity of the laser beam is m in a certain range, and is converted into The contour of the enlarged flat top 'the illumination area of the laser along with the beam profile also changes at the same time. At this time, it can be changed to a four-corner flat top 3〇〇 or a round flat top form period. According to an embodiment of the present invention The beam forming unit and the beam adjustment adjust the size and intensity of the irradiated laser beam, and the irradiated laser light-shooting is small. The longer it takes to blacken the entire majority of the pixels, the larger the size of the upper beam can be. It is suitable for production lines that are mass-produced. It is transformed into a laser with a 301 angle flat top 3〇0 or a round flat top shape, and the RGB material in multiple films is moved through the Z-axis. The liquid crystal display is blackened to the required thickness. Figure 10 shows the focus convergence range designed according to the thickness of the film to be blackened to the desired thickness of 16 200827821: film removal and blackening treatment (De_ A schematic diagram of the coffee s, D0F), that is, the process of removing the focal length after the thin mold of the required thickness is removed. The z-axis moving scanning unit 131 is used to align the range of the (D) of the thickness of the D element, and then χγ Axis movement scanning list:: '亍,., and CCD camera to confirm the degree of blackening. When blackening is insufficient, the position of the reel movement scanning unit 131 is moved again, 胄D〇F and a range equivalent to 20% of the pixel thickness. After alignment, the Leo χ γ axis moves the scan: =134 to perform the division. After repeated elimination for 2 to 4 times, the blackening reaches a satisfactory degree of privacy and the blackening is terminated. Prepare for the next step. The eleventh figure is a flow chart for performing the blackening process by moving the focus distance in accordance with the above steps. As shown in the figure, the laser light S1 is initially irradiated, and the blackening S20 of 1% is completed. After confirming the degree of blackening S30, it is judged whether or not the blackening degree s4〇 is satisfied. If the blackening reaches the requirement, the blackening S5 is terminated. Upon reaching the requirement, the z-axis moves the S60 focal length to re-illuminate the laser for blackening. The focus convergence range is not more than 1 pm, and is calculated based on the focal length of the Z-axis moving scanning unit 1 31 and the scanning mirror 1 35 and the diameter of the incident beam. Mathematical expression 1 DOF = ^/2(NA)2 Mathematical expression 2 NA = nsin0 Mathematical expression 3 17 200827821 f/# = 1 / 2(NA) Shirt type 4 f/# = efl Ιφ Using the above mathematical formula 3 and mathematical formula 4 can be derived from Mathematical Formula 5. Argon #式5 NA =0/2(efl) In the above mathematical formula, where NA (numerical aperture) is a digital aperture ’, (lambda) is the wavelength of the laser, and ef丨 is the focal length. "T knows that the larger the diameter of the incident beam, the shorter the laser wavelength, the narrower the focus convergence range. If the focal length ef| of the lens (丨ens) is short, the digital aperture will become larger, and the focal convergence range (DOF) will be narrower. . In the present invention, a focus convergence range (D〇F) of 1 " m or less is produced, and a large-diameter scanning mirror 1 35 is used, and an optical apparatus corresponding thereto is designed. The color light-passing sheet 24 使用 used for the liquid crystal display preferably has a thickness of 20 to 40%, preferably not more than 9% by weight, so that light leakage does not occur in the field of view of the night display. If the blackening treatment is to be carried out at a degree of less than 2%, it is impossible to carry out 1GQ% ::: excessive blackening may damage the film of the lower layer. In addition, it plays an important role in properly: blackening the film's laser energy as much as possible. That is, the rounding energy of the concertment adjusts the blackening thickness. Tian Twelve. a, twelve b, twelve C picture is a blackening process of the film of the pixel of the blackening image according to the present invention, and scanning can be performed (the single f adjusts the beam size of the laser pair to generate light leakage) a picture 18 200827821 Multiple times of multi-block Sh0t (block shot (10th-6th) or whole block), the laser is irradiated to the way It means that the block shot method is a method of irradiating only one i-speed to the part that is to be irradiated, and is also called the range (sc〇pe); -bl(5cksh()t) is a combination of the scanning method and the whole piece of the radiative radiation method 'continuous irradiation with the scanning side C shot while performing the irradiation. For example, a liquid crystal display having a computer screen size has a far-reaching area of pixels, and is converted into a pixel size by the beam formation. When the pixel area of the Yachi liquid crystal display is the same, a laser (4) ock shot is used. ) The entire area of the pixel can be blackened (p.: c). In another example, the pixel of a liquid crystal display for a 30-inch large-sized television set is hundreds of thousands of square micrometers (_2), and the entire area of the film corresponding to the pixel cannot be blackened only by the laser irradiation. At this time, by scanning in the "Z" shape on the entire surface of the film (12th 3rd figure) or by multiple pieces of radiation (mum she ck sh〇t) (twelfth c picture) Laser exposure. Figure 13 is a block diagram of the blackening device according to another embodiment of the present invention, comprising: a plurality of laser oscillators; and a beam adjusting unit that adjusts an output intensity of a beam oscillated by the laser oscillator And including: a beam forming unit for changing the contour of the above-mentioned laser beam and a laser detecting unit 100 for selecting a half mirror for transmitting or reflecting the laser beam in 200827821; ^ 70 for controlling the above-described laser oscillation unit 100 An image of the irradiated laser beam and an imaged focused optical unit 400. ~ Here, the description of the overlapping portion with the first figure is omitted. The optical unit 400 includes a direction conversion mirror 401 for guiding a laser beam output from the above-described laser oscillation unit 1 to a liquid crystal display to be blackened. In the present embodiment, only one direction conversion mirror 4〇1 is displayed, but the number and position of the above-described direction conversion mirror 401 can be variously changed depending on the positions of the laser oscillation unit 1〇〇 and the target object 14〇. The above-described direction conversion mirror 401 is to reflect the laser beams of all wavelengths oscillated from the laser oscillator, and is therefore designed to be used over a wide range of wavelengths. The plating shown in the sixth figure can be equally applied to this embodiment. Further, the optical unit further includes a focus sensor 415 and a focus lens (419) for automatically focusing a film to be blackened in a plurality of films. a slit (s I it) for adjusting the laser beam 41 3; a slit (s丨it) illumination 41 2 for determining the size and position of the slit (s I it ); reflecting the slit (s I It is a slit half mirror 411 for illumination; two half mirrors 414, 417 for confirming pixels of unacceptable brightness; a CCD camera 416 and a light source 418. After confirming the position of the luminance defective pixel, the focus of the laser is adjusted by the focus sensor and the focus lens to the film to be blackened among the plurality of films. After the focus sensor 41 5 and the light source 41 8 are irradiated to a specific one of the plurality of films, the re-reflected light is sensed by a splitter. 20 200827821 If the focus of the image is not allowed, the focus sensing stomach 415 controls the focus lens 419 'up and down to get a clear image and instantly pass the cCD camera. The "CCD camera determines the position of the luminance defective pixel and the black film to be blacked out". According to the type, a laser oscillator suitable for blackening is activated, 1〇2, 1〇3. The beam adjusting units 104, 1〇5, 1〇6 adjust the output laser to a state suitable for blackening processing. The laser beam adjusted to an appropriate state is irradiated to the liquid crystal display 14 through the focus lens 419 after passing through the beam forming units 107, 108, 1〇9 and then adjusting the size thereof via the slit (sm) 4i3. The process of blackening the film constituting the liquid crystal display 140 can be immediately monitored by the CCD camera 41. As described above, the present invention is described by the accompanying drawings and specific embodiments, and is not limited to the above-described embodiments, and various changes and modifications can be made by those skilled in the art without departing from the scope of the invention. EFFECT OF THE INVENTION The present invention selectively uses the wavelength of the laser beam to reduce the loss of the laser output and achieve an overall improvement in processing efficiency. Further, according to the present invention, the χγ-axis moving scanning unit can perform high-speed blackening processing, and the focal length can be adjusted via the z-axis moving scanning unit, and the film of various thicknesses can be blackened. Further, according to the present invention, the contour of the illumination beam is converted and resized by the beam forming unit, and irradiation is performed by a scanning method or a monolithic radiation shot to increase the processing speed. BRIEF DESCRIPTION OF THE DRAWINGS The first figure is a composition diagram of the blackening device of the present invention. 21 200827821 The second figure is a cross-sectional view of a liquid crystal display with adsorbed impurities. The third diagram is a transmission or reflection plot of the wavelength of a transflective mirror that selectively transmits or reflects a laser beam within the laser oscillator. The fourth diagram is a transmission or reflection plot of the wavelength of a transflective mirror that selectively transmits or reflects a laser beam within the laser oscillator. The fifth picture is an enlarged view of the scanning mirror and the illumination source. - Time / /, is the direction conversion mirror of the beam transfer unit and x 丫 - axis movement sweep ° ° X-axis galvanometer mirror (Ga|van〇meter mirror) and γ-axis galvanometer mirror wavelength Reflection curve. The seventh graph is a graph of the transmittance of the thin 臈 wavelength. =8 is a graph of the transmittance of the polarizing film for each wavelength. The ninth diagram is a laser map embodying the present invention. It is known that β field has tested the profile of the profile of the fruit. Line black == indicates that the focus distance is adjusted according to the thickness of the film to be blackened. The tenth is a flow chart of the blackening process.

第十二a、b、c圖是本發明M 篦+ = m …、化處理方法的概略圖。 十二圖是根據本發明另一 η 圖。 只知例的黑化裝置組成 【主要元件符號說明】 100 :雷射振蕩器 101 ·紅色波長雷射 102 ·近紅外線波長雷射 10)2〜1 ··青色波長雷射 22 200827821 103 104 107 110 111 120 121 130 131 132 綠色波長雷射 105、106 ··光束調整單元 108、109 ··光束形成單元 第一半透半反鏡 第二半透半反鏡 光束傳遞單元 122 :方向轉換鏡 掃描單元 Z軸移動掃描單元 攝像機連接裝置 132 - 1 :影像半透半反鏡 133 : CCD攝像機 134 : XY軸移動掃描單元 134 — 1 : X軸檢流計鏡 134 — 2 : Y軸檢流計鏡 掃描鏡 加工目標物 丨TO膜 第一基板 135 140 210 240 136 :照明光源 150 ··驅動控制單元 220 :彩色濾光片 250 ·液晶層 260a :彩色濾光片玻璃 260b :第二基板 270 300 400 雜質 四角平頂 光學單元 280 :偏光膜 301 :圓形平頂形態 401 :方向轉換鏡 41 1 :狹縫半透半反鏡41 2 :狹縫照明 23 200827821 413 : 狹缝 415 : 416 : CCD攝像機 414、 418 : 光源 419 : S10 : 照射雷射光 S20 S30 : 確認黑化程度 S40 S50 : 終止黑化 S60 聚焦感測器 417 :半透半反鏡 聚焦透鏡 完成10%的黑化 滿足黑化程度 z軸移動 24The twelfth, a, b, and c diagrams are schematic diagrams of the M 篦 + = m ... and the processing method of the present invention. The twelve figures are another η diagram according to the present invention. Only known blackening device composition [main component symbol description] 100: laser oscillator 101 · red wavelength laser 102 · near infrared wavelength laser 10) 2 ~ 1 · cyan wavelength laser 22 200827821 103 104 107 110 111 120 121 130 131 132 Green wavelength laser 105, 106 · Beam adjustment unit 108, 109 · Beam forming unit First half mirror Second half mirror beam transfer unit 122 : Direction conversion mirror scanning unit Z-axis mobile scanning unit camera connection device 132 - 1 : Image half mirror 133 : CCD camera 134 : XY axis movement scanning unit 134 — 1 : X-axis galvanometer mirror 134 — 2 : Y-axis galvanometer mirror scanning Mirror processing target 丨TO film first substrate 135 140 210 240 136 : illumination light source 150 ·· drive control unit 220 : color filter 250 · liquid crystal layer 260a : color filter glass 260b : second substrate 270 300 400 impurity Four-corner flat top optical unit 280: polarizing film 301: circular flat top form 401: direction conversion mirror 41 1 : slit half mirror 41 2 : slit illumination 23 200827821 413 : slit 415 : 416 : CCD camera 414 4 18 : Light source 419 : S10 : Irradiation laser light S20 S30 : Confirm blackening degree S40 S50 : Terminate blackening S60 Focus sensor 417 : Half-mirror focusing lens completes 10% blackening to satisfy blackening degree z-axis movement twenty four

Claims (1)

200827821 十、申請專利範圍·· 1 種液晶顯示器黑化裝置,其包括: 多個雷射振蕩器; 光束調整單元,用 治庚· 用於5周正上述雷射振蕩器振蕩的光束 =振蕩單元’包括變換上述雷射光束輪廓的光束形 反鏡^ n可選擇地透射或反射上述光束特性的半透半200827821 X. Patent application scope · A liquid crystal display blackening device, which includes: a plurality of laser oscillators; a beam adjusting unit, which is used for treating the beam of the above-mentioned laser oscillator for 5 weeks = oscillation unit' a beam shaping mirror comprising a transforming the laser beam profile to selectively transmit or reflect a transflective half of the beam characteristics 光束傳遞早疋,用於轉換上述雷射振蕩單元雷射光束 掃描單元 要黑化的部位 凋整光束的方向使上述雷射光束照射到需 窨,如中請專利範圍第1項所述的液晶顯示器黑化裝 η:、上述雷射振蕩單元包括雷射振蕩器,用於振蕩出 波長、綠色波長及近紅外線波長的雷射光束。 3如申睛專利範圍第2項所述的液晶顯示器黑化裝 置其中上述雷射振蕩單元,包括青色波長雷射光束,以 代替近紅外線雷射光束使用。 4 ·如申請專利範圍第1項所述的液晶顯示器黑化裝 置其中上述雷射振蕩單元包括紫外線(UV)或近紫外線 (NUV)波長的雷射光束。 5 .如申請專利範圍第1項所述的液晶顯示器黑化裝 置,其中上述雷射振蕩單元可選擇地振蕩出要進行黑化處 理的彩色濾光片中吸收波譜高波段的雷射光束。、 25 200827821 如申叫專利範圍弟1項所述的液晶顯示器黑化裝 置’其中上述雷射振蕩單元,當要黑化液晶顯示器中彩色 濾光片的藍色(B )波長範圍,就要振蕩出黃色波長以上 的雷射或近紫外線波長以下範圍波段的雷射;當要黑化紅 色()範圍’就要振蕩出綠色波長以下或近紅外線波長 以上的雷射;當要黑化綠色(G )範圍,就要振蕩出青色 波長以下或黃色波長以上的雷射。 7 如申请專利範圍第1項所述的液晶顯示器黑化裝 [置’其中上述雷射振蕩單元,在液晶顯示器中彩色濾光片 具有偏光薄膜時,係振蕩出上述近紅外線波長以上的雷 射。 8 ·如申請專利範圍第1項所述的液晶顯示器黑化裝 置’其中上述雷射振蕩器是雷射二極體、雷射二極體模組 或D P S S雷射。 9 ·如申請專利範圍第1項所述的液晶顯示器黑化裝 置’其中上述雷射振蕩器爲連續振蕩雷射振蕩器或脈衝振 U 蕩雷射振蕩器。 1 0 ·如申請專利範圍第1項所述的液晶顯示器黑化 裝置’其中上述光束調整單元,不僅可以調整光束的強度, 而且可以調整光束的角度及偏光狀態。 1 1 ·如申請專利範圍第1項所述的液晶顯示器黑化 裝置’其中上述光束形成單元,包括:光束整形器,將高 斯分佈的雷射光束變換爲四角平頂或圓形平頂形態;光束 狹缝,用於調整光束大小。 26 200827821 1 2 ·如申請專利範圍第1項所述的液晶顯示器黑化 裝置’其中上述半透半反鏡包括: 第一半透半反鏡,用於透射紅色波長同時反射近紅外 線波長; 第二半透半反鏡,用於透射紅色波長同時反射綠色波 長。 1 3 ·如權利要求1所述的液晶顯示器黑化裝置,其 中上述光束傳遞單元包括用於反射上述雷射振蕩單元振蕩 出的350〜11 〇0nm範圍波長的反射鏡。 1 4 ·如申請專利範圍第1 3項所述的液晶顯示器黑 化裝置’其中上述反射鏡被設計爲僅反射上述雷射振蕩單 元照射的波長範圍。 1 5 ·如申請專利範圍第1項所述的液晶顯示器黑化 裝置,其中上述掃描單元包括: Z轴移動掃描單元,用於調整上述雷射光束焦距; XY轴移動掃描I $,用於上下左右調整上述雷射光 束方向。 1 6 ·如申請專利範圍第丄5項所述的液晶顯示器黑 化裝置,其中上述掃描單元,還包括: 電荷搞合器件(CCD)攝像機,用於觀察上述雷射光 束是否照射在液晶顯示器的正確位置; 攝像機連接裝置,位於上述z軸移動掃描單元和χγ 轴移動掃描單元之間,將影像傳遞到上述CCD攝像機; 掃描鏡,將經由上述掃描單元的雷射光束照射到液晶 27 200827821 顯示器上,進而集束雷射光束,並形成照射到液晶顯示器 上的影像。 17如申印專利範圍第1 5項所述的液晶顯示器黑 化裝置,其中上述XY軸移動掃描單元,包括··變換光束 方向的X轴檢流計鏡和γ軸檢流計鏡,上述檢流計鏡反射 上述雷射振蕩器照射的350〜1 i〇〇nm範圍的波長。 18如申吻專利範圍第1 6項所述的液晶顯示器黑 化裝置,其中上述掃描鏡使用在所有位置都能形成垂直光 f 束的遠心鏡(telecentric lens )。 1 9 ·如申請專利範圍第丄6項所述的液晶顯示器黑 化裝置,其中上述CCD攝像機能即時監控處理目標物的 位置並顯示處理的影像。 2 0 ·如申請專利範圍第丄6項所述的液晶顯示器黑 化裝置,其中上述攝像機連接裝置包括影像半透半反鏡, 在可見光線範圍透射率與反射率的比例爲5〇 : 5〇。 2 1 ·如申請專利範圍第丄項所述的液晶顯示器黑化 I' 裝置,其還包括: 板台,用於裝載、卸載上述液晶顯示器,將其向X、 y、z軸移動或旋轉; 控制堂,調整雷射光束到X、γ、Z軸,使雷射照射到 上述液晶顯示器的不合格像素上; 控制器,控制上述控制臺和板台動作。 2 2 · —種包括雷射振蕩單元和爲集束上述雷射振蕩 單元照射的雷射光束的處理形狀及即時影像攝影光速用的 28 200827821 光學單疋的利用雷射的液晶顯示器的黑化裝置上述雷射 振蕩單元,包括: 多個雷射振蕩器; 光束調整單元,用於調整上述雷射振蕩器振蕩出的光 束輸出強度;和 半透半反鏡,變換上述雷射光束輪廓的光束形成單元 和可選擇地透射或反射雷射光束, 上述多個雷射振蕩器根據要黑化範圍的吸收波譜,可 選擇地照射雷射。 2 3 · —種液晶顯示器的黑化方法,包括·· “振蕩步驟,振蕩出將要黑化部分的吸收波譜高的雷射 光束; 調整步驟,調整上述雷射光束強度; 變換步驟,變換上述雷射光束的輪廓; 調整步驟,調整上述雷射光束的焦距; 照射上述雷射光束,進行黑化處理的步驟。 2 4 .如申請專利範圍第2 化方法,其中上述雷射光㈣液阳顯示器黑 波長、青色波長、近红外结、“㈨ 匕括振出紅色 波長光束。 ^ Α近紫外線 項所述的液晶顯示器黑 當要黑化液晶顯示器中 ’就要振蕩出紅色波長 就要振蕩出綠色波長雷 d D ·如甲鶴專利範圍第 化方法,其中上述雷射振蕩步 彩色濾光片的藍色(B )波長 雷射;當要黑化紅色(r )範 29 200827821 射,當要黑化綠色(G)範圍,就要振蕩出近紅外線 雷射。 2 6 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法,其中上述雷射光束強度調整步驟,在進行雷射光 束強度調整的同時,調整光束的角度及偏光狀態。 2 7 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法,其中上述變換光束輪廓的步驟,將雷射光束輪廟 變換到平頂形態,並調整光束的大小。 2 8 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法’其中上述調整光束強度的步驟,調整爲光束具有 同的大小’且集束到處理範圍的焦點的大小相同。 2 9 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法’其中在上述雷射光束強度調整步驟及焦距調整步 驟中’調整雷射光束的強度及焦距,以使薄膜2〇%〜90% 的厚度進行黑化處理。 3 〇 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法,其中上述照射雷射光束的步驟,邊調整雷射焦距 邊依次照射。 3 1 ·如申請專利範圍第2 3項所述的液晶顯示器黑 化方法’其中上述照射雷射光束的步驟爲掃描方式、整塊 掃私方式(block scan )或整塊輻射(block shot)方式。 十一、圓式·· 如次頁 30The beam is transmitted early, and is used for converting the direction of the beam to be blackened by the laser beam scanning unit of the above-mentioned laser oscillating unit, so that the laser beam is irradiated to the desired beam, as in the liquid crystal described in the first item of the patent scope. The display blackening device η: The laser oscillation unit includes a laser oscillator for oscillating a laser beam of a wavelength, a green wavelength, and a near-infrared wavelength. The liquid crystal display blackening device according to claim 2, wherein the laser oscillation unit comprises a cyan wavelength laser beam instead of the near-infrared laser beam. 4. The liquid crystal display blackening device according to claim 1, wherein the laser oscillation unit comprises a laser beam of ultraviolet (UV) or near ultraviolet (NUV) wavelength. 5. The liquid crystal display blackening device according to claim 1, wherein the laser oscillation unit selectively oscillates a laser beam having a high absorption band in a color filter to be subjected to blackening treatment. 25 200827821 For example, the liquid crystal display blackening device described in the patent scope 1 of the above-mentioned laser oscillation unit, when the blue (B) wavelength range of the color filter in the liquid crystal display is to be blackened, it is oscillated A laser with a wavelength above the yellow wavelength or a laser with a wavelength below the ultraviolet wavelength; when the red () range is to be blackened, it is necessary to oscillate a laser below the green wavelength or near the near infrared wavelength; when it is to blacken the green (G The range is to oscillate a laser below the cyan wavelength or above the yellow wavelength. 7. The liquid crystal display blackening device according to the first aspect of the invention, wherein the laser oscillation unit is provided, and when the color filter has a polarizing film in the liquid crystal display, the laser beam of the near-infrared wavelength or more is oscillated. 8. The liquid crystal display blackening device according to claim 1, wherein the laser oscillator is a laser diode, a laser diode module or a D P S S laser. 9. The liquid crystal display blackening device according to claim 1, wherein the laser oscillator is a continuous oscillation laser oscillator or a pulsed U-wave laser oscillator. The liquid crystal display blackening device according to claim 1, wherein the beam adjusting unit can adjust not only the intensity of the light beam but also the angle of the light beam and the polarization state. The liquid crystal display blackening device according to claim 1, wherein the beam forming unit comprises: a beam shaper that converts a Gaussian-distributed laser beam into a quad flat top or a round flat top form; Beam slits for adjusting the beam size. The liquid crystal display blackening device of claim 1, wherein the semi-transparent mirror comprises: a half transflective mirror for transmitting a red wavelength while reflecting a near-infrared wavelength; A half-transparent mirror for transmitting red wavelengths while reflecting green wavelengths. A liquid crystal display blackening apparatus according to claim 1, wherein said beam transfer unit comprises a mirror for reflecting a wavelength in the range of 350 to 11 〇 0 nm oscillated by said laser oscillation unit. The liquid crystal display blackening device as described in claim 13 wherein the mirror is designed to reflect only the wavelength range of the laser oscillation unit. The liquid crystal display blackening device according to claim 1, wherein the scanning unit comprises: a Z-axis moving scanning unit for adjusting the focal length of the laser beam; and an XY-axis moving scanning I $ for upper and lower Adjust the direction of the above laser beam left and right. The liquid crystal display blackening device according to claim 5, wherein the scanning unit further comprises: a charge engaging device (CCD) camera for observing whether the laser beam is irradiated on the liquid crystal display The correct position; the camera connecting device is located between the z-axis moving scanning unit and the χγ-axis moving scanning unit, and transmits the image to the CCD camera; the scanning mirror irradiates the laser beam through the scanning unit to the liquid crystal 27 200827821 display And, in turn, the laser beam is concentrated and an image that is incident on the liquid crystal display is formed. The liquid crystal display blackening device according to the fifteenth aspect of the invention, wherein the XY axis moving scanning unit comprises: an X-axis galvanometer mirror that converts a beam direction and a γ-axis galvanometer mirror, the above-mentioned inspection The flow meter mirror reflects the wavelength of the range of 350 to 1 i 〇〇 nm irradiated by the above laser oscillator. The liquid crystal display blackening device of claim 16, wherein the scanning mirror uses a telecentric lens capable of forming a vertical beam of light f at all positions. The liquid crystal display blackening device according to claim 6, wherein the CCD camera can instantly monitor the position of the processing target and display the processed image. The liquid crystal display blackening device according to claim 6, wherein the camera connecting device comprises an image half mirror, and the ratio of transmittance to reflectance in the visible light range is 5〇: 5〇 . The liquid crystal display blackening I' device of claim 1, further comprising: a plate for loading and unloading the liquid crystal display, moving or rotating the X, y, and z axes; The control hall adjusts the laser beam to the X, γ, and Z axes to cause the laser to illuminate the unqualified pixels of the liquid crystal display; the controller controls the operation of the console and the table. 2 2 - a black laser device comprising a laser oscillating unit and a laser beam for illuminating the laser oscillating unit, and a black laser device for illuminating a liquid crystal display a laser oscillating unit, comprising: a plurality of laser oscillators; a beam adjusting unit configured to adjust a beam output intensity oscillated by the laser oscillator; and a half mirror to transform the beam forming unit of the laser beam profile And optionally transmitting or reflecting a laser beam, the plurality of laser oscillators selectively illuminating the laser according to an absorption spectrum to be blackened. 2 3 · A blackening method for a liquid crystal display, comprising: “an oscillating step of oscillating a laser beam having a high absorption spectrum of a blackened portion; an adjustment step of adjusting the intensity of the laser beam; and a transformation step of transforming the ray a beam profile; an adjustment step of adjusting a focal length of the laser beam; a step of illuminating the laser beam to perform a blackening process. 2 4. A method according to the second aspect of the patent application, wherein the laser light (four) liquid positive display black Wavelength, cyan wavelength, near-infrared junction, "(9) 匕 振 红色 红色 red wavelength beam. ^ The liquid crystal display black mentioned in the near-UV terminology should be blackened in the liquid crystal display. 'It is necessary to oscillate the red wavelength to oscillate the green wavelength Ray d D · The method of the patent range of the crane, the above-mentioned laser oscillation step Blue (B) wavelength laser of color filter; when blackening red (r) fan 29 200827821 shot, when black (G) range is to be blackened, near-infrared laser is oscillated. The liquid crystal display blackening method according to the second aspect of the invention, wherein the laser beam intensity adjustment step adjusts the angle and the polarization state of the beam while performing the adjustment of the intensity of the laser beam. The liquid crystal display blackening method according to claim 23, wherein the step of converting the beam profile converts the laser beam wheel temple to a flat top shape and adjusts the beam size. The liquid crystal display blackening method as described in claim 2, wherein the step of adjusting the beam intensity is adjusted such that the beams have the same size and the focus of the focus to the processing range is the same. 2 9 · The liquid crystal display blackening method according to claim 23, wherein the intensity and focal length of the laser beam are adjusted in the above-described laser beam intensity adjustment step and focal length adjustment step, so that the film is 2%% Blackening treatment of ~90% thickness. The liquid crystal display blackening method according to the second aspect of the invention, wherein the step of irradiating the laser beam is performed by sequentially adjusting the laser focal length. 3 1 · The liquid crystal display blackening method according to claim 23, wherein the step of irradiating the laser beam is a scanning method, a block scan method or a block shot method. . XI, round type · as the next page 30
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