TWI445586B - Laser processing method and cutting method,method of dividing a structured body with multiple substrates - Google Patents
Laser processing method and cutting method,method of dividing a structured body with multiple substrates Download PDFInfo
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- TWI445586B TWI445586B TW097112157A TW97112157A TWI445586B TW I445586 B TWI445586 B TW I445586B TW 097112157 A TW097112157 A TW 097112157A TW 97112157 A TW97112157 A TW 97112157A TW I445586 B TWI445586 B TW I445586B
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/36—Removing material
- B23K26/40—Removing material taking account of the properties of the material involved
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/02—Positioning or observing the workpiece, e.g. with respect to the point of impact; Aligning, aiming or focusing the laser beam
- B23K26/06—Shaping the laser beam, e.g. by masks or multi-focusing
- B23K26/062—Shaping the laser beam, e.g. by masks or multi-focusing by direct control of the laser beam
- B23K26/0622—Shaping the laser beam, e.g. by masks or multi-focusing by direct control of the laser beam by shaping pulses
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/36—Removing material
- B23K26/38—Removing material by boring or cutting
- B23K26/382—Removing material by boring or cutting by boring
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/36—Removing material
- B23K26/38—Removing material by boring or cutting
- B23K26/382—Removing material by boring or cutting by boring
- B23K26/389—Removing material by boring or cutting by boring of fluid openings, e.g. nozzles, jets
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/50—Working by transmitting the laser beam through or within the workpiece
- B23K26/55—Working by transmitting the laser beam through or within the workpiece for creating voids inside the workpiece, e.g. for forming flow passages or flow patterns
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K26/00—Working by laser beam, e.g. welding, cutting or boring
- B23K26/50—Working by transmitting the laser beam through or within the workpiece
- B23K26/57—Working by transmitting the laser beam through or within the workpiece the laser beam entering a face of the workpiece from which it is transmitted through the workpiece material to work on a different workpiece face, e.g. for effecting removal, fusion splicing, modifying or reforming
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B28—WORKING CEMENT, CLAY, OR STONE
- B28D—WORKING STONE OR STONE-LIKE MATERIALS
- B28D5/00—Fine working of gems, jewels, crystals, e.g. of semiconductor material; apparatus or devices therefor
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K2101/00—Articles made by soldering, welding or cutting
- B23K2101/36—Electric or electronic devices
- B23K2101/40—Semiconductor devices
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K2103/00—Materials to be soldered, welded or cut
- B23K2103/50—Inorganic material, e.g. metals, not provided for in B23K2103/02 – B23K2103/26
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Mechanical Engineering (AREA)
- Plasma & Fusion (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Chemical & Material Sciences (AREA)
- General Chemical & Material Sciences (AREA)
- Oil, Petroleum & Natural Gas (AREA)
- Laser Beam Processing (AREA)
- Re-Forming, After-Treatment, Cutting And Transporting Of Glass Products (AREA)
- Processing Of Stones Or Stones Resemblance Materials (AREA)
- Liquid Crystal (AREA)
Description
本發明係關於對加工對象物體、特別是具有如同基板之平板狀的物體,採用對此物體而言是透明之波長的超短脈波雷射來效率且高品質地進行加工的方法。The present invention relates to a method for efficiently and efficiently processing an object to be processed, in particular, an object having a flat shape like a substrate, using an ultrashort pulse laser having a wavelength transparent to the object.
本發明係另外關於一種構造體之使用雷射光的分割方法,而該構造體具有平行配置至少2片基板且在其間插入有間隔物之構造且具有多層基板。適合於分割使用液晶顯示面板、電漿顯示面板等之玻璃基板的平板顯示面板。The present invention relates to a method of dividing a structure using laser light, and the structure has a configuration in which at least two substrates are arranged in parallel with a spacer interposed therebetween and has a multilayer substrate. It is suitable for dividing a flat display panel using a glass substrate such as a liquid crystal display panel or a plasma display panel.
在電子工業中,CPU和DRAM、SRAM等的半導體裝置之微細化係逐年發展,隨之而來就是謀求內部的電路的高度積體化。這些裝置的構造係在矽晶圓等的半導體基板上以高度整合的電路圖案所形成。為了從半導體晶圓中獲得多數的晶片,所以必須使分割晶片所需要的面積最小化。為此,期望在劃線步驟中,加工除去物之飛散較少。在液晶顯示器等的玻璃基板之切斷步驟中,期待能正確地以既定尺寸來進行分割。在些分割步驟中,必須以不會對加工部周圍造成熱損傷或機械損傷的條件下來進行除去加工,因此使用奈秒脈波以下之狹窄的脈波。在使用超短脈波雷射的加工中,習知技術是能減低熱加工變質層的發生、或即使對此波長而言為透明的材料,也能藉由以多光子吸收為代表的非線形光吸收來進行加工者。In the electronics industry, the miniaturization of semiconductor devices such as CPUs, DRAMs, and SRAMs has been progressing year by year, and accordingly, the internal circuits have been highly integrated. The construction of these devices is formed on a semiconductor substrate such as a germanium wafer with a highly integrated circuit pattern. In order to obtain a large number of wafers from a semiconductor wafer, it is necessary to minimize the area required to divide the wafer. For this reason, it is desirable that the scattering of the processed removal is less in the scribing step. In the cutting step of the glass substrate such as a liquid crystal display, it is expected that the division can be performed accurately with a predetermined size. In some of the division steps, it is necessary to carry out the removal processing without causing thermal damage or mechanical damage to the periphery of the processed portion, and therefore a narrow pulse wave of a nanosecond pulse wave or less is used. In the processing using ultrashort pulse laser, the conventional technique is to reduce the occurrence of the hot work metamorphic layer, or even a material transparent to this wavelength, and can be represented by a non-linear light represented by multiphoton absorption. Absorbed for processing.
使用超短脈波振動之雷射光的透明體之加工方法係由 於專利文獻2而為眾所皆知,此外,聚光於基板的內面而對被加工物體施行加工雷射一事係被記載於專利文獻3。The processing method of a transparent body using laser light of ultrashort pulse wave vibration is It is known in the patent document 2, and the case where the processing laser is condensed on the inner surface of the board|substrate and the processing object is processed is described in patent document 3.
因為照射表面吸收很大的UV雷射光時,從照射表面產生電漿,因此雷射光被吸收,所以雷射能量的利用效率下降的同時,藉由來自電漿的次要放射而照射周圍,也有影響周圍之元件特性的時候。因此,作為半導體基板、薄膜電晶體用之玻璃基板等分割成既定大小的劃線步驟,在專利文獻3中則記載了從與劃入切縫的面(加工面)相反的面將焦點對焦於加工面而照射雷射光,藉以對加工面加工切縫的方法。在此方法中,因為使雷射光聚光於與雷射光入射側相反的面,並進行雷射剝離加工,所以會有無法充分獲得加工溝槽之深度的缺點。當無法充分獲得溝槽深度時,為了沿著該溝槽而分離,只有增大為了折斷而需要的折曲力,且有時也未沿著切割線而分割。如果加工溝槽的深度夠深的話,只要少許的應力就能沿著切割線進行分割。Since the irradiated surface absorbs a large amount of UV laser light, plasma is generated from the irradiated surface, so that the laser light is absorbed, so that the utilization efficiency of the laser energy is lowered, and the surrounding radiation is irradiated by the secondary radiation from the plasma. When it comes to the characteristics of the surrounding components. Therefore, the semiconductor substrate, the glass substrate for a thin film transistor, and the like are divided into a scribe line step of a predetermined size, and Patent Document 3 describes that the focus is focused on the surface opposite to the surface (machined surface) that is cut into the slit. The method of processing the surface and irradiating the laser light to process the slit on the machined surface. In this method, since the laser light is condensed on the surface opposite to the incident side of the laser light and subjected to laser lift-off processing, there is a disadvantage that the depth of the processing groove cannot be sufficiently obtained. When the groove depth cannot be sufficiently obtained, in order to separate along the groove, only the bending force required for breaking is increased, and sometimes it is not divided along the cutting line. If the depth of the groove is deep enough, a small amount of stress can be divided along the cutting line.
另一方面,在液晶顯示裝置的製造中,有將構成面板的大型玻璃基板進行切斷之步驟。液晶顯示裝置的面板面係平行配置至少2片玻璃板,在其間設置顯示裝置所必需的彩色濾波片或液晶、薄膜電晶體(TFT)、控制電極等的配線。這些玻璃板係在製造步驟中使用比最終之顯示裝置的尺吋還要大的玻璃而同時製造多數片顯示裝置,藉以同時進行多數片顯示面板的製造,以謀求效率化。因此,最後必須配合製品的面板尺寸,而從形成有很大之多數片面板的大型玻璃基板而個別切斷。以往的玻璃板之切斷方法係 利用鑽石刃、超硬刃等之刀刃等而沿著所需之切斷線而刻入玻璃表面並設置切割線,爾後在直角方向上對該切割線施加應力並沿著該切割線來進行破斷並分離的方法,或者治著所需之切斷線來將雷射光線進行掃描、加熱,並使熱應力發生在玻璃基板上,從此部分進行破斷分割的方法等,在此情況下,使用吸收率很大的雷射波長來照射玻璃板,使局部加熱,爾後進行強制冷卻,從照射位置進行分割。On the other hand, in the manufacture of a liquid crystal display device, there is a step of cutting a large-sized glass substrate constituting a panel. At least two glass plates are arranged in parallel on the panel surface of the liquid crystal display device, and a color filter or a liquid crystal, a thin film transistor (TFT), a control electrode, or the like necessary for the display device is provided therebetween. In these glass sheets, a plurality of sheets of display devices are simultaneously produced by using a glass larger than the size of the final display device in the manufacturing process, whereby a plurality of sheets of display panels are simultaneously manufactured for efficiency. Therefore, it is necessary to finally cut the panel size of the product and to cut it from a large glass substrate on which a large number of sheets are formed. The cutting method of the conventional glass plate Cutting the glass surface along the required cutting line with a blade such as a diamond blade or a super-hard blade, and setting a cutting line, and then applying stress to the cutting line in a right angle direction and breaking along the cutting line a method of breaking and separating, or treating a required cutting line to scan and heat the laser light, and causing thermal stress to occur on the glass substrate, and thereby performing a method of breaking and dividing, etc., in this case, The glass plate is irradiated with a laser wavelength having a large absorption rate to locally heat, and then forced cooling is performed to divide from the irradiation position.
在2片玻璃板之間插入顯示要件並以密封劑來封止玻璃周圍以後分割成個別的顯示面板時,實施從2片重疊之玻璃板的兩面各針對單一側進行劃線,爾後進行切斷的方法。這因為以鑽石刃刻入,所以在單一面上進行劃線加工以後,使2層玻璃板表裹反轉並在剩餘的一面上施行劃線以後,一起分割2片重疊之玻璃板的方法。近幾年的市場由於顯示面板之尺寸大型化的傾向,而用於面板的玻璃尺寸有越來越大的趨勢,因此,製造用大型玻璃板的搬運裝置會複雜化,反轉機構之規模變得龐大且成為高價的設備。因此,玻璃板不反轉而從單一側進行劃線的方法係成為實用上有效的製造方法。在專利文獻4中已揭露從2片重疊之玻璃的單一側對各玻璃表面照射紫外線雷射,在2片重疊構造之雙方玻璃板的表面上施行劃線的提案。此方法係在玻璃對雷射光而言為具有透明性,從上部玻璃側照射雷射光的情況下,紫外線雷射光通過上部玻璃而到達下部玻璃表面則成了必要條件。因此,有用於下部玻璃之上 面和上部玻璃板之內面的金屬配線等的金屬膜時,藉由照射雷射光而金屬膜破損,或是被金屬膜遮蔽而變得很難將雷射射束導引至下部玻璃。如同這般在2片玻璃之間有介入物的情況下,以來自單一側面的雷射射束照射而通過上部玻璃板,並對下部的玻璃板進行劃線是很困難的。When a display element is inserted between two glass plates and the periphery of the glass is sealed with a sealant, and then divided into individual display panels, the two sides of the two overlapping glass plates are each scribed to a single side, and then cut. Methods. This is because the diamond blade is engraved, so after the scribing process is performed on a single surface, the two-layer glass plate is reversed and the remaining one surface is subjected to scribing, and then the two overlapping glass plates are divided together. In recent years, due to the tendency of the display panel to be enlarged in size, the size of the glass used for the panel has become larger and larger. Therefore, the handling device for manufacturing large-sized glass plates is complicated, and the scale of the reversing mechanism is changed. It is huge and has become a high-priced device. Therefore, the method of scribing from a single side without inverting the glass sheet is a practical and effective manufacturing method. Patent Document 4 discloses a proposal of irradiating an ultraviolet ray on each glass surface from a single side of two overlapping glass sheets, and performing scribing on the surfaces of both glass sheets of the two overlapping structures. In this method, when the glass is transparent to the laser light, and the laser light is irradiated from the upper glass side, it is necessary to pass the ultraviolet laser light through the upper glass to the lower glass surface. Therefore, there is a place for the lower glass When a metal film such as a metal wiring on the inner surface of the upper glass plate is irradiated with laser light, the metal film is broken or shielded by the metal film, and it is difficult to guide the laser beam to the lower glass. In the case where there is an intervening object between the two sheets of glass, it is difficult to illuminate the upper glass sheet with a laser beam from a single side and scribe the lower glass sheet.
[專利文獻1]美國再發行專利第37585號說明書[專利文獻2]特開2002-205179號公報[專利文獻3]特開2004-351466號公報[專利文獻4]特開2005-132694號公報[專利文獻5]特開平8-64556號公報[Patent Document 1] Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. Patent Document 5] Japanese Patent Publication No. 8-64556
欲解決的課題在於使用對加工物體而言為透明之波長的超短脈波雷射光,而對加工物體在與入射側相反之側(反面)實施高精度加工的時候,於加工物體內部在雷射光行進方向上,以涵蓋比聚光點的焦點深度還要長之範圍來設置小直徑的射束。The problem to be solved is to use ultrashort pulse laser light of a wavelength transparent to a processed object, and to perform high precision processing on the opposite side (reverse side) of the processed object from the incident side, in the inside of the processed object In the direction of travel of the light, a beam of small diameter is set to cover a range longer than the depth of focus of the spot.
另外,進一步的課題在於提供一種方法,其能僅從具有多層基板的構造體之一個基板面側照射雷射光並分割該構造體。另外,提供一種分割方法,其在2片基板之間具有金屬薄膜的構造中,使金屬薄膜露出。另外,提供一種構造體的分割方法,其在2片基板之間具有封止部,並在封止部內側形成電子零件的情況下,能將配線從該電子零件導出至封止部外側。Further, another object of the invention is to provide a method of irradiating laser light from only one substrate surface side of a structure having a multilayer substrate and dividing the structure. Further, a division method is provided in which a metal thin film is exposed in a structure having a metal thin film between two substrates. Further, a method of dividing a structure is provided which has a sealing portion between two substrates, and when an electronic component is formed inside the sealing portion, the wiring can be led out from the electronic component to the outside of the sealing portion.
使自集束作用發生於加工物體內部,並縮小雷射光的加工寬度,能將雷射光之行進方向的加工距離作成比通常的剝離加工明顯還要大,藉以解決上述課題。The self-bundling action occurs inside the processed object, and the processing width of the laser light is reduced, and the processing distance in the traveling direction of the laser light can be made larger than that in the normal peeling process, thereby solving the above problem.
為了解決上述課題,本發明係一種雷射加工方法,其特徵為:透過聚光手段而使具有對於具有第1面以及第2面之被加工物體而言為透明之波長的超短脈波雷射光聚光,從第1面之側照射前述雷射光,使得將被聚光之前述雷射光的射束腰部位置形成在前述被加工物體的第1面和第2面之間,藉由前述被加工物體內部之超短脈波高峰值雷射光傳播所造成的自集束作用,在前述雷射光的行進方向上形成聚光通道,藉以在前述聚光通道部中形成達到第2面的空洞或者達到第2面附近的空洞。藉此,能將雷射光行進方向的加工距離作成比通常的剝離加工還要大。In order to solve the above problems, the present invention is a laser processing method characterized in that an ultrashort pulse wave having a wavelength transparent to a workpiece having a first surface and a second surface is transmitted through a light collecting means. Irradiating the light to illuminate the laser beam from the side of the first surface such that the beam waist position of the laser light to be collected is formed between the first surface and the second surface of the object to be processed, a self-concentrating action caused by ultra-short pulse wave high-peak laser light propagation inside the object to be processed, forming a condensing channel in the traveling direction of the laser light, thereby forming a cavity reaching the second surface in the concentrating channel portion or reaching A hole near the second side. Thereby, the processing distance in the traveling direction of the laser light can be made larger than the normal peeling process.
另外,特徵為形成前述雷射光行進方向之與第2面的交點附近之隆起比周邊表面還要高且機械強度弱之隆起構造。另外,特徵為形成前述聚光通道直至第2面,藉以形成前述空洞直至第2面。另外,特徵為從第1面形成前述聚光通道直至第2面,藉以從第1面形成前述空洞直至第2面。另外,特徵為從第1面形成前述聚光通道直至前述加工物體內部,藉以從第1面形成前述空洞直至前述加工物體內部。藉由各個,能將雷射光行進方向的加工距離作成比通常的剝離加工還要大。Further, it is characterized in that a ridge structure in which the ridge of the vicinity of the intersection of the laser light traveling direction and the second surface is higher than the peripheral surface and has a weak mechanical strength is formed. Further, it is characterized in that the light collecting passage is formed up to the second surface, whereby the cavity is formed up to the second surface. Further, it is characterized in that the light collecting passage is formed from the first surface to the second surface, whereby the cavity is formed from the first surface to the second surface. Further, it is characterized in that the light collecting passage is formed from the first surface to the inside of the processed object, whereby the cavity is formed from the first surface to the inside of the processed object. By each, the processing distance in the direction in which the laser light travels can be made larger than the normal peeling process.
另外,特徵為前述被加工物體係相同種類或者相異種 類之材料的平板狀物體重疊2片以上的多層構造。藉此能同時加工2片以上的物體。In addition, it is characterized by the same type or different species of the above-mentioned workpiece system The flat object of the material of the class overlaps two or more multilayer structures. Thereby, it is possible to process two or more objects at the same time.
另外,特徵為在前述被加工物體之第1面側上設置對於前述雷射波長而言為透明的其他物體,藉以變更產生於前述被加工物體的自集束作用所造成之前述聚光通道的長度。藉此,能調整雷射光行進方向的加工距離。Further, it is characterized in that another object transparent to the laser wavelength is provided on the first surface side of the object to be processed, thereby changing the length of the condensing channel caused by the self-bundling action of the object to be processed. . Thereby, the processing distance of the direction in which the laser light travels can be adjusted.
另外,特徵為在前述被加工物體之第1面側上設置對於前述雷射波長而言為透明的其他物體,藉以使產生於前述被加工物體的自集束作用所造成之前述聚光通道到達第1面。藉此,能加工直至基板的正面。Further, it is characterized in that another object that is transparent to the laser wavelength is provided on the first surface side of the object to be processed, so that the concentrating channel caused by the self-bundling action of the object to be processed reaches the 1 side. Thereby, it can process to the front surface of a board|substrate.
另外,特徵為沿著切斷的方向並以任意速度,來使由前述聚光手段而聚光於前述被加工物體內部的前述超短脈波雷射光相對移動,藉以設置前述空洞在空間上的重疊。另外,特徵為沿著切斷的方向並以任意速度,來使由前述聚光手段而聚光於前述被加工物體內部的前述超短脈波雷射光相對移動,藉以將前述空洞設置成在空間上分離。藉由各個,能在被加工物體上製作切斷線,並且因為雷射光行進方向的加工距離大,所以能以少量的彎曲應力來進行切斷。Further, the ultra-short pulse laser light that is condensed by the concentrating means and condensed inside the object to be processed is relatively moved along the cutting direction at an arbitrary speed, thereby providing the space in the cavity. overlapping. Further, the ultra-short pulse laser light that is condensed by the concentrating means and condensed inside the object to be processed is relatively moved along the cutting direction at an arbitrary speed, thereby setting the cavity to be in space. Separated on. Each of the cutting lines can be formed on the object to be processed, and since the machining distance in the traveling direction of the laser light is large, the cutting can be performed with a small amount of bending stress.
另外,特徵為前述被加工物體係做成平面狀的物體,使前述超短脈波雷射的聚光雷射光從前述被加工物體之第1面的法線方向以一定的角度而傾斜並入射,使前述聚光雷射光具有前述角度的傾斜並旋轉,以進行圓形的掃描,並使加工面傾斜來進行加工。藉此,能作成圓形的切斷線。Further, the object to be processed is a planar object, and the condensed laser light of the ultrashort pulse laser is inclined and incident at a constant angle from a normal direction of the first surface of the object to be processed. The condensed laser light is tilted and rotated at the aforementioned angle to perform circular scanning, and the processed surface is tilted for processing. Thereby, a circular cutting line can be produced.
另外,特徵為具有進行複數次前述相對移動並在各相對移動之間變更前述雷射光之射束腰部之高度的操作。藉此,於被加工物體中形成空洞達到深部,所以能施行從部分切斷到完全切斷的加工。Further, it is characterized in that it has an operation of performing the above-described relative movement a plurality of times and changing the height of the beam waist of the aforementioned laser light between the relative movements. Thereby, a cavity is formed in the object to be processed to reach a deep portion, so that the process from the partial cutting to the complete cutting can be performed.
另一方面,本發明係一種被加工物體的切斷方法,其特徵為:在對前述記載的被加工物體進行雷射加工以後,沿著加工部分以少量的應力來切斷前述被加工物體。藉此,能正確地沿著切斷線來分割被加工物體。On the other hand, the present invention is a method for cutting an object to be processed, characterized in that after the laser processing of the object to be processed described above, the object to be processed is cut by a small amount of stress along the processed portion. Thereby, the object to be processed can be accurately divided along the cutting line.
另外,一種液晶顯示面板的基板切斷方法,其特徵為具有:液晶顯示面板具有第1基板和第2基板的積層構造,於第2片基板之第1基板側的表面所搭載之零件上塗佈、黏著或者貼緊對前述雷射波長而言為不透明的材料,從第1基板側照射雷射,使得在第1基板內形成射束腰部之步驟,在前述照射時,避免通過第1基板的雷射光對前述零件造成損害。In addition, the liquid crystal display panel has a laminated structure of a first substrate and a second substrate, and is coated on a surface of the second substrate on the surface on the first substrate side. a cloth that adheres or adheres to a material that is opaque to the aforementioned laser wavelength, and irradiates the laser from the first substrate side so as to form a beam waist portion in the first substrate, and avoids passing the first step in the irradiation. The laser light of the substrate causes damage to the aforementioned components.
另外,在本發明中,提供第1以及第2基板與在其之間部分地包夾間隔物而平行配置之構造體的分割方法。方法如下所述。Further, in the present invention, a method of dividing the first and second substrates and a structure in which the spacers are partially interposed between the first and second substrates is provided in parallel. The method is as follows.
具有:透過聚光手段而使具有對第1以及第2基板而言為透明之波長的脈波寬度100ps以下之超短脈波雷射聚光,並從第1基板外側進行照射,使得射束腰部位置會形成於任一個基板的表面或者內部,由於該超短脈波雷射傳播所造成之自集束作用而在該超短脈波雷射光之行進方向上形成聚光通道,藉以在該聚光通道部中形成空洞,使該 超短脈波雷射光相對移動,以形成切割線的切割線形成步驟;以及爾後沿著該切割線來切斷形成有前述切割線之基板的基板切斷步驟。從具有多層基板,特別是2層基板的構造體之僅一方的面照射雷射射束並進行加工,所以能謀求設備的簡化。The ultrashort pulse laser having a pulse width of 100 ps or less having a wavelength transparent to the first and second substrates is condensed by a condensing means, and is irradiated from the outside of the first substrate to cause a beam The waist position is formed on the surface or inside of any one of the substrates, and the concentrating channel is formed in the traveling direction of the ultrashort pulse laser light due to the self-concentration caused by the ultrashort pulse laser propagation, thereby Forming a cavity in the concentrating channel portion, so that The ultrashort pulse laser light is relatively moved to form a cutting line forming step of the cutting line; and the substrate cutting step of cutting the substrate on which the cutting line is formed is cut along the cutting line. Since only one of the structures having the multilayer substrate, in particular, the two-layer substrate, is irradiated with a laser beam and processed, the simplification of the device can be achieved.
另外,本發明之特徵為進一步在前述切割線形成步驟中具有下述步驟A,在該基板切斷步驟中具有下述步驟C。Further, the present invention is characterized in that it further has the following step A in the dicing line forming step, and has the following step C in the substrate cutting step.
另外,本發明之特徵為在前述切割線形成步驟中具有下述A及B之步驟,以A、B或者是B、A的順序來實施,在前述基板切斷步驟中具有下述C及D之步驟,以C、D的順序來實施。藉此,因為能形成不面對第1基板的第2基板之部分,所以變得能在第2基板內側之面上或者在其面之上部形成控制電路,能謀求液晶面板等顯示面板的薄型化。Further, the present invention is characterized in that the steps of forming A and B described below in the dicing line forming step are carried out in the order of A, B or B, A, and have the following C and D in the substrate cutting step. The steps are implemented in the order of C and D. In this way, since the portion of the second substrate that does not face the first substrate can be formed, the control circuit can be formed on the inner surface of the second substrate or on the upper surface of the second substrate, and the display panel such as the liquid crystal panel can be made thin. Chemical.
步驟A:以使該射束腰部透過第1基板而來到第2基板的方式來使該超短脈波雷射聚光,並在第2基板上形成第1切割線,進一步以使射束腰部位於第1基板的方式來進行聚光,並在和第1切割線相同之平面位置上使該超短脈波雷射相對移動,藉以在第1基板上形成第2切割線Step A: concentrating the ultrashort pulse laser light so that the beam waist passes through the first substrate and reaches the second substrate, and forms a first cutting line on the second substrate, and further emits the light. The waist portion is positioned on the first substrate to condense, and the ultrashort pulse laser is relatively moved at the same plane position as the first dicing line, thereby forming a second cutting line on the first substrate.
步驟B:以使前述射束腰部位於第1基板的方式來使前述超短脈波雷射聚光,以與第2切割線隔開既定距離而平行地使前述超短脈波雷射光相對移動,藉以在第1基板上形成第3切割線。Step B: concentrating the ultrashort pulse laser light so that the beam waist portion is located on the first substrate, and the ultrashort pulse laser light is relatively parallel with a predetermined distance from the second cutting line. The movement is performed to form a third cutting line on the first substrate.
步驟C:治著第1以及第2切割線來切斷第2以及第1 基板,藉以分割該構造體。Step C: The first and second cutting lines are pressed to cut the second and the first The substrate is used to divide the structure.
步驟D:沿著第3切割線來切斷第1基板,藉以從第1基板的第2切割線除去第3切割線的部分。Step D: The first substrate is cut along the third cutting line, and the portion of the third cutting line is removed from the second cutting line of the first substrate.
此外,前述構造體係在第2基板之面對第1基板側的面上具有金屬薄膜,此外,前述間隔物係封止材料,並構成由第1以及第2基板與該封止材料所包圍的空間,在該空間形成電子零件,前述金屬薄膜係存在為橫跨該空間內側和外側,且前述金屬薄膜係電氣連接於該電子零件時,因為金屬薄膜橫跨封止體,此金屬薄膜係電氣連接於形成在被封止體內部的該電子零件,所以此金屬薄膜能作為配線而使用,在封止部外側將該電子零件進行配線。Further, the structural system has a metal thin film on a surface of the second substrate facing the first substrate side, and the spacer is a sealing material and is surrounded by the first and second substrates and the sealing material. a space in which an electronic component is formed, the metal thin film is present across the inner side and the outer side of the space, and when the metal thin film is electrically connected to the electronic component, since the metal thin film straddles the sealing body, the metal thin film is electrically Since the electronic component is formed in the inside of the sealed body, the metal thin film can be used as a wiring, and the electronic component is wired outside the sealing portion.
此外,本發明係一種雷射加工裝置,其特徵為具有:超短脈波雷射產生裝置;旋轉鏡,使從前述超短脈波雷射產生裝置產生的脈波雷射光以一定的角度偏向並旋轉;聚光透鏡,以使被偏向之前述脈波雷射光的光路徑和光軸一致的方式,與前述旋轉鏡同步並旋轉,焦點會藉由旋轉來描繪圓軌跡;以及使前述聚光透鏡沿著前述光軸方向而移動的手段與加工物體搭載手段。藉此構成,能以圓形方式將切斷線劃入被加工物體,進一步沿著切斷線來切斷成圓形。Furthermore, the present invention is a laser processing apparatus characterized by comprising: an ultrashort pulse wave laser generating device; and a rotating mirror for deflecting the pulsed laser light generated from the ultrashort pulse wave laser generating device at a certain angle And rotating; the condensing lens, in such a manner that the light path and the optical axis of the pulsed laser light that is biased toward the same are synchronized with the rotating mirror, the focus is rotated to draw a circular trajectory; and the concentrating lens is made A means for moving along the optical axis direction and a processing object mounting means. According to this configuration, the cutting line can be drawn into the object to be processed in a circular manner, and further cut into a circular shape along the cutting line.
由於自集束作用的產生,在雷射光的行進方向上,聚光通道係形成為比射束腰部涵蓋更長的距離,在聚光通道部分中形成空洞,在聚光通道部中形成達到第2面的空洞 或者到達第2面附近的空洞,所以雷射光行進方向的加工距離會作成比通常的剝離加工還要大。Due to the self-bundling action, in the traveling direction of the laser light, the concentrating channel is formed to cover a longer distance than the beam waist, and a cavity is formed in the concentrating channel portion, and the formation is achieved in the concentrating channel portion. 2 holes Or the cavity near the second surface is reached, so the processing distance of the laser light traveling direction is made larger than the normal peeling process.
以下,說明本發明的實施形態。第1圖係表示本發明之加工方法的實施形態的圖。藉由準直儀(未圖示)來使從超短脈波雷射產生裝置1輸出之作為超短脈波15的雷射光(射束)2成平行,入射於聚光透鏡3等的聚光手段,作為集束雷射射束5而從被加工物體4之正面45入射。超短脈波的雷射就是脈波寬度100ps以內的雷射。作為前述被加工物體4的範例,則舉出玻璃、藍寶石、或者鑽石等之介電體材料、或者矽或氮化鎵等的半導體材料。另外,被加工物體4較為適當係基板等之平板狀物體。因此,以下,有時也將被加工物體4稱為基板。雷射則挑選成為對於被加工物體而言為透明之波長者。在此,透明並不一定侷限於100%使光透過的意義。也包含能透過某種程度之雷射光的情形。例如,當以被加工物體作為矽基板時,只要是波長為1 μm至2 μm的紅外區域即可。作為雷射媒體的範例除了鈦藍寶石結晶(中心波長780nm)以外,還舉出添加鉺之纖維、添加鐿之纖維、Nd:YAG結晶、Nd:YVO4 結晶、Nd:YLF結晶等。另外,在以玻璃基板作為被加工物體的情況下,雷射媒體係較佳是作為鈦藍寶石結晶(中心波長780nm)。Hereinafter, embodiments of the present invention will be described. Fig. 1 is a view showing an embodiment of a processing method of the present invention. The laser beam (beam) 2 as the ultrashort pulse wave 15 outputted from the ultrashort pulse wave laser generating device 1 is paralleled by a collimator (not shown), and is incident on the collecting lens 3 or the like. The light means is incident from the front surface 45 of the object 4 as the bundled laser beam 5. A laser with an ultrashort pulse is a laser with a pulse width of 100 ps or less. Examples of the object to be processed 4 include a dielectric material such as glass, sapphire, or diamond, or a semiconductor material such as tantalum or gallium nitride. Further, the object to be processed 4 is suitably a flat object such as a substrate. Therefore, in the following, the object to be processed 4 is sometimes referred to as a substrate. The laser is selected to be the wavelength that is transparent to the object being processed. Here, transparency is not necessarily limited to the meaning of 100% transmission of light. It also includes situations where a certain amount of laser light can pass through. For example, when the object to be processed is used as the substrate, it is only required to be an infrared region having a wavelength of 1 μm to 2 μm. Examples of the laser medium include titanium sapphire crystal (center wavelength: 780 nm), fiber added with yttrium, fiber added with yttrium, Nd:YAG crystal, Nd:YVO 4 crystal, Nd:YLF crystal, and the like. Further, in the case where a glass substrate is used as the object to be processed, the laser medium is preferably a crystal of titanium sapphire (center wavelength: 780 nm).
此外,正面就是雷射光所入射之側的面,而與其相反之側的面則稱為反面。集束雷射射束5在被加工物體4的 內部形成作為聚光點的射束腰部6。將集束雷射射束5照射於被加工物體4,將此射束腰部6對準於從正面45到反面44之被加工物體內部的適當位置而照射射束。In addition, the front side is the side on which the laser light is incident, and the side opposite to the side is called the reverse side. Cluster laser beam 5 in the object 4 being processed The beam waist 6 as a condensing point is formed inside. The bundled laser beam 5 is irradiated onto the object 4 to be processed, and the beam waist 6 is aligned with an appropriate position inside the object to be processed from the front surface 45 to the back surface 44 to illuminate the beam.
調整集束雷射射束5之能量、波長以及脈波寬度及前述聚光透鏡3的焦點距離或聚光位置,在被加工物體4的內部以高功率密度來將超短脈波聚光,從射束腰部6朝著行進方向發生根據克爾效應的自集束作用,形成具有射束腰部6程度之直徑的細射束之傳播通道8。在第1圖中,以在被加工物體4之厚度7內部,從反面44向正面方向而形成雷射射束腰部6的方式來設定照射條件時,入射的集束雷射射束5係從射束腰部6在功率密度微弱而未發生由克爾效應引起之自集束作用的區域中,一旦在因射束腰部所聚光後,作為發散性之射束10而傳播,但出現克爾效應之非常高功率密度的聚光點形成於射束腰部時,細線狀之通道8會沿著形成為涵蓋距離13,被加工物體內部之通道8而傳播,一邊消耗雷射射束能量一邊朝著反面44前進,能在反面44維持著可維持克爾效應程度的能量時,位於通道8的被加工物體之一部分會由於衝擊波而被周圍壓縮,結果會形成細的空洞,剩餘部份會從反面而被排出至外部,或者在未被排出時,就在反面44上形成隆起,細長的空洞會沿著通道8而被形成涵蓋從射束腰部6至反面44為止的距離14。到達了反面44還未被被加工物體所吸收之射束會因為不再因自集束作用而被封閉,所以會作為發散性射束11而被放出。Adjusting the energy, the wavelength, and the pulse width of the concentrated laser beam 5 and the focal length or condensing position of the condensing lens 3, and collecting the ultrashort pulse at a high power density inside the object 4, from The beam waist 6 is self-concentrating according to the Kerr effect in the direction of travel, forming a propagation path 8 of the beam of fine beams having a diameter of the beam waist 6 . In the first drawing, when the irradiation condition is set so that the laser beam waist portion 6 is formed from the reverse surface 44 to the front side in the thickness 7 of the workpiece 4, the incident concentrated laser beam 5 is received. The beam waist 6 is propagated as a divergent beam 10 in a region where the power density is weak and the self-assembly due to the Kerr effect does not occur, but after the light is concentrated by the beam waist, the Kerr effect occurs. When a very high power density spot is formed at the beam waist, the thin-line channel 8 propagates along the channel 8 formed to cover the distance 13 and the inside of the object, while consuming the laser beam energy When the reverse side 44 advances and the energy of the Kerr effect can be maintained on the reverse side 44, part of the object to be processed located in the channel 8 is compressed by the surrounding wave, and as a result, a fine void is formed, and the remaining portion is from the reverse side. When it is discharged to the outside or when it is not discharged, a bulge is formed on the reverse side 44, and an elongated cavity is formed along the passage 8 to cover a distance 14 from the beam waist 6 to the reverse side 44. The beam that has reached the reverse side 44 and has not been absorbed by the object to be processed is released as a divergent beam 11 because it is no longer closed by the self-concentration action.
作為使由在被加工物體中之自集束作用所引起的射束之聚光效果變得明顯的條件,會有根據文獻J.H.Marburger,Prog.Quantum Electron.,Vo1.4,p.35(1975).’以被稱為自集束之臨界閾值功率P cr 的數式1所表示的指標。As a condition for making the condensing effect of the beam caused by the self-bundling action in the object to be processed, there will be a condition according to the literature JH Marburger, Prog. Quantum Electron., Vo1.4, p. 35 (1975). 'An index expressed by Equation 1 which is called the critical threshold power P cr of the self-assembly.
<BR>在數式1中,λ為雷射波長,no 為物體的折射率,n 2 為物體之非線形折射率。In Equation 1, λ is the laser wavelength, no is the refractive index of the object, and n 2 is the nonlinear refractive index of the object.
根據數式1,例如石英玻璃之自集束的臨界閾值功率是2.3MW,入射於被加工物體的雷射脈波之峰值輸出(以雷射脈波寬度所除算雷射脈波能量而得的值)變得比此值更大時,會明顯地引起自集束作用。According to Equation 1, for example, the critical threshold power of the self-assembly of quartz glass is 2.3 MW, and the peak output of the laser pulse incident on the object to be processed (the value obtained by dividing the laser pulse energy by the laser pulse width) When it becomes larger than this value, it will obviously cause self-bundling.
藉由謀求超短脈波雷射的能量、波長、脈波寬度、以及聚光透鏡的焦點距離、聚光位置的調整,能改變自集束作用的產生狀況。藉此,會形成到達反面的空洞、或到達反面附近的空洞。在此,面附近就是包含從此面朝向內部方向直至作為基板等之被加工對象的物體之厚度的1/10左右的距離者。可如同以下來設定空洞形成狀態。The generation of the self-concentration action can be changed by adjusting the energy, the wavelength, the pulse width of the ultrashort pulse laser, and the adjustment of the focal length and the condensing position of the condensing lens. Thereby, a cavity that reaches the opposite side or a hole that reaches the vicinity of the opposite side is formed. Here, the vicinity of the surface is a distance including about 1/10 of the thickness of the object to be processed from the surface toward the inside direction. The void formation state can be set as follows.
(1)因為空洞未到達反面,所以會形成反面隆起比周邊表面還要高且機械強度弱的隆起構造。(1) Since the cavity does not reach the reverse side, a ridge structure in which the reverse surface ridge is higher than the peripheral surface and the mechanical strength is weak is formed.
(2)形成前述聚光通道直至反面,藉以形成空洞直至反面。(2) Forming the aforementioned concentrating channel up to the reverse side, thereby forming a cavity to the reverse side.
(3)從正面形成前述聚光通道直至反面,藉以從正面形成空洞直至反面。(3) The aforementioned concentrating channel is formed from the front surface to the reverse side, thereby forming a cavity from the front surface to the reverse side.
(4)聚光通道從正面形成僅至加工物體內部,藉以從正面形成空洞僅至加工物體內部。(4) The concentrating passage is formed from the front surface only to the inside of the processed object, thereby forming a void from the front surface only to the inside of the processed object.
藉由本發明,利用聚光光學系統,將具有對被加工物體而言為透明之波長的超短脈波雷射光,在基板內聚光成非常小之雷射光截面積,藉以在聚光點實現高功率密度的聚光點,藉此,當在基板內傳播之雷射光一旦被聚光時,會產生由克爾效應引起之自集束作用,另一方面在聚光點發生由電漿引起的散焦作用,藉由這2種作用的平衡,雷射脈波光的傳播會形成自集束作用之被自困陷 (self-trapped)的細線。此困陷的範圍,能夠以比在通常的功率等級之未出現自集束作用的條件下的焦點附近形成之射束腰部的焦點深度還要大上數倍之距離的值,來形成自集束作用的雷射光傳播通道。通道的長度會由於材料特性、雷射射束的功率密度、能量等的參數而變化。因為通道的雷射光傳播方向之端部到達反面,爾後由於蓄積在通道內部的能量而造成局部的高溫、高壓力狀態且從內部朝向外部的力量會發揮作用,所以上述自集束作用的聚光通道之通過軌跡中會形成並殘留空洞。According to the present invention, the ultra-short pulse laser light having a wavelength transparent to the object to be processed is condensed into a very small laser light cross-sectional area in the substrate by the concentrating optical system, thereby realizing at the condensing point. a high-power-density condensing point, whereby when the laser light propagating in the substrate is condensed, self-collection caused by the Kerr effect occurs, and on the other hand, the scattering caused by the plasma occurs at the condensing point. By the action of the two kinds of effects, the propagation of the laser pulse wave will form a self-collecting trap. (self-trapped) thin line. The range of the trap can be self-bundled by a value that is several times larger than the depth of focus of the beam waist formed near the focus under the condition of the normal power level without self-bundling. The action of the laser light propagation channel. The length of the channel will vary due to material characteristics, power density of the laser beam, energy, and the like. Since the end of the laser light propagation direction of the channel reaches the reverse side, and then the local high temperature and high pressure state is caused by the energy accumulated in the channel, and the force from the inside to the outside acts, the above-mentioned self-concentrating concentrating channel A void is formed and remains in the trajectory.
如第2圖所示,沿著掃描線48形成由自集束作用造成之長圓筒型通道的空洞,該自集束作用係從被加工物體4內之雷射光的聚光點,將超短脈波雷射光2在行進方向16上形成為長型。此外,在形成以後,於掃描線48以直角方 向施加彎曲應力49來進行切斷的情況下,因為相較於穴徑,形成了非常深的孔穴,所以沿著此溝的線(切割線)之作用是切斷的起點,沿著切割線,即使是較弱的應力也能進行切斷。因為在基板的反面上形成連續之淺溝槽或構造上較弱的隆起構造,所以切斷方向僅沿著掃描線48,亦即切割線便能確實地產生。會有在反面附近於表面空出孔穴的情況、或通道出口部之隆起比周圍表面還要高且機械強度弱之構造的情況,但不管是在任一種情況下,使雷射光在基板之欲切斷的方向上掃描,藉以沿著掃描線48,亦即切割線來形成從基板內部深處到達反面的加工形狀。因為能充分獲得加工溝槽的深度,所以往後能以少量的彎曲應力49沿著掃描線48來切斷基板。切割線的形成方面,亦可不藉由雷射光的移動,而是由被加工物體4的移動來完成。任一種移動都稱為相對的掃描。另外,在欲破斷的方向上掃描雷射光的情況下,藉由調整掃描速度,可在破斷面上連續地設置切割線,也可空出間隔而離散地設置切割線,在任一個情況下,可藉由少量的彎曲應力而沿著切割線來切斷基板。As shown in Fig. 2, a cavity of a long cylindrical passage caused by self-bundling is formed along the scanning line 48, and the self-bundling action is an ultrashort pulse from the condensed point of the laser light in the object 4 to be processed. The laser light 2 is formed in a long shape in the traveling direction 16. In addition, after formation, the scan line 48 is at a right angle. When the bending stress 49 is applied to perform the cutting, since a very deep hole is formed as compared with the hole diameter, the line along the groove (cutting line) acts as the starting point of the cutting, along the cutting line. It can cut even with weak stress. Since a continuous shallow groove or a structurally weak ridge structure is formed on the reverse side of the substrate, the cutting direction is only along the scanning line 48, that is, the cutting line can be surely produced. There may be a case where a hole is vacated on the surface near the reverse side, or a structure in which the ridge of the exit portion of the passage is higher than the surrounding surface and the mechanical strength is weak, but in either case, the laser light is cut on the substrate. Scanning in the direction of the break, thereby forming a machined shape from the deep inside of the substrate to the reverse side along the scan line 48, that is, the cut line. Since the depth of the processing groove can be sufficiently obtained, the substrate can be cut along the scanning line 48 with a small amount of bending stress 49 in the past. The formation of the cutting line may be performed not by the movement of the laser light but by the movement of the object 4 to be processed. Any kind of movement is called a relative scan. Further, in the case of scanning the laser light in the direction to be broken, by adjusting the scanning speed, the cutting line can be continuously provided on the broken section, or the cutting line can be discretely provided with the interval, in either case. The substrate can be cut along the cutting line by a small amount of bending stress.
第3圖係表示將雷射光聚光於被加工物體的某個高度並且掃描被加工物體一次而加工以後,變更雷射光聚光點的聚光位置,再一次進行加工的方法。首先,如第3(a)圖所示,將雷射光的射束腰部對焦於從被加工物體4的反面44朝向內部而隔開空洞形成距離57(135 μm左右)左右處,形成由自集束作用造成的通道8,沿著掃描方向47而直線 地掃描一次。藉此,直線地形成空洞列。接著,如第3(b)圖所示,沿著光軸方向使聚光透鏡3移動,僅以空洞形成距離58左右使形成射束腰部之高度朝向正面側挪移,而形成通道8並再次掃描。此時,因為在由初次掃描所造成之加工線35上進行掃描,所以空洞列會形成為與初次掃描所形成之空洞列大致連續地接續。此外,若有需要,如第3(c)圖所示,進行射束腰部的高度移動和用於形成空洞列的掃描。高度移動和掃描係僅重複必要的次數。藉由此操作之重複,而形成合體於被加工物體4之內部的直線狀之空洞壁面。最後,對被加工物體4賦予彎曲應力而沿著空洞壁來切斷。初次的掃描中,空洞不一定必須到達反面。另外,可重複高度移動以及掃描一直到射束腰部到達正面為止。藉由這種方法,因為在被加工物體上重複空洞形成於深部,所以能施行從部分切斷至完全切斷的加工。Fig. 3 is a view showing a method of concentrating the laser beam at a certain height of the object to be processed and scanning the object to be processed once, and then changing the condensing position of the laser light condensing point, and processing again. First, as shown in Fig. 3(a), the beam waist of the laser beam is focused on the cavity forming distance 57 (about 135 μm) from the opposite surface 44 of the workpiece 4 toward the inside, and is formed by Channel 8 caused by clustering, along the scanning direction 47 and straight Scan once. Thereby, a hole column is formed linearly. Next, as shown in the third figure (b), the condensing lens 3 is moved in the optical axis direction, and the height of the beam waist is shifted toward the front side only by the cavity forming distance of about 58 to form the channel 8 and again. scanning. At this time, since the scanning is performed on the processing line 35 caused by the initial scanning, the void array is formed to be substantially continuous with the hollow row formed by the initial scanning. Further, if necessary, as shown in Fig. 3(c), the height movement of the beam waist and the scanning for forming the hole row are performed. The height movement and scanning system is only repeated as many times as necessary. By repeating this operation, a linear cavity wall surface that fits inside the workpiece 4 is formed. Finally, the workpiece 4 is subjected to bending stress and cut along the cavity wall. In the initial scan, the hole does not have to reach the opposite side. In addition, the height movement and scanning can be repeated until the beam waist reaches the front. According to this method, since the cavity is formed in the deep portion in the object to be processed, the machining from the partial cutting to the complete cutting can be performed.
作為加工對象物體的基板不限於1片。即使是相同種類或者相異種類材料之重疊2片以上的基板的多層構造,也能對所有的基板進行加工。多層構造的情況下,使基板貼緊也可、或分開亦可,在分開的情況下,空隙除了是空氣以外,還可以是有機材料或透明電極層。在作為基板2片的情況下,如第4圖所示,也會有由置於雷射入射光側之上部基板81與置於相反側之下部基板82所構成,而含有空隙83的情形。若以此方法,即使是由複數層所組成的玻璃也能應用本發明的方法。The substrate as the object to be processed is not limited to one sheet. Even in a multilayer structure in which two or more substrates of the same type or different types of materials are stacked, all the substrates can be processed. In the case of a multilayer structure, the substrates may be attached to each other or may be separated. In the case of separation, the voids may be organic materials or transparent electrode layers in addition to air. In the case of two sheets as the substrate, as shown in Fig. 4, there are cases in which the upper surface substrate 81 placed on the laser incident light side and the lower surface substrate 82 are placed on the opposite side, and the space 83 is included. In this way, the method of the present invention can be applied even to a glass composed of a plurality of layers.
如第4圖所示,基板2片的情況下,下部基板82會進 行比雷射傳送方向更長的加工。這是因為自集束作用會依隨著被加工物體中的傳送距離而增加。另外,在形成由於自集束作用的聚光通道時,必須10至200 μm左右之距離的雷射在被加工物體內傳播。此距離越長,即使是相同能量也會形成長的空洞。若利用此特點,於基板之正面側載置由與其同種或對雷射光而言為透明之異種材料所組成的其他基板,藉以實效地增強自集束作用,能夠增長空洞形成距離,進行更深的加工。特別是,在被加工物體上從正面到反面形成聚光通道,也能將空洞形成為涵蓋從正面到反面。在非被加工物體的其他基板中,有時候不會形成空洞,而有時候會形成空洞。As shown in Fig. 4, in the case of two substrates, the lower substrate 82 will advance. The processing is longer than the laser transmission direction. This is because the self-concentration will increase depending on the transmission distance in the object being processed. Further, when a condensing path due to self-concentration is formed, a laser having a distance of about 10 to 200 μm must propagate in the object to be processed. The longer this distance, the longer the hole will be formed even with the same energy. By using this feature, other substrates composed of different materials which are the same kind or transparent to the laser light are placed on the front side of the substrate, thereby effectively enhancing the self-bundling effect, thereby increasing the cavity formation distance and performing deeper processing. . In particular, the formation of a collecting channel on the object to be processed from the front to the back can also form a cavity to cover from the front to the back. In other substrates of non-processed objects, sometimes voids are not formed, and sometimes voids are formed.
此方法能適用於切斷液晶顯示面板的玻璃基板。液晶顯示面板的玻璃基板之構造係由夾著空隙而置於雷射入射光側的上部基板和置於相反側的下部基板所構成。This method can be applied to cutting a glass substrate of a liquid crystal display panel. The structure of the glass substrate of the liquid crystal display panel is constituted by an upper substrate placed on the side of the laser incident light with the gap interposed therebetween and a lower substrate placed on the opposite side.
於上部玻璃基板,從上面側照射超短脈波雷射,使得雷射射束腰部來到該基板的表面或者內部之適當位置時,於上部玻璃基板形成空洞。藉由使雷射光相對地移動,而在上部玻璃基板形成切斷面(切割線)。On the upper glass substrate, an ultrashort pulse laser is irradiated from the upper side such that when the waist of the laser beam comes to a suitable position on the surface or inside of the substrate, a void is formed in the upper glass substrate. A cut surface (cut line) is formed on the upper glass substrate by relatively moving the laser light.
從下部玻璃基板也一樣地從上部玻璃基板之上面側照射超短脈波雷射,藉以形成切斷面。以雷射射束腰部來到該基板的表面或者內部之適當位置的方式進行照射。超短脈波雷射能不對上部玻璃基板造成損傷而透過,能在下部玻璃基板形成空洞。藉由掃描超短脈波雷射,於下部玻璃基板形成切斷面(切割線)。The ultrashort pulse laser is irradiated from the upper surface side of the upper glass substrate from the lower glass substrate in the same manner to form a cut surface. Irradiation is performed in such a manner that the laser beam waist comes to a suitable position on the surface or inside of the substrate. The ultra-short pulse laser can penetrate without causing damage to the upper glass substrate, and can form a void in the lower glass substrate. A cut surface (cut line) is formed on the lower glass substrate by scanning the ultrashort pulse laser.
第5(a)圖係表示液晶顯示面板截面圖。液晶顯示面板90係由玻璃基板2片組成之積層構造所構成。在上部玻璃基板91之內側表面上形成透明電極、彩色濾波片、薄膜電晶體等的零件95,在下部玻璃基板92的內側表面則形成電極等的零件96。另外,在2片的玻璃基板之間填充液晶93。液晶係被封入於氣密封止材料94中。切斷步驟中,有時會治著相同的切斷線來切斷上部玻璃基板和第2玻璃基板,或者有時是以稍微偏離的其他切斷線來進行切斷步驟。在沿著相同的切斷線來切斷的情況下,可採用前述之第4圖所示之使2片以上的基板重疊並對所有基板進行加工的情況即可。Fig. 5(a) is a cross-sectional view showing the liquid crystal display panel. The liquid crystal display panel 90 is composed of a laminated structure composed of two sheets of a glass substrate. A component 95 such as a transparent electrode, a color filter, or a thin film transistor is formed on the inner surface of the upper glass substrate 91, and a component 96 such as an electrode is formed on the inner surface of the lower glass substrate 92. Further, a liquid crystal 93 is filled between two glass substrates. The liquid crystal system is sealed in the hermetic sealing material 94. In the cutting step, the upper glass substrate and the second glass substrate may be cut by the same cutting line, or the cutting step may be performed by other cutting lines that are slightly deviated. In the case of cutting along the same cutting line, the two or more substrates may be stacked and processed on all the substrates as shown in FIG. 4 described above.
第5(a)圖係進一步表示以偏離之其他切斷線來進行切斷步驟。在此步驟中,進行上部玻璃基板的切斷97及下部玻璃基板的切斷98。從上部玻璃基板91的正面照射集束雷射射束5,使得雷射射束腰部來到該基板內部之適當位置時,在上部玻璃基板91的反面附近形成空洞61。藉由掃描集束雷射射束5,於上部玻璃基板91形成切斷面。此時,因為在上部玻璃基板91的加工中未消耗的雷射射束會透過上部玻璃基板91,並照射於在下部玻璃基板92上形成的電極等之零件96,所以對電極等的零件96造成損害,最後會對作為液晶顯示裝置之動作造成不良影響。為了防止這種不良影響,如第5(b)圖所示,事前在電極等之零件96的被雷射射束照射的位置上塗佈、黏著或者貼緊而預先形成保護用塗佈層99。保護用塗佈層99係對於集束雷射射束的 波長而言為不透明者。在此,所謂的不透明,不僅是完全不透過雷射光的情況,也包含能達成不會對保護用塗佈層99下之電極等的零件96造成損害之目的而透過微量的光者。Fig. 5(a) further shows that the cutting step is performed with other cutting lines that are offset. In this step, the cutting 97 of the upper glass substrate and the cutting 98 of the lower glass substrate are performed. When the concentrated laser beam 5 is irradiated from the front surface of the upper glass substrate 91 so that the laser beam waist comes to an appropriate position inside the substrate, a cavity 61 is formed in the vicinity of the reverse side of the upper glass substrate 91. A cut surface is formed on the upper glass substrate 91 by scanning the bundled laser beam 5. At this time, since the laser beam that is not consumed in the processing of the upper glass substrate 91 passes through the upper glass substrate 91 and is irradiated to the component 96 such as an electrode formed on the lower glass substrate 92, the component 96 such as the counter electrode is used. Damage is caused, and eventually it will adversely affect the operation as a liquid crystal display device. In order to prevent such an adverse effect, as shown in Fig. 5(b), the protective coating layer 99 is formed in advance by applying, adhering or adhering to the portion of the electrode 96 such as the electrode which is irradiated with the laser beam. . The protective coating layer 99 is for the bundled laser beam It is opaque in terms of wavelength. Here, the term "opaque" includes not only the case where the laser light is not transmitted at all, but also the ability to transmit a small amount of light without causing damage to the component 96 such as the electrode under the protective coating layer 99.
與對上部玻璃基板91的加工分開,另外進行對下部玻璃基板92的加工。這同樣地,以從上部玻璃基板91的正面照射集束雷射射束5,但雷射射束腰部來到下部玻璃基板92內部之適當位置的方式來進行照射。集束雷射射束5通過上部玻璃基板91,在下部玻璃基板92的反面附近形成空洞61。掃描集束雷射射束5,藉以在下部玻璃基板92形成切斷面。對玻璃基板施加應力而切開玻璃基板以後,經過將液晶顯示面板組裝於其他零件的步驟,以製造液晶顯示裝置。因此,本方法可用於製造液晶顯示面板以及液晶顯示裝置。The processing of the lower glass substrate 92 is performed separately from the processing of the upper glass substrate 91. Similarly, the concentrated laser beam 5 is irradiated from the front surface of the upper glass substrate 91, but the laser beam waist is irradiated to an appropriate position inside the lower glass substrate 92. The clustered laser beam 5 passes through the upper glass substrate 91, and a cavity 61 is formed in the vicinity of the reverse side of the lower glass substrate 92. The bundled laser beam 5 is scanned to form a cut surface on the lower glass substrate 92. After the glass substrate is subjected to stress and the glass substrate is cut, the liquid crystal display panel is assembled to another component to manufacture a liquid crystal display device. Therefore, the method can be used to manufacture a liquid crystal display panel and a liquid crystal display device.
表示成為複數基板時之其他的實施形態。本實施形態中係表示由2片基板組成之構造體的分割方法。第6圖係用於說明此實施形態的模式截面圖。Another embodiment is shown when it is a plurality of substrates. In the present embodiment, a method of dividing a structure composed of two substrates is shown. Fig. 6 is a schematic cross-sectional view for explaining this embodiment.
構造體70係具有上部玻璃基板91與下部玻璃基板92所平行配置而構成的構造。在作為液晶顯示面板而使用的情況下,構造體70係在2片的玻璃基板之間部分地插入間隔物。為了在2片玻璃基板之間設置空隙而需要間隔物。例如在液晶顯示面板中,配置多數個球狀的矽石或者聚苯乙烯和圓柱狀的光阻材料等之物體。在本實施形態例中,在2片的玻璃基板之間插入氣密封止材料94,原來的目的 是在該玻璃基板和此氣密封止材料94中構成封閉空間,但在未另外插入物體的情況下,也擔任間隔物的角色。在不插入氣密封止材料94的情況下,則另外插入間隔物。在下部玻璃基板92的上面,以某個範圍來設置金屬薄膜配線89。在具有前述氣密封止材料的情況下,前述封閉空間之下部玻璃基板92上配置有電子零件(未圖示),另外,金屬薄膜配線89係較佳為電氣連接於該電子零件,並配置成跨過氣密封止材料94。若構造體是液晶顯示面板時,則在該封閉空間中形成顯示裝置要件。The structure 70 has a structure in which the upper glass substrate 91 and the lower glass substrate 92 are arranged in parallel. In the case of being used as a liquid crystal display panel, the structure 70 is partially inserted into a spacer between two glass substrates. A spacer is required in order to provide a gap between two glass substrates. For example, in a liquid crystal display panel, a plurality of spherical vermiculite or an object such as a polystyrene and a cylindrical photoresist is disposed. In the present embodiment, the gas sealing material 94 is inserted between the two glass substrates, and the original purpose is In the glass substrate and the hermetic sealing material 94, a closed space is formed, but in the case where an object is not additionally inserted, it also functions as a spacer. In the case where the hermetic sealing material 94 is not inserted, a spacer is additionally inserted. On the upper surface of the lower glass substrate 92, the metal thin film wiring 89 is provided in a certain range. In the case of the gas-shielding material, the electronic component (not shown) is disposed on the glass substrate 92 on the lower portion of the closed space, and the metal film wiring 89 is preferably electrically connected to the electronic component. The gas seal stop material 94 is spanned. If the structure is a liquid crystal display panel, a display device element is formed in the closed space.
在此,為了能從外部接近下部玻璃基板92上的金屬薄膜配線89,而將構造體70分離。首先,藉由聚光透鏡3從上部玻璃基板91之上面側將超短脈波雷射射束2聚光,以雷射射束腰部來到下部玻璃板92的上面(雷射光入射側的面)或者內部之適當位置(在圖中,雷射射束腰部位於上面上,但並非侷限於此,以下亦然)的方式來進行照射。但是,在下部玻璃板當中則是無金屬薄膜配線89的位置。雷射射束2通過上部玻璃基板91,在下部玻璃基板92內形成由自集束作用造成的空洞64。藉由使雷射射束2相對地移動,以連續或者離散地形成空洞,在下部玻璃基板92形成第1切割線88。Here, the structure 70 is separated in order to be able to approach the metal thin film wiring 89 on the lower glass substrate 92 from the outside. First, the ultrashort pulse laser beam 2 is condensed from the upper surface side of the upper glass substrate 91 by the condensing lens 3, and reaches the upper surface of the lower glass plate 92 with the laser beam waist (on the incident side of the laser light) The surface or the appropriate position inside (in the figure, the laser beam waist is located above, but not limited thereto, the following is also the case) to illuminate. However, among the lower glass sheets, there is no metal film wiring 89. The laser beam 2 passes through the upper glass substrate 91, and a cavity 64 caused by self-concentration is formed in the lower glass substrate 92. The first cutting line 88 is formed on the lower glass substrate 92 by relatively continuously or discretely forming a cavity by relatively moving the laser beam 2.
接著,將聚光透鏡3移向上方,以雷射射束腰部來到上部玻璃板91上面(雷射光入射側的面)上或者內部之適當位置的方式來進行照射。在上部玻璃板91內形成由自集束作用造成的空洞63。藉由使雷射射束2相對地移動,以連 續或者離散地形成空洞,在上部玻璃基板91形成第2切割線87。第2切割線87係形成在第1切割線88的正上方。接著,在形成第1和第2切割線88以及87以前,以與第2切割線87相同的方法,於上部玻璃板91上製作第3切割線86。在此過程中形成空洞62。第3切割線86係較佳為設置在接近上部以及下部的玻璃基板91及92間之氣密封止材料或者間隔物94的位置,通常形成為跨過下部玻璃基板92上面的金屬薄膜配線89。另外,第3的切割線86係形成為與第2切割線87分開距離77(△Y)而平行。Next, the condensing lens 3 is moved upward, and irradiation is performed such that the laser beam waist reaches the upper surface of the upper glass plate 91 (the surface on the laser light incident side) or at an appropriate position inside. A cavity 63 caused by self-concentration is formed in the upper glass plate 91. By moving the laser beam 2 relatively A void is formed continuously or discretely, and a second cutting line 87 is formed on the upper glass substrate 91. The second cutting line 87 is formed directly above the first cutting line 88. Next, before the first and second cutting lines 88 and 87 are formed, the third cutting line 86 is formed on the upper glass plate 91 by the same method as the second cutting line 87. A void 62 is formed during this process. The third cutting line 86 is preferably provided at a position close to the hermetic sealing material or the spacer 94 between the upper and lower glass substrates 91 and 92, and is generally formed so as to straddle the metal thin film wiring 89 on the upper surface of the lower glass substrate 92. Further, the third cutting line 86 is formed to be parallel to the second cutting line 87 by a distance 77 (ΔY).
當具有氣密封止材料,在氣密封止材料和2片基板所構成之封閉空間內部配置電子零件的情況下,第3切割線較佳為設置在該封閉空間外部於接近該氣密封止材料94的位置。In the case of having a hermetic sealing material, in the case where an electronic component is disposed inside the enclosed space formed by the hermetic sealing material and the two substrates, the third cutting line is preferably disposed outside the closed space to approach the hermetic sealing material 94. s position.
此時,在製作上部玻璃基板91之第3切割線86時未消耗的雷射射束2會通過上部玻璃基板91,並照射於金屬薄膜配線89,所以可能會對這些帶來損害。不過,透過上部玻璃基板91的雷射射束2之強度係通常並非強到足以對該等造成損害。另外,為了防止損傷,亦可事前在金屬薄膜配線89之被雷射射束照射的位置上塗佈、黏著或者貼緊而形成保護用塗佈層。保護用塗佈層係如同後述,在沿著第3切割線而被切斷且可從外部接近以後則移除。此外,保護用塗佈層係對於雷射射束之波長而言為不透明者,所謂的不透明,不僅是完全不透過雷射光的情況,也包含能達成不會對該零件造成損害之目的而透過微量的光者。At this time, the laser beam 2 that is not consumed when the third cutting line 86 of the upper glass substrate 91 is formed passes through the upper glass substrate 91 and is irradiated onto the metal thin film wiring 89, which may cause damage thereto. However, the intensity of the laser beam 2 transmitted through the upper glass substrate 91 is generally not strong enough to cause damage thereto. Further, in order to prevent damage, the protective coating layer may be formed by applying, adhering or adhering to the position where the metal thin film wiring 89 is irradiated with the laser beam. The protective coating layer is removed as it will be cut along the third cutting line and can be accessed from the outside as will be described later. In addition, the protective coating layer is opaque to the wavelength of the laser beam, and the so-called opacity is not only completely refracted by the laser light, but also includes the purpose of not causing damage to the part. A trace of light.
如同這般,形成從第1到第3的切割線以後,沿著第1切割線88及其正上方之第2切割線87來對構造體70施加折彎應力時,下部以及上部玻璃基板皆分別設有第1和第2切割線的部分會破斷,藉以沿著第1以及第2切割線來分割構造體70。接著,沿著第3切割線對上部玻璃基板91施加折彎應力時,上部玻璃基板91當中的第2和第3切割線之距離△Y部分會被分離。由以上的順序來切斷構造體70。As described above, after the first to third cutting lines are formed, when the bending force is applied to the structure 70 along the first cutting line 88 and the second cutting line 87 directly above, both the lower portion and the upper glass substrate are formed. The portions where the first and second cutting lines are respectively provided are broken, whereby the structure 70 is divided along the first and second cutting lines. Next, when a bending stress is applied to the upper glass substrate 91 along the third cutting line, the distance ΔY portion of the second and third cutting lines in the upper glass substrate 91 is separated. The structure 70 is cut in the above order.
在第7圖中表示以此方式而切斷的2層構造體。下部玻璃基板92僅擴大相當於第2以及第3切割線間隔11的△Y,且在上部具有無上部玻璃基板91的段差構造。變得能從外部接近下部玻璃基板92擴大的部分。因此,可重新形成控制電路等之電子零件及金屬薄膜配線。另外,在下部玻璃基板上具有從氣密封止部內部導出至外側之金屬薄膜配線的情況下,能連接導出至外部之部分的配線。In Fig. 7, a two-layer structure cut in this manner is shown. The lower glass substrate 92 has only a ΔY corresponding to the second and third dicing line intervals 11 and a stepped structure having no upper glass substrate 91 at the upper portion. It becomes possible to approach the enlarged portion of the lower glass substrate 92 from the outside. Therefore, the electronic parts and the metal thin film wiring of the control circuit and the like can be reformed. Further, when the metal film wiring which is led out from the inside of the hermetic sealing portion to the outside is provided on the lower glass substrate, the wiring which is led to the outside can be connected.
在第7圖中,下部玻璃基板92以及上部玻璃基板91之各個截面66以及65係分別將第1切割線88和第3切割線86作為起點而分割的截面。與第1和第2切割線88以及87形成方法相同,從上部將超短雷射脈波聚光而分別在下部以及上部之玻璃基板上分別形成切割線以後,分割並形成玻璃板的側面68、67。In Fig. 7, each of the cross sections 66 and 65 of the lower glass substrate 92 and the upper glass substrate 91 has a cross section in which the first cutting line 88 and the third cutting line 86 are taken as starting points. Similarly to the formation methods of the first and second cutting lines 88 and 87, the ultrashort laser pulse waves are collected from the upper portion, and the cutting lines are formed on the lower and upper glass substrates, respectively, and then the side faces of the glass sheets are divided and formed. 67.
藉由本實施形態,因為僅從玻璃構造體之單面側照射雷射射束而進行加工,所以能謀求設備的簡化。另外,因為能形成在上部不具有上部基板的下部基板部分,所以能 由外部接近,能從下部基板上面或者在此基板上設置控制電路等之電子零件或者金屬薄膜配線。因此,能謀求顯示面板的薄型化。另外,可連接於從氣密封止部內部導出至外側的其他金屬薄膜配線部分。According to the present embodiment, since the laser beam is irradiated only from the one surface side of the glass structure, the processing can be simplified. In addition, since the lower substrate portion having no upper substrate at the upper portion can be formed, From the outside, an electronic component such as a control circuit or a metal thin film wiring can be provided from the upper substrate or on the substrate. Therefore, it is possible to reduce the thickness of the display panel. Further, it can be connected to another metal thin film wiring portion that is led out from the inside of the hermetic seal to the outside.
第8圖係表示將本實施形態應用於製造液晶面板時之範例的圖。在從形成有多數個液晶板之具有上下2片大型玻璃基板91以及92的大型構造體70來製造液晶面板以後而分割成個別面板80的步驟中,實施本實施形態。該玻璃基板91及92以及插入於其間的氣密封止材料94所包圍之空間中則內建液晶顯示面板所必需之彩色濾波片、液晶93、驅動電晶體、配線、間隔物等(液晶以外則未圖示)。(a)是上視圖以及截面圖,(b)是放大沿著Y方向切斷的截面圖。Z方向為垂直於紙面的方向。Fig. 8 is a view showing an example in which the present embodiment is applied to manufacture of a liquid crystal panel. In the step of manufacturing the liquid crystal panel from the large-sized structure 70 having the two large-sized glass substrates 91 and 92 on the upper and lower sides of the liquid crystal panel, the liquid crystal panel is divided into individual panels 80, and this embodiment is carried out. In the space surrounded by the glass substrates 91 and 92 and the hermetic sealing material 94 interposed therebetween, a color filter, a liquid crystal 93, a driving transistor, a wiring, a spacer, and the like necessary for the liquid crystal display panel are built in (other than the liquid crystal) Not shown). (a) is a top view and a cross-sectional view, and (b) is an enlarged cross-sectional view cut along the Y direction. The Z direction is a direction perpendicular to the paper surface.
如同以下來形成沿著X方向的切割線74-1~74-m。對下部玻璃基板92形成第1切割線88係在其上面,於下部玻璃板中無金屬薄膜配線89的部分進行。另外,在上部玻璃基板91中,於第1切割線88上形成第2切割線87。另外,於上部玻璃基板,較佳為將第3切割線設置在接近氣密封止材料94的位置。第3切割線86係與第2切割線87分開距離77(△Y)而平行。第3切割線86係通常形成為跨過金屬薄膜配線89。The cutting lines 74-1 to 74-m along the X direction are formed as follows. The lower cut glass 88 is formed on the lower glass substrate 92, and the metal thin film wiring 89 is not provided in the lower glass plate. Further, in the upper glass substrate 91, a second cutting line 87 is formed on the first dicing line 88. Further, in the upper glass substrate, it is preferable to provide the third cutting line at a position close to the gas seal stopper 94. The third cutting line 86 is parallel to the second cutting line 87 by a distance 77 (ΔY). The third cutting line 86 is usually formed to straddle the metal thin film wiring 89.
沿著Y方向的切割線73-1~73-n係僅以面板寬度76之間隔而逐一設置1條切割線即可。能與形成前述第1和第2切割線之方法相同地進行設置。The cutting lines 73-1 to 73-n along the Y direction may be provided with one cutting line one by one at intervals of the panel width 76. It can be set in the same manner as the method of forming the first and second cutting lines.
因為形成切割線以後,能沿著在其上部和下部之玻璃基板而形成的切割線而分割,以此方式在X、Y方向上分割,所以能從大型2層構造體70製造多數片液晶顯示面板80。在此情況下,特別是在液晶顯示面板80之至少1個側面上,在下部玻璃基板92之上,從氣密封止材料94內部朝向外部被拉出金屬薄膜配線89,能輕易地從外部接近,所以能實現可電氣連接的各種構造。Since the cutting line can be divided along the dicing lines formed on the upper and lower glass substrates and divided in the X and Y directions in this manner, a plurality of liquid crystal displays can be produced from the large two-layer structure 70. Panel 80. In this case, particularly on at least one side surface of the liquid crystal display panel 80, on the lower glass substrate 92, the metal thin film wiring 89 is pulled out from the inside of the hermetic sealing material 94 toward the outside, and can be easily accessed from the outside. Therefore, various configurations that can be electrically connected can be realized.
本實施形態之處理多數片之從大型2層構造體個別分割成複數個顯示面板的情況下,因為能僅從單一側照射雷射射束而對2片玻璃基板加工並設置切割線,所以不需要大型玻璃之反轉搬運手段。此外,不會因雷射射束而對從顯示面板之內部構造至外部的電氣配線等之金屬膜等造成損害,能在一方的基板上從外部輕易地接近,且以△Y的寬度在上下的2片玻璃板上形成段差構造。在靠近下部玻璃基板之表面的切割線且面對上部玻璃板之表面上設置的金屬薄膜或電子零件方面,上部玻璃基板之端作為第2和第3切割線間的部分而被除去,所以變得容易從外部接近。另外,在下部玻璃基板上跨越封止部而從顯示面板內部導出之金屬薄膜配線係可行的。因此,變得能從封止部外部進行配線。In the case where the plurality of large-sized two-layer structures are individually divided into a plurality of display panels, the processing of the present embodiment can be performed by irradiating the laser beam from only one side and processing the two glass substrates to form a cutting line. Need to reverse the handling of large glass. Further, the metal film or the like of the electric wiring or the like from the internal structure of the display panel to the outside is not damaged by the laser beam, and can be easily accessed from the outside on one of the substrates, and is widened by the width of ΔY. The two glass plates form a step structure. The end of the upper glass substrate is removed as a portion between the second and third cutting lines in the vicinity of the cutting line on the surface of the lower glass substrate and facing the metal film or electronic component provided on the surface of the upper glass plate. It is easy to get close to the outside. Further, the metal thin film wiring which is led out from the inside of the display panel across the sealing portion on the lower glass substrate is feasible. Therefore, it becomes possible to perform wiring from the outside of the sealing portion.
本方法不僅是液晶顯示面板,也能適用於切斷電漿顯示面板等之其他平板顯示面板。另外,本方法能用於這些平板顯示面板的製程。This method is applicable not only to a liquid crystal display panel but also to other flat panel display panels such as a plasma display panel. In addition, the method can be applied to the process of these flat panel display panels.
構成構造體的基板雖為玻璃,但作為發明對象的材料 並非侷限於此。另外,基板雖為2層,但很顯然也能適用於具有3層以上之基板的情況。The substrate constituting the structure is glass, but the material to be invented Not limited to this. Further, although the substrate has two layers, it is apparent that it can be applied to a substrate having three or more layers.
第9圖係表示斜角(傾斜面)加工方法的實施形態。使用旋轉鏡51,使來自超短脈波雷射產生裝置1之超短脈波雷射射束2繞著旋轉軸55而以一定角度θ偏向並且旋轉52。旋轉的雷射射束53以及54之光路徑與光軸一致並且使用與旋轉鏡51一起旋轉的聚光透鏡3,聚光透鏡3之焦點會描繪圓軌跡。在台座等的加工物體搭載手段(未圖示)預先配置基板狀的被加工物體4。預先使該圓軌跡和加工物體搭載手段之搭載面成為平行等,藉以將基板狀的被加工物體4配置成相對於其正面的法線平行於旋轉軸55時,能夠在被加工物體4上對雷射光照射位置進行旋轉掃描,並進行圓形軌跡的照射。在此情況下,在被加工物體4上從旋轉軸55傾斜角度θ而進行傾斜加工。首先,將射束腰部對焦於從被加工物體4的反面56朝向內部而隔開空洞形成距離57(135 μm左右)左右處,並以圓形進行掃描,藉以在從法線偏移角度θ的方向上以圓狀形成細線上的空洞列。此外,使聚光透鏡3沿著光軸方向而在旋轉鏡51之方向上移動,藉以依序移動空洞形成距離58、59左右,每次移動時都形成空洞列並重複掃描,形成從被加工物體4之正面至反面的圓形之空洞壁面。爾後,藉由彎曲而分離,周圍被進行傾斜面之加工,切出成圓形。以此方式,本發明係不僅是在被加工物體的表面附近,亦可達到內部而重複空洞之形成,可施行從部分切斷到完全切斷的加工。Fig. 9 is a view showing an embodiment of a method of processing a bevel (inclined surface). Using the rotating mirror 51, the ultrashort pulse laser beam 2 from the ultrashort pulse laser generating device 1 is deflected and rotated 52 by a certain angle θ about the rotating shaft 55. The light paths of the rotating laser beams 53 and 54 coincide with the optical axis and use a collecting lens 3 that rotates with the rotating mirror 51, and the focus of the collecting lens 3 draws a circular trajectory. The substrate-shaped workpiece 4 is placed in advance on a workpiece mounting means (not shown) such as a pedestal. The circular trajectory and the mounting surface of the processed object mounting means are parallel, and the substrate-shaped workpiece 4 is placed in parallel with the rotation axis 55 with respect to the normal line on the front surface thereof, so that it can be placed on the workpiece 4 The laser light irradiation position is rotated and scanned, and a circular trajectory is irradiated. In this case, the workpiece 4 is inclined by the angle θ from the rotating shaft 55. First, the beam waist is focused on the cavity forming distance 57 (about 135 μm) from the opposite surface 56 of the workpiece 4 toward the inside, and is scanned in a circle, thereby shifting the angle θ from the normal. In the direction of the circle, a hollow column on the thin line is formed in a circular shape. In addition, the condensing lens 3 is moved in the direction of the rotating mirror 51 along the optical axis direction, thereby sequentially moving the cavity to form a distance of about 58, 59, and each time the movement is formed, a hole column is formed and the scanning is repeated to form a slave. The circular hollow wall surface from the front to the back of the object 4. Thereafter, it is separated by bending, and the periphery is processed by the inclined surface, and cut into a circular shape. In this way, the present invention is not only in the vicinity of the surface of the object to be processed, but also in the interior, and the formation of the cavity is repeated, and the process from the partial cutting to the complete cutting can be performed.
在以上的雷射加工中,脈波能量較佳為1mJ以下,進一步較佳為10 μJ以下。在10 μJ以下的情況下,能獲得俐落且平滑的切斷面,很少發生裂紋且破壞強度高。當裂紋等存在時,玻璃等被加工物體之強度變弱,所以會有不佳的狀況。在脈波能量大的情況下,欲對正面附近進行加工時,由於脈波尖端部在正面附近造成的自由電子電漿,脈波中心部至後端部會被反射或散亂、吸收,所以有時候很難在玻璃內部形成空洞。在脈波能量小的情況下,因為在正面附近發生的自由電子電漿之密度變低,變得不會大幅阻礙傳送脈波,所以在玻璃內部能輕易地形成空洞通道。In the above laser processing, the pulse wave energy is preferably 1 mJ or less, and more preferably 10 μJ or less. In the case of 10 μJ or less, a slumped and smooth cut surface can be obtained, and cracks rarely occur and the breaking strength is high. When cracks or the like are present, the strength of the object to be processed such as glass is weakened, so that there is a poor condition. When the pulse wave energy is large, when the vicinity of the front surface is to be processed, the free electron plasma caused by the tip end portion of the pulse wave is reflected or scattered and absorbed at the center portion to the rear end portion of the pulse wave. Sometimes it is difficult to form a void inside the glass. When the pulse wave energy is small, since the density of the free electron plasma generated in the vicinity of the front surface becomes low, the transmission pulse wave is not greatly hindered, so that a cavity passage can be easily formed inside the glass.
另外,超短脈波的雷射就是脈波寬度100ps以內的雷射,另外,較佳為脈波寬度為500fs至10ps,進一步,在2ps左右的情況下為最佳。這是因為連續地形成破斷面以後,割斷玻璃基板時所必需的應力降低,割斷面的品質良好。Further, the ultrashort pulse laser is a laser having a pulse width of 100 ps or less, and preferably has a pulse width of 500 fs to 10 ps, and further preferably at about 2 ps. This is because the stress required for cutting the glass substrate is lowered after the fracture surface is continuously formed, and the quality of the fracture surface is good.
另外,以玻璃基板作為被加工物體的情況下,較佳為脈波寬度150飛秒、輸出能量1 μJ以上。Further, when a glass substrate is used as the object to be processed, the pulse wave width is preferably 150 femtoseconds and the output energy is 1 μJ or more.
如同以上所示,本發明係提供一種新的加工方法,能使用超短脈波之聚光射束的焦點深度小之‘射束腰部,採用形成於被加工物體內部形成的自集束作用,而使用加工之實質焦點深度的增大。此方法未見於以往的加工方法,是藉由雷射射束和加工物的相互作用而初次實現的精密加工方法。As shown above, the present invention provides a novel processing method capable of using a beam having a small depth of focus of a concentrated beam of ultrashort pulse waves, using a self-bundling formed in the inside of the object to be processed, The depth of use of the actual focus of the processing is increased. This method is not found in the conventional processing method and is a precision machining method that is first realized by the interaction of the laser beam and the workpiece.
雷射媒體是鈦藍寶石結晶(中心波長780nm),脈波寬度150飛秒、輸出能量1 μJ以上。另外,加工對象是屬於玻璃基板的Corning Eagle 2000,厚度700 μm。在各實施例中無與此相異之記載的情況下,這些在所有的實施例中為共通。The laser medium is a titanium sapphire crystal (center wavelength 780 nm), a pulse width of 150 femtoseconds, and an output energy of 1 μJ or more. In addition, the object to be processed is Corning Eagle 2000 which is a glass substrate and has a thickness of 700 μm. In the case where there is no description different from the examples in the respective embodiments, these are common to all the embodiments.
本實施例係以第1圖所示之構成,將以雷射照射被加工物體時的聚光位置從正面移向內部時,觀察於被加工物體產生的變化,並證實本加工方法之原理的實驗例。In the first embodiment, when the condensing position when the object is irradiated with laser light is moved from the front side to the inside, the change in the object to be processed is observed, and the principle of the processing method is confirmed. Experimental example.
第10圖以及第11圖係表示觀察在被加工物體內產生之變化的截面圖之顯微鏡照片。第10圖係表示作為被加工物體的基板之正面45,第11圖係表示反面44附近。對於第1圖的構成,使用透鏡之入射射束直徑為6mm,聚光透鏡3的焦點距離f為約3.1mm之已像差補正的非球面透鏡。在將雷射射束之橫向模式作為高斯分佈的射束時,則算出聚光點之射束直徑為大約1 μm,包含射束腰部之能量的90%之範圍的焦點深度為1 μm以下。如同這般,將具有小焦點深度值的超短脈波雷射射束照射於被加工物體4的情況下,以在正面45置有射束腰部之位置的方式而集束且照射射束的情況下,將第10圖中從正面45於內部以深度23所示之淺部分21進行除去加工,此外,於內部移動射束腰部時,表面除去量會減少,此外,於內部移動射束腰部的位置時,在被加工物體4的內部發生光學扭曲的範圍24、25等會根據置有射束腰部之深度方向的位置,而發生在其周邊部分。將射束腰部置於內部,減少表面的除去加 工,取而代之的是發生內部光學的扭曲,出現範圍24、25。Fig. 10 and Fig. 11 are micrographs showing a cross-sectional view of the change occurring in the object to be processed. Fig. 10 shows the front surface 45 of the substrate as the object to be processed, and Fig. 11 shows the vicinity of the reverse surface 44. In the configuration of Fig. 1, an aspherical lens having an incident beam diameter of 6 mm and a focal length f of the condenser lens 3 of about 3.1 mm is used. When the transverse mode of the laser beam is used as a beam of Gaussian distribution, the beam diameter of the condensed spot is calculated to be about 1 μm, and the depth of focus including the range of 90% of the energy of the beam waist is 1 μm or less. . As such, in the case where the ultrashort pulse laser beam having the small focus depth value is irradiated onto the object 4 to be processed, the beam is bundled and irradiated in such a manner that the front surface 45 is placed at the position of the beam waist. In the case of Fig. 10, the shallow portion 21 indicated by the depth 23 from the front surface 45 is removed from the front surface 45, and when the beam waist is moved inside, the amount of surface removal is reduced, and the beam is moved inside. At the position of the waist, the ranges 24, 25, etc., in which the optical distortion occurs inside the workpiece 4 occur in the peripheral portion depending on the position in the depth direction in which the beam waist is placed. Put the beam waist inside, reduce the removal of the surface Instead, the internal optical distortion occurs, appearing in the range of 24, 25.
第11圖係進一步在基板內部使射束腰部移動時的截面觀察照片。在正面45上無變化之條件下觀察到在射束腰部部分產生光學變化的部位31、32。此外,觀察隨著接近被加工物體之反面44,從內部至反面在數100 μm的範圍中引起光學變化的部位33。此外,射束腰部從反面44接近大約135 μm時,就以細線狀而從內部涵蓋至反面而直線地形成空洞34。此外,使雷射射束腰部對焦於反面44時,僅對反面附近進行除去加工。從這種加工結果中,即使雷射射束之焦點深度37如同前述為1 μm左右,但朝著射束的行進方向而以空洞形成距離(135 μm左右)而形成作為射束腰部之直徑的細線狀空洞34,未發現自集束作用的情況下,相較於僅在射束的焦點深度(1 μm左右)之範圍中進行加工,本方法能涵蓋2位數左右長的範圍而進行細線狀的空洞加工。Fig. 11 is a cross-sectional observation photograph when the beam waist is further moved inside the substrate. The portions 31, 32 where optical changes occur in the waist portion of the beam are observed without change on the front surface 45. Further, a portion 33 which causes an optical change in the range of several hundred μm from the inside to the reverse side as it approaches the opposite surface 44 of the object to be processed is observed. Further, when the beam waist is close to about 135 μm from the back surface 44, the cavity 34 is formed linearly from the inside to the reverse side in a thin line shape. Further, when the laser beam waist is focused on the reverse side 44, only the vicinity of the reverse side is removed. From such a processing result, even if the focal depth 37 of the laser beam is about 1 μm as described above, a hole is formed as a diameter of the beam waist by forming a distance (about 135 μm) in the direction of travel of the beam. The thin-lined cavity 34, which is not found to be self-bundling, can be processed in a range of only about 2 digits of the focal depth (1 μm) of the beam. Shaped hollow processing.
本實施例係在反面附近形成空洞通道並掃描雷射光,以形成空洞通道的切斷面的情形。This embodiment is a case where a cavity channel is formed in the vicinity of the reverse side and the laser light is scanned to form a cut surface of the cavity channel.
在形成由自集束作用所造成之細線狀空洞的情況下,如第12圖內的圖所示,有時會在反面聚集形成漏斗形的部分43。使該漏斗形的部分43互相具有鄰接部的重疊,細線狀空洞係個別形成於與通道8相同之處,沿著被加工物體的反面44,相對地以超短雷射脈波進行掃描,治著掃描方向來形成既定加工深度之並列於包絡線46的多數個細線 狀空洞。第12圖係配合以此方式形成之細線狀空洞的切斷面之顯微鏡照片而進行表示。在此例中,以3mm/s的掃描速度來進行雷射脈波的掃描以後,沿著掃描線折彎並分割,藉以觀察截面。在此圖中係表示,在被加工物體之厚度41的加工中,涵蓋從反面44達深度42之範圍的包絡線46,而形成多數個細線狀的空洞通道,以其為起點而分割之被加工物體的加工截面。第13圖係拍攝空洞61之截面而‘得的掃描型顯微鏡照片,另外,第14圖係特別擴大反面附近之掃描型顯微鏡照片。表示形成有空洞61處的表面之隆起比周圍還要高且機械強度弱之隆起構造71。In the case of forming a fine-line void caused by the self-bundling action, as shown in the graph in Fig. 12, a funnel-shaped portion 43 may be formed on the reverse side. The funnel-shaped portions 43 are overlapped with each other by the abutting portions, and the thin-line-shaped voids are formed separately at the same place as the channels 8, and are scanned along the reverse surface 44 of the object to be processed by ultrashort laser pulses. Scanning direction to form a plurality of thin lines juxtaposed on the envelope 46 of a given processing depth Empty. Fig. 12 is a view showing a micrograph of the cut surface of the fine-line void formed in this manner. In this example, after the scanning of the laser pulse wave is performed at a scanning speed of 3 mm/s, the scanning line is bent and divided to observe the cross section. In the figure, it is shown that in the processing of the thickness 41 of the object to be processed, the envelope 46 from the reverse surface 44 to the depth 42 is covered, and a plurality of thin-line hollow passages are formed, which are divided by the starting point. The processing section of the machined object. Fig. 13 is a scanning micrograph taken of the cross section of the cavity 61, and Fig. 14 is a scanning microscope photograph in the vicinity of the reverse side. The ridge structure 71 in which the surface of the cavity 61 is formed to be higher than the surrounding and has a weak mechanical strength is shown.
在如第3圖所示之構成中,改變射束腰部的高度,進行複數次的掃描,在反面附近進行加工。第15圖表示掃描次數4次、脈波能量10 μJ、脈波寬度2ps時的截面。縮小脈波能量,使脈波寬度最佳化,藉以在反面附近形成高品質的加工區域36。In the configuration shown in Fig. 3, the height of the beam waist is changed, scanning is performed plural times, and processing is performed in the vicinity of the reverse side. Fig. 15 shows a cross section of the number of times of scanning 4 times, the pulse wave energy of 10 μJ, and the pulse width of 2 ps. The pulse wave energy is reduced to optimize the pulse width, thereby forming a high quality processing region 36 near the reverse side.
在此實施例中,亦於如第3圖所示之構成,改變射束腰部的高度,進行複數次的掃描而進行加工。在此實施例中,以在玻璃基板之正面附近設定加工區域的方式來形成射束腰部。第16圖係表示掃描次數10次脈波能量1 μJ、脈波寬度2ps之情況下的截面。藉由使脈波能量以及脈波寬度最佳化,能獲得涵蓋正面的良好加工區域36。Also in this embodiment, as shown in Fig. 3, the height of the beam waist is changed, and scanning is performed for a plurality of times. In this embodiment, the beam waist is formed in such a manner that the processing region is set in the vicinity of the front surface of the glass substrate. Fig. 16 is a cross section showing the case where the number of scanning times is 10 μ pulse energy and the pulse width is 2 ps. By optimizing the pulse energy and the pulse width, a well-processed region 36 covering the front side can be obtained.
本實施例係將被加工物體做成玻璃基板2片之積層構成的情況。作為第4圖所示的構成,使雷射的聚光位置從玻璃製之上部基板81的正面變化至涵蓋反面而進行加工。於第17圖表示2片玻璃基板之加工後的顯微鏡照片。不僅是上部玻璃81,還有置於其背面側的下部玻璃82也被加工。上部玻璃81涉及最大150 μm,下部玻璃82涉及最大250 μm而進行加工。如同前述,置於下部的基板會根據雷射傳搬方向而進行長時間的加工。In the present embodiment, the object to be processed is formed by laminating two sheets of a glass substrate. As a configuration shown in Fig. 4, the condensing position of the laser is changed from the front surface of the glass upper substrate 81 to the reverse surface to be processed. Fig. 17 shows a micrograph of the processed glass substrate. Not only the upper glass 81 but also the lower glass 82 placed on the back side thereof is also processed. The upper glass 81 is involved in a maximum of 150 μm and the lower glass 82 is processed up to a maximum of 250 μm. As described above, the substrate placed in the lower portion is processed for a long time in accordance with the direction in which the laser is transmitted.
以上,已說明本發明的實施例。很顯然只要不脫離申請專利範圍所記載之發明技術思想,就能對這些施行變更。Hereinabove, the embodiments of the present invention have been described. It is obvious that changes can be made to these without departing from the inventive concept described in the claims.
作為本發明的活用例,在用於半導體裝置、液晶等之顯示裝置的被加工物體之加工中,對於從表面進行矽晶圓、薄膜電晶體和顯示裝置的基板分割、高耐壓功率半導體基板加工,此外,多層構造電子元件之層內部的除去加工之微細、且熱影響少的加工而言為有效。在高積體電路製造中,由於加工寬度的微小化、加工除去物的減少等,製品良率提升,因而能減低電子零件的製造成本。此外,在石英、藍寶石等之半導體裝置的基板之孔穴加工等也能獲得有效性。在設有多數個微細孔穴之過濾部的加工方面也有效。此外,本發明係可利用於製造使用液晶顯示面板、電漿顯示面板等之多層玻璃構造的電子裝置。In the processing of an object to be processed for a display device such as a semiconductor device or a liquid crystal, the substrate is divided into a substrate, a thin film transistor, and a display device from a surface, and a high withstand voltage power semiconductor substrate is used as an active example of the present invention. In addition, it is effective in the processing in which the inside of the layer of the multilayered electronic component is finely removed and the heat influence is small. In the production of a high-integration circuit, the product yield is improved due to the miniaturization of the processing width and the reduction of the processed material, so that the manufacturing cost of the electronic component can be reduced. Further, it is also effective in hole processing of a substrate of a semiconductor device such as quartz or sapphire. It is also effective in the processing of a filter portion in which a plurality of fine holes are provided. Further, the present invention can be utilized in the manufacture of an electronic device using a multilayer glass structure such as a liquid crystal display panel or a plasma display panel.
1‧‧‧超短脈波雷射產生裝置1‧‧‧Ultra-short pulse laser generating device
2‧‧‧雷射射束2‧‧‧Laser beam
3‧‧‧聚光透鏡3‧‧‧ Concentrating lens
4‧‧‧被加工物體4‧‧‧Processed objects
5‧‧‧集束雷射射束5‧‧‧Bundle laser beam
6‧‧‧射束腰部6‧‧‧ beam waist
7‧‧‧厚度7‧‧‧ thickness
8‧‧‧通道8‧‧‧ channel
10‧‧‧射束10‧‧‧beam
11‧‧‧發散性射束11‧‧‧Divergent beam
13、14‧‧‧距離13, 14‧‧‧ distance
15‧‧‧超短脈波15‧‧‧ Ultrashort pulse
16‧‧‧行進方向16‧‧‧Travel directions
21‧‧‧淺部分21‧‧‧ shallow part
23‧‧‧深度23‧‧‧depth
24、25‧‧‧範圍24, 25‧‧‧Scope
31~33‧‧‧引發光學變化的部位31~33‧‧‧The part that causes optical changes
34‧‧‧細線狀空洞34‧‧‧ Thin wire cavity
35‧‧‧加工線35‧‧‧Processing line
36‧‧‧加工區域36‧‧‧Processing area
37‧‧‧焦點深度37‧‧‧Depth of focus
41‧‧‧厚度41‧‧‧ thickness
42‧‧‧深度42‧‧‧depth
43‧‧‧漏斗形的部分43‧‧‧Funnel-shaped part
44‧‧‧反面44‧‧‧n
45‧‧‧正面45‧‧‧ positive
46‧‧‧包絡線46‧‧‧Envelope
47‧‧‧掃描方向47‧‧‧Scanning direction
48‧‧‧掃描線48‧‧‧ scan line
49‧‧‧彎曲應力49‧‧‧Bending stress
50‧‧‧雷射射束50‧‧‧Laser beam
51‧‧‧旋轉鏡51‧‧‧Rotating mirror
52‧‧‧旋轉52‧‧‧Rotate
53、54‧‧‧雷射射束53, 54‧‧ ‧ laser beam
55‧‧‧旋轉軸55‧‧‧Rotary axis
56‧‧‧反面56‧‧‧n
57~59‧‧‧距離57~59‧‧‧distance
61~64‧‧‧空洞61~64‧‧‧ hollow
65、66‧‧‧截面65, 66‧‧‧ section
67、68‧‧‧側面67, 68‧‧‧ side
70‧‧‧構造體70‧‧‧structure
71‧‧‧隆起構造71‧‧‧Uplift structure
77‧‧‧距離77‧‧‧distance
81‧‧‧上部基板81‧‧‧Upper substrate
82‧‧‧下部基板82‧‧‧lower substrate
83‧‧‧空隙83‧‧‧ gap
86‧‧‧第3切割線86‧‧‧3rd cutting line
87‧‧‧第2切割線87‧‧‧2nd cutting line
88‧‧‧第1切割線88‧‧‧1st cutting line
89‧‧‧金屬薄膜配線89‧‧‧Metal film wiring
90‧‧‧液晶顯示面板90‧‧‧LCD panel
91‧‧‧上部玻璃基板91‧‧‧Upper glass substrate
92‧‧‧下部玻璃基板92‧‧‧Lower glass substrate
93‧‧‧液晶93‧‧‧LCD
94‧‧‧氣密封止材料94‧‧‧Air seal material
95、96‧‧‧零件95, 96‧‧‧ parts
97、98‧‧‧切斷97, 98‧‧‧ cut off
99‧‧‧保護用塗佈層99‧‧‧Protective coating
第1圖係說明採用與本發明相關之克爾效應所引起的 自集束作用的被加工物體之加工方法的構成圖。Figure 1 illustrates the use of the Kerr effect associated with the present invention. A composition diagram of a processing method of a workpiece to be processed by focusing.
第2(a)、(b)圖係使雷射掃描,並進行基板加工的構成圖。The second (a) and (b) drawings are diagrams for scanning the laser and performing substrate processing.
第3(a)~(c)圖係掃描被加工物體而加工以後,變更雷射光聚光點之聚光位置,再次進行加工的方法之表示圖。The third (a) to (c) diagrams are diagrams showing a method of changing the condensing position of the laser light condensing point and scanning the processing object after scanning the object to be processed.
第4圖係於由2片基板組成之多層構造進行加工的構成圖。Fig. 4 is a view showing a configuration in which a multilayer structure composed of two substrates is processed.
第5(a)、(b)圖係在其他位置切斷液晶面板構造以及2片玻璃基板時的說明圖。The fifth (a) and (b) drawings are explanatory views when the liquid crystal panel structure and the two glass substrates are cut at other positions.
第6圖係用於說明由2片基板組成之構造體的分割方法之模式截面圖。Fig. 6 is a schematic cross-sectional view for explaining a method of dividing a structure composed of two substrates.
第7圖係表示由2片基板組成之玻璃構造體的概觀形狀之1例。Fig. 7 is a view showing an example of an approximate shape of a glass structure composed of two substrates.
第8(a)、(b)圖係由大型玻璃構造體分割成個別的液晶顯示面板時的說明圖。The eighth (a) and (b) drawings are explanatory views when the large-sized glass structure is divided into individual liquid crystal display panels.
第9圖係表示將本發明之加工方法應用於傾斜面加工之實施形態的圖。Fig. 9 is a view showing an embodiment in which the processing method of the present invention is applied to the inclined surface processing.
第10圖係表示第1實施例之結果的圖,是被加工物體正面附近的顯微鏡照片。Fig. 10 is a view showing the result of the first embodiment, and is a micrograph of the vicinity of the front surface of the object to be processed.
第11圖係表示第1實施例之結果的圖,是被加工物體反面附近的顯微鏡照片。Fig. 11 is a view showing the result of the first embodiment, and is a micrograph of the vicinity of the reverse side of the object to be processed.
第12圖係表示第2實施例之結果的圖,是空洞通道之切斷面的說明圖及其顯微鏡照片。Fig. 12 is a view showing the result of the second embodiment, and is an explanatory view of a cut surface of the hollow passage and a micrograph thereof.
第13圖係表示第2實施例之結果的圖,是拍攝空洞61之截面的掃描型顯微鏡照片。Fig. 13 is a view showing the result of the second embodiment, and is a scanning type microscope photograph of a cross section of the photographing cavity 61.
第14圖係特別放大在第13圖中,基板反面附近之掃描型顯微鏡照片。Fig. 14 is a magnified photograph of a scanning microscope in the vicinity of the reverse side of the substrate in Fig. 13.
第15圖係表示第3實施例之結果的圖,係切斷面的顯微鏡照片。Fig. 15 is a view showing the results of the third embodiment, and is a micrograph of the cut surface.
第16圖係表示第4實施例之結果的圖,係切斷面的顯微鏡照片。Fig. 16 is a view showing the results of the fourth embodiment, and is a micrograph of a cut surface.
第17圖係表示第5實施例之結果的圖,表示2片基板加工以後的顯微鏡照片。Fig. 17 is a view showing the results of the fifth embodiment, showing a micrograph after processing of two substrates.
1‧‧‧超短脈波雷射產生裝置1‧‧‧Ultra-short pulse laser generating device
2‧‧‧雷射射束2‧‧‧Laser beam
3‧‧‧聚光透鏡3‧‧‧ Concentrating lens
4‧‧‧被加工物體4‧‧‧Processed objects
5‧‧‧集束雷射射束5‧‧‧Bundle laser beam
6‧‧‧射束腰部6‧‧‧ beam waist
7‧‧‧厚度7‧‧‧ thickness
8‧‧‧通道8‧‧‧ channel
10‧‧‧射束10‧‧‧beam
11‧‧‧發散性射束11‧‧‧Divergent beam
13、14‧‧‧距離13, 14‧‧‧ distance
15‧‧‧超短脈波15‧‧‧ Ultrashort pulse
16‧‧‧行進方向16‧‧‧Travel directions
44‧‧‧反面44‧‧‧n
45‧‧‧正面45‧‧‧ positive
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CN101663125B (en) | 2012-11-28 |
TW200848190A (en) | 2008-12-16 |
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KR101333518B1 (en) | 2013-11-28 |
WO2008126742A1 (en) | 2008-10-23 |
KR20100015948A (en) | 2010-02-12 |
JP5784273B2 (en) | 2015-09-24 |
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CN101663125A (en) | 2010-03-03 |
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