TW201736029A - Mirror cutting method without processing sectional ends of a mirror - Google Patents

Mirror cutting method without processing sectional ends of a mirror Download PDF

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TW201736029A
TW201736029A TW106109421A TW106109421A TW201736029A TW 201736029 A TW201736029 A TW 201736029A TW 106109421 A TW106109421 A TW 106109421A TW 106109421 A TW106109421 A TW 106109421A TW 201736029 A TW201736029 A TW 201736029A
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laser
processing
light
mirror
cutting
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TW106109421A
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TWI653113B (en
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有澤真
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漢登科技股份有限公司
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Abstract

The present invention set a time difference for plural tiny inline laser beam focuses in a depthwise direction, such that non-permeable denaturations occur sequentially along the depthwise direction to seek light absorption, so as to increase a crack length by the aforementioned interactions. The focal position is moved in high speed along the depthwise direction of the cutting, and a sectional cut end of a mirror is not processed in order to increase the cutting depth and obtain a mirror section and a high anti-breaking strength for industrial laser cutting. The invention has the effects of preventing small cracks formed on sectional ends of a brittle transparent object, improving the anti-breaking strength of the product weakened by the concentrated stress, and avoiding dirty marks remained on the cut surface.

Description

剖面端部不加工鏡面切斷法 End section of the section without mirror cut

本發明係一種剖面端部不加工鏡面切斷法,尤指一種在透明脆性材料之切斷中,不對剖面端部直接加工,以切斷後剖面形成鏡面狀態,實現高破壞強度為目的之精密切斷加工者。 The invention relates to a cross-sectional end non-machining mirror cutting method, in particular to a precision cutting for the purpose of achieving high-destructive strength in the cutting of the transparent brittle material without directly processing the end portion of the section, forming a mirror state after cutting the section. Broken processor.

雖然雷射有效扮演著將玻璃等透明脆性材料切斷成自由形狀之角色,然而,因為切斷後發生微細裂紋,所以有容易破損,需要實施後處理製程之缺點。過去習知之鹼玻璃等,因為在碳酸氣體雷射中具有吸收帶,所以可藉由雷射光對玻璃之吸收及溫度上昇而發生的熱應力進行龜裂斷裂,而將剖面加工成鏡面。但是此種方法無法對強化玻璃、無鹼玻璃、藍寶石等透明體實施加工。因而,係採用將原本對透明體不吸收之脈衝雷射進行強烈聚光,藉由使透明玻璃之光學特性變性引起熱吸收,使物質溫度急遽上昇,而使物質蒸發,藉由進行熱破壞等實施加工的方法。但是,由於此種方法僅在小焦點部之高強度聚光部分產生變性,因此切斷時係採取對玻璃剖面之邊緣部分進行加工,或是藉由對內部伴隨大加工痕之照射而容易切斷的加工法。因而,切斷後會在剖面邊緣部分殘留微細裂紋,成為遇應力集中而斷裂的原因。此外,即使表面及背面不直接加工,來自內部之自然龜裂進行不一,加工後仍然成為微細裂紋之發生源。 Although the laser effectively functions to cut a transparent brittle material such as glass into a free shape, since fine cracks occur after cutting, it is easily broken and requires a post-treatment process. In the conventional alkali glass or the like, since there is an absorption band in the carbon dioxide gas laser, the thermal stress generated by the absorption of the glass by the laser light and the temperature rise can be cracked and fractured, and the cross section can be processed into a mirror surface. However, this method cannot process transparent bodies such as tempered glass, alkali-free glass, and sapphire. Therefore, the pulsed laser which is not absorbed by the transparent body is strongly concentrated, and the heat absorption of the transparent glass is caused to cause heat absorption, so that the temperature of the substance rises sharply, and the substance is evaporated, and thermal destruction is performed. The method of processing. However, since this method is only denatured in the high-intensity condensing portion of the small focus portion, the cutting is performed by processing the edge portion of the glass section or by cutting the inside with a large processing mark. Broken processing method. Therefore, after the cutting, fine cracks remain in the edge portion of the cross section, which causes the stress to concentrate and break. In addition, even if the surface and the back surface are not directly processed, natural cracks from the inside are different, and the source of fine cracks remains after processing.

使通過透明玻璃之雷射光超過某種強度聚光時,因非線性光學效應使玻璃變性而產生光之吸收,進一步增強光時熱 吸收更為活絡,而使物質溫度急速上昇。結果,材料因強烈的熱應力作用而斷裂。更加提高強度時,因高電場導致污損破壞。即使是比較弱之光,為了容易切斷,將表面或背面同時加工切斷時,剖面邊緣部仍會發生微細裂紋而強度降低。為了避免此種情況,需要僅將剖面內部藉由熱應力以不明顯之加工痕自然斷裂,並利用鏡面將平坦之裂紋誘導於表面及背面而切斷,避免人為性端面裂紋。因而,需要使雷射發生熱應力斷裂部僅可在表面、背面方向細長形成。將其以1條雷射光束實現情況下,在透明體內部聚光時,需要以與符合透鏡系統之焦點深度匹配的長度使熱應力斷裂發生。增長破壞部分時,係以長焦點距離之透鏡聚光,不過,因為此種情況下聚光點直徑變大,所以需要之雷射輸出亦非常大,因而加工痕也變大,從該加工痕引起微細裂紋之發生。 When the laser light passing through the transparent glass is concentrated beyond a certain intensity, the glass is denatured by the nonlinear optical effect to generate light absorption, further enhancing the heat of the light. The absorption is more active, and the temperature of the substance rises sharply. As a result, the material breaks due to strong thermal stress. When the strength is further increased, the fouling is destroyed by the high electric field. Even in the case of relatively weak light, in order to facilitate cutting, when the surface or the back surface is simultaneously cut and cut, fine cracks occur at the edge portion of the cross section, and the strength is lowered. In order to avoid this, it is necessary to cut only the inside of the profile by thermal stress with inconspicuous processing marks, and use a mirror surface to induce flat cracks on the surface and the back surface to avoid artificial end face cracks. Therefore, it is necessary to cause the thermal stress cracking portion of the laser to be formed elongated only in the front and back directions. In the case where it is realized by one laser beam, when concentrating inside the transparent body, it is necessary to cause thermal stress cracking to occur in a length matching the depth of focus of the lens system. When the damage is increased, the lens is concentrated by a long focal length. However, since the diameter of the spot is increased in this case, the required laser output is also very large, and the processing mark is also enlarged. Causes the occurrence of micro cracks.

如圖1所示,觀察對透明體剖面照射之雷射光束的形態差異時,照射於表面或背面情況下,在剖面端部發生裂紋,因此應力作用時,就會發生微細裂紋而造成破壞。照射中心部時,切斷端面不產生裂紋者時,需要長焦點距離之光學系統與高輸出雷射,結果發生大的加工痕殘留,從此種加工痕加工後會發生裂紋而造成斷裂。考慮透明體因變性之光的吸收,為了連接小焦點從深處向淺處依序進行加工,將透明體以一定深度加工,其製程結束後,將深度稍變淺再加工,如此反覆加工,在深度方向發生深之加工痕而切斷的方法。該方法因為係隔開時間進行深度方向之加工,所以在各個深度之加工痕喪失同時相互作用,而僅單純地堆積微小加工痕,無法引起鏡面狀之自然龜裂。 As shown in Fig. 1, when the difference in the morphology of the laser beam irradiated to the cross section of the transparent body is observed, when the surface or the back surface is irradiated, cracks occur at the end portions of the cross section, so that fine cracks are generated and damage is caused by the stress. When the center portion is irradiated, when the cut end face does not cause cracks, an optical system having a long focal length and a high-output laser are required, and as a result, a large processing mark remains, and cracks are generated and the crack is generated after the processing of the processed mark. Considering the absorption of the light due to denaturation of the transparent body, in order to connect the small focus from the deep to the shallow, the transparent body is processed at a certain depth, and after the process is finished, the depth is slightly shallowed and then processed, so that the processing is repeated. A method in which deep processing marks are formed in the depth direction and cut. Since this method performs the processing in the depth direction with a time interval, the processing marks at the respective depths are lost and interacted at the same time, and only the minute processing marks are simply deposited, and the mirror-like natural crack cannot be caused.

利用透明體特性以及光線會傳播至深部特性之雷射細絲的方法,並非僅透鏡單純聚光,而係藉由利用透明材料本身發生的非線性效應,在細絲上形成光線以進行加工。因為該方法 取決於透明體材料之光學特性,所以細絲之形成取決於透明體材料的性質。此外,為了從深度淺之部分向深的部分形成,因為有從近端消耗之光的透過與吸收加熱的差異,所以有發生細絲之部分並非依然有助於均勻加工,且為了生成細絲需要複雜之光學系統與高輸出的雷射等方面之困難。 The method of utilizing the characteristics of the transparent body and the propagation of the light to the deep-filamented laser filaments is not only the lens concentrating, but the light is formed on the filament by the nonlinear effect generated by the transparent material itself. Because of the method Depending on the optical properties of the transparent body material, the formation of the filaments depends on the nature of the transparent body material. In addition, in order to form a portion from a shallow portion to a deep portion, since there is a difference between the transmission of light consumed from the near end and the absorption heating, the portion where the filament is generated does not contribute to uniform processing, and is formed into a filament. The difficulty of complex optical systems and high output lasers is required.

透明體藉由高強度雷射光使物性引起變化,藉此透明體吸收光,因而焦點部分之溫度急速上昇並產生破壞反應,因為表面及背面與內部比較係以低強度加工,所以用強雷射光加工其附近時,因為表面及背面先反應導致在其附近的內部無法加工。因而,為了盡可能地擴大加工剖面深度,須在內部較寬的範圍形成加工部,如此又需要對各照射點實施適當的輸出調整。 The transparent body changes the physical properties by high-intensity laser light, whereby the transparent body absorbs light, so that the temperature of the focal portion rises rapidly and a destructive reaction occurs, because the surface and the back surface are compared with the inside to be processed with low strength, so strong laser light is used. When the vicinity is processed, the surface and the back surface are first reacted, so that the inside of the vicinity cannot be processed. Therefore, in order to enlarge the depth of the processing section as much as possible, it is necessary to form the processed portion in a wide range inside, and thus it is necessary to perform appropriate output adjustment for each irradiation point.

換言之,使用雷射控制剖面聚光位置而進行加工時,對雷射波長透過之透明體材料的加工,除了雷射光的聚光焦點位置之外,還需要藉由依材料剖面深度調整強度,實施表面、背面或內部加工。藉由如此操作,可避免因剖面邊緣因切斷發生微細裂紋而使強度降低、加工時因產生之塵埃飛散妨礙精密加工、造成貼在加工品下面之膠帶損傷、加工品剖面加工痕顯著變大等,導致表面凹凸明顯。掃瞄一個雷射光時,改變深度調整輸出固然容易,但是在使2個以上脈衝相互干擾,且同時進行照射時則必須考量前述因素。 In other words, when processing is performed using the laser control section concentrating position, in addition to the concentrating focus position of the laser light, in addition to the concentrating focus position of the laser light, it is necessary to adjust the intensity according to the depth of the material profile to implement the surface. , back or internal processing. By doing so, it is possible to prevent the occurrence of fine cracks due to the cutting of the edge of the section, the scattering of dust due to the processing, the precision of the processing, the damage of the tape attached to the underside of the processed product, and the significant increase in the profile of the processed product. Etc., resulting in obvious surface irregularities. When scanning a laser beam, it is easy to change the depth adjustment output, but the above factors must be considered when two or more pulses are interfered with each other and simultaneously irradiated.

如上述,因為透明體之加工僅在光強度高之焦點部分進行加工,所以需要在發生光強度吸收之剖面內部藉由控制形成良好之切斷表面形態。當焦點較短且產生較小的焦點時,局部溫度升高可進行較整齊之加工,不過因為加工區域狹窄,所以無法進行達到斷裂之加工。包含表面及背面之加工也會有發生塵埃及保持膠帶破損等問題。形成可斷裂之大加工痕時,係使用長焦 點之光學系統,不過此時因為焦點光點大,若要讓焦點光點變大,需要較大的雷射能量以形成破壞。而且,導致破壞之剖面汙損,裂紋也大。因此,最理想的方式就是採用雷射照射法,藉以在切斷方向產生平滑的剖面。但是,細絲化產生必須具備能穩定產生細絲的條件,以及隨著較長的細絲,以致細絲產生能力和吸收損耗之間不易取得平衡。因而,需要一種可在分散之焦點中進行最佳照射的系統。 As described above, since the processing of the transparent body is performed only at the focal portion where the light intensity is high, it is necessary to form a good cut surface morphology by controlling the inside of the cross section where the light intensity is absorbed. When the focus is short and a small focus is generated, the local temperature rise can be processed more neatly, but since the processing area is narrow, the processing to achieve the fracture cannot be performed. There are also problems with the processing of the surface and the back surface, which may cause damage to the tape. When forming a large breakable work mark, the telephoto is used. The optical system of the point, but because the focal spot is large at this time, if the focal spot is made larger, a large laser energy is required to cause damage. Moreover, the profile causing the damage is fouled and the crack is large. Therefore, the most ideal way is to use a laser irradiation method to produce a smooth profile in the cutting direction. However, the fibrillation production must have conditions for stably producing filaments, and with long filaments, it is difficult to balance the filament generating ability and the absorption loss. Thus, there is a need for a system that can optimally illuminate in a dispersed focus.

先前技術文獻 Prior technical literature

專利文獻 Patent literature

[專利文獻1]特開2008-264843號公報 [Patent Document 1] JP-A-2008-264843

[專利文獻2]特開2015-110248號公報 [Patent Document 2] JP-A-2015-110248

[專利文獻3]特開2013-022627號公報 [Patent Document 3] JP-A-2013-022627

[專利文獻4]特開2011-159827號公報 [Patent Document 4] JP-A-2011-159827

[專利文獻5]特開2009-190069號公報 [Patent Document 5] JP-A-2009-190069

[專利文獻6]特開2014-212282號公報 [Patent Document 6] JP-A-2014-212282

[專利文獻7]特開2014-117707號公報 [Patent Document 7] JP-A-2014-117707

[專利文獻8]特開2012-240082號公報 [Patent Document 8] JP-A-2012-240082

[專利文獻9]特開2012-186287號公報 [Patent Document 9] JP-A-2012-186287

[專利文獻10]特開2015-129076號公報 [Patent Document 10] JP-A-2015-129076

[專利文獻11]特開2015-099922號公報 [Patent Document 11] JP-A-2015-099922

[專利文獻12]特開2009-037808號公報 [Patent Document 12] JP-A-2009-037808

[專利文獻13]特開2015-050226號公報 [Patent Document 13] JP-A-2015-050226

[專利文獻14]特開2015-030040號公報 [Patent Document 14] JP-A-2015-030040

[專利文獻15]特開2015-030039號公報 [Patent Document 15] JP-A-2015-030039

[專利文獻16]特開2007-229758號公報 [Patent Document 16] JP-A-2007-229758

非專利文獻 Non-patent literature

[非專利文獻1]Measurement Science and Technology, 12(2001)1784-1794, Laser-induced breakdown and damage in bulk transparent materials induced by tightly focused femtosecond laser pulse. [Non-Patent Document 1] Measurement Science and Technology, 12 (2001) 1784-1794, Laser-induced breakdown and damage in bulk transparent materials induced by tightly focused femtosecond laser pulse.

本發明所欲解決之問題點係目前工業界尚未創造出一種雷射加工方法,可在不產生任何污損的條件下,對強化玻璃、無鹼玻璃及藍寶石等透明脆性材料的剖面邊緣不直接進行加工,而且還能在不損壞用來支撐玻璃的下層膠帶的前提下,以自然切斷方面讓剖面呈鏡面狀。 The problem to be solved by the present invention is that a laser processing method has not yet been created in the industry, and the edge of the transparent brittle material such as tempered glass, alkali-free glass and sapphire is not directly formed without any fouling. The processing is carried out, and the cross section is mirror-like in terms of natural cutting without damaging the underlying tape for supporting the glass.

本發明之主要目的在於提供一種剖面端部不加工鏡面切斷法,包括:首先,使用一雷射切斷由玻璃、藍寶石或陶瓷所構成的一透明脆性材料時,在該透明脆性材料切斷面內複數雷射光束進行方向,以一雷射脈寬度之少許時間差連結複數焦點。其次,該些焦點部位透過一變性方式,使一透明體材料變化成一吸收體,藉以吸收光線,使得每一焦點位置產生熱應力破壞,並且避免每一焦點的入射光彼此影響,而形成複數破壞點。再者,藉由細微的該些破壞點以及該些破壞點之間所產生的應力之交互作用,以產生連續、細長且細微的熱破壞力來進行鏡面狀加工。 The main object of the present invention is to provide a cross-sectional end non-machining mirror cutting method, comprising: first, when a transparent brittle material composed of glass, sapphire or ceramic is cut by a laser, the transparent brittle material is cut off. The in-plane complex laser beam is oriented to connect the complex focus with a small time difference of the width of the laser pulse. Secondly, the focus portions are transformed into an absorber by a denaturation method, thereby absorbing light, causing thermal stress damage at each focus position, and avoiding incident light of each focus affecting each other to form a complex damage. point. Furthermore, mirror-like processing is performed by creating a continuous, slender, and subtle thermal destructive force by the fine interaction of the damage points and the stresses generated between the fracture points.

於本發明之剖面端部不加工鏡面切斷法中,更包括:將每一雷射光束加以切斷,並依據照射深度,將每一切斷後的該些雷射光束調整至適當的強度,藉以讓雷射光產生多個焦點;根據彼此最近的焦點間距來設置時間差以進行集光,而該時間差必須大於一脈衝寬度;由深至淺依序將集光點慢慢錯開,並以一壓電元件等高速振盪元件作為一光學系統,讓一群焦點朝該雷射行進方向振動;以及除了讓透明體朝切斷方向移動外,同時 讓深度方向以垂直方式排列的焦點,更朝深度方向以及加工方向擴展,藉以在較深的範圍內產生細小的龜裂,如此即可對表面和背面直接進行加工,並且在剖面端部留下加工記號,或是透過內部加工點,自然產生龜裂,接著再利用正確的龜裂深度來進行切斷。 In the non-machining mirror cutting method of the cross-sectional end portion of the present invention, the method further comprises: cutting each of the laser beams, and adjusting each of the cut laser beams to an appropriate intensity according to the irradiation depth, thereby Let the laser light generate multiple focal points; set the time difference according to the closest focal distance of each other to collect light, and the time difference must be greater than a pulse width; the light collecting points are slowly staggered from deep to shallow, and a piezoelectric a high-speed oscillating element such as an element as an optical system that causes a group of focal points to vibrate toward the direction of travel of the laser; and in addition to moving the transparent body toward the cutting direction, The focus in the vertical direction is extended more in the depth direction and in the machine direction, so that fine cracks are generated in a deeper range, so that the surface and the back surface can be directly processed and left at the end of the section The machining mark, or through the internal machining point, naturally produces cracks, and then uses the correct crack depth to cut.

本發明係以雷射光束進行切斷,讓多條光線集光成為較小的焦點,並且預留一些延遲時間,利用光線依序對透明體剖面切斷深度以直線排列方式,讓透明體發生變異,並且吸收光線,以便讓溫度上升,接著藉由光學系統的振動,讓破壞動作朝剖面方向行進,藉以擴大剖面範圍,並藉由破壞力形成一個理想的剖面。 The invention cuts off with a laser beam, so that a plurality of light beams are collected into a smaller focus, and some delay time is reserved, and the transparent body cross-cutting depth is arranged in a straight line by the light sequentially, so that the transparent body occurs. It mutates and absorbs light so that the temperature rises, and then the vibration of the optical system causes the breaking action to travel in the cross-section direction, thereby expanding the section range and forming a desired section by the destructive force.

本發明所採用的透明體雷射切斷方法,其優點在於,不需要使用超高強度的雷射,即可對內面局部部位進行長距離加工,或是能讓光線以細絲狀方式通過透明體內部,而且不需要進行剖面邊緣加工,即可留下較深的加工記號,不但如此,加工剖面不易產生微裂,並且還能維持高破壞強度,以形成理想的剖面。 The transparent body laser cutting method used in the present invention has the advantages that long-distance processing of a part of the inner surface can be performed without using an ultra-high-intensity laser, or light can be passed through in a filament-like manner. Inside the transparent body, and without the need for edge edge processing, deeper processing marks can be left. In addition, the processing profile is less prone to microcracking and maintains high breaking strength to form a desired profile.

1‧‧‧雷射光束 1‧‧‧Laser beam

2‧‧‧波長板 2‧‧‧wavelength board

3‧‧‧偏振器 3‧‧‧ polarizer

4‧‧‧變焦光學系統 4‧‧‧Zoom optical system

5‧‧‧偏振器 5‧‧‧ polarizer

6‧‧‧反射鏡 6‧‧‧Mirror

7‧‧‧反射鏡 7‧‧‧Mirror

8‧‧‧第2脈衝 8‧‧‧2nd pulse

9‧‧‧第1脈衝 9‧‧‧1st pulse

10‧‧‧入射透鏡支架 10‧‧‧Injection lens holder

11‧‧‧入射透鏡 11‧‧‧Injecting lens

12‧‧‧射出透鏡 12‧‧‧Injecting the lens

13‧‧‧高速振動器 13‧‧‧High speed vibrator

14‧‧‧支撐環 14‧‧‧Support ring

15‧‧‧支撐環 15‧‧‧Support ring

16‧‧‧延遲調整元件 16‧‧‧Delay adjustment components

17‧‧‧振動元件驅動器 17‧‧‧Vibration component driver

18‧‧‧對物透鏡 18‧‧‧object lens

19‧‧‧雙光束分割結合器 19‧‧‧Double beam splitter combiner

20‧‧‧脆性透明材料 20‧‧‧ Brittle transparent material

21‧‧‧載台 21‧‧‧ stage

23‧‧‧載台 23‧‧‧The stage

22‧‧‧雷射 22‧‧‧Laser

24‧‧‧圖案加工工件 24‧‧‧patterned workpiece

為便 貴審查委員能對本發明目的、技術特徵及其功效,做更進一步之認識與瞭解,茲舉實施例配合圖式,詳細說明如下:圖1係習知透明體加工方法示意圖;圖2係本發明較佳實施例之雙光束透明體加工方法示意圖;圖3係本發明用以將雷射光束分割為二光束之透明體切斷裝置架構示意圖;圖4係不同雷射光強度與透過率之關係圖; 圖5係應用本發明進行透明體加工時,不同材料深度與使用之能量關係圖;圖6係本發明雙光束振動加工方法較佳實施例之示意圖;圖7係本發明較佳實施例系統架構示意圖;圖8係藉本發明對不同材質進行剖面加工之結果示意圖;圖9係使用不同破壞強度進行剖面加工之結果示意圖;及圖10係將本發明應用於產業之系統架構示意圖。 To further understand and understand the purpose, technical features and effects of the present invention, the following embodiments are described in detail with reference to the drawings: FIG. 1 is a schematic view of a conventional transparent body processing method; FIG. 3 is a schematic diagram of a transparent body cutting device for dividing a laser beam into two beams according to a preferred embodiment of the present invention; FIG. 4 is a schematic diagram of different laser light intensity and transmittance. relation chart; 5 is a diagram showing the relationship between the depths of different materials and the energy used in the transparent body processing according to the present invention; FIG. 6 is a schematic view showing a preferred embodiment of the double beam vibration processing method of the present invention; FIG. 7 is a system architecture of a preferred embodiment of the present invention. FIG. 8 is a schematic diagram showing the results of cross-section processing of different materials by the present invention; FIG. 9 is a schematic diagram showing the results of cross-sectional processing using different breaking strengths; and FIG. 10 is a schematic diagram of a system architecture in which the present invention is applied to an industry.

請參閱圖2所示,本發明方法係在2個以上可在雷射內部產生變性之雷射焦點光(數1000000W/cm2)的數個焦點中,藉由在透明體內部實現附加時間差進行照射,避免相互干擾,使透明體內部從背面至表面之距離的任意點分別獨立且同時藉由光吸收而變性,藉由包含焦點間發生細長龜裂而有效導向自然斷裂者。 Referring to FIG. 2, the method of the present invention is performed by using two additional focal points that can generate denatured laser focus light (1000000 W/cm 2 ) inside the laser, by implementing an additional time difference inside the transparent body. Irradiation, avoiding mutual interference, and making any point of the distance from the back surface to the surface of the transparent body independent and simultaneously denatured by light absorption, and effectively guiding the natural fracture by including a slender crack between the focal points.

圖3係顯示依據本發明之使用分割為二光束之透明體切斷裝置的說明圖。另外,使用2個以上的分割光束時,亦可將同樣方法擴張。具有直線偏光之雷射光束(1)藉由半波長板(2)之旋轉而在任意之偏光方向旋轉。旋轉後之光藉由偏振器(3)在透過方向與反射方向分割成依偏光方向之比。通過之光藉由變焦光學系統(4)來調整光束之平行度。另一方面,反射後之光藉由反射鏡(6)、(7)反射,並藉由偏振器(5)結合成一條光束。此時,透過光束將以脈衝寬度大於反射光束的時間作為延遲時間,形成脈衝(8)及脈衝(9)而結合於相同光軸。光通過入射透鏡(11)及反射透鏡(12)而到達對物透鏡(18)。此時使入射透鏡(11)稍微移動,並使藉由對物透鏡(18)產生之雷射光束焦點位置稍微移動。該移動係藉由高速振動入射透鏡與射反射鏡之距離的壓電元件等的振動元件(13)來 進行。壓電元件在支架(10)上軸對稱而配置,並使其高速振動。 Fig. 3 is an explanatory view showing a transparent body cutting device divided into two beams according to the present invention. Further, when two or more split beams are used, the same method can be expanded. The laser beam (1) having linear polarization is rotated in any polarization direction by the rotation of the half-wavelength plate (2). The rotated light is split by the polarizer (3) into a ratio of the polarization direction in the transmission direction and the reflection direction. The passing light adjusts the parallelism of the light beam by the zoom optical system (4). On the other hand, the reflected light is reflected by the mirrors (6), (7) and combined into a light beam by the polarizer (5). At this time, the transmitted light beam is combined with the pulse (8) and the pulse (9) with the pulse width larger than the reflected beam as the delay time, and is combined with the same optical axis. Light passes through the incident lens (11) and the reflective lens (12) to the objective lens (18). At this time, the incident lens (11) is slightly moved, and the focus position of the laser beam generated by the objective lens (18) is slightly moved. This movement is performed by a vibration element (13) such as a piezoelectric element that vibrates the distance between the incident lens and the reflection mirror at a high speed. get on. The piezoelectric element is axially symmetrically arranged on the holder (10) and vibrates at a high speed.

圖4所示,雷射光透過透明體時,當光能低時幾乎全部光透過。提高雷射強度時,玻璃穿透度會急遽下降。藉由超過此種強度,可能使透明體吸收光而過熱。但是,須注意破壞狀況依照射之位置(深度)而異。比方說當雷射光進行照射時,若照射深的部分會破壞背面,若照射淺的部分會破壞表面。比方說當雷射光進行照射時,若要照射較深的部位,背面就會被破壞,照射較淺的部位則表面會受到破壞,原因在於內面的破壞強度高於表面或背面,換句話說必須根據深度位置,設定適合的照射強度。 As shown in Fig. 4, when the laser light passes through the transparent body, almost all of the light is transmitted when the light energy is low. When the laser intensity is increased, the glass penetration will drop sharply. By exceeding this strength, it is possible to cause the transparent body to absorb light and overheat. However, it must be noted that the damage condition varies depending on the position (depth) of the illumination. For example, when laser light is irradiated, if the deep portion is irradiated, the back surface is destroyed, and if the light is irradiated, the surface is destroyed. For example, when laser light is irradiated, if the deeper part is to be irradiated, the back surface will be destroyed, and the lighter part will be damaged, because the inner surface is more damaged than the surface or the back surface, in other words The appropriate illumination intensity must be set according to the depth position.

舉例來說,對圖5所示之強化玻璃,根據其所需要的內部破壞熱能閥值將光束分割為2條,並根據光束熱能的分配比率來分割雷射光束以進行照射,圖5係使用2條分割光束時之說明圖。 For example, for the tempered glass shown in FIG. 5, the beam is divided into two according to the required internal thermal energy threshold, and the laser beam is divided according to the distribution ratio of the thermal energy of the beam for illumination, and FIG. 5 is used. An illustration of two split beams.

將聚光雷射光束聚光於透明體,使剖面之深位置吸收光線。其次,接著透過延遲時間大於脈衝寬度的其他入射雷射光束集光於較深的位置。首先在深部產生一吸收體,藉以避免在下一個脈衝通過之光路上產生吸收體,而使第2雷射脈衝聚光。2個聚光點依使用之對物透鏡的倍率而異,兩者距離約為20~50微米,兩者大致同時照射,藉以在剖面方向產生單一焦點時無法獲得之長龜裂。此時,若要對表面附近的內部進行照射時,即使表面的集光強度較弱仍要進行加工,就必須讓雷射靠近表面,但太靠近表面則會影響內部加工,因此只能對表面加工。此外,背面也是一樣,若將焦點配置於背面附近,則只能對表面加工而非內部。因此,如圖5所示,照射時必須考量雷射強度相對於各種深度之上限值。 The concentrated laser beam is condensed on the transparent body to absorb light at a deep position in the cross section. Secondly, other incident laser beams having a delay time greater than the pulse width are then concentrated at a deeper position. First, an absorber is generated in the deep portion to avoid the generation of the absorber on the light path through which the next pulse passes, and to converge the second laser pulse. The two condensing points vary depending on the magnification of the lens used, and the distance between them is about 20 to 50 μm, and the two are irradiated at substantially the same time, so that long cracks which cannot be obtained when a single focus is generated in the cross-sectional direction are obtained. At this time, if the interior of the surface is to be irradiated, even if the intensity of the surface is weak, the laser must be processed, and the laser must be placed close to the surface, but too close to the surface will affect the internal processing, so it can only be used on the surface. machining. In addition, the back side is the same. If the focus is placed near the back side, the surface can only be machined instead of the inside. Therefore, as shown in FIG. 5, it is necessary to consider the laser intensity with respect to various upper depth limits when irradiating.

圖6中圖式顯示分割成2條光束而照射時,使2連焦點位置高速移動同時進行加工之情況。藉由使搭載了加工物之載台 移動同時使光束在透明體的深度方向振動,可在厚度方向擴大更寬廣平整之破壞面,藉由該操作實現朝向表面及背面自然割斷的狀況。 The diagram in Fig. 6 shows a case where the two focal points are moved at high speed while being processed while being divided into two beams. By using a stage equipped with a workpiece At the same time, the beam is vibrated in the depth direction of the transparent body, and the wider and flat fracture surface can be enlarged in the thickness direction, and the operation is naturally cut off toward the surface and the back surface.

脆性透明材料應為精密加工者,而選擇強化玻璃、無鹼玻璃、藍寶石進行試驗,在進行剖面之表面狀態的粗度及鏡面狀態如何的檢查同時,藉由從外部施力實施破壞強度試驗。 The brittle transparent material should be a precision processor, and tempered glass, alkali-free glass, and sapphire are selected for testing. The thickness and surface state of the surface of the cross section are examined, and the breaking strength test is performed by external force application.

圖7係本發明裝置之實施例的說明圖,雙光束分割結合器(19)如圖3所示。雷射光束(1)通過雙光束分割結合器(19)後,第1脈衝(8)藉由對物透鏡(18)到達透明體深部進行加工。然後,第2脈衝(9)到達更淺部分進行透明體(20)之加工。該光束藉由雙光束分割結合器內部之振動器而在深度方向上下移動。加工時則利用移動工作台(21)的方式來進行。載台以精密方式製作而成,對於透明材料厚度具有將深度方向的變動範圍限制在10微米以下的效果。 Figure 7 is an explanatory view of an embodiment of the apparatus of the present invention, and the double beam splitting combiner (19) is as shown in Fig. 3. After the laser beam (1) passes through the double beam splitter combiner (19), the first pulse (8) is processed by the object lens (18) reaching the deep portion of the transparent body. Then, the second pulse (9) reaches a shallower portion to process the transparent body (20). The beam is moved up and down in the depth direction by the vibrator inside the double beam splitting combiner. The machining is performed by means of a moving table (21). The stage is manufactured in a precise manner, and has an effect of limiting the variation range in the depth direction to 10 μm or less for the thickness of the transparent material.

圖8顯示實施例之結果。使用10ps、100Micro J之脈衝雷射與25kHz的壓電振動元件之加工試驗,在試驗強化玻璃時,即使使用1000倍之放大顯微鏡剖面無加工痕,仍無法觀察表面構造而成為鏡面狀態。無鹼玻璃因為需要提高溫度,所以會有少許加工痕殘留。在試驗藍寶石時,由於其耐熱性較高,又兼具高強度,因此需要較好的熱傳導度及高溫,雖然會出現部分加工記號,但是仍以鏡面所佔的比率較高。在試驗藍寶石時,從正上方觀看加工物時,因為表面未被切斷而係自然裂開者,雖有裂溝卻無達到切斷程度之間隙,也不發生塵埃。此外,熱能也完全被消耗於內部加工,因此貼附於加工物上的支撐膠帶雖然造成光線強度衰減,但是膠帶並未因為雷射光而燒毀。 Figure 8 shows the results of the examples. When a 10 ps, 100 Micro J pulsed laser and a 25 kHz piezoelectric vibration element were used for the test, when the tempered glass was tested, even if a 1000-fold magnification microscope section was used without a process mark, the surface structure could not be observed and the mirror surface state was observed. Since the alkali-free glass needs to be heated, a small amount of processing marks remain. When testing sapphire, because of its high heat resistance and high strength, it requires better thermal conductivity and high temperature. Although some processing marks appear, the ratio of mirror surface is higher. When the sapphire is tested, when the workpiece is viewed from directly above, the surface is naturally cracked because the surface is not cut, and although there is a crack, the gap is not reached, and dust does not occur. In addition, the thermal energy is also completely consumed in the internal processing, so the support tape attached to the workpiece causes the light intensity to be attenuated, but the tape is not burnt due to the laser light.

用與實施例1同樣之試驗條件,對寬度70mm、長度 180mm、厚度550微米、強化深度90微米之強化玻璃進行加工後,再執行3點破壞試驗。圖9所示係針對切斷後的強化玻璃材料進行破壞強度測試後的測試結果,由圖9可知,針對破壞強度較低的一組進行剖面邊緣加工,對於破壞強度較高的一組則不進行剖面邊緣加工,因此瞭解顯示的數值高。 Using the same test conditions as in Example 1, the width was 70 mm and the length was A tempered glass of 180 mm, a thickness of 550 μm, and a depth of 90 μm was processed, and a three-point failure test was performed. Fig. 9 shows the test results after the breaking strength test of the tempered glass material after cutting. It can be seen from Fig. 9 that the cutting edge processing is performed for a group having a low breaking strength, and the group having a higher breaking strength is not performed. The edge of the profile is machined, so it is understood that the displayed value is high.

強化玻璃係以雷射進行切斷加工,不過,因為切斷後之產品的破壞強度低,所以在加工後需要各種機械加工及化學處理,不但製程複雜,且既費時又昂貴。使用本方法時,如圖10所示,藉由使載台(23)搭載透明脆性材料材料(24),無須增加包含曲面之自由形狀的加工,因此有產業上之優點。 The tempered glass is cut by laser. However, since the product after cutting has a low breaking strength, various mechanical processing and chemical treatment are required after the processing, which is complicated, and time consuming and expensive. When this method is used, as shown in Fig. 10, by mounting the transparent brittle material (24) on the stage (23), it is not necessary to increase the processing including the free shape of the curved surface, and therefore there is an industrial advantage.

使用本方法時,可實現平整之剖面。透明脆性材料具有熔點高、耐壓縮應力之特性。雷射加工中,因為藉由將雷射光聚光在小焦點可獲得高電場強度,所以材料比較容易破壞,不過,因為係破壞剖面所以會髒污。反之,以雷射急速加熱及急速冷卻之熱應力破壞容易被應力場支配,因此顯示如鏡面狀態之平整破壞。因為在每1平方公分數1000000MW程度之輸出密度中,會發生熱應力破壞,所以藉由透鏡選定2點達到此種輸出密度之區域,藉由同時照射,使2點相互作用之龜裂發生,即可有效實現平整之切斷。 When using this method, a flat profile can be achieved. Transparent brittle materials have the characteristics of high melting point and resistance to compressive stress. In laser processing, since the high electric field intensity is obtained by concentrating the laser light at a small focus, the material is relatively easily broken, but it is dirty because the structure is broken. Conversely, the thermal stress damage caused by rapid heating of the laser and rapid cooling is easily dominated by the stress field, thus showing flatness damage such as a mirror state. Since the thermal stress damage occurs at an output density of about 1,000,000 MW per square centimeter, the area where the output density is achieved by selecting two points by the lens, and the two-point interaction crack occurs by simultaneous irradiation. The cutting of the flat can be effectively achieved.

使用本方法時,可實現可維持高強度之切斷材料。由於脆性材料之破壞以剖面端部之微細裂紋為破壞起點,因此在切斷中,不進行剖面,特別是剖面端面部之加工,而係設法進行協助沿著自然應力場之破壞的加工。因而,為了自然地誘導裂紋,發生剖面邊緣部分為終端之自然破壞的方式,加工範圍就必須涵蓋邊緣附近。但是,為了提高聚光強度而使用短焦點透鏡時,各剖面僅一部分可加工,所以係藉由生成數個焦點部同時加工,或 是使一個焦點部分高速移動,或是藉由同時利用這2個效果,在儘量寬之範圍進行加工。藉此,若僅一部分加工形成大的破壞時無法切斷,反之,藉由堆積平整之微細破壞來實現平穩的加工。高速振動係擴大2kHz~30kHz程度之壓電元件的振動,並重複實施10微米~30微米程度之振動。 When this method is used, a cutting material capable of maintaining high strength can be realized. Since the breakage of the brittle material is the starting point of the crack at the end of the cross section, the cross section, particularly the processing of the end face portion, is not performed during the cutting, and processing for assisting the destruction along the natural stress field is sought. Therefore, in order to naturally induce cracks, the edge portion of the section is a natural destruction of the terminal end, and the processing range must cover the vicinity of the edge. However, when a short focus lens is used to increase the intensity of the condensing, only a part of each cross section can be processed, so that a plurality of focal portions are simultaneously processed, or It is to make a focus part move at a high speed, or to use the two effects at the same time to process in the widest possible range. Thereby, if only a part of the processing forms a large failure, the cutting cannot be performed, and conversely, the smooth processing by the flatness of the deposition is achieved. The high-speed vibration system expands the vibration of a piezoelectric element of about 2 kHz to 30 kHz, and repeats the vibration of about 10 μm to 30 μm.

使用本方法時,可避免加工時產生粉塵。因為表面加工時會發生塵埃,所以切斷作業後需要進行洗淨。若要避免粉塵則應捨棄表面切割。藉由本發明同時照射數個點,實現不發生塵埃之龜裂,藉由僅切斷內部減少加工痕,可防止塵埃之發生或是塵埃從切斷部飛散,所以可運用在無塵室等之加工。 When using this method, dust can be avoided during processing. Since dust is generated during surface processing, it needs to be cleaned after the cutting operation. To avoid dust, the surface cut should be discarded. By irradiating a plurality of points at the same time, it is possible to prevent cracking of dust, and it is possible to prevent the occurrence of dust or the dust from scattering from the cut portion by cutting only the inside to reduce the processing marks, so that it can be used in a clean room or the like. machining.

使用本方法進行加工時,保持材料之下面膠帶不致破損。藉由以焦點距離短之透鏡系統聚光,係以內部之加工雷射強度進行加工,不過,膠帶面因為能量通過加工部而減低,所以雷射強度極端降低,可選擇膠帶不致被加工之條件。 When processing using this method, keep the tape under the material from damage. By concentrating the lens system with a short focal length, the processing is performed with the internal processing laser intensity. However, since the tape surface is reduced by the energy passing through the processing portion, the laser intensity is extremely lowered, and the condition that the tape is not processed can be selected. .

使用本方法可對厚材料進行加工。過去厚材料需要將強力之雷射光以長焦點對物透鏡聚光,不過,焦點部會變大且形成加工污痕。因此,係依據本發明藉由在剖面方向配置數個焦點位置,或是使一個焦點高速移動,即可在容易斷裂狀態下切斷,所以可對厚材料進行加工。 Thick materials can be processed using this method. In the past, thick materials required a strong laser to condense the lens with a long focus, but the focus portion became large and formed a process stain. Therefore, according to the present invention, it is possible to cut a thick material by arranging a plurality of focus positions in the cross-sectional direction or moving a focus at a high speed to be cut in an easily broken state.

按,以上所述,僅係本發明之若干較佳實施例,惟,本發明所主張之權利範圍,並不侷限於此,按凡熟悉該項技藝之人士,依據本發明所揭露之技術內容,可輕易思及之等效變化,均應屬不脫離本發明之保護範疇。 The foregoing is only a few preferred embodiments of the present invention, but the scope of the claimed invention is not limited thereto, and the technical contents disclosed in the present invention are disclosed by those skilled in the art. Equivalent changes that can be easily considered are within the scope of protection of the present invention.

1‧‧‧雷射光束 1‧‧‧Laser beam

2‧‧‧波長板 2‧‧‧wavelength board

3‧‧‧偏振器 3‧‧‧ polarizer

4‧‧‧變焦光學系統 4‧‧‧Zoom optical system

5‧‧‧偏振器 5‧‧‧ polarizer

6‧‧‧反射鏡 6‧‧‧Mirror

7‧‧‧反射鏡 7‧‧‧Mirror

8‧‧‧第2脈衝 8‧‧‧2nd pulse

9‧‧‧第1脈衝 9‧‧‧1st pulse

10‧‧‧入射透鏡支架 10‧‧‧Injection lens holder

11‧‧‧入射透鏡 11‧‧‧Injecting lens

12‧‧‧射出透鏡 12‧‧‧Injecting the lens

13‧‧‧高速振動器 13‧‧‧High speed vibrator

14‧‧‧支撐環 14‧‧‧Support ring

15‧‧‧支撐環 15‧‧‧Support ring

16‧‧‧延遲調整元件 16‧‧‧Delay adjustment components

17‧‧‧振動元件驅動器 17‧‧‧Vibration component driver

18‧‧‧對物透鏡 18‧‧‧object lens

Claims (2)

一種剖面端部不加工鏡面切斷法,包括:使用一雷射切斷由玻璃、藍寶石或陶瓷所構成的一透明脆性材料時,在該透明脆性材料切斷面內複數雷射光束進行方向,以一雷射脈寬度之少許時間差連結複數焦點;該些焦點部位透過一變性方式,使該透明脆性材料變化成一吸收體,藉以吸收光線,使得每一焦點位置產生熱應力破壞,並且避免每一焦點的入射光彼此影響,而形成複數破壞點;以及藉由細微的該些破壞點以及該些破壞點之間所產生的一應力之交互作用,以產生連續、細長且細微的一熱破壞力來進行一鏡面狀加工。 A cross-sectional end non-machining mirror cutting method, comprising: when a transparent brittle material composed of glass, sapphire or ceramic is cut by a laser, a plurality of laser beams are oriented in the cut surface of the transparent brittle material, The plurality of focal points are connected by a time difference of a laser pulse width; the focus portions are transformed into an absorber by a denaturation method, thereby absorbing light, causing thermal stress damage at each focus position, and avoiding each The incident light of a focus affects each other to form a plurality of break points; and by the fine interaction of the break points and a stress generated between the break points, to produce a continuous, slender and subtle thermal damage Force to perform a mirror-like process. 如申請專利範圍第1項所述之剖面端部不加工鏡面切斷法,更包括:將每一雷射光束加以切斷,並依據照射深度,將每一切斷後的該些雷射光束調整至一適當強度,藉以讓雷射光產生該些焦點;根據彼此最近的該些焦點間距來設置時間差以進行一集光,而該時間差必須大於該雷射脈寬度;由深至淺依序將一集光點慢慢錯開,並以一壓電元件等高速振盪元件作為一光學系統,讓該些焦點朝該雷射行進方向振動;以及除了讓該透明脆性材料朝切斷方向移動外,同時讓深度方向以垂直方式排列的該些焦點,更朝深度方向以及加工方向擴展,藉以在較深的範圍內產生細小的龜裂,如此即可對表面和背面直接進行加工,並且在剖面端部留下加工記號,或是透過內部加工點,自然產生龜裂,接著再利用正確的龜裂深度來進行切斷。 The cross-sectional end non-machining mirror cutting method described in claim 1 further includes: cutting each of the laser beams, and adjusting each of the cut laser beams to the irradiation depth according to the irradiation depth. a suitable intensity, whereby the laser light produces the focus; the time difference is set according to the closest focal distances of each other to perform a set of light, and the time difference must be greater than the width of the laser pulse; The light collecting point is slowly staggered, and a high-speed oscillating element such as a piezoelectric element is used as an optical system to vibrate the focus toward the laser traveling direction; and in addition to moving the transparent brittle material in the cutting direction, The focal points arranged in the vertical direction in the depth direction are further expanded in the depth direction and the processing direction, thereby generating fine cracks in a deeper range, so that the surface and the back surface can be directly processed and left at the end of the section The lower processing marks, or through the internal processing points, naturally produce cracks, and then use the correct crack depth to cut.
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