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TW201221261A - Laser processing apparatus, processing method of processed object and dividing method of processed object - Google Patents

Laser processing apparatus, processing method of processed object and dividing method of processed object Download PDF

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Publication number
TW201221261A
TW201221261A TW100120441A TW100120441A TW201221261A TW 201221261 A TW201221261 A TW 201221261A TW 100120441 A TW100120441 A TW 100120441A TW 100120441 A TW100120441 A TW 100120441A TW 201221261 A TW201221261 A TW 201221261A
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Taiwan
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light
optical path
workpiece
laser light
processing
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TW100120441A
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Chinese (zh)
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TWI522199B (en
Inventor
Shohei Nagatomo
Ikuyoshi Nakatani
Mitsuru Sugata
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Mitsuboshi Diamond Ind Co Ltd
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Abstract

The present invention provides a processing method of divided object capable of more accurately dividing a processed object. The solution is to let a pulse laser light with psec pulse width emitting from a light source in its midway course to a stage branched into a first optical path and a second optical path. For each unit pulse light, the optical path length of the second optical path is so set that the second half pulse light traveling in the second optical path is more delayed than the first half pulse light traveling in the first optical path. The irradiated regions by the first half pulse light and the second half pulse light are the same, and the processing surface of irradiated region of each unit pulse light is irradiated with a pulsed laser light in a discrete way. Because cleavage is generated between the irradiated regions of the processed object, it forms as a starting point for dividing the processed object.

Description

201221261 六、發明說明: 【發明所屬之技術領域】 本發明係關於照射雷射光而對被加工物進行加工之雷射 加工方法及該方法中所使用之雷射加工裝置。 【先前技術】 作為照射脈衝.雷射光而對被加工物進行加工之技術(以 下,亦簡單地稱作雷射加工或者雷射加工技術)已周知有 各種技術(例如,參照專利文獻1至專利文獻4)。 專利文獻1所揭示者為如下方法:於對作為被加工物之 晶粒進行分割時’藉由雷射剝钱而沿著分割預定線形成剖 面V字形之槽(切斷槽),以該槽為起點對晶粒進行分割。 另一方面’專利文獻2所揭示者為如下方法:藉由沿著被 加工物(被分割體)之分割預定線照射散焦狀態之雷射光, 而於被照射區域產生與周圍相比結晶狀態受到破壞之剖面 大致V字形之熔解改質區域(變質區域),以該熔解改質區 域之最低點為起點對被加工物進行分割。 於使用專利文獻1及專利文獻2所揭示之技術形成分割起 點之情形時,肖重要的是沿著雷射光之掃描方向即分割預 定線方向形成均-形狀之V字形剖面(槽剖面或者變質區域 剖面)以良好地進行其後之分割。作為用於此之對策,例 如控制雷射光之照射以使每i脈衝之雷射光之被照射區域 (光束點)前後重疊。 例如,於設作為雷射加工之最基本參數之重複頻率(單 位kHz)為R,且設掃描速度(單位„1111/^(〇為¥時兩者之比201221261 VI. Description of the Invention: [Technical Field] The present invention relates to a laser processing method for processing a workpiece by irradiating laser light and a laser processing apparatus used in the method. [Prior Art] Various techniques are known as techniques for processing a workpiece by irradiation of laser light (hereinafter, simply referred to as laser processing or laser processing technology) (for example, refer to Patent Documents 1 to Document 4). Patent Document 1 discloses a method of forming a groove (cut groove) having a V-shaped cross section along a line to be divided by a laser stripping when dividing a crystal grain as a workpiece, The die is divided for the starting point. On the other hand, the method disclosed in Patent Document 2 is a method in which a laser beam in a defocused state is irradiated along a planned dividing line of a workpiece (divided body), and a crystal state is generated in the irradiated region as compared with the surrounding region. The fractured and modified region (metamorphic region) having a substantially V-shaped cross section is broken, and the workpiece is divided by the lowest point of the melt-modified region. When forming a division starting point using the techniques disclosed in Patent Document 1 and Patent Document 2, it is important to form a uniform-shaped V-shaped cross section (groove section or metamorphic region) along the scanning direction of the laser light, that is, the direction of dividing the line. Section) to perform the subsequent segmentation well. As a countermeasure for this, for example, the irradiation of the laser light is controlled so that the irradiated area (beam spot) of the laser light per i pulse overlaps before and after. For example, the repetition frequency (unit kHz) set as the most basic parameter for laser processing is R, and the scanning speed (in units of „1111/^(〇 is ¥)

S 156646.doc 201221261 V/R成為光束點之中心間隔,但於專利文獻丨及專利文獻2 所揭示之技術中,於V/R為1 以下之條件下進行雷射光 之照射及掃描以使光束點彼此產生重疊。 又,專利文獻3中揭示如下形態:藉由將雷射光對準聚 光點照射至表面具有積層部之基板内部而於基板内部形成 改質區域’以該改質區域為切斷起點。 又,專利文獻4中揭示如下形態:對1個分離線重複多次 進行雷射光掃描,而沿深度方向之上下形成於分離線方向 連續之槽部及改質部,與於分離線方向不連續之内部改質 部。 另一方面’專利文獻5中揭示如下形態:作為使用脈寬 為psec級之超短脈衝之雷射光之加工技術,藉由調整脈衝 雷射光之聚光點位置而自被加工物(板體)之表層部位至表 面形成成群產生有微小裂痕之微小熔解痕,從而形成該等 熔解痕連成線狀之分離容易化區域。 [先前技術文獻] [專利文獻] [專利文獻1]曰本專利特開2004-9139號公報 [專利文獻2]國際公開第2006/062017號 [專利文獻3]日本專利特開2007-83309號公報 [專利文獻4]日本專利特開2008-98465號公報 [專利文獻5]日本專利特開2005-271563號公報 【發明内容】 [發明所欲解決之問題] 156646.doc 201221261 藉由雷射光形成分割起點,其後藉由切斷器進行分割之 方法,與自先前以來進行之機械切斷法即鑽石劃片相比, 於自動性、高速性、穩定性、高精度性方面較為有利。 然而’於用先前方法藉由雷射光形成分割起點之情形 時,會π可避免地於照# ^之部分形成有所謂之加工 痕(雷射加工痕)。所謂加工痕係指照射雷射光之結果,與 照射前相比材質或結構發生變化之變質區域。加工痕之形 成通常會對所分割之各個被加工物(分割原片)之特性等造 成不良影響,因而儘可能地加以抑制為佳。 例如,於藉由專利文獻2所揭示之先前之雷射加工將於 包含藍寶石等硬脆性且光學性透明之材料之基板上形成有 LED(llght emitting diode,發光二極體)結構等之發光元件 結構之被加1物按晶片單位分割而得之發光元件之邊緣部 分(分割時受到雷射光之照射之部分),連續性地形成有寬 度數μιη左右且深度數μιη至數十μιη左右之加工痕。從而存 在該加工痕吸收於發光元件内部產生之光而導致來自元件 之光提取效率降低之問題。於使用折射率高之藍寶石基板 之發光元件結構之情形時該問題尤為顯著。 本發明之發明者進行積極研究之結果而獲得如下知識見 解,即於對被加工物照射雷射光而形成分割起點時,利用 該被加工物之劈理性或者解理性,由此可較好地抑制加工 痕之形成。又獲得如下知識見解,即於該加工中使用超短 脈衝之雷射光為佳。 專利文獻1至專利文獻5中,絲毫未揭示或暗示利用被加 156646.doc 201221261 工物之劈理性或者解理性形成分割起點之形態。 本發明係鑒於上述問題而完成者,其目的在於提供一種 可抑制加工痕之形成,並且可形成更確實地實現被加工物 之分割之分割起點之被分割體之加工方法、及此方法中所 使用之雷射加工裝置。 [解決問題之技術手段] 為解決上述問題,技術方案丨之發明係一種雷射加工裝 置,其特徵在於包括:光源,其發出脈衝雷射光;及載 台,其載置被加工物;且上述脈衝雷射光係脈寬為^%級 之超短脈衝光,自上述光源至上述載台之上述脈衝雷射光 之光路以於中途部分地分支為第丨光路與第2光路且其後合 流之方式設置;上述雷射加工裝置進而包括光路長調整機 構,其可改變上述第2光路之光路長;於定義為自上述光 源出射之上述脈衝雷射光分支為於上述第丨光路中前進之 第1雷射光與於上述第2光路中前進之第2雷射光,且上述 脈衝雷射光之單位脈衝光分支為上述第1#射光之單位脈 衝光即第1半脈衝光與上述第2雷射光之單位脈衝光即第2 半脈衝光時’上述光路長調整機構以於合流後之上述光路 中使上述第2半脈衝光較上述第i半脈衝光更為延遲之方式 設定上述第2光路之光路長;於將上述被加工物載置於上 述载台之狀態下,藉由一面使上述載台移動一面將上述脈 衝雷射光…、射至上述被加工物’而使上述各個單位脈衝光 之上述第1半脈衝光與上述第2半脈衝光之被照射區域於上 述被加工物之被加工面上實質上相同、並且於上述被加工 156646.doc 201221261 物之被加工面上離散地形成上述各個單位脈衝光之上述被 照射區域。 技術方案2之發明係如技術方案!之雷射加工裝置,其中 光路長調整機構以使上述第2半脈衝光相對於上述第丨半脈 衝光僅延遲上述單位脈衝光之半值寬之1/3倍以上且1〇 —下之延遲時間之方式,較上述第2光路之光路 長。 技術方案3之發明係如技術方案2之雷射加工裝置,其中 進而包括調整上述第2雷射光之強度之強度調整機構;上 述光路長調整機構以使上述第2半脈衝光相對於上述第1半 脈衝光僅延遲上述單位脈衝光之半值寬之丨倍以上且2倍以 下之延遲時間之方式,設定上述第2光路之光路長;上述 強度調整機構以使上述第2雷射光之強度小於上述第丨雷射 光之強度之方式調整上述第2雷射光之強度。 技術方案4之發明係如技術方案2之雷射加工裝置,其中 進而包括調整上述第2雷射光之焦點之焦點調整機構;上 述光路長調整機構以使上述第2半脈衝光相對於上述第1半 脈衝光僅延遲上述單位脈衝光之半值寬之丨倍以上且2倍以 下之延遲時間之方式,設定上述第2光路之光路長;上述 焦點調整機構以使上述第2雷射光之光束直徑大於上述第工 雷射光之光束直徑之方式調整上述第2雷射光之焦點。 技術方案5之發明係一種用以於被加工物形成分割起點 之加工方法,其特徵在於包括:光路設定步驟,將自出射 脈寬為psec級之超短脈衝光之脈衝雷射光之光源至載置被 156646.doc 201221261 加工物之载台之光路設定為於中途部分地分支為^光路 與第2光路且其後合流;光路長調整步驟,於定義為自上 述光源出射之上述脈衝雷射光分支為於上述第(光路中前 進之第i雷射光與於上述第2光路中前進之第2雷射光,且 上述脈衝雷射光之單位脈衝光分支為上述第丨雷射光之單 位脈衝光即第i半脈衝光與上述第2雷射光之單位脈衝光即 第2半脈衝光時’以使上述第2半脈衝光較上述第ι半脈衝 光更為延遲之方式設定上述第2光路之光路長;載置步 驟,將上述被加工物載置於上述載台上;及照射步驟,以 使上述各個單位脈衝光之上述第丨半脈衝光與上述第2半脈 衝光之被照射區域相同,且上述各個單位脈衝光之上述被 舨射區域於上述被加工物之被加工面上離散性地形成之方 式,將上述脈衝雷射光照射至上述被加工物,由此於上述 被照射區域彼此之間使上述被加工物產生劈理或者解理, 從而於上述被加工物形成用以進行分割之起點。 技術方案6之發明係如技術方案5之被加工物之加工方 法’其中於光路長調整步驟中’以使上述第2半脈衝光相 對於上述第1半脈衝光僅延遲上述單位脈衝光之半值寬之 1/3倍以上且2倍以下之延遲時間之方式,設定上述第2光 路之光路長。 技術方案7之發明係如技術方案6之被加工物之加工方 法’其中進而包括調整上述第2雷射光之強度之強度調整 步驟;於上述光路長調整步驟中’以使上述第2半脈衝光 相對於上述第1半脈衝光僅延遲上述單位脈衝光之半值寬 156646.doc 201221261 之1倍以上且2倍以下之延遲時間之方式,設定上述第2光 路之光路長;於上述強度調整步驟中,以使上述第2雷射 光之強度小於上述第丨雷射光之強度之方式調整上述第2雷 射光之強度。 技術方案8之發明係如技術方案6之被加工物之加工方 法,其巾進而包括調整上述第2雷#光之焦點之焦點調整 步驟;於上述光路長調整步驟中,以使上述第2半脈衝光 相對於上述第1半脈衝光僅延遲上述單位脈衝光之半值寬 之1倍以上且2倍以下之延遲時間之方式,設定上述第2光 路之光路長,·於上述焦點調整步驟中,以使上述第2雷射 光之光束直徑大於上述第丨雷射光之光束直徑之方式調整 上述第2雷射光之焦點。 技術方案9之發明係如技術方案5至8中任一項之被加工 物之加工方法’其中以於上述被加工物之容易劈開或者裂 開之方向上相鄰之方式形成藉由不同之上述單位脈衝光所 形成之至少2個被照射區域。 技術方案10之發明係如技術方案9之被加工物之加工方 法’其中沿著上述被加工物之容易劈開或者裂開之方向形 成所有之上述被照射區域。 技術方案11之發明係如技術方案9之被加工物之加工方 法’其中於上述被加工物之不同之2個上述容易劈開或者 裂開之方向上交替進行上述至少2個被照射區域之形成。 技術方案12之發明係如技術方案5至8中任一項之被加工 物之加工方法’其中於相對於上述被加工物之不同之= 156646.doc 201221261 而等價之方向上形成上述被照射 容易劈開或者裂開之方向 區域。 技術方案13之發明係-種分割被加工物之方法,且對藉 由技術方案5至] 項之方法而形成有分割起點之被 加工物沿著上述分割起點進行分割。 [發明之效果] 根據技術方案1至13之發明,可使因被加工物之變質而 導致之加工痕之形成或被加工物之飛散等為僅限於局部之 現象另方面可藉由積極地使被加工物產生劈理或者解 理而與先前相比以極高之速度對被加工物形成分割起點。 尤其,如技術方案2至4及6至8之發明,脈衝雷射光之能 量利用效率提高’因此可更有效率且確實地形成分割起 【實施方式】 <加工之原理> 百先,對以下所示之本發明之實施方式中所實現之加工 之原理進行說明。本發明中所進行之加工概略地說為如下 者:一面掃描脈衝雷射光(以下,亦簡單地稱作雷射光)一 面將該脈衝雷射光照射至被加工物之上表面(被加工面), 由此於各個脈衝之被照射區域之間使被加工物依序產生劈 理或者解理,作為於各自上所形成之劈理面或者解理面之 連續面而形成用以進行分割之起點(分割起點)。 再者,本實施方式中,裂開係指被加工物沿著解理面以 外之結晶面大致規則地斷.裂之現象,將該結晶面稱作解理 156646.doc •10· 201221261 者’除完全沿著結晶面之作為微觀現象之劈開 裂之裂广生 疋之…日日方位產生作為宏觀斷 痕之情形。根據物質之不同,亦存在僅主要產生辟 理、解理或者裂痕之任—去 71 對劈理“ 為避免說明之繁瑣而 解理及裂痕不加以區別地統稱為劈理/解理等。 :’有時亦將上述形態之加工簡單地稱作劈開/裂開加工 等。 以下,以被加工物為六方晶之單晶物質,且其U轴' U :及a3軸之各軸方向為容易劈開/裂開之方向之情形為例 仃說明。例如,c面藍寶石基板等符合此。六方晶之ai 轴、a2轴及a3軸於c面内處於相互均成12〇。之角度且相互 對稱位置。本發明之加工中,根據該等軸之方向與預定加 工線之方向(預定加工方向)之關係而存在幾個圖案。以 下對,亥等圖案進行說明。再者,以下,將按照各個脈衝 而照射之雷射光稱作單位脈衝光。 <第1加工圖案> 第1加工圖案係a i軸方向、a2轴方向及a3軸方向之任一 者與預疋加工線平行之情形之劈開/裂開加工之形態。更 一般而言為容易劈開/裂開之方向與預定加工線之方向一 致之情形之加工形態。 圖1係模式性地表示第丨加工圖案之加工形態之圖。圖i 中例不al轴方向與預定加工線L平行之情形。圖1(a)係表示 該情形之al軸方向、a2軸方向及a3軸方向與預定加工線[ 之方位關係之圖。圖1(b)表示雷射光之第1脈衝之單位脈衝 156646.doc 201221261 光照射至預定加工線L端部之被照射區域re丨之狀態。 一般而言,單位脈衝光之照射會對被加工物之極微小區 域施加較高之能量’因此該照射會導致於被照射面之相當 於單位脈衝光(雷射光)之被照射區域或者較被照射區域宽 之範圍内產生物質之變質、熔融、蒸發除去等。 然而’當將單位脈衝光之照射時間即脈寬設定得極短 時’處於較雷射光之光點尺寸狹小之、被照射區域RE1之 大致中央區域之物質自照射之雷射光獲得運動能量而等離 子化或者南溫化至氣體狀態等而變質,進而向與被照射面 垂直之方向飛散’另一方面以伴隨該飛散而產生之反作用 力為代表之藉由單位脈衝光之照射而產生之衝擊或應力作 用於該被照射區域之周圍,尤其作用於作為容易劈開/裂 開之方向之al轴方向、a2轴方向及a3轴方向。由此,沿著 該方向於外觀上保持接觸狀態但部分地產生微小劈理或者 解理’或者產生内有熱變形但不至於引起劈理或解理之狀 態。換言之’亦可說超短脈衝之單位脈衝光之照射作為用 以形成朝向容易劈開/裂開之方向之俯視大致直線狀之弱 強度部分之驅動力發揮作用。 圖1 (b)中以虛線箭頭模式性地表示於上述各容易劈開/裂 開之方向上形成之弱強度部分中,與預定加工線L之延伸 方向一致之+al方向上之弱強度部分wi。 繼而’當如圖1 (c)所示照射雷射光之第2脈衝之單位脈衝 光而於預定加工線L上之自被照射區域RE1僅離開特定距 離之位置形成被照射區域rE2時,與第1脈衝相同地,於該 156646.doc 12 201221261 第2脈衝下亦形成有沿著容易劈開/裂開之方向之弱強度部 分。例如,於_al方向形成有弱強度部分W2a,於+ai方向 上形成有弱強度部分W2b。 但於此時間點,藉由第1脈衝之單位脈衝光之照射而形 成之弱強度部分貿丨處於弱強度部分W2a之延伸方向上。 即,弱強度部分W2a之延伸方向成為可以較其他部位更小 之能量產生劈理或解理(能量吸收率高)之部位。因此,實 際上,當照射第2脈衝之單位脈衝光時,此時產生之衝擊 或應力向容易劈開/裂開之方向及處於其前端之弱強度部 为傳播,大致於照射之瞬間,自弱強度部分W2a至弱強度 部分wi產生徹底之劈理或者解理。由此,形成有圖i(d)所 不之劈理/解理面C1。再者,劈理/解理面C1於被加工物之 自圖中觀察垂直之方向上可形成至數4111至數十μιη左右之 深度。而且’如下上述,於劈理/解理面C1上,作為受到 較強之衝擊或應力之結果而於結晶面產生滑動,且於深度 方向產生起伏。 然後’當如圖1(e)所示藉由之後沿著預定加工線L掃描 雷射光而對被照射區域RE1、RE2、RE3、RE4·..依序照射 單位脈衝光時’對應於此而依序形成劈理/解理面C2、 C3 —。該形態中連續地形成劈理/解理面者為第1加工圖案 之劈開/裂開加工。 若自其他觀點來看則可說,因藉由照射單位脈衝光施加 熱能量而導致被加工物之表層部分膨脹,於被照射區域 RE1、RE2、RE3、RE4…之各自之較大致中央區域而靠外 156646.doc -13- 201221261 側作用有與劈理/解理 從而推進劈開/裂開。C2、。·..垂直之拉伸應力, 之多工圖案中,沿著預定加工線l而離散地存在 ‘、、、、區域與形成於該等多個被照射區域之間之劈 理/解理面整體卜士 *j ^ ^ 割時之八^ 者預定加工線L對被加工物進行分 1且亦Iβ㉟°於形成該分割起點之後,進行使用特定 置之分割而可以大致沿著狀加工線L之形態對 被加工物進行分割。 者為實現該劈開/裂開加工而需要照射脈寬較短之 短脈衝之雷射光。具體而言,需要使用脈寬為100 psec以 下之雷射光。例如,使用具有i㈣至%㈣左右之脈寬 之雷射光為佳。 另一方面,單位脈衝光之照射間距(被照射光點之中心 間隔)於4 μιη至50 μηι之範圍内設定即可。若照射間距大於 此,則會產生容易劈開/裂開之方向之弱強度部分之形成 無法進展至可形成劈理/解理面之程度之情形,因而自確 實地形成包含上述劈理/解理面之分割起點之觀點考慮欠 佳。再者’自掃描速度、加工效率及產品品質之方面考 慮,照射間距較大者為佳,但為更確實地形成劈理/解理 面,較為理想的是於4 μιη至30 μηι之範圍内設定,更佳為4 μηι至15 μπι左右。 當前,於雷射光之重複頻率為R(kHz)之情形時,按照 1/R(msec)自雷射光源發出單位脈衝光。於雷射光相對於被 加工物而相對性地以速度V(mm/sec)移動之情形時,照射 156646.doc •14- 201221261 間距Δ(μιη)以Δ^ν/R規定。因此’雷射光之掃描速度v與重 複頻率以△為數μιη左右之方式規定。例如,掃描速度乂為 50 mm/sec至3000 mm/sec左右,重複頻率尺為1 kHz至2〇〇 kHz’尤佳為10 kHz至200 kHz左右。V*R之具體值亦可 考慮被加工物之材質或吸收率、熱傳導率、熔點等而適當 地設定。 雷射光以約1 μπι至10 μϊη左右之光束直徑照射為佳。該 情形時,雷射光之照射之峰值功率密度為大致〇j TW/cm2 至數 10 TW/cm2。 又,雷射光之照射能量(脈衝能量)亦可於〇丨卜;至5〇 之範圍内適當規定。 圖2係藉由以第丨加工圖案進行之劈開/裂開加工而形成 有分割起點之被加工物之表面之光學顯微鏡圖像。具體而 言,表示以藍寶石C面基板作為被加工物,於其c面上進 行以al軸方向為預定加工線:之延伸方向而以7 之間隔 離散地形成被照射光點之加工之結果。圖2所示之結果暗 示實際上之被加工物以上述機制進行加工。 又,圖3係將藉由第丨加工圖案之加工而形成有分割起點 之藍寶石c面基板沿著該分割起點分割後之自表面(c面)至 〇J 面之 SEM(scanning electron microscope,掃描電子顯微 鏡)圖像。再者,圖3中,以虛線表示表面與剖面之邊界部 分。 圖3中觀察到之於自該表面起丨〇 左右之範圍内大致等 間隔地存在之、自被加工物之表面向内部具有長度方向之 156646.doc , ^ 201221261 細長之三角形狀或者針狀區域為藉由單位脈衝光之照射而 直接產生變質或飛散除去等現象之區域(以下稱作直接變 質區域)。而且’觀察到存在於該等直接變質區域之間 之、於自圖中觀察左右方向上具有長度方向之條紋狀部分 以亞微米間距於自圖中觀察上下方向連續有數個之區域為 劈理/解理面。較該等直接變質區域及劈理/解理面更靠下 方為藉由分割而形成之分割面。 形成有劈理/解理面之區域不為受到雷射光之照射之區 域’因此於該第1加工圖案之加工中,僅離散地形成之直 接變質區域成為加工痕。而且,直接變質區域於被加工面 上之尺寸只不過為數百nm至1 μιη左右。即’藉由以第i加 工圖案進行加工,與先前相比可實現分割起點之形成而又 較好地抑制加工痕之形成。 再者’ SEM圖像中作為條紋狀部分而觀察到者,實際上 為形成於劈理/解理面上之具有^ μηι至丨μιη左右之高低差 之微小凹凸。該凹凸係於以如藍寶石般之硬脆性之無機化 合物為對象進行劈開/裂開時,因藉由單位脈衝光之照射 而對被加工物作用較強之衝擊或應力所導致於特定結晶面 產生滑動所形成者。 雖然存在該微細凹凸’但根據圖3判斷出表面與剖面以 波、、文線部分為邊界大致正交,因此可說只要微細凹凸於作 為加工誤差而容許之範圍内,且藉由第丨加工圖案形成分 割起點,並沿著該分割起點對被加工物進行分割,則可= 對於其表面而大致垂直地分割被加工物。 156646.doc -16· 201221261 情形時。㈣上存在積極地形成該微細凹凸為佳之 龙磁 時亦可藉由第1加工圖案之加工,而於 '、程度上實現藉由下述之第2加工圖牵夕心 5 得之光提取效率之提高之效果。' 1而顯著獲 <第2加工圖案> 第加工圖案W、al轴方向、a2抽方向及 定加工線垂直之情形之劈開/裂開加工之形態。再= ^ 2加工一圖f令所使用之雷射光之條件與第】加工圖案相 Ί-般而言為相對於不同之2個容易劈開/裂開之方向 而等價之方向(成為2個容易劈開/裂開之方向之對稱轴之方 向)成為預定加工線之方向之情形之加工形態。 圖4係模式性地表示第2加工圖案之加工形態之圖。圖4 中例不al軸方向與預定加工線L正交之情形。圖4(句係表示 該情形之al輛方向、a2軸方向及“軸方向與預定加工線l 之方位關係之圖。圖4(b)表示雷射光之第丨脈衝之單位脈衝 光照射至預定加工線L端部之被照射區域R]E112狀態。 於第2加工圖案之情形時,亦與第j加工圖案相同地藉由 照射超短脈衝之單位脈衝光而形成弱強度部分。圖4(b) 中’以虛線箭頭模式性地表示形成於上述各容易劈開/裂 開之方向上之弱強度部分中,與預定加工線L之延伸方向 接近之-a2方向及+a3方向上之弱強度部分wi la、W12a。 而且’如圖4(c)所示,當照射雷射光之第2脈衝之單位脈 衝光而於預定加工線L上之自被照射區域re 11僅離開特定 距離之位置形成被照射區域RE12時,與第丨脈衝相同地, 156646.doc 17. 201221261 於該第2脈衝下亦形成有沿著容易劈開/裂開之方向之弱強 度部分。例如,於-a3方向形成弱強度部分Wllb,於+a2方 向形成弱強度部分W12b,於+a3方向形成弱強度部分 Wile,於-a2方向形成弱強度部分W12c。 該情形時,亦與第1加工圖案之情形相同地,藉由第1脈 衝之單位脈衝光之照射而形成之弱強度部分W1 la、W12a 分別處於弱強度部分W11 b、W12b之延伸方向,因此實際 上當進行第2脈衝之單位脈衝光之照射時,此時產生之衝 擊或應力會向容易劈開/裂開之方向及位於其前端之弱強 度部分傳播。即,如圖4(d)所示’形成劈理/解理面cila、 Cllb。再者’該情形時’劈理/解理面cna、Cllb亦可於 被加工物之自圖中觀察垂直方向上形成至數pm至數十μιη 左右之深度。 繼而’當如圖4(e)所示沿著預定加工線l掃描雷射光而 對被照射區域RE11、RE12、RE13、RE14...依序照射單位 脈衝光時,藉由該照射時所產生之衝擊或應力,沿著預定 加工線L依序形成自圖中觀察為直線狀之劈理/解理面cUa 及 Cllb、C12a 及 C12b、C13a 及 C13b、C14a 及 C14b...。 其結果,實現劈理/解理面相對於預定加工線[而位於對 稱位置之狀態。第2加工圖案中,沿著預定加工線L離散地 存在之複數個被照射區域,與該等鋸齒狀地存在之劈理/ 解理面整體上成為沿著預定加工線L分割被加工物時之分 割起點。 圖5係藉由第2加工圖案之劈開/裂開加工而形成有分割 156646.doc -18- 201221261 起點之被加工物之表面之光學顯微鏡圖像。具體而言,其 表示以藍寶石c面基板作為被加工物,於其c面上‘行以 與“轴方向正交之方向為預定加工線[之延伸方向且以7 μηι間隔離散地形成被照射光點《加工之結果。㈣圖5, 於貫際之被加工物中’亦與圖4(e)"莫式性地所示者相同 地確認出自正面觀察為鋸齒狀(鋸齒狀)之劈理/解理面。其 結果暗示實際之被加工物係以上述機制進行加工。 八 又’圖6為將藉由第2加工圖案之加工而形成有分割起點 之藍寶石C面基板沿著該分割起點進行分狀後之自表面 (C面)至剖面之SEM圖像。再者,圖6中以虛線表示表面與 刮面之邊界部分》 根據圖6,於分割後之被加工物之剖面之自表面起 左右之範圍内,確認出被加工物之剖面具有與圖4(幻中模 式性地表示之鋸齒狀配置對應之凹凸。形成該凹凸者為劈 理/解理面。再者,圖6中之凹凸之間距為5 μιη左右。與第 1加工圖案之加工情形相同地,劈理/解理面不平坦,伴隨 因單位脈衝光之照射以致於特定結晶面產生滑動而產生亞 微米間距之凹凸。 又,與该凹凸之凸部位置對應而自表面部分向深度方向 延伸者為直接變質區域之剖面。與藉由圖3所示之第1加工 圖案之加工而形成之直接變質區域相比,該形狀不均勻。 而且’較該等直接變質區域及劈理/解理面而更靠下方者 為藉由分割而形成之分割面。 於第2加工圖案之情形亦同’僅離散地形成之直接變質 .¾ 156646.doc 201221261 區域成為加工痕之方面與第1加工圖案相同。而且,直接 變質區域於被加工面中之尺寸不過為數百nm至2 μιη& 右。即,於以第2加工圖案進行加工之情形時,亦可實現 加工痕之形成好於先前之分割起點之形成。 於第2加工圖案之加工之情形時,除形成於劈理/解理面 之亞微米間距之凹凸以外,相鄰之劈理/解理面彼此以數 μιη左右之間距形成凹凸。形成具有該凹凸形狀之剖面之 形態於如下情形較為有效’即’將於包含藍寶石等硬脆性 且光學性透明之材料之基板上形成有led結構等發光元件 結構之被加工物,按晶片(分割原片)單位進行分割。於發 光元件之情形時,當於藉由雷射加工而形成於基板上之加 工痕之部位吸收發光元件内部所產生之光時,來自元件之 光提取效率降低,但於有意圖地藉由進行第丨加工圖案之 加工而於基板之加工剖面形成該圖6所示之凹凸之情形 時,於該位置之總反射率降低,於發光元件中實現更高之 光提取效率。 <第3加工圖案> 第3加工圖案於使用超短脈衝之雷射光之方面,及“軸 方向a2軸方向及a3轴方向均與預定加工線垂直(相對於 不同之2個容易劈開/裂開之方向而等價之方向成為預定加 工線之方向)之方面與第2加工圖案相同,但雷射光之照射 形態不同於第2加工圖案。 圖7係模式性地表示第3加工圖案之加工形態之圖。圖7 中例不&1軸方向與預定加工線L正交之情形。圖7(a)係表示 ]56646.doc -20- 201221261 該情形之al軸方向、a2軸方向及a3轴方向與預定加工線L 之方位關係之圖。 上述之第2加工圖案中,於與圖7(a)所示者相同之方位關 係下,沿著預定加工線L之延伸方向、即a2軸方向與a3軸 方向之正中間方向(相對於a2轴方向與a3轴方向而等價之 方向)直線性地掃描雷射光。第3加工圖案中,代替此,如 圖7(b)所示,以使各個被照射區域以交替地沿著夾持預定 加工線L之2個容易劈開/裂開之方向之形態呈鋸齒狀(鋸齒 狀)地形成之方式,照射形成各個被照射區域之單位脈衝 光。若為圖7之情形時,則交替地沿著-a2方向與+a3方向 而形成被照射區域RE21、RE22、RE23、RE24、RE25...。 於以該形態照射單位脈衝光之情形時,與第1加工圖案 及第2加工圖案相同地,亦伴隨各個單位脈衝光之照射而 於被照射區域之間形成劈理/解理面。若為圖7(b)所示之情 形,則藉由依序形成被照射區域RE21、RE22、RE23、 RE24、RE25...,而依序形成劈理/解理面C21、C22、 C23、C24...。 其結果,於第3加工圖案中,於以預定加工線L為軸之鋸 齒狀之配置令離散地存在之多個被照射區域,與形成於各 個被照射區域之間之劈理/解理面,整體上成為沿著預定 加工線L對被加工物進行分割時之分割起點。 而且,於實際上沿著該分割起點進行分割之情形時,與 第2加工圖案相同地於分割後之被加工物之剖面之自表面 起10 μιη左右之範圍内,形成有由劈理/解理面所引起之數 156646.doc •21 - 201221261 μπι間距之凹凸。而且,於各個劈理/解理面,與第!加工圖 案及第2加工圖案之情形相同地,伴隨因單位脈衝光之照 射所導致於特定結晶面產生滑動而產生亞微米間距之凹 凸又,直接變質區域之形成形態亦與第2加工圖案相 同。即,於第3加工圖案中,加工痕之形成亦被抑制於與 第2加工圖案為同程度。 因此,於該第3加工圖案之加工情形時,亦與第2圖案之 加工相同地,除形成於劈理/解理面之亞微米間距之凹凸 以外,藉由劈理/解理面彼此而形成數μιη&右之間距之凹 凸,因此於以發光元件為對象進行第3加工圖案之加工之 情形時,所獲得之發光元件自上述之光提取效率之提高之 觀點考慮更佳。 再者,根據被加工物之種類,為更確實地產生劈理/解 理,亦可於均為預定加工線L上之位置即圖7(b)之被照射 區域RE21與被照射區域RE22之中點、被照射區域RE22與 被照射區域RE23之中點、被照射區域RE23與被照射區域 RE24之中點、被照射區域RE24與被照射區域rE25之中 點…形成被照射區域。 且說,第3加工圖案中之被照射區域之配置位置部分地 沿著容易劈開/裂開之方向。於如上所述亦於預定加工線L 上之中點位置形成被照射區域之情形時亦相同。即,第3 加工圖案於被加工物之容易劈開/裂開之方向上相鄰形成 至少2個被照射區域之方面可設為與第1加工圖案共通。因 此’換言之’第3加工圖案亦可視作一面使掃描雷射光之 156646.doc -22· 201221261 方向週期性地不一致一面進行第i加工圖案之加工。 又,於第i加工圖案及第2加工圖案之情形時,被照射區 域位於-直線上,因此每次於使雷射光之出射源沿著'預: 加工線於-直線上移動而到達特定形成對象位置時照射: 位脈衝光而形成被照射區域即可,該形成形態最有效率早 然而,於第3加工圖案之情形時’不於一直線上而呈錄齒 狀(鋸齒狀)地形成被照射區域,因此不僅可用使雷射光 出射源實際上呈鋸齒狀(鋸齒狀)地移動之方法,亦可用之 種方法形成被照射區域。再者,本實施方各 、| 印射源之 移動係指被加工物與出射源之相對移動,不僅包含被加工 物固定而出射源移動之情形,亦包含出射源固定而被加I 物移動(實際上係載置被加工物之載台移動)之形態。 例如,m面使出射源與載台呈與預定加卫線平行地 以等速相對移動,-面使雷射光之出射方向於與預定加工 線垂直之面内呈週期性地變化等,亦可以滿足上述之鑛齒 狀配置關係之形態形成被照射區域。 或者’藉由-面使多個出射源平行地以等速相對移動, 面使來自各個出射源之單位脈衝光之照射時序呈週期性 地變化’亦可以滿足上述之鑛齒狀配置關係之形態形 照射區域❶ 一圖8係表示該等2個情形之預定加工線與被照射區域之預 定形成位置之關係之圖。於任一情形時,均可視作如圖8 所示’宛如將被照射區域RE21、re22 re23 re24、 RE25·.·之預定形成位置⑵、P22、P23 ' P24、p25…交替 156646.doc -23- 201221261 6X定於與預定加工線L平行之直線La、ίβ上,同時並行地 進行於沿著直線La之預定形成位置之P21、P23、P25...之 被照射區域之形成,與於沿著直線Lp之預定形成位置 P22、P24...之被照射區域之形成。 再者’於使出射源鋸齒狀(鋸齒狀)地移動之情形時,使 雷射光之出射源直接移動,或藉由使載置有被加工物之載 台移動而使雷射光相對性地掃描,出射源或者載台之移動 為二軸同時動作。相對於此,僅使出射源或者載台與預定 加工線平行地移動之動作為單軸動作。因此,於實現出射 源之高速移動即加工效率之提高之方面,後者更佳。 如以上之各加工圖案所示,於本實施方式中進行之劈開 /裂開加工’為將單位脈衝光之離散性之照射主要用作賦 予用以於被加工物上產生連續之劈理/解理之衝擊或應力 之機構之加工形態。被照射區域中之被加工物之變質(加 工痕之形成)或飛散等終歸只不過係附帶性地於局部產生 者。具有該特徵之本實施方式之劈開/裂開加工之機制, 於本質上不同於藉由一面使單位脈衝光之照射區域交疊一 面連續性地或者斷續性地產生變質、熔融、蒸發除去而進 行加工之先前之加工方法。 而且,對各個被照射區域瞬間性地施加較強之衝擊或應 力即可,因此可使雷射光一面以高速掃描一面進行照射。 具體而S ’可貫現最大為1000 mm/sec之極高速之掃描即 南速加工。雲於先前之加工方法之加工速度最大為200 mm/sec左右,該差異較為顯著。當然,可說本實施方式中 156646.doc -24· 201221261 所實現之加工方法與先前之加 〇 工方法相比顯著地提高生產 冉者,本實施方式中之劈開/裂 ..5、π 丄,於如上述之各 :工圖案般被加工物之結晶方位(容易劈開/裂開之方向之 方位)與預定加卫線處㈣定關係之情形時尤為有效,作 適用對象並不限定㈣等,於原理上亦可適用㈣者處於 =關係之ff形或被加马為多結晶體之情^於該等情 形時,相對於預定加玉線而產生劈理/解理之方向未必固 定;’因此雖會於分割起點產生不規則之凹凸,但藉由適當 地叹疋被照射區域之間、及以脈寬為代表之雷射光之照 射條件,可進行該凹凸停㈣加卫誤差之容許範圍内之於 只用上不存在問題之加工。 <刀離光束能®利用效率之向上> 本實施方式之劈開/裂開加工,為如上述般藉由以4 pm 至50 μηι左右之間隔離散地照射具有1〇〇 psec以下之脈寬之 單位脈衝光而於各個被照射區域之中心部分產生物質之變 質、熔融、蒸發除去等,從而使劈開/裂開進展至被照射 區域間之方法。因此,無須於被照射區域進行超過必要之 加工,當然需要使劈理/解理自被照射區域相對於容易劈 開/裂開之方向確實地進展。 例如’於照射峰值功率密度較大且脈寬較小之單位脈衝 光之情形時’施加至被照射區域之能量過剩而導致對被照 射區域造成超過必要之傷害,另一方面會引起劈理/解理 無法較佳地進展。其原因在於,照射之單位脈衝光之能量 156646.doc •25· 201221261 未充分地用於劈理/解理之進展。更詳細而言,可認為於 自電子系統之能量吸收向因該能量所引起之分子系統之振 動之遷移中需要10 psec左右之時間。目此,為使照射之單 位脈衝光之能量更多地用於劈理/解理之進展,可說一面 將峰值功率密度抑制於形成有弱強度部分之最低限度一面 將增大脈寬之單位脈衝光照射至被加工物之形態為佳。該 情形時’雷射光之能量利用效率提高。 本實施方式中,藉由如下方式實現該能量利用效率之提 高:將各個單位脈衝光於光學上暫時分為兩個部分,藉由 使兩者之光路長不同而使一者相對於另一者稍微(最多10 nsec左右)延遲,並且照射至被加工物上之實質上相同之被 照射區域。將該形態之加工稱作分離光束加工。以下,具 體地進行說明。 圖9係模式性地表示延遲時間不同之情形時之實際上照 射至被加工物之雷射光之強度分佈(光束強度之時間變化) 之變化之情況之圖。具體而言’考慮如圖9(a)所示將峰 值強度(峰值功率密度)1且半值寬ω之單位脈衝光UP分為分 佈均等之2個第1半脈衝光H1與第2半脈衝光H2,藉由使兩 者之光路長不同而使第2半脈衝光H2相對於第1半脈衝光 H1而延遲之情形。將延遲時間設為d。 首先’於例如圖9(b)所示之延遲時間D為單位脈衝光UP 之半值寬ω(數Psec至數十psec左右)之1/3左右之情形 (D=co/3之情形)般延遲時間〇比較小之情形時,於時間上交 豐而照射第1半脈衝光H1與第2半脈衝光H2,於外觀上兩 156646.doc ‘26- 201221261 者之合成脈衝光CP1作為峰值強度丨丨且半值寬…之單一單 位脈衝光而透過。然而,藉由相對於第i半脈衝光m而延 遲照射第2半脈衝光H2,而使第2半脈衝光H2照射至照射 第1半脈衝光H1引起物質產生變質進而開始產生劈理/解理 " 之能量吸收效率較高狀態(等離子狀態或高溫狀態)之被照 ' 射區域。此時,第2半脈衝光H2之能量主要用於劈理/解理 之進展。 當然,隨著增大延遲時間D,第1半脈衝光出與第2半脈 衝光H2之時間上之交疊變少。但如圖9(c)所示,若為延遲 時間D係與單位脈衝光!^!»之半值寬(〇同程度之情形時(〇=ω 之情形時)’第1半脈衝光HI與第2半脈衝光Η2之合成脈衝 光CP2具有較合成脈衝光cpi之峰值強度11更小之峰值強度 12之2個峰值。然而,於第2半脈衝光只2照射至照射第】半 脈衝光Η1而成為能量吸收效率較高之狀態之被照射區域之 方面,與照射合成脈衝光CP1之情形相同。再者,合成脈 衝光CP2整體上可視作半值寬ω2(>ω1)之單位脈衝光。 於使延遲時間D較ω更大而如圖9(d)所示為單位脈衝光 UP之半值寬ω之2倍左右之情形時(D=2〇)之情形時),第1半 - 脈衝光H1與第2半脈衝光Η2幾乎不存在交疊,合成脈衝光 CP3(名稱上如此稱呼)’實質上只不過為以延遲時間d依序 照射相當於第1半脈衝光出與第2半脈衝光112(即峰值強度 13大致為P/2)之2個個別之單位脈衝光UP3a、uP3b。 然而,該情形時之延遲時間D即便增大亦最多為1〇〇 pSeC左右,因此於藉由照射單位脈衝光UP3a而產生之能量 156646.doc 27· 201221261 吸收效率較高之狀態未消失之期間照射單位脈衝*up3b。 因此,單位脈衝光UP3b之能量用於劈理/解理面之進展。 即,該情形時,亦與實質上交疊於第丨半脈衝光1^與第2半 脈衝光H2之情形相同地,可有效率地利用自光源出射之單 位脈衝光UP之能量。 再者,本發明之發明者確認出若延遲時間D為大致 nsec之範圍,則可獲得提高上述之單位脈衝光upi能量利 用效率之效果。可認為其原因在於,維持藉由單位脈衝光 UP3 a之照射而實現之能量吸收效率較高之狀態之時間最多 為lOnsec左右。又,於延遲時間D低於ω/3之情形時,無法 充分獲得使第2半脈衝光Η2延遲之效果,被加工物1〇易於 受到過多之傷害,因而欠佳。 根據以上内容,若以作為10 nsec以下之範圍内之值規定 延遲時間D之方式設定第1半脈衝光出與第2半脈衝光H22 光路長差,則即便於自光源出射之單位脈衝光具有會對被 照射區域造成過多傷害之程度之峰值功率密度之情形時, 亦可使實際上照射至被加工物之單位脈衝光之峰值強度降 低,且可實質上使照射時間增大,從而可針對各個單位脈 衝光提高用於劈理/解理之進展之能量之比率。具體而 s ’可將延遲照射之第2半脈衝光H2之能量主要用於劈理/ 解理之進展。即’若以延遲時間D滿足該範圍之方式設定 第1半脈衝光H1與第2半脈衝光H2之光路長差而進行分離 光束加工,則可貫現進一步提高能量利用效率之劈開/裂 156646.doc •28- 201221261 開加工。由此,可更有效率地且確實地對被加工物10形成 分割起點。 且說,至此為止說明之分離光束加工係一面使第2半脈 衝光Η2較第1半脈衝光Η1而於時間上延遲,一面使兩者照 射至實質上相同之被照射區域,但另一方面,本實施方式 中如上所述,一面以50 mm/sec至3000 mm/sec左右之掃描 速度相對性地掃描雷射光一面進行加工。乍一看兩者似自 相矛盾。其原因在於’於照射第1半脈衝光H1之後至照射 第2半脈衝光H2為止之期間’雷射光與被加工物丨〇亦相對 移動,因此各個半脈衝光之被照射區域之形成位置應有不 同。然而,即便設定例如雷射光之掃描速度為3〇〇〇 mm/sec(=3 m/sec)且延遲時間d為1〇 nsec之、第1半脈衝光 H1之照射位置與第2半脈衝光H2之照射位置最為偏離之情 形時,兩位置之計算上之偏離亦只不過為3〇 ηιη❶另一方 面,雷射光之光束直彳空為約1 μιη至丨〇 μπ1左右,或於劈開/ 裂開加工時形成於被加工物1〇上之被照射區域彼此之間隔 為4 μιη至50 μιη。30 nm之值為該等之約1/1〇〇至1/1〇〇〇左 右,可視作充分處於誤差範圍内。因此於進行加工時即便 第1半脈衝光H1與第2半脈衝光H2M射至實質上相同之被 照射區域亦無妨。 又,分離光束加工於進行上述第丨加工圖案至第3加工圖 案之任一者之加工之情形時均可執行。 再者,至此為止之說明中,以第1半脈衝光H1與第2半脈 衝光H2具有均等分佈之情況為前提進行說明但此非必需S 156646.doc 201221261 V/R becomes the center interval of the beam spot, but in the technique disclosed in Patent Document 2 and Patent Document 2, laser light is irradiated and scanned under the condition that V/R is 1 or less to make the beam. Points overlap each other. Further, Patent Document 3 discloses a mode in which a modified region is formed inside a substrate by irradiating laser light to a focused spot on a substrate having a laminated portion on the surface thereof, and the modified region is a cutting starting point. Further, Patent Document 4 discloses a method in which a laser beam scanning is repeated a plurality of times for one separation line, and a groove portion and a reforming portion which are continuous in the direction of the separation line in the depth direction are formed, and are discontinuous in the direction of the separation line. Internal reform department. On the other hand, Patent Document 5 discloses a configuration in which laser light is processed using an ultrashort pulse having a pulse width of psec, and the workpiece (plate body) is adjusted by adjusting the position of the focused spot of the pulsed laser light. From the surface layer portion to the surface, minute melting traces of minute cracks are formed in a group to form a separation facilitating region in which the melting traces are connected in a line shape. [PRIOR ART DOCUMENT] [Patent Document 1] Japanese Patent Laid-Open Publication No. Hei. No. Hei. No. 2006-139. [Patent Document 4] Japanese Patent Laid-Open Publication No. 2008-98465 [Patent Document 5] Japanese Patent Laid-Open Publication No. Hei No. 2005-271563 [Summary of the Invention] [Problems to be Solved by the Invention] 156646.doc 201221261 Segmentation by laser light The starting point and the subsequent division by the cutter are advantageous in terms of autonomy, high speed, stability, and high precision as compared with the diamond dicing which is a mechanical cutting method which has been performed before. However, in the case where the starting point of the division is formed by the laser light by the prior method, π can be avoided to form a so-called processing mark (laser processing mark). The term "processing mark" refers to a metamorphic region in which the material or structure changes as compared with that before irradiation. The formation of the processing marks usually adversely affects the characteristics of the divided workpieces (the original sheets), and is preferably suppressed as much as possible. For example, in the prior laser processing disclosed in Patent Document 2, a light-emitting element having an LED (llght emitting diode) structure or the like is formed on a substrate including a hard brittle and optically transparent material such as sapphire. The edge portion of the light-emitting element (the portion irradiated by the laser light at the time of division) which is divided by the wafer unit is added, and the processing is performed continuously with a width of about μηη and a depth of about μηη to several tens of μηη. mark. Therefore, there is a problem in that the processing mark absorbs light generated inside the light-emitting element, resulting in a decrease in light extraction efficiency from the element. This problem is particularly remarkable in the case of using a light-emitting element structure of a sapphire substrate having a high refractive index. As a result of active research, the inventors of the present invention have obtained the knowledge that when the workpiece is irradiated with laser light to form a starting point of the division, the rationality or ambiguity of the workpiece can be utilized, thereby suppressing it well. The formation of processing marks. Further, it is obtained that the use of ultrashort pulsed laser light in the processing is preferred. In Patent Document 1 to Patent Document 5, there is no disclosure or suggestion that the form of the starting point of the division is formed by the rationality or ambiguity of the object added to the 156646.doc 201221261. The present invention has been made in view of the above problems, and an object thereof is to provide a method for processing a divided body capable of suppressing formation of a processing mark and forming a dividing starting point for more reliably achieving division of a workpiece, and Laser processing equipment used. [Technical means for solving the problem] In order to solve the above problems, the invention provides a laser processing apparatus characterized by comprising: a light source that emits pulsed laser light; and a stage on which the workpiece is placed; The pulsed laser light has an ultrashort pulse light having a pulse width of ^%, and the optical path of the pulsed laser light from the light source to the stage is partially branched into a second optical path and a second optical path in the middle and then merged. The laser processing apparatus further includes an optical path length adjusting mechanism that changes an optical path length of the second optical path; and the pulsed laser light defined as being emitted from the light source branches into a first thunder that advances in the first optical path And projecting the second laser light that is advanced in the second optical path, and the unit pulse light of the pulsed laser light is branched into a unit pulse of the first half pulse light and the second laser light When the light is the second half-pulse light, the optical path length adjusting means is configured to delay the second half-pulse light by the ith half-pulse light in the optical path after the merging The light path length of the second optical path is such that the pulsed light is transmitted to the workpiece while the workpiece is being placed on the stage, and the pulsed light is transmitted to the workpiece The first half pulse light of each unit pulse light and the second half pulse light are irradiated on the processed surface of the workpiece, and are processed on the processed surface of the processed object 156646.doc 201221261 The above-described irradiated regions of the respective unit pulse lights are discretely formed. The invention of the technical solution 2 is as a technical solution! In the laser processing apparatus, the optical path length adjusting mechanism delays the second half pulse light by only 1/3 times the half value width of the unit pulse light with respect to the third half pulse light, and a delay of 1 〇-down The mode of time is longer than the optical path of the second optical path. The invention of claim 2 is the laser processing apparatus according to claim 2, further comprising: a strength adjustment mechanism for adjusting the intensity of the second laser light; and the optical path length adjustment mechanism for causing the second half pulse light to be relative to the first The half pulse light sets the optical path length of the second optical path only by delaying the delay time of the half value width of the unit pulse light by more than 丨 and twice or less; and the intensity adjusting mechanism makes the intensity of the second laser light smaller than The intensity of the second laser light is adjusted in such a manner as to increase the intensity of the first laser light. The invention of claim 4 is the laser processing apparatus according to claim 2, further comprising: a focus adjustment mechanism for adjusting a focus of the second laser light; and the optical path length adjustment mechanism for causing the second half pulse light to be relative to the first The half pulse light sets the optical path length of the second optical path such that the delay time of the half value width of the unit pulse light is delayed by more than 丨 and twice or less; and the focus adjustment mechanism causes the beam diameter of the second laser light The focus of the second laser light is adjusted in a manner larger than the beam diameter of the laser light. The invention of claim 5 is a processing method for forming a starting point of the workpiece, wherein the optical path setting step includes a light source of the pulsed laser light having an ultrashort pulse of light having a pulse width of psec. The optical path of the stage of the processing object is set to be halved to the optical path and the second optical path and merged thereafter; the optical path length adjusting step is defined as the pulsed laser branch of the pulse emitted from the light source. In the above-mentioned (the i-th laser light that advances in the optical path and the second laser light that advances in the second optical path, and the unit pulse light of the pulsed laser light is branched into the unit pulse light of the second laser light, that is, the i-th The half-pulse light and the second half-pulse light of the unit laser light of the second laser light are set to set an optical path length of the second optical path such that the second half-pulse light is delayed more than the first half-pulse light; a placing step of placing the workpiece on the stage; and an irradiation step of irradiating the second half pulse light and the second half pulse light of each unit pulse light The region is the same, and the pulsed region of the unit pulse light is discretely formed on the surface to be processed of the workpiece, and the pulsed laser light is irradiated onto the workpiece to be irradiated The above-mentioned workpiece is processed or cleaved between the regions to form a starting point for the division of the workpiece. The invention of claim 6 is a method for processing a workpiece according to claim 5 In the optical path length adjustment step, the above-described second half-pulse light is set to be delayed by only 1/3 times or more and twice or less the half-value width of the unit pulse light with respect to the first half-pulse light. The invention is the method of processing the workpiece according to the sixth aspect of the invention, wherein the method further includes the step of adjusting the intensity of the second laser light; and the step of adjusting the optical path length The second half-pulse light is delayed by only one time or more and two times or less the half value width of the unit pulse light with respect to the first half pulse light by 156646.doc 201221261. The optical path length of the second optical path is set in a delay time manner, and the intensity of the second laser light is adjusted so that the intensity of the second laser light is smaller than the intensity of the second laser light in the intensity adjustment step. The invention of claim 8 is the method for processing a workpiece according to claim 6, wherein the towel further includes a focus adjustment step of adjusting a focus of the second light #光; in the optical path length adjustment step, the second half pulse is The light path length of the second optical path is set so that the first half-pulse light is delayed by one time or more and two times or less the half-value width of the unit pulse light, and the focus adjustment step is performed. The focus of the second laser light is adjusted such that the beam diameter of the second laser beam is larger than the beam diameter of the second laser beam. The invention of claim 9 is the method for processing a workpiece according to any one of claims 5 to 8, wherein the above-mentioned workpiece is formed adjacent to each other in a direction in which it is easy to open or split, and the above is different. At least two illuminated regions formed by unit pulsed light. The invention of claim 10 is the method for processing a workpiece according to claim 9, wherein all of the irradiated regions are formed along a direction in which the workpiece is easily split or split. The invention of claim 11 is the method for processing a workpiece according to claim 9, wherein the formation of the at least two irradiated regions is alternately performed in two directions in which the workpiece is different from the above-mentioned workpiece. The invention of claim 12 is the method for processing a workpiece according to any one of claims 5 to 8, wherein the irradiation is performed in a direction equivalent to the difference of the above-mentioned workpiece = 156646.doc 201221261 An area that is easy to open or split. The invention of claim 13 is a method of dividing a workpiece, and the workpiece having the division starting point formed by the method of the fifth aspect of the invention is divided along the division starting point. [Effects of the Invention] According to the inventions of the first to thirteenth aspects, the formation of the processing marks or the scattering of the workpiece due to the deterioration of the workpiece can be limited to a local phenomenon, and the other can be actively The workpiece is subjected to cleavage or cleavage to form a starting point of the workpiece at a very high speed compared to the prior art. In particular, according to the inventions of claims 2 to 4 and 6 to 8, the energy utilization efficiency of the pulsed laser light is improved, so that the division can be performed more efficiently and surely. <Principle of Processing> The principle of processing realized in the embodiment of the present invention shown below will be described. The processing performed in the present invention is roughly as follows: scanning pulsed laser light (hereinafter also referred to simply as laser light) to irradiate the pulsed laser light onto the upper surface (processed surface) of the workpiece, Thereby, the workpiece is sequentially processed or cleaved between the irradiated regions of the respective pulses, and the starting point for the division is formed as the continuous surface of the cleavage plane or the cleavage plane formed on each of the pulses ( Split the starting point). Further, in the present embodiment, the cleavage means that the workpiece is substantially regularly broken along the crystal plane other than the cleavage plane, and the crystal surface is called cleavage 156646.doc •10·201221261 In addition to the microscopic phenomenon of the microscopic phenomenon, the cleavage of the nucleus is completely along the surface of the crystal. Depending on the substance, there are also only those that are mainly responsible for philosophical, cleavage, or cracking—to 71 pairs of 劈 “to avoid the cumbersome explanations and the cleavage and the cracks are not treated separately as cleavage/cleavage, etc.: 'The processing of the above-described form is sometimes referred to simply as splitting/cracking processing, etc. Hereinafter, the workpiece is a hexagonal single crystal material, and the U-axis 'U: and the axis of the a3 axis are easy. The case of the direction of splitting/cracking is exemplified. For example, the c-plane sapphire substrate or the like conforms to this. The ai axis, the a2 axis, and the a3 axis of the hexagonal crystal are mutually symmetrical at an angle of 12 于 in the c-plane. In the processing of the present invention, there are several patterns depending on the relationship between the direction of the equiaxions and the direction of the predetermined processing line (predetermined processing direction). Hereinafter, the pattern such as the hai will be described. The laser light that is pulsed and irradiated is called unit pulse light. <First Processing Pattern> The first processing pattern is a form in which the i-axis direction, the a2-axis direction, and the a3-axis direction are parallel to the pre-twisting line. More generally, it is a processing form in which the direction of easy splitting/cracking is consistent with the direction of the predetermined processing line. Fig. 1 is a view schematically showing a processing form of a second processing pattern. In the case of Fig. i, the case where the axis of the al axis is not parallel to the predetermined processing line L is exemplified. Fig. 1(a) is a view showing the relationship between the a-axis direction, the a2-axis direction, and the a3-axis direction in the case of a predetermined processing line. Fig. 1(b) shows a unit pulse of the first pulse of the laser light 156646.doc 201221261 A state in which the light is irradiated to the irradiated region re丨 at the end of the predetermined processing line L. In general, the irradiation of the unit pulsed light applies a higher energy to the extremely small area of the workpiece. Therefore, the irradiation causes the irradiated area corresponding to the unit pulse light (laser light) of the illuminated surface or is more The deterioration, melting, evaporation, and the like of the substance are generated within a wide range of the irradiation area. However, when the irradiation time of the unit pulsed light, that is, the pulse width is set to be extremely short, the substance in the substantially central region of the irradiated area RE1 which is narrower than the spot size of the laser light obtains the kinetic energy from the irradiated laser light and the plasma The temperature is changed to a gas state or the like, and is further pulverized in a direction perpendicular to the surface to be irradiated. On the other hand, the impact generated by the irradiation of the unit pulse light represented by the reaction force generated by the scattering or The stress acts on the periphery of the irradiated region, and particularly acts in the a-axis direction, the a2-axis direction, and the a3-axis direction which are directions which are easy to open/split. Thereby, the contact state is maintained in the direction in the direction but partially generates minute cleavage or cleavage' or a state in which thermal deformation is caused but does not cause cleavage or cleavage. In other words, it can be said that the irradiation of the unit pulse light of the ultrashort pulse functions as a driving force for forming a weak portion having a substantially linear shape in a plan view in a direction in which the opening/cleaving is easy. In FIG. 1(b), a weak intensity portion in the +al direction which coincides with the direction in which the predetermined processing line L extends is schematically indicated by a broken line arrow in a weak intensity portion formed in each of the above-described easy splitting/cracking directions. . Then, when the unit pulse light of the second pulse of the laser light is irradiated as shown in FIG. 1(c), the irradiated region r1 is formed at a position on the predetermined processing line L from the irradiated region RE1 only by a certain distance, and Similarly to the 1 pulse, a weak intensity portion along the direction of easy splitting/cracking is also formed under the second pulse of 156646.doc 12 201221261. For example, a weak intensity portion W2a is formed in the _al direction, and a weak intensity portion W2b is formed in the +ai direction. However, at this point of time, the weak intensity portion formed by the irradiation of the unit pulse light of the first pulse is in the extending direction of the weak intensity portion W2a. That is, the direction in which the weak-strength portion W2a extends is a portion where energy can be generated or cleaved (high energy absorption rate) smaller than other portions. Therefore, in actuality, when the unit pulse light of the second pulse is irradiated, the impact or stress generated at this time is propagated in the direction of easy splitting/cleaving and the weak intensity portion at the tip end thereof, which is substantially weak at the moment of irradiation. The intensity portion W2a to the weak intensity portion wi produces a thorough cleavage or cleavage. Thereby, the cleavage/cleavage plane C1 which is not shown in Fig. i(d) is formed. Further, the texture/cleavage plane C1 can be formed to a depth of about 4,111 to several tens of μηη in the direction perpendicular to the self-image of the workpiece. Further, as described above, on the cleavage/cleavage plane C1, slippage occurs on the crystal plane as a result of strong impact or stress, and undulation occurs in the depth direction. Then, when the irradiated areas RE1, RE2, RE3, RE4, .. are sequentially irradiated with the unit pulse light by scanning the laser light along the predetermined processing line L as shown in FIG. 1(e), 'corresponding to this The cleavage/cleavage planes C2, C3 — are formed in sequence. In this form, the cleavage/cleavage plane is continuously formed into a split/cleavage process of the first processed pattern. It can be said from other viewpoints that the surface layer portion of the workpiece is expanded by applying heat energy by irradiating the unit pulse light, and the larger central region of each of the irradiated regions RE1, RE2, RE3, RE4, ... Outside 156646.doc -13- 201221261 Side effects and cleavage / cleavage to promote splitting / splitting. C2. · Vertical tensile stress, in the multiplexed pattern, the ',,,, and regions are discretely disposed along the predetermined processing line 1 and the cleavage/cleavage plane formed between the plurality of illuminated regions When the total processing is performed, the predetermined processing line L divides the workpiece into 1 and also Iβ 35°. After forming the starting point of the division, the division is performed using a specific division, and the processing line L can be substantially along the line L. The form divides the workpiece. In order to realize the splitting/cracking process, it is necessary to irradiate a short pulse of laser light having a short pulse width. Specifically, it is necessary to use laser light having a pulse width of 100 psec or less. For example, it is preferable to use laser light having a pulse width of about i (four) to about (four). On the other hand, the irradiation pitch of the unit pulse light (the center interval of the irradiated spot) may be set within a range of 4 μm to 50 μm. If the irradiation pitch is larger than this, the formation of the weak strength portion in the direction in which the splitting/cleaving is easy to occur cannot progress to the extent that the cleavage/cleavage plane can be formed, and thus the self-contained cleavage/cleavage is formed. The viewpoint of the starting point of the segmentation is not considered well. Furthermore, in terms of scanning speed, processing efficiency and product quality, it is preferable that the irradiation distance is larger, but in order to form the cleavage/cleavage surface more reliably, it is preferable to be in the range of 4 μm to 30 μm. The setting is preferably from 4 μηι to 15 μπι. Currently, when the repetition frequency of the laser light is R (kHz), unit pulse light is emitted from the laser light source at 1/R (msec). When the laser light is relatively moved at a speed V (mm/sec) with respect to the workpiece, the irradiation 156646.doc • 14 - 201221261 The pitch Δ (μιη) is defined by Δ^ν/R. Therefore, the scanning speed v of the laser light and the repetition frequency are defined in such a manner that Δ is several μηη. For example, the scanning speed 乂 is about 50 mm/sec to 3000 mm/sec, and the repetition rate is from 1 kHz to 2 kHz kHz, preferably from about 10 kHz to about 200 kHz. The specific value of V*R can also be appropriately set in consideration of the material, absorption rate, thermal conductivity, melting point, and the like of the workpiece. The laser light is preferably irradiated with a beam diameter of about 1 μm to 10 μϊη. In this case, the peak power density of the laser light irradiation is approximately 〇j TW/cm2 to several 10 TW/cm2. Further, the irradiation energy (pulse energy) of the laser light can also be appropriately determined within the range of 5 〇. Fig. 2 is an optical microscope image of the surface of the workpiece having the division starting point formed by the splitting/cracking process by the second processing pattern. Specifically, the sapphire C-plane substrate is used as a workpiece, and the result of the processing of the irradiated spot is discretely formed at intervals of 7 with the a-axis direction being the extending direction of the predetermined processing line on the c-plane. The results shown in Fig. 2 indicate that the actual workpiece is processed by the above mechanism. Moreover, FIG. 3 is a SEM (scanning electron microscope) from the surface (c surface) to the 〇J plane of the sapphire c-plane substrate having the division starting point formed by the processing of the second processing pattern along the division starting point. Electron microscope) image. Further, in Fig. 3, the boundary portion between the surface and the cross section is indicated by a broken line. 3, 156646.doc, ^ 201221261 elongated triangular shape or needle-like region is observed from the surface of the workpiece to the inside at substantially equal intervals in the range from the left and right sides of the surface. It is a region (hereinafter referred to as a direct metamorphic region) in which a phenomenon such as deterioration or scattering is directly caused by irradiation of a unit pulsed light. Moreover, it is observed that a stripe-shaped portion having a longitudinal direction in the left-right direction observed between the direct metamorphic regions is observed at a submicron pitch in a plurality of regions viewed from the upper and lower directions in the drawing. Cleavage face. The lower part of the direct metamorphic area and the cleavage/cleavage plane are the split planes formed by the division. The region where the cleavage/cleavage plane is formed is not the region irradiated with the laser light. Therefore, in the processing of the first processing pattern, only the directly deformed regions which are discretely formed become the processing marks. Moreover, the size of the directly deteriorated region on the surface to be processed is only about several hundred nm to 1 μmη. Namely, by performing the processing in the i-th processing pattern, the formation of the division starting point can be realized as compared with the prior art, and the formation of the processing marks can be preferably suppressed. Further, as observed in the SEM image as a stripe portion, it is actually a micro unevenness having a height difference of about ηηι to 丨μιη formed on the cleavage/cleavage surface. When the embossing is caused by an inorganic compound such as sapphire hard and brittle, the impact or stress caused by the irradiation of the unit pulse light on the workpiece is caused by the specific crystal plane. The person formed by the slide. According to FIG. 3, it is determined that the surface and the cross section are substantially orthogonal to each other by the wave and the line portion. Therefore, it can be said that the fine unevenness is within the allowable range as a machining error, and the second processing is performed. When the pattern forms the starting point of the division and divides the workpiece along the starting point of the division, the workpiece can be divided substantially vertically with respect to the surface. 156646.doc -16· 201221261 Situation. (4) When there is a positive magnetism to form the fine concavities and convexities, the first processing pattern can be processed, and the light extraction efficiency obtained by the second processing pattern described below can be achieved to the extent that The effect of improvement. '1 and significantly <Second processing pattern> The shape of the first processing pattern W, the a-axis direction, the a2 drawing direction, and the fixed processing line are perpendicular to the split/split processing. Then = ^ 2 processing a picture f to make the conditions of the laser light used in contrast with the first] processing pattern - generally equivalent to the direction of the two different easy to open / split directions (to become 2 The direction in which the direction of the axis of symmetry of the direction in which the splitting is easy to open/break is the processing direction of the predetermined processing line. Fig. 4 is a view schematically showing a processing form of the second processing pattern. In Fig. 4, the case where the direction of the a-axis is not orthogonal to the predetermined processing line L is exemplified. Fig. 4 (sentence diagram shows the direction of the ag direction, the direction of the a2 axis, and the relationship between the direction of the axis and the orientation of the predetermined processing line l in Fig. 4. Fig. 4(b) shows the unit pulse light of the third pulse of the laser light irradiated to the predetermined In the case of the second processing pattern, in the case of the second processing pattern, the weak intensity portion is formed by irradiating the unit pulse light of the ultrashort pulse as in the jth processing pattern. b) in the 'dash arrow' schematically indicates the weak intensity in the -a2 direction and the +a3 direction which are formed in the weak intensity portion in the direction of the above-mentioned easy splitting/cracking, which is close to the extending direction of the predetermined processing line L. a portion of wi la, W12a. Further, as shown in FIG. 4(c), when the unit pulse light of the second pulse of the laser light is irradiated, a position on the predetermined processing line L from the irradiated region re 11 is separated by a specific distance. In the irradiated area RE12, similarly to the second pulse, 156646.doc 17. 201221261 also forms a weak intensity portion along the direction of easy splitting/cleaving under the second pulse. For example, weakly formed in the -a3 direction. The strength portion Wllb forms weak in the +a2 direction The portion W12b forms a weak intensity portion Tile in the +a3 direction and a weak intensity portion W12c in the -a2 direction. In this case, as in the case of the first processing pattern, the unit pulse light of the first pulse is irradiated. The formed weak strength portions W1 la, W12a are respectively in the extending direction of the weak intensity portions W11 b, W12b, so that when the unit pulse light of the second pulse is irradiated, the impact or stress generated at this time is easily split/cracked. The direction of the opening and the weak intensity portion at the front end propagate, that is, as shown in Fig. 4(d), 'the cleavage/cleavage planes cila, Cllb are formed. Further, in this case, the cleavage/cleavage plane cna, Cllb can also be formed in the vertical direction of the workpiece to a depth of several pm to several tens of μm. Then, when scanning the laser light along the predetermined processing line l as shown in Fig. 4(e), When the irradiation areas RE11, RE12, RE13, and RE14 are sequentially irradiated with the unit pulse light, the impact or stress generated during the irradiation is sequentially formed along the predetermined processing line L as a straight line viewed from the drawing. / cleavage plane cUa and Cllb, C12a and C12b, C 13a and C13b, C14a, and C14b.... As a result, the state in which the cleavage/cleavage plane is located at a symmetrical position with respect to the predetermined processing line is realized. In the second processing pattern, the plural number exists discretely along the predetermined processing line L. The area to be irradiated is the starting point of the division when the workpiece is divided along the predetermined processing line L as a whole, and the processing/disintegration surface existing in the zigzag shape is as shown in Fig. 5. Fig. 5 is the opening/split by the second processing pattern An optical microscope image of the surface of the workpiece having the starting point of 156646.doc -18-201221261 is formed by machining. Specifically, it indicates that a sapphire c-plane substrate is used as a workpiece, and a row is formed on the c-plane by a direction orthogonal to the axial direction as a predetermined processing line [the extending direction and discretely formed at intervals of 7 μm. The light spot "The result of the processing. (4) Fig. 5, in the workpiece to be processed in the same way as in the figure 4(e)", as shown in the figure, it is confirmed that it is jagged (serrated) from the front. The result is that the actual workpiece is processed by the above mechanism. [8] FIG. 6 is a sapphire C-plane substrate having a division starting point formed by processing the second processing pattern. The SEM image from the surface (C surface) to the cross section after the splitting start point is divided. Further, the boundary portion between the surface and the scraping surface is indicated by a broken line in Fig. 6. According to Fig. 6, the cross section of the workpiece after the division In the range from the surface to the left and right, it is confirmed that the cross section of the workpiece has the unevenness corresponding to the zigzag arrangement schematically shown in Fig. 4, and the irregularities are formed as the cleavage/cleavage plane. The distance between the bumps in Fig. 6 is about 5 μηη. In the same manner as in the processing of the pattern, the cleavage/cleavage plane is not flat, and the specific crystal plane is slid by the irradiation of the unit pulsed light, and the unevenness of the submicron pitch is generated. The surface extending from the surface portion in the depth direction is a cross section of the direct metamorphic region, and the shape is uneven compared to the direct metamorphic region formed by the processing of the first processing pattern shown in Fig. 3. Moreover, 'these are directly deteriorated. The area and the cleavage/cleavage plane are lower than the split surface formed by the division. The case of the second processing pattern is also the same as the direct deterioration of the discrete formation. 3⁄4 156646.doc 201221261 The area becomes the processing mark The aspect is the same as that of the first processing pattern. Moreover, the size of the directly deteriorated region in the surface to be processed is only several hundred nm to 2 μm and the right side, that is, when processing is performed in the second processing pattern, processing can also be realized. The formation of the mark is better than the formation of the previous starting point of the segmentation. In the case of the processing of the second processed pattern, except for the unevenness of the submicron pitch formed on the cleavage/cleavage plane, adjacent The texture/cleavage planes are formed with irregularities at a distance of about several μm. The form of the cross section having the uneven shape is effective in the case where it is to be on a substrate containing a hard brittle and optically transparent material such as sapphire. The object to be processed having the structure of a light-emitting element such as a led structure is divided into units of a wafer (divided original piece). In the case of a light-emitting element, light is absorbed at a portion of a processing mark formed on the substrate by laser processing. When the light generated inside the element is light, the light extraction efficiency from the element is lowered, but when the concave and convex portions shown in FIG. 6 are formed on the processed cross section of the substrate by intentionally processing the second processing pattern, The total reflectance of the position is lowered to achieve higher light extraction efficiency in the light-emitting element. <Third processing pattern> The third processing pattern is perpendicular to the predetermined processing line in terms of the use of the ultrashort pulse laser light, and the "axis direction a2 axis direction and the a3 axis direction are both perpendicular to the predetermined processing line (the two are easy to open with respect to each other) The direction in which the direction of the split is equivalent to the direction of the predetermined processing line is the same as that of the second processed pattern, but the irradiation form of the laser light is different from the second processed pattern. FIG. 7 schematically shows the third processed pattern. Fig. 7 is a case where the direction of the &1 axis is orthogonal to the predetermined processing line L. Fig. 7(a) shows]56646.doc -20- 201221261 The a-axis direction and the a2-axis direction of the case And a view of the azimuthal relationship between the a3 axis direction and the predetermined processing line L. In the second processing pattern described above, in the same orientation relationship as that shown in Fig. 7(a), along the extending direction of the predetermined processing line L, The a2 axis direction and the a3 axis direction are in the middle direction (the direction equivalent to the a3 axis direction and the a3 axis direction), and the laser light is linearly scanned. In the third processing pattern, instead of this, as shown in FIG. 7(b) So that each of the illuminated areas is alternately processed along the clamping The two directions of the L-opening/cleaving direction are formed in a zigzag (zigzag) manner, and the unit pulse light forming each of the irradiated regions is irradiated. If the case of Fig. 7 is used, the alternately along - In the a2 direction and the +a3 direction, the irradiated regions RE21, RE22, RE23, RE24, RE25, ... are formed. When the unit pulse light is irradiated in this manner, similarly to the first processed pattern and the second processed pattern, The cleavage/cleavage plane is formed between the irradiated regions with the irradiation of the respective unit pulsed light. If it is the case shown in Fig. 7(b), the irradiated regions RE21, RE22, RE23, RE24 are sequentially formed. RE25..., and the cleavage/cleavage planes C21, C22, C23, C24, ... are sequentially formed. As a result, in the third processing pattern, a zigzag arrangement with the predetermined processing line L as an axis is used. The plurality of irradiated regions which are discretely present and the texture/cleavage plane formed between the respective irradiated regions are the starting points of the division when the workpiece is divided along the predetermined processing line L as a whole. Actually, when dividing along the starting point of the segmentation, and the second The work pattern is similarly formed in a range of about 10 μm from the surface of the cross-section of the workpiece to be processed, and the unevenness of the number of 156646.doc •21 - 201221261 μπι caused by the cleavage/cleavage plane is formed. In the same manner as in the case of the second processing pattern and the second processing pattern, the respective processing/cleavage planes are caused by the sliding of the specific crystal plane due to the irradiation of the unit pulsed light, and the submicron pitch unevenness is directly generated. The formation form of the metamorphic region is also the same as that of the second processing pattern. That is, in the third processing pattern, the formation of the processing marks is also suppressed to the same extent as the second processing pattern. Therefore, in the case of processing the third processed pattern, in addition to the processing of the second pattern, in addition to the unevenness formed on the submicron pitch of the cleavage/cleavage surface, the cleavage/cleavage planes are mutually In the case where the third processing pattern is processed for the light-emitting element, the obtained light-emitting element is more preferable from the viewpoint of improving the light extraction efficiency described above. Further, depending on the type of the workpiece, it is possible to produce the cleavage/cleavage more reliably, or the position on the predetermined processing line L, that is, the irradiated area RE21 and the irradiated area RE22 of Fig. 7(b). The midpoint, the midpoint of the irradiated area RE22 and the irradiated area RE23, the point of the irradiated area RE23 and the irradiated area RE24, and the point of the irradiated area RE24 and the irradiated area rE25 form an illuminated area. Further, it is said that the arrangement position of the irradiated area in the third processing pattern is partially along the direction in which the opening/cleaving is easy. The same applies to the case where the irradiated area is formed at the midpoint position on the predetermined processing line L as described above. In other words, the third processing pattern can be formed to be common to the first processed pattern in that at least two of the irradiated regions are adjacently formed in the direction in which the workpiece is easily split/cleared. Therefore, the 'in other words' third processing pattern can also be regarded as processing the i-th processing pattern while periodically omitting the direction of the scanning laser light 156646.doc -22· 201221261. Further, in the case of the i-th processing pattern and the second processing pattern, the irradiated area is located on a straight line, so that the emission source of the laser light is moved along the 'pre-processing line on the straight line every time to reach a specific formation. Irradiation at the position of the object: It is only necessary to form the irradiated area by the pulsed light. This formation form is most effective early. However, in the case of the third processing pattern, it is formed in a recorded shape (zigzag) without being aligned. Since the irradiation area is used, not only can the laser light source be actually moved in a zigzag manner (zigzag), but also the irradiated area can be formed by such a method. Furthermore, the movement of the print source in the present embodiment refers to the relative movement of the workpiece and the exit source, and includes not only the workpiece being fixed but the source being moved, but also the source being fixed and being moved by the object. (actually, it is a form in which the stage on which the workpiece is placed is moved). For example, the m-plane causes the exit source and the stage to move at a constant speed in parallel with the predetermined guard line, and the -plane causes the exit direction of the laser light to periodically change in a plane perpendicular to the predetermined processing line, etc. The irradiated region is formed in a form satisfying the above-described mineral tooth configuration. Alternatively, 'the plurality of emission sources are relatively moved in parallel at a constant speed by the surface, and the irradiation timing of the unit pulse light from each of the emission sources is periodically changed' to satisfy the above-described configuration of the ore-like arrangement relationship. Shaped Irradiation Area ❶ Fig. 8 is a view showing the relationship between the predetermined processing line and the predetermined formation position of the irradiated area in the two cases. In either case, it can be regarded as shown in Fig. 8 'like the predetermined formation positions (2), P22, P23 'P24, p25... of the areas to be irradiated RE21, re22 re23 re24, RE25·., 156646.doc -23 - 201221261 6X is set on the straight line La, ίβ parallel to the predetermined processing line L, and is simultaneously formed in parallel with the irradiated area of P21, P23, P25, ... along the predetermined formation position of the straight line La, and The formation of the illuminated regions of the predetermined positions P22, P24, ... of the straight line Lp is formed. In addition, when the output source is moved in a zigzag manner (serration), the source of the laser light is directly moved, or the laser beam is relatively scanned by moving the stage on which the workpiece is placed. The movement of the exit source or the stage is simultaneous operation of the two axes. On the other hand, the operation of moving only the source or the stage in parallel with the predetermined processing line is a single-axis operation. Therefore, the latter is preferable in terms of realizing high-speed movement of the discharge source, that is, improvement in processing efficiency. As shown in each of the above processing patterns, the splitting/cracking process performed in the present embodiment is mainly for imparting a discrete treatment of the unit pulse light to impart a continuous treatment/solution for the workpiece. The processing form of the mechanism of impact or stress. The deterioration of the workpiece in the irradiated area (formation of the processing marks) or the scattering, etc., is only incidental to the local producer. The mechanism of the splitting/cracking process of the present embodiment having this feature is substantially different from the fact that the irradiation region of the unit pulsed light is repeatedly or intermittently deformed, melted, and evaporated by one side. The previous processing method for processing. Further, it is sufficient to apply a strong impact or stress to each of the irradiated regions instantaneously, so that the laser light can be irradiated while scanning at a high speed. Specifically, S ′ can be scanned at a very high speed of up to 1000 mm/sec, that is, south speed machining. The processing speed of the cloud in the previous processing method is at most about 200 mm/sec, which is more significant. Of course, it can be said that the processing method realized by 156646.doc -24· 201221261 in the present embodiment significantly improves the production compared with the previous finishing method, and the opening/spliting in the present embodiment is 5, π 丄It is particularly effective in the case where the crystal orientation of the workpiece (the direction in which the direction is easy to open/split) is determined in relation to the predetermined line (4), and the object to be applied is not limited (4). In principle, it can also be applied. (4) The person is in the relationship of ff or the gamma is multi-crystal. In such cases, the direction of cleavage/cleavage relative to the predetermined jade line is not necessarily fixed; Therefore, irregular irregularities are generated at the starting point of the splitting, but by appropriately sighing the irradiation conditions of the irradiated regions and the laser light represented by the pulse width, the allowable range of the bumping and stopping (four) guarding error can be performed. It is only used for processing that does not have problems. <Cutter-off beam energy utilization efficiency upwards> The split/crack process of the present embodiment is such that the pulse width of 1 〇〇psec or less is separated by the separation between about 4 pm and 50 μηι as described above. The unit pulsed light causes deterioration, melting, evaporation, and the like of the substance in the central portion of each of the irradiated regions, thereby causing the cleaving/cracking to progress to between the irradiated regions. Therefore, it is not necessary to carry out the necessary processing in the irradiated area, and it is of course necessary to make the cleavage/cleavage progress from the irradiated area with respect to the direction in which it is easy to open/crack. For example, 'in the case of a unit pulse light having a large peak power density and a small pulse width, the excess energy applied to the irradiated area causes more damage than necessary to the irradiated area, and on the other hand causes lumps/ Cleavage cannot progress better. The reason for this is that the energy of the unit pulsed light that is irradiated is not fully utilized for the progress of the cleavage/cleavage. 156646.doc •25· 201221261. More specifically, it can be considered that it takes about 10 psec in the energy absorption from the electronic system to the vibration of the molecular system caused by the energy. Therefore, in order to make the energy of the unit pulsed light of the irradiation more used for the progress of the cleavage/cleavage, it can be said that the peak power density is suppressed to the unit of the weakest intensity portion and the unit of the pulse width is increased. It is preferable that the pulsed light is irradiated to the form of the workpiece. In this case, the energy utilization efficiency of the laser light is increased. In the present embodiment, the improvement of the energy use efficiency is achieved by optically temporarily dividing each unit pulse light into two parts, and one of the two is different from the other by making the optical path lengths of the two different. A slight delay (up to about 10 nsec) is applied to the substantially identical illuminated area on the workpiece. The processing of this form is referred to as split beam processing. Hereinafter, the description will be specifically made. Fig. 9 is a view schematically showing a change in the intensity distribution (time change of the beam intensity) of the laser light actually irradiated to the workpiece when the delay time is different. Specifically, it is considered that the unit pulse light UP having the peak intensity (peak power density) 1 and the half value width ω is divided into two first half-pulse lights H1 and a second half pulse having the same distribution as shown in FIG. 9( a ). The light H2 is delayed by the second half pulse light H2 with respect to the first half pulse light H1 by making the optical path lengths of the two different. Set the delay time to d. First, for example, the delay time D shown in FIG. 9(b) is about 1/3 of the half value width ω (number of Psec to several tens of psec) of the unit pulse light UP (in the case of D=co/3). When the delay time is small, the first half pulse light H1 and the second half pulse light H2 are irradiated in time, and the composite pulse light CP1 of the two 156646.doc '26-201221261 is used as the peak. A single unit of pulsed light with a strong intensity and a half-value width is transmitted through. However, by delaying the irradiation of the second half-pulse light H2 with respect to the ith half-pulse light m, the second half-pulse light H2 is irradiated to the first half-pulsed light H1 to cause the substance to be deteriorated, and the cleavage/solution is started. The energy absorption efficiency of the higher state (plasma state or high temperature state) is taken as the 'radiation area'. At this time, the energy of the second half-pulsed light H2 is mainly used for the progress of the cleavage/cleavage. Of course, as the delay time D is increased, the time overlap between the first half pulse light and the second half pulse H2 is small. However, as shown in Fig. 9(c), if the delay time D is wider than the half value of the unit pulse light!^!» (when the same degree is used (when 〇 = ω), the first half pulse light HI The combined pulsed light CP2 with the second half-pulse diaphragm 2 has two peaks of the peak intensity 12 smaller than the peak intensity 11 of the combined pulsed light cpi. However, only the second half-pulse light is irradiated to the second half of the irradiation. The area to be irradiated in the state in which the energy absorption efficiency is high is the same as that in the case of irradiating the combined pulsed light CP1. Further, the combined pulsed light CP2 as a whole can be regarded as a unit of the half value width ω2 (> ω1). Pulse light. When the delay time D is larger than ω and is about twice the half value width ω of the unit pulse light UP as shown in Fig. 9(d) (when D=2〇), 1 half-pulse light H1 and the second half-pulse diaphragm 2 have almost no overlap, and the combined pulsed light CP3 (so named in the name) is essentially merely irradiating the first half-pulse light out in order with the delay time d. The two individual unit pulse lights UP3a and uP3b of the second half pulse light 112 (that is, the peak intensity 13 is approximately P/2). However, the delay time D in this case is at most about 1 〇〇pSeC even if it is increased, so the energy generated by the irradiation of the unit pulse light UP3a is 156646.doc 27· 201221261 The period in which the absorption efficiency is high is not lost. Irradiation unit pulse *up3b. Therefore, the energy of the unit pulsed light UP3b is used for the progress of the cleavage/cleavage plane. In other words, in this case as well, the energy of the unit pulsed light UP emitted from the light source can be efficiently utilized in the same manner as the case where the second half pulse light 1 and the second half pulse light H2 are substantially overlapped. Furthermore, the inventors of the present invention have found that when the delay time D is in the range of approximately n sec, the effect of improving the energy efficiency of the unit pulse light upi described above can be obtained. This is considered to be because the time during which the energy absorption efficiency achieved by the irradiation of the unit pulse light UP3a is maintained is at most about 1 secsec. Further, when the delay time D is lower than ω/3, the effect of delaying the second half-pulse diaphragm 2 cannot be sufficiently obtained, and the workpiece 1〇 is liable to be excessively damaged, which is not preferable. According to the above, if the optical path length difference between the first half-pulse light output and the second half-pulse light H22 is set such that the delay time D is set as a value within a range of 10 nsec or less, even if the unit pulse light emitted from the light source has When the peak power density is excessively damaged to the irradiated area, the peak intensity of the unit pulse light actually irradiated to the workpiece can be lowered, and the irradiation time can be substantially increased, thereby making it possible to Each unit of pulsed light increases the ratio of energy used for the progress of cleavage/cleavage. Specifically, s ' can mainly use the energy of the second half-pulsed light H2 of delayed irradiation for the progress of the cleavage/cleavage. In other words, when the optical path length difference between the first half pulse light H1 and the second half pulse light H2 is set so that the delay time D satisfies the range, and the separation beam processing is performed, the energy utilization efficiency can be further improved. .doc •28- 201221261 Open processing. Thereby, the starting point of the division of the workpiece 10 can be formed more efficiently and surely. In addition, the split beam processing system described so far causes the second half-pulse diaphragm 2 to be delayed in time compared with the first half-pulse diaphragm 2, and both of them are irradiated to substantially the same irradiated region, but on the other hand, In the present embodiment, as described above, the laser beam is relatively scanned while scanning at a scanning speed of about 50 mm/sec to 3000 mm/sec. At first glance, the two seem to be contradictory. This is because 'the period between the irradiation of the first half-pulse light H1 and the second half-pulse light H2 is irradiated, and the laser beam and the workpiece 相对 are also relatively moved. Therefore, the formation position of the irradiated region of each half-pulse light should be There are different. However, even if the scanning speed of the laser light is set to 3 〇〇〇mm/sec (=3 m/sec) and the delay time d is 1 〇nsec, the irradiation position of the first half pulse light H1 and the second half pulse light are set. When the position of H2 is most deviated, the calculation of the deviation between the two positions is only 3〇ηιη❶. On the other hand, the beam of the laser beam is about 1 μιηη to about πμπ1, or is split/cracked. The areas to be irradiated formed on the workpiece 1 at the time of the opening are spaced apart from each other by 4 μm to 50 μm. The value of 30 nm is about 1/1 〇〇 to 1/1 〇〇〇, which can be considered to be sufficiently within the error range. Therefore, even when the first half pulse light H1 and the second half pulse light H2M are incident on substantially the same irradiated region during processing, it is possible. Further, the separation beam processing can be performed when the processing of any of the above-described second processing pattern to the third processing pattern is performed. In the above description, the first half pulse light H1 and the second half pulse light H2 are equally distributed, but this is not necessary.

S 156646.doc -29- 201221261 之形態。圖10係例示延遲時間為單位脈衝光之半值宽之2 倍左右但第2半脈衝光H2之峰值強度小於第1半脈衝光出 之峰值強度之情形之雷射光之強度分佈之圖。於使用該形 態之雷射光進行分離光束加工之情形時,亦可實現有效率 之劈開/裂開加工。 於該情形時,亦可藉由使第2半脈衝光H2之光束直徑或 擴散角不同於第1半脈衝光H1,而使照射至被加工物時之 第2半脈衝光H2之照射光點直徑大於第1半脈衝光H1之照 射光點直徑。該情形時,第2半脈衝光H2之半值寬大於第工 半脈衝光Η1之半值寬’因此可進一步延遲照射時間。 <雷射加工裳置之概要> 下面’對可實現上述各種加工圖案之加工之雷射加工裝 置進行說明。 圖11係概略性地表示本實施方式之雷射加工裝置5〇之構S 156646.doc -29- 201221261 Form. Fig. 10 is a view showing the intensity distribution of the laser light in the case where the delay time is about twice the half value width of the unit pulse light, but the peak intensity of the second half pulse light H2 is smaller than the peak intensity of the first half pulse light. When the laser beam of this form is used for the separation beam processing, efficient splitting/cracking processing can also be realized. In this case, the beam spot diameter or the diffusion angle of the second half-pulse light H2 may be different from the first half-pulse light H1, so that the irradiation spot of the second half-pulsed light H2 when irradiated to the workpiece may be made. The diameter of the illumination spot having a diameter larger than that of the first half pulse light H1. In this case, the half value width of the second half-pulse light H2 is larger than the half value width of the second half pulsed aperture 1 so that the irradiation time can be further delayed. <Summary of Laser Processing and Swinging> Next, a laser processing apparatus capable of realizing processing of the above various processing patterns will be described. Figure 11 is a view schematically showing the construction of the laser processing apparatus 5 of the present embodiment.

馬目載置於载台7之侧(將其稱作背面或裁置 汗W射光之側(將其稱 工物10,該背面觀察 或裁置面)經由該載台 156646.doc 201221261 7觀察該被加工物1 0 β 載台7 S史為可藉由移動機構7m而於雷射光照射部5〇Α與 觀察部50Β之間沿水平方向移動。移動機構7m借助未圖示 之驅動機構之作用而使載台7於水平面内沿特定之χ γ 2軸 方向移動。由此,貫現雷射光照射部5〇α内之雷射光照射 位置之移動、觀察部50Β内之觀察位置之移動、或雷射光 照射部50Α與觀察部50Β之間之載台7之移動等。再者,移 動機構7m之以特定旋轉軸為中心之水平面内之旋轉(㊀旋 轉)動作亦可與水平驅動獨立地進行。 又,於雷射加工裝置50中,可進行適當地切換正面觀察 與背面觀察。由此,可靈活且迅速地進行與被加工物1〇之 材質或狀態對應之最佳之觀察。 載台7由石英等透明構件形成,於其内部設置有成為用 以吸附固定被加工物10之進氣通路之未圖示之抽吸用配 官。抽吸用配管藉由例如利用機械加工對載台7之特定位 置進行削孔而設置。 於將被加工物1〇載置於載台7上之狀態下,藉由例如抽 吸泵等抽吸機構11對抽吸用配管進行抽吸,而對設置於抽 吸用配官之載台7載置面側之前端之抽吸孔施加負壓,由 此使被加工物10(及固定片材4)固定於載台7。再者,圖u 中例不作為加工對象之被加工物1〇貼附於固定片材4之情 形,但較佳為,於固定片材4之外緣部配置用以固定該固 定片材4之未圖示之固定環。 &lt;照明系統及觀察系統&gt; 156646.doc 2 -31 - 201221261 觀察部50B以如下方式構成:一面對載置於載台7上之被 加工物10自載台7之上方重疊性地進行來自落射照明光源 S1之落射照明光L1之照射與來自斜光照明光源82之斜光透 過照明光L2之照射’一面可以自載台7之上方側藉由正面 觀察機構6進行正面觀察,及自載台7之下方側藉由背面觀 察機構16進行背面觀察。 具體而言’自落射照明光源S 1發出之落射照明光l 1於設 置於省略圖示之鏡筒内之半鏡片9反射並照射至被加工物 10。又,觀察部5 0B具備正面觀察機構6,該正面觀察機構 6包含設置於半鏡片9上方(鏡筒上方)之CCD(charge coupled device,電荷耦合器件)相機6a及與該CCD相機以 連接之監視器6b,可於使落射照明光L1照射之狀態下即時 地進行被加工物10之明視野像之觀察。 又,於觀察部50B中,於載台7之下方更佳具備背面觀察 機構16,β亥背面觀察機構16包括設置於後述之半鏡片Η下 方(鏡筒下方)之CCD相機16a及與該CCD相機16a連接之監 視器16b。再者,監視器16b與正面觀察機構6所具備之監 視器6b亦可為共通者。 又,自載台7之下方所具備之同轴照明光源33發出之同 軸照明光L3 ’亦可於設置於省略圖示之鏡筒内之半鏡片19 反射並於聚光透鏡18聚光,且經由載台7照射至被加工物 1〇。更佳為亦可於載台7下方具備斜光照明光源S4,而將 斜光照明光L4經由載台7照射至被加工物1〇。該等同軸照 月光原S3或斜光照明光源μ可較佳地用在於例如被加工物 156646.doc •32- 201221261 ι〇之表面侧具有不透明金屬層等’導致自表面側之觀察難 以產生來自該金屬層之反射之情形等自背面侧觀察被加工 物10時。 &lt;雷射光源&gt; 作為雷射光源SL,使用波長500 nm至1600 nm者。又, 為貫現利用上述之加工圖案之加工,雷射光Lb之脈寬需要 為1 psec至50 psec左右。又,較佳為,重複頻率尺為1〇 kHz至200 kHz左右,雷射光之照射能量(脈衝能量)為〇」 μ·ί至50 μ«ί左右。 再者,自雷射光源SL出射之雷射光LB之偏光狀態為圓 偏光或直線偏光均可。但於直線偏光之情形時,自結晶性 被加工材料中之加工剖面之彎曲與能量吸收率之觀點考 慮,較佳設為偏光方向與掃描方向大致平行,例如兩者所 成之角度處於±1。以内。 光學系統5為設定雷射光照射至被加工物1〇時之光路之 部位。依照由光學系統5所設定之光路而對被加工物之特 定照射位置(被照射區域之預定形成位置)照射雷射光。 圖12係例禾光學系統5之構成之模式圖。光學系統5主要 包括光束擴展器51、物鏡宇% _ 筑糸、.先52分支鏡片53及合成鏡片 又亦可於光學系統5中之適當位置設置適當個數之 鏡片5a以變換雷射光β 個鏡片5仏情形。以之方向。圖12中例示設置有4 又’於出射光為直線偏光之情形時’較佳為光學系統$The horse's eye is placed on the side of the stage 7 (referred to as the side of the back or the side of the cut sweat (referred to as the work object 10, the back view or cut surface) via the stage 156646.doc 201221261 7 The workpiece 10 0 β stage 7 S is movable in the horizontal direction between the laser beam irradiation unit 5 〇Α and the observation unit 50 藉 by the moving mechanism 7 m. The moving mechanism 7 m is driven by a driving mechanism not shown. The movement of the stage 7 in the horizontal direction of the χ γ 2 axis in the horizontal plane is performed, whereby the movement of the laser light irradiation position in the laser light irradiation unit 5〇α and the movement of the observation position in the observation unit 50Β are performed. Or the movement of the stage 7 between the laser beam irradiation unit 50A and the observation unit 50A. Further, the rotation (one rotation) in the horizontal plane centered on the specific rotation axis of the movement mechanism 7m may be independent of the horizontal drive. Further, in the laser processing apparatus 50, the front view and the back view can be appropriately switched, whereby the optimum observation corresponding to the material or state of the workpiece 1 can be flexibly and quickly performed. The stage 7 is formed of a transparent member such as quartz, A suction controller (not shown) for sucking and fixing the intake passage of the workpiece 10 is provided inside. The suction pipe is provided by, for example, machining a specific position of the stage 7 by machining. In a state in which the workpiece 1 is placed on the stage 7, the suction pipe is sucked by a suction mechanism 11 such as a suction pump, and the suction pipe is placed on the suction stage. 7 The negative pressure is applied to the suction hole at the front end of the mounting surface side, whereby the workpiece 10 (and the fixing sheet 4) is fixed to the stage 7. Further, in the figure u, the workpiece 1 which is not processed is processed. In the case where the crucible is attached to the fixing sheet 4, it is preferable that a fixing ring (not shown) for fixing the fixing sheet 4 is disposed on the outer edge portion of the fixing sheet 4. <Lighting system and observation system> 156646.doc 2 -31 - 201221261 The observation portion 50B is configured such that the workpiece 10 placed on the stage 7 overlaps the epi-illumination from the epi-illumination light source S1 over the stage 7 The illumination of the light L1 and the oblique light from the oblique illumination source 82 are transmitted through the illumination light L2. The upper side of the stage 7 is viewed from the front by the front view mechanism 6, and the lower side of the stage 7 is viewed from the back side of the stage 7. The specific view is the 'emission illumination light emitted from the epi-illumination source S1. The half lens 9 provided in the lens barrel (not shown) is reflected and irradiated to the workpiece 10. The observation unit 50B is provided with a front observation mechanism 6 including the upper surface of the half lens 9 ( A CCD (charge coupled device) camera 6a and a monitor 6b connected to the CCD camera can perform a bright field of the workpiece 10 in a state where the epi-illumination light L1 is irradiated. Like observation. Further, in the observation unit 50B, the back view mechanism 16 is preferably provided below the stage 7, and the β-Hui back view mechanism 16 includes a CCD camera 16a provided below the half lens unit (below the lens barrel), which will be described later, and the CCD. The monitor 16b to which the camera 16a is connected. Further, the monitor 16b and the monitor 6b provided in the front observation mechanism 6 may be common. Further, the coaxial illumination light L3' emitted from the coaxial illumination light source 33 provided under the stage 7 can also be reflected by the half mirror 19 provided in the lens barrel (not shown) and collected by the collecting lens 18, and The workpiece 7 is irradiated to the workpiece 1 via the stage 7. More preferably, the oblique illumination light source S4 is provided below the stage 7, and the oblique illumination light L4 is irradiated to the workpiece 1 via the stage 7. The coaxial illumination source S3 or the oblique illumination source μ can be preferably used, for example, to have an opaque metal layer or the like on the surface side of the workpiece 156646.doc • 32-201221261 ι〇, which makes it difficult to generate observation from the surface side. When the metal material is reflected, the workpiece 10 is observed from the back side. &lt;Laser light source&gt; As the laser light source SL, a wavelength of 500 nm to 1600 nm is used. Further, in order to realize the processing using the above-described processing pattern, the pulse width of the laser light Lb needs to be about 1 psec to 50 psec. Further, it is preferable that the repetition frequency scale is from about 1 kHz to about 200 kHz, and the irradiation energy (pulse energy) of the laser light is about μ"μ·ί to 50 μ«ί. Further, the polarization state of the laser light LB emitted from the laser light source SL may be either circularly polarized or linearly polarized. However, in the case of linear polarization, it is preferable that the polarization direction is substantially parallel to the scanning direction from the viewpoint of the bending of the processed section and the energy absorption rate in the material to be processed, for example, the angle formed by the two is ±1. . Within. The optical system 5 is a portion where the optical path when the laser light is irradiated to the workpiece 1 is set. The laser beam is irradiated with a specific irradiation position (a predetermined formation position of the irradiated region) of the workpiece in accordance with the optical path set by the optical system 5. Fig. 12 is a schematic view showing the configuration of the optical system 5. The optical system 5 mainly includes a beam expander 51, an objective lens _ 糸 糸, a first 52 branch lens 53 and a synthetic lens, and an appropriate number of lenses 5a may be disposed at appropriate positions in the optical system 5 to convert the laser light β Lens 5 仏 situation. In the direction. In Fig. 12, it is exemplified that 4 and 'when the emitted light is linearly polarized,' is preferably an optical system $

S 156646.doc -33· 201221261 具備衰減器5b。衰減器5b配置於雷射光LB之光路上之適當 位置,擔負對出射之雷射光LB之強度進行調整之作用。 如圖12所例示,光學系統5中,於自雷射光源SL發出之 雷射光LB之光路OP上配置有均為半鏡片之分支鏡片53及 合成鏡片54。光路OP藉由分支鏡片53而分支為第1分支光 路OP1與第2分支光路OP2,第1分支光路OP1與第2分支光 路OP2於合成鏡片54合流而再次成為一個光路OP。由此, 自雷射光源SL出射之雷射光LB藉由分支鏡片53而分離為 於第1分支光路OP1中前進之第1雷射光LB1與於第2分支光 路OP2中前進之第2雷射光LB2。該情形時,第1半脈衝光 H1相當於第1雷射光LB1之單位脈衝光,第2半脈衝光H2相 當於第2雷射光LB2之單位脈衝光。 又,於第2分支光路OP2上配置有光路長調整機構55。 光路長調整機構55包含使於第2分支光路OP2上前進之第2 雷射光LB2向合成鏡片54反射之多個鏡片群。而且,光路 長調整機構55如箭頭AR1所示以如下方式構成,藉由可於 第2分支光路OP2之延伸方向上改變其位置,而可自如地調 整第2雷射光LB2之反射位置。藉由以該形態調整第2雷射 光LB2之反射位置,可任意地設定於第2分支光路OP2中前 進之第2雷射光LB2之光路長。 藉由光路長調整機構55而將第2分支光路OP2之光路長 設定得長於第1分支光路OP1之光路長,由此於較第1分支 光路OP1與第2分支光路OP2合流之合成鏡片54更靠下游側 之光路OP中,第2雷射光LB2相對於第1雷射光LB1而延 156646.doc • 34· 201221261 遲。因此,雷射加工裝置50中,藉由光路長調整機構55而 適當地設定第1分支光路OP1與第2分支光路〇p2之光路長 差,上述之分離光束加工可以任意之延遲時間D進行。 再者’若設光路長差為AL,則延遲時間d與光路長差之 關係可使用光之速度c表不為AI^cD。於例如D=10 psec之 情形時 ’ s免為 c=3&gt;&lt;108 m/sec,AL=3 mm。 又’於第2分支光路〇P2上設置有焦點調整用透鏡系統 56。藉由適當地設定該焦點調整用透鏡系統56,可使第2 雷射光LB2之單位脈衝光即第2半脈衝光H2之光束直徑或 擴散角不同於第2雷射光LB2之單位脈衝光即第!半脈衝光 H1。由此,使照射至被加工物時之第2半脈衝光H2之照射 光點直徑大於第1半脈衝光H1之照射光點直徑之狀態下之 分離光束加工成為可能。 又’藉由適當地調整第1分支光路OP所具有之衰減器5b 或者第2分支光路〇P2所具有之衰減器5b,可使第2雷射光 LB 2之強度小於第1雷射光lb 1之強度,從而亦可進行圖1〇 所示之分佈下之分離光束加工。 且說’藉由準備不同之2個雷射光源,並使各個雷射光 之出射時序延遲而進行上述之分離光束加工之形態乍一看 有可能’但實際上,於使被照射區域離散地形成之條件 下’難以高精度地以pSec級或者nsec級控制來自2個雷射光 源之出射時序之延遲,因而不現實》 再者’圖12中例示自物鏡系統5 2至被加工物1 〇之雷射光 LB之光路為固定之情形。亦可將合成鏡片54以下之光路 156646.doc •35· 201221261 〇p於實際上或者假設性地設定多個,並且藉由未圖示之光 路設定機構而將雷射光LB之各個單位脈衝光照射至被加工 物時之光路於設定之多個光路中依序切換地構成。該情形 時’實現於被加工物10之上表面之多個部位同時並行地進 行掃描之狀態,或者假設性地視作如此之狀態。換言之, 可說此使雷射光LB之光路變多。 &lt;控制器&gt; 控制器1進而包括:控制部2,其控制上述各部分之動作 而實現被加工物10之加工處理;及存儲部3,其存儲控制 雷射加工裝置50之動作之程式3p或加工處理時所參照之各 種資料。 控制部2藉由例如個人電腦或微電腦等常用之電腦實 現’藉由存儲於存儲部3中之程式3p被讀入至該電腦並加 以執行,而使各種構成要素作為控制部2之功能性構成要 素而加以實現。 具體而言,控制部2主要包括:驅動控制部21,其控制 移動機構7m對載台7之驅動或聚光透鏡18之聚焦動作等與 加工處理相關之各種驅動部分之動作;攝像控制部2 2,其 控制CCD相機6a及16a之攝像;照射控制部23,其控制來 自雷射光源SL之雷射光LB之照射及光學系統5中之光路之 设定形態;吸附控制部24,其控制藉由抽吸機構11向載台 7吸附固定被加工物1 〇之動作;及加工處理部2 5,其依照 所提供之加工位置資料D1(後述)及加工模式設定資料 D2(後述)而對加工對象位置執行加工處理。 156646.doc -36- 201221261 存儲。Ρ 3藉由R〇M(read-only memory,祇讀存儲器)或 RAM(rand〇m-access memory,隨機存取存儲器)及硬盤等 存儲媒體而實現。再者,存儲部3亦可為藉由實現控制都2 之電腦之構成要素而實現之形態,於為硬盤之情形時等, 亦可為與該電腦分開設置之形態。 記述有對被加m設;t之財加卫線之位置之加工位 置資料m自外部提供並存儲於存儲部3中。又,存儲部艸 預先存儲有按照加工模式而記述有雷射光之各個參數之條 件、光學系統5中之光路之設定條件或載台7之驅動條件 (或者該等之可設Μ圍)等之加卫模式蚊資料D2。 再者,操作人員對雷射加工裝置5〇提供之各種輸入指 不,較佳為利用控制器!中實現之Gm(graphicai咖 如抓ce,圖形使用者介面)而實現。例如,借助加工處理 部25之作用而以Gm提供加工處理用選單。操作人員基於 該加工處理用選單而進行後述之加工模式之選擇或加工條 件之輸入等。 &lt;對準動作&gt; 雷射加工裝置50中’於加工處理之前,可於觀察部_ 中進行微調被加工物10之配置位置之對準動作。對準動作S 156646.doc -33· 201221261 equipped with an attenuator 5b. The attenuator 5b is disposed at an appropriate position on the optical path of the laser beam LB, and functions to adjust the intensity of the emitted laser light LB. As illustrated in Fig. 12, in the optical system 5, a branch lens 53 and a composite lens 54 each having a half lens are disposed on the optical path OP of the laser light LB emitted from the laser light source SL. The optical path OP branches into the first branched optical path OP1 and the second branched optical path OP2 by the branch lens 53, and the first branched optical path OP1 and the second branched optical path OP2 merge in the combined lens 54 to become the optical path OP again. Thereby, the laser light LB emitted from the laser light source SL is separated into the first laser light LB1 that advances in the first branch optical path OP1 and the second laser light LB2 that advances in the second branched optical path OP2 by the branch lens 53. . In this case, the first half pulse light H1 corresponds to the unit pulse light of the first laser light LB1, and the second half pulse light H2 corresponds to the unit pulse light of the second laser light LB2. Further, an optical path length adjusting mechanism 55 is disposed on the second branch optical path OP2. The optical path length adjusting mechanism 55 includes a plurality of lens groups that reflect the second laser light LB2 advancing on the second branched optical path OP2 toward the synthetic lens 54. Further, the optical path length adjusting mechanism 55 is configured as shown by an arrow AR1 in such a manner that the reflection position of the second laser light LB2 can be freely adjusted by changing the position in the extending direction of the second branch optical path OP2. By adjusting the reflection position of the second laser beam LB2 in this manner, the optical path length of the second laser light LB2 advanced in the second branch optical path OP2 can be arbitrarily set. The optical path length adjustment mechanism 55 sets the optical path length of the second branched optical path OP2 to be longer than the optical path length of the first branched optical path OP1, thereby forming the combined lens 54 that merges with the first branched optical path OP1 and the second branched optical path OP2. In the optical path OP on the downstream side, the second laser light LB2 is delayed by 156646.doc • 34· 201221261 with respect to the first laser light LB1. Therefore, in the laser processing apparatus 50, the optical path length difference between the first branched optical path OP1 and the second branched optical path 2p2 is appropriately set by the optical path length adjusting mechanism 55, and the above-described split beam processing can be performed for any delay time D. Furthermore, if the optical path length difference is AL, the relationship between the delay time d and the optical path length difference can be expressed as AI^cD using the speed c of the light. For example, in the case of D = 10 psec, 's is not c=3> &lt;108 m/sec, AL = 3 mm. Further, the focus adjustment lens system 56 is provided on the second branch optical path P2. By appropriately setting the focus adjustment lens system 56, the beam diameter or the diffusion angle of the second pulse light H2 which is the unit pulse light of the second laser light LB2 can be made different from the unit pulse light of the second laser light LB2. ! Half pulse light H1. Thereby, it is possible to process the separated beam in a state where the irradiation spot diameter of the second half pulse light H2 when the object is irradiated is larger than the diameter of the irradiation spot of the first half pulse light H1. Further, by appropriately adjusting the attenuator 5b of the first branch optical path OP or the attenuator 5b of the second branch optical path P2, the intensity of the second laser light LB 2 can be made smaller than that of the first laser light lb 1 The intensity, and thus the separation beam processing under the distribution shown in Fig. 1A, can also be performed. And it is said that it is possible to perform the above-described method of separating the beam processing by preparing two different laser light sources and delaying the emission timing of each laser light, but in fact, the irradiated regions are discretely formed. Under the condition, it is difficult to control the delay of the emission timing from the two laser light sources with pSec level or nsec level with high precision, so it is unrealistic. Furthermore, the image from the objective lens system 52 to the workpiece 1 is illustrated in FIG. The light path of the light LB is fixed. It is also possible to set a plurality of optical paths 156646.doc •35· 201221261 〇p below the synthetic lens 54 in a practical or hypothetical manner, and irradiate each unit pulse light of the laser light LB by an optical path setting mechanism not shown. The optical path to the workpiece is sequentially switched in a plurality of set optical paths. In this case, it is realized in a state in which a plurality of portions on the upper surface of the workpiece 10 are simultaneously scanned in parallel, or assumed to be in such a state. In other words, it can be said that the optical path of the laser light LB is increased. &lt;Controller&gt; The controller 1 further includes a control unit 2 that controls the operation of each of the above-described parts to realize processing of the workpiece 10, and a storage unit 3 that stores a program for controlling the operation of the laser processing apparatus 50 3p or various materials referenced during processing. The control unit 2 realizes, by a computer such as a personal computer or a microcomputer, that the program 3p stored in the storage unit 3 is read into the computer and executed, and various components are used as the functional components of the control unit 2. The elements are implemented. Specifically, the control unit 2 mainly includes a drive control unit 21 that controls the operation of the various driving portions related to the machining process such as the driving of the stage 7 or the focusing operation of the collecting lens 18 by the moving mechanism 7m; the imaging control unit 2 2, which controls the imaging of the CCD cameras 6a and 16a; the illumination control unit 23 controls the illumination of the laser light LB from the laser light source SL and the setting mode of the optical path in the optical system 5; the adsorption control unit 24 controls the borrowing The operation of sucking and fixing the workpiece 1 to the stage 7 by the suction mechanism 11 and the processing unit 25 are processed in accordance with the supplied processing position data D1 (described later) and the processing mode setting data D2 (described later). The object position performs machining processing. 156646.doc -36- 201221261 Storage. Ρ 3 is realized by a storage medium such as R〇M (read-only memory) or RAM (rand〇m-access memory) and a hard disk. Furthermore, the storage unit 3 may be realized by implementing the components of the computer of the control unit 2, and may be in a form separate from the computer when the hard disk is used. The machining position data m of the position where the wealth is added to the line is provided from the outside and stored in the storage unit 3. Further, the storage unit 艸 stores in advance the conditions in which the respective parameters of the laser light are described in the processing mode, the setting conditions of the optical path in the optical system 5, or the driving conditions of the stage 7 (or the settable circumferences), and the like. Add mode mosquito information D2. Furthermore, the operator refers to the various inputs provided by the laser processing apparatus 5, preferably using a controller! Realized in the implementation of Gm (graphicai coffee, such as catching ce, graphical user interface). For example, the processing processing menu is provided by Gm by the action of the processing unit 25. The operator selects a processing mode, a processing condition, and the like described later based on the processing processing menu. &lt;Alignment Operation&gt; In the laser processing apparatus 50, the alignment operation of the arrangement position of the workpiece 10 can be finely adjusted in the observation unit _ before the processing. Alignment action

係為使被加中所規^χγ座標軸與載台7之座W 一致而進行之處理。於進行上述之加工圖案之加工之㈣ 時,該對準處理於使被加工物之結晶方位、預定加工線及 雷射光之掃插方向滿足各加工圖案中所需之特定關 面較為重要。 156646.doc -37- 201221261 對準動作可應用周 技術執仃’只要根據加工圖案而以 、田&amp;、進行即可。例如,若為對使用!個母基板製作 之數個器件晶粒進行切割之情形時等於被加工物ι〇表面形 成重複圖案之情形時,則可藉由使用圖案匹配等方法實現 適當之對準動作。該情形時,概略性地說,則咖相機^ 或者W獲取形成於被加工物1〇上之多個對準用標記之拍 攝圖像,加工處理部25基於該等拍攝圖像之拍攝位置之相 對性關係而指定對準量,且驅動控制部川艮據該對準量而 藉由移動機構7讀載台7移動,由此實現對準。 藉由進行該對準動作’可正碟地指定加工處理中之加工 位置。再者,於對準動作結束後,载置有被加工物1〇之載 台7向雷射光照射部50A移動,繼而進行藉由照射雷射光 ^之加工處理。再者,載纟7自觀察部5〇b向雷射光照射 部50A之移動以於對準動作時設定之預定加工位置與實際 上之加工位置不偏離之方式被保證。 &lt;加工處理之概略&gt; 下面,對本貫施方式之該雷射加工裝置5〇之加工處理進 行說明。於雷射加工裝置50中,藉由組合進行自雷射光源 發出並皱過光學系統5之雷射光lb之照射與載置固定有 被加工物10之載台7之移動,可一面使經過光學系統$之雷 射光B相對於被加工物1〇相對性掃描一面進行被加工物⑺ 之加工。具體而言,可以上述之第!加工圖帛至第3加工圖 案進行劈開/裂開 加工。 於以第1加工圖案進行加工之情形時,至於預定加工線l 156646.doc •38· 201221261 與谷易劈開/裂開之方向平行 該容易劈開/裂開之方㈣”之:::加工物1〇’以使 之預定加1〇:行對準,並且藉由雷射光LB而於被加工物 之預疋加工線L上掃描。 於以第2加工圖荦谨名^ 與容易劈_ 時,至於狀加工社 ::易相/裂開之方向垂直地設定之被加工物〗 方向與載台7之移動方向正交之方式二 被加工物!0進行對準,並且藉由雷射光⑽被加工 預定加工線L上掃描。 ;、第3加工圖案進行加工之情形時,以使預定加工線匕 相對於2個劈開/裂開方向而成為對等位置之方式對被加工 物1〇進行對準,並且以於各個劈開/裂開方向上交替地進 行雷射光LB之掃描之方式交替地使載台7之移動方 即可。 或者,於以第3加工模式進行加工之情形時,亦可沿著 圖8所示之與預定加工線L平行之直線La、邙或者進=沿 著預疋加工線L自身,實體性地或者假設性地使多個雷射 光掃描。再者,假設性地使多個雷射光掃描係指實際上以 1個光路照射雷射光但該光路呈時間性地變化,由此實現 與以多個光路照射雷射光之情形相同之掃描形態。 又,即便於任一加工圖案之情形時,亦可藉由適當地設 定光路長差AL而將延遲時間D設定為脈寬之2倍左右以下 之值’從而可較佳地進行分離光束加工。 【圖式簡單說明】 Ο. 156646.doc •39· 201221261 圏叫)至⑷係模式性地表示第m圖案之加工形態之 圖2係藉由以第丨加工圖案進行之劈開,裂開加工 I刀割起點之被加工物之表面之光學顯微鏡圖像。 二=3由第1加工圖案之加工而形成有分割起點之藍 :賺圖;。4該分割起點分割後之自表面(C面)至剖面 圖4 (a)至⑷係模式性地表示第2加工圖案之加工形態之 圖。 “ 圖5係藉由以第2加工同安vte — &gt; « 乐2加工圖案進订之劈開/裂開加工而形成 有分割起點之被加工物之表面之光學顯微鏡圖像。 圖6係將藉由第2加工圖案之加工而形成有分割起點之藍 寶石c面基板沿著該分割起點分割後之自表面(c面)至剖面 之SEM圖像。 圖7(a)、(b)係模式性地表示第3加工圖案之加工形態之 圖。 圖8係表示第3加工圖案之預定加工線與被照射區域之預 定形成位置之關係之圖。 圖9係模式性地表示延遲時間不同之情形時之實際上照 射至被加工物之雷射光之強度分佈之變化情況之圖。 圖10係例示延遲時間為單位脈衝光之半值寬之2倍左右 但第2半脈衝光H2之峰值強度小於第1半脈衝光⑴之峰值 強度之情形時之雷射光之強度分佈之圖。 圖11係概略性地表示本實施方式之該雷射加工裝置50之 156646.doc -40- 201221261 構成之模式圖。 圖12係例示光學系統5之構成之模式圖。 【主要元件符號說明】 1 控制器 2 控制部 3 存儲部 3p 程式 4 固定片材 5 光學系統 5a 鏡片 5b 衰減器 6 正面觀察機構 6a ' 16a CCD相機 6b 、 16b 監視器 7 載台 7m 移動機構 10 被加工物 10a (被加工物之)載置面 11 抽吸機構 16 背面觀察機構 18 聚光透鏡 19 半鏡片 21 驅動控制部 22 攝像控制部 156646.doc - 41 - 201221261 23 24 25The processing is performed in such a manner that the γ coordinate axis of the gamma coordinate is matched with the seat W of the stage 7. In the case of performing the processing of the above-described processing pattern (4), the alignment processing is important in satisfying the specific orientation required for each processing pattern so that the crystal orientation of the workpiece, the predetermined processing line, and the scanning direction of the laser light are satisfied. 156646.doc -37- 201221261 Alignment action can be applied to the week. Technology 仃 can be carried out according to the processing pattern. For example, if it is for use! When a plurality of device dies made by a mother substrate are cut in a case where a repeating pattern is formed on the surface of the workpiece, the alignment operation can be realized by using pattern matching or the like. In this case, roughly, the coffee camera or the W acquires the captured image of the plurality of alignment marks formed on the workpiece 1 , and the processing unit 25 determines the relative position of the captured image based on the captured image. The alignment amount is specified in the sexual relationship, and the drive control unit Kawasaki moves the reading stage 7 by the moving mechanism 7 according to the alignment amount, thereby achieving alignment. By performing this alignment operation, the processing position in the processing can be specified on the disk. Further, after the alignment operation is completed, the stage 7 on which the workpiece 1 is placed is moved to the laser light irradiation unit 50A, and then processed by irradiation of the laser light. Further, the movement of the carrier 7 from the observation portion 5〇b to the laser beam irradiation unit 50A is ensured so that the predetermined processing position set at the time of the alignment operation does not deviate from the actual machining position. &lt;Summary of Processing Process&gt; Next, the processing of the laser processing apparatus 5A of the present embodiment will be described. In the laser processing apparatus 50, by the combination of the irradiation of the laser light lb emitted from the laser light source and creased by the optical system 5, and the movement of the stage 7 on which the workpiece 10 is placed and fixed, the optical processing can be performed while being optically The laser light B of the system is processed by the workpiece (7) while being scanned relative to the workpiece 1 。. Specifically, you can do the above! The processing drawing is performed until the third processing pattern is opened/cleaved. In the case of processing in the first processing pattern, as for the predetermined processing line l 156646.doc •38· 201221261 parallel to the direction of the valley open/cracking, the side which is easy to open/split (4):::Processing 1〇' so that it is predetermined to add 1〇: line alignment, and scanning by the laser beam LB on the pre-processing line L of the workpiece. As for the processing company:: the direction of the easy phase/cracking direction is set vertically. The direction is orthogonal to the direction of movement of the stage 7. The second workpiece is aligned with 0, and by laser light (10) When the third processing pattern is processed, the workpiece 1 is processed so that the predetermined processing line 成为 becomes the equivalent position with respect to the two split/split directions. Aligning and alternately moving the stage 7 in such a manner that the scanning of the laser light LB is alternately performed in each of the split/split directions. Alternatively, when processing in the third processing mode, A line La parallel to the predetermined processing line L as shown in FIG. Alternatively, along the pre-processing line L itself, a plurality of laser beams are scanned substantially or hypothetically. Further, a plurality of laser scanning means are hypothetically irradiated with laser light by one optical path. The optical path is temporally changed, thereby realizing the same scanning pattern as in the case of irradiating the laser light with a plurality of optical paths. Further, even in the case of any of the processed patterns, the optical path length difference AL can be appropriately set. The delay time D is set to a value equal to or less than about 2 times the pulse width, so that the split beam processing can be preferably performed. [Simple description of the drawing] 156. 156646.doc •39· 201221261 圏)) to (4) is modewise Fig. 2 showing the processing form of the mth pattern is an optical microscope image of the surface of the workpiece to be processed by the first cutting edge by splitting with the second processing pattern. 2 = 3 by the first processing pattern The processing is performed to form a blue of the starting point of the division: the earning map; 4 from the surface (C surface) after the division starting point is divided to the sectional view 4 (a) to (4) schematically showing the processing pattern of the second processing pattern. " Figure 5 is the same as the second processing vte - &gt; «Raku 2 into the prescribed processing pattern of cleavage / cleavage processed to form an optical microscope image of the surface with a division start point of the workpiece. Fig. 6 is an SEM image of a self-surface (c-plane) to a cross-section of a sapphire c-plane substrate having a division starting point formed along the division starting point by processing of the second processing pattern. Fig. 7 (a) and (b) are diagrams schematically showing the processing form of the third processing pattern. Fig. 8 is a view showing the relationship between a predetermined processing line of the third processing pattern and a predetermined formation position of the irradiated area. Fig. 9 is a view schematically showing a change in intensity distribution of laser light actually irradiated to a workpiece when the delay time is different. Fig. 10 is a view showing the intensity distribution of the laser light when the delay time is about twice the half value width of the unit pulse light, but the peak intensity of the second half pulse light H2 is smaller than the peak intensity of the first half pulse light (1). Fig. 11 is a schematic view showing the configuration of 156646.doc - 40 - 201221261 of the laser processing apparatus 50 of the present embodiment. Fig. 12 is a schematic view showing the configuration of the optical system 5. [Description of main components] 1 Controller 2 Control unit 3 Storage unit 3p Program 4 Fixed sheet 5 Optical system 5a Lens 5b Attenuator 6 Front view mechanism 6a ' 16a CCD camera 6b, 16b Monitor 7 Stage 7m Movement mechanism 10 Workpiece 10a (to-be-processed object) mounting surface 11 suction mechanism 16 back surface observation mechanism 18 condensing lens 19 half lens 21 drive control unit 22 imaging control unit 156646.doc - 41 - 201221261 23 24 25

50 50A 50B 51 52 53 54 55 56 AR150 50A 50B 51 52 53 54 55 56 AR1

Cl 至 C3、Clla 至 C14b、 C21至C24Cl to C3, Clla to C14b, C21 to C24

Cpl至CP3Cpl to CP3

D D1 D2D D1 D2

HI H2HI H2

II、12 L LI 至 L4 照射控制部 吸附控制部 加工處理部 雷射加工裝置 雷射光照射部 觀察部 光束擴展器 物鏡糸統 分支鏡片 合成鏡片 光路長調整機構 焦點調整用透鏡系統 箭頭 劈理/解理面 合成脈衝光 延遲時間 加工位置資料 加工模式設定資料 第1半脈衝光 第2半脈衝光 峰值強度 預定加工線 落射照明光 156646.doc -42· 201221261 LB 雷射光 LB1 第1雷射光 LB2 第2雷射光 La ' Lp 直線 OP 光路 OP1 第1分支光路 OP2 第2分支光路 P21至P25 預定形成位置 RE、RE1 至 RE4、RE11 至 REI5、 被照射區域 RE21 至 RE25 SI 至 S4 落射照明光源 SL 雷射光源 UP、UP3a、UP3b 單位脈衝光 W1、W2、W2a、W2b、 弱強度部分 Wlla、W12a、Wllb、 W12b ' Wile ' W12c ω 、 ω1 、 ω2 半值寬 156646.doc 43II, 12 L LI to L4 Irradiation control unit Adsorption control unit Processing unit Laser processing device Laser beam irradiation unit Observation unit Beam expander Objective lens Branch lens Synthetic lens Optical path length Adjustment mechanism Focus adjustment lens system Arrow treatment/solution Surface Synthetic Pulse Light Delay Time Processing Position Data Processing Mode Setting Data 1st Half Pulse Light 2nd Half Pulse Light Peak Intensity Scheduled Processing Line Epi-Illumination Light 156646.doc -42· 201221261 LB Laser Light LB1 1st Laser Light LB2 2nd Laser light La ' Lp Straight OP optical path OP1 First branch optical path OP2 Second branch optical path P21 to P25 Predetermined formation positions RE, RE1 to RE4, RE11 to REI5, illuminated areas RE21 to RE25 SI to S4 Falling illumination source SL Laser source UP, UP3a, UP3b unit pulse light W1, W2, W2a, W2b, weak intensity portion Wlla, W12a, W11b, W12b ' Wile ' W12c ω , ω1 , ω2 Half value width 156646.doc 43

Claims (1)

201221261 七、申請專利範圍: 1. -種雷射加工裝i,其特徵在於包括: 光源’其發出脈衝雷射光;及 載台’其载置被加工物;且 上述脈衝雷射光係脈寬為psec級之超短脈衝光; 自上述光源至上述載台之上述脈衝雷射光之光路以於 中途部分地分支為第!光路與第2光路且其後合流之 設置; 上述雷射加工裝置進而包括光路長調整 變上述第2光路之光路長; &quot; 於定義為自上述光源出射之上述脈衝雷射光分支為於 上述第1光路中前進之第1雷射光與於上述第2光路中前 進之第2雷射光’且上述脈衝雷射光之單位脈衝光分支 為上述第1雷射光之單位脈衝光即第丨半脈衝光與上述第 2雷射光之單位脈衝光即第2半脈衝光時,上述光路長調 整機構以於合流後之上述光路中使上述第2半脈衝光較 上述第1半脈衝光更為延遲之方式設定上述第2光路之光 路長; 於將上述被加工物載置於上述載台之狀態下,藉由一 面使上述載台移動一面將上述脈衝雷射光照射至上述被 加工物,而使上述各個單位脈衝光之上述第丨半脈衝光 與上述第2半脈衝光之被照射區域於上述被加工物之被 加工面上貫質上相同、並且於上述被加工物之被加工面 上離散地形成上述各個單位脈衝光之上述被照射區域。 156646.doc 201221261 2. 如請求項1之雷射加工裝置’其中光路長調整機構以使 上述第2半脈衝光相對於上述第1半脈衝光僅延遲上述單 位脈衝光之半值寬之1/3倍以上且1〇 nsec以下之延遲時 間之方式’設定上述第2光路之光路長。 3. 如請求項2之雷射加工裝置,其中進而包括調整上述第2 雷射光之強度之強度調整機構; 上述光路長調整機構以使上述第2半脈衝光相對於上 述第1半脈衝光僅延遲上述單位脈衝光之半值寬之丨倍以 上且2倍以下之延遲時間之方式,設定上述第2光路之光 路長; 上述強度調整機構以使上述第2雷射光之強度小於上 述第1雷射光之強度之方式調整上述第2雷射光之強度。 4·如請求項2之雷射加工裝置,其中進而包括調整上述第2 雷射光之焦點之焦點調整機構; 上述光路長調整機構以使上述第2半脈衝光相對於上 述第1半脈衝光僅延遲上述單位脈衝光之半值寬之丨倍以 上且2倍以下之延遲時間之方式,設定上述第2光路之光 路長; 上述焦點調整機構以使上述第2雷射光之光束直徑大 ;上述第1田射光之光束直徑之方式調整上述第2雷射光 之焦點。 種被加工物之加工方法,其特徵在於,其係用以於被 加工物=分割起點之加工方法,且包括: • 定步驟’將自出射脈寬為psec級之超短脈衝光 156646.doc 201221261 之脈衝雷射光之光源至載置被加工物之載台之光路設定 為於中途部分地分支為第丨光路與第2光路且其後合流; 光路長調整步驟,於定義為自上述光源出射之°上&quot;述脈 衝雷射光分支為於上述第1光路中前進之第丨雷射光與於 上述第2光路中前進之第2雷射光,且上述脈衝雷射光之 單位脈衝光分支為上述第丨雷射光之單位脈衝光即第工半 脈衝光與上述第2雷射光之單位脈衝光即第2半脈衝光 時,以使上述第2半脈衝光較上述第!半脈衝光更為延遲 之方式設定上述第2光路之光路長; 載置步驟,將上述被加工物載置於上述載台上;及 照射步驟,以使上述各個單位脈衝光之上述第丨半脈 衝光與上述第2半脈衝光之被照射區域相同,且上述各 個單位脈衝光之上述被照射區域於上述被加工物之被加 工面上離散性地形成之方式,將上述脈衝雷射光照射至 上述破加工物,由此於上述被照射區域彼此之間使上述 被加工物產生劈理或者解理,從而於上述被加工物形成 用以進行分割之起點。 6. 如π求項5之被加工物之加工方法,其中於光路長調整 步驟中,以使上述第2半脈衝光相對於上述第丨半脈衝光 僅乙遲上述單位脈衝光之半值寬之1/3倍以上且丨〇加“ 以I之延遲時間之方式,設定上述第2光路之光路長。 7. 如請求項6之被加工物之加工方法,#中進而包括調整 上述第2雷射光之強度之強度調整步驟; 於上述光路長調整步驟中,以使上述第2半脈衝光相 156646.doc 201221261 對於上述第i半脈衝光僅延遲上述單位脈衝光之半值寬 之1倍以上且2倍以下之延遲時間之方式,設定上述第2 光路之光路長; 於上述強度調整步驟中,以使上述第2雷射光之強度 小於上述第1雷射光之強度之方式調整上述第2雷射光之 強度。 8·項6之被加工物之加工方法,其中進而包括調整 上述第2雷射光之焦點之焦點調整步驟; 於上述光路長調整步驟中,r 斜w处 ^ Y ^使上述第2半脈衝光相 對於上述第丨半脈衝光僅延遲 上述皁位脈衝光之半值寬 之1倍U上且2倍以下之延遲時 光路之光路長; ㈣之方式,設定上述第2 於上述焦點調整步驟中,以使上述第2雷射光 直徑大於上述第丨雷射光光 雷射光之焦點。 4束直役之方式調整上述第2 9. 如請求項5至8中任一項之被加工物 ^ V 之加工方法’其中以 於上述破加工物之容易劈開或者裂開 式形成藉由不同之上if〇D 向上相鄯之方 个u i上;早位脈衝朵 照射區域。 先所形成之至少2個被 10. 如請求項9之被加工物之加工方法, 工物之容易劈開或者裂開 /、中沿著上述被加 區域。 °形成所有之上述被照射 &quot;·如請求項9之被加工物之加工方法 物之不同之2個上述容易 八中於上述被加工 易劈開或者裂開之方向上交替進 156646.doc 201221261 行上述至少2個被照射區域之形成。 12. 如請求項5至8中任一項之被加工物之加工 相對於上述被加工物之不同之2個容易劈 方向而等償之方向上形成上述被照射區域 13. —種被加工物之分割方法,其特徵在於: 工物之方法,且 對藉由請求項5至12中任一項之方法而 點之被加工物沿著上述分割起點進行分割 方法,其中於 開或者裂開之 〇 其係分割被加 形成有分割起 156646.doc201221261 VII. Patent application scope: 1. A laser processing apparatus i, characterized in that: a light source 'which emits pulsed laser light; and a stage 'which carries a workpiece; and the pulsed laser light pulse width is Ultra-short pulse light of the psec level; the optical path of the pulsed laser light from the light source to the stage is partially branched in the middle! The optical path and the second optical path are connected to each other; the laser processing device further includes an optical path length that changes to an optical path length of the second optical path; and the pulse laser light defined by the light source is branched from the first a first laser light that advances in the optical path and a second laser light that advances in the second optical path and the unit pulse light of the pulsed laser light is branched into a unit pulse light that is a unit pulse light of the first laser light and In the second half-pulse light, which is the unit pulse light of the second laser beam, the optical path length adjusting means sets the second half-pulse light more delayed than the first half-pulse light in the optical path after the merged light. The optical path of the second optical path is long; and when the workpiece is placed on the stage, the pulsed laser light is irradiated onto the workpiece while the stage is moved, and the respective units are The second half pulse light of the pulsed light and the irradiated area of the second half pulse light are substantially identical in the processed surface of the workpiece, and are added as described above. Discretely forming the irradiated region of the light pulse of the above-described various units of the processed surface thereof. 156646.doc 201221261 2. The laser processing apparatus of claim 1, wherein the optical path length adjusting mechanism delays the second half pulse light by only one-half of a half value width of the unit pulse light with respect to the first half pulse light The optical path length of the second optical path is set by the method of delay time of 3 times or more and 1 〇 nsec or less. 3. The laser processing apparatus of claim 2, further comprising: an intensity adjustment mechanism for adjusting the intensity of the second laser light; and the optical path length adjustment mechanism to cause the second half pulse light to be optical only with respect to the first half pulse light Setting an optical path length of the second optical path by delaying a delay time equal to or larger than a half value width of the unit pulse light; and the intensity adjusting mechanism is configured to make the intensity of the second laser light smaller than the first thunder The intensity of the second laser light is adjusted in such a manner as to increase the intensity of the light. 4. The laser processing apparatus according to claim 2, further comprising: a focus adjustment mechanism for adjusting a focus of said second laser light; said optical path length adjustment mechanism for causing said second half pulse light to be said only with respect to said first half pulse light Setting an optical path length of the second optical path by delaying a delay time equal to or larger than a half value width of the unit pulse light; and the focus adjustment mechanism is configured to increase a beam diameter of the second laser beam; The focus of the second laser light is adjusted in such a manner that the beam diameter of the field light is emitted. The processing method of the workpiece is characterized in that it is used for the processing method of the workpiece = the starting point of the division, and includes: • a step of 'ultra-short pulse light with a pulse width of psec of 156646.doc The light path of the pulsed laser light source of 201221261 to the stage on which the workpiece is placed is set to be partially branched into the second light path and the second light path in the middle and merged thereafter; the optical path length adjustment step is defined as being emitted from the light source The pulse laser light branch is a second laser light that advances in the first optical path and a second laser light that advances in the second optical path, and the unit pulse light of the pulsed laser light branches into the first When the unit pulsed light of the laser light is the second half pulse light, which is the unit pulse light of the second laser light, the second half pulse light is made higher than the above! The half pulse light is further delayed to set the optical path length of the second optical path; the placing step is to place the workpiece on the stage; and the irradiating step is such that the first half of each unit pulse light is The pulsed light is irradiated to the irradiated region of the second half-pulse light, and the irradiated region of the unit pulse light is discretely formed on the processed surface of the workpiece, and the pulsed laser light is irradiated to The workpiece is thereby subjected to processing or cleavage of the workpiece between the irradiated regions, thereby forming a starting point for dividing the workpiece. 6. The method of processing a workpiece according to π, wherein, in the optical path length adjusting step, the second half pulse light is delayed by a half value of the unit pulse light with respect to the third half pulse light. The optical path length of the second optical path is set to be 1/3 times or more and the delay time of the second optical path is set. 7. The processing method of the workpiece according to claim 6 further includes adjusting the second The intensity adjustment step of the intensity of the laser light; in the optical path length adjustment step, the second half pulse optical phase 156646.doc 201221261 is delayed by only one times the half value width of the unit pulse light for the ith half pulse light The optical path length of the second optical path is set to be longer than the delay time of 2 times or less; and the second adjustment is performed so that the intensity of the second laser light is smaller than the intensity of the first laser light in the intensity adjustment step The method for processing a workpiece according to Item 6, further comprising a focus adjustment step of adjusting a focus of the second laser light; wherein in the optical path length adjustment step, r is oblique at w The second half-pulse light is delayed by only one time U of the half-value width of the soap-level pulse light with respect to the second half-pulse light, and the optical path length of the optical path is delayed by two times or less; (4) the second aspect is set In the focus adjustment step, the second laser light diameter is larger than the focus of the first laser light laser light. The second light is adjusted according to any one of the claims 5 to 8. The processing method of the workpiece ^V is such that the above-mentioned broken material is easily opened or split-formed by a different ui on the upper side of the if〇D; the early pulse irradiation area. At least two of them are formed. 10. The processing method of the workpiece according to claim 9, the workpiece is easily opened or split, and the middle portion is along the above-mentioned added region. ° All of the above-mentioned irradiated &quot; The two processing methods of the workpiece according to Item 9 are alternately formed in the direction in which the processing is easy to open or split, and 156646.doc 201221261 is formed to form at least two of the irradiated regions. Such as The processing of the workpiece according to any one of claims 5 to 8 forms the irradiated region 13 in a direction that is equal to the two different directions of the workpiece, and the method of dividing the workpiece. And the method of the object, and the method of dividing the workpiece processed by the method of any one of claims 5 to 12 along the segmentation starting point, wherein the system is opened or split The segmentation is added to form a segmentation 156646.doc
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