200912375 九、發明說明: 【發明所屬之技術領域】 發明領域 本發明係有關於一種雷射照射裝置及使用該雷射照射 5 裝置之雷射加工系統。 背景技術 過去 10 15 20 匕知有藉由對被加工物的期望領域照射雷射光 而進行加工之雷射加工裝置(雷射照射裝置)。例如,已知有 可在液晶顯示器等的製造中,作為對存在於玻璃基板上的 配線圖案或曝光用光罩上的無用殘留物等缺陷部進行修正 之設備的雷射修護裝置。 例如,專利文獻W特開平8-174242號公報)中,揭示有 具田射源、載置被加工物之加工台、微小鏡面陣列(微鏡陣 列)且藉由對微小鏡面陣列之多數鏡片角度進行⑽⑽ 控制來切換’而可錢加讀上形成任意圖案形狀的雷射 加工裝置。 …、而如專利文獻2(特開鹰6_35〇123號公報)所記載, 種田射加:η裝置,—旦在固定相對於微小鏡面陣列之雷 率降低之現象變波長’則會有雷射光的使用效 鏡陣:影===ΓΓ裝置’係藉顯微_ 心至破加讀上。由於微鏡陣列係等間 型鏡面的結構,故其反射出的雷射光會分散成 5 200912375 多數的繞射光。但,由於一般顯微鏡的後側數值孔徑很小, 故無法供分散成多數的繞射光完全射入。 例如,第8圖係可切換YAG雷射的第2高諧波(波長λ 2=532nm)與第3高諧波(波長λ 3=354.7nm)之雷射加工裝置 5 的繞射光角度分布之範例。即,將經微鏡陣列反射之繞射 光的角度分布(α、/3)標示於以射入之顯微鏡光軸502為中 心的角度平面501上者。 如圖示X記號所示,波長;13在光軸502附近具有1個繞 射階數504。相當於雷射光照射領域的小型鏡面傾斜成可朝 10 光軸502的方向反射雷射光,故靠近光軸502的繞射階數504 成為唯一且具有較大強度的繞射光。該繞射階數5〇4位於顯 微鏡的後側角孔徑503的範圍内,故雷射光之強度足以效率 良好地對被加工物照射。 另一方面,如圖示〇記號所示’一旦波長切換為入2, 15 則光軸502附近將沒有繞射階數,且在以相同角度遠離之位 置上存在有4個繞射階數505。因此,雷射之強度會因前述 多數繞射階數505而分散,並且不會射入顯微鏡之後侧角孔 徑503。雖然可改變相對於顯微鏡之入射角度而使丨個繞射 階數射入,但即使如此仍無法改善雷射光的使用效率。 2〇 專利文獻2中,針對前述問題記載有一種雷射加工裝置 (雷射照射裝置),且該雷射加工裝置係構造成使調變光投影 光學系統之光軸與多數波長光之繞射光大略共同的方向大 略一致。具體而言,依據雷射光的多數波長以及微鏡的排 列間隔,調整微鏡陣列的傾斜角,藉此將正反射光的反射 200912375 方向設定成各繞射光共同的方向後,使調變光投影光學系 統之光轴與其反射方向一致。 然而,前述習知雷射照射裝置有下述問題。 專利文獻2記載之技術中,由於有在調整微鏡的傾斜 5 角,故因波長光呈多數,而會有無法使用具泛用性的微鏡 陣列,需使用高價微鏡陣列的問題。 【發明内容】 發明揭示 本發明係有鑑於前述問題而作成者,其目的在於提供 10 即使雷射光的波長或微小鏡面陣列的傾斜角改變,亦可得 到良好的光使用效率的雷射照射裝置及使用該裝置之雷射 加工系統。 為解決前述課題,本發明之雷射照射裝置係採包含 有:雷射光源;藉由受到支撐且可動的偏向面,將從前述 15 雷射光源射出的雷射光偏向的光程偏向部;配置成可使前 述光程偏向部之偏向面相對於前述雷射光之光軸傾斜移 動,且可往前述光轴方向移動的偏向面移動機構;將以前 述光程偏向部偏向後之雷射光空間調變,且具有形成朝向 被照射面之ON光的多數微小鏡面的空間調變元件;將藉前 20 述空間調變元件形成之ΟN光投影至前述被照射面上的投 影光學系統的構造。 根據此發明,可藉由偏向面移動機構,使光程偏向部 之偏向面的相對於雷射光軸之傾斜度、以及光軸方向之位 置改變。因此,可使從雷射光源射出且藉偏向面偏向之雷 7 200912375 射光改變相對於空間調變元件之入射角以及入射位置。其 結果,例如,在雷射光源的波長被切換的情況下,或是在 因空間調變元件改變而改變了 ON狀態之微小鏡面的傾斜 角的情況下,可依據該等波長或傾斜角,設定適合各種情 5 況的入射角、入射位置。 本發明之雷射加工系統係採包含有:本發明之雷射照 射裝置;為了拍攝配置於前述雷射照射裝置之被照射面上 的被加工物,而與前述雷射照射裝置之前述投影光學系統 同軸地配置的拍攝光學系統;設置於前述拍攝光學系統之 10 成像位置的拍攝部;將藉前述拍攝部拍攝之影像進行影像 處理,來抽取前述被加工物之缺陷的影像處理部,且,該 雷射加工系統依據藉前述影像處理部抽取之缺陷的形狀, 調變驅動前述雷射照射裝置的前述空間調變元件,並將經 前述空間調變後之雷射光照射至前述被加工物,進行前述 15 被加工物的加工的構造。 根據此發明,由於使用本發明之雷射照射裝置,故具 有與本發明之雷射照射裝置同樣的作用效果。 發明效果 根據本發明之雷射照射裝置及使用該裝置之雷射加工 20 系統,可藉由偏向面移動機構使相對於空間調變元件及微 小鏡面之雷射光的入射角及入射位置產生變化,故即使雷 射光的波長或微小鏡面陣列的傾斜角改變,亦可得到良好 的光使用效率。 圖式簡單說明 200912375 第1圖係顯示本發明之實施態樣的雷射照射裝置及使 用該裝置之雷射加工系統的概略構造的含光軸之截面示意 說明圖。 第2A圖、第2B圖、第2C圖係說明本發明之實施態樣的 5 雷射照射裝置之空間調變元件的繞射現象的示意截面圖。 第3圖係顯示本發明之實施態樣的雷射加工系統之控 制單元的概略構造的功能方塊圖。 第4圖係說明本發明之實施態樣的雷射照射裝置之偏 向面移動機構的作用的示意說明圖。 10 第5圖係顯示本發明之實施態樣之第1變形例的雷射照 射裝置之偏向面移動機構的構造的示意說明圖。 第6圖係顯示本發明之實施態樣之第2變形例的雷射照 射裝置之光程偏向部以及偏向面移動機構的構造的示意立 體圖。 15 第7圖係顯示本發明之實施態樣之第3變形例的雷射照 射裝置之光程偏向部以及偏向面移動機構的構造的示意說 明圖。 第8圖係用以說明可切換波長之雷射加工裝置的繞射 光角度分布之一例的角度分布圖。 20 【實施方式】 實施發明之最佳態樣 以下,參照附加圖式說明本發明之實施態樣。在所有 的圖式中,即使實施態樣不同,亦對相同或相符之構件附 上相同符號,並省略共同之處的說明。 9 200912375 [第1實施態樣] 在此說明本發明之第1實施態樣的雷射照射裝置及使 用該裝置之雷射加工系統。 第1圖係顯示本發明之實施態樣的雷射照射裝置及使 5 用該裝置之雷射加工系統的概略構造的含光轴之截面示意 說明圖。第2A圖、第2B圖、第2C圖係說明本發明之實施態 樣的雷射照射裝置之空間調變元件的繞射現象的示意截面 圖。第3圖係顯示本發明之實施態樣的雷射加工系統之控制 單元的概略構造的功能方塊圖。 10 圖中的XYZ座標線係為了方便參考方向而設置於各圖 共同之位置關係者,垂直方向為Z軸,且水平面為XY平面, 而從Y轴負方向朝向Y轴正方向的方向與正視方向一致(以 下,其他圖亦相同)。 圖中表示光束的線係示意性地描繪對試樣的某一點照 15 射雷射光的情形。 本實施態樣之雷射加工系統10 〇係對被加工物照射雷 射光來進行修護加工的裝置。例如,LCD(液晶顯示器)的玻 璃基板或半導體晶圓基板等,藉光刻處理製程於基板上形 成有電路圖案等的被加工物中,檢測出例如配線部分短 20 缺、光阻露出等缺陷部時,本實施態樣之雷射加工系統100 可適用於缺陷部之除去等修護加工。 雷射加工系統100的概略構造如第1圖所示,係由雷射 光源50、加工頭20、加工頭移動機構31、載置台21、控制 單元22、顯示部30、及使用者介面32所構成。作為被加工 10 200912375 置於加工頭20下方所設 物之基板11在加工時,係水平地载200912375 IX. DESCRIPTION OF THE INVENTION: FIELD OF THE INVENTION The present invention relates to a laser irradiation apparatus and a laser processing system using the same. Background Art In the past, there has been known a laser processing apparatus (laser irradiation apparatus) which performs processing by irradiating laser light to a desired area of a workpiece. For example, a laser repairing device that can correct a defective portion such as a wiring pattern existing on a glass substrate or an unnecessary residue on an exposure mask in the manufacture of a liquid crystal display or the like is known. For example, Patent Document No. 8-174242 discloses a field source, a processing table on which a workpiece is placed, a micro mirror array (micromirror array), and a plurality of lens angles by a micro mirror array. Perform (10) (10) control to switch 'and can read and read the laser processing device to form an arbitrary pattern shape. In addition, as described in the patent document 2 (Japanese Patent Publication No. Hei 6-35-123), the seeding and gamma irradiation device has a laser beam that has a reduced lightning rate with respect to the micro-mirror array. The use of the mirror array: shadow === ΓΓ device 'by the microscopic _ heart to break plus read. Due to the structure of the inter-mirror mirror, the reflected laser light is scattered into most of the diffracted light of 200912375. However, since the numerical aperture of the rear side of the general microscope is small, it is impossible to completely inject the diffracted light which is dispersed in a large amount. For example, Fig. 8 is a diagram showing the angle distribution of the diffracted light of the laser processing device 5 of the second harmonic (wavelength λ 2 = 532 nm) and the third harmonic (wavelength λ 3 = 354.7 nm) of the switchable YAG laser. example. That is, the angular distribution (α, /3) of the diffracted light reflected by the micromirror array is indicated on the angle plane 501 centered on the incident microscope optical axis 502. As shown by the X mark, the wavelength 13 has one diffraction order 504 near the optical axis 502. The small mirror surface corresponding to the field of laser light irradiation is inclined so as to reflect the laser light in the direction of the optical axis 502, so that the diffraction order 504 close to the optical axis 502 becomes the only diffracted light having a large intensity. The diffraction order 5〇4 is located within the range of the rear side angular aperture 503 of the microscope, so that the intensity of the laser light is sufficient to efficiently illuminate the workpiece. On the other hand, as shown by the symbol ', once the wavelength is switched to 2, 15, there will be no diffraction order near the optical axis 502, and there are 4 diffraction orders 505 at positions away from the same angle. . Therefore, the intensity of the laser is dispersed by the above-described majority of the diffraction orders 505, and does not enter the side corner aperture 503 of the microscope. Although it is possible to change the incident angle with respect to the microscope so that one diffraction order is incident, even this does not improve the efficiency of use of the laser light. In Patent Document 2, a laser processing apparatus (laser irradiation apparatus) is constructed in which the optical axis of the modulated light projection optical system and the diffracted light of a plurality of wavelengths of light are configured. The general direction is roughly the same. Specifically, the tilt angle of the micromirror array is adjusted according to the majority wavelength of the laser light and the arrangement interval of the micromirrors, thereby setting the direction of the reflection of the specular reflected light to the direction common to the respective diffracted lights, and then shifting the modulated light. The optical axis of the optical system coincides with its direction of reflection. However, the aforementioned conventional laser irradiation apparatus has the following problems. In the technique described in Patent Document 2, since the tilt angle of the micromirror is adjusted, the wavelength of light is large, and there is a problem that a micromirror array having versatility cannot be used, and a high-priced micromirror array is required. SUMMARY OF THE INVENTION The present invention has been made in view of the above problems, and an object thereof is to provide a laser irradiation apparatus capable of obtaining good light use efficiency even when the wavelength of laser light or the tilt angle of a micro mirror array is changed. A laser processing system using the device. In order to solve the above problems, the laser irradiation apparatus of the present invention includes: a laser light source; and an optical path deflecting portion that deflects the laser light emitted from the 15 laser light sources by a supported and movable deflecting surface; And a deflecting surface moving mechanism that can move the deflecting surface of the optical path deflecting portion obliquely with respect to the optical axis of the laser light, and can move in the optical axis direction; and spatially modulate the laser light deflected by the optical path deflecting portion And a spatial modulation element having a plurality of minute mirror surfaces that form ON light toward the illuminated surface; and a structure of a projection optical system that projects the ΟN light formed by the spatial modulation element of the previous 20 onto the illuminated surface. According to the invention, the inclination of the deflecting optical axis of the optical path deflecting portion and the position of the optical axis direction can be changed by the deflecting surface moving mechanism. Therefore, the laser beam can be emitted from the laser light source and deflected by the deflecting surface. 7 200912375 The light is changed with respect to the incident angle and the incident position of the spatial modulation element. As a result, for example, in the case where the wavelength of the laser light source is switched, or in the case where the tilt angle of the micro mirror surface in which the ON state is changed due to the change of the spatial modulation element, depending on the wavelength or the tilt angle, Set the incident angle and incident position for each situation. The laser processing system of the present invention comprises: the laser irradiation device of the present invention; and the projection optics of the laser irradiation device in order to capture a workpiece disposed on the illuminated surface of the laser irradiation device a photographing optical system that is disposed coaxially with the system; an imaging unit that is disposed at 10 imaging positions of the imaging optical system; and an image processing unit that performs image processing on the image captured by the imaging unit to extract a defect of the workpiece, and The laser processing system modulates the spatial modulation element of the laser irradiation device by a shape of a defect extracted by the image processing unit, and irradiates the spatially modulated laser light to the workpiece. The structure in which the above-mentioned 15 workpieces are processed is performed. According to the invention, since the laser irradiation apparatus of the present invention is used, the same effects as those of the laser irradiation apparatus of the present invention are obtained. Advantageous Effects of Invention According to the laser irradiation apparatus of the present invention and the laser processing 20 system using the same, the incident angle and the incident position of the laser light with respect to the spatial modulation element and the micromirror surface can be changed by the deflection surface moving mechanism. Therefore, even if the wavelength of the laser light or the tilt angle of the micro mirror array is changed, good light use efficiency can be obtained. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic cross-sectional view showing an optical axis including a laser irradiation apparatus according to an embodiment of the present invention and a schematic configuration of a laser processing system using the apparatus. 2A, 2B, and 2C are schematic cross-sectional views illustrating a diffraction phenomenon of a spatial modulation element of the 5 laser irradiation apparatus according to an embodiment of the present invention. Fig. 3 is a functional block diagram showing a schematic configuration of a control unit of a laser processing system according to an embodiment of the present invention. Fig. 4 is a schematic explanatory view showing the action of the deflecting surface moving mechanism of the laser irradiation apparatus according to the embodiment of the present invention. Fig. 5 is a schematic explanatory view showing the structure of a deflection surface moving mechanism of the laser irradiation device according to the first modification of the embodiment of the present invention. Fig. 6 is a schematic perspective view showing the structure of the optical path deflecting portion and the deflecting surface moving mechanism of the laser irradiating device according to the second modification of the embodiment of the present invention. Fig. 7 is a schematic view showing the structure of the optical path deflecting portion and the deflecting surface moving mechanism of the laser irradiating device according to the third modified example of the embodiment of the present invention. Fig. 8 is an angular distribution diagram for explaining an example of the diffracted light angle distribution of the laser processing device capable of switching wavelengths. [Embodiment] BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings. In all the drawings, even if the embodiments are different, the same reference numerals are attached to the same or corresponding components, and the description of the common points is omitted. 9 200912375 [First Embodiment] A laser irradiation apparatus according to a first embodiment of the present invention and a laser processing system using the same will be described. Fig. 1 is a schematic cross-sectional view showing a laser irradiation apparatus according to an embodiment of the present invention and an optical axis including a schematic structure of a laser processing system using the apparatus. Fig. 2A, Fig. 2B, and Fig. 2C are schematic cross-sectional views showing the diffraction phenomenon of the spatial modulation element of the laser irradiation apparatus according to the embodiment of the present invention. Fig. 3 is a functional block diagram showing a schematic configuration of a control unit of a laser processing system according to an embodiment of the present invention. 10 The XYZ coordinate line in the figure is set to the common positional relationship of each figure for the convenience of the reference direction, the vertical direction is the Z axis, and the horizontal plane is the XY plane, and the direction from the negative direction of the Y axis to the positive direction of the Y axis and the front view The directions are the same (the other figures are the same below). The line showing the beam of light schematically depicts the situation in which a laser beam is incident on a point of the sample. The laser processing system 10 of the present embodiment is a device for irradiating a workpiece with a laser beam for repair processing. For example, in a glass substrate or a semiconductor wafer substrate of an LCD (Liquid Crystal Display), a workpiece such as a circuit pattern is formed on a substrate by a photolithography process, and defects such as a short wiring portion and a photoresist are detected, for example. In the case of the portion, the laser processing system 100 of the present embodiment can be applied to repair processing such as removal of defective portions. The schematic structure of the laser processing system 100 is shown in FIG. 1 by the laser light source 50, the processing head 20, the processing head moving mechanism 31, the mounting table 21, the control unit 22, the display unit 30, and the user interface 32. Composition. As the processed 10 200912375, the substrate 11 placed under the processing head 20 is horizontally loaded during processing.
置之載置台21上,且將缺4 轴正方向側)。、σ工面Ua(被照射面)朝向上側(Z ;·、光源50係修護加工用 4+ AA ^ 用的先源。本實施態樣中,雷 射光源的構造係採用由雷 振盪态1、耦合透鏡2、纖維3、 以及杈衫透鏡4所構成之構 苒绝仁疋,本實施態樣之投影透 鏡4係配置於加工頭20的内部。 雷射㈣器1係振錢長、輸出均已設定之雷射光,使 σ *去基板11上的軸者。例如,宜可剌可振盡脈衝 Κ)的彻雷射等作為雷射振盈器1。雷射振盡器i係呈可依據 修護對象切換多數振蘯波長的構造。 f射«器m電性地連接於控制單心,且依據來自 控制單元22的控制信號控制振盪。 輕合透鏡2係用以將從雷射振射出之雷射光光麵 15 合至纖維3的光學元件。 纖維3係在内部傳輸藉耦合透鏡2光耦合至纖維端面3a 的雷射光並導入加工頭20内後,作為雷射光6〇,使其從纖 維端面3b射出者。由於雷射光60係在纖維3内部傳輸後才被 射出,故即使雷射振盪器丨的雷射光呈高斯分布,亦會成為 2〇 光量分布均勻化的擴散光。 投影透鏡4係將投影倍率設定成可使纖維端面3b的影 像照射至後述空間調變元件6之調變領域的透鏡或透鏡 群。投影透鏡4係固定於加工頭20之外殼2〇a。本實施態樣 中,係以將投影透鏡4配置成使其光軸?1與2軸大略平行的 11 200912375 例子作為其中一例來說明,但配置位置不受限於此。 由於第1圖A示意圖,故投影光學系統中僅描緣軸上的 光束。雷射振盪器1雖沿著Z軸方向配置,但雷射振盪器1 的配置位置、姿勢等不受限於此,可藉由適當地配繞纖維 5 3而5又定為適當的配置位置、姿勢。又,亦可裝設用以使 纖,准之模(mode)安定的模態授亂器(m〇de scrambier)。 雷射光的均勻化設備亦可不使用前述纖維3,而改用其 他光學元件。例如,亦可為使用均質機(H〇m〇genizer)等的 構is·且該均質機包含使用複眼透鏡(Dy eye lens)、繞射元 10件、非球面透鏡、或萬花筒型桿狀者等各種構造。 加工頭20係將反射鏡面33(光程偏向部)、鏡面移動機 構34(偏向面移動機構)、空間調變元件6、投影光學系統8、 觀察用光源16、觀察用成像透鏡12、拍攝元件13等光學元 件、裝置等保持於外殼20a内的構造,且該外殼20a受到具 15有適當驅動設備的加工頭移動機構31保持住而可相對於栽 置台21往XYZ轴方向進行相對移動。 本實施態樣中,關於相對移動,係以藉由加工頭移動 機構31將加工頭20往與被加工面11a平行的X軸方向以及與 被加工面11a垂直的方向(Z轴方向)移動,且藉由載置台21 20 將基板11往Y轴方向移動的例子來說明。然而,相對移動並 不受限於此,可採用例如,加工頭20往Z軸方向移動且栽置 台21往XY軸方向移動,或載置台21經固定且加工頭2〇往 XYZ軸方向移動等適當搭配的相對移動。 加工頭移動機構31中宜使用例如,滚珠螺桿、線性馬 12 200912375 達等。又,在對焦等微量移動方面亦可搭配壓電元件等。 反射鏡面33係藉由偏向面33a將從雷射光源50之投影 透鏡4射出的雷射光6〇之光軸Ρι作為朝向空間調變元件6的 光軸P2反射,並將該雷射光6〇作為雷射光61,使其偏向成 5可延著光軸P2行進者,且,反射鏡面33受到鏡面移動機構 34支揮而可動。 鏡面移動機構34係由使反射鏡面33相對於光軸Ρι傾斜 移動的鏡面傾斜移動部34a、及使反射鏡面33往延著光軸Pi 的方向平移移動的鏡面平移移動部34b所構成。鏡面傾斜移 動434a與鏡面平移移動部34b各自電性地連接於控制單元 22’可藉由來自控制單元22的控制信號,控制反射鏡㈣ 的傾斜移動方向、傾斜移動角度、以及平移移動量。 藉此’可變更光轴p2的方向以及空間調變元件6上 轴的位置。 5 * $間調變元件6,係將以偏向面33a偏向後之雷射光61 :間·者’且係由作為則、鏡㈣狀DMD(數位微鏡裝 :構成。即’空間調變元件6如第2A圖所示,係相對於 二準面M以旋細為中心,且可做到僅傾斜角度_多數 ^鏡面⑽例如,於兩邊駿XH的矩形狀調變領域内, 邊的延伸方向作為排列方向二維地排列著。 微小鏡面6a之傾斜心的大小雖會因裝置的構造等而 不同’但可從例如約1G。〜約16。的角度範圍當中選 ^面Μ可配置於適當方向,本實施態樣中,係以將微^ a朝向Ζ軸方向反方向側,並平行地配置於平面的 13 200912375 例子作為其中一例來說明。 空間調變元件6的各微小鏡面6a係藉由依據來自控制 單元22的控制信號產生的靜電電場而旋轉,例如,在on狀 態下,從基準面Μ旋轉+火圖示逆時針旋轉),且在〇FF狀態 5下,從基準面Μ旋轉-叭圖示噸時針旋轉)。以下,將藉由 ON狀態之微小鏡面6a反射的光稱為〇Ν光,並將藉由0FF 狀態之微小鏡面6a反射的光稱為〇砰光。本實施態樣中, ON光62(參照第1圖)的光軸p3被設定成大略平行於z軸方 向。 10 各微小鏡面6a的位置可藉由長度W之邊的列編號m、長 度Η之邊的行編號n(m、η係〇以上之整數)以(m,n)表示,且 可從微小鏡面6a的排列間隔換算成基準面M上的位置座 標。 投影光學系統8係構成可將藉空間調變元件6空間調 15變,且朝向固定方向反射之ON光62所產生之影像以倍率/5 成像於基板11之被加工面Ua上的成像光學系統的光學元 件群。投影光學系統8的空間調變元件6側配置有成像透鏡 8A,且基板U侧配置有物鏡8B。 本實施態樣中,倍率相異的多數個物鏡8B受到迴轉機 2〇構保持而可切換。因此,藉由使迴轉機構旋轉來切換物鏡 8B ’可變更投影光學系統8的倍率冷。以下,只要未特別事 先°兒明’物鏡8B係指用以構成投影光學系統8而選擇的透 鏡。 本實施態樣中,成像透鏡8A的光軸P4係平行地被置於 200912375 x軸方向,且物鏡8B的光軸p5係平行地被置於2軸方向。 因此,在空間調變元件6與成像透鏡8A之間,設有可反 射ON光62,並使之延著光軸匕射入的鏡面7。然後,在成 像透鏡8A與物鏡8B之間’設有可反射穿透成像透鏡8A的 5光,並使之延著光軸P1 2 3 4射入的半透鏡9。 投影光學系統8的投影倍率沒可依據被加工面ila上的 所需加工精度適當地設定。例如,設定成使調變領域全體 之尺寸為WxH的影像可在被加工面lla上變為w,χΗ’的 倍率。 0 另外’成像透鏡8Α的數值孔徑(ΝΑ)係採不會使光射入 的尺寸,且該光係指作為〇1^光63而被反射者。 觀察用光源16係可產生用以照亮被加工面lla上之可 加工領域内的觀察用光80的光源,且設置於半透鏡9與物鏡 8B之間的光程側方向。 15 1 在半透鏡5與物鏡8B之間的光程上,相對於觀察用光源 2 16的位置設有半透鏡14,且該半透鏡14係可供以半透鏡9反 射後之ON光62穿透且朝向物鏡83反射觀察用光8〇者。然 後’在觀察用光源16與半透鏡14之間,設有可將觀察用光 80聚光成適當直徑之照明光束的聚光透鏡15。 3 0 觀察用光源16可採用例如,產生可見光之氙弧燈 4 (Xenon arc lamp)或LED等適當光源。 5 觀察用成像透鏡12(拍攝光學系統)係於半透鏡9之上方 側’與物鏡8B的光輛I同軸地設置者。觀察用成像透鏡12 係用以將從觀察用光8〇所照亮之被加工面lla反射,並藉由 200912375 物鏡8B聚光的光成像於拍攝元件13(拍攝部)之拍攝面 光學元件。 拍攝元件13係將成像於拍攝面上的影像進行光電轉換 者,係由例如CCD等所構成。以拍攝元件13進行光電轉換 5後的影像信號會送出至電性地連接於拍攝元件13的控 元22。 控制單元22係用以控制雷射加工系統1〇〇之動作者如 第3圖所示,係由影像擷取部4〇、資料記憶部43、空間調變 7G件驅動部41、裝置控制部42、移動機構控制部35、以及 10 影像處理部44所構成。 控制單元22的裝置構造在本實施態樣中,係由以 CPU、記憶體、輸出輸入部、外部記憶裝置等構成之電腦 與適當硬體之搭配所構成。資料記憶部43係藉由使用該電 腦的記憶體或外部記憶裝置來實現。又,其他構造係藉由 15以CPU執行對應各控制功能、處理功能所作成之程式來實 現。 影像擷取部40係擷取以拍攝元件13取得之影像信號來 得到被加工面11a的二維影像者。所擷取之二維影像會被送 出並顯示於由監視器等所構成之顯示部30,並且同時作為 2〇影像資料150被送出並記憶於由影像記憶體所構成之資料 記憶部43。 空間調變元件驅動部41係根據以影像處理部44生成之 加工資料’來控制空間調變元件6的各微小鏡面以的 ΟΝ/OFF狀態者。 16 200912375 根據來自具有例如―鍵盤、 1田的#作輸人設備的 來控制雷射加工系統71面32的操作輸入, 接於影像擁取部40、空間 件^置控制部42電性地連 機仙、雷射«器加工頭移動 而可控制各元件的動作或動作日^。6、移動機構控制部35, 移動機構控制部35係根據 10 15 入或裝置控制部42的控制信=介面32的操作輸 鏡面傾斜移動職機⑽ 影像處理部44係叫出記恃 者 15。並施行適當的影像處理者:且:料 缺陷抽取部45與加工資料生成部%。包3有 缺陷抽取和係相對於μ_ι5() 理,並將加工雜:纽作為 “取處 資料生成部46者。 ^像^⑸’送出至加工 —該缺陷抽取處理亦可使用眾所周知的所謂缺陷抽㈣ :法。例如,可在得_取得彡像㈣與事先記憶之正 吊被加工面Ua之圖案影像資料的亮度差分後,從以某閣值 將其差分資料二值化後的資料當中抽取缺陷。 加工資料生成部46係可生成控制空間調變元件6之各 微小鏡油之⑽聊的加工資料152(調變資料),以使⑽ 光62可依據從祕抽取部45所㉔之加工資訊照射至 被加工面1 la者。 除了雷射光源50、 以上說明的雷射加工系統1〇〇當中 17 200912375 反射鏡面33、鎊面鉍知 率统8 η 動機構34、空間調變元件6、投影光學 糸統8、以及影像處理部 "九予 造,亦構成有卿元22所構成之構 巧由对狀射裝置2〇〇,且該雷 將以空間調變元件6空間調變後m #置200係 lla上去“ Ί周變後之田射光照射至被加工面 上者。此種雷射照射裝置2〇〇亦 100獨立的裝晋估田 下為攸雷射加工系統 狀之影像資料進為接收對應加工形 各貝Τ十進仃雷射加工的雷射加工 途方面亦可作, 衣置使用,其他用 用。 Μ例如,错魏光投影之影像投影裝置等使 10 15 20 接著,說明雷射加工系統100的動作。 第4圖係說明本發明之實施態樣的雷射照射裝置 向面移動機構的作用的示意說明圖。 ,以雷射加工系統100進行雷射加工日夺,如第項所示, 首先,將作為被加工物之基板u載置於栽置台Μ上。 接著,藉由加工頭移動機構31移動加工頭2〇,設定好 最初的加工位置後,取得被加卫面lla的可加卫領域的影 像。即,點亮觀察用光源16,使觀察用光8〇產生。觀察用 光8〇被半透鏡14反射一部分後,該反射光會經由物鏡83聚 光而照亮被加工面11 a上的可加工領域。 受到被加工面11a反射後之反射光會經由物鏡祀聚 光’且部分反射光會穿透半透鏡14。然後,經由半透鏡9使 部分反射光更進一步地穿透後,會導向觀察用成像透鏡 12。射入觀察用成像透鏡12的光會成像於拍攝元件13的拍 攝面。 18 200912375 拍攝元件13會將所成像之被加 + 加工面1 la的影像進行光 电轉換,並送出至影像擷取部4〇。 之影像信號施行雜 示部30。又,依據 的影像信號轉換成 如此一來,即可取 影像擷取部40會依據必要性將送出 訊除去、亮度修正等處理,並顯示於顯 5裝置控制部42的控制信號,將適當時機 影像資料150,並記憶於資料記憶部。 付被加工面11 a的可加工領域的影像。 接著,影像處理部44中,會蔣々& τ將尤憶於資料記憶部4 3的 影像資料150讀取至缺陷抽取部45並進行缺陷抽取。然後, Η)在判定出抽取之缺陷的種類或尺寸等後,判斷該缺陷是需 進行修護加工的缺陷時,會作為缺陷影像資料ΐ5ΐ送出至加 工資料生成部46。 被加工面11a的可加工領域與空間調變元件⑽調變領 域係藉由彳xw光料統8而呈共輛關係,且由於投影光學系 統8的倍率為石,故將可加工領域上的位置座標設為^ 倍,即可使其對應空間調變元件6的調變領域上的位置。 如此一來,加工資料生成部46中,從缺陷影像資料151 可決定為了將ON光62照射至缺陷影像資料151所表示之被 加工面11a上的各位置而需控制在⑽狀態的微小鏡面6a, 20並可生成驅動空間調變元件6使該等微小鏡面6a呈ON狀 態’且使其他微小鏡面6a呈〇ff狀態的加工資料152。例如, 依據各微小鏡面6a的位置(m,n),作為對應〇N狀態為丨且 OFF狀態為0之數值的表格資料,來生成加工資料丨52。 所生成之加工資料152會送出至空間調變元件驅動部 19 200912375 41 〇 元件驅動料會根據裝置㈣部如 唬與所送出之加工資料152,來# 工制k 小鏡物的傾斜角 來控制空間調變元件6的各微 5 10 15 20 邊的=著’裝置控制部42會對雷射振盈器1送出使雷射光振 2制信號’並根據依基板11所事先選擇的照射條件 波長射=1振綱光。雷射光的振盪條件可舉例如, 我先輸出、振盪脈衝寬度等。 端面=盪之雷射光經_合透鏡2_合於_3的纖維 a後,會作為雷射光60從纖維端面补射出且該 光60係光強度分布呈大略均自化的發散光。 雷射光6〇會藉由投影透鏡4沿著光糾行進,且被反射 鏡面33的偏向面33a反射。然後,作為雷射光咖著光轴p2 订進,且投影至空間調變元件6上後,再被空間調變元件6 上的各微小鏡面6a反射。 因此,會事先驅動鏡面移動機構34,使偏向面33a的相 對於光軸Pl之傾斜度(以下,僅稱之為偏向面33a的傾斜度) 與光轴P,方向的位置(以下,僅稱之為偏向面Ma的光轴方向 位置)’可供作為反射鏡面33之反射光的雷射光“在被空間 調變元件6的ON狀態之微小鏡面&反射時,得以有效地射 入投影光學系統8。 該偏向面33a的傾斜度以及光軸方向位置係根據使用 者介面32的操作輸入以及裝置控制部42所收集之雷射振盪 器1的波長資訊等,藉由控制單元22的移動機構控制部35演 20 200912375 算出來的。 被傾斜角呈OFF狀態之微小鏡面6a反射的OFF光63,會 反射至成像透鏡8A的NA範圍外。 被傾斜角呈ON狀態之微小鏡面6a反射的on光62,會 5 沿著光軸P3行進,且在受到鏡面7反射後,改沿著光軸P4行 進’而在射入成像透鏡8A並聚光後,將抵達半透鏡9,然後 再被半透鏡9反射。 被半透鏡9反射之ON光62會沿著光軸P5行進,並藉由 物鏡8B成像於被加工面1 la上。 10 如此一來,以加工資料152為依據的藉on光62所產生 之調變領域影像會投影至被加工面11a上。其結果,〇N光 62會照射於被加工面11&的缺陷而可除去缺陷。 到此完成1次的雷射加工。 該加工後,藉由拍攝元件13再度取得被加工面Ua的影 15 像,並依據必要性重複前述步驟,對未除去部再度進行雷 射加工’或是’移動可加工領域對其他部分進行雷射加工。 接著,說明本實施態樣中,用以使ON光62可有效地射 入投影光學系統8並投影至被加工面1 la的偏向面33a的傾 斜度的條件。 20 空間調變元件6中,由於微小鏡面6a係呈規則性地排 列,故ON光62的光強度分布係藉由微小鏡面如所產生之繞 射現象來決定。 例如,如第2A圖所示,雷射光61相對於空間調變元件6 的基準面Μ以入射角θ()=2ίζ)射入後,相對於基準面M朝圖示 21 200912375 逆時針旋轉為僅傾斜角度多的ON狀態之多數微小鏡面6a之 反射光的ON光62會產生夫朗和斐繞射(Fraunh〇fer diffraction)70與繞射71。ON光62的光強度分布可摺積 (convolution)該等繞射光而獲得。 5 夫朗和斐繞射70取決於微小鏡面6a的孔徑,且在微小 鏡面6a的正反射方向(本例中為Z軸負方向)具有具峰值之釣 鐘型光強度分布。 另一方面,繞射71係呈由微小鏡面6a之排列間隔與雷 射光61之波長決定的離散性分布。即,雷射光61的相對於 10 基準面Μ之正反射光(本例中係相對於z軸負方向朝圖示順 時針旋轉角度θ〇的方向)會產生0階折射光d〇,且在單一取決 於微小鏡面6a之排列間隔與雷射光61之波長的相異繞射角 方向會產生N階繞射光dN(但是,N=l,2,...)。 此時’在繞射71之任一階數的繞射光方向與夫朗和斐 15 繞射7〇之峰值強度方向呈大略一致的狀態下,只要可射入 投影光學系統8的話,被摺積之光強度分布會變大,故可提 高繞射效率。因此,可提高光使用效率。 例如,第2A圖的情形中’夫朗和斐繞射70之峰值強度 方向相對於投影光學系統8的光軸方向呈一致,且繞射71的 20 3階繞射光d3、4階繞射光d4分別僅傾斜角度θ3、θ4(但是,θ4 $θ3)時,至少任一之繞射光可包含在投影光學系統8的孔徑 角範圍内,故可提高繞射效率’並實現良好的光使用效率。 夫朗和斐繞射70之峰值強度方向係由入射角以及微 小鏡面6a之傾斜角0所決定’且繞射71之繞射角係由微小鏡 22 200912375 面6a之排列間隔與雷射光61之波長所決定,故藉由從裝置 控制σΜ2取件該等資訊,移動機構控制部35可判定夫朗和 斐繞射70之峰值強度方向與任_之繞射光方向使否有進入 投影光學系統8的孔徑角範圍内。 5 任一之繞射光方向均未進入投影光學系統8的孔徑角 範圍内時’移動機構控制部35會令偏向面❿傾斜移動,使 夫朗和斐繞射70之峰值強度方向與任一之繞射光方向至少 有進入投景戌學线8的孔彳“範圍内,且有可能與投影光 學系統8的光轴一致。 10 例如,如第2Β圖中虛線所示,藉由鏡面移動機構34改 變偏向面33a的傾斜度,變更成使雷射光61Α相對於基準面 Μ以入射角(θ〇+ΔΘ)射入。各繞射光的繞射方向會依據該入 射角的變化而產生變化。因此,藉由適當地設定Δθ,可做 到例如’使4階繞射光ο#之繞射方向與投影光學系統8之光 15 軸方向一致的動作。 此時’相對於微小鏡面以之正反射方向亦產生變化, 故夫朗和斐繞射70之峰值強度方向亦產生變化,因此,實 際上可設定ΔΘ的值,使各繞射方向均可進入投影光學系統 8的孔徑角範圍内。 20 在變更雷射振盪器1的振盪波長時,宜依據其波長來進 行前述偏向面333之移動。 例如’如第2C圖所示,藉由空間調變元件6射入短波長 之雷射光61Β後’夫朗和斐繞射70雖與第2Α圖的情形相 同,但繞射71會依據波長之變化,在基準面Μ的正反射方 23 200912375 向產生〇階繞射光e〇,且在與第2A圖之高階繞射光相異的繞 射方向產生N階繞射光以(但是,N=1,2,.··)。然後,具有最 接近彳又影光學系統8之光軸方向的繞射方向的繞射光會成 為例如,與投影光學系統8之光軸呈角度心的6階繞射光“, 5 故光使用效率與第2A圖不同。 因此,藉由依據該角度Θ6移動偏向面33a,即使雷射振 盪器1的振盪波長改變,亦可得到良好的繞射效率。 接著舉出數值例來說明偏向面33a的傾斜度的角度設 定。 0 數值例1顯示於表1。數值例1係在微小鏡面6a的排列間 隔為19.05 μ m,且微小鏡面6a的〇N狀態之傾斜角沴為 ^15.3deg的情況下,令雷射光61之波長為266nm、355nm、 532nm時的設定例。在此,各波長係對應YAG雷射的第2高 諧波、第3高諧波、第4高諧波。 5 表1分別顯不有相對於各波長之1階繞射光的繞射角 (deg)、最接近投影光學系統8之光轴p3的繞射光的繞射階 數、空間調變元件6的相對於基準面5^之入射角θ〇的設定 值、從夫朗和斐繞射的強度分布與繞射光的摺積所算出的 繞射效率(%)、投影光學糸統8的相對於光軸ρ3之角度(deg)。 20 表1 波長(nm) 繞射角(deg) 繞射階數 對空間調變 元件之入射 角(deg) 繞射效率^ (%) 投影光學系統 的相對於光軸 之角度(deg) 數值例1-a 266 0.80 卜261 30.8 65 0.08 數值例1-b 355 1.07 ~~19 30.9 57 0.70 數值例1-c 532 1.60 13 — 30.7 85 0.17 從表1可彳于知,依據各波長將對空間調變元件6之入射 24 200912375 角分別設定成30.8deg、30.9deg、30.7deg,可令繞射效率達 57%以上。此時,最接近光軸P3的繞射光的繞射階數分別為 26、19、13,且相對於光軸P3之角度為〇.〇8deg、〇.7〇deg、 0.17deg ’故依據最大值0.7deg,令投影光學系統8的ΝΑ為 5 0.012以上,可使各波長之繞射光射入投影光學系統8的孔 徑角範圍。 接著’數值例2顯示於表2。數值例2係在微小鏡面6a的 排列間隔為24// m,且微小鏡面6a的ON狀態之傾斜角0為 _14.0deg的情況下,令雷射光61之波長為330nm、440nm、 10 660nm時的設定例。在此,各波長係對應YAG雷射的第2高 諧波、第3高諧波、第4高諧波。 表2分別顯示有與表1相同的繞射角(deg)、繞射階數、 入射角θ〇的設定值、繞射效率(%)、相對於光轴p3之角度 (deg)。 15 表2 波長(nm) 繞射角(deg) 繞射階數 對空間調變 元件之入射 角(deg) 繞射效率 (%) 投影光學系統 的相對於光軸 之角度(deg) 數值例2-a 330 0.798 24 28.0 83 0.15 數值例2 -b 440 1.05 18 27.9 87 0.07 數值例2-c 660 1.58 12 27.8 91 0.017 從表2可得知,依據各波長將對空間調變元件6之入射 角分別設定成28.0deg、27_9deg、27.8deg,可令繞射效率達 83%以上。此時,最接近光軸p3的繞射光的繞射階數分別為 24、18、12,且相對於光軸P3之角度為〇.15deg、0.07deg、 20 〇.〇17deg,故依據最大值0.15deg,令投影光學系統8的ΝΑ 為0·003以上,可使各波長之繞射光射入投影光學系統8的 25 200912375 孔控角範圍。 此種偏向面33a的傾斜移動亦可適用於針對例如,在交 換空間調變元件6時’因空間調變元件6的製造差異而使微 小鏡面6a的ON狀態之傾斜角產生變化的情況的調整。以表 5 3所示之數值例3來朗針對該情況的調整。 數值例3係在微小鏡面6a的排列間隔為17 9//m,且雷 射光61之波長為355nm的情況下,微小鏡面如的〇]^狀態之 傾斜角卢變化成卢=15.〇deg、i4.97nm的範例。微小鏡面6a的 傾斜角可藉由以預定角度射入基準光並測定反射光的抵達 10 位置,來實驗性地求得。 表3連同ON狀態之微小鏡面63的傾斜角多,顯示有與表 1相同的繞射角(deg) '繞射階數、入射角0〇的設定值、繞射 效率(%)、相對於光軸P3之角度(deg)。 表3 波長 (nm) 繞射角 (deg) 繞射階數 對空間調變 元件之入射 角(deg) 繞射效 率(%) ON狀態之微 小鏡面的傾 斜角(deg) 投影光學系統 的相對於光軸 之角度(deg) 數值例3-a 355 1.14 18 30.0 80 15.00 0.28 數值例3 -b 355 1.14 18 30.0 73 14.97 0.28 數值例3-c 355 1.14 18 29.5 80 H 14.97 0.71 15 表3的數值例3-a、3-b顯示出,在固定為入射角〇〇=3〇deg 的情況下,即使傾斜角^僅變化〇.〇3deg,亦會使繞射效率變 化7%。 數值例3-c顯示出,將偏向面33a傾斜移動〇.5deg’即可 恢復繞射效率,即使是^=14.97deg的空間調變元件6,亦可 20 與^15deg的空間調變元件6同樣得到80%的繞射效率。 另外’僅以反射鏡面33的傾斜移動變更偏向面33a的傾 26 200912375 斜度的話,雷射光61的相對於空間元件6之入射位置將會偏 離。本實施態樣中,鏡面移動機構34包含有鏡面傾斜移動 部34a與鏡面平移移動部34b ’故搭配反射鏡面33的平移移 動,可使雷射光61正確地射入投影光學系統8的光軸上。 5 例如,如第4圖所示,在偏向面33a被保持於鏡面傾斜 移動部34a,使與光軸匕之交點Q成為傾斜移動中心的情況 下,一旦從對空間調變元件6之入射角係呈角度θ〇的反射鏡 面33Α的狀態僅旋轉角度(ΔΘ/2) ’而傾斜移動至反射鏡面 33Β的位置的話,則來自雷射光源5〇之雷射光61的相對於空 10間调變元件6之基準面Μ之入射角會變成角度(Θ+ΔΘ),但根 據到空間調變元件6的距離,反射光有時會偏離空間調變元 件6,或是偏離投影光學系統8的有效範圍。 此時,藉由鏡面平移移動部34b,使反射鏡面33Β往光 軸Pl之方向僅平移移動例如距離L,而移動至反射鏡面33(: 15的位置,即可使反射鏡面33C之反射光正確地射入與反射鏡 面33A之反射光相同的位置。 根據此種雷射加工系統1〇〇,藉由可藉鏡面移動機構34 相對於光軸PJS斜移動,並且可往光軸匕方向移動的偏向 面33a偏向來自雷射光源5〇之雷射光61,來改變相對於空間 20調變元件6之基準面Μ以及ON狀態之微小鏡面以的入射 角,即可對空間調變元件6照射不改變入射位置的雷射光 61。因此,可在不改變微小鏡面〜的01^狀態之傾斜角的情 況下’使藉微小鏡面6a之孔徑所產生之夫朗和斐繞射7〇與 藉微小鏡面6a之排列間隔所產生之繞射71的繞射方向與投 27 200912375 影光學系統8的孔徑角範圍—致。复姓 系統8’且賴°工_啦軸if光學 因此,依據雷射振盪器i的振麵長改㈣照射。 對於空_變元件6之人射肖, 以射光61的相 化所產生之光使収率的變化。糟田射光61的波長變 又,即使存切因”調變元件⑽ =面6_狀態之傾斜_,亦可依== 用2=肖’難雷射細U㈣,觀到使光使 10 接著,說明本實施態樣之第1變形例。 第5圖係顯示本發明之實施態樣之第!變形例的雷射照 射裝置之偏向面移動機構的構造的示意說明圖。 本變幵v例包含有第5圖所示之鏡面移動機構36(偏向面 移動機構),以取代前述實施態樣的鏡面移動機構料。以 15下,將以與前述實施態樣相異之處為中心來說明。 鏡面移動機構36係由與鏡面移動機構34相同的鏡面傾 斜移動部34a、鏡面平移移動部34b所構成,且將反射鏡面 33女裝成可以其端部的點g為中心來傾斜移動。又,鏡面移 動機構36電性地連接於控制單元22的移動機構控制部35。 0 此時,在考慮偏向面33a上的光軸的反射位置與點g之 間的距離的情況下,Z軸方向的平移移動量可決定成與前述 實施態樣相同,且可與前述實施態樣同樣地使偏向面33a傾 斜移動以及平移移動。 接著’ s兒明本實施態樣之第2變形例。 28 200912375 第6圖係顯示本發明之實施態樣之第2變形例的雷射照 射裝置之光程偏向部以及偏向面移動機構的構造的示意立 體圖。 本變形例包含有第6圖所示之反射鏡塊37(光程偏向 5部)、鏡面移動機構38(偏向面移動機構),以取代前述實施 態樣的反射鏡面33 '鏡面移動機構34。以下,將以與前述 實施態樣相異之處為中心來說明。 反射鏡塊37如第6圖所示,在與χγ平面平行之安裝面 37a相反側的面上,往Υ軸方向並列設置有/χ平面内之傾斜 ίο度與z軸方向之咼度均相異的偏向面37八、37B、37C。 鏡面移動機構38係由往圖示¥軸方向延伸安裝於未圖 示之外殼的滑件導座38b、與固定於反射鏡塊37之安裝面 37a’且设置成可在滑件導座38b上往圖示γ轴方向移動的滑 件38a所構成的單軸移動機構。 15 鏡面移動機構38電性地連接於控制單元22的移動機構 控制部35,且可藉由移動機構控制部35的控制信號,往γ 軸方向階梯狀地移動。 本變形例中,係依據例如雷射光源5〇的3個波長久a、 入B、Ac’將偏向面37A、37B、37C的相對於Z軸之傾斜度、 20 z軸方向之位置設定成最適當的值。然後,每當藉由裝置控 制部42切換雷射振盪器丨的振盪波長,例如,從波長人a切 換成波長Ac時,反射鏡塊37會往γ軸方向移動,使偏向面 37C代替偏向面37A來反射雷射光61。 如此一來,根據本變形例,在事先將偏向面之傾斜量 29 200912375 限定成多數的情況下,無需在每次切換時進行人 算,而可迅速地進行偏“的設定4,由於不會相對= 該偏向面進行傾斜移動,故可使偏向面移動機構的構造簡 5 10 15 20 面以平行於y軸的1個軸為 但亦可為使各偏向面適當 另外,第6圖中顯示出各偏向 中心來改變傾斜角的形狀範例, 地往Z軸方向移動的形狀。 接著,說明本實施態樣之第3變形例。 第7圖係顯示本發明之實施態樣之第3變形例的雷射照 射#置之絲偏向部以及偏向面移動機構的構造的示意說 錢形例包含有第7圖所示之反射鏡塊39(光程偏向 部)、鏡面移動機構48(偏向面移動機構),以取代前述實施 態樣的反射鏡面33、鏡面移動簡34。以下,將以與前述 實施態樣相異之處為中心來說明。 反射鏡塊39如第7圖所示,在與χγ平面平行之安裝面 相反側的面上,往χ軸方向並列設置有狀平面内之傾斜 度與Ζ轴方向高度均相㈣偏向 面 39Α、39Β、39C。 一 ±移動機構48係、由往圖示X軸方向延伸安裝於未圖 丁之卜成的q件導座48b、與於Ζ軸正方向側包含有固定反 :兄鬼之各偏向面之内面側之安裝面他的固定面饭, 且設置成可在滑仕道十 〇〇 導座48b上往X軸方向移動的滑件48a所 構成的單轴移動機構。 兄移動機構48電性地連接於控制單元22的移動機構 30 200912375 控制部35,b -r -丄 可猎由移動機構控制部35的控制信號,往γ 抽方向階梯狀地移動。 軸方向之 > 卜第圖中顯不出各偏向面的Ζ 幵m 7置雨度朝向Χ軸正方向階梯狀地增大而形成的 移動值亦可為各偏向面的配置高度適當地往ζ軸方向 的形狀,例如,可形成為在ζχ截面呈鉅齒狀的形狀。 方。ρ形例相對於前述第2變形例’係偏向偏向面之配置 的面之移動方向者,且具有與前述第2變形例同樣 卜如述說明中,係以藉由移動機構控制部控制偏 =移動機構之傾斜移動以及平移移動的移動量的例子來 °、明,但偏向面移動機構亦可做成以機械性工作台等構 成,且可藉由手動進行傾斜移動以及平移移動。It is placed on the mounting table 21 and will be missing the positive side of the 4-axis). The σ working surface Ua (irradiated surface) faces the upper side (Z; ·, the light source 50 is the source for 4+ AA ^ for repair processing. In the present embodiment, the structure of the laser light source is controlled by the lightning oscillation state 1 The projection lens 4 of the present embodiment is disposed inside the processing head 20, and the coupling lens 2, the fiber 3, and the armor lens 4 are arranged. The laser (four) device 1 is long and output. The laser light has been set so that σ* goes to the axis on the substrate 11. For example, a laser or the like can be used as the laser oscillator 1. The laser vibrator i is a structure that can switch a majority of the vibrating wavelength depending on the object to be repaired. The device is electrically connected to the control unit and controls the oscillation in accordance with a control signal from the control unit 22. The light-fitting lens 2 is an optical element for bonding the laser beam surface 15 from the laser to the fiber 3. The fiber 3 internally transmits the laser light that is optically coupled to the fiber end face 3a by the coupling lens 2, and is introduced into the processing head 20, and then emitted as laser light 6 从 from the fiber end face 3b. Since the laser light 60 is emitted after being transmitted inside the fiber 3, even if the laser light of the laser oscillator has a Gaussian distribution, it will become a diffused light in which the light amount distribution is uniform. The projection lens 4 sets the projection magnification so that the image of the fiber end surface 3b is irradiated to a lens or a lens group in the modulation domain of the spatial modulation element 6 to be described later. The projection lens 4 is fixed to the outer casing 2A of the processing head 20. In this embodiment, is the projection lens 4 arranged such that its optical axis? 1 is substantially parallel to the 2 axes. The 200912375 example is described as an example, but the arrangement position is not limited thereto. Due to the schematic view of Fig. 1A, only the beam on the edge axis is drawn in the projection optical system. Although the laser oscillator 1 is disposed along the Z-axis direction, the arrangement position, posture, and the like of the laser oscillator 1 are not limited thereto, and can be appropriately arranged by appropriately arranging the fibers 53 and 5 ,posture. Further, a modal discriminator (m〇de scrambier) for stabilizing the fiber and the mode can be installed. The laser light homogenizing apparatus may also use other optical components instead of the aforementioned fibers 3. For example, it is also possible to use a homogenizer (H〇m〇genizer) or the like and the homogenizer includes a Dy eye lens, a diffraction element 10, an aspheric lens, or a kaleidoscope type rod. And other structures. The processing head 20 is a mirror surface 33 (optical path deflecting portion), a mirror moving mechanism 34 (biasing surface moving mechanism), a spatial modulation element 6, a projection optical system 8, an observation light source 16, an observation imaging lens 12, and an imaging element. The optical element, the device, and the like are held in the outer casing 20a, and the outer casing 20a is held by the machining head moving mechanism 31 having a suitable driving device, and is relatively movable in the XYZ-axis direction with respect to the planting table 21. In the present embodiment, the relative movement is performed by moving the machining head 20 in the X-axis direction parallel to the workpiece surface 11a and the direction perpendicular to the workpiece surface 11a (Z-axis direction) by the machining head moving mechanism 31. The example in which the substrate 11 is moved in the Y-axis direction by the mounting table 21 20 will be described. However, the relative movement is not limited thereto, and for example, the processing head 20 may be moved in the Z-axis direction, and the planting table 21 may be moved in the XY-axis direction, or the mounting table 21 may be fixed and the processing head 2 may be moved in the XYZ-axis direction. The relative movement of the appropriate match. It is preferable to use, for example, a ball screw, a linear horse 12 200912375, etc. in the machining head moving mechanism 31. In addition, a piezoelectric element or the like can be used for a small amount of movement such as focusing. The mirror surface 33 is reflected by the deflecting surface 33a from the optical axis P of the laser light 6 emitted from the projection lens 4 of the laser light source 50 toward the optical axis P2 of the spatial modulation element 6, and the laser light 6 is used as the laser beam 6 The laser light 61 is deflected by 5 to extend the optical axis P2, and the mirror surface 33 is movable by the mirror moving mechanism 34. The mirror moving mechanism 34 is composed of a mirror tilt moving portion 34a that tilts the mirror surface 33 with respect to the optical axis, and a mirror translation moving portion 34b that shifts the mirror surface 33 in the direction of the optical axis Pi. The mirror tilt movement 434a and the mirror translation moving portion 34b are each electrically connected to the control unit 22'. The tilt movement direction, the tilt movement angle, and the translation movement amount of the mirror (4) can be controlled by a control signal from the control unit 22. Thereby, the direction of the optical axis p2 and the position of the upper axis of the spatial modulation element 6 can be changed. The 5*$ intermodulation element 6 is a laser light 61 that is biased backward by the deflecting surface 33a: and is a mirror-like (four-dimensional) DMD (digital micromirror assembly: a spatial modulation component) 6, as shown in Fig. 2A, is centered on the second surface of the quasi-surface M, and can be tilted only _ most ^ mirror surface (10), for example, in the rectangular modulation field of both sides XH, the extension of the side The direction is arranged two-dimensionally as the arrangement direction. The size of the slanting center of the micro-mirror surface 6a varies depending on the structure of the device, etc., but it can be selected from the range of angles of, for example, about 1 G to about 16. In the present embodiment, an example in which the micro-a is oriented in the opposite direction to the x-axis direction and arranged in parallel on the plane is described as an example. The micro-mirrors 6a of the spatial modulation element 6 are described as an example. Rotating by an electrostatic electric field generated according to a control signal from the control unit 22, for example, in the on state, from the reference plane + rotation + the fire icon is rotated counterclockwise), and in the 〇FF state 5, from the reference plane Μ Rotate - the bat icon rotates in a ton hour hand). Hereinafter, the light reflected by the minute mirror surface 6a in the ON state is referred to as a neon light, and the light reflected by the minute mirror surface 6a in the 0FF state is referred to as a neon light. In the present embodiment, the optical axis p3 of the ON light 62 (see Fig. 1) is set to be substantially parallel to the z-axis direction. 10 The position of each of the minute mirrors 6a can be represented by (m, n) by the column number m of the side of the length W and the row number n (m, η 〇 or more) of the side of the length ,, and can be from a micro mirror surface The arrangement interval of 6a is converted into a position coordinate on the reference plane M. The projection optical system 8 constitutes an imaging optical system that can spatially adjust the image of the ON light 62 reflected by the spatial modulation element 6 and is reflected in the fixed direction at a magnification of /5 on the processed surface Ua of the substrate 11. Group of optical components. The imaging lens 8A is disposed on the side of the spatial modulation element 6 of the projection optical system 8, and the objective lens 8B is disposed on the substrate U side. In the present embodiment, a plurality of objective lenses 8B having different magnifications are held by the rotary unit 2 to be switchable. Therefore, the magnification of the projection optical system 8 can be changed by switching the objective lens 8B' by rotating the turning mechanism. Hereinafter, unless otherwise specified, the objective lens 8B refers to a lens selected to constitute the projection optical system 8. In the present embodiment, the optical axis P4 of the imaging lens 8A is placed in parallel in the x-axis direction of 200912375, and the optical axis p5 of the objective lens 8B is placed in parallel in the two-axis direction. Therefore, between the space modulating element 6 and the imaging lens 8A, there is provided a mirror surface 7 which reflects the ON light 62 and projects it through the optical axis 匕. Then, between the imaging lens 8A and the objective lens 8B, a half lens 9 which can reflect the light penetrating the imaging lens 8A and which is incident on the optical axis P1 2 3 4 is provided. The projection magnification of the projection optical system 8 is not appropriately set in accordance with the required machining accuracy on the processed surface ila. For example, it is set such that the image having the size WxH of the entire modulation area can be changed to the magnification of w, χΗ' on the processed surface 11a. Further, the numerical aperture (ΝΑ) of the imaging lens 8 is a size that does not cause light to enter, and the light is referred to as a light 63. The observation light source 16 is capable of generating a light source for illuminating the observation light 80 in the processable region on the processed surface 11a, and is disposed in the optical path side direction between the half mirror 9 and the objective lens 8B. 15 1 In the optical path between the half mirror 5 and the objective lens 8B, a half mirror 14 is provided with respect to the position of the observation light source 216, and the half lens 14 is permeable to the ON light 62 which is reflected by the half mirror 9. The object 83 is reflected toward the objective lens 83. Then, between the observation light source 16 and the half mirror 14, a condensing lens 15 that condenses the observation light 80 into an illumination beam of an appropriate diameter is provided. The observation light source 16 can employ, for example, a suitable light source such as a xenon arc lamp or an LED that generates visible light. 5 The observation imaging lens 12 (photographing optical system) is disposed on the upper side of the half mirror 9 coaxially with the light vehicle I of the objective lens 8B. The observation imaging lens 12 is for reflecting the surface to be processed 11a illuminated by the observation light 8 ,, and the light collected by the objective lens 8B of 200912375 is imaged on the imaging surface optical element of the imaging element 13 (imaging portion). The imaging element 13 is a photoelectric conversion device that converts an image formed on the imaging surface, for example, by a CCD or the like. The image signal subjected to photoelectric conversion 5 by the imaging element 13 is sent to the control element 22 electrically connected to the imaging element 13. The control unit 22 is used to control the laser processing system 1 as shown in FIG. 3, and is composed of an image capturing unit 4, a data storage unit 43, a spatially modulated 7G device driving unit 41, and a device control unit. 42. The moving mechanism control unit 35 and the 10 image processing unit 44 are configured. In the present embodiment, the device configuration of the control unit 22 is constituted by a combination of a computer including a CPU, a memory, an output input unit, an external memory device, and the like, and an appropriate hardware. The data storage unit 43 is realized by using a memory of the computer or an external memory device. Further, other structures are realized by the CPU executing a program corresponding to each control function and processing function by the CPU. The image capturing unit 40 captures a two-dimensional image of the processed surface 11a by capturing a video signal obtained by the imaging element 13. The captured two-dimensional image is sent out and displayed on the display unit 30 constituted by a monitor or the like, and simultaneously sent as a video data 150 and memorized in the data storage unit 43 composed of the image memory. The spatial modulation element drive unit 41 controls the ΟΝ/OFF state of each of the micro mirror surfaces of the spatial modulation element 6 based on the processing data generated by the image processing unit 44. 16 200912375 Controls the operation input of the face 32 of the laser processing system 71 from the input device having, for example, "keyboard, 1 field", and is connected to the image capturing unit 40 and the space device control unit 42 electrically connected. The movement of the machine and the laser «machine head can control the action or action day of each component ^. 6. The moving mechanism control unit 35, the moving mechanism control unit 35 is based on the control signal of the device control unit 42 or the operation of the interface 32 to tilt the mobile phone (10). The image processing unit 44 calls the recorder 15. An appropriate image processor is also applied: the material defect extracting unit 45 and the processed material generating unit %. The package 3 has the defect extraction and the system relative to the μ_ι5(), and the processing impurity: the button is used as the "access data generation unit 46. ^^^(5)' is sent to the processing - the defect extraction processing can also use the well-known so-called defect (4): Method. For example, after obtaining the image (4) and the brightness of the pattern image data of the processed surface Ua that is memorized in advance, the data may be binarized from the difference data by a certain value. The processing data generating unit 46 generates processing data 152 (modulation data) for controlling the (10) chat of each of the micro mirror oils of the spatial modulation element 6, so that the (10) light 62 can be based on the secret extraction unit 45. The processing information is irradiated to the surface to be processed 1 la. In addition to the laser light source 50, the laser processing system 1 described above, 17 200912375 mirror surface 33, the pound surface 统 统 8 η moving mechanism 34, spatial modulation element 6, the projection optical system 8, and the image processing department " Jiu Yuzhuang, also constitutes the composition of the Qingyuan 22 consists of the directional device 2, and the lightning will be spatially modulated by the spatial modulation component 6 After the change m # set 200 series lla go up The light from the rear field is irradiated onto the surface to be processed. The laser irradiation device 2〇〇 is also independently installed in the field, and the image data of the laser processing system is used to receive the laser processing method corresponding to the processing of each type of Pelican. Can be used, clothing, other use. For example, an image projection device such as a sinusoidal projection projection 10 10 20 Next, the operation of the laser processing system 100 will be described. Fig. 4 is a schematic explanatory view showing the action of the face-to-face moving mechanism of the laser irradiation device according to the embodiment of the present invention. The laser processing system 100 performs laser processing, and as shown in the first item, first, the substrate u as a workpiece is placed on the planting table. Next, the machining head 2 is moved by the machining head moving mechanism 31, and after the first machining position is set, the image of the defendable field of the surface to be protected 11a is obtained. That is, the observation light source 16 is turned on, and the observation light 8 is generated. After the observation light 8 is partially reflected by the half mirror 14, the reflected light is concentrated by the objective lens 83 to illuminate the processable region on the processed surface 11a. The reflected light reflected by the processed surface 11a is collected by the objective lens 且 and partially reflected light penetrates the half mirror 14. Then, after the partially reflected light is further penetrated via the half mirror 9, it is guided to the observation imaging lens 12. The light incident on the observation imaging lens 12 is imaged on the photographing surface of the imaging element 13. 18 200912375 The imaging element 13 photoelectrically converts the image of the imaged surface 1 la that has been imaged and sends it to the image capturing unit 4〇. The video signal is applied to the video display unit 30. Further, the image signal to be converted is converted into the image signal capturing unit 40, and the image capturing unit 40 performs processing such as sending out information and brightness correction according to necessity, and displays the control signal on the display device control unit 42 to display an appropriate timing image. Information 150, and is stored in the data memory department. The image of the processable area of the processed surface 11 a is paid. Next, in the image processing unit 44, Jiang Yu & τ reads the image data 150 of the data storage unit 43 to the defect extracting unit 45 and performs defect extraction. Then, when it is judged that the defect is a defect requiring repair processing after determining the type or size of the extracted defect, etc., it is sent to the processing data generating unit 46 as the defective image data. The processable area of the machined surface 11a and the spatial modulation component (10) are in a common vehicle relationship by the xw light source system 8, and since the magnification of the projection optical system 8 is stone, it will be processed in the field. The position coordinate is set to ^ times, so that it corresponds to the position on the modulation domain of the spatial modulation element 6. In this way, the processed material generating unit 46 determines the minute mirror surface 6a to be controlled in the state of (10) in order to irradiate the ON light 62 to each position on the processed surface 11a indicated by the defective image data 151 from the defective image data 151. 20 can generate the processing material 152 in which the driving space modulation element 6 is in the ON state of the micro mirror surface 6a and the other micro mirror surface 6a is in the 〇 ff state. For example, the processing data 丨 52 is generated as the table data corresponding to the position (m, n) of each of the minute mirror faces 6a as a value corresponding to the 〇N state being 丨 and the OFF state being 0. The generated processing data 152 is sent to the spatial modulation element driving unit 19 200912375 41 〇 The component driving material is controlled according to the inclination angle of the device (4) and the processed processing data 152 The respective micro 5 10 15 20 sides of the spatial modulation element 6 = 'the device control unit 42 sends the laser oscillator 2 a signal for making the laser light 2' and the wavelength of the irradiation condition previously selected according to the substrate 11 Shoot = 1 vibration light. The oscillation condition of the laser light can be, for example, an output, an oscillation pulse width, and the like. The end face = the slanted laser light is fused to the fiber a of the _3, and is incident as the laser light 60 from the end face of the fiber and the light intensity distribution of the light 60 is substantially uniform. The laser light 6 is guided along the optical path by the projection lens 4 and is reflected by the deflecting surface 33a of the reflecting mirror 33. Then, it is bound as the laser light axis p2, and is projected onto the spatial modulation element 6, and then reflected by the respective minute mirrors 6a on the spatial modulation element 6. Therefore, the mirror moving mechanism 34 is driven in advance so that the inclination of the deflecting surface 33a with respect to the optical axis P1 (hereinafter, simply referred to as the inclination of the deflecting surface 33a) and the position of the optical axis P in the direction (hereinafter, only The position in the optical axis direction of the deflecting surface Ma) 'the laser light that can be used as the reflected light of the mirror surface 33 is effectively incident on the projection optics when reflected by the tiny mirror surface of the ON state of the spatial modulation element 6 System 8. The inclination of the deflecting surface 33a and the position of the optical axis direction are based on the operation input of the user interface 32 and the wavelength information of the laser oscillator 1 collected by the device control unit 42, etc., by the moving mechanism of the control unit 22. The control unit 35 calculates the OFF light 63 reflected by the micro mirror surface 6a whose OFF angle is in an OFF state, and is reflected outside the NA range of the imaging lens 8A. The minute mirror surface 6a whose angle of inclination is ON is reflected on the on mirror. The light 62, which will travel along the optical axis P3, and after being reflected by the mirror 7, will travel along the optical axis P4, and after entering the imaging lens 8A and concentrating, will reach the half-lens 9, and then be half The lens 9 is reflected. The ON light 62 reflected by the lens 9 travels along the optical axis P5 and is imaged on the processed surface 1 la by the objective lens 8B. 10 Thus, the modulation caused by the on-light 62 based on the processed material 152 The field image is projected onto the surface 11a to be processed. As a result, the 〇N light 62 is irradiated onto the surface of the processed surface 11& and the defect can be removed. The laser processing is completed once. The element 13 again acquires the image 15 of the surface to be processed Ua, repeats the above steps as necessary, and performs laser processing again on the unremoved portion or laser processing the other portions in the movable processable area. In the embodiment, the condition for causing the ON light 62 to be efficiently incident on the projection optical system 8 and projected to the inclination of the deflecting surface 33a of the processed surface 1 la. 20 In the spatial modulation element 6, due to the minute mirror surface 6a The light intensity distribution of the ON light 62 is determined by a microscopic mirror such as the resulting diffraction phenomenon. For example, as shown in FIG. 2A, the laser light 61 is relative to the spatial modulation element 6. The reference plane 射 is shot at an incident angle θ()=2ίζ) After the entry, the ON light 62 that is rotated counterclockwise with respect to the reference plane M to the display 21 200912375 to the majority of the minute mirrors 6a in the ON state with only a large inclination angle generates Fraunhof diffraction. 70 and diffraction 71. The light intensity distribution of the ON light 62 can be obtained by convolving the diffracted light. 5 The Fraunhofer diffraction 70 depends on the aperture of the minute mirror 6a and the regular reflection at the minute mirror 6a The direction (in this example, the Z-axis negative direction) has a bell-type light intensity distribution with a peak. On the other hand, the diffraction 71 is a dispersion distribution which is determined by the arrangement interval of the minute mirror faces 6a and the wavelength of the laser light 61. That is, the regular reflection light of the laser light 61 with respect to the 10 reference plane ( (in this example, the direction of the clockwise rotation angle θ 相对 with respect to the z-axis negative direction) generates 0-order refracted light d〇, and The N-order diffracted light dN is generated by a different diffraction angle direction depending on the arrangement interval of the minute mirrors 6a and the wavelength of the laser light 61 (however, N = 1, 2, . . . ). At this time, in the state where the direction of the diffracted light of any order of the diffraction 71 is substantially coincident with the direction of the peak intensity of the diffraction of the Fran and the fifteenth, the projection optical system 8 is decomposed as long as it can be incident on the projection optical system 8. The light intensity distribution becomes large, so the diffraction efficiency can be improved. Therefore, the light use efficiency can be improved. For example, in the case of FIG. 2A, the peak intensity directions of the 'Fran and Fiji diffractions 70 are uniform with respect to the optical axis direction of the projection optical system 8, and the 20 3rd-order diffracted light d3 and the fourth-order diffracted light d4 of the diffraction 71 are When only the angles θ3 and θ4 (but θ4 $θ3) are respectively inclined, at least either of the diffracted lights can be included in the aperture angle range of the projection optical system 8, so that the diffraction efficiency can be improved and good light use efficiency can be achieved. The peak intensity direction of the Fraun and Fiji diffractions 70 is determined by the angle of incidence and the tilt angle 0 of the micro-mirror 6a' and the diffraction angle of the diffraction 71 is arranged by the arrangement of the micromirrors 22, 200912375 faces 6a and the laser light 61. The wavelength is determined, so that the moving mechanism control unit 35 can determine whether the peak intensity direction of the Fraunhofer diffraction 70 and the direction of the diffracted light of the Fraunhofer are entered into the projection optical system 8 by taking the information from the device control σΜ2. The range of aperture angles. 5 When either of the diffracted light directions does not enter the aperture angle range of the projection optical system 8, the moving mechanism control unit 35 causes the deflecting surface to tilt obliquely, so that the peak intensity direction of the Fraun and Fiji diffraction 70 is either The direction of the diffracted light is at least within the aperture of the projection line 8 and may coincide with the optical axis of the projection optical system 8. 10 For example, as indicated by the broken line in Fig. 2, by the mirror moving mechanism 34 The inclination of the deflecting surface 33a is changed so that the laser beam 61 is incident on the reference plane Μ at an incident angle (θ〇+ΔΘ). The diffraction direction of each of the diffracted lights changes depending on the change in the incident angle. By appropriately setting Δθ, for example, 'the direction in which the diffraction direction of the fourth-order diffracted light ο# coincides with the direction of the light 15 axis of the projection optical system 8 can be achieved. At this time, 'the direction of the regular reflection with respect to the minute mirror surface There is also a change, so the peak intensity direction of the Fulang and Fiji diffractions 70 also changes. Therefore, the value of ΔΘ can be set so that each diffraction direction can enter the aperture angle range of the projection optical system 8. 20 Change laser When the oscillation wavelength of the singer 1 is appropriate, the movement of the deflection surface 333 is preferably performed according to the wavelength thereof. For example, as shown in FIG. 2C, the spatial modulation element 6 is incident on the short-wavelength laser light 61, and then 'Fran and Although the Fission diffraction 70 is the same as the case of the second diagram, the diffraction 71 will generate the 绕-order diffracted light e〇 in the normal reflection side 23 200912375 of the reference plane according to the change of the wavelength, and is in the higher order than the 2A diagram. The diffracted direction of the diffracted light produces N-order diffracted light (but, N = 1, 2,. ··). Then, the diffracted light having the diffraction direction closest to the optical axis direction of the optical system 8 becomes, for example, 6th-order diffracted light having an angular center with respect to the optical axis of the projection optical system 8, 5 2A is different. Therefore, by moving the deflecting surface 33a in accordance with the angle Θ6, good diffraction efficiency can be obtained even if the oscillation wavelength of the laser oscillator 1 is changed. Next, a numerical example will be described to explain the tilt of the deflecting surface 33a. The angle setting of the degree is 0. Numerical example 1 is shown in Table 1. The numerical example 1 is arranged at an interval of 19 in the micro mirror surface 6a. 05 μ m, and the tilt angle 〇 of the 〇N state of the minute mirror 6a is ^15. In the case of 3 deg, the setting of the wavelength of the laser light 61 is 266 nm, 355 nm, and 532 nm. Here, each wavelength corresponds to the second harmonic, the third harmonic, and the fourth harmonic of the YAG laser. 5 Table 1 shows the diffraction angle (deg) of the first-order diffracted light with respect to each wavelength, the diffraction order of the diffracted light closest to the optical axis p3 of the projection optical system 8, and the relative of the spatial modulation element 6 The set value of the incident angle θ 于 at the reference plane 5^, the diffraction efficiency (%) calculated from the dispersion of the intensity distribution of the Fraun and Fiji diffraction and the diffracted light, and the optical axis of the projection optical system 8 The angle of ρ3 (deg). 20 Table 1 Wavelength (nm) Diffraction angle (deg) The angle of incidence of the diffraction order to the spatial modulation element (deg) Diffraction efficiency ^ (%) Angle of the projection optical system relative to the optical axis (deg) Numerical example 1-a 266 0. 80 卜 261 30. 8 65 0. 08 Numerical Example 1-b 355 1. 07 ~~19 30. 9 57 0. 70 Numerical Example 1-c 532 1. 60 13 — 30. 7 85 0. 17 It can be seen from Table 1 that the angle of incidence of the spatial modulation component 6 is set to 30 according to each wavelength. 8deg, 30. 9deg, 30. 7deg, the diffraction efficiency can be more than 57%. At this time, the diffraction order of the diffracted light closest to the optical axis P3 is 26, 19, and 13, respectively, and the angle with respect to the optical axis P3 is 〇. 〇8deg, 〇. 7〇deg, 0. 17deg' is based on the maximum value of 0. 7 deg, so that the projection optical system 8 is 50. 012 or more, the diffracted light of each wavelength can be incident on the aperture angle range of the projection optical system 8. Next, Numerical Example 2 is shown in Table 2. In Numerical Example 2, the arrangement interval of the micro mirror surface 6a is 24 // m, and the inclination angle 0 of the ON state of the micro mirror surface 6a is _14. In the case of 0 deg, a setting example in which the wavelength of the laser light 61 is 330 nm, 440 nm, or 10 660 nm is set. Here, each wavelength corresponds to the second harmonic, the third harmonic, and the fourth harmonic of the YAG laser. Table 2 shows the diffraction angle (deg), the diffraction order, the set value of the incident angle θ 、, the diffraction efficiency (%), and the angle (deg) with respect to the optical axis p3, respectively, as in Table 1. 15 Table 2 Wavelength (nm) Diffraction angle (deg) Angle of incidence of the diffraction order to the spatial modulation element (deg) Diffraction efficiency (%) Angle of the projection optical system relative to the optical axis (deg) Numerical example 2 -a 330 0. 798 24 28. 0 83 0. 15 Numerical Example 2 -b 440 1. 05 18 27. 9 87 0. 07 Numerical Example 2-c 660 1. 58 12 27. 8 91 0. 017 It can be seen from Table 2 that the incident angle of the spatial modulation element 6 is set to 28. 0deg, 27_9deg, 27. 8deg, the diffraction efficiency can be more than 83%. At this time, the diffraction order of the diffracted light closest to the optical axis p3 is 24, 18, 12, respectively, and the angle with respect to the optical axis P3 is 〇. 15deg, 0. 07deg, 20 〇. 〇17deg, so according to the maximum value of 0. At 15 deg, the 光学 of the projection optical system 8 is 0·003 or more, and the diffracted light of each wavelength can be incident on the 25 200912375 aperture angle range of the projection optical system 8. The tilting movement of the deflecting surface 33a can also be applied to, for example, the adjustment of the tilt angle of the ON state of the micro mirror surface 6a due to the manufacturing difference of the spatial modulation element 6 when the spatial modulation element 6 is exchanged. . The adjustment of this case is made in the numerical example 3 shown in Table 5.3. In Numerical Example 3, in the case where the arrangement interval of the micro mirror surface 6a is 17 9 / / m, and the wavelength of the laser light 61 is 355 nm, the inclination angle of the micro mirror surface such as 〇 ^ ^ state changes to Lu = 15. 〇deg, i4. An example of 97nm. The inclination angle of the minute mirror surface 6a can be experimentally obtained by injecting the reference light at a predetermined angle and measuring the arrival position of the reflected light. Table 3 together with the small mirror 63 of the ON state has a large inclination angle, and shows the same diffraction angle (deg) as that of Table 1. 'Diffraction order, set value of incident angle 0〇, diffraction efficiency (%), relative to The angle (deg) of the optical axis P3. Table 3 Wavelength (nm) Diffraction angle (deg) The angle of incidence of the diffraction order to the spatial modulation element (deg) The diffraction efficiency (%) The tilt angle of the tiny mirror of the ON state (deg) The relative angle of the projection optical system Angle of the optical axis (deg) Numerical example 3-a 355 1. 14 18 30. 0 80 15. 00 0. 28 Numerical Example 3 -b 355 1. 14 18 30. 0 73 14. 97 0. 28 Numerical Example 3-c 355 1. 14 18 29. 5 80 H 14. 97 0. 71 15 The numerical examples in Table 3, 3-a and 3-b, show that even if the angle of inclination 〇〇 = 3 〇 deg, the inclination angle ^ changes only 〇. 〇3deg also changes the diffraction efficiency by 7%. Numerical example 3-c shows that the deflecting surface 33a is tilted and moved. 5deg' can restore the diffraction efficiency even if ^=14. The spatially modulating element 6 of 97 deg can also achieve an 80% diffraction efficiency similarly to the spatially modulating element 6 of 15 deg. Further, when the inclination of the deflecting surface 33a is changed only by the inclination of the mirror surface 33, the incident position of the laser light 61 with respect to the space element 6 is deviated. In the present embodiment, the mirror moving mechanism 34 includes the mirror tilting movement portion 34a and the mirror translation moving portion 34b, so that the translational movement of the mirror surface 33 is matched, so that the laser light 61 can be correctly incident on the optical axis of the projection optical system 8. . For example, as shown in Fig. 4, when the deflecting surface 33a is held by the mirror tilting moving portion 34a so that the intersection point Q with the optical axis 成为 becomes the center of the tilting movement, the incident angle from the spatially modulating element 6 is obtained. When the state of the mirror surface 33 呈 at an angle θ 仅 is only a rotation angle (ΔΘ/2)′ and is tilted to the position of the mirror surface 33 ,, the laser light from the laser light source 5 调 is modulated with respect to the space 10 . The incident angle of the reference plane of the element 6 becomes an angle (Θ+ΔΘ), but depending on the distance to the spatial modulation element 6, the reflected light sometimes deviates from the spatial modulation element 6, or is effective from the projection optical system 8. range. At this time, by the mirror translation moving portion 34b, the mirror surface 33 is shifted by only the distance L in the direction of the optical axis P1, and moved to the position of the mirror surface 33 (: 15), so that the reflected light of the mirror surface 33C is correct. The ground is incident on the same position as the reflected light of the mirror surface 33A. According to the laser processing system 1 〇〇, the mirror movement mechanism 34 can be obliquely moved with respect to the optical axis PJS, and can be moved in the direction of the optical axis 匕The deflecting surface 33a is deflected toward the laser light 61 from the laser light source 5 to change the incident angle with respect to the reference surface 调 of the spatially modulating element 6 and the minute mirror surface of the ON state, so that the spatial modulating element 6 can be illuminated. The laser light 61 at the incident position is changed. Therefore, the Fraunhofer and the Fidelity diffraction generated by the aperture of the micromirror 6a can be made without changing the tilt angle of the 01^ state of the micro mirror surface. The diffraction direction of the diffraction 71 generated by the arrangement interval of 6a is the same as the aperture angle range of the projection optical system 8 of the 200912375. The system of the surname system 8' and the optical axis of the image are as follows. Therefore, according to the laser oscillator i The vibration surface is changed long (4) Irradiation. For the person of the _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ The inclination of the state _ can also be described as follows: ============================================================================================ The first aspect of the invention is a schematic illustration of the structure of the deflecting surface moving mechanism of the laser irradiation device according to the modification. The example of the present invention includes the mirror moving mechanism 36 (biasing surface moving mechanism) shown in FIG. The mirror-moving mechanism material of the above-described embodiment will be described with a focus on the difference from the above-described embodiment. The mirror-moving mechanism 36 is the same mirror-side tilting portion 34a and mirror surface as the mirror-moving mechanism 34. The translational movement portion 34b is constructed, and the mirror surface 33 is tilted and moved about the point g of the end portion thereof. Further, the mirror movement mechanism 36 is electrically connected to the movement mechanism control portion 35 of the control unit 22. At this time, the reflection of the optical axis on the deflecting surface 33a is considered. In the case where the distance between the point g and the point g is set, the amount of translational movement in the Z-axis direction can be determined to be the same as that of the above-described embodiment, and the deflecting surface 33a can be tilted and translated in the same manner as in the above-described embodiment. The second modification of the embodiment of the present invention is shown in the following. 28 200912375 FIG. 6 is a view showing the structure of the optical path deflecting portion and the deflecting surface moving mechanism of the laser irradiation device according to the second modified example of the embodiment of the present invention. The present modification includes a mirror block 37 (optical path deflecting portion 5) and a mirror moving mechanism 38 (biasing surface moving mechanism) shown in FIG. 6 instead of the mirror surface 33' mirror moving mechanism of the above-described embodiment. 34. Hereinafter, the description will be focused on differences from the above-described embodiments. As shown in Fig. 6, the mirror block 37 is arranged side by side in the x-axis direction on the surface opposite to the mounting surface 37a parallel to the χγ plane, and has a tilt in the /χ plane and a uniformity in the z-axis direction. Different deflection faces 37, 37B, 37C. The mirror moving mechanism 38 is attached to a slider guide 38b that is attached to a casing (not shown) in the direction of the drawing, and is attached to the mounting surface 37a' of the mirror block 37 and is provided on the slider guide 38b. The single-axis moving mechanism constituted by the slider 38a that moves in the γ-axis direction is shown. The mirror moving mechanism 38 is electrically connected to the moving mechanism control unit 35 of the control unit 22, and can be moved stepwise in the γ-axis direction by the control signal of the moving mechanism control unit 35. In the present modification, the inclination of the deflection surfaces 37A, 37B, and 37C with respect to the Z-axis and the position of the 20-axis direction are set in accordance with, for example, three wavelengths a of the laser light source 5A, and B and Ac'. The most appropriate value. Then, each time the device control unit 42 switches the oscillation wavelength of the laser oscillator ,, for example, when switching from the wavelength person a to the wavelength Ac, the mirror block 37 moves in the γ-axis direction, and the deflection surface 37C is substituted for the deflection surface. 37A to reflect the laser light 61. In this way, according to the present modification, when the tilt amount 29 200912375 of the deflecting surface is limited to a large number in advance, it is not necessary to perform the human calculation every time the switching is performed, and the setting of the partial "4" can be quickly performed. Relative = The tilting movement is performed on the deflecting surface. Therefore, the structure of the deflecting surface moving mechanism can be made simple, and the surface of the deflecting surface can be parallel to the one axis of the y-axis. However, the deflecting surfaces can be appropriately adjusted. A shape in which the shape of the inclination angle is changed in each of the deflection centers, and a shape in which the ground is moved in the Z-axis direction. Next, a third modification of the embodiment will be described. Fig. 7 is a view showing a third modification of the embodiment of the present invention. The laser irradiation example of the wire deflection portion and the deflection surface moving mechanism includes a mirror block 39 (optical path deflecting portion) shown in Fig. 7, and a mirror moving mechanism 48 (biasing surface movement) The mirror surface 33 and the mirror surface movement 34 in place of the above-described embodiment are described below. The following description will focus on differences from the above-described embodiment. The mirror block 39 is as shown in Fig. 7, Χγ plane parallel mounting surface On the opposite side, the inclination in the plane of the yaw axis and the height in the y-axis direction are arranged in parallel with each other in the direction of the yaw axis. (4) Deflection planes 39Α, 39Β, 39C. A movement mechanism 48 is extended from the X-axis direction of the figure. The q-shaped guide 48b which is attached to the unillustrated body and the fixed side of the inner side of each of the deflecting faces of the opposite side of the yoke are provided with a fixed surface rice, and is set to be A single-axis moving mechanism constituted by a slider 48a that moves in the X-axis direction on the sliding guide 48b. The brother moving mechanism 48 is electrically connected to the moving mechanism 30 of the control unit 22 200912375 Control unit 35, b - r - 丄 can be hunted by the control signal of the moving mechanism control unit 35, and moves in a stepwise direction in the γ pumping direction. > 轴 显 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 The movement value formed by increasing the stepwise direction in the positive direction may be a shape in which the arrangement height of each of the deflection surfaces is appropriately oriented in the z-axis direction, and for example, may be formed in a shape having a large tooth shape in the cross-section of the crucible. With respect to the second modification, the movement of the surface of the deflection surface is shifted. In the same manner as the second modification described above, the direction of the movement of the tilting movement and the translational movement by the movement mechanism control unit is controlled by the movement mechanism control unit, but the deflection movement mechanism is used. It can also be constructed by a mechanical table or the like, and can be manually moved by tilting and translational movement.
匕種Μ況下,只要依據例如波長或微小鏡面之傾斜角 等條件事先算出傾斜移動角度或平移移動量,而可在移動 15時作為參考即可。或是,做成可監測被加工面的光量,在 動量改變時’邊測定被加工面上的光量邊進行設定亦可。 ^特別是前述第2、第3變形例的構造中,偏向面移動機 構係往單軸方向階梯狀地移動來選擇性地切換偏向面,故 無需高精度的移動精度,適合手動操作。 2〇 月1J述說明中,係以令照射至空間調變元件6上的雷射光 搭配傾向面之傾斜移動與對光軸方向之平移移動,而做到 即使入射角改變,入射位置亦不會改變的例子來說明,但 亦可依據必要性改變入射位置,以移動加工頭來抵銷藉入 射位置變化所產生之被加工面上的移動量。 31 200912375 此種情況下,可邊移動相對於空間調變元件之照射位 置邊進行雷射照射,故可分散相對於微小鏡面之雷射光的 照射負荷,而可延長空間調變元件的壽命。 前述說明中,係以藉1個雷射振盪器產生多數波長光的 5 例子來說明,但雷射光源亦可為搭配振盪波長相異的多數 雷射振盪器的構造。 前述說明中,係以將雷射加工使用於半導體晶圓基板 等的修護加工的例子來說明,但被加工物不受限於此,亦 可使用於針對例如,多層膜、塗佈膜、薄金屬物體或有機 10 物體、半導體等種種被加工物的雷射加工。 【圖式簡單說明3 第1圖係顯示本發明之實施態樣的雷射照射裝置及使 用該裝置之雷射加工系統的概略構造的含光軸之截面示意 說明圖。 15 第2A圖、第2B圖、第2C圖係說明本發明之實施態樣的 雷射照射裝置之空間調變元件的繞射現象的示意截面圖。 第3圖係顯示本發明之實施態樣的雷射加工系統之控 制單元的概略構造的功能方塊圖。 第4圖係說明本發明之實施態樣的雷射照射裝置之偏 20 向面移動機構的作用的示意說明圖。 第5圖係顯示本發明之實施態樣之第1變形例的雷射照 射裝置之偏向面移動機構的構造的示意說明圖。 第6圖係顯示本發明之實施態樣之第2變形例的雷射照 射裝置之光程偏向部以及偏向面移動機構的構造的示意立 32 200912375 體圖。 第7圖係顯示本發明之實施態樣之第3變形例的雷射照 射裝置之光程偏向部以及偏向面移動機構的構造的示意說 明圖。 5 第8圖係用以說明可切換波長之雷射加工裝置的繞射 光角度分布之一例的角度分布圖。 【主要元件符號說明】 1 雷射振盪器 14 半透鏡 2 耦合透鏡 15 聚光透鏡 3 纖維 16 觀察用光源 3a 纖維端面 20 加工頭 3b 纖維端面 20a 外殼 4 投影透鏡 21 載置台 6 空間調變元件 22 控制單元 6a 微小鏡面 30 顯不部 7 鏡面 31 加工頭移動機構 8 投影光學系統 32 使用者介面 8A 成像透鏡 33 反射鏡面 8B 物鏡 33a 偏向面 9 半透鏡 33A 反射鏡面 11 33B 反射鏡面 11a 被加工面 33C 反射鏡面 12 觀察用成像透鏡 34 鏡面移動機構 13 拍攝元件 34a 鏡面傾斜移動部 33 200912375 34b 鏡面平移移動部 48a 滑件 35 移動機構控制部 48b 滑件導座 36 鏡面移動機構 48c 固定面 37 反射鏡塊 50 雷射光源 37a 安裝面 60 雷射光 37A 偏向面 61 雷射光 37B 偏向面 61A 雷射光 37C 偏向面 61B 雷射光 38 鏡面移動彳幾構 62 ON光 38a 滑件 63 OFF光 38b 滑件導座 70 夫朗和斐繞射 39 反射鏡塊 71 繞射 39a 安裝面 80 觀察用光 39A 偏向面 100 雷射加工系統 39B 偏向面 150 影像貨料 39C 偏向面 151 缺陷影像資料 40 影像擷取部 152 加工資料 41 空間調變元件驅動部 200 雷射照射裝置 42 裝置控制部 501 角度平面 43 資料記憶部 502 顯微鏡光軸 44 影像處理部 503 後側角孔徑 45 缺陷抽取部 504 繞射階數 46 加工貢料生成部 505 繞射階數 48 鏡面移動機構 λΑ 波長 34 200912375 λβ 波長 L 距離 Ac 波長 R 旋動軸 又2 波長 θο 入射角 又3 波長 θ〇+ΔΘ 入射角 Pi 光軸 ΔΘ/2 角度 p2 光轴 3階繞射光 p3 光轴 4階繞射光 p4 光轴 d4 4階繞射光 p5 光車由 e〇 〇階繞射光 p6 光轴 θ3 角度 Q 交點 θ4 角度 g 點 Φ 傾斜角 M 基準面 β 倍率 35In other cases, the tilt movement angle or the translation movement amount may be calculated in advance based on conditions such as the wavelength or the inclination angle of the micro mirror surface, and may be referred to as a reference when moving 15. Alternatively, it is possible to monitor the amount of light on the surface to be processed, and to set the amount of light on the surface to be processed when the momentum is changed. In particular, in the structures of the second and third modifications described above, the deflecting surface moving mechanism moves in a stepwise direction in the uniaxial direction to selectively switch the deflecting surface, so that high precision movement accuracy is not required, and it is suitable for manual operation. In the description of 2〇月1J, the oblique movement of the laser light incident on the spatial modulation element 6 with the tilting direction of the tilting surface and the translational movement of the optical axis direction are performed, so that even if the incident angle is changed, the incident position is not The example of the change is explained, but the incident position can also be changed according to the necessity to move the machining head to offset the amount of movement on the machined surface resulting from the change in the incident position. 31 200912375 In this case, it is possible to perform laser irradiation while moving relative to the irradiation position of the spatial modulation element, so that the irradiation load of the laser light with respect to the micro mirror surface can be dispersed, and the life of the spatial modulation element can be extended. In the above description, the example in which a plurality of wavelengths of light are generated by one laser oscillator is described. However, the laser light source may have a configuration in which a plurality of laser oscillators having different oscillation wavelengths are used. In the above description, the laser processing is applied to a semiconductor wafer substrate or the like. However, the workpiece is not limited thereto, and may be used for, for example, a multilayer film or a coating film. Laser processing of various metal objects such as thin metal objects or organic 10 objects and semiconductors. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic cross-sectional view showing an optical axis including a laser irradiation apparatus according to an embodiment of the present invention and a schematic configuration of a laser processing system using the apparatus. 15A, 2B, and 2C are schematic cross-sectional views illustrating a diffraction phenomenon of a spatial modulation element of a laser irradiation apparatus according to an embodiment of the present invention. Fig. 3 is a functional block diagram showing a schematic configuration of a control unit of a laser processing system according to an embodiment of the present invention. Fig. 4 is a schematic explanatory view showing the action of the partial-direction moving mechanism of the laser irradiation apparatus according to the embodiment of the present invention. Fig. 5 is a schematic explanatory view showing the structure of a deflection surface moving mechanism of the laser irradiation device according to the first modification of the embodiment of the present invention. Fig. 6 is a schematic view showing the structure of the optical path deflecting portion and the deflecting surface moving mechanism of the laser irradiating device according to the second modified example of the embodiment of the present invention. Fig. 7 is a schematic view showing the structure of the optical path deflecting portion and the deflecting surface moving mechanism of the laser irradiating device according to the third modified example of the embodiment of the present invention. 5 Fig. 8 is an angular distribution diagram showing an example of an angular distribution of diffracted light of a laser processing device capable of switching wavelengths. [Main component symbol description] 1 Laser oscillator 14 Half lens 2 Coupling lens 15 Condenser lens 3 Fiber 16 Observation light source 3a Fiber end face 20 Processing head 3b Fiber end face 20a Housing 4 Projection lens 21 Mounting table 6 Space modulation element 22 Control unit 6a micro mirror 30 display portion 7 mirror surface 31 processing head moving mechanism 8 projection optical system 32 user interface 8A imaging lens 33 mirror surface 8B objective lens 33a deflection surface 9 half lens 33A mirror surface 11 33B mirror surface 11a processed surface 33C Mirror surface 12 observation imaging lens 34 mirror movement mechanism 13 imaging element 34a mirror tilting movement 33 200912375 34b mirror translation moving portion 48a slider 35 movement mechanism control portion 48b slider guide 36 mirror moving mechanism 48c fixing surface 37 mirror block 50 Laser light source 37a Mounting surface 60 Laser light 37A Deflection surface 61 Laser light 37B Deflection surface 61A Laser light 37C Deflection surface 61B Laser light 38 Mirror surface movement 62 ON light 38a Slide 63 OFF light 38b Slide guide 70 Long and Fiji Diffraction 39 Mirror Block 71 Diffraction 39a Ann Face 80 viewing light 39A deflecting surface 100 laser processing system 39B deflecting surface 150 image material 39C deflecting surface 151 defect image data 40 image capturing unit 152 processing data 41 spatial modulation element driving unit 200 laser irradiation device 42 device control Part 501 Angle plane 43 Data storage unit 502 Microscope optical axis 44 Image processing unit 503 Rear side angular aperture 45 Defect extraction unit 504 Diffraction order 46 Processing tributary generation unit 505 Diffraction order 48 Mirror moving mechanism λ 波长 Wavelength 34 200912375 λβ Wavelength L Distance Ac Wavelength R Spinning axis 2 Wavelength θο Incident angle 3 Wavelength θ〇+ΔΘ Incident angle Pi Optical axis ΔΘ/2 Angle p2 Optical axis 3rd order diffracted light p3 Optical axis 4th order diffracted light p4 Optical axis d4 4 Order diffracted light p5 Light car by e〇〇 order diffracted light p6 Optical axis θ3 Angle Q Intersection point θ4 Angle g Point Φ Tilt angle M Base plane β Magnification 35