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TW200952103A - Inspection device - Google Patents

Inspection device Download PDF

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Publication number
TW200952103A
TW200952103A TW098111992A TW98111992A TW200952103A TW 200952103 A TW200952103 A TW 200952103A TW 098111992 A TW098111992 A TW 098111992A TW 98111992 A TW98111992 A TW 98111992A TW 200952103 A TW200952103 A TW 200952103A
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TW
Taiwan
Prior art keywords
substrate
wafer
light
unit
optical system
Prior art date
Application number
TW098111992A
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Chinese (zh)
Inventor
Toru Yoshikawa
Original Assignee
Nikon Corp
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Application filed by Nikon Corp filed Critical Nikon Corp
Publication of TW200952103A publication Critical patent/TW200952103A/en

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/84Systems specially adapted for particular applications
    • G01N21/88Investigating the presence of flaws or contamination
    • G01N21/95Investigating the presence of flaws or contamination characterised by the material or shape of the object to be examined
    • G01N21/956Inspecting patterns on the surface of objects
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/84Systems specially adapted for particular applications
    • G01N21/88Investigating the presence of flaws or contamination
    • G01N21/95Investigating the presence of flaws or contamination characterised by the material or shape of the object to be examined
    • G01N2021/9513Liquid crystal panels

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  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Materials By The Use Of Optical Means Adapted For Particular Applications (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

An inspection device (1) includes: an illumination optical system (10) which applies an illumination light onto a surface of a wafer (W); a detection optical system (20) for observing the surface of the wafer (W) illuminated by the illumination light in an enlarged scale; detection elements (36a, 36b, 36c) for detecting luminance of reflected light from the wafer (W) on a pupil surface in the inspection optical system (20); a CPU (43) which inspects the surface of the wafer (W) in accordance with the luminance detected by the detection elements (36a, 36b, 36c); and a scan unit (60) which scans the range of the wafer (W) corresponding to the pupil surface on which the luminance is detected.

Description

200952103 六、發明說明: 【發明所屬之技術領域】 本發明係有關在半導體元件或液晶顯示元件等之製造 過程中’用以檢測形成於被檢測基板表面之圖案之狀態之 檢查裝置。 【先前技術】 以往’利用由形成於被檢測基板(如半導體晶圓或液晶 玻璃基板等)表面之圖案所發出之反射光,以供檢查基板表 面之不均勻或損傷等缺陷之裝置,已知有各種提案(例如參 照專利文獻1)。特別是,近年來隨著半導體製程的微細化, 對於被檢測基板之缺陷管理亦有更高的精度要求。 例如,藉由SEM(掃描型電子顯微鏡)進行被檢測基板之 圖案寬度之測定時,雖然有高測定精度,但由於觀察倍率 亦高而須取樣數個點進行測定,因而在測定上會耗上大量 時間。對此,已提出一種方法,其係使由光源射出之既定 波長的光透過偏光元件及物鏡,藉由落射照明照射在被檢 測基板的表面,使用透過物鏡、及能滿足偏光元件與正交 偏光鏡之條件的檢光元件獲得之影像評價該照明當中來自 被檢測基板的反射光。 [專利文獻1]日本特開2000-155099號公報 【發明内容】 然而,即使使用上述方法時,由於觀察倍率較高,因 200952103 此為了檢查被檢測基板整體必須使觀察範圍移動。此時, 一般而言係使保持被檢測基板之載台移動以使觀察範圍移 動’但由於使載台移動較花時間,因此檢查時間增加。 本發明係有鑑於此問題而完成者,其目的在於提供能 以咼感度高速地進行檢查之檢查裝置。The present invention relates to an inspection apparatus for detecting a state of a pattern formed on a surface of a substrate to be inspected during manufacture of a semiconductor element or a liquid crystal display element or the like. [Prior Art] Conventionally, a device that uses a reflected light emitted from a pattern formed on a surface of a substrate to be inspected (such as a semiconductor wafer or a liquid crystal glass substrate) to inspect defects such as unevenness or damage on the surface of the substrate is known. There are various proposals (for example, refer to Patent Document 1). In particular, in recent years, as the semiconductor process has been miniaturized, there has been a higher accuracy requirement for defect management of the substrate to be inspected. For example, when measuring the pattern width of the substrate to be inspected by SEM (scanning electron microscope), although the measurement accuracy is high, since the observation magnification is also high, it is necessary to sample a few points for measurement, and thus it is consumed in the measurement. lot of time. In response to this, there has been proposed a method of transmitting light of a predetermined wavelength emitted from a light source through a polarizing element and an objective lens, irradiating the surface of the substrate to be inspected by epi-illumination, using a transmissive objective lens, and satisfying the polarizing element and the orthogonal polarization. The image obtained by the photodetecting element under the condition of the mirror evaluates the reflected light from the substrate to be detected in the illumination. [Patent Document 1] Japanese Laid-Open Patent Publication No. 2000-155099. SUMMARY OF THE INVENTION However, even when the above method is used, since the observation magnification is high, it is necessary to move the observation range in order to inspect the entire substrate to be inspected in 200952103. At this time, in general, the stage holding the substrate to be inspected is moved to move the observation range. However, since the stage is moved more time, the inspection time is increased. The present invention has been made in view of the above problems, and an object thereof is to provide an inspection apparatus capable of performing inspection at a high speed with a high sensitivity.

為達成上述目的,本發明之檢查裝置,具備:照明部, 將照明光照射至被檢測基板表面;觀察光學系統,用以放 大觀察被該照明光照射之該被檢測基板表面;檢測部,檢 測該觀察光學系統中來自該被檢測基板之反射光在光瞳面 的亮度;檢查部,根據該檢測部所檢測之該亮度檢查=被 檢測基板表面;以及掃描部,掃描與檢測出該亮度之該光 瞳面對應之該被檢測基板的範圍。 此外,上述發明中較佳為,該掃描部具有:具備作為 視野光闌之光學開口部的板狀構件、及驅動該光學開口部 的驅動部;使用該驅動部使該光學開口部掃描於該範圍。 再者,上述發明中較佳為,該板狀構件形成為圓板狀, 且作為該光學開π部之複數個孔部係分別形成在該板狀構 2上彼此相異之直徑方向及周方向位置;該驅動部係構成 ^以該板狀構件之旋轉對象軸為“軸旋轉驅動該板狀構 ,使用相動部使形成於該板狀構件之該複數個孔部分 =轉移動,據以從該複數個孔部中之任_孔部依序掃描 5 200952103 狀構件上相對該直線移動方向斜向排列之方式形成“吏用 該驅動部冑形成於該板狀構件之該複數個孔部 動’據以從該複數個孔部中之任—孔部依序掃描該範圍。 又,上述發明中較佳為,該檢測部係檢測在該光瞳面 上,對應該被檢測基板表面㈣之變化❿亮度大幅變化部 分之亮度。 又,上述發明中較佳為,該照明光係照射至具有反覆 圖案之該被檢測基板表面的直線偏光;該檢測部檢測來 自該被檢測基板之光中之偏光方向與該直線偏光大致正交 之偏光成分。 又,上述發明中較佳為,該照明部,係藉由落射照明 將該照明光照射至該被檢測基板表面。 根據本發明’能以高感度高速地進行檢查。 【實施方式】 以下,參照圖式說明本發明之較佳實施形態。圖1係 本發明之檢查裝置。本實施形態之檢查裝置丨之主體構成 如圖1所不’包含晶圓載台5、物鏡6、半反射鏡7、照明 光學系統10、檢測光學系統20、掃描部60、攝影部3〇、 及控制單元40。 晶圓載台5係以圖案(反覆圖案)形成面朝上之狀態袭 載著作為被檢測基板之半導體晶圓W(以下稱為晶圓w)。該 晶圓載台5,係以可朝彼此正交之x、y、z軸之3個方向移 動之方式構成(此外,圖1之上下方向為z轴方向)。藉此, 200952103 晶圓載台5’係將晶圓W支擇成可移動於X、y、z軸方向。 又’晶圓載台5能以z轴為中心旋轉。 照明光學系統1 〇 ’由圖1之左側朝右侧,依其配置順 序依序具有:光源1 1 (例如白色LED或鹵素燈等)、聚光透 / 鏡12、照度均一化單元13、孔徑光闌14、視野光闌15、 準直透鏡16、及可拆裝之偏光元件17(偏光過濾器)。 此處’由照明光學系統1 0之光源1 1所放出的光,透In order to achieve the above object, an inspection apparatus according to the present invention includes: an illumination unit that irradiates illumination light onto a surface of a substrate to be inspected; and an observation optical system that amplifies observation of a surface of the substrate to be inspected by the illumination light; and a detection unit detects In the observation optical system, the brightness of the reflected light from the substrate to be detected is on the pupil plane; the inspection unit checks the surface of the substrate to be detected based on the brightness detected by the detecting unit; and the scanning unit scans and detects the brightness. The pupil plane corresponds to the range of the substrate to be inspected. Further, in the above invention, preferably, the scanning unit includes a plate-shaped member including an optical opening as a field stop, and a driving unit that drives the optical opening, and the optical opening is scanned by the driving unit. range. Further, in the above invention, it is preferable that the plate-like member is formed in a disk shape, and the plurality of hole portions as the optical opening π portion are respectively formed in the diametrical direction and the circumference different from each other in the plate-like structure 2. a direction position; the drive unit is configured to rotate the target axis of the plate-shaped member to "rotate the plate-like structure", and use the phase-moving portion to rotate the plurality of holes formed in the plate-shaped member = Forming a plurality of holes formed in the plate-shaped member from the plurality of holes in the plurality of holes, and sequentially aligning the direction of the linear movement direction on the 200952103-shaped member. The portion moves to scan the range sequentially from any of the plurality of holes. Further, in the above invention, it is preferable that the detecting unit detects the brightness of the portion of the pupil surface that is largely changed in brightness due to a change in the surface (4) of the substrate to be detected. Further, in the above invention, preferably, the illumination light is applied to linearly polarized light having a surface of the substrate to be detected having a reverse pattern; and the detecting portion detects that a polarization direction of light from the substrate to be detected is substantially orthogonal to the linearly polarized light. The polarizing component. Further, in the above invention, it is preferable that the illumination unit irradiates the illumination light onto the surface of the substrate to be detected by epi-illumination. According to the present invention, inspection can be performed at high speed with high sensitivity. [Embodiment] Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is an inspection apparatus of the present invention. The main structure of the inspection apparatus 本 according to the present embodiment includes the wafer stage 5, the objective lens 6, the half mirror 7, the illumination optical system 10, the detection optical system 20, the scanning unit 60, the imaging unit 3A, and Control unit 40. The wafer stage 5 is loaded with a semiconductor wafer W (hereinafter referred to as a wafer w) which is a substrate to be inspected in a state in which the pattern (reverse pattern) is formed to face upward. The wafer stage 5 is configured to be movable in three directions of x, y, and z axes orthogonal to each other (in addition, the upper and lower directions in Fig. 1 is the z-axis direction). Thereby, the 200952103 wafer stage 5' selects the wafer W to be movable in the X, y, and z axis directions. Further, the wafer stage 5 can be rotated around the z-axis. The illumination optical system 1 〇 'from the left side to the right side of FIG. 1 has, in order of its arrangement, a light source 1 1 (for example, a white LED or a halogen lamp, etc.), a condensing lens 12, an illuminance uniformization unit 13, and an aperture. The aperture 14, the field stop 15, the collimator lens 16, and the detachable polarizing element 17 (polarizing filter). Here, the light emitted by the light source 1 1 of the illumination optical system 10 is transparent.

過聚光透鏡12及照度均一化單元13,被導向孔徑光蘭14 A 及視野光闌15。照度均一化單元13能使照明光分散進而使 光量分布均一化。又’亦可包含干涉濾光器。孔徑光闌14 及視野光闌15 ’係以可相對照明光學系統1〇之光軸變更其 開口部大小及位置的方式而構成。因此,照明光學系統1 〇, 可藉由孔徑光闌14及視野光闌15的操作,進行照明區域 之大小及位置的變更,以及照明之開口角的調整。又,通 過孔徑光闌14及視野光闌15的光,經準直透鏡16而成為 & 平行光後,通過偏光元件17而射入半反射鏡7。 半反射鏡7將來自照明光學系統1〇的光反射至下方而 導向物鏡6。藉此,通過物鏡6之來自照明光學系統1〇的 光,落射照明於晶圓W。另一方面’落射照明於晶圓w的 光’可在晶圓W反射再次回到物鏡6,透過半反射鏡7而 射入至檢測光學系統20。 檢測光學系統20,由圖1之下側朝上側依其配置順序 依序具有:可拆裝之檢光元件21 (偏光濾光器)、透鏡22、 半稜鏡23、勃氏透鏡(Bertrand Lens)24、及具有視野光闌之 7 200952103 功能的圓板構件63。檢光元件21被配置成相對照明光學系 統10之偏光元件17成正交的狀態(偏光方向正交之狀態)。 由於照明光學系統10之偏光元件17與檢測光學系統2〇之 檢光元件21有滿足正交偏光鏡(cr〇ssedNic〇i)條件因此, 只要在晶圓w之圖案未旋轉偏光主轴,由檢測光學系統2〇 所檢測之光量會近於零。 半棱鏡23將入射光束分歧為二方向。通過半稜鏡Μ 之一方之光束,會透過勃氏透鏡24將晶圓w之像成像於具 有視野光闌之功能的圓板構件63,且將物鏡6之光瞳面= 像(亮度分布)投影至攝影部30之DMD (數位微鏡元件)元件 31。由於攝影部30之二維攝影元件33與dmd元件η成 共軛’因而會在二維攝影元件33之攝影面重現物鏡6在光 瞳面上之亮度分布’可藉二維攝影元# 33,對經過傅立葉 轉換之晶® W之影像(以下稱為傅立葉影像)進行攝影。此 外,勃氏透鏡(Bertrand Lens)24 一般雖係指使物鏡之後部焦 點面之像成像於目鏡之焦點面的會聚透鏡,但顯微鏡等之 光學系統-般而言像側為遠心狀態,且物鏡之後部焦點面 為光瞳面,因此本實施形態中’係將用以將物鏡6之光瞳 面之像成像於二維攝影元件33之攝影面的透鏡Μ稱為勃 氏透鏡24。 又,通過半稜鏡23之另—方的光束,被導向用以對未 經傅立葉轉換之通常之晶圓w影像進行攝影的第2攝影部 5〇。藉由將第2攝影部50拍攝之晶圓w之影像顯示在監測 器44,操作員能以目視放大觀察晶圓w表面。 200952103 此處,在本實施形態之缺陷檢查中拍攝傅立葉影像(亦 即物鏡6之光瞳面之像)乃是基於以下理由。若在缺陷檢查The condensing lens 12 and the illuminance uniformizing unit 13 are guided to the aperture light blue 14 A and the field stop 15 . The illuminance uniformization unit 13 disperses the illumination light to uniformize the light amount distribution. Also, an interference filter can be included. The aperture stop 14 and the field stop 15' are configured such that the size and position of the opening can be changed with respect to the optical axis of the illumination optical system 1A. Therefore, the illumination optical system 1 can change the size and position of the illumination area and the adjustment of the aperture angle of the illumination by the operation of the aperture stop 14 and the field stop 15. Further, the light passing through the aperture stop 14 and the field stop 15 is collimated by the collimator lens 16 and then incident on the half mirror 7 through the polarizing element 17. The half mirror 7 reflects the light from the illumination optical system 1 to the lower side and guides the objective lens 6. Thereby, the light from the illumination optical system 1 through the objective lens 6 is incident on the wafer W by the epi-illumination. On the other hand, the light that is incident on the wafer w can be reflected back on the wafer W and returned to the objective lens 6, and transmitted through the half mirror 7 to the detection optical system 20. The detecting optical system 20 is sequentially provided from the lower side toward the upper side of FIG. 1 in the order of its arrangement: a removable photodetecting element 21 (polarizing filter), a lens 22, a half turn 23, and a Bühler lens (Bertrand Lens) 24) and a disc member 63 having a function of a field of view of 200920091. The light detecting element 21 is disposed in a state orthogonal to the polarizing element 17 of the illumination optical system 10 (a state in which the polarization directions are orthogonal). Since the polarizing element 17 of the illumination optical system 10 and the photodetecting element 21 of the detecting optical system 2 have a condition of a crossed polarizer (cr〇ssedNic〇i), as long as the pattern of the wafer w does not rotate the polarizing spindle, the detection is performed. The amount of light detected by the optical system 2 会 will be close to zero. The half prism 23 divides the incident beam into two directions. The image of the wafer w is imaged by the Bühler lens 24 to the disk member 63 having the function of the field of view by the beam of one of the half beams, and the pupil plane of the objective lens 6 = image (luminance distribution) The DMD (Digital Micromirror Element) element 31 is projected onto the imaging unit 30. Since the two-dimensional photographic element 33 of the photographic portion 30 is conjugated with the dmd element η, the luminance distribution of the objective lens 6 on the pupil plane can be reproduced on the photographic surface of the two-dimensional photographic element 33. The image of the Fourier-transformed Crystal® W (hereinafter referred to as Fourier image) is photographed. Further, a Bertrand lens 24 generally refers to a converging lens that images an image of a focal plane behind a objective lens on a focal plane of an eyepiece, but an optical system such as a microscope is generally a telecentric state, and after the objective lens Since the focal plane of the portion is a pupil plane, in the present embodiment, a lens for imaging the image of the pupil plane of the objective lens 6 on the imaging surface of the two-dimensional imaging element 33 is referred to as a Bühler lens 24. Further, the other light beam passing through the half turn 23 is guided to the second imaging unit 5 for photographing the normal wafer w image not subjected to Fourier transform. By displaying the image of the wafer w imaged by the second imaging unit 50 on the monitor 44, the operator can visually observe the surface of the wafer w. 200952103 Here, the Fourier image (i.e., the image of the pupil plane of the objective lens 6) is taken during the defect inspection of the present embodiment for the following reasons. If the defect is checked

t使用將晶圓w之圖案直接拍攝出的影像,當圖案之間I 在檢查裝置之解析度以下時,則不能以光學方式檢測出圖 案的缺陷。另一方面,在傅立葉影像中,若是晶圓W之圖 案具有缺陷則會破壞反射光的對稱性’因構造性複折射所 致,與傅立葉影像之光轴正交之部分彼此之亮度或顏色等 參會產生變化。因此,即使圖案之間距在檢查裝置之解析度 以下時,仍可藉由檢測出傅立葉影像中之上述變化,而檢 測出圖案的缺陷(變化)。 進一步地,以下參昭圖?句 …圖2說明射入晶圓W之照明光之 入射角度與在光瞳面内之点德A g 像位置的關係。如圖2之虛線 所不’ §射入晶圓'之昭明本从 之成像位置為光瞳中心:另 λ ^ ^ , 另方面,如圖2之實線所示, :二=6:(相當時,光曈上之成像位置為 ❹=外緣一亦即’射入晶圓W之照明光的入射角度, t里上對應於光瞳内之半徑方向的位置mu 之光軸成像於同一半徑内之 入晶圊w的光。 ㈣先h㈣_角度射 _板二°:::::、,及具::述圓板構件63、旋轉 的旋轉編碼器62。馬達61,以圓板::件63之旋轉角 為中心轴,將圓板構件63旋轉驅動於相對^^對稱轴 之光軸呈垂直方向的面内。 d光學系統20 9 200952103 圓板構件63’如圖3所示,形成為具有17個針孔63ai 〜咖7的圓板狀。各針孔63al〜63an,係分別配置在圓 板構件63上彼此相異之直徑方向位置及周方向位置,第i 〜第17針孔63al〜63al7之中之任一針孔位於檢測光學系 統20之光學視野範圍内。藉此,決定晶圓w表面上之檢測 範圍(視野)。此外,本實施形態中,各針孔63ai〜63ai7, 以等間距間隔配置於圓板構件63之周方向,且隨著從位於 一端之第1針孔63al至位於另一端之第17針孔63ai7,其 直徑方向位置以等間距間隔向圓板構件63之中心(旋轉對 稱軸)偏移。 又,各針孔63al〜63al7之直徑0lmm,當使用倍率1〇〇 倍之物鏡6時,晶圓w表面上之檢測範圍(視野)成為直徑 0l〇//m。因此,各針孔63al〜63al7之形狀較佳為圓形(或 矩形)圖4所示之光學視野D,表示晶圓w表面上之檢測 光學系統20之光學視野,本實施形態中為直徑025〇^m。 又,位於光學視野D之内側的掃描區域c,係用以取得檢 查資料的正方形區域,其i邊為約17〇"m。 藉由馬達61使圓板構件63旋轉時,第1針孔63al掃 撝掃描區域C中最上列之資料取得位置A(1,”、A(2, ”、... (,1)第1〜第U針孔63al〜63al7,分別以在掃描區 域C偏移1次掃描量之位置依序掃描之方式,在圓板構件 63偏移於直徑方向位置。因此,第ι針孔63ai之掃描結束 後,第2針孔63a2掃描從第丨針孔63al之掃描位置偏移】 人掃拖量之位置之資料取得位置A(1,2)、A(2, 2)、…a(i7, 200952103 2)。因此,複數個針孔不會同時進入掃描區域c内。以下, 以同樣方式掃描偏移丨次掃描量之位置之資料取得位置 時第17針孔63al7掃描掃描區域c中最下列之資料取得 位置 A(l,17)、A(2,17)、…a(17,17)。t Using an image directly taken by the pattern of the wafer w, when the pattern I is below the resolution of the inspection device, the defect of the pattern cannot be optically detected. On the other hand, in the Fourier image, if the pattern of the wafer W has a defect, the symmetry of the reflected light is destroyed. The brightness or color of the portions orthogonal to the optical axis of the Fourier image due to the structural birefringence. Participation changes. Therefore, even if the distance between the patterns is below the resolution of the inspection apparatus, the defect (change) of the pattern can be detected by detecting the above change in the Fourier image. Further, the following is a map? [Fig. 2] illustrates the relationship between the incident angle of the illumination light incident on the wafer W and the position of the point image in the pupil plane. As shown by the dotted line in Figure 2, the imaging position of the Zhaoming this is the center of the pupil: another λ ^ ^ , on the other hand, as shown by the solid line in Figure 2, :==6: (equivalent When the imaging position on the pupil is ❹ = the outer edge, that is, the incident angle of the illumination light incident on the wafer W, the optical axis corresponding to the position mu in the radial direction in the pupil is imaged at the same radius The light entering the crystal 圊 w. (4) First h (four) _ angle shot _ board two °:::::, and:: said circular plate member 63, rotating rotary encoder 62. Motor 61, with a circular plate: The rotation angle of the member 63 is a central axis, and the disk member 63 is rotationally driven in a plane perpendicular to the optical axis of the axis of symmetry. d Optical system 20 9 200952103 The disk member 63' is as shown in FIG. It is formed into a disk shape having 17 pinholes 63ai to 7a. Each of the pinholes 63a1 to 63an is disposed in a diametrical position and a circumferential position which are different from each other on the disk member 63, and the i-th to the 17th pins are respectively arranged. Any one of the holes 63al to 63al7 is located within the optical field of view of the detecting optical system 20. Thereby, the detection range (field of view) on the surface of the wafer w is determined. Further, in the present embodiment, the pinholes 63ai to 63ai7 are arranged at equal intervals in the circumferential direction of the disk member 63, and from the first pinhole 63a1 at one end to the 17th pinhole 63ai7 at the other end. The diametrical position is offset from the center (rotational symmetry axis) of the disc member 63 at equal intervals. Further, the diameter of each of the pinholes 63a1 to 63al7 is 0 mm, and when the objective lens 6 is used at a magnification of 1 ,, the wafer is used. The detection range (field of view) on the surface of w becomes a diameter of 0 〇 / / m. Therefore, the shape of each of the pinholes 63a1 to 63al7 is preferably a circular (or rectangular) optical field D as shown in Fig. 4, indicating the surface of the wafer w The optical field of view of the detection optical system 20 is 025 〇m in the present embodiment. The scanning area c located inside the optical field of view D is a square area for obtaining inspection data, and the i side is about 17 〇"m. When the disc member 63 is rotated by the motor 61, the first pinhole 63al sweeps the data acquisition position A (1, ", A (2, ", ... ( 1) the first to the Uth pinholes 63a1 to 63al7 are respectively shifted by one scanning amount in the scanning area C In the sequential scanning mode, the disk member 63 is offset from the diametrical position. Therefore, after the scanning of the first pinhole 63ai is completed, the second pinhole 63a2 is scanned from the scanning position of the third pinhole 63al. The position of the sweeping position is obtained by the position A (1, 2), A (2, 2), ... a (i7, 200952103 2). Therefore, the plurality of pinholes do not enter the scanning area c at the same time. In the same manner, when scanning the data acquisition position at the position of the offset scan amount, the 17th pinhole 63al7 scans the most data acquisition position A(l, 17), A(2, 17), ... a (17) in the scan area c. , 17).

由於圓板構件63與晶圓W為共軛位置,因此藉由馬達 61使圓板構件63旋轉時,能一邊從任一針孔依序掃描晶圓 w之掃描區域C,一邊以攝影部3〇之各檢測元件36a,3补, 3 6c檢測關於掃描區域c的資料。以此方式,使用視野光闌 之針孔63al〜63al7來掃描,藉此,不需使晶圓載台5移動 於本實施形態中之1邊約17〇 # m的廣泛範圍,能高速地、 以與SEM(掃也型電子顯微鏡)相同之感度測定圖案的變 化。此外,伴隨圓板構件63之旋轉,各針孔63al〜63ai7 雖旋轉,但由於掃描區域c相對圓板構件63的半徑較小, 因此各針孔63al〜63al7之掃描執跡接近直線。 攝影部30的構成如圖1所示,具有DMD(DigitalSince the disk member 63 and the wafer W are in a conjugate position, when the disk member 63 is rotated by the motor 61, the scanning portion C of the wafer w can be sequentially scanned from any of the pinholes, and the image capturing portion 3 is used. Each of the detecting elements 36a, 3 is complemented, and 3 6c detects the data about the scanning area c. In this manner, the scanning is performed using the pinholes 63a1 to 63al7 of the field of view, whereby the wafer stage 5 does not need to be moved over a wide range of about 17 〇 #m in the present embodiment, and can be performed at a high speed. The change in sensitivity was measured in the same manner as the SEM (sweep electron microscope). Further, with the rotation of the disk member 63, the respective pinholes 63a1 to 63ai7 rotate, but since the radius of the scanning region c with respect to the disk member 63 is small, the scanning of the respective pinholes 63a1 to 63al7 is close to a straight line. The configuration of the photographing unit 30 is as shown in FIG. 1 and has a DMD (Digital).

Micromirror Device)元件 31、透鏡 32、二維攝影元件 33、 設置在反向側之透鏡34、分光稜鏡35、及3個檢測元件 36b,36c。DMD元件31具有在平面上並排之複數個可動式 微鏡(未圖示)。DMD元件31之微鏡,藉由電氣驅動,在 ON狀態時傾斜成使來自檢測光學系統2〇的光朝二維攝影 元件33的方向反射,在〇FF狀態時傾斜成使來自檢測光學 系統20的光朝檢測元件36a,36b,36c(分光稜鏡35)的方向 反射。 因此’由ON狀態之微鏡所反射之來自檢測光學系統 11 200952103 20的光,通過透鏡32(角度調整(Aorizu)光學系統)而被導向 二維攝影元件33的攝影面。另一方面,由0FF狀態之微鏡 所反射之來自檢測光學系統20的光,通過透鏡34(角度調 整光學系統),被分光稜鏡35分成R(紅色)、G (綠色)、B(藍 色)之光後,分別導向3個檢測元件36a,36b,36c。此外, 各檢測元件36a,36b,36c所獲得之光電訊號,係藉由未圖 示之配線傳至CPU43。 二維攝影元件33,係具有貝爾(Bayer)排列之彩色濾光 片陣列之CCD或CMOS等,以對前述之傅立葉影像實施攝 Ο 影。又,3個檢測元件36a,36b, 36c,係光二極體或突崩元 件等之高感度光檢測元件’分別檢測被分光稜鏡3 5分光後 之R(紅色)、G (綠色)、B(藍色)之光。 控制單元40的構成中具有:用以記錄傅立葉影像之資 料之記錄部41、輸入介面42、用以執行各種運算處理之 CPU43、監測器44、及操作部45,供執行檢查裝置}的統 籌控制。又,記錄部41、輸入介面42、監測器44、及操作 部45,分別與CPU43成電氣連接。cpiJ43係藉由程式的執 ❹ 行而解析傅立葉影像,求出由二維攝影元件33所拍攝之傅 立葉影像中對於圖案變化有高感度的區域。又,輸入介面 42具有連接記錄媒體(未圖示)之接頭,或是用來與外部電 腦(未圖示)連接的連接端子,以讀取來自記錄媒體或電腦之 資料。 以下參照圖8至圖10所示之流程圖說明使用具有上述 構成之檢查裝置i來檢查晶圓W的方法。首先係使用圖8 12 200952103 所示之流程圖,說明二維攝影元件33與DMD3 1之像素對 應表的作成方法。像素對應表之作成方法,首先在步驟 S101 ’係使照明光學系統1〇之偏光元件17與檢測光學系 統20之檢光元件21自光軸離開。接著,在步驟S102,將 圓板構件63定位成使檢查點(任一針孔63al〜63al7)成為 視野的中心。在次一步驟S103,將不具圖案之晶圓W藉晶 圓載台5而移動至物鏡6的下方(觀察位置)。 在次一步驟S104,係將照明光學系統1〇之光源丨丨點 亮。此時’由光源11所放出之照明光,透過聚光透鏡j 2 及照度均一化單元13,通過孔徑光闌14及視野光闌15, 經準直透鏡16成為平行光而由半反射鏡7反射後,通過物 鏡6照射於晶圓W。接著,來自晶圓w的反射光,通過物 鏡6及半反射鏡7射入檢測光學系統20,射入檢測光學系 統20的光’通過透鏡22、半稜鏡23、勃氏透鏡24、及圓 板構件63,將傅立葉影像投影在攝影部30的DMD元件3 1。 在次一步驟S105 ’使DMD元件31之1個像素(微鏡) 呈ON狀態,其他像素(微鏡)則呈OFF狀態。如此,由〇N 狀態之像素所反射之來自檢測光學系統20的光,通過透鏡 32而被導至二維攝影元件33的攝影面。 在次一步驟S106 ’由二維攝影元件33進行攝影,檢測 出由ON狀態之像素(微鏡)所反射的光,由CPU43算出由 ON狀態之像素所反射的光在攝影面上(二維攝影元件33)的 像素位置。 在次一步驟S107, CPU43將步驟S106所求出之二維攝 13 200952103 影元件33之像素位置,與此 (微鏡的位置)之關# ' 70件31的像素位置 )之關係’且錄於記錄部41的像素對應表。 隹-人—步驟S108,CPU43剌它b $ a 之所古後主μ U43判疋疋否已對DMD元件31 之所有像素皆實施測定。若 應夹之你士、 右以為π」,則結束像素對 應表之作成,若判定為「 *」 則進入步驟S109 〇 ^Sl〇9將DMD兀件31中呈〇N狀態之像素(微 兄)變更為尚未完成測定的像素,回到步驟議。藉由上述 之步驟’可將二維攝影元件 ,、件33之像素與DMD元件31之像 素之關係登錄於像素對應表。 其次’使用圖9所示之流程圖,說明在二維攝影元件 33所拍攝之傅立葉影像中,決定出對於圖案變化有高感度 之區域的方法。高咸声4 饮度Q域之決定方法,首先,在步驟 S201,將照明光學系統1〇 υ之偏先7L件17與檢測光學系統 20之檢光元件心成為正交偏光鏡咖⑽驗罐態之 方式插入至光轴上。接著,在步驟咖,以檢查點(任一針 孔63U〜咖7)成為視野中心之方式^位圓板構件W。在 次-步驟S203,使DMD元件31之所有像素(微鏡)成為〇n 狀態,使來自晶圓w的光完全朝二維攝影元件33的方向反 射。在次一步驟S 2 0 4,將· gg gp ju eg,. 將照明光學系統10的光源11點亮。 在-人步驟S205,將形成有反覆圖案之晶圓w裝載於 晶圓載台5上’將晶圓w上之測定圖案個照射區域之一 部分)藉晶圓載台5而移動至物鏡6下方。此時,係使用形 成有曝光條件(劑量及聚焦)各自不同之複數個同一形狀之 圖案之晶圓W。 200952103 如此,由光源11所放出之照明光,透過聚光透鏡i 2 及照度均一化單元13,通過孔徑光闌14及視野光闌ι5, 經準直透鏡16成為平行光後,通過偏光元件I?而被半反 射鏡7反射,之後通過物鏡6照射在晶圓w。又,來自晶 圓W之反射光,通過物鏡6及半反射鏡7而射入檢測光學 系統20,射入檢測光學系統20的光,通過檢光元件21、 透鏡22、半複鏡23、勃氏透鏡24、及圓板構件63,將傅 ©立葉像投影在攝影部30的DMD元件31。此時,由於DMD 元件31之所有像素(微鏡)呈on狀態,因此,由dmD元件 31所反射的光會通過透鏡32 ’將傅立葉像投影在二維攝影 元件3 3的攝影面。 在次一步驟S206 ’由二維攝影元件33對傅立葉像進行 攝影,將攝得之傅立葉影像記錄於記錄部41。 在次一步驟S207,由CPU43判定是否已對晶圓w上 之所有必要之圖案皆已實施測定。若判定為「是」,則前 ❿ 進至步驟S208,若判定為「否」,則回到步驟S205,將尚 未完成測定之圖案(其他之照射區域)移動至物鏡6的下 方,進行步驟S206的攝影。藉此,在記錄部41,對於同— 形狀之圖案,將會記錄有曝光條件相異之複數個傅立葉影 像的色彩資料。 ^ 在步驟S208,CpU43對於各傅立葉影像,於傅立葉影 像各個位置分別生成R(紅色)、G(綠色)、B(藍色)的亮度,資 料(平均值)。亮度資料之求取方法,首先,如圖n所示, 將傅立葉影像(例如帛1個幢框(frame)之傅立葉影像Fli)以 15 200952103 縱向、橫向成等間隔之方式分割成正方格子狀的複數個分 割區域P’對於傅立葉影像之各個分割區域p,各依照色別 而刀别求取RGB之免度值的平均。繼而,對於各個傅立葉 影像進行此步驟。藉此,對於由帛Η貞框至第n龍之傅 立葉影像FIl至FIn,分別就各傅立葉影像之各個分割區域 P,各自生成用以表示R、G、B各色成分之灰階的亮度資 、在次一步驟S209,如圖⑽示般地著眼於相同分割區 域CPU43按照R、G、B的各色成分分別生成灰階差資❹ 料,該灰階差資料,係表示在相同分割區域於傅立葉影像 !立至In間之灰階差。具體而言’若設傅立葉影像Η上之 任意分割區域為Pm,首先,對於各傅立葉影像叫至FIn, 分別抽出在各分割區域p之欠A二、、 之各色成分的亮度資料(在步驟 S208所求出者接英,作八^ )#者從與分龍域^對應之亮度資料 之灰階值中,抽出R、G、B各色成分各自之最大值與最小 值’算出所抽出之最大值與最小值的差分值。又對於所 有分割區域進行此等之步驟 ^ ^藉此,對於傅立葉影像之所❹ 有分割區域,按照R、G、B各弟出八々a 色成刀’各自生成用以表 在分割區域Pm之傅立葦影後网认> y、 之傅立葉影像間的灰階差的灰階差 階之最大值與最小值之差分值)。 在步驟S21〇’CPU43根據在步驟s2〇9所求出之灰 階差貝料(灰階之最大值與最 徂差分值),求出在傅 影像之分割區域中,灰階之最大值 ^ 大之顏色與分割區域,將嗲八、 力值為最 礼域冑該分割區域決定為高感度區域, 16 200952103 將此決定為檢測條件。圖13至圖i 5,係按照各個色成分示 出傅立葉影像之各分割區域之灰階差的分布狀態。在圖13 至圖15之例中’在圖15所示之B之灰階差的左上區域, 係最大感度的區域。藉此,可決定為了要高感度地檢測圖 案之線寬或分布狀態之變化,宜使用R、G、b中的哪一種 顏色、及使用傅立葉影像中的哪—個分割區域為佳。 如上述,可藉由以二維攝影元件33所攝得之影像檢測 未知之圖案的變化。然而,來自晶圓W之反射光微弱,二 維攝影元件33之曝光時間變長,會有產率無法提升的情形。 此處,使用圖1〇所示之流程圖,說明以高感度高速地 檢測圖案變化的方法。該圖案之檢測方法,首先,在步驟 S301,係將照明光學系統1〇之偏光元件17與檢測光學系 統20之檢光元件21插入於光軸上。 繼而’在步驟S302,CPU43決定DMD元件31之像素 (微鏡)中的ΟΝ/OFF狀態,以將來自晶圓w之反射光導至 各檢測元件36a,36b,36c的方向。具體而言,係參照由步 驟S101至S109所求出之二維攝影元件33與DMD元件31 的像素對應表,求出DMD元件31的像素中,與步驟S2〇1 至S210所求出之在二維攝影元件33上之高感度像素區域 (分割區域)相對應者。 在次一步驟S303’ CPU43將步驟S302所求出之與高感 度像素區域(分割區域)相對應之DMD元件31的像素設定成 OFF狀態’以導向各檢測元件36a,36b,36c的方向,且將 其他像素設定成ON狀態以導向二維攝影元件33的方向。 17 200952103 在次一步驟S304,將照明光學系統1〇之光源丨丨點亮β 其次,於步驟S305,藉由馬達61使圓板構件63以一定速 度旋轉。在次一步驟S306,將待檢查之晶圓w裝載於晶圓 載台5上,將晶圓W上之待檢查圖案(1個照射區域量)藉晶 圓載台5而移動至物鏡6的下方。Micromirror Device 31, lens 32, two-dimensional imaging element 33, lens 34 disposed on the opposite side, beam splitter 35, and three detecting elements 36b, 36c. The DMD element 31 has a plurality of movable micromirrors (not shown) arranged side by side on a plane. The micromirror of the DMD element 31 is electrically driven, and is tilted in the ON state so that the light from the detecting optical system 2A is reflected toward the two-dimensional imaging element 33, and is tilted in the 〇FF state so as to be from the detecting optical system 20 The light is reflected toward the direction of the detecting elements 36a, 36b, 36c (the beam splitter 35). Therefore, the light from the detecting optical system 11 200952103 20 reflected by the micromirror in the ON state is guided to the photographing surface of the two-dimensional imaging element 33 by the lens 32 (angle adjustment (Aorizu optical system)). On the other hand, the light from the detecting optical system 20 reflected by the micromirror of the 0FF state is divided into R (red), G (green), and B (blue) by the lens 35 (angle adjusting optical system). After the light of the color, the three detecting elements 36a, 36b, 36c are respectively guided. Further, the photoelectric signals obtained by the respective detecting elements 36a, 36b, 36c are transmitted to the CPU 43 by wires not shown. The two-dimensional imaging element 33 is a CCD or CMOS having a Bayer array of color filter arrays for performing imaging on the aforementioned Fourier image. Further, the three detecting elements 36a, 36b, 36c, the high-sensitivity photodetecting element 'such as a photodiode or a sag element, respectively detect R (red), G (green), B after being split by the splitter 35 (blue) light. The control unit 40 has a recording unit 41 for recording data of a Fourier image, an input interface 42, a CPU 43 for performing various arithmetic processing, a monitor 44, and an operation unit 45 for performing overall control of the inspection device. . Further, the recording unit 41, the input interface 42, the monitor 44, and the operation unit 45 are electrically connected to the CPU 43, respectively. The cpiJ43 analyzes the Fourier image by the execution of the program, and obtains a region having high sensitivity to the pattern change in the Fourier image captured by the two-dimensional imaging element 33. Further, the input interface 42 has a connector for connecting a recording medium (not shown) or a connection terminal for connecting to an external computer (not shown) for reading data from a recording medium or a computer. A method of inspecting the wafer W using the inspection apparatus i having the above configuration will be described below with reference to a flowchart shown in Figs. 8 to 10 . First, a method of creating a pixel corresponding table of the two-dimensional imaging element 33 and the DMD 31 will be described using the flowchart shown in Fig. 8 12 200952103. In the method of creating the pixel correspondence table, first, in step S101, the polarizing element 17 of the illumination optical system 1 and the light detecting element 21 of the detecting optical system 20 are separated from the optical axis. Next, in step S102, the disk member 63 is positioned such that the checkpoint (any of the pinholes 63a1 to 63al7) becomes the center of the field of view. In the next step S103, the unpatterned wafer W is moved to the lower side (observation position) of the objective lens 6 by the wafer stage 5. In the next step S104, the light source of the illumination optical system 1 is turned on. At this time, the illumination light emitted by the light source 11 passes through the condenser lens j 2 and the illuminance uniformizing unit 13, passes through the aperture stop 14 and the field stop 15 , passes through the collimator lens 16 and becomes parallel light, and is guided by the half mirror 7 . After the reflection, the objective lens 6 is irradiated onto the wafer W. Then, the reflected light from the wafer w is incident on the detection optical system 20 through the objective lens 6 and the half mirror 7, and the light incident on the detection optical system 20 passes through the lens 22, the half turn 23, the Bühler lens 24, and the circle. The plate member 63 projects the Fourier image onto the DMD element 31 of the imaging unit 30. In the next step S105', one pixel (micromirror) of the DMD element 31 is turned on, and the other pixels (micromirrors) are turned off. Thus, the light from the detecting optical system 20 reflected by the pixels of the 〇N state is guided to the imaging surface of the two-dimensional imaging element 33 through the lens 32. In the next step S106', the two-dimensional imaging element 33 performs imaging, and the light reflected by the pixel (micromirror) in the ON state is detected, and the CPU 43 calculates the light reflected by the pixel in the ON state on the imaging surface (two-dimensional The pixel position of the photographic element 33). In the next step S107, the CPU 43 compares the pixel position of the two-dimensional camera 13 200952103 image element 33 obtained in step S106 with the pixel position of the (the position of the micromirror) # '70 pixel 31'. The pixel correspondence table of the recording unit 41.隹-人-Step S108, the CPU 43 determines whether or not the B/A has been determined by all the pixels of the DMD element 31. If you want to clip it, the right is π", the completion of the pixel correspondence table is completed, and if it is judged as "*", the process proceeds to step S109. S^Sl〇9 to display the pixel of the DMD element 31 in the N state (micro-brother) ) Change to a pixel that has not completed the measurement and return to the step. The relationship between the two-dimensional imaging element, the pixel of the member 33 and the pixel of the DMD element 31 can be registered in the pixel correspondence table by the above-described step '. Next, a method of determining a region having high sensitivity to pattern change in the Fourier image captured by the two-dimensional imaging device 33 will be described using a flowchart shown in FIG. The method for determining the Q-domain of the high-salt sound 4 first, in step S201, the first 7L member 17 of the illumination optical system 1 and the detection element core of the detection optical system 20 are orthogonal polarized mirrors (10) The mode is inserted onto the optical axis. Next, in the step coffee, the disc member W is placed in such a manner that the checkpoint (any of the pinholes 63U to 7) becomes the center of the field of view. In the next step S203, all the pixels (micromirrors) of the DMD element 31 are brought into the 〇n state, and the light from the wafer w is completely reflected in the direction of the two-dimensional photographic element 33. In the next step S 2 0 4, the light source 11 of the illumination optical system 10 is turned on by gg gp jueg. In the step S205, the wafer w on which the reverse pattern is formed is placed on the wafer stage 5, and a portion of the irradiation pattern on the wafer w is moved by the wafer stage 5 to the lower side of the objective lens 6. At this time, a wafer W in which a plurality of patterns of the same shape having different exposure conditions (dose and focus) are formed is used. 200952103 In this way, the illumination light emitted by the light source 11 passes through the condensing lens i 2 and the illuminance homogenization unit 13 , passes through the aperture stop 14 and the field of view light 5 , passes through the collimator lens 16 and becomes parallel light, and passes through the polarizing element I. It is reflected by the half mirror 7, and then irradiated onto the wafer w through the objective lens 6. Further, the reflected light from the wafer W enters the detection optical system 20 through the objective lens 6 and the half mirror 7, and enters the light of the detection optical system 20, passes through the light detecting element 21, the lens 22, the half mirror 23, and the ray. The lens 24 and the disk member 63 project the Fourier image on the DMD element 31 of the imaging unit 30. At this time, since all the pixels (micromirrors) of the DMD element 31 are in the on state, the light reflected by the dmD element 31 projects the Fourier image on the photographic surface of the two-dimensional photographic element 33 through the lens 32'. The Fourier image is imaged by the two-dimensional imaging element 33 in the next step S206', and the captured Fourier image is recorded on the recording unit 41. At the next step S207, it is determined by the CPU 43 whether or not the measurement has been performed on all necessary patterns on the wafer w. If the determination is YES, the process proceeds to step S208. If the determination is "NO", the process returns to step S205, and the pattern (other irradiation region) that has not been measured is moved to the lower side of the objective lens 6, and the process proceeds to step S206. Photography. Thereby, in the recording unit 41, color information of a plurality of Fourier images having different exposure conditions is recorded for the same-shaped pattern. ^ In step S208, CpU43 generates luminances (average values) of R (red), G (green), and B (blue) at each position of the Fourier image for each Fourier image. For the method of obtaining the luminance data, first, as shown in FIG. n, the Fourier image (for example, the Fourier image Fli of one frame) is divided into square lattices at equal intervals in the longitudinal direction and the horizontal direction of 15 200952103. The plurality of divided regions P' are averaged for each of the divided regions p of the Fourier image, and each of the RGB values are obtained according to the color. This step is then performed for each Fourier image. Thereby, for each of the divided regions P of the Fourier images from the frame to the nth-long Fourier image FI1 to FIn, the brightness of each of the R, G, and B color components is generated. In the next step S209, focusing on the same divided area as shown in (10), the CPU 43 generates grayscale difference data for each color component of R, G, and B, and the grayscale difference data is expressed in the same divided region in Fourier. Image! The gray level difference between the two. Specifically, if any of the divided regions on the Fourier image is Pm, first, for each Fourier image, FIn is extracted, and luminance data of each color component of each of the divided regions p is extracted (in step S208). The obtained one is connected to the English, and the eight ^)# extracts the maximum and minimum values of the R, G, and B color components from the grayscale values of the luminance data corresponding to the sub-long field ^ The difference between the value and the minimum value. In addition, these steps are performed for all the divided regions. ^ Thus, for the Fourier image, the divided regions are formed according to the R, G, and B. The value of the difference between the maximum value and the minimum value of the gray-scale difference between the gray-scale differences between the Fourier images of the Fourier image. In step S21, the CPU 43 obtains the maximum value of the gray scale in the divided region of the Fu image based on the gray-scale difference beaker (the maximum value of the gray scale and the final difference value) obtained in the step s2〇9. The color of the big color and the segmentation area are determined as the most favorable area, and the divided area is determined as the high-sensitivity area. 16 200952103 This is determined as the detection condition. Fig. 13 to Fig. 5 show the distribution state of the gray scale difference of each divided region of the Fourier image in accordance with each color component. In the example of Figs. 13 to 15, the upper left area of the gray level difference of B shown in Fig. 15 is the area of the maximum sensitivity. Thereby, it can be determined that it is preferable to use which of the R, G, and b colors and which of the Fourier images are used in order to detect the change in the line width or the distribution state of the pattern with high sensitivity. As described above, the change of the unknown pattern can be detected by the image captured by the two-dimensional imaging element 33. However, the reflected light from the wafer W is weak, and the exposure time of the two-dimensional photographic element 33 becomes long, and there is a case where the yield cannot be improved. Here, a method of detecting a pattern change at a high speed with high sensitivity will be described using a flowchart shown in Fig. 1A. In the method of detecting the pattern, first, in step S301, the polarizing element 17 of the illumination optical system 1 and the light detecting element 21 of the detecting optical system 20 are inserted on the optical axis. Then, in step S302, the CPU 43 determines the ΟΝ/OFF state in the pixel (micromirror) of the DMD element 31 to direct the reflected light from the wafer w to the direction of each of the detecting elements 36a, 36b, 36c. Specifically, referring to the pixel correspondence table of the two-dimensional imaging element 33 and the DMD element 31 obtained in steps S101 to S109, the pixel of the DMD element 31 is obtained and found in steps S2〇1 to S210. The high-sensitivity pixel area (divided area) on the two-dimensional imaging element 33 corresponds to each other. In the next step S303', the CPU 43 sets the pixel of the DMD element 31 corresponding to the high-sensitivity pixel area (divided area) determined in step S302 to the OFF state ' to guide the directions of the respective detecting elements 36a, 36b, 36c, and The other pixels are set to the ON state to guide the direction of the two-dimensional imaging element 33. 17 200952103 In the next step S304, the light source 丨丨 of the illumination optical system 1 is turned on β. Next, in step S305, the disk member 63 is rotated by the motor 61 at a constant speed. In the next step S306, the wafer w to be inspected is loaded on the wafer stage 5, and the pattern to be inspected (the amount of one irradiation area) on the wafer W is moved to the lower side of the objective lens 6 by the wafer stage 5.

如此,由光源11放出的照明光,透過聚光透鏡丨2及 照度均一化單元13,通過孔徑光闌14及視野光闌15,經 準直透鏡16而成為平行光後,通過偏光元件17,在半反射 鏡7的反射之後,通過物鏡6而照射在晶圓w。繼而,來 自晶圓W的反射光,通過物鏡6及半反射鏡7而射入檢測 光學系統20,射入檢測光學系統2〇的光,通過檢光元件 21、透鏡22、半棱鏡23、勃氏透鏡24、及圓板構件63, 到達攝影部30的DMD元件31。 此時,對於晶圓W之圖案變化具有高感度之區域之反 射光,受到DMD元件31中呈〇FF业能★你t , 丁主UFF狀態之像素(微鏡)的反In this way, the illumination light emitted from the light source 11 passes through the condensing lens 丨 2 and the illuminance uniformizing unit 13 , passes through the aperture stop 14 and the field stop 15 , passes through the collimator lens 16 , becomes parallel light, and passes through the polarizing element 17 . After the reflection of the half mirror 7, the wafer w is irradiated through the objective lens 6. Then, the reflected light from the wafer W enters the detection optical system 20 through the objective lens 6 and the half mirror 7, and enters the light of the detection optical system 2, passes through the light detecting element 21, the lens 22, the half prism 23, and the ray. The lens 24 and the disk member 63 reach the DMD element 31 of the imaging unit 30. At this time, the reflected light of the region having high sensitivity to the pattern change of the wafer W is subjected to the inverse of the pixel (micromirror) of the UFF state in the DMD element 31.

射而通過透鏡34’藉由分光稜鏡35、红色之光被導向第W 測元件…、綠色之光被導向第2檢測元件36b、藍色之光 料向第3檢測元# H此時,使掃描部60之旋轉 構件63旋轉,據以從第1〜第π針孔63al〜63al7中之任 —針孔依序—邊掃描晶® W之掃描區域C,-邊高速地以 各檢測元件36a, 36b,36c檢測關於— % —維掃描區域C的資料。 在次一步驟 S307,CPU43 作 士 & W 、 作成資料取传表並記錄於記 錄部41。資料取得表,係表示 取丁上述資料取得位置A(l,1)… 與旋轉編碼器62之計數值(亦 1邛即,圓板構件63之旋轉角) 18 200952103 之對應關係的表。 將第之作成方法,首先,使圓板構件63旋轉, M . al(參照圖4)到達資料取得位置A(l, 之計數值登錄至資料取得表。接著,將第3 = 取彳·^置他1)時之旋轉編碼㈣之計 到達資料取得位置l(t i 將第1針孔63al分別 Λ計數值登錄至資料取H07,1)時之旋轉編碼器62之 © 钭取得表。藉此,完成1次掃描量之資料 取得表的登錄。 "田Ϊ惑貧村 旋轉=:6第2針孔63a2到達資料取得位置Α(1,2)時之 D 2之核值登錄至資料取得表。接著,將第2 f 2到達資料取得位置A(2,2)時之旋轉編碼器62之 別到達資料取 ,)Α(17,2)時之旋轉編碼器62 之汁數值登錄至資料取得表。 • 樣方式’對所有針孔63ai〜63an,分別將到 ^貝枓取得位置時之旋轉編碼器62之計數值登錄至資料取 1 °藉此’完成資料取得表。_ 5係顯示作為旋轉編碼 盗62使用丄周2〇〇〇〇脈衝之編碼器時之資料取得表的例 子。此外,資料取得位置的間隔亦可藉由解析度來改變。 :次-步驟測,_利用在步驟⑽作成之資料 得表,判定是否在所有資料取得位置藉由各檢測元件取 =,36c取得關於掃描區域料。未完成資料取得時, 則進至步驟S3G9,已完成資料取得時,前進至步驟s⑴。 19 200952103 此外’取得資料之順序,依資料取得位置Α(ι,1)〜A(i 7, 0、A(l’ 2)〜A(17, 2)、…A(l,17)〜A(17, 17)之順序進行亦 可,隨機進行亦可。 在步驟S309,CPU43利用在步驟S307作成之資料取得 表’藉由圓板構件63之旋轉’判定針孔是否到達未完成資 料取彳于的資料取得位置。若未到達則回到步驟S3〇9,若已 到達則前進至步驟S 3 10。 在步驟S3 10,CPU43在任一資料取得位置,藉由各檢 測元件36a, 36b,36c檢測自DMD元件31導引之高感度之 Ο 反射光,自該檢測訊號測定反射光之亮度(灰階)。此時,如 上所述,在各檢測元件36a, 36b,36c使用光二極體或突崩 疋件等’藉此可將與來自晶圓W之反射光對應之微弱訊號 同速地轉換成電氣訊號(檢測訊號)(例如,CCD為100ms程 度,相對於此,突崩元件則取樣頻率為數kHz、i個取樣時 間為數ms程度)’高速地檢測晶圓w上之圖案狀態(變化)。 此外’圖13至圖15之例,使用以第3檢測元件36c檢測之 藍色光。又,DMD元件3 1之像素(微鏡),即便〇N狀態時 〇 位置精度較高,但仍設定成在〇FF狀態時導向各檢測元件 36a,36b,3 6c,藉由使透鏡34為縮小透鏡,即使〇FF狀態 時之反射方向產生偏差,亦可將其控制在容許範圍内。 此外’檢測之反射光的亮度資料記錄在記錄部41,在 5己錄部4 1之資料取得表’登錄在進行該檢測之資料取得位 置已取得資料。接著,步驟S310之處理結束後返回步驟 S3 08。如上述,在步驟S3 〇8已完成所有資料取得時,前進 20 200952103 至步驟S311。 接著,在步驟S3U,CpU43從在步驟S31〇測定之亮度 資料及資料取仔表’作成圖16所示之二維亮度分布(灰階分 布)。圖16係測定結果的_ a丨. 果的一例,在一個格子記載一個亮度資 ❹ 料(本實施形態之情形,為晶圓W表面之副"爪之區域的 測定值)圖16之各格子的位置關係,與圖4之資料取得位 置A(l,^〜八⑴,〜A(i7,2)、··部⑺〜a⑴ 17)對應。 ’ 又’-維売度分布係顯示在監測器44,藉由操作人員 以目視確認測定結果(檢查結果),而能檢測出晶圓W上之 圖案的變化(亦即圖牵^^ *、 _ 圃茶之缺陷)。又’藉由將二維亮度分布顯 不成圖17所不之二維圖表,可易於辨識圖案的變化。 此夺亦可從測定之亮度資料自動地判定圖案之 優劣。關於圖案之自動敎方法,cpU43首先從圖Μ ^測 定結果算出亮度(灰階)之平均值,並比較所算出之平均值與 =設定:良品範圍。接著,若所算出之平均值為良品範 則判定為良品,若為良品範圍外則判定為不良。藉此, =判定圖案之優劣。此外,#由改變予以平均之資料 要範圍,駐料取彳技變^ K w上之視野尺寸的效 :二,☆了亮度之平均值以外,藉由算出最大值或最小 若欲算Γ定之良品範圍比較,亦能發現局部缺陷。再者, 出標準偏差,則可檢查圖案的偏差。又,於 SE= 雖直接使用測定之亮度資料,但藉由使其與 (掃描型電子顯微鏡)之圖案形狀之敎結果相關聯,從 21 200952103 測定之亮度資料算出圖案的線寬,使用算出之圖案的線寬 進行同樣的優劣判定亦可(參照後述(1)式)。 如上述’根據本實施形態之檢查裝置,由於具備掃描 部60 ,該掃描部60掃描與藉由各檢測元件36a,36b,36c 檢測亮度之光瞳面對應的晶圓W之範圍(亦即,掃描區域 C)’因此在二維檢查區域不使晶圓載台5移動,即可高速 地以與SEM(掃描型電子顯微鏡)同等之高感度,檢查形成於 晶圓W表面的圖案。 此外,掃描部60使用馬達61使形成於視野光闌之圓 © 板構件63之針孔(孔部)移動,以掃描掃描區域c。如此, 能以由馬達61與圓板構件63構成之簡單構造高速地進行 檢查。 又,此時,使用馬達61使形成於圓板構件63之複數 個針孔63al〜63ai7分別旋轉移動,據以從複數個針孔63&1 〜63al7中之任一針孔依序掃描掃描區域c。如此,利用圓 板構件63之旋轉移動進行掃描區域c的掃描,因此能縮小 掃描部60的尺寸。 ❹ 又,如上述,各檢測元件36a,36b,36c,在光瞳面(傅 立葉影像),檢測對應晶圓W表面狀態之變化(圖案的變 化)、亮度大幅變化之部分的亮度,藉此能進行高感度的檢 查。 又,一維攝影元件33及各檢測元件36a,36b,36c,檢 測來自晶圓W的光中與屬於直線偏光的照明光在偏光方向 大致正交的偏光成分,藉此而成為所謂的正交偏光鏡狀 22 200952103 態,而可㈣構造性複折射進行高感度的檢查。此外,偏 光元件17與檢光兀件21的偏光方向並不侷限於9〇。(正交 偏光鏡的狀態)’亦可配合在檢查對象圖案所產生之構造性 複折射造成之擴圓偏光的旋轉,而施以微幅的調整。 又,在此時,係藉由落射照明來照明於晶圓w的表面, 藉此而能使裝置尺寸達到小型化。 此外,於上述實施形態,設各針孔63al〜63ai7之尺寸 為直徑0lmm,但並不限於此,尺寸設為直徑0〇 5mm亦可。 此時,如圖6所示,在圓板構件63,形成有34個針孔63Η 〜63b34。此外,各針孔63bl〜63b34,與上述實施形態之 情形相同,在圓板構件63 ’上分別配置於彼此相異之直徑方 向位置及周方向位置,第1〜第34針孔63bl〜63b34中之 任一個針孔位於檢測光學系統2〇的光學視野範圍内。如 此,當使用倍率100倍之物鏡6時,晶圓w表面之檢測範 圍(視野)成為直徑05 // m,可變更解析度。此外,此時,藉 由馬達61使圓板構件63,旋轉後,如圖7所示,第1〜第 34針孔63bl〜63b34 ’分別在掃描區域c以資料取得位置 B(l, 1)〜B(34, 1)、B(1,2)〜B(34, 2)、…B(l,34)〜B(34, 34) 之順序進行掃描。 又’於上述實施形態’掃描部60之構成具有馬達61 及圓板構件63,但並不限於此。接著,參照圖18及圖19 說明掃描部的變形例。變形例之掃描部1 60之構成,如圖 18所示’具有矩形板狀之視野光闌板163、使視野光闌板 163直線移動之線性驅動部16丨、及檢測視野光闌板163之 23 200952103 位置之線性編碼器1 62。 線性驅動部161係由固定部161a與可動部161b構成。 固定部161 a係固定於裝置(檢測光學系統20),將可動部 161b驅動在直線上。在可動部161b安裝有視野光闌板 1 63 ’視野光闌板163係藉由線性驅動部161被驅動在相對 檢測光學系統20之光轴之垂直方向。 視野光闌板163,如圖19所示’形成為具有17個針孔 163&1〜163&17之矩形板狀。各針孔163&1〜163&17,在視 野光闌板163上係相對視野光闌板163之直線移動方向呈 斜向排列配置,第1〜第17針孔163al〜 163al7中之任一 個針孔位於檢測光學系統20的光學視野範圍内。藉此,決 定晶圓W表面上之檢測範圍(視野)。 又,各針孔163al〜I63al7為直徑0lmm,當使用倍率 100倍之物鏡6時,晶圓W表面之檢測範圍(視野)成為直徑 0l〇//m。藉由線性驅動部161使視野光闌板163直線移動 後,與上述實施形態之情形相同,第〗針孔丨63al掃描掃描 區域c中最上列之資料取得位置Α(1, υ、Α(2, υ、…A(i7, 1)(參照圖4)。第1〜第17針孔163al〜163al7,分別以在 掃描區域C偏移i讀㈣之位置依序掃描之方式,偏移 於與視野光《 163之直徑移動方向垂直之方向的位置。 因此, 第1針孔163al之掃描結束後,第2針孔l63a2掃描 從第1針孔163al之掃描位 取得位置 A(l,2)、A(2, 2)、 掃描偏移1次掃描量之位置The light passing through the lens 34' is guided to the Wth measuring element by the beam splitter 35, the red light is directed to the second detecting element 36b, and the blue light is directed to the third detecting element #H. The rotating member 63 of the scanning unit 60 is rotated, and the scanning area C of the crystal scanning layer W is sequentially scanned from any of the first to the πth pinholes 63a1 to 63al7, and the detecting elements are scanned at high speed. 36a, 36b, 36c detect data about the -%-dimensional scan area C. In the next step S307, the CPU 43 creates a data transfer table and records it in the recording unit 41. The data acquisition table is a table showing the correspondence between the above-mentioned data acquisition position A(l, 1)... and the count value of the rotary encoder 62 (i.e., the rotation angle of the disk member 63) 18 200952103. In the first method, first, the disk member 63 is rotated, and M. al (see Fig. 4) reaches the data acquisition position A (l, and the count value is registered in the data acquisition table. Next, the third = 彳·^ When the 1) rotation code (4) is reached, the data acquisition position l (ti is used to register the first pinhole 63al and the count value is registered to the data acquisition H07, 1). In this way, the registration of the data acquisition table of one scan amount is completed. "Tian Yu confuses the village. Rotation=:6 The second pinhole 63a2 reaches the data acquisition position Α(1,2) and the value of D 2 is registered in the data acquisition form. Next, when the 2nd f 2 arrives at the data acquisition position A (2, 2), the rotation encoder 62 arrives at the data acquisition, and when Α (17, 2), the juice value of the rotary encoder 62 is registered to the data acquisition table. . • Sample mode 'For each of the pinholes 63ai to 63an, the count value of the rotary encoder 62 when the position is obtained by the Becker is registered to the data 1° to complete the data acquisition table. The _ 5 shows an example of a data acquisition table when the encoder of the 编码 〇〇〇〇 〇〇〇〇 丄 丄 62 is used as the rotary code hacker 62. In addition, the interval at which the data is acquired can also be changed by the resolution. : Sub-step measurement, _ using the data created in step (10) to determine whether or not to take all the data acquisition locations by the respective detection elements =, 36c to obtain information about the scanning area. When the data acquisition is not completed, the process proceeds to step S3G9, and when the data acquisition is completed, the process proceeds to step s(1). 19 200952103 In addition, 'the order of obtaining the data, according to the data acquisition location ι(ι,1)~A(i 7, 0, A(l' 2)~A(17, 2),...A(l,17)~A The order of (17, 17) may be performed randomly, or may be performed at random. In step S309, the CPU 43 determines whether the pinhole has reached the unfinished data by the rotation of the disk member 63 by the data acquisition table created in step S307. If the data has not been reached, the process returns to step S3 to 9. If it has arrived, the process proceeds to step S3 10. In step S310, the CPU 43 obtains the position by any of the detecting elements 36a, 36b, 36c. The reflected light is detected from the high sensitivity guided by the DMD element 31, and the brightness (gray scale) of the reflected light is measured from the detection signal. At this time, as described above, the light detecting diodes are used for the respective detecting elements 36a, 36b, 36c or The smashing element, etc., can convert the weak signal corresponding to the reflected light from the wafer W into an electrical signal (detection signal) at the same speed (for example, the CCD is about 100 ms, and the sag component is sampled accordingly) The frequency is several kHz, i sampling time is a few ms)) 'High-speed detection of the wafer w The state of the case (change). In addition, in the example of Fig. 13 to Fig. 15, the blue light detected by the third detecting element 36c is used. Further, the pixel (micromirror) of the DMD element 31 has a higher positional accuracy even in the 〇N state. High, but still set to guide each of the detecting elements 36a, 36b, 3 6c in the 〇FF state, and by making the lens 34 a reduced lens, it can be controlled within the allowable range even if the direction of reflection in the FF state is deviated. Further, the brightness data of the detected reflected light is recorded in the recording unit 41, and the data acquisition table of the 5 recorded portion 4 1 is registered in the data acquisition position at which the detection is performed. Then, after the processing of step S310 is completed, Returning to step S3 08. As described above, when all the data acquisitions have been completed in step S3, the process proceeds to 20 200952103 to step S311. Next, in step S3U, CpU43 creates the brightness data and data from the measurement table in step S31. The two-dimensional luminance distribution (gray scale distribution) shown in Fig. 16. Fig. 16 is an example of the result of the measurement, and a luminance material is described in one grid (in the case of the present embodiment, the wafer W table) The positional relationship of each of the squares of the figure of Fig. 16 and the position A of the data of Fig. 4 (l, ^~8(1), ~A(i7,2), ···(7)~a(1) 17) Correspondence. The 'and'-dimensionality distribution is displayed on the monitor 44, and the operator can visually confirm the measurement result (inspection result), thereby detecting the change of the pattern on the wafer W (that is, the drawing ^^ *, _ 缺陷 tea defects). And 'by changing the two-dimensional brightness distribution to a two-dimensional chart not shown in Figure 17, the pattern change can be easily identified. This can also automatically determine the pros and cons of the pattern from the measured brightness data. Regarding the automatic 敎 method of the pattern, cpU43 first calculates the average value of the brightness (gray scale) from the measurement result, and compares the calculated average value with the = setting: good product range. Then, if the calculated average value is a good product, it is judged to be a good product, and if it is outside the good product range, it is judged to be bad. Thereby, = the merits of the pattern. In addition, the range of the data to be averaged by the change is determined by the effect of the size of the field of view on the K w: 2, ☆ outside the average value of the brightness, by calculating the maximum or minimum Local defects can also be found by comparing the range of good products. Furthermore, the standard deviation can be used to check the deviation of the pattern. Further, although the measured luminance data is directly used in SE=, the line width of the pattern is calculated from the luminance data measured in 21 200952103 by correlating the result with the pattern shape of the (scanning electron microscope), and the calculated line width is used. The line width of the pattern may be determined in the same manner (refer to the formula (1) described later). As described above, the inspection apparatus according to the present embodiment includes the scanning unit 60 that scans the range of the wafer W corresponding to the pupil plane of the luminance detected by each of the detecting elements 36a, 36b, and 36c (that is, In the scanning area C)', the wafer stage 5 is not moved in the two-dimensional inspection area, and the pattern formed on the surface of the wafer W can be inspected at high speed with the same high sensitivity as that of the SEM (scanning electron microscope). Further, the scanner unit 60 moves the pinhole (hole portion) of the disk member 63 formed in the field of view by the motor 61 to scan the scanning region c. Thus, the inspection can be performed at a high speed with a simple structure composed of the motor 61 and the disk member 63. Further, at this time, the plurality of pinholes 63a1 to 63ai7 formed in the disc member 63 are respectively rotated by the motor 61, and the scanning region is sequentially scanned from any of the plurality of pinholes 63 & 1 to 63al7. c. Thus, the scanning of the scanning region c is performed by the rotational movement of the disk member 63, so that the size of the scanning portion 60 can be reduced. Further, as described above, each of the detecting elements 36a, 36b, and 36c detects the change in the surface state of the wafer W (the change in the pattern) and the brightness of the portion in which the brightness greatly changes in the pupil plane (Fourier image). Perform a high-sensitivity inspection. Further, the one-dimensional imaging element 33 and each of the detection elements 36a, 36b, and 36c detect a polarization component that is substantially orthogonal to the polarization direction of the illumination light belonging to the linearly polarized light from the wafer W, thereby forming a so-called orthogonality. Polarized mirror 22 200952103 state, and (4) structural birefringence for high sensitivity inspection. Further, the polarization direction of the polarizing element 17 and the light detecting element 21 is not limited to 9 inches. The state of the (orthogonal polarizer) can also be adjusted in a slight adjustment by the rotation of the circularly polarized light caused by the structural birefringence generated by the inspection target pattern. Further, at this time, the surface of the wafer w is illuminated by epi-illumination, whereby the size of the device can be reduced. Further, in the above embodiment, the size of each of the pinholes 63a1 to 63ai7 is 0 mm, but the size is not limited thereto, and the size may be 0 to 5 mm in diameter. At this time, as shown in Fig. 6, 34 pin holes 63A to 63b34 are formed in the disk member 63. Further, in the same manner as in the above-described embodiment, each of the pinholes 63b1 to 63b34 is disposed in the disk member 63' in the diametrical position and the circumferential direction, and is in the first to 34th pinholes 63b1 to 63b34. Any one of the pinholes is located within the optical field of view of the detection optical system 2〇. Thus, when the objective lens 6 having a magnification of 100 times is used, the detection range (field of view) of the surface of the wafer w becomes a diameter of 05 // m, and the resolution can be changed. Further, at this time, after the disk member 63 is rotated by the motor 61, as shown in Fig. 7, the first to 34th pinholes 63b1 to 63b34' respectively acquire the position B (l, 1) in the scanning area c. Scanning is performed in the order of ~B(34, 1), B(1,2)~B(34, 2), ...B(l, 34)~B(34, 34). Further, in the above embodiment, the configuration of the scanning unit 60 includes the motor 61 and the disk member 63, but the invention is not limited thereto. Next, a modification of the scanning unit will be described with reference to Figs. 18 and 19 . In the configuration of the scanning unit 1 60 of the modified example, as shown in FIG. 18, a view plate 163 having a rectangular plate shape, a linear drive unit 16 that linearly moves the view stop plate 163, and a detection field stop plate 163 are provided. 23 200952103 Position linear encoder 1 62. The linear drive unit 161 is composed of a fixed portion 161a and a movable portion 161b. The fixing portion 161a is fixed to the device (detection optical system 20), and drives the movable portion 161b on a straight line. A field stop plate 1 63 is attached to the movable portion 161b. The field stop plate 163 is driven by the linear drive unit 161 in the vertical direction of the optical axis of the detection optical system 20. The field stop plate 163, as shown in Fig. 19, is formed in a rectangular plate shape having 17 pinholes 163 & 1 to 163 & Each of the pinholes 163 & 1 to 163 & 17 is arranged obliquely in the direction of linear movement of the field-of-view aperture plate 163 on the field-of-view aperture plate 163, and any one of the first to seventeenth pinholes 163a1 to 163al7 The holes are located within the optical field of view of the inspection optical system 20. Thereby, the detection range (field of view) on the surface of the wafer W is determined. Further, each of the pinholes 163a1 to I63al7 has a diameter of 0 lmm, and when the objective lens 6 having a magnification of 100 times is used, the detection range (field of view) of the surface of the wafer W becomes a diameter of 0 〇//m. After the linear driving unit 161 linearly moves the field stop plate 163, as in the case of the above-described embodiment, the pinhole hole 63a scans the uppermost data acquisition position 扫描 (1, υ, Α (2) in the scanning area c. , υ, ... A (i7, 1) (refer to Fig. 4). The first to seventeenth pinholes 163a1 to 163al7 are sequentially scanned in the scanning area C offset i reading (four) position, respectively, offset When the scanning of the first pinhole 163a1 is completed, the second pinhole 163a2 scans the position A (1, 2) from the scanning position of the first pinhole 163a1, A(2, 2), scan offset 1 scan position

置偏移1次掃描量之位置之資料 …A(17, 2)。以下’以同樣方式 之資料取得位置時,第17針孔 24 200952103 163al7掃描掃描區域c中最下列之資料取得位置Α〇, 17)、A(2,17)、·.. a(17,17)。 此外’視野光闌板163,與圓板構件63同樣地配置在 與晶圓W共輛的位置,因此藉由線性驅動部ι61使視野光 闌板163直線移動時,能一邊從任一針孔依序掃描晶圓w 之掃描區域c’ 一邊以攝影部30之各檢測元件36a,36b,36c 檢測關於掃描區域C的二維資料。以此方式,與上述實施 形態之情形相同’不需使晶圓載台5移動於1邊約17〇 " m 的廣泛範圍,能高速地、以與SEM(掃描型電子顯微鏡)相同 之感度測定圖案的變化。此外,視野光闌板163(可動部l61b) 之位置係由線性編碼器162檢測’若使用線性編碼器162 之計數值,則同樣地可作成上述資料取得表。 此外’上述實施形態中,雖係將對應於步驟S302所求 出之尚感度像素區域(分割區域)之DMD元件31的像素設定 成OFF狀態,而導向各檢測元件36a,36b, 36c的方向,且 使其他像素成ON狀態而導向二維攝影元件33的方向,但 並不侷限於此。例如’亦可如圖20所示,將半稜鏡38配 置在DMD元件3 1與透鏡32之間,使由DMD元件31朝向 一維攝影元件33之光的一部分,由半棱鏡38透過透鏡34 及分光棱鏡35而導向各檢測元件36a,36b,36c。在此情 形,步驟S303中的CPU43,係將對應於步驟S302所求出 之高感度像素區域(分割區域)之DMD元件31的像素設定成 ON狀態,而導向二維攝影元件33及各檢測元件36a,36b, 36c的方向,且將其他像素設為0FF狀態而不導向各檢測元 25 200952103 件36a,36b, 36c的方向。藉此,可使DMD元件31之像素 處於位置精度較高的ON狀態,將來自晶圓w的光導向各 檢測元件36a,36b,36c的方向。 又,在上述實施形態中,係以用來進行晶圓W之缺陷 檢查之檢查裝置1為其說明例,但被檢測基板並不侷限於 晶圓W ’例如液晶玻璃基板亦可。 又,在上述實施形態中’係根據灰階差資料(灰階之最 大值與最小值的差分值),以決定對圖案變化具有高感度的 區域,但其並不偈限於此。此處,使用圖21之流程圖,說 0 明咼感度區域之決定方法的變形例。此方法,與上述實施 形態之情形同樣地,係使用形成有曝光條件(劑量及聚焦) 各自不同之複數個同一形狀圖案的晶圓w,並根據各個圖 案之傅立葉影像與各圖案之線寬資料,來決定對於圖案變 化具有高感度的區域。此外,與上述之圖案相對應的線寬 資料,例如係利用散射計或掃描型電子顯微鏡(SEM)等線寬 測定器而測定者,&等線寬之㈣群,係預先藉由輸入介 面42之輸入而記錄於記錄部4卜又,作為掃描部,使用具 〇 有上述圓板構件63的掃描部6〇。 首先,與上述實施形態之情形同樣地,在步驟S25 i, 將照明光學系统1 〇之值伞;>、,^ 予示既ιυ之偏先疋件17與檢測光學系統2〇之檢 光兀件21插入光軸上。繼而,在步驟s252,以檢查點(任 針孔63al〜63al7)成為視野中心之方式定位圓板構件 63。在次步驟S253,使DMD元件31之所有像素(微鏡) 成0N狀態’使來自晶圓W的光完全朝二維攝影元件33的 26 200952103 方向反射。在次一步驟S254, 將照明光學系統10之光泝 1 1點亮。 K员、 在次一步驟S255,將形成有 自不同之複數個同一形狀圖案之7::=11量及聚焦)各 上,將…上之待測定圖案(/二裝::-載台5 叫‘、、、射區域之一部分、藉曰 圓載台5而移動至物鏡6的下方. 日曰 卜方。在之後的步驟S256,藉 Φ Ο 二維攝影元件33對傅立葉影像進行攝影,將測得之傅立葉 影像記錄於記錄部41。 在次一步驟S257,CPU43划-> β τ rU43判疋是否已對晶圓w上之 有圖案皆實施測定。若判定為「是 疋」則刖進至步驟S258, 若判定為「否」,則回到步驟S255,將尚未完成測定之圖 案(其他照射區域)移動至物鏡6的 J卜万以進行步驟S256 的攝影。 在步驟S258,CPU43與上述實施形態之情形同樣地, 對於各傅立葉影像,分別在各個傅立葉影像的分割區域生 成R(紅色)' G(綠色)、B(藍色)之亮度資料(平均值 繼而,在次-步驟S259’著眼於相同分割區域CPU” 依照R、G、B之各色成分,分別求出可表示各傅立葉影像 FL至FIn之相同分割區域中之灰階值與圖案線寬之變化率 的近似式。具體而言,若將傅立葉影像耵上之任意的分割 區域設為Pm’首先,係從記錄部41之中,讀取與各個傅 立葉影像FI,至FIn相對應之圖案線寬的資料。又,在此時, 對於各個傅立葉影像FIl至FIn,係分別抽出在分割區域pm 之各色成分的亮度資料(步驟S258所求出者)。接著,對於 27 200952103 各個傅立葉影像FI!至FIn,求出圖案線寬與在分割區域pm 之亮度資料之灰階值的對應關係。Set the data of the position of the offset by one time...A(17, 2). In the following section, when the position is obtained in the same manner, the 17th pinhole 24 200952103 163al7 scans the scanning area c for the most recent data acquisition position, 17), A(2, 17), ..... a (17, 17 ). Further, the 'viewing aperture plate 163 is disposed at a position shared with the wafer W in the same manner as the disk member 63. Therefore, when the field stop plate 163 is linearly moved by the linear drive unit ι 61, it can be taken from any pinhole. The two-dimensional data on the scanning area C is detected by the respective detecting elements 36a, 36b, 36c of the photographing unit 30 while sequentially scanning the scanning area c' of the wafer w. In this way, as in the case of the above-described embodiment, the wafer mount 5 can be moved at a high speed and the same sensitivity as that of the SEM (scanning electron microscope) without moving the wafer stage 5 to a wide range of about 17 Å. Pattern changes. Further, the position of the field stop plate 163 (movable portion l61b) is detected by the linear encoder 162. If the count value of the linear encoder 162 is used, the above-described data acquisition table can be similarly created. Further, in the above-described embodiment, the pixels of the DMD element 31 corresponding to the sensitivity pixel region (divided region) obtained in the step S302 are set to the OFF state, and the directions of the respective detecting elements 36a, 36b, and 36c are guided. Further, the other pixels are turned to the ON state to be directed to the direction of the two-dimensional imaging element 33, but the invention is not limited thereto. For example, as shown in FIG. 20, the half turn 38 may be disposed between the DMD element 31 and the lens 32 such that a portion of the light directed from the DMD element 31 toward the one-dimensional imaging element 33 passes through the lens 34 by the half prism 38. And the dichroic prism 35 is guided to the respective detecting elements 36a, 36b, 36c. In this case, the CPU 43 in step S303 sets the pixel of the DMD element 31 corresponding to the high-sensitivity pixel area (divided area) obtained in step S302 to the ON state, and guides the two-dimensional imaging element 33 and each detection element. The directions of 36a, 36b, 36c, and the other pixels are set to the 0FF state without being directed to the directions of the respective detecting elements 25 200952103 pieces 36a, 36b, 36c. Thereby, the pixels of the DMD element 31 can be placed in an ON state with a high positional accuracy, and the light from the wafer w can be directed to the direction of each of the detecting elements 36a, 36b, 36c. Further, in the above-described embodiment, the inspection apparatus 1 for performing defect inspection of the wafer W is exemplified, but the substrate to be inspected is not limited to the wafer W' such as a liquid crystal glass substrate. Further, in the above-described embodiment, the region having high sensitivity to the pattern change is determined based on the gray scale difference data (difference value between the maximum value and the minimum value of the gray scale), but the present invention is not limited thereto. Here, a modification of the method for determining the sensitivity region will be described using the flowchart of Fig. 21. In this method, as in the case of the above-described embodiment, a wafer w in which a plurality of patterns of the same shape having different exposure conditions (dose and focus) are formed is used, and the line width information of the Fourier image and each pattern of each pattern is used. To determine the area with high sensitivity to pattern changes. Further, the line width data corresponding to the above-described pattern is measured by, for example, a line width measuring device such as a scatterometer or a scanning electron microscope (SEM), and the (4) group of line widths is input in advance through an input interface. The input of 42 is recorded in the recording unit 4, and as the scanning unit, the scanning unit 6A having the above-described disc member 63 is used. First, in the same manner as in the above embodiment, in step S25i, the value of the illumination optical system 1 is erected; >, and the detection of the eccentricity 17 and the detection optical system 2 The jaw 21 is inserted into the optical axis. Then, in step s252, the disc member 63 is positioned such that the checkpoint (the pinholes 63a1 to 63al7) becomes the center of the field of view. In the next step S253, all the pixels (micromirrors) of the DMD element 31 are brought into the ON state, and the light from the wafer W is completely reflected toward the direction of the 26200952103 of the two-dimensional imaging element 33. At the next step S254, the light of the illumination optical system 10 is turned on. The K member, in the next step S255, will form a pattern of 7::=11 and focus from a plurality of different patterns of the same shape, and the pattern to be determined on the top (:2::-stage 5) One part of the ',, and shot area is moved to the lower side of the objective lens 6 by the round stage 5. The next step S256, the Fourier image is photographed by the Φ 二维 two-dimensional imaging element 33, and the measurement is performed. The obtained Fourier image is recorded in the recording unit 41. In the next step S257, the CPU 43 determines whether or not the pattern on the wafer w has been measured. If the determination is "Yes", then the image is made. In step S258, if the determination is "NO", the process returns to step S255, and the pattern (other irradiation area) that has not been measured is moved to the image of the objective lens 6 to perform the shooting in step S256. In step S258, the CPU 43 and the above In the same manner as in the embodiment, for each Fourier image, luminance data of R (red) 'G (green) and B (blue) are generated in the divided regions of the respective Fourier images (average, then, sub-step S259' Focus on the same split area CPU" according to R For each color component of G and B, an approximate expression that can represent the rate of change of the grayscale value and the pattern line width in the same divided region of each Fourier image FL to FIn is obtained. Specifically, if the Fourier image is arbitrarily selected First, the divided area is set to Pm'. First, the data of the pattern line width corresponding to each of the Fourier images FI and FIn is read from the recording unit 41. Also, at this time, for each of the Fourier images FI1 to FIn, The luminance data of each color component in the divided region pm is extracted (the one obtained in step S258). Next, for each of the Fourier images FI! to FIn of 27 200952103, the pattern line width and the grayness of the luminance data in the divided region pm are obtained. The correspondence between the order values.

繼而’根據圖案線寬與在分割區域Pm之灰階值的對應 關係,藉由最小平方法求出表示在分割區域pm之灰階值與 圖案線寬之變化率的近似式。此處’將對應於各傅立葉影 像FI!至FIn之圖案的線寬設為y,將分割區域Pm之B(4 R 或是G)的灰階值設為x ’斜率設為a,y截距設為b,則近 似式能以下列之(1)式來表示。Then, based on the correspondence relationship between the pattern line width and the gray scale value in the divided region Pm, an approximate expression indicating the rate of change of the gray scale value and the pattern line width in the divided region pm is obtained by the least square method. Here, 'the line width corresponding to the pattern of each Fourier image FI! to FIn is set to y, and the gray scale value of B (4 R or G) of the divided area Pm is set to x 'the slope is set to a, y When the distance is set to b, the approximate expression can be expressed by the following formula (1).

y = ax + b......⑴ 再者,係數a之絕對值,相當於對應圖案線寬之變化之 灰階變化的逆數(亦即,係對於圖案變化之檢測感度的逆 數)。換言之,上述係數a之絕對值越小,就算線寬的差相 同,仍使傅立葉影像的灰階變化增大,因此,對於圖案變 化之檢測感度將會更高。又,對於所有分割區域,依R、'G、 B之各色成分而分別進行此等之步驟。y = ax + b (1) Furthermore, the absolute value of the coefficient a corresponds to the inverse of the gray-scale change of the change in the line width of the corresponding pattern (that is, the inverse of the sensitivity of the detection of the pattern change) ). In other words, the smaller the absolute value of the above coefficient a, the more the difference in line width is, the more the gray scale change of the Fourier image is increased, and therefore the detection sensitivity for the pattern change will be higher. Further, for all the divided regions, these steps are performed for each of the color components of R, 'G, and B.

繼而’在步驟S260,CPU43在傅立葉影像上之各分: 區域,依R、G、B之各色成分,分別求出在步驟⑽』 得到之近似式與圖案之線寬的相關誤差。具體而言,係彳 照R、G、B之各色成分’分別算出對應於各傅立葉影像ρ 至FIn之圖案線寬、與使用近似式所算出之圖案線寬的偏 之資料,根據所算出之偏差之資料,對於各分割區域之: 個色成分分別算出標準差’以該值作為相關誤差。 繼而,在步驟S261,CPU43根據在步驟s259 係數a與步驟S260所求出的相關誤差,求出在傅立葉影; 28 200952103 之分割區域中,係數a之絕對值低且相關誤差極小的分割區 域將該刀割區域決定為高感度之區域,將此決定為檢測 條件。具體而言,例如,係按照係數a之絕對值低與相關誤 差小而對各個分割區域進行計分,根據該計分的結果而決 定出感度高之分割區域。藉此方式,同樣能夠為了要高感 度地檢測圖案線寬或分布狀態的變化,而決定宜使用r、G、 B中的哪一種頻色,及使用傅立葉影像中的哪一分割區域為 佳。 ’ 此外,上述實施形態中,雖使用DMD元件3丨將反射 角度切換在ON狀態與〇FF狀態,但並不限於此,使用 SLM(空間光調變器:sPaCe Light Modulator)等之光空間調 變器,可分別取出R(紅色)、G(綠色)、B(藍色)用之取樣光。 又’藉由掃描固定微鏡求出最佳檢測位置,在將微鏡配置 於該最佳檢測位置之狀態下進行取樣亦可獲得與使用 DMD元件3 1等之情形同等的資訊。 【圖式簡單說明】 圖1係本發明之檢查裝置的概要圖。 圖2係顯示進入晶圓之照明光之入射角度與在光瞳内 之成像位置之關係的說明圖。 圖3係圓板構件的俯視圖。 圖4係顯示掃描區域與資料取得位置的圖。 圖5係顯示資料取得表的圖。 圖6係顯示圓板構件之變形例的俯視圖。 29 200952103 圖7係顯示掃描區域與資料取得位置之變形例的圖。 圖§係顯示二維攝影元件與DMD元件之像素對應表之 作成方法的流程圖。 圖9係顯示對於圖案變化有高感度之區域之決定方法 的流程圖。 圖1 〇係顯示以高感度高速地檢測圖案之變化之方法的 流程圖。 圖11係顯示將傅立葉影像予以區域分割之狀態之一例 的圖。 ❹ 圖係顯示亮度資料之取出狀態的示意圖。 圖 13 係 顯 示 傅 立 葉 影像 中 R 之 灰階 差 之 分布 狀 態 的 圖‘ > 圖 14 係 顯 示 傅 立 葉 影像 中 G 之 灰階 差 之 分布 狀 態 的 圖‘ 3 圖 15 係 顯 示 傅 立 葉 影像 中 B 之 灰階 差 之 分布 狀 態 的 圖’ 3 圖16係顯示檢查結果之顯示例的圖。 圖17係顯示檢查結果之另一顯示例的圖。 圖1 8係顯示檢查裝置之變形例的概要圖。 圖19係視野光闌構件的俯視圖。 圖20係顯示檢查裝置之第2變形例的概要圖。 圖21係顯示高感度區域之決定方法之變形例的流程 圖0 30 200952103 主要元件符號說明 W 晶圓(被檢測基板) 1 檢查裝置 10 照明光學系統(照明部) 17 偏光元件 20 檢測光學系統(觀察光學系統) 21 檢光元件 30 攝影部 36a 第1檢測元件(檢測部) 36b 第2檢測元件(檢測部) 36c 第3檢測元件(檢測部) 40 控制單元 43 CPU(檢查部) 60 掃描部 61 馬達(驅動部) 63 圓板構件(板狀構件) 63 圓板構件(變形例) 63al〜63al7 針孔(孔部) 63bl〜63b34 針孔(變形例) 160 掃描部(變形例) 161 線性驅動部(161a固定部,161b 163 視野光闌構件(板狀構件) 31Then, in step S260, the CPU 43 obtains the correlation error between the approximate expression obtained in the step (10) and the line width of the pattern, based on the respective color components of R, G, and B on the Fourier image. Specifically, the data of each of the color components R of R, G, and B is calculated by calculating the line width of each of the Fourier images ρ to FIn and the deviation of the line width calculated by using the approximate expression. For the data of the deviation, for each of the divided regions: the color component is calculated as the standard deviation', and the value is used as the correlation error. Then, in step S261, the CPU 43 obtains, based on the correlation error obtained in the step a s259 coefficient a and the step S260, that the divided region in which the absolute value of the coefficient a is low and the correlation error is extremely small in the divided region of Fourier shadow; 28 200952103 This cutting area is determined as a region of high sensitivity, which is determined as a detection condition. Specifically, for example, each divided region is scored according to the low absolute value of the coefficient a and the correlation error is small, and the divided region having high sensitivity is determined based on the result of the scoring. In this way, it is also possible to determine which one of r, G, and B is to be used, and which of the Fourier images is used, in order to detect the change in the line width or the distribution state with high sensitivity. Further, in the above-described embodiment, the DMD element 3 is used to switch the reflection angle between the ON state and the 〇FF state. However, the present invention is not limited thereto, and an optical spatial adjustment such as an SLM (SPaCe Light Modulator) is used. For the transformer, the sampled light for R (red), G (green), and B (blue) can be taken out separately. Further, by scanning the fixed micromirror to obtain an optimum detection position, sampling with the micromirror disposed at the optimum detection position can also obtain information equivalent to the case of using the DMD element 31 and the like. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view of an inspection apparatus of the present invention. Fig. 2 is an explanatory view showing the relationship between the incident angle of the illumination light entering the wafer and the imaging position in the pupil. Figure 3 is a top plan view of the disc member. Fig. 4 is a view showing a scanning area and a data acquisition position. Fig. 5 is a view showing a data acquisition table. Fig. 6 is a plan view showing a modification of the disk member. 29 200952103 Fig. 7 is a view showing a modification of the scanning area and the data acquisition position. Figure § is a flow chart showing a method of creating a pixel correspondence table between a two-dimensional imaging element and a DMD element. Fig. 9 is a flow chart showing a method of determining an area having high sensitivity to pattern change. Fig. 1 is a flow chart showing a method of detecting a change in a pattern at a high speed with high sensitivity. Fig. 11 is a view showing an example of a state in which a Fourier image is divided into regions. ❹ The figure shows a schematic diagram of the removal status of the brightness data. Fig. 13 is a diagram showing the distribution state of the gray level difference of R in the Fourier image. Fig. 14 is a diagram showing the distribution state of the gray level difference of G in the Fourier image. 3 Fig. 15 shows the gray scale of B in the Fourier image. Diagram of the distribution state of the difference '3 Fig. 16 is a diagram showing a display example of the inspection result. Fig. 17 is a view showing another display example of the inspection result. Fig. 1 is a schematic view showing a modification of the inspection apparatus. Figure 19 is a plan view of a field stop member. Fig. 20 is a schematic view showing a second modification of the inspection apparatus. Fig. 21 is a flowchart showing a modification of the method for determining the high sensitivity region. 0 30 200952103 Main component symbol description W Wafer (substrate to be inspected) 1 Inspection device 10 Illumination optical system (illumination portion) 17 Polarization element 20 Detection optical system ( Observation optical system 21 Photodetection element 30 Photodetection unit 36a First detection element (detection unit) 36b Second detection element (detection unit) 36c Third detection element (detection unit) 40 Control unit 43 CPU (inspection unit) 60 Scanning unit 61 Motor (drive unit) 63 Disc member (plate member) 63 Disc member (Modification) 63al to 63al7 Pinhole (hole) 63bl to 63b34 Pinhole (Modification) 160 Scanning section (Modification) 161 Linear Drive unit (161a fixing portion, 161b 163 field diaphragm member (plate member) 31

Claims (1)

200952103 七、申請專利範圍: i一種檢查裝置,具備: 照明部’將照明光照射至被檢測基板表面; 觀察光學系統,用以放大觀察被該照明光照射之該被 檢測基板表面; 檢測部’檢測該觀察光學系統中來自該被檢測基板之 反射光在光瞳面的亮度;200952103 VII. Patent application scope: i An inspection device comprising: an illumination unit that illuminates illumination light onto a surface of the substrate to be inspected; an observation optical system for magnifying observation of a surface of the substrate to be inspected illuminated by the illumination light; Detecting brightness of the reflected light from the detected substrate in the viewing optical system on the pupil plane; 檢查部,根據該檢測部所檢測之該亮度檢查該被檢測 基板表面;以及 掃描部,掃描與檢測出該亮度之該光曈面對應之該被 檢測基板的範圍。 2·如申請專利範圍第i項之檢查裝置,其中,該掃描部 :有··具備作為視野光闌之光學開口部的板狀構件、及驅 動該光學開口部的驅動部; 便用該驅動部使該光學 邱揮描於該範闲„ 件形成H請專利錢第2項之檢查裝置,其中,該板狀The inspection unit checks the surface of the substrate to be inspected based on the brightness detected by the detecting unit, and the scanning unit scans a range of the substrate to be inspected corresponding to the pupil surface on which the brightness is detected. 2. The inspection apparatus according to claim i, wherein the scanning unit includes: a plate-shaped member having an optical opening as a field stop, and a driving unit that drives the optical opening; The Ministry of the Ministry of the People’s Republic of China, in the form of an inspection device, 別形成在,板狀且作為該光學開口部之複數個孔部係 =成在該板狀構件上彼此相異之直財向及周方向 s驅動。Ρ係構成為以該板狀構件之 軸旋轉驅動該板狀構件; ㈣象軸為中心 使用該驅動部使形成於該板狀構 別旋轉移動,攄 〜複數個孔部分 媒U從3亥複數個孔部中夕知 該範圍。 一孔部依序掃描 32 200952103 其中,該驅動部 4.如申請專利範圍第2項之檢查裝置 使該板狀構件直線移動; 孔部係分別以在該板狀構 列之方式形成; 作為該光學開口部之複數個 件上相對該直線移動方向斜向排 使用該驅動部使形成於該板狀構 调·旰之该複數個孔部分 別直線移動’據以從該複數個孔部中 | τ之任一孔部依序掃描 該範圍。 ❹Further, the plurality of hole portions which are formed in a plate shape and serve as the optical opening portion are driven in a straight line direction and a circumferential direction s which are different from each other on the plate member. The lanthanoid system is configured to rotationally drive the plate-shaped member by the axis of the plate-shaped member; (4) the driving portion is used to rotate the plate-shaped member by using the driving portion as a center, and the plurality of holes are partially U-shaped from The range is known in the middle of the hole. a hole portion is sequentially scanned 32 200952103, wherein the driving portion 4. The inspection device of claim 2 of the patent scope moves the plate member linearly; the hole portions are respectively formed in the plate-like configuration; The plurality of optical opening portions are obliquely aligned with respect to the linear movement direction. The driving portion is used to linearly move the plurality of holes formed in the plate-like configuration and the plurality of holes from the plurality of holes. Any of the holes of τ sequentially scans the range. ❹ 5.如申請專利範圍帛i項之檢查裳置,其中,該檢測部 係檢測在該光瞳面上,對應該被檢測基板表面狀態之變化 而亮度大幅變化部分之亮度。 6·如申請專利範圍第1項之檢查裝置,其中,該照明光 係照射至具有反覆圖案之該被檢測基板表面的直線偏光; 該檢測部,檢測來自該被檢測基板之光中之偏光方向 與該直線偏光大致正交之偏光成分。 7.如申請專利範圍第6項之檢查裝置,其中,該照明 部’係藉由落射照明將該照明光照射至該被檢測基板表面。 八、圖式: (如次頁) 335. The inspection apparatus according to the scope of application of the patent item ii, wherein the detection unit detects the brightness of the portion where the brightness of the substrate is largely changed in response to a change in the surface state of the substrate to be detected. 6. The inspection apparatus according to claim 1, wherein the illumination light is irradiated onto a linearly polarized light having a surface of the detected substrate having a reverse pattern; and the detecting portion detects a polarization direction of light from the detected substrate A polarized component that is substantially orthogonal to the linearly polarized light. 7. The inspection apparatus of claim 6, wherein the illumination unit illuminates the illumination light onto the surface of the substrate to be inspected by epi-illumination. Eight, the pattern: (such as the next page) 33
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