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TW201901291A - Apparatus and method for detecting a photomask - Google Patents

Apparatus and method for detecting a photomask Download PDF

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Publication number
TW201901291A
TW201901291A TW106141158A TW106141158A TW201901291A TW 201901291 A TW201901291 A TW 201901291A TW 106141158 A TW106141158 A TW 106141158A TW 106141158 A TW106141158 A TW 106141158A TW 201901291 A TW201901291 A TW 201901291A
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mask
wafer
test
images
different
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TW106141158A
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TWI755453B (en
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阿布都拉罕 賽斯金納
穆罕默德 梅迪 丹尼斯帕納
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美商克萊譚克公司
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Priority claimed from US15/803,628 external-priority patent/US10395361B2/en
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    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/20Exposure; Apparatus therefor
    • G03F7/2051Exposure without an original mask, e.g. using a programmed deflection of a point source, by scanning, by drawing with a light beam, using an addressed light or corpuscular source
    • G03F7/2059Exposure without an original mask, e.g. using a programmed deflection of a point source, by scanning, by drawing with a light beam, using an addressed light or corpuscular source using a scanning corpuscular radiation beam, e.g. an electron beam
    • G03F7/2063Exposure without an original mask, e.g. using a programmed deflection of a point source, by scanning, by drawing with a light beam, using an addressed light or corpuscular source using a scanning corpuscular radiation beam, e.g. an electron beam for the production of exposure masks or reticles
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F1/00Originals for photomechanical production of textured or patterned surfaces, e.g., masks, photo-masks, reticles; Mask blanks or pellicles therefor; Containers specially adapted therefor; Preparation thereof
    • G03F1/68Preparation processes not covered by groups G03F1/20 - G03F1/50
    • G03F1/82Auxiliary processes, e.g. cleaning or inspecting
    • G03F1/84Inspecting
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/0002Lithographic processes using patterning methods other than those involving the exposure to radiation, e.g. by stamping
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70483Information management; Active and passive control; Testing; Wafer monitoring, e.g. pattern monitoring
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70483Information management; Active and passive control; Testing; Wafer monitoring, e.g. pattern monitoring
    • G03F7/70605Workpiece metrology
    • G03F7/706843Metrology apparatus
    • G03F7/706851Detection branch, e.g. detector arrangements, polarisation control, wavelength control or dark/bright field detection
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70691Handling of masks or workpieces
    • G03F7/70733Handling masks and workpieces, e.g. exchange of workpiece or mask, transport of workpiece or mask
    • G03F7/70741Handling masks outside exposure position, e.g. reticle libraries
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/027Making masks on semiconductor bodies for further photolithographic processing not provided for in group H01L21/18 or H01L21/34
    • H01L21/0271Making masks on semiconductor bodies for further photolithographic processing not provided for in group H01L21/18 or H01L21/34 comprising organic layers
    • H01L21/0273Making masks on semiconductor bodies for further photolithographic processing not provided for in group H01L21/18 or H01L21/34 comprising organic layers characterised by the treatment of photoresist layers
    • H01L21/0274Photolithographic processes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L22/00Testing or measuring during manufacture or treatment; Reliability measurements, i.e. testing of parts without further processing to modify the parts as such; Structural arrangements therefor
    • H01L22/10Measuring as part of the manufacturing process
    • H01L22/12Measuring as part of the manufacturing process for structural parameters, e.g. thickness, line width, refractive index, temperature, warp, bond strength, defects, optical inspection, electrical measurement of structural dimensions, metallurgic measurement of diffusions

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Health & Medical Sciences (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Library & Information Science (AREA)
  • Toxicology (AREA)
  • Preparing Plates And Mask In Photomechanical Process (AREA)
  • Investigating Materials By The Use Of Optical Means Adapted For Particular Applications (AREA)
  • General Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
  • Quality & Reliability (AREA)
  • Theoretical Computer Science (AREA)
  • Signal Processing (AREA)

Abstract

Disclosed are methods and apparatus for qualifying a photolithographic reticle. A reticle inspection tool is used to acquire a plurality of images at different imaging configurations from each of a plurality of pattern areas of a test reticle. A reticle near field is recovered for each of the pattern areas of the test reticle based on the acquired images from each pattern area of the test reticle. The recovered reticle near field is then used to determine whether the test reticle or another reticle will likely result in unstable wafer pattern or a defective wafer.

Description

用於檢測光罩之設備及方法Equipment and method for detecting photomask

本發明大體上係關於光罩檢測之領域。更特定言之,本發明係關於圖案合格性鑑定。The present invention relates generally to the field of photomask inspection. More specifically, the present invention relates to pattern qualification.

一般而言,半導體製造產業涉及用於使用分層且圖案化至一基板上之半導體材料(諸如矽)製作積體電路之高度複雜技術。歸因於半導體裝置之大規模積體電路化及減小的大小,所製作之裝置已變得對缺陷愈來愈敏感。即,引起裝置中之故障之缺陷變得愈來愈小。裝置在運送至終端使用者或客戶之前係無故障的。 通常由複數個光罩製作一積體電路。首先,電路設計者將描述一特定積體電路(IC)設計之電路圖案資料提供至一光罩生產系統或光罩寫入器。電路圖案資料通常呈所製作IC裝置之實體層之一代表性佈局之形式。代表性佈局包含IC裝置之各實體層之一代表性層(例如,閘極氧化物、多晶矽、金屬化等),其中各代表性層由界定特定IC裝置之一層的圖案化之複數個多邊形組成。光罩寫入器使用電路圖案資料來寫入(例如,通常使用一電子束寫入器或雷射掃描器來曝露一光罩圖案)稍後將用以製作特定IC設計之複數個光罩。 一些光罩或光遮罩呈含有至少透明及不透明區、半透明及相移區或吸收體及反射區(其等一起界定諸如一積體電路之一電子裝置中之共面特徵之圖案)之一光學元件之形式。在光微影期間使用光罩來界定一半導體晶圓之指定區以進行蝕刻、離子植入或其他製作過程。 在製作各光罩或光罩群組之後,各新光罩通常有資格於晶圓製作中使用。例如,光罩圖案需要無可印刷缺陷。另外,用光罩製作之任何晶圓需要無缺陷。因此,繼續需要改良的光罩與晶圓檢測及合格性鑑定技術。In general, the semiconductor manufacturing industry involves highly sophisticated technologies for making integrated circuits using semiconductor materials (such as silicon) that are layered and patterned onto a substrate. Due to the large-scale integrated circuitization and reduced size of semiconductor devices, the devices made have become increasingly sensitive to defects. That is, defects that cause malfunctions in the device become smaller and smaller. The device is trouble-free before being shipped to the end user or customer. An integrated circuit is usually made from a plurality of photomasks. First, a circuit designer provides circuit pattern data describing a specific integrated circuit (IC) design to a mask production system or a mask writer. The circuit pattern data is usually in the form of a representative layout of the physical layers of the IC device being fabricated. The representative layout includes a representative layer (e.g., gate oxide, polycrystalline silicon, metallization, etc.) of each physical layer of the IC device, where each representative layer is composed of a plurality of patterned polygons defining a layer of a specific IC device . The mask writer uses circuit pattern data to write (eg, an electron beam writer or laser scanner is typically used to expose a mask pattern) which will later be used to make a number of masks for a specific IC design. Some reticlees or photomasks have a pattern containing at least transparent and opaque regions, translucent and phase-shifted regions, or absorbers and reflective regions (which together define a pattern of coplanar features in an electronic device such as an integrated circuit) The form of an optical element. A photomask is used during photolithography to define a designated area of a semiconductor wafer for etching, ion implantation, or other fabrication processes. After making each reticle or reticle group, each new reticle is usually qualified for use in wafer fabrication. For example, the mask pattern needs to be free of printable defects. In addition, any wafer made with a photomask needs to be defect free. Therefore, there is a continuing need for improved photomask and wafer inspection and qualification techniques.

下文呈現本發明之一簡化概述以提供對本發明之特定實施例之一基本理解。此概述並非本發明之一廣泛綜述,且其不識別本發明之必要/關鍵元件或描寫本發明之範疇。其唯一目的係以一簡化形式呈現本文中揭示之一些概念作為稍後呈現之更詳細描述之一序言。 在一項實施例中,揭示一種鑑定一光微影光罩合格性之方法。使用一成像工具依不同照明組態及/或不同成像組態自一測試光罩之複數個圖案區域之各者獲取複數個影像。針對該測試光罩之該等圖案區域之各者基於自該測試光罩之各圖案區域獲取之該等影像恢復一光罩近場。接著,使用該經恢復光罩近場來判定該測試光罩或另一光罩是否將可能導致不穩定晶圓圖案或一缺陷晶圓。 在一個實施方案中,直接分析該光罩近場以判定該測試光罩或另一光罩是否將可能導致一不穩定晶圓圖案或一缺陷晶圓。在另一態樣中,使用該經恢復光罩近場來偵測該測試光罩中或自該經恢復光罩近場模擬之模擬晶圓影像中之缺陷,其中缺陷偵測包含:比較不同時間之一相同晶粒、相鄰晶粒、一晶粒與其對應黃金晶粒(golden die)或一晶粒與來自與該測試光罩具有相同設計的一光罩複本之一對應晶粒之強度及/或相位。 在一個態樣中,在一場平面或一光瞳平面處獲取該等影像。在一特定實施例中,在不使用用以製作該光罩之一設計資料庫之情況下恢復該光罩近場。在另一態樣中,該等經獲取影像包含在經選擇以導致一相同光罩近場之不同成像條件下獲取之至少三個反射/透射影像。在此態樣中,該等不同成像條件包含不同焦點設定及不同光瞳形狀,且不同照明條件包含不同光源強度分佈及/或偏光設定。 在一替代實施方案中,該方法包含:(i)將一微影模型應用於該測試光罩之該光罩近場以模擬複數個測試晶圓影像;及(ii)分析該等模擬測試晶圓影像以判定該測試光罩是否將可能導致一不穩定或缺陷晶圓。在此態樣中,該微影模型經組態以模擬一光微影製程。在另一態樣中,該微影模型模擬一照明源,該照明源具有與用於獲取該測試光罩或者另一光罩或晶圓之影像的一檢測工具之一照明形狀不同之一形狀。在另一態樣中,運用自用於一校準光罩之一設計資料庫生成之影像校準該微影模型。在另一實例中,運用自一校準光罩獲取之影像校準該微影模型。在又一態樣中,在複數個不同微影製程條件下將該微影模型應用於針對該測試光罩恢復之該光罩近場,且分析該等模擬測試晶圓影像包含:藉由比較與不同製程條件及一相同光罩區域相關聯之該等模擬測試影像之部分而判定該測試光罩在該等不同微影製程條件下是否將可能導致一不穩定晶圓。 在一替代實施例中,本發明係關於一種用於鑑定一光微影光罩合格性之檢測系統。該系統包含:一光源,其用於產生一入射光束;及一照明光學模組,其用於將該入射光束引導至一光罩上。該系統亦包含:一收集光學模組,其用於將來自該光罩之各圖案區域之一輸出光束引導至至少一個感測器,該至少一個感測器用於偵測該輸出光束且基於該輸出光束產生一影像或信號。該系統進一步包括一控制器,該控制器經組態以執行類似於一或多個上述方法操作之操作。 下文參考圖進一步描述本發明之此等及其他態樣。A simplified overview of the invention is presented below to provide a basic understanding of one particular embodiment of the invention. This summary is not an extensive overview of the invention, and it does not identify essential / critical elements of the invention or describe the scope of the invention. Its sole purpose is to present some concepts disclosed herein in a simplified form as a prelude to the more detailed description that is presented later. In one embodiment, a method for qualifying a lithographic reticle is disclosed. An imaging tool is used to obtain a plurality of images from each of the plurality of pattern areas of a test mask according to different lighting configurations and / or different imaging configurations. Each of the pattern areas for the test mask restores a mask near field based on the images obtained from the pattern areas of the test mask. Next, the restored photomask near field is used to determine whether the test photomask or another photomask may cause an unstable wafer pattern or a defective wafer. In one embodiment, the photomask near field is directly analyzed to determine whether the test photomask or another photomask will likely result in an unstable wafer pattern or a defective wafer. In another aspect, the restored mask near field is used to detect defects in the test mask or simulated wafer images simulated from the restored mask near field, wherein the defect detection includes: comparing different The strength of one of the same grains, adjacent grains, one grain and its corresponding golden die, or one grain and one corresponding grain from a mask replica with the same design as the test mask And / or phase. In one aspect, the images are acquired at a field plane or a pupil plane. In a specific embodiment, the near field of the mask is restored without using a design database used to make the mask. In another aspect, the acquired images include at least three reflection / transmission images acquired under different imaging conditions selected to result in a near field of the same mask. In this aspect, the different imaging conditions include different focus settings and different pupil shapes, and different lighting conditions include different light source intensity distributions and / or polarized light settings. In an alternative embodiment, the method includes: (i) applying a lithographic model to the near field of the mask of the test mask to simulate a plurality of test wafer images; and (ii) analyzing the simulated test crystals Circle the image to determine if the test mask will cause an unstable or defective wafer. In this aspect, the lithographic model is configured to simulate a photolithographic process. In another aspect, the lithography model simulates an illumination source having a shape different from an illumination shape of a detection tool used to acquire an image of the test mask or another mask or wafer . In another aspect, the lithographic model is calibrated using an image generated from a design database for a calibration mask. In another example, the lithographic model is calibrated using images acquired from a calibration mask. In yet another aspect, the lithographic model is applied to the near-field of the reticle restored for the test reticle under a plurality of different lithographic process conditions, and analyzing the simulated test wafer images includes: by comparison The portions of the simulated test images associated with different process conditions and an identical mask area determine whether the test mask will likely result in an unstable wafer under the different lithographic process conditions. In an alternative embodiment, the invention relates to a detection system for identifying the qualification of a light lithographic mask. The system includes: a light source for generating an incident light beam; and an illumination optical module for guiding the incident light beam to a photomask. The system also includes: a collection optical module for directing an output beam from each of the pattern areas of the mask to at least one sensor, the at least one sensor is used to detect the output beam and is based on the The output beam produces an image or signal. The system further includes a controller configured to perform operations similar to one or more of the above method operations. These and other aspects of the invention are described further below with reference to the drawings.

相關申請案之交叉參考 本申請案主張由Rui-fang Shi等人在2017年7月3日申請之美國專利申請案第15/641,150號之優先權利且係其之一部分接續申請案,該美國專利申請案第15/641,150號根據35 U.S.C. § 120規定主張由Abdurrahman Sezginer等人在2016年8月5日申請之PCT申請案第PCT/US2016/045749號之優先權利,該PCT申請案第PCT/US2016/045749號主張由Abdurrahman Sezginer等人在2015年8月10日申請之先前申請案美國申請案第14/822,571號(現為於2017年1月17日發佈之美國申請案第9,547,892號)之優先權利。本申請案亦主張2017年5月18日申請之美國臨時申請案第62/508,369號之優先權利。此等申請案及專利之全文為全部目的以引用的方式併入本文中。 在以下描述中,闡述諸多特定細節以提供對本發明之一透徹理解。可在無一些或全部此等特定細節之情況下實踐本發明。在其他例項中,未詳細描述熟知過程操作或設備組件以免不必要地使本發明模糊。雖然將結合特定實施例描述本發明,但將瞭解,並不意欲將本發明限於該等實施例。 在將遮罩運送至一製作設施之前、在使用此遮罩製作晶圓之前偵測各遮罩之缺陷且以其他方式特性化遮罩之各種態樣(例如,圖案穩定性、CD、CD均勻性)對於製作及/或在此遮罩已在製作過程中使用達某時段之後週期性地再鑑定此遮罩合格性將為有利的。 本發明之一項實施例包含用於基於在複數個不同成像參數下自一檢測工具獲得之光罩影像恢復一光罩之近場影像之技術。接著,可在許多光罩合格性鑑定應用中使用此光罩近場影像。在一項實例中,可將光罩近場影像輸入至一微影模型以預測與所得圖案將如何印刷於晶圓上相關之一晶圓影像或各種晶圓圖案特性。接著,經預測晶圓影像及/或各種晶圓特性可經分析用於缺陷偵測、光罩合格性鑑定或再鑑定,及/或任何其他適合度量或檢測應用。光罩近場影像本身亦可經分析用於如本文中進一步描述之各種目的。 術語「光罩」、「遮罩」及「光遮罩」在本文中可互換地使用且各自大體上可包含其上形成有一不透明材料層之一透明基板,諸如玻璃、硼矽酸鹽玻璃、石英或熔融矽石。不透明(或實質上不透明)材料可包含完全或部分阻擋光微影光(例如,深UV或極UV)之任何適合材料。例示性材料包含鉻、矽化鉬(MoSi)、矽化鉭、矽化鎢、玻璃上不透明MoSi (OMOG)等。亦可在不透明層與透明基板之間添加一多晶矽膜以改良黏著。可在不透明材料上方形成一低反射膜,諸如氧化鉬(MoO2 )、氧化鎢(WO2 )、氮化鈦(TiO2 )或氧化鉻(CrO2 )。在一特定實例中,一EUV光罩可包含具有具不同折射率與低吸收特性(諸如鉬(Mo)及矽(Si))的交替層之多個層及一吸收體材料(諸如由一薄抗反射氧化物加蓋之氮化鉭硼膜)。 術語光罩指代不同類型之光罩,包含但不限於一清晰場(clear-field)光罩、一暗場光罩、一二元光罩、一相移遮罩(PSM)、一交替PSM、一衰減或半色調PSM、一三元衰減PSM、一無鉻相位微影PSM及無鉻相位微影(CPL)。一清晰場光罩具有透明之場或背景區域,且一暗場光罩具有不透明之場或背景區域。一二元光罩係具有透明或不透明之圖案化區域之一光罩。例如,可使用由具有由鉻金屬吸附膜界定之一圖案的一透明熔融矽石坯料製成之一光遮罩。二元光罩不同於相移遮罩(PSM),相移遮罩(PSM)之一個類型可包含僅部分透射光之膜,且此等光罩通常可稱為半色調或嵌入式相移遮罩(EPSM),諸如ArF及KrF遮罩。若將一相移材料放置於一光罩之交替凈空間上,則光罩被稱為一交替PSM、一ALT PSM或一Levenson PSM。應用於任意佈局圖案之一種類型的相移材料稱為一衰減或半色調PSM,其可藉由用一部分透射或「半色調」膜取代不透明材料而製作。一三元衰減PSM係亦包含完全不透明特徵之一衰減PSM。 下一代微影已引進使用極紫外線輻射(EUV,波長13.5 nm),其在常態大氣以及玻璃中被吸收。為此,微影EUV製程在真空下發生,且光學反射透鏡/鏡用於聚焦至將具有反射及吸收體圖案而非半透明及不透明圖案之EUV光遮罩。 圖1係根據本發明之一項實施例之繪示一遮罩近場恢復程序100之一流程圖。可在一光罩之生命週期中的任何適合時間針對一特定光罩或一組光罩執行以下遮罩恢復過程100,如下文在經恢復遮罩近場之各種使用案例中進一步描述。藉由實例,可在用此(等)遮罩製作任何晶圓之前、在開始大量晶圓製作或在再鑑定此(等)光罩合格性期間恢復一遮罩近場。 首先,在操作102中,使用一遮罩檢測工具依不同成像組態獲取遮罩之至少三個影像。替代地,可使用兩個影像,但已發現使用三個影像運作良好。運用不同成像組態之獲取可為同時的或循序的。經獲取影像不必在場平面處。藉由實例,可在可直接存取繞射強度之光瞳平面處獲取兩個或更多個影像。 可利用照明及/或收集組態之各種適合組合來獲取兩個或更多個影像。大體上選擇不同成像組態以提供可自其計算遮罩近場之影像。可選擇任何適合成像或光學組態,使得遮罩近場在不同操作條件下保持相同。實例包含不同焦點設定、不同照明形狀(例如,不同方向或圖案)、用於整個照明光瞳或照明光瞳之不同部分之不同偏光、遮蔽收集光束之不同部分之不同變跡(apodization)設定等。在一項實施例中,可使用不同焦點設定(遍及聚焦及散焦(諸如0聚焦、±800或±1600散焦等))來獲取不同影像。在另一實例中,照明光瞳之不同象限可具有不同偏光設定。在另一實例中,成像組態可包含高解析度影像,諸如具有不同光瞳形狀及/或不同焦點狀況之透射影像(例如,針對ArF遮罩)。在另一實施例中,可(例如,針對EUV遮罩)獲得具有不同光瞳形狀及/或不同焦點狀況之三個或更多個反射影像。 可使用一相對較低NA (例如,小於0.5)以一「實質上低解析度」成像光罩。相比之下,一「實質上高解析度影像」大體上指代其中印刷於光罩上之特徵實質上顯現為其等形成於光罩上(在用以產生影像之光罩檢測系統之光學限制內)之一光罩之一影像。一光罩之一「實質上高解析度影像」係藉由用一實質上高解析度光罩檢測系統(例如,大於0.8之一數值孔徑(NA))在光罩平面處成像實體光罩而產生之一影像。用以產生一光罩影像之「實質上低NA」可實質上與光罩側上由一曝光/微影系統使用以將光罩之一影像投影至一晶圓上藉此將光罩之特徵轉印至該晶圓上之NA相同。在實質上低NA影像(或LNI)中,光罩特徵可具有與實際光罩特徵實質上不同之一外觀。例如,光罩特徵在一特徵之一LNI中可看似比形成於光罩上之實際特徵具有更多經修圓隅角。 一般而言,任何適合成像工具可用於遮罩近場恢復過程。在本文中描述之特定實施例中,一初始恢復過程之結果稍後可基於來自一特定檢測工具之額外光罩影像用於關於該相同光罩或其他光罩之圖案穩定性或缺陷偵測評估。為了此等使用案例之一致性,可用將用於相同或其他光罩之後續檢測的光罩檢測系統之偵測器或一類似組態之光罩檢測系統(例如,具有與將用於檢測之光罩檢測系統相同之做法及模型之一不同光罩檢測系統)之一類似組態之偵測器來獲取用於遮罩近場恢復之光罩之影像。換言之,可在如將在後續遮罩檢測或合格性鑑定過程期間使用之相同光學條件下獲取可用於遮罩恢復之影像。以此方式,可儘可能直接地量測光罩與檢測系統之照明電磁波之相互作用。 在替代實施例中,用於遮罩近場恢復之工具可不同於一光罩檢測系統。例如,成像工具可利用與其中光罩將用於晶圓製造之微影系統相同之波長(例如,波長(DUV係193.3 nm或EUV係13.5 nm))。事實上,任何適合電磁波長可用於遮罩近場恢復。 再參考所繪示實例,接著,在操作104中,可將三個或更多個影像彼此對準或可將各影像與後OPC資料庫對準。例如,可經由空間域或頻域方法對準經獲取影像。對準調整可取決於所使用之成像系統之特定幾何形狀。若使用不同收集路徑獲得不同影像,則可作出影像之某一調整以補償光學路徑之差異。 在成像工具中,藉由自許多方向入射之電磁(EM)波照明具有各種圖案之一光罩。此入射光依彼此不同干擾之不同電磁場相位自遮罩圖案之不同點繞射。光罩之近場係距光罩數波長之一接近距離處之電磁場。 收集光學器件大體上將來自光罩之光之一繞射限制部分引導朝向一偵測器(或晶圓)以形成一影像。偵測器偵測為歸因於遮罩近場之干擾之結果之強度,但不偵測相位。 儘管在經偵測信號中獲得遠場強度,然可期望恢復包含振幅及相位之遮罩近場。在所繪示之實施例中,基於此等經獲取遮罩影像恢復且儲存遮罩近場,如在操作106中繪示。大體上使用多個影像(或信號)來恢復包含相位及振幅分量兩者之遮罩近場。可基於自光罩獲取之影像藉由一迴歸技術判定近場資料。例如,可使用一擬牛頓(quasi-Newton)或共軛梯度技術自記錄於一偵測器平面處之光罩之經獲取光學影像或影像之強度恢復(迴歸)該光罩之一選定部分之近場。另外,可使用任何其他適合迴歸方法及/或演算法自一或多個實際影像判定近場資料。 通常可藉由解決一最佳化問題而達成遮罩近場恢復,其尋求最小化觀察到的強度影像與假定遮罩光學場之所得影像之間的差異。特定言之,自一光罩之強度影像恢復該光罩之近場係一逆算問題或一迴歸問題。可藉由最小化一成本函數(例如,能量或處罰函數)而迭代地恢復近場。最小化之數量可為經獲取影像與在偵測器處自遮罩近場計算之強度影像之間的差異之平方之總和。換言之,可針對各種光學系統性質組自最終遮罩近場計算強度影像,且當發現遮罩近場時,此等經計算影像將最緊密匹配經獲取影像。在藉由Abdurrahman Sezginer等人於2016年10月25日發佈之美國專利第9,478,019號中進一步描述各種遮罩近場恢復方法論及系統實施例,該專利之全文為全部目的以引用的方式併入本文中。 在其中於各種光學條件下獲取多個影像之情況中,攜載相位及振幅資訊之經恢復近場遮罩m 可藉由以下方程式判定:方程式1 在上述方程式1中,係針對成像條件α之經量測影像,係描述檢測成像系統之一組特徵向量,係成像系統之一組對應特徵值,且係0與1之間的一非負加權因數。可例如透過諸如擬牛頓或共軛梯度之方法迭代地求解上述方程式。 另一實例係Gerchberg-Saxton演算法,其中可利用場平面影像及光瞳平面繞射級之一組合來求解物件之振幅及相位兩者。 在一項實施例中,可基於經獲取影像經由一霍普金斯(Hopkins)近似法判定遮罩近場。在另一實施例中,迴歸不包含薄遮罩近似法。例如,光罩之近場係計算為當由一法向入射平面波照明時出現在光罩之表面附近之電磁場。在微影及檢測中,藉由自許多方向入射之平面波照明一光罩。當入射方向改變時,根據霍普金斯近似法,繞射級之方向改變但其等振幅及相位近似保持不變。本文中描述之實施例可使用霍普金斯相位近似法但不進行所謂的薄遮罩或克希荷夫(Kirchhoff)近似法。 恢復公式亦可隨不同範數或一正則項R 之相加而改變,此不利於近場中之振盪,如下:其中正則項R可併有關於近場之先前資訊或基於遮罩基板/材料之實體理解之預期。另外,用於影像差異之範數可為一l-範數(l-norm)且可基於最佳化函數之特定需求而調整。 有趣的是應注意,歸因於一較高NA之光之入射角之較廣範圍及相關聯干擾電場分量,由一較高NA所致之遮罩電磁場向量之干擾將較大(大於一較低NA檢測系統)。 實際遮罩可歸因於遮罩寫入過程而隨預期設計圖案改變。自遮罩之影像獲得近場遮罩意謂自實際實體遮罩而非設計資料庫獲得此近場遮罩。即,可在不使用設計資料庫之情況下恢復遮罩近場。 接著,可在各種應用中使用遮罩近場結果。在一項實施例中,可使用遮罩近場結果來使用一或多個模型預測晶圓圖案。即,可使用經恢復遮罩近場來模擬微影影像。可利用任何適合技術來基於遮罩近場影像模擬微影影像。一項實施例包含透過部分同調模型運算微影影像:方程式2 其中λi 表示微影TCC (交叉轉印(transfer cross)係數)之特徵值;表示TCC之特徵向量(核心);s 係晶圓堆疊,其包含膜折射率;f 係焦點;且z 係微影平面在抗蝕劑材料中之垂直位置。方程式2之交叉轉印係數(TCC)可包含場通過微影投影儀(包含晶圓上之膜堆疊)之向量傳播。 在使用一模型來預測晶圓結果之前,可校準模型以產生儘可能準確的結果。可使用任何適合技術來校準模型。本發明之特定實施例提供用於基於自一校準遮罩恢復之遮罩近場結果校準一微影模型之技術。在替代實施例中,使用設計資料庫來校準模型。例如,可自設計資料庫生成校準光罩影像。 一校準光罩通常將經設計以具有實質上類似於待檢測以用於缺陷偵測或待量測以用於度量目的之光罩之(若干)特性。例如,校準光罩及測試光罩較佳由具有實質上相同厚度及組成之實質上相同材料形成。另外,可已使用相同製程形成兩個光罩。該兩個光罩可不一定具有印刷於其上之相同圖案,只要光罩上之圖案可分解成實質上相同之片段(例如,具有類似寬度之線等)。另外,將檢測之光罩及用以獲取影像之光罩可為同一光罩。 圖2係根據本發明之一特定實施方案之繪示一模型校準過程200之一流程圖。如所展示,在操作208中,可使用一組初始模型參數來模型化如應用於自一校準光罩恢復之遮罩近場影像(201)的光微影製程及光阻劑。替代地,校準過程200可使用自設計資料庫模擬之模擬校準光罩影像(202)。可藉由模擬設計資料庫上之光罩製作及成像過程而自資料庫生成光罩影像。可使用任何適合模型來針對設計資料庫之特徵產生光學影像。藉由實例,此模擬可包含使用本文中描述之同調系統加總(SOCS)或阿貝(Abbe)方法論。存在可自一已知設計資料庫模擬一光學系統之強度影像之若干軟體套件。一項實例係在德國埃蘭根的Fraunhofer IISB開發之Dr.LiTHO。在自設計資料庫模擬一影像202之情況中,可首先模擬近場,此可藉由上文引用之軟體套件以及若干其他套件(包含KLA-Tencor之Prolith、Panoramic Technologies之HyperLith,等等)而完成。 用於基於光罩近場影像產生晶圓影像之模型可僅包含光微影掃描器之效應,且其亦可包含抗蝕劑、蝕刻、CMP或任何其他晶圓製程之效應。一個例示性製程模擬模型工具係可購自加利福尼亞州苗必達市之KLA-Tencor公司之Prolith。可嚴密地或近似地模型化抗蝕劑及蝕刻製程。在一特定實施例中,模型可呈一緊湊抗蝕劑模型之形式,其包含一特定抗蝕劑材料內部之3D酸擴散及其中強加邊界條件之組態,以及經應用以形成潛像之一單一臨限值。 應注意,模型化微影工具可具有與用於獲取光罩之實際影像的光罩檢測工具不同之一照明形狀或光源。在特定實施例中,模型化微影工具可具有與一光罩檢測器工具相同或類似之一光源。 可使用其他模擬方法,諸如SOCS或阿貝。通常稱為同調系統加總(SOCS)之演算法嘗試將成像系統轉換為其等輸出經求平方、經按比例調整且經加總之一組(a bank of)線性系統。已在別處描述SOCS方法,包含Nicolas Cobb之博士論文「Fast Optical and Process Proximity Correction Algorithms for Integrated Circuit Manufacturing」 (加州大學柏克萊分校,1998年春)。阿貝演算法包含針對各點源一次一個地計算物件之影像,且接著將強度影像加總在一起且考慮到各源點之相對強度。 模型及其模型化參數之輸入包含應用於一經恢復近場遮罩之一組製程條件。即,模型經組態以模擬經重建近場遮罩(或模擬遮罩影像)上之不同組之製程條件。各組製程條件大體上對應於特性化或部分特性化用於自遮罩形成一晶圓圖案之晶圓製程之一組晶圓製程參數。例如,可將一特定焦點及曝光設定輸入至模型。其他可調整模型參數亦可包含以下參數之一或多者:一投影透鏡波前參數、一變跡參數、一色差焦點誤差參數、一振動參數、一抗蝕劑輪廓指數、一抗蝕劑浮渣度量、頂部損失度量等。與不同組製程條件一起使用此模型可導致由經重建近場遮罩在不同處理條件下形成之一組模擬晶圓或抗蝕劑圖案影像,且此等模擬晶圓影像可用於圖案穩定性及缺陷偵測評估,如本文中進一步描述。 在操作216中,亦可使用一校準光罩來製作自其獲得實際影像之一校準晶圓。在一項實例中,使用一臨界尺寸(CD)掃描電子顯微鏡(SEM)獲取實際影像。可利用其他成像工具,但較佳為一高解析度工具。 一般而言,校準晶圓將含有任何數目個已知結構,其可廣泛地變化。結構可呈通常為週期性之光柵之形式。各光柵可在一個方向(X或Y)上為週期性的(舉例而言,如一線空間光柵),或其可在兩個方向(X及Y)上為週期性的(舉例而言,如一柵格空間光柵)。一柵格空間光柵之實例可包含Y方向上之一線陣列,其中各線在X方向上分段。另一柵格空間實例係一點結構陣列。即,各結構可採取一線空間光柵、柵格空間光柵、棋盤圖案結構等之形式。結構設計特性可各自包含線寬度(在一特定高度處之寬度)、線空間寬度、線長度、形狀、側壁角度、高度、節距、光柵定向、頂部輪廓(頂部修圓或T型頂之程度)、底部輪廓(基腳)等。校準晶圓可含有具此等特徵特性之不同組合之結構。如應明白,不同結構特性(諸如不同寬度、間距、形狀、節距等)展現對焦點之不同回應,且因此校準遮罩較佳包含具有不同特性之不同結構。 在一特定實施例中,校準晶圓可採取具有經受不同處理條件之不同量測點之一「實驗設計(DOE)」晶圓之形式。在更一般實施例中,製程參數變動組織於一半導體晶圓(稱為一DOE晶圓)之表面上之一圖案中。以此方式,量測點對應於具有不同相關聯製程參數值之晶圓表面上之不同位置。在一項實例中,DOE圖案係一焦點/曝光矩陣(FEM)圖案。通常,展現一FEM圖案之一DOE晶圓包含量測點之一柵格圖案。在一個柵格方向(例如,x方向)上,曝光劑量變化而焦點深度保持恆定。在正交柵格方向(例如,y方向)上,焦點深度變化而曝光劑量保持恆定。以此方式,自FEM晶圓收集之量測資料包含與焦點及劑量製程參數之已知變動相關聯之資料。 FEM量測點大體上跨焦點曝光矩陣晶圓定位。事實上,每場大體上可存在一或多個量測點。可使用焦點及曝光組合之一不同組合(或可僅為焦點或曝光)形成各場。例如,可使用一第一組合產生一第一場,且可使用不同於第一組合之一第二組合產生一第二場。可使用變化的焦點及變化的曝光、變化的焦點-恆定曝光、恆定焦點-變化的曝光及類似者產生多個組合。 量測點之數目亦可不同。每場之點數目在生產晶圓上通常較少,此係因為生產晶圓上之面積(real estate)極其珍貴。再者,在一生產晶圓上進行之量測歸因於生產中之時間約束而比在一焦點曝光矩陣晶圓上進行之量測更少。在一項實施例中,每場量測一單一點。在另一實施例中,每場量測多個點。 在大多數FEM情況中,使用不同處理參數由同樣設計之圖案形成量測點結構。然而,應注意,不同焦點曝光矩陣可具有不同結構。例如,可使用一第一光柵類型執行一第一矩陣,且可使用不同於第一光柵類型之一第二光柵類型執行一第二矩陣。 在一替代實施例中,自用於一校準光罩之設計資料庫生成之模擬校準影像(202)可用作至模型之輸入。即,可在未自一實體校準光罩恢復近場之情況下校準模型。代替性地,藉由自設計資料庫模擬(非恢復)近場且將微影成像模型應用於模擬近場以達成與來自晶圓之實際結果(216)相當的微影結果而模擬微影影像。 一般而言,可設想與任何組之製程參數、結構參數或兩者之已知變動相關聯的光學信號資料。無論形式為何,校準晶圓結構可印刷於多種不同晶圓層中。特定言之,大體上使用標準微影製程(例如,將一電路影像投影穿過一光罩且至塗佈有光阻劑之一矽晶圓上)來將經印刷結構印刷於一光阻劑層中。晶圓可為具有對應於在測試過程中之該步驟時通常存在於產品晶圓上的材料之材料層之一校準晶圓。經印刷結構可印刷於下層中之其他結構上方。校準晶圓可為具有產生工作裝置之潛力之一產品晶圓。校準晶圓可為僅用於校準模型之一簡單晶圓。校準晶圓可為用以校準OPC設計模型之相同晶圓。一個以上校準晶圓可用以校準微影模型。當使用多個校準晶圓時,可使用相同或不同校準光罩。不同校準光罩可具有具不同尺寸之圖案以產生一較廣範圍之影像資料。 用以形成校準結構之製程參數大體上經組態以使圖案之特性保持在所要規格內。例如,校準結構可印刷於一校準晶圓上作為一校準程序之一部分,或其等可在生產期間印刷於一生產晶圓上。在生產時,校準結構通常印刷於安置在一生產晶圓上之裝置區域(例如,界定IC之晶粒)之間的切割道中。量測點可為安置於裝置結構周圍之專用校準結構,或其等可為裝置結構之一部分(例如,一週期性部分)。如應明白,使用裝置結構之一部分可更困難,但其因為係裝置結構之一部分而趨於更準確。在另一實施例中,校準結構可跨一整個校準晶圓印刷。 再參考圖2,在操作210中,可比較對應模型化結果與校準結果(例如,影像)。接著,在操作212中,可判定是否將調整模型參數。若將調整模型參數,則在操作214中調整該等模型參數且程序200重複操作208以使用經調整參數模型化微影製程(及抗蝕劑)。可調整模型參數直至模型影像與校準影像之間的差異之一量化已達到亦低於一預定義臨限值之一最小值。經最小化之數量可為經獲取校準影像與模擬影像之間的差異之平方之總和。此過程200之輸出係一微影/抗蝕劑模型及其最終模型參數。此組模型參數藉由使用遮罩近場之本質而克服與遮罩製程模型化及遮罩3D繞射計算相關聯之技術障礙。 基於經恢復遮罩近場結果之模擬晶圓圖案可用於許多遮罩檢測、度量及/或合格性鑑定目的。在一項實施例中,藉由評估經恢復遮罩近場在一系列模擬晶圓製作條件下是否將可能導致晶圓圖案缺陷而執行一光罩合格性鑑定。對於缺陷偵測,一光罩缺陷在晶圓上之可印刷性係重要的,且光罩缺陷之可印刷性直接取決於光罩近場及微影系統。 在獲得用於一特定過程之一最終經校準微影/抗蝕劑/蝕刻模型之後(不管如何獲得此模型),此模型可用以在運用一遮罩進行晶圓製作之前自此遮罩產生準確晶圓平面抗蝕劑影像(例如,在顯影或蝕刻之後)或用於再鑑定此遮罩合格性。此等抗蝕劑影像將容許吾人以高保真度且透過不同焦點及曝光設定或其他微影參數來評估任何檢測圖案之晶圓影像。由於此評估過程可在晶圓製作之前發生,故可顯著地縮短合格性鑑定及缺陷偵測循環。模擬晶圓影像亦可使能夠藉由比較微影之後、抗蝕劑模型應用之後及蝕刻之後的模擬晶圓影像而分離不同圖案化問題根源。 圖3繪示根據本發明之一項實施例之表示一光罩合格性鑑定過程300之一流程圖。在操作302中,例如針對一特定光罩基於自此特定光罩獲取之影像恢復一遮罩近場影像。此操作可包含圖1之遮罩近場恢復操作。在獲得一遮罩近場之後,在操作303中,亦可使用關於經恢復遮罩近場之最終模型參數來模型化微影製程(及抗蝕劑)。例如,使用最終模型來使用一遮罩近場影像模擬晶圓影像。 接著,在操作322中,可評估模擬晶圓圖案以判定圖案穩定性及/或定位缺陷。大體上可判定對應光罩是否將可能導致不穩定或缺陷晶圓圖案。在一項實施例中,使用複數個不同製程條件(諸如焦點及劑量)將模型應用於遮罩近場影像或結果以在變化的製程條件下評估光罩設計穩定性。 圖4A係根據本發明之一例示性應用之繪示用於判定晶圓圖案穩定性之一過程400之一流程圖。首先,在操作402中,可將各測試影像與其對應參考影像對準,該等影像亦係由模型在不同組之製程條件下產生。藉由模型在不同處理條件/參數下計算不同測試影像及參考影像。 在操作404中,可將各對經對準影像彼此比較以獲得一或多個晶圓圖案差異。接著,在操作406中,可使臨限值與各晶圓圖案差異相關聯。晶圓圖案差異及其等相關聯臨限值可一起用以特性化圖案穩定性。即,在不同模擬製程條件下一特定圖案之偏差量(圖案差異)及此偏差是否跨一相關聯臨限值一起特性化圖案穩定性。一製作過程之製程窗指定一預期或定義製程偏差量,在該製程偏差量下評估所得圖案以確保其等將保持穩定或在某些指定偏差容限(例如,臨限值)內。 可將用於評估圖案穩定性之不同臨限值指派至光罩之不同區域及藉此對應晶圓圖案。基於各種因素(諸如圖案設計背景、圖案MEEF (或如下文進一步描述之遮罩誤差增強因數)等級或裝置效能對晶圓圖案變動之敏感度等),臨限值可全部相同或不同。例如,與光罩之一半密集區相比,吾人可針對一密集區中之圖案選取一更緊密臨限值。 可視情況在參考遮罩圖案及測試遮罩圖案兩者中識別一組初始熱點或圖案弱點區域。例如,一設計者可提供對裝置功能至關重要之設計熱點座標之一清單。例如,定義為熱點之區域可被指派一個偵測臨限值,而非熱點區域可被指派一更高臨限值(用於缺陷偵測)。此差別可用以最佳化檢測資源。 可使用此圖案穩定性評估來促進光罩合格性鑑定,藉此克服此領域中之諸多挑戰。隨著積體電路(IC)之密度及複雜性不斷增加,檢測光微影遮罩圖案變得愈來愈具挑戰性。每新一代IC具有目前達到且超過微影系統之光學限制之更密集且更複雜之圖案。為克服此等光學限制,已引入各種解析度增強技術(RET),諸如光學近接校正(OPC)。例如,OPC藉由修改光遮罩圖案使得所得印刷圖案對應於原始所要圖案而幫助克服一些繞射限制。此等修改可包含對主要IC特徵(即,可印刷特徵)之大小及邊緣之擾動。其他修改涉及將襯線添加至圖案隅角及/或提供附近次解析度輔助特徵(SRAF),不期望此導致經印刷特徵且因此被稱為非可印刷特徵。期望此等非可印刷特徵取消否則將在印刷過程期間發生之圖案擾動。然而,OPC使遮罩圖案甚至更為複雜且通常與所得晶圓影像極其不同。此外,OPC缺陷通常未轉化為可印刷缺陷。光遮罩圖案之增加的複雜性及不期望全部圖案元件直接影響經印刷圖案之事實使檢測光遮罩之有意義圖案缺陷之任務遠更困難。由於半導體產業向甚至更小特徵發展,故尖端製造商開始使用甚至更為奇特的OPC,諸如逆微影技術(ILT),此導致遮罩上之高度複雜圖案。因此,高度期望在實體製作晶圓之前知道遮罩寫入保真度及其晶圓印刷品質。 一缺陷之重要性之一個量度係其MEEF或遮罩誤差增強因數。此因數使遮罩平面中之缺陷之大小與其將影響經印刷影像之量級相關。高MEEF缺陷對經印刷圖案具有高影響;低MEEF缺陷對經印刷圖案具有較小或不具影響。一圖案之一密集細線部分中之一尺寸過小主要圖案特徵係具有高MEEF之一缺陷之一實例,其中一小遮罩平面大小誤差可引起經印刷圖案之一完全坍塌。一隔離小針孔係具有低MEEF之一缺陷之一實例,其中缺陷本身過小而無法印刷且距最近主要圖案邊緣足夠遠以不影響如何印刷該邊緣。如此等實例展示,一缺陷之MEEF係缺陷類型及其中定位缺陷之圖案背景之一稍複雜函數。 除引起更顯著晶圓缺陷之更高MEEF遮罩缺陷之外,特定設計圖案及對應遮罩圖案亦可比其他設計及遮罩圖案對製程變化更穩健。當製作過程開始偏離最佳製程條件時,特定遮罩圖案可導致更顯著晶圓圖案擾動及缺陷。 圖4B係根據本發明之另一實施例之繪示一缺陷檢測程序450之一流程圖。在操作452中,可將各模型化測試晶圓影像與其對應參考影像對準。在一項實施例中,可完成一晶粒對晶粒或單元對單元對準。在另一實施例中,將模型化測試晶圓影像與自對應後OPC設計生成之一參考影像對準。例如,後OPC設計經處理以模擬此設計之光罩製作過程。例如,隅角經修圓。一般而言,一參考影像可源自與一較早時間之測試影像相同之晶粒、源自一相鄰的相同晶粒,或自設計資料庫生成。在一特定實例中,自被證實為無缺陷(例如,緊接在製造光罩且鑑定光罩合格性之後)之一「黃金」晶粒獲得參考影像。可儲存在已知光罩無缺陷時自該光罩獲得之黃金光罩影像,且稍後在需要時依需求使用其來運算黃金光罩近場影像及晶圓影像。或者,可儲存黃金光罩近場影像以備存取而在未來檢測時無需再運算近場。 在操作454中,基於一相關聯臨限值比較各對經對準測試影像與參考影像以定位光罩缺陷。可使用任何適合機制來使臨限值與特定光罩區域相關聯,如上文進一步描述。可比較測試影像與參考影像之任何適合度量。例如,可比較測試及參考晶圓影像之輪廓作為邊緣放置誤差(EPE)之一度量。 接著,在操作456中,可針對各光罩缺陷比較對應經模擬晶圓缺陷區域與其對應參考預OPC區域。即,評估模擬晶圓圖案以判定光罩缺陷是否導致隨預期設計變化之一晶圓缺陷。 再參考圖3,在操作324中,接著可基於模擬光罩影像判定設計是否有缺陷。在一項實施例中,判定在製程條件之一指定範圍(或製程窗)下設計圖案是否導致不可接受的晶圓圖案變動。判定是否存在歸因於製程變異性之一顯著差異。若不同處理之晶圓圖案之間的差異高於一對應臨限值,則此等晶圓圖案可被認為有缺陷。此等系統缺陷稱為熱點。亦可判定來自光罩之一模擬晶圓圖案與其對應預OPC圖案之間的任何差異是否高於一預定義臨限值。若判定設計有缺陷,則在操作332中可修改設計。 一旦一光罩之設計經驗證,則光罩可能仍含有應監測之熱點。以下操作被描述為在一遮罩上實施,該遮罩存在至少一些經識別熱點。當然,若遮罩不含有任何經識別熱點,則可跳過圖3之以下操作,且使用遮罩而在製作及檢測期間不執行熱點監測。 在所繪示實例中,若不認為設計有缺陷,則在操作326中可判定是否可監測任何熱點。若判定可監測熱點,則在操作334中可在晶圓製程期間監測熱點。例如,可在晶圓製作期間監測熱點圖案以判定製程是否已偏離出規格且已引起對應晶圓圖案具有改變為不可接受的值之關鍵參數。一項實施方案可涉及設定一相對較高MEEF等級以檢測對應熱點之光罩及/或晶圓圖案。隨著條件進一步遠離標稱製程條件,CD或EPE可變大且危及晶圓製程之完整性。 僅當一測試遮罩圖案改變達一預定義量時可識別熱點圖案,而不管如何比較此改變與原始預期設計(例如,預OPC資料)。換言之,在不同製程條件下實體遮罩圖案中之一顯著改變可指示預期設計圖案之一問題。對應模型化影像部分之間的差異表示製程條件對經設計圖案與經製造遮罩之效應之差異。與一特定設計圖案相關聯之差異通常稱為「設計熱點」或僅為「熱點」,且表示設計中關於已檢查之特定製程條件(可能亦關於經製造遮罩)之弱點。可在不同製程條件之模型化影像之間發現之差異種類之實例係CD (臨界尺寸)或EPE (邊緣放置誤差)。 在另一實施例中,若將模型應用於後OPC設計資料庫,則所得晶圓圖案可對應於設計者意欲印刷於晶圓上之圖案。視情況,將模型應用於後OPC資料庫之結果可與模型化影像一起使用以改良熱點偵測。例如,後OPC資料庫之一模型僅考慮到設計效應,且因此可用以分離晶圓製程對設計之效應與晶圓製程對經製造遮罩之效應。可比較來自遮罩近場之模型化圖案與來自對應後OPC圖案之模型化晶圓影像。例如,當不同製程改變之一組模型化晶圓圖案匹配相同製程改變之對應模型化後OPC晶圓圖案時,可判定歸因於製程改變之晶圓圖案(或抗蝕劑圖案)之改變源自可再設計或監測之設計圖案,而非源自遮罩圖案中之一缺陷。然而,若歸因於來自後OPC資料庫之製程變動的晶圓上之改變不同於歸因於來自經恢復遮罩(或遮罩近場)之相同製程變動的晶圓上之改變,則此等熱點被視為源自來自實際遮罩之可修復或監測之一熱點。 亦可分析模擬晶圓影像差異以判定跨晶粒或隨時間(在光罩改變發生在製造過程中之曝光期間時)之晶圓CD均勻性(CDU)度量。例如,若解析度足夠高,則可藉由分析及量測目標邊緣之間的距離而量測各影像之各目標之CD。或者,可校準參考影像與測試影像之間的強度差異且將其變換成CD變動,如由Carl E.Hess等人於2015年3月20日申請之美國專利申請案第14/664,565號及由Rui-fang Shi等人於2014年10月6日申請之美國專利申請案第14/390,834號中進一步描述,該等申請案之全文為全部目的以引用的方式併入本文中。 在操作328中,亦可判定是否應修復光罩。可判定預期晶圓圖案變動超出期望在微影製程期間使用之製程窗之規格。在特定情況中,光罩可含有在操作336中修復之一缺陷。接著,可再鑑定光罩合格性。否則,在操作330中,若光罩無法修復則可丟棄光罩。接著,可製造一新光罩且再鑑定其合格性。 除使用一經恢復遮罩近場影像在一合格性鑑定過程中模擬晶圓影像之外或替代使用一經恢復遮罩近場影像在一合格性鑑定過程中模擬晶圓影像,亦可直接在一光罩合格性鑑定過程中評估一遮罩近場影像或結果。圖5係根據本發明之一替代實施例之繪示應用於一經恢復遮罩近場影像或結果之一光罩合格性鑑定過程500之一流程圖。首先,在操作502中,自一光罩恢復遮罩近場結果。可針對一特定光罩基於自此特定光罩獲取之影像恢復此遮罩近場影像。此操作可類似於圖1之遮罩近場恢復操作而實踐。另外,圖5之若干操作可依與圖3之操作類似之一方式實施,但對於經恢復光罩近場影像,包含此影像之強度及/或相位分量。 如所展示,接著,在操作522中,可評估遮罩近場結果以特性化及/或定位缺陷。大體上可判定對應光罩是否有缺陷或具有需要監測之熱點。更明確言之,本文中描述之用於評估模擬晶圓影像之一些技術可在遮罩近場影像上實施。在一缺陷偵測過程中,可比較測試遮罩近場影像與參考遮罩近場影像之任何適合度量。例如,可比較強度及/或相位。不同缺陷類型將對強度及/或相位值具有不同影響。可將此等差異判定為將可能導致一缺陷晶圓或識別可修復或可監測之熱點圖案或區域之真實缺陷(與無影響公害缺陷相反)。 例如,接著,在操作524中,可判定設計是否有缺陷。若判定設計有缺陷,則在操作532中可修改設計。例如,可判定一光罩近場影像與其對應基於後OPC之近場之間的任何差異是否高於用於偵測缺陷之一預定義臨限值。程序500可繼續以判定是否監測晶圓熱點、修復光罩、或再設計光罩,如上文描述。若不認為設計有缺陷,則在操作526中可判定是否可監測任何熱點。例如,可判定一測試光罩近場影像與參考光罩近場影像之間的任何強度及/或相位差異接近一相關聯臨限值。 例如,若判定可監測熱點,則在操作534中可在晶圓製程期間監測熱點。例如,可在晶圓製作期間監測熱點圖案以判定製程是否已偏離出規格且已引起對應晶圓圖案具有改變為不可接受的值之關鍵參數。一項實施方案可涉及設定一相對較高敏感度等級以檢測對應熱點之光罩及/或晶圓圖案。隨著條件進一步遠離標稱製程條件,CD誤差或EPE可變大且危及晶圓製程之完整性。 在操作528中,亦可判定是否將修復光罩。在特定情況中,光罩可含有在操作536中修復之一缺陷。接著,可再鑑定光罩合格性。否則,在操作530中,若光罩無法修復則可丟棄該光罩。接著,可製造一新光罩且再鑑定其合格性。 本發明之特定技術在開始晶圓製造之前提供遮罩圖案合格性鑑定及對實體遮罩上之弱圖案或熱點之早期偵測。除提供基於光罩影像恢復光罩近場之外,亦可考量晶圓製程效應(包含焦點及曝光之諸多設定,及晶圓抗蝕劑、蝕刻、CMP及任何其他晶圓製程之效應)之一完整範圍如何影響晶圓圖案。由於僅使用光罩影像恢復遮罩近場而不使用光罩設計資料,故無需遮罩之先前知識。由於遮罩圖案大體上為晶圓圖案之4倍,故可判定圖案相對於設計資料庫之更確切位置。上述技術亦可擴展至任何適合類型之遮罩,諸如EUV遮罩之圖案合格性鑑定。 本發明之技術可在硬體及/或軟體之任何適合組合中實施。圖6係其中可實施本發明之技術之一例示性檢測系統600之一圖形表示。檢測系統600可自模仿一掃描器(未展示)之一高NA檢測工具或一低NA檢測器接收輸入602。檢測系統亦可包含:一資料分配系統(例如,604a及604b),其用於分配經接收輸入602;一強度信號(或區塊(patch))處理系統(例如,區塊處理器及光罩合格性鑑定系統(例如,612)),其用於遮罩近場及晶圓恢復、製程模型化等;一網路(例如,交換式網路608),其容許檢測系統組件之間的通信;一選用大容量儲存裝置616;及一或多個檢測控制及/或檢視站(例如,610),其用於檢視遮罩近場強度及相位(值、影像或差異)、光罩/晶圓影像、經識別熱點、CD、CDU圖、製程參數等。檢測系統600之各處理器通常可包含一或多個微處理器積體電路且亦可含有介面及/或記憶體積體電路,且另外可耦合至一或多個共用及/或全域記憶體裝置。 用於產生輸入資料602之檢測器或資料獲取系統(未展示)可採取用於獲得一光罩之強度信號或影像之任何適合儀器(舉例而言,如本文中進一步描述)之形式。例如,低NA檢測器可建構一光學影像或基於反射、透射或以其他方式引導至一或多個光感測器的經偵測光之一部分而產生光罩之一部分之強度值。接著,低NA檢測器可輸出強度值或影像。 在一入射光束跨一光罩之各區塊掃描時,低NA檢測工具可操作以偵測且收集反射及/或透射光。如上文所述,入射光束可跨各自包括複數個區塊之光罩掃描帶掃描。回應於來自各區塊之複數個點或子區域之此入射光束而收集光。 低NA檢測工具大體上可操作以將此經偵測光轉換成對應於強度值之經偵測信號。經偵測信號可採取具有對應於光罩之不同位置處的不同強度值之振幅值之一電磁波形之形式。經偵測信號亦可採取強度值及相關聯光罩點座標之一簡單清單之形式。經偵測信號亦可採取具有對應於光罩上之不同位置或掃描點之不同強度值之一影像之形式。可在光罩之全部位置經掃描且轉換成經偵測信號之後產生光罩之兩個或更多個影像,或可在各光罩部分經掃描具有最終兩個或更多個影像時產生兩個或更多個影像之部分以在掃描整個光罩之後完成光罩。 經偵測信號亦可採取空中影像之形式。即,可使用一空中成像技術來模擬光微影系統之光學效應以產生曝露於晶圓上之光阻劑圖案之一空中影像。一般而言,模仿光微影工具之光學器件以基於來自光罩之經偵測信號產生一空中影像。空中影像對應於自行進穿過光微影光學器件及光罩而至一晶圓之光阻劑層上之光產生之圖案。另外,亦可模仿用於特定類型之光阻劑材料之光阻劑曝光過程。 入射光或經偵測光可行進穿過任何適合空間孔徑以依任何適合入射角產生任何入射或經偵測光輪廓。例如,可利用可程式化照明或偵測孔徑來產生一特定光束輪廓,諸如偶極、四極、類星體、環形等。在一特定實例中,可實施光源遮罩最佳化(SMO)或任何像素化照明技術。入射光亦可行進穿過一線性偏光器以使照明光瞳之全部或一部分在一或多個偏光中線性地偏光。經偵測光可行進穿過變跡組件以阻擋收集光束之特定區域。 可藉由資料分配系統經由網路608接收強度或影像資料602。資料分配系統可與用於保持經接收資料602之至少一部分之一或多個記憶體裝置(諸如RAM緩衝區)相關聯。較佳地,總記憶體足夠大以保持資料之一整個樣本。例如,一個十億位元組之記憶體良好運用於1百萬乘1000像素或點之一樣本。 資料分配系統(例如,604a及604b)亦可控制經接收輸入資料602之部分至處理器(例如,606a及606b)之分配。例如,資料分配系統可將一第一區塊之資料投送至一第一區塊處理器606a,且可將一第二區塊之資料投送至區塊處理器606b。亦可將多個區塊之多組資料投送至各區塊處理器。 區塊處理器可接收對應於光罩之至少一部分或區塊之強度值或一影像。區塊處理器亦可各自耦合至一或多個記憶體裝置(諸如提供局部記憶體功能,諸如保持經接收資料部分之DRAM裝置) (未展示)或與該一或多個記憶體裝置整合。較佳地,記憶體足夠大以保持對應於光罩之一區塊之資料。例如,8百萬位元組之記憶體良好運用於對應於512乘1024像素之一區塊之強度值或一影像。或者,區塊處理器可共用記憶體。 各組輸入資料602可對應於光罩之一掃描帶。可將一或多組資料儲存於資料分配系統之記憶體中。此記憶體可由資料分配系統內之一或多個處理器控制,且可將記憶體劃分成複數個分區。例如,資料分配系統可將對應於一掃描帶之一部分之資料接收至一第一記憶體分區(未展示)中,且資料分配系統可將對應於另一掃描帶之另一資料接收至一第二記憶體分區(未展示)中。較佳地,資料分配系統之記憶體分區之各者僅保持將投送至與此記憶體分區相關聯之一處理器之資料之部分。例如,資料分配系統之第一記憶體分區可保持第一資料且將第一資料投送至區塊處理器606a,且第二記憶體分區可保持第二資料且將第二資料投送至區塊處理器606b。 資料分配系統可基於資料之任何適合參數定義且分配資料之各組資料。例如,可基於光罩上之區塊的對應位置而定義且分配資料。在一項實施例中,各掃描帶與對應於掃描帶內之像素的水平位置之行位置之一範圍相關聯。例如,掃描帶之行0至256可對應於一第一區塊,且此等行內之像素將包括投送至一或多個區塊處理器之第一影像或第一組強度值。同樣地,掃描帶之行257至512可對應於一第二區塊,且此等行中之像素將包括投送至(若干)不同區塊處理器之第二影像或第二組強度值。 檢測設備可適於檢測半導體裝置或晶圓與光學光罩以及EUV光罩或遮罩。適合檢測工具之實例係在193 nm下操作之Teron™或可購自加利福尼亞州苗必達市之KLA-Tencor之TeraScan™ DUV光罩檢測工具。可使用本發明之檢測設備檢測或成像之其他類型之樣本包含任何表面,諸如一平板顯示器。 一檢測工具可包含:至少一個光源,其用於產生一入射光束;照明光學器件,其用於將入射光束引導至一樣本上;收集光學器件,其用於引導回應於入射光束而自樣本發射之一輸出光束;一感測器,其用於偵測輸出光束且產生輸出光束之一影像或信號;及一控制器/處理器,其用於控制檢測工具之組件且促進遮罩近場產生及分析技術,如本文中進一步描述。 在以下例示性檢測系統中,入射光束可呈同調光之任何適合形式。另外,可使用任何適合透鏡配置來將入射光束引導朝向樣本且將源自樣本之輸出光束引導朝向一偵測器。輸出光束可自樣本反射或散射或透射穿過樣本。對於EUV光罩檢測,輸出光束通常自樣本反射。同樣地,可使用任何適合偵測器類型或任何適合數目之偵測元件來接收輸出光束且基於經接收輸出光束之特性(例如,強度)提供一影像或一信號。 首先將描述一一般化光微影工具,但一EUV光微影工具通常將僅具有反射型光學器件。圖7A係根據特定實施例之可用以將一遮罩圖案自一光遮罩M轉印至一晶圓W上之一典型微影系統700之一簡化示意性表示。此等系統之實例包括掃描器及步進器,更明確言之可購自Veldhoven, Netherlands之ASML之TWINSCAN NXT:1970Ci步進及掃描系統。一般而言,一照明源703將一光束引導穿過一照明光學器件707 (例如,透鏡705)而至定位於一遮罩平面702中之一光遮罩M上。照明透鏡705在該平面702處具有一數值孔徑701。數值孔徑701之值影響光遮罩上之哪些缺陷係微影顯著缺陷且哪些缺陷並非微影顯著缺陷。行進穿過光遮罩M之光束之一部分形成經引導穿過成像光學器件713且至一晶圓W上以起始圖案轉印之一圖案化光學信號。在一反射系統(未展示)中,照明光束自遮罩M之特定部分反射(且由此遮罩M之其他部分吸收)且形成經引導穿過一晶圓W上之反射成像光學器件之一圖案化信號。 檢測工具可利用類似組件或與上文描述之光微影工具類似地組態,例如,LNI能力。然而,檢測工具可替代地或額外地組態以產生高解析度影像。圖7B提供根據特定實施例之具有照明光學器件751a且包含在一光罩平面752處具有一相對較大數值孔徑751b的一成像透鏡之一例示性檢測系統750之一示意性表示。例如,檢測系統之光罩平面752處之數值孔徑751b可比微影系統700之光罩平面702處之數值孔徑701大得多,此將導致測試檢測影像與實際印刷影像之間的差異。 本文中描述之檢測技術可在各種專門組態之檢測系統(諸如圖7B中示意性地繪示之檢測系統)上實施。所繪示系統750包含一照明源760,該照明源760產生經引導穿過照明光學器件751a而至光罩平面752中之一光遮罩M上之一光束。光源之實例包含一同調雷射光源(例如,深UV或氣體雷射產生器)、一過濾燈、LED光源等。在特定實施例中,一光源通常可提供高脈衝重複速率、低雜訊、高功率、穩定性、可靠性及擴展性。應注意,雖然一EUV掃描器在13.5nm波長下操作,但用於一EUV光罩之一檢測工具不必在相同波長下操作(儘管其可以)。在一項實例中,光源係一193 nm雷射。 照明光學器件751a可包含用於精確光束定位之一光束操控裝置及可用以提供光位準控制、斑點雜訊降低及高光束均勻性之一光束調節裝置。光束操控及/或光束調節裝置可為與例如一雷射分離之實體裝置。照明光學器件751a亦可包含用於控制偏光、焦點、放大、照明強度分佈等之光學器件。 如上文說明,檢測系統750可在光罩平面752處具有可等於或大於對應微影系統之一光罩平面數值孔徑(例如,圖7A中之元件701)之一數值孔徑751b。待檢測光遮罩M經放置於光罩平面752處之一遮罩載台上且曝露於光源。 所描繪檢測系統750可包含偵測光學器件753a及753b,該等偵測光學器件753a及753b亦可包含經設計以提供例如60倍至200倍放大或更大放大用於增強檢測之顯微鏡放大光學器件。收集光學器件753a及753b可包含用於調節輸出光/光束之任何適合光學器件。例如,收集光學器件753a及753b可包含用於控制焦點、光瞳形狀、偏光分析儀設定等之光學器件。 在一透射模式中,可將來自遮罩M之圖案化影像引導穿過光學元件753a之一集合,該等光學元件753a將圖案化影像投影至一感測器754a上。在一反射模式中,收集元件(例如,光束分離器776及偵測透鏡778)將來自遮罩M之反射光引導且捕獲至感測器754b上。儘管展示兩個感測器,然可在相同光罩區域之不同掃描期間使用一單一感測器來偵測反射光及透射光。適合感測器包含電荷耦合裝置(CCD)、CCD陣列、時間延遲積分(TDI)感測器、TDI感測器陣列、光電倍增管(PMT)及其他感測器。 可使照明光學器件行相對於遮罩載台及/或由任何適合機構相對於一偵測器或相機移動之載台移動以掃描光罩之區塊。例如,可利用一馬達機構來移動載台。例如,馬達機構可由一螺桿驅動器及步進馬達、具有回饋位置之線性驅動器,或帶致動器及步進馬達形成。系統700可利用一或多個馬達機構以使系統組件之任一者相對於照明或收集光學路徑移動。 可藉由一電腦系統773或更一般而言藉由一或多個信號處理裝置處理由各感測器(例如,754a及/或754b)捕獲之信號,該一或多個信號處理裝置可各自包含經組態以將來自各感測器之類比信號轉換成數位信號以供處理之一類比轉數位轉換器。電腦系統773通常具有耦合至輸入/輸出埠之一或多個處理器及經由適當匯流排或其他通信機構之一或多個記憶體。 電腦系統773亦可包含一或多個輸入裝置(例如,一鍵盤、滑鼠、操縱桿)以提供使用者輸入,諸如改變焦點及其他檢測配方參數。電腦系統773亦可連接至載台以控制例如一樣本位置(例如,聚焦及掃描),且連接至其他檢測系統組件以控制此等檢測系統組件之其他檢測參數及組態。 電腦系統773可經組態(例如,用程式化指令)以提供一使用者介面(例如,一電腦螢幕),以顯示遮罩近場強度及相位(值、影像或差異)、光罩/晶圓影像、經識別熱點、CD、CDU圖、製程參數等。電腦系統773可經組態以分析反射及/或透射之經偵測及/或模擬信號或影像、經恢復光罩近場結果之強度、相位及/或其他特性等。電腦系統773可經組態(例如,用程式化指令)以提供一使用者介面(例如,在一電腦螢幕上),以顯示所得強度及/或相位值、影像及其他檢測特性。在特定實施例中,電腦系統773經組態以實行上文詳述之檢測技術。 因為此等資訊及程式指令可在一專門組態之電腦系統上實施,所以此一系統包含用於執行本文中描述之各種操作之可儲存於一電腦可讀媒體上之程式指令/電腦程式碼。機器可讀媒體之實例包含但不限於:磁性媒體,諸如硬碟、軟碟及磁帶;光學媒體,諸如CD-ROM光碟;磁光媒體,諸如光碟;及經專門組態以儲存且執行程式指令之硬體裝置,諸如唯讀記憶體裝置(ROM)及隨機存取記憶體(RAM)。程式指令之實例包含諸如由一編譯器產生之機器碼及含有可由電腦使用一解譯器執行之較高階程式碼之檔案兩者。 圖7B展示其中將一照明光束以相對於受檢測表面之一實質上法向角引導朝向樣本表面之一實例。在其他實施例中,可以一傾斜角引導一照明光束,此容許分離照明光束與反射光束。在此等實施例中,一衰減器可定位於反射光束路徑上以在反射光束到達一偵測器之前衰減該反射光束之一零階分量。此外,一成像孔徑可定位於反射光束路徑上以使反射光束之零階分量的相位偏移。 應注意,上文描述及圖式不應解釋為限制系統之特定組件且系統可以諸多其他形式具體實施。例如,預期檢測或量測工具可具有來自經配置以偵測缺陷及/或解析一光罩或晶圓之特徵之關鍵態樣的任何數目個已知成像或度量工具之任何適合特徵。例如,一檢測或量測工具可經調適用於亮場成像顯微術、暗場成像顯微術、全天空成像顯微術、相位對比顯微術、偏光對比顯微術及同調探測顯微術。亦預期可使用單影像及多影像方法來捕獲目標之影像。此等方法包含例如單抓取、雙抓取、單抓取同調探測顯微術(CPM)及雙抓取CPM方法。亦預期非成像光學方法(諸如散射測量法)形成檢測或度量設備之部分。 儘管為清楚理解之目的已相當詳細地描述前述發明,但將明白,可在隨附申請專利範圍之範疇內實踐某些改變及修改。應注意,存在實施本發明之過程、系統及設備之諸多替代方式。因此,本實施例被視為闡釋性的且非限制性的,且本發明不限於本文中給出之細節。Cross-References to Related Applications This application claims the priority right of U.S. Patent Application No. 15 / 641,150 filed by Rui-fang Shi et al. On July 3, 2017, and is a part of its continuation application. The U.S. Patent Application No. 15 / 641,150 claims the priority right of PCT Application No. PCT / US2016 / 045749 filed by Abdurrahman Sezginer et al. On August 5, 2016 under 35 USC § 120, which is PCT / US2016 / 045749 claims the priority of the previous application filed by Abdurrahman Sezginer and others on August 10, 2015, U.S. Application No. 14 / 822,571 (now U.S. Application No. 9,547,892, issued on January 17, 2017) right. This application also claims the priority of US Provisional Application No. 62 / 508,369, filed on May 18, 2017. The entire contents of these applications and patents are incorporated herein by reference for all purposes. In the following description, numerous specific details are set forth to provide a thorough understanding of the present invention. The invention may be practiced without some or all of these specific details. In other instances, well-known process operations or equipment components have not been described in detail so as not to unnecessarily obscure the present invention. Although the invention will be described in conjunction with specific embodiments, it will be understood that it is not intended to limit the invention to those embodiments. Before masks are shipped to a production facility, defects of each mask are detected and other features of the mask are otherwise characterized (e.g., pattern stability, CD, CD uniformity) before wafers are fabricated using this mask (Properties) It would be advantageous to make and / or periodically requalify this mask after it has been used in the production process for a certain period of time. One embodiment of the present invention includes a technique for restoring a near-field image of a mask based on a mask image obtained from a detection tool under a plurality of different imaging parameters. This mask near-field image can then be used in many mask qualification applications. In one example, a mask near-field image can be input to a lithographic model to predict a wafer image or various wafer pattern characteristics related to how the resulting pattern will be printed on the wafer. The predicted wafer image and / or various wafer characteristics can then be analyzed for defect detection, mask qualification or requalification, and / or any other suitable measurement or inspection application. The mask near-field image itself can also be analyzed for various purposes as described further herein. The terms "mask", "mask", and "light mask" are used interchangeably herein and each may generally include a transparent substrate, such as glass, borosilicate glass, Quartz or fused silica. Opaque (or substantially opaque) materials can include any suitable material that completely or partially blocks light lithographic light (eg, deep UV or extreme UV). Exemplary materials include chromium, molybdenum silicide (MoSi), tantalum silicide, tungsten silicide, opaque MoSi on glass (OMOG), and the like. A polycrystalline silicon film can also be added between the opaque layer and the transparent substrate to improve adhesion. A low-reflection film such as molybdenum oxide (MoO 2 ), Tungsten oxide (WO 2 ), Titanium nitride (TiO 2 ) Or chromium oxide (CrO 2 ). In a specific example, an EUV mask may include multiple layers having alternating layers with different refractive indices and low absorption characteristics, such as molybdenum (Mo) and silicon (Si), and an absorber material such as Anti-reflective oxide capped tantalum boron nitride film). The term photomask refers to different types of photomasks, including but not limited to a clear-field photomask, a dark-field photomask, a binary photomask, a phase shift mask (PSM), and an alternate PSM , An attenuation or halftone PSM, a ternary attenuation PSM, a chromium-free phase lithography PSM, and a chromium-free phase lithography (CPL). A clear field mask has a transparent field or background area, and a dark field mask has an opaque field or background area. A binary mask is a mask having patterned areas that are transparent or opaque. For example, a light mask made from a transparent fused silica blank having a pattern defined by a chrome metal adsorption film may be used. Binary masks are different from phase-shift masks (PSM). One type of phase-shift mask (PSM) can include a film that only partially transmits light, and these masks are often referred to as halftone or embedded phase-shift masks. Masks (EPSM), such as ArF and KrF masks. If a phase shift material is placed on the alternate clear space of a reticle, the reticle is called an alternate PSM, an ALT PSM, or a Levenson PSM. One type of phase-shifting material applied to any layout pattern is called an attenuating or halftone PSM, which can be made by replacing an opaque material with a part of a transmissive or "halftone" film. A ternary attenuation PSM system also includes one of the completely opaque features of the attenuation PSM. The next generation of lithography has introduced the use of extreme ultraviolet radiation (EUV, wavelength 13.5 nm), which is absorbed in the normal atmosphere and glass. For this reason, the lithography EUV process takes place under vacuum, and the optical reflection lens / mirror is used to focus to an EUV light mask that will have a reflective and absorber pattern instead of a translucent and opaque pattern. FIG. 1 is a flowchart of a mask near-field recovery program 100 according to an embodiment of the present invention. The following mask recovery process 100 can be performed for a particular mask or set of masks at any suitable time in the life cycle of a mask, as described further below in various use cases of the restored mask near field. By way of example, a mask near-field can be restored before any wafers are made with this (etc.) mask, before starting a large number of wafer fabrications, or during requalification of this (etc.) mask eligibility. First, in operation 102, a mask detection tool is used to obtain at least three images of a mask according to different imaging configurations. Alternatively, two images can be used, but it has been found to work well with three images. Acquisition using different imaging configurations can be simultaneous or sequential. The acquired image need not be at the field plane. By way of example, two or more images can be acquired at a pupil plane with direct access to the diffraction intensity. Various suitable combinations of lighting and / or collection configurations may be utilized to acquire two or more images. Generally, different imaging configurations are selected to provide an image from which the near field of the mask can be calculated. Any suitable imaging or optical configuration can be selected so that the mask near field remains the same under different operating conditions. Examples include different focus settings, different illumination shapes (e.g., different directions or patterns), different polarized light for the entire illumination pupil or different parts of the illumination pupil, different apodization settings that obscure different parts of the collected beam, etc . In one embodiment, different focus settings (over focus and defocus (such as 0 focus, ± 800 or ± 1600 defocus, etc.) can be used to acquire different images. In another example, different quadrants of the illumination pupil may have different polarization settings. In another example, the imaging configuration may include high-resolution images, such as transmission images with different pupil shapes and / or different focus conditions (eg, for ArF masks). In another embodiment, three or more reflected images having different pupil shapes and / or different focus conditions may be obtained (e.g., for an EUV mask). A relatively low NA (eg, less than 0.5) can be used to image the mask with a "substantially low resolution". In contrast, a "substantially high-resolution image" generally refers to a feature in which a feature printed on a reticle appears substantially as it is formed on the reticle (in the optics of the reticle detection system used to produce the image). (Within limits), one mask, one image. A "substantially high-resolution image" of a mask is obtained by imaging a physical mask at the plane of the mask with a substantially high-resolution mask detection system (e.g., a numerical aperture (NA) greater than 0.8). Generate an image. The "substantially low NA" used to generate a reticle image can be used essentially on the reticle side by an exposure / lithography system to project an image of the reticle onto a wafer to thereby characterize the reticle. The NA transferred to the wafer is the same. In a substantially low NA image (or LNI), the mask feature may have an appearance that is substantially different from the actual mask feature. For example, a mask feature may appear to have more rounded corners in an LNI, one of the features, than an actual feature formed on the mask. In general, any suitable imaging tool can be used to mask the near-field recovery process. In the specific embodiment described herein, the results of an initial recovery process can later be used for pattern stability or defect detection evaluations of the same or other masks based on additional mask images from a particular inspection tool . For consistency in these use cases, a photomask detection system detector that will be used for subsequent inspections of the same or other photomasks or a similarly configured photomask detection system (e.g., The same method and model of the photomask detection system (a different photomask detection system) is a similarly configured detector to obtain the image of the photomask used for mask near-field recovery. In other words, images that can be used for mask recovery can be acquired under the same optical conditions as would be used during subsequent mask testing or qualification processes. In this way, the interaction between the photomask and the illumination electromagnetic waves of the detection system can be measured as directly as possible. In alternative embodiments, the means for mask near-field recovery may be different from a mask detection system. For example, the imaging tool may utilize the same wavelength (eg, wavelength (DUV-based 193.3 nm or EUV-based 13.5 nm) as the lithography system in which the reticle will be used for wafer manufacturing). In fact, any suitable electromagnetic wavelength can be used to mask near-field recovery. Referring again to the illustrated example, then, in operation 104, three or more images may be aligned with each other or each image may be aligned with a post-OPC database. For example, acquired images may be aligned via a spatial or frequency domain method. The alignment adjustment may depend on the specific geometry of the imaging system used. If different images are obtained using different collection paths, an adjustment of the images can be made to compensate for the differences in optical paths. In imaging tools, a mask having one of various patterns is illuminated by electromagnetic (EM) waves incident from many directions. This incident light is diffracted from different points of the mask pattern according to different electromagnetic field phases which interfere with each other. The near field of the mask is an electromagnetic field at a distance close to one of the wavelengths of the mask. The collection optics generally directs a diffraction-restricted portion of the light from the mask toward a detector (or wafer) to form an image. The detector detects the intensity as a result of interference due to the near field of the mask, but does not detect the phase. Although the far-field intensity is obtained in the detected signal, it is desirable to recover the mask near-field including amplitude and phase. In the illustrated embodiment, the near-field of the mask is restored and stored based on these acquired mask images, as illustrated in operation 106. Multiple images (or signals) are generally used to recover a masked near field that contains both phase and amplitude components. The near field data can be determined by a regression technique based on the images acquired from the photomask. For example, a quasi-Newton or conjugate gradient technique can be used to recover (regress) a selected portion of a reticle from an optical image or intensity of the reticle recorded at a detector plane Near field. In addition, any other suitable regression method and / or algorithm can be used to determine near-field data from one or more actual images. Masking near-field recovery can usually be achieved by solving an optimization problem, which seeks to minimize the difference between the observed intensity image and the image obtained from the assumed masked optical field. In particular, restoring the near field of a mask from the intensity image of a mask is an inverse calculation problem or a regression problem. The near field can be restored iteratively by minimizing a cost function (eg, energy or penalty function). The minimized number may be the sum of the squares of the differences between the acquired image and the intensity image calculated from the near field of the mask at the detector. In other words, the intensity images can be calculated from the final mask near field for various optical system property groups, and when the mask near field is found, these calculated images will most closely match the acquired images. Various mask near field recovery methodologies and system embodiments are further described in U.S. Patent No. 9,478,019 issued by Abdurrahman Sezginer et al. On October 25, 2016, the entirety of which is incorporated herein by reference for all purposes. in. In the case where multiple images are acquired under various optical conditions, a restored near-field mask carrying phase and amplitude information m Can be determined by the following equation: Equation 1 In Equation 1 above, Is the measured image for imaging condition α, Is a set of feature vectors describing detection imaging systems, A set of corresponding eigenvalues of the imaging system, and A non-negative weighting factor between 0 and 1. The above equations can be solved iteratively, for example, by methods such as quasi-Newton or conjugate gradients. Another example is the Gerchberg-Saxton algorithm, in which one of a field plane image and a pupil plane diffraction level can be used to solve both the amplitude and phase of an object. In one embodiment, the near field of the mask may be determined based on the acquired image via a Hopkins approximation. In another embodiment, the regression does not include a thin mask approximation. For example, the near field of a mask is calculated as an electromagnetic field that appears near the surface of the mask when illuminated by a normal incident plane wave. In lithography and inspection, a photomask is illuminated by plane waves incident from many directions. When the direction of incidence changes, according to the Hopkins approximation, the direction of the diffraction order changes but its constant amplitude and phase remain approximately unchanged. The embodiments described herein may use the Hopkins phase approximation but not the so-called thin mask or Kirchhoff approximation. The recovery formula can also vary with different norms or a regular term. R Adding and changing, this is not conducive to oscillations in the near field, as follows: The regular term R may have previous information about the near field or an expectation based on a physical understanding of the mask substrate / material. In addition, the norm used for image differences can be an l-norm and can be adjusted based on the specific needs of the optimization function. It is interesting to note that due to the wider range of incident angles of light of a higher NA and associated interference electric field components, the interference of the masked electromagnetic field vector caused by a higher NA will be larger (greater than a Low NA detection system). The actual mask can be attributed to the mask writing process and changes with the intended design pattern. Obtaining a near-field mask from the masked image means that this near-field mask is obtained from the actual physical mask rather than the design database. That is, the near field of the mask can be restored without using a design database. Masked near-field results can then be used in various applications. In one embodiment, masked near-field results can be used to predict wafer patterns using one or more models. That is, the restored mask near field can be used to simulate a lithographic image. Any suitable technique can be used to simulate a lithographic image based on a masked near-field image. One embodiment includes computing a lithographic image through a partial homology model: Equation 2 where λ i Represents the characteristic value of lithography TCC (transfer cross coefficient); Feature vector (core) representing TCC; s Wafer stack, which contains the refractive index of the film; f Focus; and z The vertical position of the lithographic plane in the resist material. The cross-transfer coefficient (TCC) of Equation 2 may include the vector propagation of a field through a lithographic projector (including a film stack on a wafer). Before using a model to predict wafer results, the model can be calibrated to produce the most accurate results possible. The model can be calibrated using any suitable technique. A specific embodiment of the present invention provides a technique for calibrating a lithography model based on a near-field result of a mask recovered from a calibration mask. In an alternative embodiment, a design library is used to calibrate the model. For example, calibration mask images can be generated from a design library. A calibration reticle will typically be designed to have properties (s) that are substantially similar to the reticle to be inspected for defect detection or to be measured for metrology purposes. For example, the calibration mask and the test mask are preferably formed of substantially the same material having substantially the same thickness and composition. Alternatively, two photomasks may have been formed using the same process. The two reticles may not necessarily have the same pattern printed thereon, as long as the patterns on the reticle can be broken down into substantially the same segments (eg, lines with similar widths, etc.). In addition, the photomask to be detected and the photomask used to obtain an image may be the same photomask. FIG. 2 is a flowchart illustrating a model calibration process 200 according to a specific embodiment of the present invention. As shown, in operation 208, a set of initial model parameters may be used to model the photolithography process and photoresist as applied to the mask near-field image (201) recovered from a calibration mask. Alternatively, the calibration process 200 may use a simulated calibration mask image (202) simulated from a design database. The mask image can be generated from the database by simulating the mask making and imaging process on the design database. Any suitable model can be used to generate optical images for the characteristics of the design database. By way of example, this simulation may include using the coherent system summation (SOCS) or Abbe methodology described herein. There are several software packages that can simulate intensity images of an optical system from a known design database. An example was developed by Dr. Fraunhofer IISB in Erlangen, Germany. LiTHO. In the case of simulating an image 202 from the design database, the near field can be simulated first. This can be achieved by using the software package cited above and several other packages (including Prolith by KLA-Tencor, HyperLith by Panoramic Technologies, etc.) carry out. The model used to generate the wafer image based on the near field image of the mask may include only the effects of a photolithography scanner, and it may also include the effects of resist, etching, CMP, or any other wafer process. An exemplary process simulation model tool is available from Prolith of KLA-Tencor, Inc. of Milpitas, California. Resist and etching processes can be closely or approximately modeled. In a specific embodiment, the model may be in the form of a compact resist model, which includes a 3D acid diffusion inside a particular resist material and a configuration that imposes boundary conditions therein, and is applied to form one of the latent images Single threshold. It should be noted that the modeled lithography tool may have a lighting shape or light source different from the mask detection tool used to obtain the actual image of the mask. In a particular embodiment, the modeled lithography tool may have a light source that is the same as or similar to a mask detector tool. Other simulation methods can be used, such as SOCS or Abbe. An algorithm commonly referred to as coherent system summation (SOCS) attempts to transform an imaging system into a bank of linear systems whose output is squared, scaled, and summed. The SOCS approach has been described elsewhere, including Nicolas Cobb's PhD thesis "Fast Optical and Process Proximity Correction Algorithms for Integrated Circuit Manufacturing" (University of California, Berkeley, Spring 1998). The Abbe algorithm involves calculating object images one at a time for each point source, and then summing the intensity images together taking into account the relative intensity of each source point. The input of the model and its modeling parameters includes a set of process conditions applied to the restored near-field mask. That is, the model is configured to simulate different sets of process conditions on the reconstructed near-field mask (or simulated mask image). Each set of process conditions generally corresponds to a set of wafer process parameters that are characterised or partially characterised as a wafer process for forming a wafer pattern from a mask. For example, a specific focus and exposure setting can be entered into the model. Other adjustable model parameters can also include one or more of the following parameters: a projection lens wavefront parameter, an apodization parameter, a chromatic aberration focus error parameter, a vibration parameter, a resist profile index, and a resist float Slag measurement, top loss measurement, etc. Using this model with different sets of process conditions can result in a set of simulated wafer or resist pattern images formed by the reconstructed near-field mask under different processing conditions, and these simulated wafer images can be used for pattern stability and Defect detection evaluation, as described further herein. In operation 216, a calibration mask may also be used to fabricate one of the calibration wafers from which the actual image was obtained. In one example, a critical dimension (CD) scanning electron microscope (SEM) is used to acquire actual images. Other imaging tools can be used, but a high-resolution tool is preferred. In general, a calibration wafer will contain any number of known structures, which can vary widely. The structure may be in the form of a grating that is usually periodic. Each grating can be periodic in one direction (X or Y) (for example, a linear spatial grating), or it can be periodic in two directions (X and Y) (for example, a linear grating) Raster space raster). An example of a grid space grating may include a line array in the Y direction, where each line is segmented in the X direction. Another example of grid space is a one-point structure array. That is, each structure can take the form of a one-line space grating, a grid space grating, a checkerboard pattern structure, and the like. Structural design characteristics can each include line width (width at a specific height), line space width, line length, shape, sidewall angle, height, pitch, grating orientation, top profile (top rounded or T-top level ), Bottom contour (footing), etc. The calibration wafer may contain structures with different combinations of these characteristics. As should be understood, different structural characteristics (such as different widths, pitches, shapes, pitches, etc.) exhibit different responses to the focal point, and therefore the calibration mask preferably includes different structures with different characteristics. In a specific embodiment, the calibration wafer may take the form of a "design-of-experience (DOE)" wafer having one of different measurement points subjected to different processing conditions. In a more general embodiment, process parameter variations are organized in a pattern on the surface of a semiconductor wafer (referred to as a DOE wafer). In this way, the measurement points correspond to different locations on the surface of the wafer with different associated process parameter values. In one example, the DOE pattern is a focus / exposure matrix (FEM) pattern. Generally, a DOE wafer exhibiting a FEM pattern includes a grid pattern of measurement points. In one grid direction (for example, the x direction), the exposure dose changes while the depth of focus remains constant. In an orthogonal grid direction (for example, the y direction), the depth of focus changes while the exposure dose remains constant. In this way, the measurement data collected from the FEM wafer includes data associated with known changes in focus and dosage process parameters. FEM measurement points are generally positioned across the focal-exposure matrix wafer. In fact, there can generally be one or more measurement points per field. Each field may be formed using a different combination of focus and exposure combinations (or may be just focus or exposure). For example, a first field may be generated using a first combination, and a second field may be generated using a second combination different from the first combination. Multiple combinations can be generated using changing focus and changing exposure, changing focus-constant exposure, constant focus-changing exposure, and the like. The number of measurement points can also be different. The number of dots per field is usually smaller on the production wafer because the real estate on the production wafer is extremely precious. Furthermore, measurements performed on a production wafer are less due to time constraints in production than measurements performed on a focus exposure matrix wafer. In one embodiment, a single point is measured per field. In another embodiment, multiple points are measured per field. In most FEM cases, the measurement point structure is formed from the same designed pattern using different processing parameters. It should be noted, however, that different focus exposure matrices may have different structures. For example, a first matrix may be performed using a first raster type, and a second matrix may be performed using a second raster type different from the first raster type. In an alternative embodiment, a simulated calibration image (202) generated from a design database for a calibration mask can be used as input to the model. That is, the model can be calibrated without recovering the near field from a physical calibration mask. Instead, the lithographic image is simulated by simulating (non-recovering) the near field from the design database and applying the lithography imaging model to the simulated near field to achieve a lithographic result comparable to the actual result from the wafer (216) . In general, optical signal data associated with known changes in process parameters, structural parameters, or both of any group can be envisaged. Regardless of the form, the calibration wafer structure can be printed on many different wafer layers. In particular, a standard lithography process is generally used (e.g., a circuit image is projected through a photomask and onto a silicon wafer coated with a photoresist) to print a printed structure onto a photoresist Layer. The wafer may be one of the calibration wafers having a layer of material corresponding to the material normally present on the product wafer at this step in the testing process. The printed structure can be printed over other structures in the lower layer. The calibration wafer can be one of the product wafers with the potential to produce a working device. The calibration wafer may be one of the simple wafers used for calibration models only. The calibration wafer may be the same wafer used to calibrate the OPC design model. More than one calibration wafer can be used to calibrate the lithographic model. When using multiple calibration wafers, the same or different calibration masks can be used. Different calibration masks can have patterns with different sizes to generate a wider range of image data. The process parameters used to form the calibration structure are generally configured to maintain the characteristics of the pattern within the desired specifications. For example, the calibration structure may be printed on a calibration wafer as part of a calibration procedure, or they may be printed on a production wafer during production. During production, calibration structures are typically printed in scribe lines between device regions (eg, the dies defining an IC) placed on a production wafer. The measurement point may be a dedicated calibration structure disposed around the device structure, or it may be part of the device structure (eg, a periodic portion). As should be understood, it may be more difficult to use part of the device structure, but it tends to be more accurate because it is part of the device structure. In another embodiment, the alignment structure may be printed across an entire alignment wafer. Referring again to FIG. 2, in operation 210, a corresponding modeling result and a calibration result (eg, an image) may be compared. Then, in operation 212, it may be determined whether the model parameters will be adjusted. If the model parameters are to be adjusted, the model parameters are adjusted in operation 214 and the process 200 repeats operation 208 to model the lithography process (and the resist) using the adjusted parameters. The model parameters can be adjusted until one of the differences between the model image and the calibration image has reached a minimum value that is also below a predefined threshold. The minimized number may be the sum of the squares of the differences between the acquired calibration image and the simulated image. The output of this process 200 is a lithography / resist model and its final model parameters. This set of model parameters overcomes the technical obstacles associated with mask process modeling and mask 3D diffraction calculations by using the nature of the mask near field. The simulated wafer pattern based on the recovered mask near-field results can be used for many mask inspection, measurement, and / or qualification purposes. In one embodiment, a mask qualification is performed by assessing whether the restored mask near-field will likely cause wafer pattern defects under a range of simulated wafer fabrication conditions. For defect detection, the printability of a mask defect on a wafer is important, and the printability of a mask defect directly depends on the near field of the mask and the lithography system. After obtaining a final calibrated lithography / resist / etching model for one of a specific process (regardless of how the model is obtained), this model can be used to produce accurate masks from this mask before wafer fabrication using a mask Wafer planar resist images (for example, after development or etching) or used to requalify this mask eligibility. These resist images will allow us to evaluate wafer images of any inspection pattern with high fidelity and through different focus and exposure settings or other lithographic parameters. Because this evaluation process can occur before wafer fabrication, the cycle of qualification and defect detection can be significantly reduced. The simulated wafer image also enables the source of different patterning problems to be separated by comparing simulated wafer images after lithography, after application of the resist model, and after etching. FIG. 3 is a flowchart illustrating a mask qualification process 300 according to an embodiment of the present invention. In operation 302, for example, a mask near-field image is restored for a specific mask based on an image acquired from the specific mask. This operation may include the mask near-field recovery operation of FIG. 1. After obtaining a near field of the mask, in operation 303, the lithographic process (and the resist) may also be modeled using the final model parameters regarding the restored near field of the mask. For example, a final model is used to simulate a wafer image using a masked near-field image. Next, in operation 322, the simulated wafer pattern may be evaluated to determine pattern stability and / or positioning defects. In general, it can be determined whether the corresponding photomask may cause unstable or defective wafer patterns. In one embodiment, a plurality of different process conditions (such as focus and dose) are used to apply a model to a mask near-field image or result to evaluate the mask design stability under varying process conditions. FIG. 4A is a flowchart illustrating a process 400 for determining the stability of a wafer pattern according to an exemplary application of the present invention. First, in operation 402, each test image may be aligned with its corresponding reference image, and these images are also generated by the model under different sets of process conditions. The model calculates different test images and reference images under different processing conditions / parameters. In operation 404, each pair of aligned images may be compared to each other to obtain one or more wafer pattern differences. Then, in operation 406, the threshold value may be associated with each wafer pattern difference. Wafer pattern differences and their associated thresholds can be used together to characterize pattern stability. That is, the amount of deviation (pattern difference) of a particular pattern under different simulation process conditions and whether this deviation crosses an associated threshold value together characterize the pattern stability. A process window of a manufacturing process specifies an expected or defined process deviation amount under which the resulting patterns are evaluated to ensure that they will remain stable or within certain specified deviation tolerances (eg, threshold values). Different thresholds for assessing pattern stability can be assigned to different areas of the mask and thereby correspond to the wafer pattern. Thresholds can all be the same or different based on various factors (such as pattern design background, pattern MEEF (or mask error enhancement factor as described further below) level, or sensitivity of device performance to wafer pattern variations). For example, compared to a semi-dense area of the mask, we can choose a closer threshold for the pattern in a dense area. Optionally, a set of initial hot spots or pattern weakness areas can be identified in both the reference mask pattern and the test mask pattern. For example, a designer may provide a list of one of the design hotspots that is critical to the function of the device. For example, an area defined as a hot spot may be assigned a detection threshold, and a non-hot spot area may be assigned a higher threshold (for defect detection). This difference can be used to optimize detection resources. This pattern stability assessment can be used to facilitate mask qualification, thereby overcoming many challenges in this area. As the density and complexity of integrated circuits (ICs) continue to increase, detecting photolithographic mask patterns becomes increasingly challenging. Each new-generation IC has denser and more complex patterns that currently meet and exceed the optical limits of lithography systems. To overcome these optical limitations, various resolution enhancement techniques (RET), such as optical proximity correction (OPC), have been introduced. For example, OPC helps overcome some diffraction restrictions by modifying the light mask pattern so that the resulting printed pattern corresponds to the original desired pattern. Such modifications may include disturbances in the size and edges of the main IC features (ie, printable features). Other modifications involve adding serifs to the corners of the pattern and / or providing nearby sub-resolution assistance features (SRAF), which is not expected to result in printed features and therefore are referred to as non-printable features. It is expected that these non-printable features cancel out pattern disturbances that would otherwise occur during the printing process. However, OPC makes the mask pattern even more complicated and often very different from the resulting wafer image. In addition, OPC defects are usually not converted into printable defects. The increased complexity of light mask patterns and the fact that all pattern elements are not expected to directly affect the printed pattern make the task of detecting meaningful pattern defects of light masks much more difficult. As the semiconductor industry moves toward even smaller features, cutting-edge manufacturers are starting to use even more exotic OPCs, such as inverse lithography (ILT), which results in highly complex patterns on the mask. Therefore, it is highly desirable to know the mask write fidelity and its wafer print quality before physically manufacturing the wafer. A measure of the importance of a defect is its MEEF or mask error enhancement factor. This factor correlates the size of the defect in the mask plane with the magnitude of the defect it will affect the printed image. High MEEF defects have a high effect on printed patterns; low MEEF defects have little or no effect on printed patterns. A pattern that is too small in a dense thin line portion of a pattern is an example of a defect with a high MEEF, where a small mask plane size error can cause one of the printed patterns to completely collapse. An isolated small pinhole is one example of a defect with a low MEEF, where the defect itself is too small to print and is far enough from the nearest major pattern edge to not affect how the edge is printed. Such examples show that the MEEF of a defect is a slightly more complex function of the defect type and the pattern background in which the defect is located. In addition to higher MEEF mask defects that cause more significant wafer defects, specific design patterns and corresponding mask patterns can also be more robust to process variations than other designs and mask patterns. When the manufacturing process starts to deviate from optimal process conditions, certain mask patterns can cause more significant wafer pattern disturbances and defects. FIG. 4B is a flowchart of a defect detection program 450 according to another embodiment of the present invention. In operation 452, each modeled test wafer image may be aligned with its corresponding reference image. In one embodiment, a die-to-die or cell-to-cell alignment can be accomplished. In another embodiment, the modeled test wafer image is aligned with a reference image generated from the corresponding OPC design. For example, a post-OPC design is processed to simulate the mask making process for this design. For example, the corners are rounded. Generally, a reference image can be derived from the same die as an earlier test image, from an adjacent identical die, or generated from a design database. In a specific example, a reference image is obtained from one of the "gold" grains that has been proven to be defect-free (eg, immediately after manufacturing the mask and qualifying the mask). The gold mask image obtained from the mask when the known mask is free of defects can be stored and used later to calculate the gold mask near-field image and wafer image when needed. Alternatively, the near-field image of the golden mask can be stored for future access without the need to calculate the near-field during future inspections. In operation 454, the pairs of aligned test images and reference images are compared based on an associated threshold value to locate mask defects. Any suitable mechanism can be used to associate a threshold with a particular mask area, as described further above. Any suitable metric can be compared between the test image and the reference image. For example, the profile of the test and reference wafer images can be compared as a measure of edge placement error (EPE). Then, in operation 456, the corresponding simulated wafer defect area and its corresponding reference pre-OPC area may be compared for each mask defect. That is, the simulated wafer pattern is evaluated to determine whether a mask defect causes a wafer defect with an expected design change. Referring again to FIG. 3, in operation 324, it can then be determined whether the design is defective based on the simulated mask image. In one embodiment, it is determined whether the design pattern under an specified range (or process window) of one of the process conditions results in unacceptable wafer pattern variations. Determine if there is a significant difference due to process variability. If the difference between different processed wafer patterns is higher than a corresponding threshold, then these wafer patterns can be considered defective. These system defects are called hot spots. It can also be determined whether any difference between an analog wafer pattern from a photomask and its corresponding pre-OPC pattern is higher than a predefined threshold. If it is determined that the design is defective, the design may be modified in operation 332. Once a reticle design is verified, the reticle may still contain hot spots that should be monitored. The following operations are described as being performed on a mask that has at least some identified hot spots. Of course, if the mask does not contain any identified hotspots, the following operations in FIG. 3 can be skipped and the masks are used without hotspot monitoring during production and inspection. In the illustrated example, if the design is not considered defective, a determination can be made in operation 326 as to whether any hot spots can be monitored. If the hotspot is determined to be monitorable, the hotspot may be monitored during the wafer process in operation 334. For example, a hot pattern can be monitored during wafer fabrication to determine whether the process has deviated from specifications and has caused the corresponding wafer pattern to have key parameters that change to unacceptable values. One embodiment may involve setting a relatively high MEEF level to detect masks and / or wafer patterns corresponding to hot spots. As conditions move further away from the nominal process conditions, the CD or EPE can grow larger and endanger the integrity of the wafer process. Hotspot patterns can be identified only when a test mask pattern changes by a predefined amount, regardless of how this change is compared to the original intended design (e.g., pre-OPC data). In other words, a significant change in one of the physical mask patterns under different process conditions may indicate a problem with the expected design pattern. The difference between the corresponding modeled image portions indicates the difference in the effects of the process conditions on the designed pattern and the manufactured mask. The differences associated with a particular design pattern are often referred to as "design hotspots" or simply "hot spots" and represent weaknesses in the design regarding specific process conditions that have been checked (and possibly also on manufactured masks). Examples of the types of differences that can be found between modeled images under different process conditions are CD (critical size) or EPE (edge placement error). In another embodiment, if the model is applied to a post-OPC design database, the resulting wafer pattern may correspond to a pattern that the designer intends to print on the wafer. Optionally, the results of applying the model to a post-OPC database can be used with modeled images to improve hotspot detection. For example, one of the models of the post-OPC database only considers design effects, and thus can be used to separate the effects of wafer processing on design and the effects of wafer processing on manufactured masks. The modeled pattern from the near field of the mask can be compared with the modeled wafer image from the corresponding post OPC pattern. For example, when a group of modeled wafer patterns of different process changes match the corresponding modeled OPC wafer pattern of the same process change, the source of the change in the wafer pattern (or resist pattern) due to the process change can be determined Design patterns that can be redesigned or monitored rather than derived from a defect in the mask pattern. However, if a change on a wafer due to a process change from a post-OPC database is different from a change on a wafer due to the same process change from a recovered mask (or mask near field), then this The hot spot is considered to originate from a hot spot that can be repaired or monitored from the actual mask. The simulated wafer image differences can also be analyzed to determine wafer CD uniformity (CDU) metrics across the die or over time (when mask changes occur during exposure during the manufacturing process). For example, if the resolution is high enough, the CD of each target of each image can be measured by analyzing and measuring the distance between the edges of the targets. Alternatively, the intensity difference between the reference image and the test image can be calibrated and transformed into a CD variation, such as by Carl E. Hess et al., U.S. Patent Application No. 14 / 664,565, filed on March 20, 2015, and U.S. Patent Application No. 14 / 390,834, filed by Rui-fang Shi et al. On October 6, 2014 The entire text of these applications is incorporated herein by reference for all purposes. In operation 328, it may also be determined whether the photomask should be repaired. It can be determined that the expected wafer pattern change exceeds the specifications of the process window expected to be used during the lithography process. In certain cases, the reticle may contain one of the defects repaired in operation 336. Then, the mask eligibility can be re-qualified. Otherwise, in operation 330, if the photomask cannot be repaired, the photomask may be discarded. Then, a new photomask can be manufactured and requalified. In addition to using a restored mask near-field image to simulate a wafer image during a qualification process, or instead of using a restored mask near-field image to simulate a wafer image during a qualification process, you can also directly A mask near-field image or result is evaluated during mask qualification. FIG. 5 is a flowchart illustrating a mask qualification process 500 applied to a restored near-field image or result according to an alternative embodiment of the present invention. First, in operation 502, a mask near-field result is restored from a mask. The near-field image of the mask can be restored for a specific mask based on the image acquired from the specific mask. This operation may be practiced similar to the mask near-field recovery operation of FIG. 1. In addition, some operations of FIG. 5 may be implemented in a manner similar to that of FIG. 3, but for the restored mask near-field image, the intensity and / or phase components of the image are included. As shown, then, in operation 522, the mask near-field results may be evaluated to characterize and / or locate defects. Generally, it can be determined whether the corresponding photomask is defective or has hot spots that need to be monitored. More specifically, some of the techniques described herein for evaluating simulated wafer images can be implemented on masked near-field images. During a defect detection process, any suitable measure of the test mask near-field image and the reference mask near-field image can be compared. For example, the intensity and / or phase can be compared. Different defect types will have different effects on intensity and / or phase values. These discrepancies can be judged to be true defects that may cause a defective wafer or identify hot spots or areas that can be repaired or monitored (as opposed to non-impacting defects). For example, then, in operation 524, it may be determined whether the design is defective. If the design is determined to be defective, the design may be modified in operation 532. For example, it can be determined whether any difference between a mask near-field image and its corresponding post-OPC-based near field is higher than a predefined threshold for detecting defects. The process 500 may continue to determine whether to monitor wafer hot spots, repair the mask, or redesign the mask, as described above. If the design is not considered to be defective, a determination can be made in operation 526 as to whether any hot spots can be monitored. For example, it can be determined that any intensity and / or phase difference between a test mask near-field image and a reference mask near-field image is close to an associated threshold. For example, if it is determined that a hot spot can be monitored, the hot spot can be monitored during the wafer process in operation 534. For example, a hot pattern can be monitored during wafer fabrication to determine whether the process has deviated from specifications and has caused the corresponding wafer pattern to have key parameters that change to unacceptable values. One embodiment may involve setting a relatively high sensitivity level to detect masks and / or wafer patterns corresponding to hot spots. As conditions move further away from the nominal process conditions, CD errors or EPEs can become large and endanger the integrity of the wafer process. In operation 528, it may also be determined whether the photomask will be repaired. In certain cases, the reticle may contain one of the defects repaired in operation 536. Then, the mask eligibility can be re-qualified. Otherwise, in operation 530, if the photomask cannot be repaired, the photomask may be discarded. Then, a new photomask can be manufactured and requalified. The specific technology of the present invention provides mask pattern qualification and early detection of weak patterns or hot spots on a physical mask before starting wafer fabrication. In addition to providing a mask-based image recovery mask near field, wafer process effects (including many settings for focus and exposure, and effects of wafer resist, etching, CMP, and any other wafer process) How a full range affects the wafer pattern. Since only the mask image is used to restore the near field of the mask without using the mask design data, prior knowledge of the mask is not required. Since the mask pattern is roughly four times larger than the wafer pattern, it can be determined that the pattern is more accurately positioned relative to the design database. The above-mentioned technology can also be extended to any suitable type of mask, such as the pattern qualification of EUV masks. The techniques of this invention may be implemented in any suitable combination of hardware and / or software. FIG. 6 is a graphical representation of an exemplary detection system 600 in which the techniques of the present invention can be implemented. The detection system 600 may receive input 602 from a high NA detection tool or a low NA detector that mimics a scanner (not shown). The detection system may also include: a data distribution system (for example, 604a and 604b) for distributing the received input 602; an intensity signal (or patch) processing system (for example, a block processor and a photomask) Qualification system (e.g., 612)) for masking near-field and wafer recovery, process modeling, etc .; a network (e.g., switched network 608) that allows communication between inspection system components ; A mass storage device 616 is selected; and one or more detection control and / or inspection stations (for example, 610) for inspecting the near field intensity and phase (value, image or difference) of the mask, the mask / crystal Circle image, identified hot spots, CD, CDU map, process parameters, etc. Each processor of the detection system 600 may typically include one or more microprocessor integrated circuits and may also include interfaces and / or memory volume circuits, and may additionally be coupled to one or more shared and / or global memory devices. . The detector or data acquisition system (not shown) used to generate the input data 602 may take the form of any suitable instrument (for example, as described further herein) for obtaining the intensity signal or image of a photomask. For example, a low NA detector may construct an optical image or generate intensity values for a portion of a mask based on a portion of the detected light that is reflected, transmitted, or otherwise directed to one or more light sensors. The low NA detector can then output an intensity value or image. The low NA detection tool is operable to detect and collect reflected and / or transmitted light as an incident beam is scanned across blocks of a mask. As described above, the incident light beam can be scanned across the mask scanning strips each including a plurality of blocks. Light is collected in response to this incident beam from a plurality of points or sub-regions of each block. The low NA detection tool is generally operable to convert this detected light into a detected signal corresponding to an intensity value. The detected signal may take the form of an electromagnetic waveform having an amplitude value corresponding to different intensity values at different positions of the mask. The detected signal can also take the form of a simple list of intensity values and one of the associated mask point coordinates. The detected signal may also take the form of an image having different intensity values corresponding to different positions or scanning points on the mask. Two or more images of the mask can be generated after the entire position of the mask is scanned and converted into a detected signal, or two can be generated when each part of the mask is scanned with the final two or more images Parts of one or more images to complete the mask after scanning the entire mask. The detected signals can also take the form of aerial images. That is, an aerial imaging technique can be used to simulate the optical effects of the photolithography system to generate an aerial image of a photoresist pattern exposed on the wafer. Generally, the optics of a photolithography tool are simulated to generate an aerial image based on a detected signal from a photomask. The aerial image corresponds to a pattern generated by light that enters the photoresist layer of a wafer through the photolithography optics and the photomask. In addition, a photoresist exposure process for a specific type of photoresist material can be simulated. Incident or detected light may pass through any suitable spatial aperture to produce any incident or detected light profile at any suitable incident angle. For example, a specific beam profile such as dipole, quadrupole, quasar, ring, etc. can be generated using programmable illumination or detection aperture. In a particular example, light source mask optimization (SMO) or any pixelated lighting technique may be implemented. Incident light may also travel through a linear polarizer to linearly polarize all or a portion of the illumination pupil in one or more polarized light. The detected light can pass through the apodization component to block a specific area of the collected light beam. The intensity or image data 602 may be received via a network 608 by a data distribution system. The data distribution system may be associated with one or more memory devices (such as a RAM buffer) for holding at least a portion of the received data 602. Preferably, the total memory is large enough to hold one entire sample of data. For example, a gigabyte of memory works well for a sample of 1 million by 1000 pixels or points. Data distribution systems (e.g., 604a and 604b) may also control the distribution of portions of the input data 602 received to processors (e.g., 606a and 606b). For example, the data distribution system may post data of a first block to a first block processor 606a, and may post data of a second block to a block processor 606b. Multiple sets of data from multiple blocks can also be delivered to each block processor. The block processor may receive an intensity value or an image corresponding to at least a portion of the mask or the block. The block processors may also be individually coupled to or integrated with one or more memory devices (such as providing local memory functions, such as a DRAM device holding a received data portion) (not shown). Preferably, the memory is large enough to hold data corresponding to a block of the mask. For example, 8 megabytes of memory works well for an intensity value or an image corresponding to a block of 512 by 1024 pixels. Alternatively, the block processors may share memory. Each set of input data 602 may correspond to one scanning band of the photomask. One or more sets of data can be stored in the memory of the data distribution system. The memory can be controlled by one or more processors in the data distribution system, and the memory can be divided into a plurality of partitions. For example, the data distribution system may receive data corresponding to a portion of a scan zone into a first memory partition (not shown), and the data distribution system may receive another data corresponding to another scan zone to a first zone. Two memory partitions (not shown). Preferably, each of the memory partitions of the data distribution system maintains only the portion of data that will be delivered to a processor associated with this memory partition. For example, the first memory partition of the data distribution system may hold the first data and post the first data to the block processor 606a, and the second memory partition may hold the second data and post the second data to the block Block processor 606b. The data distribution system can define and allocate groups of data based on any suitable parameters of the data. For example, data may be defined and assigned based on the corresponding positions of the blocks on the reticle. In one embodiment, each scan band is associated with a range of row positions corresponding to the horizontal position of pixels within the scan band. For example, rows 0 to 256 of the scanning zone may correspond to a first block, and the pixels in these rows will include a first image or a first set of intensity values that are delivered to one or more block processors. Similarly, the rows 257 to 512 of the scanning zone may correspond to a second block, and the pixels in these rows will include a second image or a second set of intensity values that are delivered to different block processors (s). Inspection equipment can be adapted to inspect semiconductor devices or wafers and optical masks as well as EUV masks or masks. Examples of suitable detection tools are Teron ™ operating at 193 nm or TeraScan ™ DUV photomask inspection tools available from KLA-Tencor, Milpitas, California. Other types of samples that can be detected or imaged using the detection device of the present invention include any surface, such as a flat panel display. A detection tool may include: at least one light source for generating an incident beam; illumination optics for directing the incident beam onto a sample; collection optics for directing emission from the sample in response to the incident beam An output beam; a sensor for detecting the output beam and generating an image or signal of the output beam; and a controller / processor for controlling the components of the detection tool and promoting the generation of a mask near field And analysis techniques, as described further herein. In the following exemplary detection system, the incident beam may be in any suitable form of co-dimming. In addition, any suitable lens configuration can be used to direct the incident beam toward the sample and the output beam originating from the sample toward a detector. The output beam can be reflected or scattered from the sample or transmitted through the sample. For EUV mask inspection, the output beam is usually reflected from the sample. Likewise, any suitable detector type or any suitable number of detection elements may be used to receive the output beam and provide an image or a signal based on the characteristics (eg, intensity) of the received output beam. A generalized photolithography tool will be described first, but an EUV light lithography tool will typically have only reflective optics. FIG. 7A is a simplified schematic representation of one of a typical lithographic system 700 that can be used to transfer a mask pattern from a light mask M to a wafer W according to a particular embodiment. Examples of such systems include scanners and steppers, and more specifically TWINSCAN NXT: 1970Ci stepping and scanning systems available from ASML, Veldhoven, Netherlands. Generally, an illumination source 703 directs a light beam through an illumination optical device 707 (eg, a lens 705) to a light mask M positioned in a mask plane 702. The illumination lens 705 has a numerical aperture 701 at the plane 702. The value of the numerical aperture 701 affects which defects on the light mask are significant lithographic defects and which defects are not significant lithographic defects. A portion of the light beam traveling through the light mask M forms a patterned optical signal that is guided through the imaging optics 713 and transferred onto a wafer W in an initial pattern. In a reflection system (not shown), the illumination beam is reflected from a specific portion of the mask M (and thereby absorbed by other portions of the mask M) and forms one of the reflective imaging optics guided through a wafer W Patterned signal. The detection tool may utilize similar components or be configured similarly to the light lithography tool described above, for example, LNI capabilities. However, detection tools may be alternatively or additionally configured to produce high-resolution images. FIG. 7B provides a schematic representation of an exemplary detection system 750 having illumination optics 751a and including an imaging lens with a relatively large numerical aperture 751b at a mask plane 752 according to a particular embodiment. For example, the numerical aperture 751b at the mask plane 752 of the inspection system may be much larger than the numerical aperture 701 at the mask plane 702 of the lithography system 700, which will cause a difference between the test image and the actual printed image. The detection techniques described herein can be implemented on a variety of specially configured detection systems, such as the detection system shown schematically in Figure 7B. The illustrated system 750 includes an illumination source 760 that generates a light beam that is guided through the illumination optics 751 a to a light mask M in a mask plane 752. Examples of the light source include a laser light source (eg, a deep UV or gas laser generator), a filter lamp, an LED light source, and the like. In certain embodiments, a light source can generally provide high pulse repetition rate, low noise, high power, stability, reliability, and scalability. It should be noted that although an EUV scanner is at 13. It operates at a wavelength of 5 nm, but one of the detection tools for an EUV mask need not operate at the same wavelength (although it can). In one example, the light source is a 193 nm laser. Illumination optics 751a may include a beam steering device for precise beam positioning and a beam adjustment device that may provide light level control, speckle noise reduction, and high beam uniformity. The beam steering and / or beam adjusting device may be a physical device separate from, for example, a laser. The illumination optics 751a may also include optics for controlling polarization, focus, magnification, illumination intensity distribution, and the like. As described above, the detection system 750 may have a numerical aperture 751b at the mask plane 752 that may be equal to or larger than a numerical aperture of a mask plane of the corresponding lithography system (eg, the element 701 in FIG. 7A). The to-be-detected light mask M is placed on a mask stage at a mask plane 752 and is exposed to a light source. The depicted detection system 750 may include detection optics 753a and 753b, and these detection optics 753a and 753b may also include microscope magnification optics that are designed to provide, for example, 60x to 200x or greater magnification for enhanced detection Device. The collection optics 753a and 753b may include any suitable optics for adjusting the output light / beam. For example, the collection optics 753a and 753b may include optics for controlling focus, pupil shape, polarization analyzer settings, and the like. In a transmission mode, the patterned image from the mask M can be guided through a collection of optical elements 753a, which project the patterned image onto a sensor 754a. In a reflection mode, a collection element (eg, beam splitter 776 and detection lens 778) directs and captures the reflected light from the mask M onto the sensor 754b. Although two sensors are shown, a single sensor can be used to detect reflected light and transmitted light during different scans of the same mask area. Suitable sensors include charge-coupled devices (CCD), CCD arrays, time delay integration (TDI) sensors, TDI sensor arrays, photomultiplier tubes (PMT), and other sensors. The row of illumination optics can be moved relative to the mask stage and / or by any suitable mechanism relative to a stage moved by a detector or camera to scan a block of the mask. For example, a motor mechanism can be used to move the stage. For example, the motor mechanism can be formed by a screw driver and a stepper motor, a linear driver with a feedback position, or an actuator and a stepper motor. The system 700 may utilize one or more motor mechanisms to move any of the system components relative to the illumination or collection optical path. The signals captured by each sensor (e.g., 754a and / or 754b) can be processed by a computer system 773 or more generally by one or more signal processing devices, which can be individually Contains an analog-to-digital converter configured to convert analog signals from each sensor into digital signals for processing. Computer system 773 typically has one or more processors coupled to input / output ports and one or more memories via appropriate buses or other communication mechanisms. The computer system 773 may also include one or more input devices (eg, a keyboard, mouse, joystick) to provide user input, such as changing focus and other test recipe parameters. The computer system 773 may also be connected to a stage to control, for example, the same position (eg, focus and scan), and to other detection system components to control other detection parameters and configurations of these detection system components. The computer system 773 may be configured (e.g., with programmed instructions) to provide a user interface (e.g., a computer screen) to display mask near-field intensity and phase (value, image, or difference), mask / crystal Circle image, identified hot spots, CD, CDU map, process parameters, etc. The computer system 773 may be configured to analyze reflected and / or transmitted detected and / or analog signals or images, the intensity, phase, and / or other characteristics of the near-field results of the recovered reticle. Computer system 773 may be configured (e.g., with programmed instructions) to provide a user interface (e.g., on a computer screen) to display the resulting intensity and / or phase values, images, and other detection characteristics. In a particular embodiment, the computer system 773 is configured to implement the detection techniques detailed above. Because such information and program instructions can be implemented on a specially configured computer system, this system contains program instructions / computer code that can be stored on a computer-readable medium for performing the various operations described herein. . Examples of machine-readable media include, but are not limited to: magnetic media such as hard disks, floppy disks, and magnetic tapes; optical media such as CD-ROM disks; magneto-optical media such as optical disks; and specially configured to store and execute program instructions Hardware devices, such as read-only memory (ROM) and random access memory (RAM). Examples of program instructions include both machine code generated by a compiler and files containing higher-level code executable by a computer using an interpreter. FIG. 7B shows an example in which an illumination beam is directed toward the sample surface at a substantially normal angle relative to the surface being detected. In other embodiments, an illumination beam can be directed at an oblique angle, which allows separation of the illumination beam from the reflected beam. In these embodiments, an attenuator may be positioned on the reflected beam path to attenuate a zeroth order component of the reflected beam before the reflected beam reaches a detector. In addition, an imaging aperture can be positioned on the reflected beam path to shift the phase of the zeroth order component of the reflected beam. It should be noted that the above description and drawings should not be construed as limiting specific components of the system and that the system may be embodied in many other forms. For example, the intended inspection or measurement tool may have any suitable feature from any number of known imaging or metrology tools configured to detect defects and / or resolve key features of a mask or wafer. For example, a detection or measurement tool may be adjusted for bright field imaging microscopy, dark field imaging microscopy, all-sky imaging microscopy, phase contrast microscopy, polarized contrast microscopy, and homogeneous detection microscopy. Surgery. It is also expected that single-image and multi-image methods can be used to capture the image of the target. These methods include, for example, single-grip, double-grip, single-grip coherent detection microscopy (CPM), and dual-grip CPM methods. It is also contemplated that non-imaging optical methods, such as scatterometry, form part of the detection or metrology equipment. Although the foregoing invention has been described in considerable detail for purposes of clarity of understanding, it will be understood that certain changes and modifications may be practiced within the scope of the accompanying patent application. It should be noted that there are many alternative ways of implementing the processes, systems, and devices of the present invention. Therefore, this embodiment is to be considered as illustrative and not restrictive, and the invention is not limited to the details given herein.

100‧‧‧遮罩近場恢復程序/遮罩恢復過程100‧‧‧Mask near-field recovery procedure / mask recovery process

102‧‧‧操作102‧‧‧Operation

104‧‧‧操作104‧‧‧Operation

106‧‧‧操作106‧‧‧Operation

200‧‧‧模型校準過程/程序200‧‧‧ Model Calibration Process / Procedure

201‧‧‧自校準光罩恢復之遮罩近場影像201‧‧‧Mask near-field image restored from calibration mask

202‧‧‧自設計資料庫模擬之模擬校準光罩影像/自設計資料庫模擬影像/自設計資料庫生成之模擬校準影像202‧‧‧Simulated calibration mask image simulated from design database / Simulated image from design database / Simulated calibration image generated from design database

208‧‧‧操作208‧‧‧Operation

210‧‧‧操作210‧‧‧ Operation

212‧‧‧操作212‧‧‧Operation

214‧‧‧操作214‧‧‧Operation

216‧‧‧操作/來自晶圓之實際結果216‧‧‧operation / actual results from wafer

300‧‧‧光罩合格性鑑定過程300‧‧‧ Mask Qualification Process

302‧‧‧操作302‧‧‧Operation

303‧‧‧操作303‧‧‧operation

322‧‧‧操作322‧‧‧ Operation

324‧‧‧操作324‧‧‧ Operation

326‧‧‧操作326‧‧‧operation

328‧‧‧操作328‧‧‧operation

330‧‧‧操作330‧‧‧ Operation

332‧‧‧操作332‧‧‧Operation

334‧‧‧操作334‧‧‧Operation

336‧‧‧操作336‧‧‧Operation

400‧‧‧過程400‧‧‧ process

402‧‧‧操作402‧‧‧operation

404‧‧‧操作404‧‧‧operation

406‧‧‧操作406‧‧‧Operation

450‧‧‧缺陷檢測程序450‧‧‧ Defect detection procedure

452‧‧‧操作452‧‧‧ Operation

454‧‧‧操作454‧‧‧ Operation

456‧‧‧操作456‧‧‧ Operation

500‧‧‧光罩合格性鑑定過程/程序500‧‧‧Photomask qualification process / procedure

502‧‧‧操作502‧‧‧operation

522‧‧‧操作522‧‧‧operation

524‧‧‧操作524‧‧‧ Operation

526‧‧‧操作526‧‧‧operation

528‧‧‧操作528‧‧‧ Operation

530‧‧‧操作530‧‧‧operation

532‧‧‧操作532‧‧‧operation

534‧‧‧操作534‧‧‧operation

536‧‧‧操作536‧‧‧operation

600‧‧‧檢測系統600‧‧‧ Detection System

602‧‧‧輸入/輸入資料/強度或影像資料602‧‧‧Enter / input data / intensity or image data

604a‧‧‧資料分配系統604a‧‧‧Data Distribution System

604b‧‧‧資料分配系統604b‧‧‧Data Distribution System

606a‧‧‧第一區塊處理器606a‧‧‧The first block processor

606b‧‧‧區塊處理器606b‧‧‧block processor

608‧‧‧交換式網路608‧‧‧switched network

610‧‧‧檢測控制/檢視站610‧‧‧Inspection control / viewing station

612‧‧‧區塊處理器及光罩合格性鑑定系統612‧‧‧block processor and photomask qualification system

616‧‧‧大容量存儲裝置616‧‧‧ Mass storage device

700‧‧‧微影系統700 ‧ ‧ lithography system

701‧‧‧數值孔徑/元件701‧‧‧NA / element

702‧‧‧遮罩平面702‧‧‧Mask plane

703‧‧‧照明源703‧‧‧light source

705‧‧‧透鏡705‧‧‧lens

707‧‧‧照明光學器件707‧‧‧lighting optics

713‧‧‧成像光學器件713‧‧‧ Imaging Optics

750‧‧‧檢測系統750‧‧‧ Detection System

751a‧‧‧照明光學器件751a‧‧‧Lighting Optics

751b‧‧‧數值孔徑751b‧‧‧ NA

752‧‧‧光罩平面752‧‧‧mask plane

753a‧‧‧偵測光學器件/收集光學器件/光學元件753a‧‧‧detection optics / collection optics / optical components

753b‧‧‧偵測光學器件/收集光學器件753b‧‧‧detection optics / collection optics

754a‧‧‧感測器754a‧‧‧Sensor

754b‧‧‧感測器754b‧‧‧Sensor

760‧‧‧照明源760‧‧‧light source

773‧‧‧電腦系統773‧‧‧Computer System

776‧‧‧光束分離器776‧‧‧ Beam Splitter

778‧‧‧偵測透鏡778‧‧‧detection lens

M‧‧‧光遮罩/遮罩M‧‧‧Light Mask / Mask

W‧‧‧晶圓W‧‧‧ Wafer

圖1係根據本發明之一項實施例之繪示一遮罩近場恢復程序之一流程圖。 圖2係根據本發明之一特定實施方案之繪示一模型校準過程之一流程圖。 圖3繪示根據本發明之一項實施例之表示一光罩合格性鑑定過程之一流程圖。 圖4A係根據本發明之一例示性應用之繪示用於判定光罩圖案穩定性之一過程之一流程圖。 圖4B係根據本發明之一另一實施例之繪示一缺陷檢測程序之一流程圖。 圖5係根據本發明之一替代實施例之繪示應用於一經恢復遮罩近場影像或結果之一光罩合格性鑑定過程之一流程圖。 圖6係其中可實施本發明之技術之一例示性檢測系統之一圖形表示。 圖7A係根據特定實施例之用於將一遮罩圖案自一光遮罩轉印至一晶圓上之一微影系統之一簡化示意性表示。 圖7B提供根據特定實施例之一光遮罩檢測設備之一示意性表示。FIG. 1 is a flowchart illustrating a mask near-field recovery procedure according to an embodiment of the present invention. FIG. 2 is a flowchart illustrating a model calibration process according to a specific embodiment of the present invention. FIG. 3 is a flowchart illustrating a mask qualification process according to an embodiment of the present invention. 4A is a flowchart illustrating a process for determining the stability of a mask pattern according to an exemplary application of the present invention. 4B is a flowchart illustrating a defect detection procedure according to another embodiment of the present invention. FIG. 5 is a flowchart illustrating a mask qualification process applied to a near-field image or result of a restored mask according to an alternative embodiment of the present invention. FIG. 6 is a graphical representation of an exemplary detection system in which the techniques of the present invention can be implemented. FIG. 7A is a simplified schematic representation of a lithography system for transferring a mask pattern from a light mask to a wafer according to a particular embodiment. FIG. 7B provides a schematic representation of a light mask detection device according to a particular embodiment.

Claims (30)

一種鑑定一光微影光罩合格性之方法,該方法包括: 使用一成像工具依不同照明組態及/或不同成像組態自一測試光罩之複數個圖案區域之各者獲取複數個影像; 針對該測試光罩之該等圖案區域之各者基於自該測試光罩之各圖案區域獲取之該等影像恢復一光罩近場;及 分析該經恢復光罩近場以特性化該測試光罩或判定此測試光罩是否有缺陷。A method for identifying the eligibility of a light lithography mask, the method includes: using an imaging tool to obtain a plurality of images from each of a plurality of pattern areas of a test mask according to different lighting configurations and / or different imaging configurations ; Each of the pattern areas of the test mask restores a near field of the mask based on the images obtained from each pattern area of the test mask; and analyzes the near field of the restored mask to characterize the test Mask or determine if this test mask is defective. 如請求項1之方法,其中在一光瞳平面處獲取該複數個影像。The method of claim 1, wherein the plurality of images are acquired at a pupil plane. 如請求項1之方法,其中分析該經恢復光罩近場以偵測該測試光罩中之缺陷,其中缺陷偵測包含:比較不同時間之一相同晶粒、相鄰晶粒、一晶粒與其對應黃金晶粒或一晶粒與來自與該測試光罩具有相同設計的一光罩複本之一對應晶粒之強度及/或相位。The method of claim 1, wherein the near field of the restored photomask is analyzed to detect defects in the test photomask, wherein the defect detection includes: comparing an identical crystal grain, an adjacent crystal grain, and a crystal grain at different times. The intensity and / or phase of the corresponding gold crystal grain or a crystal grain and a corresponding crystal grain from a photomask replica having the same design as the test photomask. 如請求項1之方法,其中在不使用用以製作該測試光罩之一設計資料庫之情況下恢復該光罩近場。The method of claim 1, wherein the near field of the photomask is restored without using a design database used to make the test photomask. 如請求項1之方法,其中該等經獲取影像包含在經選擇以導致一相同光罩近場之不同成像條件下獲取之至少三個反射影像,且其中該等不同成像條件包含不同焦點設定、不同光瞳形狀及/或偏光分析儀設定,其中不同照明條件包含不同光源強度分佈及/或偏光設定。The method of claim 1, wherein the acquired images include at least three reflection images acquired under different imaging conditions selected to result in a near field of the same mask, and wherein the different imaging conditions include different focus settings, Different pupil shapes and / or polarization analyzer settings, where different lighting conditions include different light source intensity distributions and / or polarization settings. 如請求項1之方法,其中該等經獲取影像包含在經選擇以導致一相同光罩近場之不同成像條件下獲取之至少三個透射影像,且其中該等不同成像條件包含不同焦點設定、不同光瞳形狀或偏光分析儀設定,其中該等不同照明條件包含不同光源強度分佈及/或偏光設定。The method of claim 1, wherein the acquired images include at least three transmission images acquired under different imaging conditions selected to result in a near field of the same mask, and wherein the different imaging conditions include different focus settings, Different pupil shapes or polarization analyzer settings, where the different lighting conditions include different light source intensity distributions and / or polarization settings. 如請求項1之方法,其進一步包括: 將一微影模型應用於該測試光罩之該光罩近場以模擬複數個測試晶圓影像,及 分析該等模擬測試晶圓影像以判定該測試光罩是否將可能導致一不穩定或缺陷晶圓, 其中該微影模型經組態以模擬一光微影製程。The method of claim 1, further comprising: applying a lithography model to the near field of the mask of the test mask to simulate a plurality of test wafer images, and analyzing the simulated test wafer images to determine the test Whether the photomask will cause an unstable or defective wafer, wherein the lithographic model is configured to simulate a photolithographic process. 如請求項7之方法,其中該微影模型模擬一照明源,該照明源具有與用於獲取該測試光罩或者另一光罩或晶圓之影像的一檢測工具之一照明形狀不同之一形狀。The method of claim 7, wherein the lithography model simulates an illumination source having a different illumination shape from one of a detection tool used to acquire an image of the test mask or another mask or wafer shape. 如請求項7之方法,其中運用自用於一校準光罩之一設計資料庫生成之影像校準該微影模型。The method of claim 7, wherein the lithographic model is calibrated using an image generated from a design database for a calibration mask. 如請求項7之方法,其中運用自一校準光罩獲取之影像校準該微影模型。The method of claim 7, wherein the lithographic model is calibrated using an image obtained from a calibration mask. 如請求項7之方法,其中該微影模型包含一緊湊抗蝕劑模型。The method of claim 7, wherein the lithographic model comprises a compact resist model. 如請求項7之方法,其中在複數個不同微影製程條件下將該微影模型應用於針對該測試光罩恢復之該光罩近場,且其中分析該等模擬測試晶圓影像包含:藉由比較與不同製程條件及一相同光罩區域相關聯之該等模擬測試影像之部分而判定該測試光罩在該等不同微影製程條件下是否將可能導致一不穩定晶圓。The method of claim 7, wherein the lithographic model is applied to the photomask near-field recovered for the test photomask under a plurality of different photolithography process conditions, and wherein analyzing the simulated test wafer images includes: borrowing By comparing portions of the simulated test images associated with different process conditions and the same mask area, it is determined whether the test mask may cause an unstable wafer under the different lithography process conditions. 如請求項7之方法,其進一步包括重複以下操作:獲取影像、恢復、應用該微影模型,及分析在應用光微影模型化、抗蝕劑模型化及蝕刻模型化之各者之後獲得的該等模擬測試晶圓影像以分離任何光罩缺陷之根源。The method of claim 7, further comprising repeating the following operations: acquiring an image, restoring, applying the lithographic model, and analyzing the obtained after applying each of photolithographic modeling, resist modeling, and etching modeling. These simulation test wafer images to isolate the root cause of any mask defects. 如請求項7之方法,其中該成像工具利用與其中該測試光罩將用於晶圓製造之一光微影系統相同之一波長範圍。The method of claim 7, wherein the imaging tool utilizes a wavelength range that is the same as a photolithography system in which the test mask is to be used in wafer manufacturing. 如請求項7之方法,其中該成像工具利用與其中該測試光罩將用於晶圓製造之一光微影系統不同之一波長範圍,且其中分析該等模擬測試晶圓影像以藉由對該等測試晶圓影像執行缺陷偵測而判定該測試光罩是否將可能導致一缺陷晶圓。The method of claim 7, wherein the imaging tool uses a wavelength range different from a photolithography system in which the test mask is to be used for wafer manufacturing, and wherein the simulated test wafer images are analyzed to The test wafer images perform defect detection to determine whether the test mask may cause a defective wafer. 一種用於鑑定一光微影光罩合格性之成像系統,該系統包括: 一光源,其用於產生一入射光束; 一照明光學模組,其用於將該入射光束引導至一光罩上; 一收集光學模組,其用於將來自該光罩之各圖案區域之一輸出光束引導至至少一個感測器; 至少一個感測器,其用於偵測該輸出光束且基於該輸出光束產生一影像或信號;及 一控制器,其經組態以執行以下操作: 引起依不同照明組態及/或不同成像組態自一測試光罩之複數個圖案區域之各者獲取複數個影像; 針對該測試光罩之該等圖案區域之各者基於自該測試光罩之各圖案區域獲取之該等影像恢復一光罩近場;及 分析該經恢復光罩近場以判定該測試光罩或另一光罩是否將可能導致一不穩定晶圓圖案或一缺陷晶圓。An imaging system for identifying the eligibility of a light lithographic mask, the system includes: a light source for generating an incident light beam; an illumination optical module for guiding the incident light beam to a mask A collection optical module for guiding an output beam from each of the pattern areas of the mask to at least one sensor; at least one sensor for detecting the output beam and based on the output beam Generating an image or signal; and a controller configured to perform the following operations: cause a plurality of images to be obtained from each of a plurality of pattern areas of a test mask according to different lighting configurations and / or different imaging configurations ; Each of the pattern areas of the test mask is restored a mask near field based on the images obtained from the pattern areas of the test mask; and the restored mask near field is analyzed to determine the test light Whether a mask or another mask will cause an unstable wafer pattern or a defective wafer. 如請求項16之系統,其中在一光瞳平面處獲取該複數個影像。The system of claim 16, wherein the plurality of images are acquired at a pupil plane. 如請求項16之系統,其中分析該經恢復光罩近場以偵測該測試光罩中之缺陷,其中缺陷偵測包含:比較不同時間之一相同晶粒、相鄰晶粒、一晶粒與其對應黃金晶粒或一晶粒與來自與該測試光罩具有相同設計的一光罩複本之一對應晶粒之強度及/或相位。If the system of claim 16, wherein the near field of the restored photomask is analyzed to detect defects in the test photomask, the defect detection includes: comparing an identical grain, an adjacent grain, and a grain at different times. The intensity and / or phase of the corresponding gold crystal grain or a crystal grain and a corresponding crystal grain from a photomask replica having the same design as the test photomask. 如請求項16之系統,其中在不使用用以製作該測試光罩之一設計資料庫之情況下恢復該光罩近場。The system of claim 16, wherein the near field of the photomask is restored without using a design database used to make the test photomask. 如請求項16之系統,其中該等經獲取影像包含在經選擇以導致一相同光罩近場之不同成像條件下獲取之至少三個反射影像,且其中該等不同成像條件包含不同焦點設定、不同光瞳形狀及/或偏光分析儀設定,其中不同照明條件包含不同光源強度分佈及/或偏光設定。If the system of claim 16, wherein the acquired images include at least three reflection images acquired under different imaging conditions selected to result in a near field of the same mask, and wherein the different imaging conditions include different focus settings, Different pupil shapes and / or polarization analyzer settings, where different lighting conditions include different light source intensity distributions and / or polarization settings. 如請求項16之系統,其中該等經獲取影像包含在經選擇以導致一相同光罩近場之不同成像條件下獲取之至少三個透射影像,且其中該等不同成像條件包含不同焦點設定、不同光瞳形狀及/或偏光分析儀設定,其中該等不同照明條件包含不同光源強度分佈及/或偏光設定。The system of claim 16, wherein the acquired images include at least three transmission images acquired under different imaging conditions selected to result in a near field of the same mask, and wherein the different imaging conditions include different focus settings, Different pupil shapes and / or polarization analyzer settings, where the different lighting conditions include different light source intensity distributions and / or polarization settings. 如請求項16之系統,其中該控制器進一步經組態以: 將一微影模型應用於該測試光罩之該光罩近場以模擬複數個測試晶圓影像,及 分析該等模擬測試晶圓影像以判定該測試光罩是否將可能導致一不穩定或缺陷晶圓, 其中該微影模型經組態以模擬一光微影製程。The system of claim 16, wherein the controller is further configured to: apply a lithographic model to the mask near field of the test mask to simulate a plurality of test wafer images, and analyze the simulated test crystals A circle image is used to determine whether the test mask may cause an unstable or defective wafer, wherein the lithography model is configured to simulate a photolithography process. 如請求項22之系統,其中該微影模型模擬一照明源,該照明源具有與用於獲取該測試光罩或者另一光罩或晶圓之影像的一檢測系統之一照明形狀不同之一形狀。The system of claim 22, wherein the lithographic model simulates an illumination source having an illumination shape different from that of one of a detection system for acquiring an image of the test mask or another mask or wafer shape. 如請求項22之系統,其中運用自用於一校準光罩之一設計資料庫生成之影像校準該微影模型。The system of claim 22, wherein the lithographic model is calibrated using an image generated from a design database for a calibration mask. 如請求項22之系統,其中運用自一校準光罩獲取之影像校準該微影模型。The system of claim 22, wherein the lithographic model is calibrated using an image acquired from a calibration mask. 如請求項22之系統,其中該微影模型包含一緊湊抗蝕劑模型。The system of claim 22, wherein the lithographic model comprises a compact resist model. 如請求項22之系統,其中在複數個不同微影製程條件下將該微影模型應用於針對該測試光罩恢復之該光罩近場,且其中分析該等模擬測試晶圓影像包含:藉由比較與不同製程條件及一相同光罩區域相關聯之該等模擬測試影像之部分而判定該測試光罩在該等不同微影製程條件下是否將可能導致一不穩定晶圓。The system of claim 22, wherein the lithographic model is applied to the photomask near-field restored for the test photomask under a plurality of different photolithographic process conditions, and wherein analyzing the simulated test wafer images includes: borrowing By comparing portions of the simulated test images associated with different process conditions and the same mask area, it is determined whether the test mask may cause an unstable wafer under the different lithography process conditions. 如請求項22之系統,其中該控制器進一步經組態以重複以下操作:獲取影像、恢復、應用該微影模型,及分析在應用光微影模型化、抗蝕劑模型化及蝕刻模型化之各者之後獲得的該等模擬測試晶圓影像以分離任何光罩缺陷之根源。The system of claim 22, wherein the controller is further configured to repeat the following operations: acquiring an image, restoring, applying the lithographic model, and analyzing the application of photolithographic modeling, resist modeling, and etching modeling These simulated test wafer images obtained after each of them to isolate the source of any mask defects. 如請求項22之系統,其中該成像系統利用與其中該測試光罩將用於晶圓製造之一光微影系統相同之一波長範圍。The system of claim 22, wherein the imaging system utilizes a wavelength range that is the same as a photolithography system in which the test mask is to be used in wafer manufacturing. 如請求項22之系統,其中該成像系統利用與其中該測試光罩將用於晶圓製造之一光微影系統不同之一波長範圍,且其中分析該等模擬測試晶圓影像以藉由對該等測試晶圓影像執行缺陷偵測而判定該測試光罩是否將可能導致一缺陷晶圓。 附圖翻譯 圖1 102 使用一遮罩檢測工具依不同成像組態獲取一遮罩之至少三個影像 104 將影像彼此對準或將各影像與後OPC DB對準 106 基於經獲取遮罩影像恢復且儲存遮罩近場 Mask Near Field (NF) Recovery 遮罩近場(NF)恢復 Mask Near-Field 遮罩近場 End 結束 圖2 201 自校準光罩恢復之遮罩近場影像 202 自設計資料庫模擬之校準光罩影像 208 使用一組初始或經調整模型參數來模型化如應用於遮罩近場(或模擬光罩)影像之微影製程(及抗蝕劑) 210 藉由比較經模型化結果與經校準結果而校準微影模型 212 是否調整模型參數? 214 調整模型參數 216 所製作校準晶圓之校準影像 Model Calibration 模型校準 Modelled Wafer Images 經模型化晶圓影像 Adjusted Model parameters 經調整模型參數 Calibrated model parameters 經校準模型參數 Y 是 N 否 End 結束 圖3 302 恢復遮罩近場結果 303 使用關於遮罩近場之最終模型參數來模型化微影製程(及抗蝕劑) 322 評估模擬晶圓圖案以判定圖案穩定性及/或定位缺陷 324 設計是否有缺陷? 326 熱點是否可監測? 328 是否修復光罩? 330 丟棄光罩 332 修改設計 334 在晶圓製程期間監測熱點 336 修復光罩(重複光罩合格性鑑定) Reticle Qualification Use I 光罩合格性鑑定使用I Simulated Wafer Images 經模擬晶圓影像 Y 是 N 否 End 結束 圖4A 402 將各測試影像相對於其對應參考影像對準,該等影像係由模型在不同組之製程條件下模擬 404 比較各對經對準影像以獲得一或多個晶圓圖案差異 406 使臨限值與各晶圓圖案差異相關聯 Pattern stability 圖案穩定性 End 結束 圖4B 452 將各測試光罩影像與其對應參考影像對準 454 基於相關聯臨限值比較各對經對準測試影像與參考影像以定位光罩缺陷 456 針對各光罩缺陷,比較模擬晶圓缺陷與對應參考預OPC Defect Inspection 缺陷檢測 End 結束 圖5 502 恢復遮罩近場結果 522 評估遮罩近場結果以特性化遮罩品質及/或定位缺陷 524 設計是否有缺陷? 526 熱點是否可監測? 528 是否修復光罩? 530 丟棄光罩 532 修改設計 534 在晶圓製程期間監測熱點 536 修復光罩(重複光罩合格性鑑定) Reticle Qualification Use II 光罩合格性鑑定使用II Y 是 N 否 End 結束 圖6 602 來自檢測工具之輸入 604a 分配器處理器&記憶體 604b 分配器處理器&記憶體 606a 區塊處理器&記憶體 606b 區塊處理器&記憶體 608 交換式網路 612 光罩合格性鑑定處理器&記憶體 616 資料 Defect Review 缺陷檢視 Keyboard 鍵盤 Mouse 滑鼠The system of claim 22, wherein the imaging system uses a wavelength range different from a photolithography system in which the test mask is to be used for wafer manufacturing, and wherein the simulated test wafer images are analyzed to The test wafer images perform defect detection to determine whether the test mask may cause a defective wafer. Drawing translation Figure 1 102 Use a mask detection tool to obtain at least three images of a mask according to different imaging configurations 104 Align the images with each other or align the images with the rear OPC DB 106 Image restoration based on the acquired mask And save Mask Near Field (NF) Recovery Mask Near-Field Mask Near Field End End Figure 2 201 Mask near-field image recovered from self-aligning mask 202 Self-design database Simulated Calibration Mask Image 208 Models using a set of initial or adjusted model parameters, such as lithography (and resist) applied to mask near-field (or simulated mask) images 210 Modeled by comparison Results and Calibration Results Calibrate the lithographic model 212 Do you adjust model parameters? 214 Adjusting the model parameters 216 Calibration image of the calibration wafer produced Model Calibration Wafer Images Adjusted Model parameters Calibrated model parameters Calibrated model parameters Y Yes N No End End Figure 3 302 Recovery Mask near-field results 303 Use final model parameters for the mask near-field to model the lithographic process (and resist) 322 Evaluate the simulated wafer pattern to determine pattern stability and / or locate defects 324 Is the design defective? 326 Can hot spots be monitored? 328 Is the photomask repaired? 330 Discard photomask 332 Modify design 334 Monitor hot spots during wafer process 336 Repair photomask (repeated photomask qualification) Reticle Qualification Use I Simulated Wafer Images Simulated wafer image Y Yes N No End Figure 4A 402 Align each test image relative to its corresponding reference image. These images are simulated by the model under different sets of process conditions. 404 Compare each pair of aligned images to obtain one or more wafer pattern differences. 406 Associate the threshold with the wafer pattern difference Pattern stability End End Figure 4B 452 Align each test mask image with its corresponding reference image 454 Compare each pair of aligned test images based on the associated threshold Masking defect with reference image 456 For each mask defect, compare the simulated wafer defect with the corresponding reference pre-OPC Defect Inspection Defect Inspection End End Figure 5 502 Restore mask near field results 522 Evaluate mask near field results to characterize Mask quality and / or positioning defects 524 Is there a defect in the design? Can 526 hot spots be monitored? 528 Is the photomask repaired? 530 Discard photomask 532 Modify design 534 Monitor hot spots during wafer process 536 Repair photomask (repeated photomask qualification) Reticle Qualification Use II Photomask qualification use II Y Yes N No End End Figure 6 602 From Inspection Tool Input 604a Distributor Processor & Memory 604b Distributor Processor & Memory 606a Block Processor & Memory 606b Block Processor & Memory 608 Switched Network 612 Photomask Qualification Processor & Memory 616 Data Defect Review Keyboard Mouse
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