TW200415793A - Method and apparatus for exposing or forming pattern on thin substrate or the like - Google Patents
Method and apparatus for exposing or forming pattern on thin substrate or the like Download PDFInfo
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- TW200415793A TW200415793A TW092131011A TW92131011A TW200415793A TW 200415793 A TW200415793 A TW 200415793A TW 092131011 A TW092131011 A TW 092131011A TW 92131011 A TW92131011 A TW 92131011A TW 200415793 A TW200415793 A TW 200415793A
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- 239000000758 substrate Substances 0.000 title claims abstract description 205
- 238000000034 method Methods 0.000 title claims description 34
- 238000006073 displacement reaction Methods 0.000 claims abstract description 47
- 230000033001 locomotion Effects 0.000 claims abstract description 21
- 239000011521 glass Substances 0.000 claims description 71
- 238000001514 detection method Methods 0.000 claims description 27
- 230000007246 mechanism Effects 0.000 claims description 15
- 230000008859 change Effects 0.000 claims description 13
- 238000004519 manufacturing process Methods 0.000 claims description 6
- 230000014759 maintenance of location Effects 0.000 claims description 2
- 230000003287 optical effect Effects 0.000 description 24
- 238000012937 correction Methods 0.000 description 23
- 238000009826 distribution Methods 0.000 description 13
- 238000010586 diagram Methods 0.000 description 10
- 239000004065 semiconductor Substances 0.000 description 10
- 230000005284 excitation Effects 0.000 description 9
- 238000003384 imaging method Methods 0.000 description 9
- 239000000463 material Substances 0.000 description 9
- 238000005259 measurement Methods 0.000 description 9
- 238000012545 processing Methods 0.000 description 9
- 229920002120 photoresistant polymer Polymers 0.000 description 8
- 239000004973 liquid crystal related substance Substances 0.000 description 6
- 230000008901 benefit Effects 0.000 description 5
- 238000005224 laser annealing Methods 0.000 description 5
- 230000000873 masking effect Effects 0.000 description 5
- 238000000137 annealing Methods 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 230000008602 contraction Effects 0.000 description 3
- 238000002425 crystallisation Methods 0.000 description 3
- 230000008025 crystallization Effects 0.000 description 3
- 238000005286 illumination Methods 0.000 description 3
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 3
- 229910052753 mercury Inorganic materials 0.000 description 3
- 238000012546 transfer Methods 0.000 description 3
- 238000004458 analytical method Methods 0.000 description 2
- 230000003796 beauty Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- NIHNNTQXNPWCJQ-UHFFFAOYSA-N fluorene Chemical compound C1=CC=C2CC3=CC=CC=C3C2=C1 NIHNNTQXNPWCJQ-UHFFFAOYSA-N 0.000 description 2
- 238000005499 laser crystallization Methods 0.000 description 2
- 238000001459 lithography Methods 0.000 description 2
- 239000011148 porous material Substances 0.000 description 2
- 206010011469 Crying Diseases 0.000 description 1
- 238000011387 Li's method Methods 0.000 description 1
- 241001494479 Pecora Species 0.000 description 1
- 235000009827 Prunus armeniaca Nutrition 0.000 description 1
- 244000018633 Prunus armeniaca Species 0.000 description 1
- 230000033228 biological regulation Effects 0.000 description 1
- 238000005266 casting Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
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- 230000007547 defect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 235000013399 edible fruits Nutrition 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000012634 optical imaging Methods 0.000 description 1
- 230000005693 optoelectronics Effects 0.000 description 1
- 238000000059 patterning Methods 0.000 description 1
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- 230000004044 response Effects 0.000 description 1
- 229910052702 rhenium Inorganic materials 0.000 description 1
- WUAPFZMCVAUBPE-UHFFFAOYSA-N rhenium atom Chemical compound [Re] WUAPFZMCVAUBPE-UHFFFAOYSA-N 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
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Classifications
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70058—Mask illumination systems
- G03F7/70075—Homogenization of illumination intensity in the mask plane by using an integrator, e.g. fly's eye lens, facet mirror or glass rod, by using a diffusing optical element or by beam deflection
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70216—Mask projection systems
- G03F7/703—Non-planar pattern areas or non-planar masks, e.g. curved masks or substrates
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70691—Handling of masks or workpieces
- G03F7/70791—Large workpieces, e.g. glass substrates for flat panel displays or solar panels
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Life Sciences & Earth Sciences (AREA)
- Sustainable Development (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Optics & Photonics (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
Abstract
Description
200415793200415793
五、發明說明(l) 發明背景 發明關於在一« -χΐι ^Λ- Li . ? 裝置, 板以用 半 圖案化 化係利 根 光卩且劑 層予以 或沉積 晶體於 曝光, 光圖案 以形成 像)〇 ^先敏材料上曝光一特定圖案之方法及 符別關於在一呈右綠儿广> 於·f^曰w /、有、笑化厚度之基板如典型之玻璃基 於L C D ( /夜晶顯示哭)室 導體基板中使用::璃之其V反上曝光之方法。V. Description of the invention (l) Background of the invention The invention relates to a «-χΐι ^ Λ- Li. · Device, which uses a semi-patterning system to lighten the photoresist and deposits or deposits a crystal on the exposure layer. The light pattern forms an image. ) ○ ^ Method and symbol for exposing a specific pattern on a sensitive material About a right-angled green > Yu f ^ y w /, with a thickness of a substrate such as a typical glass based on LCD (/ night Crystal display crying) used in the chamber conductor substrate :: Li's method of reverse exposure of V.
V 及堆疊許多材料如如液晶顯示器等係由 用微影技術 ¥體層,絕緣層等形成。圖案 據微影技術,一綠也Rn μ , 0,, 種先阻劑加於待處理之材料以構成 i除層(λ面)上形成,光阻 選m f u /以顯影,處理,如钱刻 是形成:曝逛左側)’-電路,-電 鏡投影Λ光笨^ ^法為杈影曝光,如透鏡投影 )投:上/ 此曝光方法,光罩之影像(曝 對應7光阻:理物件之表面,光阻層即加於其上, " i上曝光圖案之影像(形成曝光圖案之影 第U圖$,置:t t重硬法及分步掃描法久已知义 M以自光源1〇 掃描法曝光装置之結構。—拍 影像由投:4及如、明系統1 〇 2之光束輕照耖,掩罩Μ圖等V and stacking many materials such as liquid crystal displays are formed by using lithography technology, bulk layers, insulation layers, etc. According to the lithography technology, a green also Rn μ, 0 ,, a kind of pre-resistance is added to the material to be processed to form the i removal layer (λ surface), and the photoresist is selected by mfu / for development and processing, such as money engraving It is formed: exposure on the left side) '-circuit,-electron microscope projection Λ light stupid ^ ^ method is exposure of shadows, such as lens projection) cast: up / this exposure method, the image of the photomask (exposure corresponds to 7 photoresistors: physical objects On the surface, a photoresist layer is added thereon, and the image of the exposure pattern on the image (the image forming the exposure pattern is shown in FIG. U). Set: tt hardening method and step scanning method have been known for a long time. 〇 The structure of the scanning exposure device. — The image is shot by the light beam of 4 and Ru, Ming system 1 〇 2 light, illuminate, etc.
因此,稱為瞧朵具f夕直二級以同向移動。 後在分步及掃描震置;曝光、。一區與基板3相對被掃描’Therefore, it is said that the duo has two straight movements in the same direction. After the step and scan set; exposure ,. A region is scanned relative to the substrate 3 ’
200415793 五、發明說明(2) 傻椹^ :曝光中,投影機之焦[即投影曝光形成之$ 阻表面)。 、/、自投衫為至曝光表面之距離相等(光 面層::伏2 I :表面:即曝光表面有微小波浪。光阻表 ## 4·’、 阻宫形成其上之基板厚度之不平,美;^ 之黏接丄基板置於該級之不平所引起。 +基板 制i LCD面使用:夕基板作為半導體技術方面之處理材料。去 Ρ二與# ^ I於日本專利申請公開號碼20 0 1 —3 6 0 88,當 二:Γΐΐ板在厚度上有一特性分布1-方面,“ 之貝她未考慮玻離基板表面之固有波浪。 〗、九 之*光之解析度(線寬度)R及D0F (焦點深度)可由下式表 D〇F=+/-K2/K!2XR2/X (1) 稱程=代表曝光波長’⑽2為係數’視程序而定,亦 當貫施曝光時,基板表面之全曝光場必須在公 =應範圍内。如基板表面不在D0F範圍,無) 影像或撕法形成適當之光阻圖案。 、王 在液晶顯示器製造中使用之大量生產之曝光裝置中 在超高壓水銀燈之丨線之最大解析度為15um。此時,Z組 析度為R = l. Sum,曝光波長為;線),κι^ = 0.5(K1及K2之值在I線使用時),公式(1) tD〇F = = +厂· 8. 6um,D0F之範圍為17· 2um。D0F寬度之一半,即需要 200415793200415793 V. Description of the invention (2) Silly ^: In exposure, the focus of the projector [that is, the $ resist surface formed by the projection exposure]. The distance from the self-casting shirt to the exposed surface is equal (Glossy layer :: Volt 2 I: Surface: That is, there is a small wave on the exposed surface. Photoresistance meter ## 4 · ', the thickness of the substrate on which the resistance palace forms Unevenness, beauty; ^ caused by the adhesion of the substrate placed in this level of unevenness. + Substrate made i LCD surface use: Yu substrate as a semiconductor technology processing materials. P2 and # ^ I in Japanese Patent Application Publication Number 20 0 1 —3 6 0 88, when two: Γΐΐ plate has a characteristic distribution in the thickness of 1-side, "Zhe she did not consider the inherent wave of the glass surface off the substrate.", The resolution of the light (line width ) R and D0F (focus depth) can be expressed by the following formula: D0F = + /-K2 / K! 2XR2 / X (1) Weighing range = Representation exposure wavelength '⑽2 is a coefficient' depends on the program, and it should also be used for continuous exposure At this time, the full exposure field on the substrate surface must be within the common range. If the substrate surface is not in the D0F range, there is no image or tearing method to form an appropriate photoresist pattern. Wang, a mass-produced exposure device used in the manufacture of liquid crystal displays The maximum resolution of the line of the medium and high pressure mercury lamp is 15um. At this time, the Z group analysis R = l. Sum, exposure wavelength is; line), κι ^ = 0.5 (the values of K1 and K2 are used on the I line), formula (1) tD〇F = = + factory · 8. 6um, D0F range 17.2um. One half of the width of D0F, that is, 200415793
第11頁 200415793Page 11 200415793
同時’日本專利申請公開 一方法在玻璃基板之全表面上 玻璃基板具有大化之厚度。根 如歪曲π ,"波浪,,等可能發生 向。經由使拉出方向對應弓形 光’隨後沿掃描方向實施自動 甚小時亦可維持。 但’本發明人經分析結果 在對角線方向較玻璃基在製造 拉出方向之變化較小。 此外,該文件未指出自動 厚度變化之玻璃基板之均勻曝 本發明概述 本發明之目的為提供一曝 大規尺寸液晶顯示裝置中使用 圖案。 根據本發明之一特性,備 圖案,而繼續或隨後將待曝光 該方法包含沿在基板之曝光表 光區域。 根據本發明另一特性,備 曝光基板曝光表面之位移之機 續或隨後移除基板上之曝光區 以沿波浪方向移動一曝光區域 文件號碼2 0 0 1 - 3 6 0 8 8已建今義 實施D0F範圍内之曝光,該 據該文件,厚度之變化 在製造日τ玻璃基板之拉出方 裂口之掃描方向及實施曝 聚焦,焦點邊際甚至在d〇f 證實,玻璃基板之厚度變化 拉出方向為大’及厚度在 聚焦方法,及未建立具有大 光。 光方法及裝置以確實形成供 之玻璃基板之全面積上形成 有一曝光方法以曝光一預定 之基板上一曝光區域移除。 面上存在之波浪方向移除曝 有一曝光裝置包含一偵測待 構,以曝光一預定圖案而連 域。該裝置尚包含一機構用 ’該波浪存在於基板之曝光At the same time, "Japanese Patent Application Publication" discloses a method in which the glass substrate has an enlarged thickness on the entire surface of the glass substrate. Such as distortion of π, " waves, etc., may occur. It can be maintained even when the pull-out direction corresponds to the bow-shaped light 'and then the auto-direction is performed in the scanning direction. However, according to the analysis result of the present inventor, the change in the diagonal direction is smaller than that in the glass substrate in the pull-out direction. In addition, this document does not indicate uniform exposure of glass substrates with automatic thickness change. SUMMARY OF THE INVENTION The object of the present invention is to provide a pattern for use in large-size liquid crystal display devices. According to a feature of the present invention, a pattern is prepared while continuing or subsequently to be exposed. The method includes exposing a light region on a substrate along an exposed surface. According to another characteristic of the present invention, the machine for preparing the exposure of the exposed surface of the substrate is continued or the exposure area on the substrate is subsequently removed to move an exposure area along the wave direction. File number 2 0 0 1-3 6 0 8 8 The exposure within the range of D0F is implemented. According to the document, the thickness changes in the scanning direction of the glass substrate's pull-out square slit on the manufacturing date and the exposure focus is implemented. The focus margin is even confirmed at dof, the thickness change of the glass substrate is pulled out. The orientation is large 'and the thickness is in the focusing method, and is not established with large light. The light method and apparatus are formed over the entire area of the glass substrate that is actually formed. An exposure method is used to expose a predetermined area of the substrate and remove an exposed area. The wave direction existing on the surface is removed and exposed. An exposure device includes a detection structure to expose a predetermined pattern in a field. The device still includes a mechanism for the exposure of the wave existing on the substrate
第12頁 200415793 五、發明說明(5) 表面上。 根據本發 在一曝光時間 明之另一特性 或隨後待曝光 置用以沿特定 大量發生。 明之另一特性 括偵測裝置用 保留裝置,其 之方向以直角 在消除偵測裝 寺空制裝置以控 明另一特性, 之曝光 構以便 一裝置 案而隨 出之位 向移動 厚度變 根 裝置, 裝置包 變化在 根 物件。 度不均 供之表 置之四 移,及 量 ° 本 可自說 優點可 以 明本發 在待曝 用以控 後移動 移,以 曝光區 化,可 據本發 並繼續 括一裝 該方向 據本發 裝置包 勻處, 面延伸 個角落 包含一 發明之 明變為 由各裝 下所附 明之較 光基板 制基板 該基板 控制基 域,在 目檩及 日月_或 I及以 _式併 #實施 表面之 之一曝 板表面 該方向 備有一 表面偵 傾斜及 光區域 之傾斜 中造成 之任何 ,備有 之基板 方向移 曝光裝置, 出曝光表面 高度,以曝 。該裝置尚 及高度,及 表面實質上 時間發生。 一曝光預定 上移動一曝 動曝光區域 ,備有一裝置以處 一偵測物件表面上 中複數個位移機構 交叉之方向位移, 置债出之位移之方 制支撐機構之保留 其包含一機 之位移’及 光一預定圖 包含根據偵 沿一特定方 對應基板之 圖案之曝光 光區域。該 ,基板厚度 理一級上之 之波浪或厚 可在物件提 至少保留裝 向獨立位 裝置之運動 優點將揭示於以下之說明中’部分將 貝施本發明而學習。本發明之目標及 下指出之裝置之組合實現及獲得。 入及構成本說明書之一部分,用以說 例’與以上所提之一般說明及以下交Page 12 200415793 V. Description of the invention (5) On the surface. According to another characteristic of the present invention at an exposure time or subsequent exposure to be set to occur along a specific mass. Another feature of the Ming Dynasty includes the retention device for the detection device. Its direction is at a right angle to eliminate the detection device. The empty device is installed to control the other characteristic. The exposure structure is designed to change the thickness of the device as it moves. Device, device package changes in the root object. The degree of unevenness of the table is set to four shifts, and the amount of ° can be said that the advantages can be explained that the hair will be moved after the exposure to control, to expose the area, according to the hair and continue to include a direction data The hair device has a uniform package, and the corners of the surface extension include an invention. The substrate is controlled by the lighter substrate made of the attached substrate. The substrate control base area is combined with the _ or I and _ types. #One of the implementation surfaces One of the surface of the exposure board is provided with a surface detection tilt and any inclination of the light area in the direction. A substrate direction shift exposure device is provided to expose the height of the exposure surface to expose. The device reaches height, and the surface takes substantially time to occur. An exposure is scheduled to move and an exposure exposure area is provided. A device is provided to detect the displacement of a plurality of displacement mechanisms on the surface of an object in the direction of the intersection. 'Heguang-predetermined map contains exposed light areas based on a pattern corresponding to a substrate along a specific side. The wavy or thick level of the substrate thickness can be lifted on the object and at least the movement of the device to the independent position can be preserved. The advantages will be disclosed in the following description. The section will teach the present invention. The object of the present invention is achieved and obtained by a combination of the devices indicated below. Enter and constitute a part of this specification, for the purpose of example 'and the general description mentioned above and the following
第13頁 光源1 1為高壓水銀燈或雷射裝置輸出曝光用之能量。 高壓水銀燈放射g-線( 43 6nm)或I-線( 3 6 5nm)。該雷射裝置 可為一 XeCL激勵雷射裝置( 3 0 8nm),KrF激勵雷射裝置t 200415793 五、發明說明(6) 叉實施例之詳細說明用以解釋本發明之原理。 本發明詳細說明 本發明之特性將參考以下圖式予以說明。 第1圖顯示一曝光裝置之結構之一例,該裝置能在一 物件之曝光表面上根據本發明將波浪或厚度不平均之影響 移除。 一曝光裝置1包括一照明光系統1 2,一掩罩台丨3,一 影像光學系統1 4及一基板台1 5,彼等隨後安排在光源1 1之 光軸中。一掩罩Μ安排在掩罩台13上,及一玻璃基板s安排 在基板台1 5上。 ( 248nm),ArF激勵雷射裝置(I93nm)等。 一光學系統6包括一照明光系統12,一中繼透鏡,掩 罩Μ及影像光學系統1 4備於光源丨丨放射之光路徑中。一 曝光之基板或液晶顯示裝置之玻璃基板s配置在影 系統1 4之影像聚焦位置。玻璃基板s及掩 予 供。掩罩Μ配置在掩罩臺13上之預定'此成-軛' 要外士 > 暴板量1 5上之預定位 置’心在預定方向Μ之相同方向線性運 板堂1 5上之玻璃基板S之曝光表面之歪攸,、里置' ; 件偵測器10偵測曝光表面之歪曲條 條件’ 一歪曲條 機。一CPU71由匯流排9連接至歪曲,1X1)…像 1本件偵測器1 0,其構?Page 13 The light source 11 is the energy used by the high-pressure mercury lamp or laser device to output exposure. The high-pressure mercury lamp emits g-rays (43 6nm) or I-rays (365 nm). The laser device may be an XeCL-excitation laser device (308 nm), and a KrF-excitation laser device t 200415793 V. Description of the invention (6) The detailed description of the fork embodiment is used to explain the principle of the present invention. Detailed description of the present invention The characteristics of the present invention will be described with reference to the following drawings. Fig. 1 shows an example of the structure of an exposure device capable of removing the influence of wave or uneven thickness on the exposed surface of an object according to the present invention. An exposure device 1 includes an illumination light system 12, a mask stage 3, an image optical system 14, and a substrate stage 15, which are then arranged in the optical axis of the light source 11 1. A mask M is arranged on the mask table 13 and a glass substrate s is arranged on the substrate table 15. (248nm), ArF excitation laser device (I93nm), etc. An optical system 6 includes an illumination light system 12, a relay lens, a mask M, and an image optical system 14 in a light path radiated from a light source. An exposed substrate or a glass substrate s of the liquid crystal display device is arranged at an image focusing position of the shadow system 14. Glass substrates and masks are provided. The mask 'M' is arranged on the mask table 13 at a predetermined 'this formation-yoke' to a foreigner > at a predetermined position on the plate amount 15, the glass is linearly transported on the board 15 in the same direction as the predetermined direction M The distortion of the exposed surface of the substrate S is placed inside; the piece detector 10 detects the distortion condition of the exposed surface. A CPU71 is connected to the distortion by the bus 9, 1X1) ... like 1 this detector 10, its structure?
200415793 五 '發明說明(7) 可控制歪曲條件偵測器丨〇之測量作業,以測量曝光表面之 歪曲條件。CPU71儲存不平資料於記憶體裝置中RAM72,該 裝置以來自歪曲條件偵測器丨〇之測量結果及玻璃基板S之 位置食訊與匯流排9連接。C P U 7 1之該控制程式預先儲存在 連接至匯流排9之記憶體裝置iR〇M73中。 曝光區域決定部分7 4之掃描方向決定與波浪資訊相關 之曝光區域E之曝光區域e及掃描方向資訊丨,該資訊係自 RjM 72根據CPU 7 1控制之歪曲條件偵測器丨〇之測量結果所 ^取。CPU 71可使RAM 72儲存位置資訊相關之資訊。cpu = 置76連接至匯流排9,以顯示與位置資訊相關 =士:域之曝光區域資訊Ε及掃描方向資tfu,及 不 < 貝訊。 自光源1 1之光束由日、召明朵與么 罩Μ之光學圖案影像由影像光子加於掩上’掩 成。在曝光時間,CPU 71同步在玻璃基板S上形 箭頭A方θϊ 夕動掩罩台13及基板台15於 刖頭A万向,及決疋曝光位置。 影像反麵,- △ ,、,士 c: 如衫像光學系統1 4形成之 〜傢夂轉,一台以相反方向移動。 方向移動。 々其係直立,二台以同 掩罩台13及基板台η為八 A之方向移動,CPU 制在曝描計射’可以箭頭 相關稱為曝光區域(場)f之某、置1,掃描與玻璃基板S 業。 Μ ασ ’及執行曝光步驟之作 剖面明光學系統1 2自曝 掩罩台13及基板台15 自光源1 1之光束形狀具有矩形 光區域貢訊所得,並加至掩罩Μ上200415793 5 'Invention description (7) The measurement operation of the distortion condition detector 丨 〇 can be controlled to measure the distortion condition of the exposed surface. The CPU 71 stores the unevenness data in the RAM 72 in the memory device, and the device is connected to the bus 9 with the measurement result from the distortion condition detector 丨 0 and the position of the glass substrate S. The control program of C P U 7 1 is stored in advance in a memory device iROM 73 connected to the bus 9. The scanning direction of the exposure area determination section 74 determines the exposure area e and the scanning direction information of the exposure area E related to the wave information. This information is from the measurement results of the distortion condition detector 丨 0 controlled by RjM 72 according to the CPU 71. ^ 取。 Taken. The CPU 71 may cause the RAM 72 to store information related to the position information. cpu = set 76 is connected to bus 9 to display the location information related = taxi: exposure area information E and scanning direction information tfu of the domain, and not < Beixun. The light beam from the light source 11 is masked by the optical pattern image of the sun, Zhaomingduo, and Ma. During the exposure time, the CPU 71 synchronously shapes an arrow A on the glass substrate S, and moves the mask stage 13 and the substrate stage 15 at the head A, and determines the exposure position. On the reverse side of the image,-△ ,,, and c: If the shirt-like optical system 14 is formed, the furniture is turned, and one moves in the opposite direction. Move in the direction. 々It is upright. The two units move in the same direction as the mask stage 13 and the substrate stage η. The CPU controls the exposure meter. The arrow can be referred to as the exposure area (field) f. Set 1 and scan. With glass substrate S industry. Μ ασ ′ and the work of performing the exposure step, the profile optical system 1 2 is self-exposed, the mask stage 13 and the substrate stage 15 are obtained from the light source 11 with a rectangular light region, and are added to the mask M.
第15頁 200415793 五、發明說明(8) ΐ自;tfl:·安描方向資訊1以予定之時間同時移動。因 掩罩Μ之圖木曝光在玻璃基板§上。當第i圖中之曝光 衣置1中之影旱光學系統i 4將掩罩圖案反向日寺 及基板台15在曝光時間,彼此以相反方向移動。此外,玻 之厚度變化大之方向與掩罩台13及基 動方向平行。 μ 1 fi基=I丨5較佺包括傾斜機構。基板1 5由一稱為傾斜機 韻之制動器所支標,其有四個壓電元件其上有四角落, 母一凡件之投影量(高度)可各別控制。 一 J言之,基板台15可以直角交叉之任-方向傾斜-預 疋2:1平面區之延伸方向(投影平面)或與此等方向相關 之㈣線方向(傾斜)。此外,基板15可與投影平面平行i =m直》動)。傾斜及垂直移動可由控制裝置同時控 制’揭後再說明。 曝光裝置1亦包括一傾斜偵測機構以測量基板s上曝光 m之立私傾斜偵測機構包括一半導體雷射裝置1 8,里 光源、’一PSD(位置敏感裝置)2。以偵測反射光。玻璃、 Γ+ ΐ =位移方向及位移量可利用半導體雷射裝置18之雷 夕θ以3一角度射至基板S之表面,接收在玻璃基板S上 屮。與ϋ II之反射光束R,卩由PSD 2(3偵出反射光束R而測 二4焦位置可自輪出至二電極以拾取PSD 20之信號 值而獲得。因此,玻璃基板s之位移方向及位移 里可自SD 20之電中央位置之方向及距離獲得。 PSD 20之輸出電流係由A/D轉換器之a/d(未示出)。例Page 15 200415793 V. Description of the invention (8) ΐ Since; tfl: · Ansing direction information 1 moves simultaneously at a predetermined time. Because the mask M is exposed on the glass substrate§. When the exposure optical system i 4 in the exposure set 1 in the figure i reverses the mask pattern to the temple and substrate stage 15 during the exposure time, they move in opposite directions to each other. In addition, the direction in which the thickness of the glass changes greatly is parallel to the mask stage 13 and the base movement direction. The μ 1 fi base = I 丨 5 includes a tilt mechanism. The base plate 15 is supported by a brake called a tilting machine. It has four piezoelectric elements with four corners on it. The projection amount (height) of a female component can be controlled individually. In other words, the substrate stage 15 can be crossed at any angle in a right-angle direction-preliminary extension direction (projection plane) of the 2: 1 plane area or a ray line direction (tilt) related to these directions. In addition, the substrate 15 may move parallel to the projection plane (i = m). The tilt and vertical movement can be controlled by the control device at the same time. The exposure device 1 also includes a tilt detection mechanism to measure the exposure m on the substrate s. The private tilt detection mechanism includes a semiconductor laser device 18, a light source, and a 'PSD (position sensitive device) 2. To detect reflected light. Glass, Γ + ΐ = displacement direction and displacement amount can be shot on the surface of the substrate S at an angle of 3 using the laser beam θ of the semiconductor laser device 18 and received on the glass substrate S 屮. The reflected beam R and 卩 of II are detected by PSD 2 (3, the reflected beam R is detected, and the 2 and 4 focal positions can be obtained from the wheel to the two electrodes to pick up the signal value of PSD 20. Therefore, the displacement direction of the glass substrate s And the displacement can be obtained from the direction and distance of the electric central position of SD 20. The output current of PSD 20 is a / d (not shown) of the A / D converter.
200415793 五、發明說明(9) 如,其係第11圖所示之控制裝置(電腦)21 存於控制裝置或外部之記情酽中 輸入^後儲 分布(波浪或厚度不均)可在‘美後,曝光表面之位移 面積,或波浪及不平甚大二之投影平面之所有 均已獲得後獲得。在基板表:力方Π所有部分(曝光場) 光功率比較具有足夠小之光為/源時,與曝 圍不同。因此,即使光阻材光波長之波長範 ^ 材科加在玻璃基板s之表面,弁 阻材料不能曝光於光中。 十:=:f位移分布加在-近似直線上,例如以最小 二乘方方法靶加,&直線之傾斜及所有位移之平均高产加 以計异,此點將於第12圖中解釋。因此,壓電 = 展及收縮之方向及*’其作為制動器16在四角落得以;申 算有”伸展及收縮方向及量之極性及強度之 出至母一壓笔元件(制動器)16。結果,此一傾斜變 為"〇"及所有位移之平均高度與影像光學系統14200415793 V. Description of the invention (9) For example, it is the control device (computer) shown in Figure 11 21 It can be stored in the control device or external memory card. ^ After storage distribution (wave or uneven thickness) can be entered in ' After the beauty, all the displacement areas of the exposed surface, or the projection planes of waves and unevenness, are obtained. In the substrate table: the power of all parts (exposure field) is relatively different from the exposure when the light power is sufficiently small for the light source / source. Therefore, even if the wavelength range of the light wavelength of the photoresist material is added to the surface of the glass substrate s, the photoresist material cannot be exposed to light. Ten: =: f displacement distribution is added to-approximate line, such as target addition using the least squares method, & the slope of the straight line and the average high yield of all displacements plus the difference, this point will be explained in Figure 12. Therefore, the piezoelectricity = the direction of expansion and contraction and * 'can be used as the brake 16 in the four corners; the extension and contraction direction and amount of polarity and strength are calculated to the female one pen element (the brake) 16. Result , This tilt becomes " 〇 " and the average height of all displacements and the image optical system 14
焦表面之高度重合。 〜像I 其次,本發明之曝裝置1作業說明於下。 前 有一相同咼度。該校正值由原始偵測作業中設定,其 量裝置之技術範圍甚為知名,其細節予以省略。 在曝光%中之位移及掃描曝光之測量予以重復,並同 時與影像光學系統1 4相對移動掩罩臺丨3及基板臺丨5。一原 始電壓加在壓電元件1 6,在配置玻璃基板3與基板臺丨5之 設定,ον(或預先獲得之校正值),以使所有制動器uThe heights of the focal surfaces coincide. ~ Image I Next, the operation of the exposure device 1 of the present invention is described below. The front has the same degree. The correction value is set in the original detection operation. The technical range of the measuring device is well known, and its details are omitted. The measurement of the displacement in the exposure% and the scanning exposure are repeated, and the mask stage 丨 3 and the substrate stage 丨 5 are moved relative to the image optical system 14 at the same time. An initial voltage is applied to the piezoelectric element 16 and the setting of the glass substrate 3 and the substrate table 5 is arranged. Ον (or a correction value obtained in advance) so that all the brakes u
第17頁 200415793 五、發明說明(10) 其次,在曝光場中之每一複數個位置之位移,利用 導體雷射1 8之雷射光束L加在玻璃基板S之曝光表面予fPage 17 200415793 V. Description of the invention (10) Secondly, the laser beam L of the conductor laser 18 is applied to the exposure surface of the glass substrate S at the displacement of each plural positions in the exposure field to f
量。 /貝J 隨後,玻璃基板S以預定角傾斜於與直角交又之任立 方向’平面面積之延伸方向(投影平面),其由<掩罩M ^ = 曝光圖案所限定’或與此等方向有關之一對角線方向, 3离基板S之高度加以調整以供玻璃基板3之位移中差異破 效降低。高度之傾斜及調整之實施係根據破璃基板Μ 〇有 斜)之曝光表面偵出之位移(波浪)以改正傾斜,及將 玄 板S上下移動以調整玻璃基板s與掩罩Μ間距離(垂直移祝 為更詳細說明,玻璃基板s之曝光表面以 下移動玻璃:板;之^時… 像學系統U影像形成表面之面高度俾重曝合先:…均高度與影 偵測玻:J ίs不之二表面 |一 y子度不十僅能發一the amount. / 贝 J Subsequently, the glass substrate S is inclined at a predetermined angle to an arbitrary direction that intersects with a right angle, the extending direction of the planar area (projection plane), which is defined by < Mask M ^ = exposure pattern 'or the like One of the directions is a diagonal direction, and the height of 3 from the substrate S is adjusted so that the difference in the displacement of the glass substrate 3 is reduced. The implementation of the inclination and adjustment of the height is based on the displacement (wave) detected by the exposed surface of the broken glass substrate (M0 has a slope) to correct the inclination, and the black plate S is moved up and down to adjust the distance between the glass substrate s and the mask M For a more detailed explanation, the moving surface of the glass substrate s is moved below the exposed surface of the glass: plate; at the time ... the height of the surface of the image formation surface of the imaging system U is heavily exposed before: ... the average height and the shadow detection glass: J ίs not the two surface | A y child is not ten can only send one
之縱向,不發生在基板3 ° σ,玻璃基板S 平實際上為一維如第2 1 特性1波浪及厚度不 方法之結果。 ΰ及弟3圖所不,係由破璃基板製造 偵測波浪或厚度轡介少女i Α R之外,亦可利用弁4方法,除利用上述之反射光束 j j扪用先干涉或感測筆。 第18頁 415793 五、發明說明(11) __ 根據上述之、、卩丨丨 曝光表面,接收由J心ΐ及以雷射光束[輻照基板3之 等,基板s之波,、纟:二、.、°果產生之反射光束及處理信號 聚焦位移感測哭或:睡測及厚度不平之位移量可利用雷射 至於焦點;J,商二)而,ί。·1㈣之精確度。 曝光場f掃描之真日士門—夕/里及基板台之15控制較佳根據 波浪可在曝光前^間貫化1,玻璃基板S之全表面上之 施。 日守間測I,及控制可根據測量結果實 ^ 3 ^ P *光已^明如上。但本發明之曝光方法不限於f 景》曝光亦可靡用Α οη λ 1 。7広个丨良於才又 優點自^ 王心照像術技術。此外,特別大之 2明之曝光方法獲得,在分步及 步及_由2 $貝^曝先。但本發明亦可應用於分 光重“射,其可使曝光場在固定位置靜止時實施曝 玻璃基板被稱為典型基板 大變化,但基板並不受限於此 相似特性時,其可用於本發明 第2圖顯示玻璃基板s厚度 之分布)。 ’其具有在一方向厚度之較 。例如,如一塑料基板具有 之曝光方法中。 之測量值之一例(厚度不平The longitudinal direction does not occur at the substrate 3 ° σ, and the glass substrate S plane is actually a one-dimensional result such as the 2 1 characteristic 1 wave and thickness. As shown in Figure 3 and Figure 3, the detection of waves or thickness is made by a broken glass substrate. In addition to the girl i Α R, you can also use the 4 method. In addition to using the reflected beam jj above, use the interference or sensing pen first. . Page 18 415793 V. Description of the invention (11) __ According to the above, 卩 丨 丨 exposes the surface, and receives the laser beam [by irradiating the substrate 3 and the like, the wave of the substrate s], and The reflected light beam and processing signal generated by the fruit, focus displacement sensing, or: the displacement of sleep measurement and thickness unevenness can be focused by laser; J, Shang II) and ί. · Accuracy of 1㈣. Exposure field f-scanning of the real Shimen-Xi / Li and 15 of the substrate table is preferably controlled according to the wave 1 before the exposure, and is applied on the entire surface of the glass substrate S. Day-to-day measurement I, and the control can be based on the measurement results ^ 3 ^ P * The light has been illuminated as above. However, the exposure method of the present invention is not limited to f scene. Exposure can also be used Α οη λ 1. 7 丨 good and good advantages from ^ Wang Xin imaging technology. In addition, a particularly large exposure method of 2 Ming is obtained in step and step and _ exposed by 2 $ 贝 ^. However, the present invention can also be applied to spectroscopic re-emission, which can make the exposure of the glass substrate when the exposure field is stationary at a fixed position is called a large change of a typical substrate. The second figure of the invention shows the distribution of the thickness of the glass substrate s.) 'It has a thickness comparison in one direction. For example, as in the exposure method of a plastic substrate. An example of the measured value (uneven thickness)
旦具有平均厚度〇.7顏之玻璃基板厚度在一特別方向測 里。大約10um之變化(峰至峰)在1〇〇 —2〇〇mm之循環中可以 ^到。厚度中之變化方向已顯示,但,已經證實在以直角 父又之方向中甚難見到變化。亦經證實,當破璃基板s置 於臺15上時,#度中之變化實質上被反射,及玻璃基板表The thickness of a glass substrate having an average thickness of 0.7 is measured in a particular direction. A change (peak-to-peak) of about 10um can be achieved in a cycle of 100-200mm. The direction of change in thickness has been shown, but it has been confirmed that it is very difficult to see the change in the direction of the right angle father. It has also been confirmed that when the broken glass substrate s is placed on the stage 15, changes in #degrees are substantially reflected, and the glass substrate surface
第19頁 200415793 五、發明說明(12) 面之位移(波浪)亦可出現如第3圖所說明。在玻璃基板$之 曝光表面厚度變化之方向大量出現在以X代表方向,該方 向中厚度貫質上為平均之方向以γ代表,位移之軸以Z代 表。 生產玻離基板有熔解及浮動方法。已經證實二計割均 有相同特性。在此計劃中,具有實際上不變厚度之玻璃基 板,可利用在熔解狀態時拉出玻璃材料而獲得。但已知顯 示大厚度變化之方向為製造玻璃時,與拉出玻璃材料之方 向成直角交叉。換言之,Y方向為製造玻璃基板時拉出玻 璃材料之方向。 弟4 A圖及弟4 B圖說明曝光场中掃描方向與位移間之關 係差。第4A圖中,掃描方向,矩形之曝光場之縱向以一方 向延長與第3圖中之X方向平行。第4B圖中,掃描方向,即 矩形之曝光場之縱向延一方向延伸與第3圖中之γ方向平 行。此等方向與第5圖,第6圖中之關係對應,稍後說明。 因此,如玻璃基板S利用有相同面積之矩形曝光場曝 光日可’位移差d如第4 B圖中沿X方向安排之短側b時,則較 弟4 A圖中沿X方向安排之長側&為短。換言之,破璃美板之 厚度分布特性或導自厚度分布之玻璃基板S之曝光表面之 位移加以考慮時,則與第6圖之方法對應之方法,即沿χ方 向女排短側b,及在X方向描,在D 0 F之觀點下甚為停異。 第7圖說明在第6圖之方向曝光之破璃基板8之波動及 厚度不平與曝光場間之關係。 自第7圖可知,傾斜及垂直移動之實施可使曝光場f經Page 19 200415793 V. Description of the invention (12) The displacement (wave) of the surface can also appear as illustrated in Figure 3. The direction of the change in the thickness of the exposed surface of the glass substrate $ appears largely in the direction represented by X, the direction in which the thickness is uniform throughout is represented by γ, and the axis of displacement is represented by Z. There are melting and floating methods for the production of glass substrates. It has been confirmed that the two meter cuts have the same characteristics. In this plan, a glass substrate with a virtually constant thickness can be obtained by pulling out the glass material while in the molten state. However, it is known that the direction showing a large thickness change is that when the glass is manufactured, it crosses at right angles to the direction in which the glass material is pulled out. In other words, the Y direction is the direction in which the glass material is pulled out when the glass substrate is manufactured. Figure 4A and Figure 4B illustrate the difference between the scanning direction and displacement in the exposure field. In Fig. 4A, in the scanning direction, the longitudinal direction of the rectangular exposure field is extended in one direction and parallel to the X direction in Fig. 3. In Fig. 4B, the scanning direction, that is, the longitudinal extension of the rectangular exposure field extends in one direction parallel to the γ direction in Fig. 3. These directions correspond to the relationships in Figs. 5 and 6, which will be described later. Therefore, if the glass substrate S uses a rectangular exposure field with the same area, the exposure date can be shifted d. As shown in Figure 4B, the short side b arranged in the X direction is longer than that arranged in the X direction in Figure 4A. Side & is short. In other words, when considering the thickness distribution characteristics of the broken glass board or the displacement of the exposed surface of the glass substrate S derived from the thickness distribution, the method corresponding to the method of FIG. X-direction tracing is very different from the viewpoint of D 0 F. Fig. 7 illustrates the relationship between fluctuations and thickness irregularities of the broken glass substrate 8 exposed in the direction of Fig. 6 and the exposure field. As can be seen from Figure 7, the implementation of tilt and vertical movement can make the exposure field f
第20頁 200415793 五、發明說明 常根據位移保柱曰 Μ 日臭杏尸护α /、持取仏本焦,即破璃基板S表面之τ 曝光%知描已吉士 衣向之不平。去 呈Π A、 几成曝先%在與掃描方向交叉少 田 里’y 移動,及再實施相同之掃描(夫-ψ ^方向以定 及步進加以重復以使基板之全声而,此曝 通吊,曝光在步進時不實施。 、曝光。 掩罩台1 3之支撐部分;[7可予以 1 5之制動器1 6。所用之制動器1 6 不私動基板台 可為磁鐵如電螺管等,或為靜電。 第8A圖及第8B圖說明焦點調整 移動,如第4A圖,第4B圖,第5 〜圖、::斜直 解,第8B圖說明之傾斜後獲得 H U。應瞭 傾:f㈣…差d為小。最大 二均/二3:冉圖之水準點’影像光學系統14 之^/像|焦表面即配置在水準點。 第5圖之例中’在掃描矩形曝光射在第6圖之γ方向具 X 20匪尺寸時,位移差之最大值為75um,在掃描 本&明之X方向中矩形曝光場f之最大位移差為4 8隱。因 ί命在一例中,位移之最大值間有明顯之差。當曝光場之 見度(、第6圖)較大時’在一時間之曝光區域範圍擴展,生 產率增加。事貫上,曝光場之形狀及尺寸受到影像光學系 統1 4之透鏡製造限制之限制。 4寸別是,可製造之透鏡之直徑為2〇〇_3〇〇mm,曝光場 之寬度根據曝光波長及解析度約為5〇 —1〇〇mm。Page 20 200415793 V. Description of the invention Often, according to the displacement protection column, the solar odor apricot body protects α /, holding the coke, that is, the τ exposure% of the surface of the broken glass substrate S is known to be uneven. To show Π A, first move %% in Shao-ri, which crosses the scanning direction, and then perform the same scan (Fu-ψ ^ direction is repeated in steps and steps to make the substrate full. Exposure crane, exposure is not carried out during stepping. Exposure. Supporting part of masking table 13; [7 can be used as a brake for 15 5. 16. The used brake 16 can be used as a magnet. Solenoids, etc., or static electricity. Figures 8A and 8B illustrate the focus adjustment movement, such as Figure 4A, Figure 4B, Figures 5 to Figures ::: Straight and straight solution, HU obtained after tilting as shown in Figure 8B. It should be tilted: f㈣ ... the difference d is small. The maximum two averages / two 3: Rantu's level point 'image / image | focus surface of the image optical system 14 is arranged at the level point. In the example of Figure 5' is scanning When the rectangular exposure has X 20 band size in the γ direction of Fig. 6, the maximum value of the displacement difference is 75um, and the maximum displacement difference of the rectangular exposure field f in the scan X direction is 48. In one example, there is a significant difference between the maximum values of the displacement. When the visibility of the exposure field (Figure 6) is large, the exposure at one time The area range is expanded, and productivity is increased. In general, the shape and size of the exposure field are limited by the lens manufacturing limitations of the imaging optical system 14. In addition, the diameter of the lens that can be manufactured is 2000-300mm The width of the exposure field is about 50-100 mm according to the exposure wavelength and resolution.
第21頁 200415793 五、發明說明(14) 應為約5 0 - 1 0 0 m m長,及第7圖所示之曝光場f之短側b之長 度應為弟7圖所示之曝光場f所示之長側a之長度之1/5至 1 / 3。曝光場形狀可為一長形孔隙。但,影像系統丨4所需 之孔隙應具有較高收斂放大,以便有效利用自光源之光 束’光系統變為更為複雜。將曝光場之形狀使為橢圓形亦 屬有效,因光系統之負擔可以減輕。 弟9 A圖及弟9 B圖說明傾斜及垂直移動之一例,其可改 進焦點調整之效應,如第4A圖,第4B圖,第5圖及第6圖所 說明。 第9 A圖說明單軸傾斜之結果(包括垂直移動),其中曝 光場f之旋轉軸r安排在γ方向。第9B圖說明雙軸傾斜及垂 直移動之結果,其中曝光長f之旋轉軸^安排在X方向,及 旋轉軸r2安排在Y方向。此外,第丨〇a圖及第ιοΒ圖說明由 第9 A圖及第9 B圖說明之傾斜獲得之曝光表面之有效變化。 第1 0 A圖中,表面上波浪之分布,及波浪或厚度不平 之幅度’掩罩Μ之圖案由影像光學系統1 4投射在其上,被 限制在2. Oum或更小。位移差之最大值自4· 8um降低至 2 · 0 um,傾斜及垂直移動之焦點調整之效益因此可獲得證 實。 第10B圖中,可證實位移差之最大值與第1〇a圖說明之 條件比較可進一步限制,具有位移差為丨· 〇um或更小之面 積被擴展,位移差之最大值可限制在丨· 9uni。因此,曝光 圖案可在玻璃基板S上利用雙軸傾斜(垂直及傾斜移動)在 破璃基板S之全面積以高度準確曝光,如第9 B圖說明,而Page 21 200415793 V. Description of the invention (14) It should be about 50-100 mm long, and the length of the short side b of the exposure field f shown in Figure 7 should be the exposure field f shown in Figure 7. The length of the long side a shown is 1/5 to 1/3. The shape of the exposure field may be an elongated pore. However, the pores required for the imaging system should have a higher convergence magnification, in order to effectively use the light beam from the light source, and the light system becomes more complicated. It is also effective to make the shape of the exposure field elliptical, because the burden on the light system can be reduced. Brother 9A and Brother 9B illustrate an example of tilt and vertical movement, which can improve the effect of focus adjustment, as illustrated in Figures 4A, 4B, 5 and 6. Figure 9A illustrates the results of uniaxial tilt (including vertical movement), in which the rotation axis r of the exposure field f is arranged in the γ direction. Fig. 9B illustrates the results of the biaxial tilt and vertical movement, in which the rotation axis ^ of the exposure length f is arranged in the X direction, and the rotation axis r2 is arranged in the Y direction. In addition, Figures 丨 〇a and ιοΒ illustrate the effective changes in the exposed surface obtained from the tilt illustrated in Figures 9A and 9B. In FIG. 10A, the distribution of waves on the surface, and the amplitude of the wave or thickness unevenness' masking M is projected thereon by the imaging optical system 14 and is limited to 2. Oum or less. The maximum value of the displacement difference was reduced from 4 · 8um to 2 · 0 um, and the benefits of the focus adjustment of tilt and vertical movement can be verified. In Fig. 10B, it can be confirmed that the maximum value of the displacement difference can be further limited compared with the conditions illustrated in Fig. 10a. The area with a displacement difference of 丨 · um or less is expanded, and the maximum value of the displacement difference can be limited to丨 · 9uni. Therefore, the exposure pattern can be exposed on the glass substrate S with a biaxial tilt (vertical and tilt movement) over the entire area of the broken glass substrate S with high accuracy, as illustrated in FIG. 9B, and
第22頁 200415793 五、發明說明(15) ' --Page 22 200415793 V. Description of Invention (15) '-
不增加玻璃基板S之曝光表面上之波浪之實際準確度所需 者為夕。換5之,通常—高解析度由波浪或厚度不平之妒 響,在最近可購之具有—般平整度之破璃基板s係不可W ,:但,利用本發明具有高解析度之完全光阻圖案可在曝 光表面之全面積獲得。 例,如上所述’基板表面上之 不千可在曝光期間予以改正,以便使曝光之表面在 系統之D0F範圍内。因此,聚焦之表面及曝光之二 大致彼此重合。即使曝光圖案由具有一小D0F曝先^壯 :光’在曝光表面上構成之曝光圖案糢糊及/或失t可以 板上實施,特別是,顯示器等在玻璃基 理之物件)。 〃有較大波動或厚度不平之基板(處 此外’已證貫位移差即平整产 基板方向及掃描方向計彳 ^ 9 ,可由考慮玻璃 仰y U σΤ低至i · 9un]或較 之主旨,及實施水平及番亩 此”、、έ為本發明 差。因此,根據本發明之曝光方法, * ^ ΚΓί?激勵雷射在現有玻璃基板上達成析度0·5·可利用 根據本發明,如上所述,置於A 在特殊方向(即以直角交 、口上之玻祸基板之表面 之方向)有較大變化。因 1,製造時拉出玻璃基板 移差,可在大變化之方,h光場内玻璃基板表面之位 :降低。此外,玻Μ板表暴光場之短側 基板之波浪及以傾斜私可使曝光場對應玻璃 及孟直私動貫施焦點調整而進一步改What is required is not to increase the actual accuracy of the waves on the exposed surface of the glass substrate S. In other words, usually—high resolution is caused by jealousy of waves or uneven thicknesses. Recently, commercially available broken glass substrates with ordinary flatness cannot be used. However, using the present invention, high-resolution complete light The resist pattern can be obtained over the entire area of the exposed surface. For example, as described above, the defects on the substrate surface can be corrected during exposure so that the exposed surface is within the DOF range of the system. Therefore, the focused surface and exposure two are approximately coincident with each other. Even if the exposure pattern is formed by having a small DOF exposure, the exposure pattern formed by the light on the exposure surface may be blurred and / or lost on the surface, especially, glass-based objects such as displays).基板 Substrates with large fluctuations or uneven thicknesses (in addition, the difference of the proven displacement is to flatten the substrate direction and the scanning direction are calculated. ^ 9 can be calculated by considering the glass y U σΤ as low as i · 9un] or less than the purpose, And the implementation level and Fanmu are poor. Therefore, according to the exposure method of the present invention, * ^ ΚΓί? Stimulates the laser to achieve a resolution of 0.5 on the existing glass substrate. According to the present invention, As mentioned above, there is a large change in the special direction (that is, the direction of the surface of the glass substrate on the mouth that intersects at right angles). Because of 1, the glass substrate is pulled out during the manufacturing process, which can be changed in a large way. The position of the surface of the glass substrate in the h-light field: lower. In addition, the waves on the short-side substrate of the exposure field of the glass plate and the tilting can make the exposure field corresponding to the glass and Meng Zhili to adjust the focus and further
第23頁 200415793 五、發明說明(16) 進。 第11圖顯示第1圖中控制裝置2 1之控制系統之方塊 圖。基板裝置21包括輸入埠31,作業部分32,改正量設定 部分3 3,制動器驅動部分(電壓設定部分)3 4,控制部分 CCPU)35,及一記憶體36。在輸入埠31,自PSD 20輪出電 流(由A/D轉換器數位化)在此輸入。作業部分32根據輪入 PSD 20之輸出獲得位移量。改正量設定部分33設定對應作 業部分32所得之位移量之改正量(制動器16)。制動器驅動 口 (3刀3 4根據改正量設定部分3 3之改正量操作制動器1 6。控 制f分(CPU)35控制作業部分32,改正量設定部分33及制 =器驅動部分34之操作。記憶體36儲存作業部分32之作業 結果,即玻璃基板S之波浪或厚度不平或不平分布。一顯 不裝置37經一介面(未示出)需要時連接至控制部分35。 # $2D、2〇之輸出電流係A/D —轉換並由作業部分32操作。 机在控制部分3 5之控制下轉換為改正量。玻璃基板 果,祐t及厚度不平中之方向及位移量可加以計算。結 # p主㈤基板S之曝光表面配置在影像光學系統1 4限定之 技衫表面=D0F以内,如第4B圖中所述。 + - ^ϋ羊細說明’根據波浪方向及位移量設定之每一壓 ::收:收縮之方向及量加嗜,具有對應擴 電元件16 >二里之電壓由電壓設定部分34輸出至每一壓 位於D0F之^圍\及輪出實施後’曝光表面上之所有各點可 在作章部q。1 一 2中,自厚度測量偵感器或PSD 20於每一Page 23 200415793 V. Description of Invention (16). Fig. 11 shows a block diagram of the control system of the control device 21 in Fig. 1. The substrate device 21 includes an input port 31, an operation portion 32, a correction amount setting portion 33, a brake driving portion (voltage setting portion) 34, a control portion CCPU) 35, and a memory 36. At input port 31, the current from the PSD 20 wheels (digitized by the A / D converter) is input here. The operating portion 32 obtains the displacement amount based on the output of the PSD 20 in the turn. The correction amount setting section 33 sets a correction amount (brake 16) corresponding to the displacement amount obtained by the operation section 32. Brake drive port (3 cutters 3 4 Operate the brake 1 6 according to the correction amount of the correction amount setting section 33. Control f-point (CPU) 35 controls the operation section 32, the correction amount setting section 33 and the actuator driving section 34 operation. The memory 36 stores the operation result of the operation portion 32, that is, the wave or thickness of the glass substrate S is uneven or unevenly distributed. A display device 37 is connected to the control portion 35 through an interface (not shown) when needed. # $ 2D 、 2 The output current of 〇 is A / D-converted and operated by the operation section 32. The machine is converted to the correction amount under the control of the control section 35. The direction and displacement of the glass substrate, the thickness t, and the uneven thickness can be calculated.结 # p The exposure surface of the main substrate S is located within the surface of the technical shirt defined by the imaging optical system 14 = D0F, as shown in Figure 4B. +-^ Ϋ Sheep's detailed description according to the wave direction and displacement Each pressure :: close: The direction and amount of shrinkage are added, and the voltage corresponding to the power extension element 16 > Erli is output by the voltage setting section 34 to each pressure located within the range of D0F \ and after the rotation is implemented. All points on the surface can be found in the chapter q. 1 in 2 since the thickness measurement sensor or PSD 20 in each
第24頁 200415793Page 24 200415793
預定期間輸出,並於Y方向移動曝光場,並以預定速度在 第6圖之X方向移動。曝光場中之位移分布(波浪或厚度不 平之方向及位移量)自PSD 20之輸出(A/D轉換)予以計算, 如以下第1 2圖(S 1 1 )所說明。 # 自在SI 1所得之曝光場之位移分布,改正量z之&及!^由 下式代表: Z二 ax+b 由最小二乘方(S12)之線性進似值所規定(平面)。 其杯根/m2所十得之改正量2“,b),*臺15支撑之玻璃 移動之傾斜量及垂直移動量可以獲 件16::=獲= 斜二直移動之量,η 縮量)在臺15上以預定方法對齊、、:δ::量(擴展量/收 (S 1 4 )。 3作業方向可以獲得 每一壓電元件16獲得之作 (擴展量/收縮量)被轉換為極〃、方向(擴展/收縮)及其量 為D/A轉換器之電壓設定部丄’生及大。。小之電壓,以備由作 壓電元件1 6。 制動益驅動部分)3 4供應至 —根據另-線性進似算法,旦 疋,垂直移動量由平均值決+ 、斜里由最大及最小值決 基板S之曝光表面之焦黑疋。 光場之每一範圍均加以控制、、、έ。控制傾斜及/或垂直移動在曝 (真時間)或步進作業期間同萨f =,波浪之偵測可以曝光 _ 了汽知。因為全部波浪不需事 200415793It is output during a predetermined period, and moves the exposure field in the Y direction, and moves in the X direction in FIG. 6 at a predetermined speed. The displacement distribution (direction or amount of wave or thickness unevenness) in the exposure field is calculated from the output (A / D conversion) of the PSD 20, as illustrated in Figure 12 (S 1 1) below. # The displacement distribution of the exposure field obtained from SI 1, & and! ^ Of the correction amount z are represented by the following formula: Z2 ax + b is specified by the linear approximation value of the least square (S12) (plane). The correct amount of the cup root / m2 is 2 ", b), and the tilt and vertical movement of the glass supported by the stage 15 can be obtained. 16 :: = Get = the amount of oblique straight movement, η shrinkage ) Aligned on the stage 15 in a predetermined method, the: δ :: amount (expanded amount / received (S 1 4). 3 working direction can obtain the work (expanded amount / contracted amount) obtained by each piezoelectric element 16 is converted The voltage setting part of the D / A converter is extremely large, the direction (expansion / contraction), and the amount is small and large. The small voltage is prepared for use as a piezoelectric element. 16. The braking benefit driving part) 3 4Supply to—According to another-linear approximation algorithm, once the vertical movement amount is determined by the average +, the slope is determined by the maximum and minimum of the focal surface of the exposed surface of the substrate S. Each range of the light field is controlled, 、、. Control the tilt and / or vertical movement during exposure (real time) or stepping operation f =, the detection of waves can be exposed _ the steam knowledge. Because all the waves do not need to be 200415793
五、發明說明(18) 先偵測,偵測時間可降低。 因此,本發明之曝光裝置中,保留基板之基板臺為獨 立垂直及水平移動,宛如基板之曝光表面可被平整。曝光 圖案因此可在光學影像系統之D0F範圍正確構成於液晶顯 不之玻璃基板上,或具有波浪或厚度不平之基板上,特別 疋k大之厚度不平。換言之,無糢糊之曝光圖案可在基板 表面上或曝光表面上構成。5. Description of the invention (18) Detection first, detection time can be reduced. Therefore, in the exposure apparatus of the present invention, the substrate stage holding the substrate is moved vertically and horizontally independently, as if the exposed surface of the substrate can be flattened. The exposure pattern can therefore be correctly formed on the glass substrate of the liquid crystal display in the DOF range of the optical imaging system, or on a substrate having a wave or uneven thickness, especially the uneven thickness of 疋 k. In other words, the exposure pattern without blurring can be formed on the surface of the substrate or on the exposed surface.
士以上已說明曝光裝置及方法。但本發明亦可應用在處 理衣置如雷射晶體化裝置。應用之不同舉例如下所述。在 應用中處理可不必除聚焦之下實施,而不論基板表面上波 /良之么布’其方法為使基板之曝光表面之相對位置(距 離)’即,由影像光學系統限定之曝光(處理)物件及投影 表面位於影像光學系統之D〇F之範圍内。 第1 3圖顯示結晶化裝置之結構。 二第13圖之結晶化裝置53有一激勵雷射光源52,一掩罩 、口 5 3 ’台驅動部分5 4,基板台5 5,苗光學系統5 6,校正偵 /則部分5 7,基板偵測部分5 8,及控制部分5 9等。 、 激勵雷射光源5 2安排在退火室外(未示出),其產生一 波長;I = 248nm之KrF激勵雷射波束。The exposure device and method have been described above. However, the present invention can also be applied to a processing device such as a laser crystallization device. Examples of different applications are described below. In the application, the processing can be performed without focusing, regardless of the wave / goodness on the substrate surface. The method is to make the relative position (distance) of the exposed surface of the substrate. Objects and projection surfaces are within the DOF range of the imaging optical system. Figure 13 shows the structure of the crystallization device. The crystallization device 53 in FIG. 13 has an excitation laser light source 52, a mask, a port 5 3 ′, a stage driving part 5 4, a substrate stage 5 5, a Miao optical system 5 6, a correction detection / regulation part 5 7, and a substrate. Detection section 5 8 and control section 5 9 and so on. The excitation laser light source 52 is arranged outside the annealing room (not shown), which generates a wavelength; I = 248nm KrF excitation laser beam.
— 激勵雷射波束自激勵雷射光源52導入退火室内部(未 =出)。在退火室中,當薄膜半導體基板置於基板台55上 才,基板台55可在二維水平平面移動。 a μ掩2。5 3女排在基板台5 5之上,當一相移器置於掩罩 上守可以一維水平平面上移動,圖未示出。掩罩台— Excited laser beam Self-excited laser light source 52 is introduced into the interior of the annealing chamber (not shown). In the annealing chamber, when the thin-film semiconductor substrate is placed on the substrate stage 55, the substrate stage 55 can be moved in a two-dimensional horizontal plane. a μ mask 2. 5 3 The women's volleyball team is on the substrate table 5 5. When a phase shifter is placed on the mask, the upper guard can move on a one-dimensional horizontal plane, which is not shown in the figure. Masking table
第26頁 200415793Page 26 200415793
I3之構型僅與相移器之外緣接觸 器之雷射光束。 俾不致切斷傳輸至像移 台《部分54調整基板台55及掩罩台53之位置,並將 〃、溥胺半導體基板長度方向將其掃描。 , 激4:==56之鏡56“加自激勵雷射光源52之 板S之s 土主 °及使激勵雷射入射在薄膜半導體基 /光表面通過掩罩M。基板s由自掃描學系統56之教 勵每射光束在寬度方向所掃描。The configuration of I3 is only with the laser beam of the phase shifter outer edge contactor.俾 will not be cut and transferred to the image shift stage "section 54 to adjust the positions of the substrate stage 55 and the mask stage 53, and scan the rhenium and fluorene semiconductor substrate lengthwise. , 4: == 56 of the mirror 56 "plus the self-excitation laser light source 52, the plate S of the S, and the excitation laser is incident on the thin film semiconductor substrate / light surface through the mask M. The substrate s is determined by self-scanning The system 56 instructs each beam to be scanned in the width direction.
k正偵測部分57為一光學偵感器,用以偵測相移器側 暴板S側之校正記號之目標圖案(未說明)之校正條件。 ^ 基板偵測部分58由複數個光偵感器組成,該等偵感器 ^在將曝光至一表面之基板臺55中。該基板偵測部分58偵 1由備於退火室(未示出)上之轉移臂放置在基板臺5 5上之 基板S之放置狀態。 、、 控制部分59控制該台驅動部分54,掃描光學系統56及 勵語射光源5 2 ’以響應自基板偵測部分5 8之信號及校正 偵剛部分57之信號。 雖未示出,基板台5 5及掩罩台5 3在控制部分5 9之控制 I由該台驅動部分5 4所驅動,並包含傾斜調整機構以在水The k-positive detection section 57 is an optical sensor for detecting a correction condition of a target pattern (not illustrated) of a correction mark on the side of the phase shifter and the plate S. ^ The substrate detecting portion 58 is composed of a plurality of light sensors, and these sensors are in a substrate stage 55 to be exposed to a surface. The substrate detection section 58 detects the placement state of the substrate S on the substrate table 55 by a transfer arm provided in an annealing chamber (not shown). The control section 59 controls the drive section 54, the scanning optical system 56, and the excitation light source 5 2 'in response to the signal from the substrate detection section 58 and the signal from the correction detection section 57. Although not shown, the control of the substrate stage 55 and the mask stage 5 3 in the control section 59 is driven by the stage driving section 54, and includes a tilt adjustment mechanism for
平方向ό又疋基板s及掩罩μ,即,臺1 5及制動器(壓電元件) 1 6如第1圖所示。 即 土 其次’第1 3圖中所示之晶體化裝置作業說明如下。 當基板S由轉移臂放置於基板台5 5後,基板s在基板台 已上之放置狀態由基板偵測部分5 8通知控制部分5 9。根據The plane direction 疋 also includes the substrate s and the mask μ, that is, the stage 15 and the brake (piezoelectric element) 16 are shown in FIG. 1. That is, the operation of the crystallizer shown in Fig. 13 is as follows. When the substrate S is placed on the substrate table 55 by the transfer arm, the substrate s on the substrate table is placed on the substrate table by the substrate detection section 58 and the control section 59 is notified. according to
第27頁 200415793 五、發明說明(20) 此點控部分5 9控制該台驅動部分5 4。 ㈣部分59控制台驅動部分54以沿基衫長度方向掃 掐基板台55及掩罩台53俾彼等橫過校正偵測裝置π。Page 27 200415793 V. Description of the invention (20) This point control part 5 9 controls the drive part 5 4 of this station. The console section 59 drives the console section 54 to scan the substrate table 55 and the mask table 53 along the length of the base shirt, and they cross the correction detection device π.
k制部分5 9以翏考校正記號狀(第丨4圖)校正狀態及校 正積測部分57同時偵出之目標圖案Rp(第14圖),以控制台 驅動4 7刀54二在控制之下,台驅動部分54調整基板台55之 位置#將每一权正記號Μ K可設定在目標圖案r p之對應圖 木之:央二如第1 4圖所示。如校正記號ΜΚ或目標圖案RP 失真時,薄膜半導體基板之傾斜或記號Μ之傾斜需由傾斜 調整機構加以改正。 、當1及基板S間之校正之調整已完成,激勵雷射光 源52及掃描光學系統56由控制部分59控制,以根據記號μ 施加激勵雷射光束於基板s之曝光表面。同時,(或在預定 時序)’基板台55及掩罩台53之位置(長度方向中)改變, 俾台驅動部分54橫跨校正偵測部分57。基板s之暴光表面 隨後得以晶體化。 第1 5圖為能處理而不需失焦之雷射退火裝置之一例之 略圖。處理可用基板之曝光表面之相對位置(距離)實施而 不計基板表面之波浪分布,即,處理之物件與影像光學系 統限定之投影面均位於影像系統之D〇F範圍内。雷射退火 裝置151與第13圖之晶體化裝置相同,除已省略掩罩台 53,在第1 3圖中之晶體化裝置中之掩罩台53及校正偵測部 分57上設定記號Μ及修改控制部分59之結構。因此,與第 1 3圖所示之組成元件相同或相似之件以同一代號表之詳細The k system part 5 9 uses the test correction mark (Fig. 4) to adjust the correction state and the target pattern Rp (Fig. 14) detected by the correction measurement part 57 at the same time. It is driven by the console 4 7 knife 54 2 in the control. Next, the stage driving section 54 adjusts the position of the substrate stage 55 # to set each right sign M K in the corresponding figure of the target pattern rp: Yang Er as shown in FIG. 14. If the correction mark MK or the target pattern RP is distorted, the tilt of the thin-film semiconductor substrate or the mark M needs to be corrected by the tilt adjustment mechanism. When the adjustment of the correction between 1 and the substrate S has been completed, the excitation laser light source 52 and the scanning optical system 56 are controlled by the control portion 59 to apply the excitation laser beam to the exposure surface of the substrate s according to the symbol μ. At the same time, (or at a predetermined timing) the positions of the substrate stage 55 and the mask stage 53 (in the longitudinal direction) are changed, and the stage driving section 54 straddles the correction detecting section 57. The exposed surface of the substrate s is then crystallized. Fig. 15 is a schematic diagram of an example of a laser annealing apparatus capable of processing without defocusing. The processing can be carried out by the relative position (distance) of the exposed surface of the substrate, irrespective of the wave distribution of the substrate surface, that is, the processed object and the projection plane defined by the imaging optical system are located within the DOF range of the imaging system. The laser annealing device 151 is the same as the crystallizing device in FIG. 13 except that the masking table 53 has been omitted. Marks M and 53 are set on the masking table 53 and the correction detection section 57 in the crystallizing device in FIG. 13. The structure of the control section 59 is modified. Therefore, the same or similar components as those shown in Figure 13 are listed in the same code.
第28頁 200415793 五、發明說明(21)Page 28 200415793 V. Description of the invention (21)
說明予以簡化。 第15圖之雷射退火裝置中 以下控制作業。 控制部分59已修改 以實施 當基板S已由轉移臂放置在基板台55上,基板台55 之基板S之放置狀態自基板偵測部分5 8通知控制部分5 g t 根據此通知,基板台5 5由基板驅動部份5 4移動,俾美板$ 在控制部分5 9之控制之下。 & 之後激勵雷射光源5 2及掃描光學系統5 6由控制部分5 9 所控制,同時調和在基板S之位置中之關係。 換g之’激勵雷射波束加在基板S之曝光表面,美板 台5 5由基板驅動部分5 4以基板S之長度方向移動。 如亡所述’本發明可應用在第13圖中之晶體化之裝置 上’及第15圖中之雷射退火裝置上。 乂The description is simplified. In the laser annealing apparatus of Fig. 15, the following control operations are performed. The control section 59 has been modified to implement that when the substrate S has been placed on the substrate table 55 by the transfer arm, the placement state of the substrate S of the substrate table 55 is notified from the substrate detection section 5 8 to the control section 5 gt According to this notification, the substrate table 5 5 The substrate driving part 5 4 moves, and the Rimage board is under the control of the control part 59. & Thereafter, the laser light source 52 and the scanning optical system 56 are controlled by the control section 59, and the relationship in the position of the substrate S is adjusted at the same time. In other words, the excitation laser beam is applied to the exposed surface of the substrate S, and the substrate stage 5 5 is moved by the substrate driving portion 54 in the length direction of the substrate S. As described above, the present invention can be applied to the crystallization device in FIG. 13 and the laser annealing device in FIG. 15. Qe
面積(基板表面, 雖未提及, 成之及曝光—光^ 膜上形成光阻層 TFT圖案(薄 一預定圖案形成 正之裝態形成, 例如有預定之液 透氣’及增加一 表面退火後可在基板(處理之物件)處理」 即曝光表面)有一均勻之深度。 半導體圖案之組合可利用預先在基板上f 影像(Μ 0 S - T F T,即薄膜電晶體)半導體薄 而獲得’即將記號Μ通過光阻層之表面。 膜基板)形成其上之玻璃基板於是形成, 其上之相對基板已以波浪及厚度不平已g 備於預定空間之相對位置。一光電基才反 晶,可安排於基板之間。基板間之&隔; 驅動電路。一液晶面板於是構成。Area (substrate surface, although not mentioned, formation and exposure-formation of photoresist layer TFT pattern on the film (thin, a predetermined pattern is formed in a positive state, such as a predetermined liquid permeability, and adding a surface can be annealed) Processing on the substrate (processed object) (ie the exposed surface) has a uniform depth. The combination of semiconductor patterns can be obtained by using a thin f image (M 0 S-TFT, ie, thin film transistor) of the semiconductor on the substrate in advance to obtain the 'coming mark M' Through the surface of the photoresist layer (film substrate), the glass substrate formed thereon is formed, and the opposite substrate thereon has been prepared at a relative position in a predetermined space with waves and uneven thickness. An optoelectronic substrate is inverted and can be arranged between the substrates. &Amp; spacer between substrates; drive circuits. A liquid crystal panel is then constructed.
第29頁 200415793 圖式簡單說明 第1圖為本發明一特性之曝光裝置之一例之概略圖。 第2圖為 < 曲線顯示待曝光物件厚度之不均句分布。 第3圖為略圖說明第2圖中一物件之三維曝光表面。 第4 A圖及第4B圖為略圖說明一曝光場之掃描方向及位移差 間之關係。 在Y方向掃描一曝光場 根據本發明在X方向掃 根據本發明之一特性 第5圖為略圖說明曝光方法之一例 與本發明之實施例作一比較。 第6圖為略圖說明曝光方法之一例 描一曝光場。 第7圖為略圖說明曝光方法之一例 同時實施傾斜及垂直運動。 第8A圖及第8B圖為略圖說明第7圖中說明之傾斜及垂直運 動之效應。 第9A圖及第9B圖為略圖說明在第8A圖及第8B圖說明之條件 下曝光場之傾斜及旋轉軸間之關係。 第10A圖及第10B圖為略圖說明因第9A圖及第9B圖中之傾斜 控制之結果所獲得之明顯波浪之平面分布之一例。 第1 1圖為略圖顯示可用於第1圖之曝光裝置中之控制裝置 之 例 第12圖為略圖顯示本發明之傾斜及垂直運動中之一壓電元 件設定一作業量(控制量)之方法之一例。 第1 3圖為略圖顯示本發明之平坦化機構應用在一雷射晶體 化裝置之一例。 第1 4圖為略圖說明第1 3圖中晶體化之雷射裝置之作業(控Page 29 200415793 Brief Description of Drawings Fig. 1 is a schematic diagram of an example of an exposure apparatus having a characteristic of the present invention. Figure 2 shows the uneven sentence distribution of the thickness of the object to be exposed. Fig. 3 is a schematic illustration of the three-dimensional exposed surface of an object in Fig. 2. Figures 4A and 4B are diagrams illustrating the relationship between the scanning direction and the displacement difference of an exposure field. Scanning an exposure field in the Y direction Scanning in the X direction according to the present invention According to a feature of the present invention FIG. 5 is a diagram illustrating an example of an exposure method in comparison with an embodiment of the present invention. Fig. 6 is a schematic illustration of an example of the exposure method. An exposure field is depicted. Fig. 7 is a schematic diagram illustrating an example of an exposure method, and tilt and vertical movements are performed simultaneously. Figures 8A and 8B are schematic diagrams illustrating the effects of tilt and vertical motion described in Figure 7. Figures 9A and 9B are schematic diagrams illustrating the relationship between the tilt of the exposure field and the rotation axis under the conditions described in Figures 8A and 8B. Figures 10A and 10B are schematic diagrams illustrating an example of the obvious wave plane distribution obtained as a result of the tilt control in Figures 9A and 9B. FIG. 11 is a schematic view showing an example of a control device that can be used in the exposure device of FIG. 1 and FIG. 12 is a schematic view showing a method for setting a work amount (control amount) of a piezoelectric element in the tilt and vertical movement of the present invention An example. Fig. 13 is a schematic view showing an example of the planarization mechanism of the present invention applied to a laser crystallization device. Figure 14 is a schematic illustration of the operation of the crystallized laser device in Figure 13 (control
第30頁 200415793 圖式簡單說明 制)之一例。 第1 5圖為略圖說明本發明之平坦化機構用於雷射退火裝置 之一例。 第16圖為略圖顯示分布及掃描曝光裝置之一例。 元件符號說明: 1 曝光裝置 6 光學系統 9 匯流排 10 歪曲條件偵測器 11 光源 12 照明光系統 13 掩罩台 14 影像光學系統 15 基板台 16 制動器(壓電元件, 17 支撐部分 18 半導體雷射裝置 20 PSD(位置敏感裝置) 21 控制裝置(電腦) 21 基板裝置 31 輸入埠 32 作業部分 33 改正量設定部分 34 制動器驅動部分(電壓設定部分) 35 控制部分 36 記憶體 37 顯示裝置 52 激勵雷射光源 53 掩罩台 54 台驅動部分 55 基板台 56 掃描光學系統 56A 鏡 57 校正偵測部分 58 基板偵測部分 59 控制部分 71 、CPU 中央處理器 72 、RAM 隨機存取記憶 73 、ROM 唯讀記憶體 74 曝光區域決定部分Page 30 200415793 Simple illustration of the system). Fig. 15 is a schematic diagram illustrating an example of the planarization mechanism of the present invention applied to a laser annealing apparatus. FIG. 16 is an example of a schematic display distribution and scanning exposure device. Description of component symbols: 1 exposure device 6 optical system 9 bus bar 10 distortion condition detector 11 light source 12 illumination light system 13 mask stage 14 image optical system 15 substrate stage 16 brake (piezo element, 17 support part 18 semiconductor laser Device 20 PSD (Position Sensing Device) 21 Control Device (Computer) 21 Base Unit 31 Input Port 32 Operating Section 33 Correction Setting Section 34 Brake Driving Section (Voltage Setting Section) 35 Control Section 36 Memory 37 Display Device 52 Laser Exciter Light source 53 Mask stage 54 Drive section 55 Substrate stage 56 Scanning optical system 56A Mirror 57 Calibration detection section 58 Substrate detection section 59 Control section 71, CPU, central processing unit 72, RAM random access memory 73, ROM read-only memory Volume 74 Exposure area determination section
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TWI424516B (en) * | 2007-10-10 | 2014-01-21 | Asml Netherlands Bv | Method of placing a substrate, method of transferring a substrate, support system and lithographic projection apparatus |
TWI807775B (en) * | 2021-04-14 | 2023-07-01 | 日商斯庫林集團股份有限公司 | Drawing apparatus and drawing method |
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TWI407338B (en) * | 2008-04-18 | 2013-09-01 | Innolux Corp | Method of fabricating touch-control panel |
KR100940239B1 (en) * | 2009-08-11 | 2010-02-04 | (주)프로비전 | The etching method and device for making pattern of the electric capacity type touch screen using excimer laser |
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US4952858A (en) * | 1988-05-18 | 1990-08-28 | Galburt Daniel N | Microlithographic apparatus |
KR100358422B1 (en) * | 1993-09-14 | 2003-01-24 | 가부시키가이샤 니콘 | Plain positioning device, scanning exposure device, scanning exposure method and device manufacturing method |
US6304316B1 (en) * | 1998-10-22 | 2001-10-16 | Anvik Corporation | Microlithography system for high-resolution large-area patterning on curved surfaces |
JP2001036088A (en) * | 1999-07-15 | 2001-02-09 | Seiko Epson Corp | Method of manufacturing thin film transistor and electro-optical device |
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TWI424516B (en) * | 2007-10-10 | 2014-01-21 | Asml Netherlands Bv | Method of placing a substrate, method of transferring a substrate, support system and lithographic projection apparatus |
TWI807775B (en) * | 2021-04-14 | 2023-07-01 | 日商斯庫林集團股份有限公司 | Drawing apparatus and drawing method |
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NL1024809C2 (en) | 2005-04-05 |
NL1024809A1 (en) | 2004-09-14 |
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