TW200423224A - Exposure system, exposure method, and device fabricating method - Google Patents
Exposure system, exposure method, and device fabricating method Download PDFInfo
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- TW200423224A TW200423224A TW92133809A TW92133809A TW200423224A TW 200423224 A TW200423224 A TW 200423224A TW 92133809 A TW92133809 A TW 92133809A TW 92133809 A TW92133809 A TW 92133809A TW 200423224 A TW200423224 A TW 200423224A
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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
- G03F7/708—Construction of apparatus, e.g. environment aspects, hygiene aspects or materials
- G03F7/70858—Environment aspects, e.g. pressure of beam-path gas, temperature
- G03F7/70883—Environment aspects, e.g. pressure of beam-path gas, temperature of optical system
- G03F7/70891—Temperature
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200423224 玫、發明說明: 【發明所屬之技術領域】 本發明係有關-種曝光裝置、曝光方法、及元件製造 θ方法:詳言之’係-種形成半導體元件(積體電路)、液晶 顯不元件等電子元件的微小圖案時,所使用之曝光裝置及 曝光方法,以及使用上述曝光裝置之元件製造方法。 【先前技術】 _ 一直卩來’在參!造半導體元件及液晶顯示元件等電子 兀件的微影製程中’係使用各式曝光裝置。近年所主要使 用的係投影曝光裝置的型式,有步進重複(咖_ repeat)方式之縮小投影曝光裝置(亦即步進器),其係將擬 形成的圖案擴大4〜5倍以成為光罩(或稱標線片)上的圖案 ,透過投影光學系統將圖案縮小轉印於晶圓等被曝光物體 上’或是經改良該步進器後所構成之步進掃描式(step㈣ scan)的掃描型投影曝光裝置(亦即掃描式步進器)等。 ^因應隨半導體元件的高集成化而漸趨細微之電路圖 、/投衫曝光裝置中的曝光波長逐漸往短波長發展。現 在的波長雖以KrF準分子雷射光的248nm為主流,然而更 域㈣ArF準分子f射光的193nm亦逐步進人實用化階 :。再者,投影曝光裝置之光源可振盪出波長短至157⑽ 田子九之f2雷射(氟化雷射)、可振^出波長短至126⑽雷 5^ Ar2雷射等,亦即,可輪出真空紫外線區域之波長 :為,、光源(真空紫外光)的投影曝光裝置,亦 發階段。 200423224 此種波長在200mn以下的真空紫外光’會被一般透鏡 材料的玻璃之大量吸收,因此可使用之透鏡材料,侷限於 合成石英或螢石(氟化鈣結晶)等氟化物結晶。特別是,以 ,長157nm的&雷射光為曝光用光源時,透鏡材料侷限於 螢石。然而,即使使用這些材料,曝光用光源仍並非完全 不被吸收,在透鏡内曝光用光源每穿透lcm約被吸收 〜〇· 5%的曝光用光源。 又,真$紫外光亦會被大氣中的氧或纟;4氣大量.吸收 ,因而’使用真空紫外光的曝光裝置時,必須將其光程空 間之内部氣體置換(氣體淨化,gas purge)成幾乎不吸收曝 光用光源的氮或稀有氣體等低吸收性氣體。例如,以振盪 波長157nm的~雷射為光源的曝光裝置,必須將從雷射至 晶圖止之光程的大部分,將殘存的氧濃度控制在一以下 又,不僅是藉由短波長化,由於加大投影光學系統的 數值孔徑(N.A)亦能提高解析度,因而投影光學系統的大 MA化亦在開發之中。再者’為達高解析度之目標,使投影 光學系統的殘存像差小是一重要的課題。200423224 Description of the invention: [Technical field to which the invention belongs] The present invention relates to an exposure device, an exposure method, and a device manufacturing method θ: in detail, the 'system'-a method for forming a semiconductor element (integrated circuit), and a liquid crystal display. For micropatterns of electronic components such as devices, the exposure device and exposure method used, and the device manufacturing method using the above exposure device. [Prior art] _I have been using various exposure devices in the lithography process of manufacturing electronic components such as semiconductor devices and liquid crystal display devices. The types of projection exposure devices that have been mainly used in recent years include step-and-repeat (repeated) reduction projection exposure devices (ie steppers), which expand the pattern to be formed by 4 to 5 times to become light. The pattern on the hood (or reticle) is reduced and transferred to the exposed object such as a wafer through a projection optical system, or a step-scan type formed by improving the stepper. Scanning projection exposure device (ie scanning stepper), etc. ^ In response to the high integration of semiconductor devices, the circuit diagram becomes gradually finer, and the exposure wavelength in the exposure device is gradually developing to a shorter wavelength. Although the current wavelength is mainly 248nm of KrF excimer laser light, 193nm of the FArF excimer f light has gradually entered the practical stage. In addition, the light source of the projection exposure device can oscillate f2 lasers (fluorinated lasers) with a wavelength as short as 157⑽ Tian Zijiu, and ^ ar2 lasers with a wavelength as short as 126⑽, 5 ^ Ar2 lasers, etc., that is, can be rotated out The wavelength of the vacuum ultraviolet region: is, the projection exposure device of the light source (vacuum ultraviolet light), also issued. 200423224 This kind of vacuum ultraviolet light with a wavelength below 200mn will be absorbed by a large amount of glass of general lens materials, so the lens materials that can be used are limited to synthetic quartz or fluoride crystals such as fluorite (calcium fluoride crystal). In particular, when & laser light having a length of 157 nm is used as the light source for exposure, the lens material is limited to fluorite. However, even if these materials are used, the light source for exposure is not completely absorbed, and the light source for exposure in the lens is absorbed by ~ 0.5% of the light source for exposure per 1 cm of penetration. In addition, the true ultraviolet light will be absorbed by the oxygen or tritium in the atmosphere; a large amount of 4 gas is absorbed. Therefore, when using a vacuum ultraviolet light exposure device, the internal gas in its optical path space must be replaced (gas purge) It is formed so as not to absorb low-absorptive gas such as nitrogen or rare gas of the light source for exposure. For example, an exposure device using an oscillation wavelength of 157nm ~ laser as a light source must control the remaining oxygen concentration below the most of the optical path from the laser to the crystal pattern, not only by shortening the wavelength. Since increasing the numerical aperture (NA) of the projection optical system can also improve the resolution, the large MA of the projection optical system is also under development. Furthermore, to achieve the goal of high resolution, it is an important issue to reduce the residual aberration of the projection optical system.
欲貫現上述大NA 成低像差化,視野愈小的光學系統 愈易貫現。然而,就暖古驶里 a 就曝先裝置而言,曝光區域愈大則處理 能力(thr〇Ugh Put)愈佳,故而,最近係以掃描型曝光穿置 ==係使用兼具小視野及大NA的投影光學系統,為 又付曝光區4,在曝光當中使標線片與晶圓維持固定的 成像關係以相對行進掃描。 200423224In order to realize the above-mentioned large NA and reduce the aberration, the optical system with a smaller field of view becomes easier to realize. However, in terms of warm-up driving, as far as the exposure-first device is concerned, the larger the exposure area, the better the processing capacity (thr0Ugh Put). The large NA projection optical system, in order to provide an additional exposure area 4, maintains a fixed imaging relationship between the reticle and the wafer during the exposure to scan in a relatively progressive manner. 200423224
另-方面’使用同一波長、同_ N 解析度之蒋相々庐始ΰ ^ 尤予♦、、统以提昇 式仏線片(phase shift⑽❿)等超 術’亦進入實用化階段。此種超解析技術所使用 例如’吾人所咸知者,所使用的「移相式標線片」,係在 標線片上的圖案中,使穿透相鄰透過圖案之光 ⑽ 。的相位差,來提昇解析度。 、 此時’由於移相式標線片的照明光之入射角範圍命小 、解析度提昇效果愈佳,因此希望併用入射角範圍窄的照 明條件,亦即相干度(coherence fact〇r,即照日月^ )小的 照明條件。 至於其他的超解析技術,如4極照明或2極照明等變 形照明,亦已進入實用化階段。 如以上所述,使用真空紫外光為曝光用光源時,構成 投影光學系統的透鏡(透鏡元件)吸收了曝光用光源,除了 意味著到達晶圓的曝光用光源之能量受到衰減,同時,亦 意味著上述透鏡因吸收曝光用光源的能量而發熱。又,因 上述發熱(溫度變化)而造成透鏡膨脹時,折射率將會變化 ’而產生像差。 如前所述,對投影光學系統要求的殘存像差要小,然 而,僅是因上述吸收曝光用光源所伴隨的發熱而導致的像 差,恐怕已超過投影光學系統所能容許的最大像差值(容 許值)。 特別是,採用上述移相式標線片及小σ照明之組合時 ’透過投影光學系統内之曝光用光束易於局部化,使得投 影光學糸統内的透鐘蘇勒介 壬局部化(或偏置化),而易產 生的像差:::熱。此現象即意味著,在投影光學系統内產 =r…為中心的旋轉對稱像差,恐大㈣ ::卜’為更進一步的提昇c—m〇s—lsi的性能,當使 内的方Ba®其晶圓表面係結晶面之《⑴》面時,因晶圓面 或雷、 電子或電洞的移動度不同,最好是能使電子 門極動方向切結晶之[11°]方向。因而,各電晶體 .,, 頁在《1U》面内與[110]方向之正交 ⑵方向)-致。再者,上述面及方向的記載中 亚不冲各指數的符號。 此時’閘極製程用的標線片圖案之方向,在 之全面對*杳一古A m 對'二向,因而’從標線片圖案產生的繞射光亦 ―月、方向。特別是,使用移相式標線片且併用小口照明 通過投影光學系統的曝光用光束明顯有局部化現象, :而,構成投影光學系統的透鏡因吸收曝光用光源而產生 备熱亦呈旋轉非對稱,以致在投影光學系統内發生明顯 的旋轉非對稱像差。 、 ,者右與先刖的C_廳_ LSi同樣的,使用的石夕晶 °之曰曰圓表面為結晶面《J 〇〇》面時,有時間極圖案的方 白曰 ' 方向者為佳,此時亦與上述同樣地發生繞射光 的明顯局部化’以致在投影光學系統產生旋轉非對稱之像 差0 又 ,即使是使用變形照明時,造成通過投影光學系 統 10 200423224 内的曝光用光束之局部化(或偏置化),而發生與上述相同 的問題。 【發明内容】 本發明乃基於上揭問題點而提出者,其第1目的,在 長:供可貫現南精度曝光之曝光裝置。 本發明之第2目的,在提供可實現高精度曝光之曝光 方法。 本毛明之第3目的,在提供元件製造方法以提昇高集 成化元件之生產性。 本杂明第1觀點之第1曝光裝置’係以能量束照明光 罩’俾將形成於該光罩之圖案透過投影光學系統轉印於感 光物體上’其特徵在於,具備:㈣系、統,係以該能量束 照明該光罩;光罩載台,其形成有開口,俾在不透過該光 罩的情況下,使虛擬照射用能量束穿透至投影光學系統, 二;外繞於该光罩周圍、用以將光罩周圍與外部隔離之 日w 土的至少一部分,可保持該光罩而移動自如。 根據此發明,保持光罩而能移動自如之光罩载△中, ==擬照射用能量束不透過光罩而穿透至投:光學 統轉印至感光物體上時(曝光時),即使在構成 統的光學構件被局部(不均勻地)加熱的情形下, 進仃曝先時,.透過上述開口對光學構 ^ ^ + , A 、奇了虛擬照射用能 二光學構件在上述曝光中未受到加熱 —果,可緩和光學構件的加熱狀態之不均勻性。藉此, 即能抑制上述光學構件因不 之修正困難的像差,亦… 所產生投影光學系統 即此抑制非以光軸為中心的旋轉對 稱像差(即旋轉非對稱像差) 。疋轉對 對稱像差,可Μ由將既6丄 ’投影光學系統之旋轉 反 j糟由將既定光學槿杜《 ^ 而容易的加以修正。 +構件被幅驅動於光軸方向’ 又’光罩載台具有間隔壁(或其中 於光罩周圍,俾將光罩附近實 ” U ^ 直1 S队Λ. 貝貝乳雄、以和外部隔離,因此 其效果除了等同以間隔壁 使裝置小型、輕量化。又,^1全^之外’且亦能 ,, 又例如,將間隔壁内空間以能量 ^性低的氣體加以置換時,係與藉間隔壁覆於光罩 、曲;時相同地’可降低光罩周邊空間内的吸光物質之 :更可因為降低氣體的使用量而降低成本。因而,在 見_曝光的同時’亦能達成裝置的小型、輕量化。 躺广所叫%轉對稱」’係指異於-般所指的「旋 :t」’亦即’並非指「-個圖形等僅在-固定角度繞 一固定軸(對稱轴)旋轉而能保持不變之性質」之-般定義 ’而係指「-個圖形得以。。〜36。。之所有角度沿一固定 轴(對稱軸)旋轉而不改變其性質」。除此以外之情形,皆 為紅轉非對稱。因&,即使在以投影光學系統或光學構件 與“軸為中u之〇〜36〇。的範圍内以任意角度旋轉光 、構件6產生同樣像差時之像差為旋轉對稱像差,除此 :外之像差則為旋轉非對稱像差。本說明書中,所採用的 「旋轉對稱」A「旋轉對稱之像差」用語,以及「旋轉非 對私」與「旋轉非對稱像差」用語,係採如上定義。 12 200423224 此% ’在上述光罩载台所形成的開口之一部分亦可 2:曝:用開口,俾在將上述圖案轉印於感光物體上時使 能量束穿透至投影光學系統側;或者,於上述光罩载台, 使光罩圖案轉印至感光物體上時用以使能量束穿透至^ 光學系統側之曝光用開口、與上述開口,係分開形成;: 可了上述開口,具有與上述圖案投影至咸 先物體上時該能量束照射於光罩的區域大致相同的大小Γ 作本發明之第1曝光裝置中,進-步具備變更照明條件 之Μ更機構’其係在將該圖案轉印於該感光物體上時、以 及透過該開口照射作為虛擬照射用能量束之該能量束日士, 變更該照明系統之照明條件。 才 此時,透過該開口照射該能量束之照明條件, 和該投影光學系統内之光學構件因該能量束之照射而產ί 的熱偏置狀態。 $ 本發明之第1曝光裝置,進—步具 ,係透過既U r間隙配置於該光罩載台的該照明系2 ’供該能量束穿透之光穿透部設於其中—部分,並 於該光罩載台的面作為光罩载台的移動引導面;以及第。 光罩平台,係透過既定第2間際配置於該光罩載台的卜 光學系統側’供該能量束穿透之光穿透部設於其中—二 ’並以對向於該光罩載台的面作為光罩載台的移動引導面。刀 此時,該第1光罩平台之光穿透部及第2光罩平A 光穿透部,係兼作為不同於該能量束之虛擬照 = 的通路。 犯里术 13 200423224 本發明之第1曝光裝置,進一步具備分束器,係在該 虛擬照射時插入照明系統内部或照明系統與投影光學系統 間的光程上’透過該開口使該虚擬照射用能量束射入該投 影光學系統。 令I切之第1曝光裝 擬照射用能量束係紅外線_ 本發明第2觀點之第2曝光裝置,係以能量束照明光 罩’俾將形成於光罩的圖案轉印於感光物體上,其特徵在 衣,具備:投影光學系統,係將該圖案像投影至該感光物 體以及紅外線照射機構,係以紅外線照射構成該投影 光學系統之光學構件,而能將該光學構件予以局部加熱。 根據此發明,其具備以紅外線照射構成該投影光學系 T之光學構件,而能將該光學構件予以局部加熱的紅外線 月?、射機構。因此,蔣报# …成先罩的圖案透過投影光學系統 ==物體上時(曝光時),即使在構成投影光 的先子構件因能量束之照射而被局部(不均勾地)加埶的情 I下,亦能以紅外線照射機構照射紅外線,以μ光學構 件中未因能量束之照射而被加熱之其他部分,立处 大致均勻的加熱光學構件。據 八、° ,月b 勺^ 據此,此抑制因光學構件不均 二:加熱所產生之投影光學系統之修正固難 性像差的發生。此場合,由於 “冉 ^ L M 、、卜線照射機構對光學構# 之加熱,在曝光尹亦能進行,因此盘 子構件 較,能更為確實的抑制投影光 冑先裝置相 的發生。因此,能良好的维持投影光^走轉非對稱性像差 先予系統之成像特性進 14 200423224 行曝光:而得以實現高精度之曝光。 处I β a外線照射機構,藉由將該光學構件局部加 置狀Γ和該光學構件中因該能量束的照射所產發之熱偏 學構2Γ’該光學構件可以是折射光學元件,或者該光 ::件亦可以是反射光學元件。若為後者 射機構係對反射光學开杜由ffl 卜線,、" 牛中,用以反射該能量束之反射面 的月面,照射該紅外線。 本發明之第2 oR出爿it | *先波置中,該紅外線照射機構可對光 構件表面之一部分照射紅外線。 “此%,该光學構件表面之一部分,係將該圖案像投影 於該感光物體上時,未A,女处旦 ’ 未又忒此罝束照射之光學構件的表面 分〇 枣發明之第 *光裝置中,該光學構件係螢石構成之 透鏡,該紅外線照射機構,可將波長6叫―程度 線照射於光學構件。 、 本發明之第2曝弁努署由 V.,, ^ ,该、工外線照射機構包含複 數條光纖,其一端係配設於該朵與播 发尤子構件附近,以對該并輋 構件照射紅外線。 干 本發明之第1、第2曝光妒w φ,叮、在 尤衣置中可進一步具備驅動 機構,以將構成該投影光學系統之光學構件的至少一個, •驅動於該投影光學系統的光軸方向。 本’X月之第1帛2曝光裝置中,該能量束係波長 157nm的氟雷射光,或是波長19—的㈣準分子雷射光。 15 200423224 本發明第3觀點之曝光方法,其特徵在於,具備··轉 印製程,係以能量束照射配置在第1面上的光罩,將形成 於该光罩之圖案透過投影光學系統轉印至配置在第2面上 之感光物體上;以及照射製程,係在未配置該感光物體的 狀態下,以可緩和在該轉印製程中該投影光學系統内之光 學構件因能量束照射所產生的熱偏置狀態之照射條件,不 透過该光罩,朝該投影光學系統照射虛擬照射用能量束。 根據此發明,係以能量束照明配置在第丨面上的光罩 ,將形成於光罩的圖案透過投影光學系轉印在配置於第2 面上之感光物體上(轉印製程),在未將感光物體配置於第 2面上的狀態下,以足可緩和上述轉印製程中其投影光學 系内的光學材料因能量光束照射而發生的熱偏置狀態者來 作為=射條件,不透過光罩,朝投影光學系照射虛擬照射 ^里束(”、、射製私)。因此,即使在轉印製矛呈中構成投影 一子系的光子材料被局部性地(不均勻地)加熱,卻仍可藉 由照射製程的處理,將光學材料加熱成幾乎一致的狀態。 斤揭示的上述妝射製程之處理,可於轉印製程後進行 ,亦可於之前進行。 、無論採任一作法,皆可抑制光學材料的不均勻加熱, 而避免投影光學系統發生難以補償之旋轉非對稱像差,可 維持投^光學系之良好成像特性,以實現高精度之曝光。 :時’可進-步包含在該照射製程前,將分束器插入 二::束:光程空間内的製·;該照射製程中,係透過該 刀為來照射虛擬照射用能量束。 16 200423224 本發明之第1曝光方法中,該照射製程,係在保持嗲 感光物體之物體載台上進行該感光物體的交換時進行。人 本發明第4觀點之曝光方法,其特徵在於,具L ••轉 印製程,係以能量束照明光罩,透過投影光學系統將形成 於該光罩的圖案轉印於感光物體上;以及加熱製程,係對 構成該投影光學系統之光學構件照射紅外線,以將該光與 構件局部加熱。 % 根據此發明,其係以能量束照明光罩,將形成於 的圖案透過投影光學系統轉印至感光物體上(轉印, 對構成投影光學系統之光學構件照射紅外線 該:學構件(加熱製程)。因此,於轉印製程中,即使在轉 印衣私中構成投影光學系統之光學材 被局部性地(不均勾地u拥岵 此里束之照射而 ^^ _ )加熱%,亦能對加熱製程中未被能 里束之心射加熱之光學構件 熱,因此,其他部分照射紅外線予以加 據此,处永在/ 光學構件加熱成幾乎一致的狀態。 系統之:二’因光學構件不均勻之加熱所產生之投影光學 於構對的發生。此場合’* ,因此與前述第1 匕、’在曝光中亦能進行 光學系統之旋二二f相較’能更為確實的抑制投影 持投影光學季蜞 冉像差的發生。因此,能良好的维 之曝光系統之成像特性進行曝光,而得以實現高精度 此場合,贫 量束所造成之‘、、、衣私’係考慮該轉印製程中照射之能 子構件之熱分布,而加熱成使該熱分布以 17 200423224 光學構件之光軸為中心呈旋轉對稱的結果。 此場合,該加熱製程,可由複數條光纖對該光學構件 照射紅外線。 此場合,該加熱製程,可因應該光學構件的熱偏置狀 悲,由選自該複數條光纖中的至少丨條光纖,對光學構件 照射紅外線。 此場合,該紅外線之照射處,可將該圖案像投影至該 感光物體上之期間,未受該能量束照射之該光學構件的 面部分。 < 本發明之第 同時進行。 2曝光方法中,該轉印製程與加熱製程係 本發明f 5觀點之元件製造方法,係包含微影製程, 其特被在於:該微影製程係使用本發明第i、第2曝光穿 置之任一者,來將電路圖案形成在感光物體上。 、 叫干W丹、枯葫孕由 [1 1 1 ]轴大致一致的秒晶圓,形成於兮功a问 小成於4矽晶圓上的閘極圖 之長邊方向,係與[110]軸方向或其等價軸方向之正交方 一致。或者,該感光物體係垂直於盆丰 主且y、具表面軸與結晶軸 [110]軸大致-致时晶圓’形成於該^圓上的閉極圖 之長邊方向,係與[110]軸方向或其等價軸方向之正交方 一致。 【實施方式】 《第1實施形態》 實施形態。 以下,根據圖1〜圖10說明本發明之第 18 200423224 圖1係第1實施形態之曝光梦署沾4 ^ 裝置⑽巾,係以直*妙、 圖。在該曝光 光E /…、4外域的能量束,作為曝光用照射On the other hand, “Using the same wavelength and the same _N resolution as Jiang Xiang'an Lu Shi’ ^ You Yu ♦, and super-techniques such as phase shift⑽❿, etc., have also entered the practical stage. This kind of super-resolution technology is used, for example, ‘I ’m familiar with it’. The “phase-shift reticle” used in the pattern on the reticle makes the light 穿透 that passes through the adjacent transmission pattern. Phase difference to improve resolution. At this time, 'Because the incident angle range of the illumination light of the phase-shift reticle is smaller, the resolution improvement effect is better, so it is desirable to use the illumination condition with a narrow incident angle range, that is, coherence fact, According to the sun and moon ^) small lighting conditions. As for other super-analysis technologies, such as deformed lighting such as 4-pole lighting or 2-pole lighting, they have also entered the practical stage. As described above, when vacuum ultraviolet light is used as the light source for exposure, the lens (lens element) constituting the projection optical system absorbs the light source for exposure, in addition to the fact that the energy of the light source for exposure that reaches the wafer is attenuated, and it also means that The above-mentioned lens generates heat by absorbing the energy of the light source for exposure. In addition, when the lens expands due to the above-mentioned heat generation (temperature change), the refractive index changes' and aberrations occur. As mentioned above, the residual aberration required for the projection optical system is small. However, the aberration caused by the heat generated by the above-mentioned absorption exposure light source may exceed the maximum aberration allowed by the projection optical system. Value (allowable value). In particular, when using the combination of the above-mentioned phase-shift reticle and small σ illumination, the exposure beam transmitted through the projection optical system is easy to localize, so that the through-thickness of the projection optical system is localized (or biased). (Setting)), and easy to produce aberration ::: heat. This phenomenon means that in the projection optical system, a rotationally symmetric aberration at the center of r =... Is feared to greatly improve the performance of c-m0s-lsi. When the surface of the Ba® wafer is the "面" plane of the crystal plane, the wafer gate or mine, electrons, or holes have different degrees of movement, so it is best to cut the direction of the crystal's [11 °] direction . Therefore, the .., pages of the transistors are in the "1U" plane orthogonal to the [110] direction). In addition, in the description of the above faces and directions, Asia does not punch the signs of each index. At this time, the direction of the reticle pattern used for the gate process is completely opposite to * 杳 一 古 A m to the 'two-way', so the diffraction light generated from the reticle pattern is also the month and direction. In particular, the use of phase-shift reticles and small-mouth illumination to pass through the projection optical system has a significant localization phenomenon. Moreover, the lenses constituting the projection optical system generate heat by absorbing the light source for exposure. Symmetry such that significant rotational asymmetric aberrations occur in the projection optical system. The right side is the same as the C_hall_ LSi of the previous one. When the surface of Shi Xijing used is a crystal surface "J 〇〇", the square direction with the time pole pattern is the direction. At this time, obvious localization of the diffracted light occurs at the same time as above, so that the rotational asymmetric aberration of 0 occurs in the projection optical system, and even when deformed illumination is used, it causes exposure through the projection optical system 10 200423224. The beam is localized (or biased), and the same problem occurs as described above. [Summary of the Invention] The present invention is proposed based on the problems of the above disclosure. The first purpose of the present invention is to provide an exposure device capable of exposing exposures with high accuracy. A second object of the present invention is to provide an exposure method capable of realizing high-precision exposure. The third object of the present invention is to provide a component manufacturing method to improve the productivity of highly integrated components. The first exposure device of the first aspect of the present invention is "lighting a mask with an energy beam" and transferring a pattern formed on the mask onto a photosensitive object through a projection optical system. It is characterized by: , The light beam is illuminated with the energy beam; the mask stage is formed with an opening, and the energy beam for virtual irradiation is penetrated to the projection optical system without passing through the light mask; At least a part of the soil around the reticle to isolate the perimeter of the reticle from the outside, can hold the reticle freely and move freely. According to this invention, in the mask △ which can be moved freely while holding the mask, == the energy beam to be irradiated penetrates through the mask without passing through the mask: when the optical system is transferred to the photosensitive object (during exposure), In the case where the optical components of the system are locally (not uniformly) heated, the exposure is performed preliminarily. The optical structure ^ ^ +, A through the above openings is strange, and the two optical components for the virtual irradiation are in the above exposure. Without heating, the unevenness of the heating state of the optical member can be alleviated. In this way, it is possible to suppress the aberrations that are difficult to correct for the above-mentioned optical components, and also to produce the projection optical system that suppresses the rotational asymmetric aberration (ie, the rotational asymmetric aberration) that is not centered on the optical axis.疋 Turn to symmetrical aberrations, which can be easily corrected by reversing the rotation of the existing 6 ’′ projection optical system. + The component is driven in the direction of the optical axis by the 'mask' stage with a partition wall (or in the periphery of the mask, and the vicinity of the mask is solid. "U ^ Straight 1 S team Λ. Babe nipples, and external Isolation, so its effect is equivalent to making the device small and lightweight with a partition wall. It can also be used in addition to ^ 1, and, for example, when the space in the partition wall is replaced with a gas with low energy, It is the same as covering the photomask and curved wall with a partition wall. 'It can reduce the amount of light absorbing substances in the peripheral space of the photomask: it can also reduce costs by reducing the amount of gas used. Therefore, when you see _exposure' also Can achieve the device's small size and light weight. "Lai Guang called"% symmetric "" refers to the "rotation: t" which is different from the general meaning, that is, does not mean that "-a figure, etc. only go around at a fixed angle The general definition of "the fixed axis (the axis of symmetry) rotates and can remain unchanged" means "-a figure can be obtained. ~ 36 ... all angles of rotation are rotated along a fixed axis (the axis of symmetry) without changing its Nature ". In all other cases, red to asymmetric. Because & Rotate the light at any angle within the range of the projection optical system or the optical component and the axis is “0 ~ 36〇. The aberration when the component 6 produces the same aberration is a rotationally symmetric aberration. Aberration is rotational asymmetric aberration. In this specification, the terms "rotational symmetry" A "rotational symmetry aberration", and the terms "rotational non-private" and "rotational asymmetric aberration" are adopted as above. Definition: 12 200423224 This% 'can also be part of the opening formed by the above photomask stage 2: exposure: using the opening, the energy beam penetrates to the projection optical system side when the above pattern is transferred on the photosensitive object; Alternatively, when the mask pattern is transferred onto the photosensitive object on the photomask stage, the exposure opening for penetrating the energy beam to the optical system side is formed separately from the aforementioned opening; the aforementioned opening is possible It has the same size as the area where the energy beam is irradiated on the mask when the above pattern is projected on the object. As the first exposure device of the present invention, it is further provided with a mechanism for changing the lighting conditions. In the When the pattern is transferred on the photosensitive object, and the energy beam is irradiated as an energy beam for virtual irradiation through the opening, the lighting conditions of the lighting system are changed. Only then is the illumination of the energy beam radiated through the opening. Conditions, and the thermal bias state of the optical components in the projection optical system due to the irradiation of the energy beam. The first exposure device of the present invention, the step-by-step device, is arranged on the light through the U r gap. The illumination system 2 'of the mask stage is provided with a light penetrating portion through which the energy beam penetrates, a portion thereof, and a surface of the mask stage is used as a movement guide surface of the mask stage; and The platform is provided with a light penetrating portion for the energy beam penetrating through the optical system side of the predetermined second interval disposed on the mask stage 'two-' and facing the mask stage. Acts as a guide surface for the mask stage. At this time, the light penetrating portion of the first mask platform and the light penetrating portion of the second mask flat A light both serve as a path different from that of the virtual beam of the energy beam. Guiliju 13 200423224 The first exposure device of the present invention further includes a beam splitter, which is inserted into the lighting system or the optical path between the lighting system and the projection optical system during the virtual irradiation, and passes through the opening for the virtual irradiation. An energy beam is incident on the projection optical system. Let the first exposure device of I cut be an infrared energy beam for irradiation. The second exposure device of the second aspect of the present invention illuminates the photomask with the energy beam, and transfers the pattern formed on the photomask to the photosensitive object. The utility model is characterized in that it comprises a projection optical system for projecting the pattern image on the photosensitive object and an infrared irradiation mechanism, and irradiating an optical member constituting the projection optical system with infrared rays, so that the optical member can be locally heated. According to this invention, it is provided with the infrared radiation and radiation mechanism which irradiates the optical member which comprises this projection optical system T with infrared rays, and can heat this optical member locally. Therefore, Jiang Bao #… the pattern of the first mask is transmitted through the projection optical system == on the object (at the time of exposure), even if the progeny component constituting the projection light is partially (unevenly) added due to the irradiation of the energy beam In the case of I, it is also possible to irradiate infrared rays with an infrared irradiation mechanism, and to heat the optical member substantially uniformly at other parts of the μ optical member that are not heated by the irradiation of the energy beam. According to 、, °, b, ^, ^ According to this, this suppresses the occurrence of the correction of the aberration of the projection optical system caused by the unevenness of the optical components due to heating. In this case, because the heating of the optical structure # by the Ran LM and Bu line irradiation mechanism can also be performed during exposure Yin, the plate member can more reliably suppress the occurrence of the projected light phase. Therefore, it can be good. The projection characteristics of the asymmetry aberration pre-maintaining system are adjusted to advance the exposure characteristics of the system into 14 200423224 lines: to achieve high-precision exposure. I β a external light irradiation mechanism, by adding the optical component locally Γ and the thermal polarization structure 2Γ ′ generated by the energy beam irradiation in the optical component. The optical component may be a refractive optical element, or the light :: element may also be a reflective optical element. If the latter is a radiation mechanism system The reflection optics are opened by the ffl line, " In cattle, to reflect the lunar surface of the reflecting surface of the energy beam, and irradiate the infrared rays. The second oR output of the present invention | The infrared irradiating mechanism can irradiate a part of the surface of the light member. "This%, part of the surface of the optical member, when the pattern image is projected on the photosensitive object, it is not A, the woman is virgin." This catching rabbits surface of the optical member of the sub-beam irradiation square date of invention * optical device, the lens system of the optical member constituted of fluorite, the infrared irradiation means, can be called a wavelength of 6 - the degree of the optical irradiation member. 2. The second exposure unit of the present invention is composed of V. ,, ^, and the external line irradiation mechanism includes a plurality of optical fibers, one end of which is arranged near the flower and the broadcast sub-member to irradiate the parallel member. infrared. The first and second exposures w φ of the present invention can be further provided with a driving mechanism in the ui clothes to drive at least one of the optical components constituting the projection optical system, and the light driven by the projection optical system Axis direction. In the first 帛 2 exposure apparatus of this month, the energy beam is a fluorine laser light having a wavelength of 157 nm or a pseudo excimer laser light having a wavelength of 19-. 15 200423224 The exposure method according to the third aspect of the present invention is characterized by comprising: a transfer process, irradiating a photomask disposed on the first surface with an energy beam, and transferring the pattern formed on the photomask through a projection optical system. Printed on a photosensitive object arranged on the second surface; and an irradiation process in a state where the photosensitive object is not arranged, in order to ease the irradiation of the optical member in the projection optical system by the energy beam during the transfer process The irradiation conditions of the generated thermal offset state do not pass through the mask, and irradiate the projection optical system with a virtual irradiation energy beam. According to this invention, the photomask disposed on the first surface is illuminated with energy beam, and the pattern formed on the photomask is transferred to the photosensitive object disposed on the second surface through the projection optical system (transfer process). In the state where the photosensitive object is not arranged on the second surface, the condition that is sufficient to alleviate the thermal bias state of the optical material in the projection optical system of the above-mentioned transfer process due to the irradiation of the energy beam is used as the radiation condition. Through the reticle, the projection optical system is irradiated with a virtual beam (","). Therefore, even in the transfer system, the photonic material constituting the projection system is locally (unevenly). Heating, but the optical material can still be heated to a nearly consistent state by the treatment of the irradiation process. The above-mentioned makeup and shot process disclosed by Jin can be performed after the transfer process or before. One method can suppress the uneven heating of optical materials, avoid the occurrence of rotational asymmetric aberrations that are difficult to compensate for the projection optical system, and maintain the good imaging characteristics of the projection optical system to achieve high-precision exposure. : 时 '可可-Steps included before the irradiation process, insert a beam splitter 2 :: beam: system in the optical path space; in this irradiation process, the energy beam for virtual irradiation is irradiated through the knife action 16 200423224 In the first exposure method of the present invention, the irradiation process is performed when the photosensitive object is exchanged on an object stage holding a photosensitive object. The exposure method of the fourth aspect of the present invention is characterized in that: With the L •• transfer process, the mask is illuminated with an energy beam, and the pattern formed on the mask is transferred to the photosensitive object through the projection optical system; and the heating process is used to irradiate the optical components constituting the projection optical system Infrared light to locally heat the light and the component.% According to the invention, the photomask is illuminated with an energy beam, and the formed pattern is transferred to a photosensitive object through a projection optical system (transfer, to a component constituting the projection optical system). The optical component is irradiated with infrared rays: the component (heating process). Therefore, even in the transfer process, the optical material constituting the projection optical system in the transfer clothing is locally (Unevenly, u support the irradiation of the beam here and ^^ _) The heating% can also heat the optical components that are not heated by the beam of the heart during the heating process, so the other parts are irradiated with infrared rays to add evidence Therefore, the state is always / the optical component is heated to almost the same state. The second system: the occurrence of the projection optical pair formation caused by the uneven heating of the optical component. In this case, '*, so it is the same as the first dagger, 'The rotation of the optical system can also be performed in the exposure, compared to', which can more surely suppress the occurrence of the projection quarter optical aberration. Therefore, it can expose the imaging characteristics of the exposure system with good dimensions, In order to achieve high accuracy in this case, the ',,, and clothing' caused by the poor beam is considered by the heat distribution of the energy sub-members irradiated in the transfer process, and the heating is performed so that the heat distribution is equal to 17 200423224 of the optical member. The optical axis is the result of rotational symmetry. In this case, in the heating process, the optical member may be irradiated with infrared rays by a plurality of optical fibers. In this case, the heating process may irradiate the optical member with infrared rays from at least one of the plurality of optical fibers in response to the thermal offset of the optical member. In this case, the part of the surface of the optical member that is not irradiated with the energy beam can be projected on the photosensitive object during the infrared irradiation position. < The first aspect of the present invention is performed simultaneously. In the 2 exposure method, the transfer process and the heating process are the element manufacturing method according to the aspect 5 of the present invention, which includes a lithography process, and the special feature is that the lithography process uses the i and the second exposure wear of the present invention. Either way, a circuit pattern is formed on a photosensitive object. , Called Gan W Dan and Ku Hu Ge are formed from the second wafer with the [1 1 1] axis approximately the same, formed on the long side of the gate pattern of the gate graph on the 4 silicon wafer, which is related to [110 ] The orthogonal directions of the axis direction or its equivalent axis direction are the same. Alternatively, the photoreceptor system is perpendicular to the main body of the pot, and has a surface axis and a crystal axis [110] axis approximately-so that when the wafer is formed on the circle, the long side direction of the closed pole graph is related to [110]. ] The orthogonal directions of the axis direction or its equivalent axis direction are the same. [Embodiment] "First Embodiment" An embodiment. Hereinafter, the eighteenth 200423224 of the present invention will be described with reference to Figs. 1 to 10. Fig. 1 is an exposure device according to the first embodiment of the present invention. The device is shown in a straight line. The energy beams in the outer regions of the exposure light E / ..., 4 are used as exposure radiation
盥作A片11 罩之私線片R,精由該標線片R :: 為感先物體的晶The toilet thread A is a private thread piece R covered by the 11 piece, and the marking piece R :: is the crystal of the first object
=相對曰知描,來將標線片R的圖案透過投影光學系統PL 光方,係步進掃描式(办p and SCan)的投影曝 尤万式,亦即所謂的掃描步進器。 該曝光裝置10°包含光源101及照明單元ILU,1中 照明系 >统’其係藉曝光用照明光(以下稱為「曝光 :先」Μ來照明標線片R;標線片載台m,其係用以保 寺標線…載台;投影光學系、統孔,其係用以使標線片 R射出的曝光用光EL投射於晶圓评上;以及晶圓載台m ,其係為載物載台,用以保持晶圓w。 上述光源1G1係使用輪出波長(振盈波長η%的氣 田射光(f2雷射)。又’光源1〇1亦可使用屬於波長約 12〇m„〜18_的真空紫外域之其他光源,例如,輸出波長 146nm的氪二分子雷射叫雷射)、輸出波長126⑽的氯二 分子雷射(Ah雷射)、或是輪出波長193nm的ArF準分子雷 射等。 光源101透過具有由光束擴徑器103a、柱面透鏡i〇3b 等光學兀件構成光束整形光學系統21的送光光學系統(光 束路徑,即beam line)l〇2,連接至構成照明單元ILU之 照明系統外殼105的-端。光源1〇1之實際設置處,並非 含照明單元ILU及投影光學系統札等曝光裝置本體所設置 19 200423224 的無塵室,而係潔淨等級較低的其他空間,或是設置於無 塵室地板下之公設管線等。 上述照明單元 ILU具備:照明系統外殼1 〇5 ;繞射光 學單元106,係以既定之位置關係配置於其内部;中繼透 鏡107, 109;反射鏡108;光學積分器11〇;照明系統孔 徑光闌板111 ;中繼透鏡112、114 ;作為視野光圈之標線 片遮板(reticle blind)機構BL;由彎曲反射鏡115及聚束 器116等所構成之照明光學系統。再者,本實施形態係以 ^眼透鏡作為光學積分器110,因而,以下的敘述中,有 時亦適需要以「複眼透鏡110」稱之。 上述繞射光學單元106具備了 2個繞射光學元件6a, 6b ’以及用以保持該繞射光學元件6a,此於既定位置關係 之保持器6c(參照圖9)。保持器“係藉由未圖示的控制裝 置及未圖#的驅動機才冓,使之進行旋轉或滑動式的驅動, 進而選擇繞射光學元件6a,6b的其中—者,設定於發自光 源101的照明光(雷射光)之光程上。 作為上述一繞射光學元件6a’其用途在於,係使入射 的照明光發散於既定角度範圍,俾成為具既定廣度之光束 :入射至酉己置於光錢方的才复眼透鏡110 _入射面。本實 也形‘%中’繞射光學元件6a主要使用於後述之小α照明的 知明條件中。 久又,另一繞射光學元件6b的用途在於,其係具有繞射 子圖木(簽知、圖9),當裝置係由配置於複眼透鏡110的 射出側焦點面、構成照明系統孔徑光闌板lu的複數個孔 20 200423224 徑光闌當中,選取係在離光軸既定距離處具有開口之後述 的變形照明光圈等孔徑光闌時,能夠使入射的照明光以較 廣的角度範圍發散,以較佳的效率使照明光束聚光至該變 形照明光圈之開口部的相當位置。 作為上述光學積分器之複眼透鏡丨丨0,係在其射出側 焦點面與照明光學系統的瞳面(照明於標線片R上的各位置 之照明光,其主光線的收斂面)一致之狀態下配置,使照 明標線片R的照明光之照度分布均勻化。由該複眼透鏡 11 〇射出的光(紫外脈衝光)侷限為曝光用光源EL。 又’光學積分器110並非僅能使用複眼透鏡,亦可使 用八他的均勻化構件,例如玻離棒(四角柱的玻璃,利用 其側面的多次内面反射以使照度均勻化者)亦可使用。此 t由於必須使玻璃棒的射出側焦點面與標線片R圖案面 /、#厄面致,因此,係將標線片遮板機構bl配置於玻璃 棒的射出側焦點面,$配置於更接近標線# R側之該射出 側焦點面之共輛面,又,此時,係將繞射光學元件^,肋 配置於玻璃棒的入射側焦點面,或配置於更接近光源ι〇ι ,的該:射側焦點面的共輛面附近。如此,在使用玻璃棒 呀’為貫現上述位置關係,必須變更照明單元⑽ 鏡或反射鏡之配置。 .........,,囚本實施形潑 以波長短於20—的紫外線作為曝光用光,故而,以截 =通過㈣長光之光學構件(合成石英或螢石、敦化鐘 ”]土。理所當然的,構成照明光學系統的其他透鏡材料 21 200423224 亦以能同樣使曝光波長完好通過的材料為佳。 上述妝明系統孔徑光闌板丨丨丨,係以配置於複眼透鏡 11 〇的射出面附近,亦即本實施形態中與照明光學系統的 目里面大致一致之該射出側焦點面内所配置的圓板狀材料所 構成此圓板狀構件(亦即照明系統孔徑光闌板11 1 ),係 以大致等角度的間隔,包含有例如彩虹光闌所構成的α光 闌、輪帶照明料輪帶狀孔徑錢1於變形光源用之複 數個(例如2個或4個)偏心開口所構成之變形孔徑光閣、 /以及虛擬照射用光闌等。再者,圖!中僅是其中2種之孔 仅光鬧亦即圖i 〇所不之σ光闌j 及虛擬照射用光閑 llb。由圖10可了解,虛擬照射用光圈lib之中,具有圓 形的遮光部,其係以土 γ,方向(相當於圖1中的:tz方向)中 ,光軸中心保有既定距離的2點為中心,而其他的部分為 々卜 ·- 一,·、叫,·,W 1工W衣置,在既, 範圍内連續變更開口徑。該σ光闌Ua,在大的開口徑^ ,係-般照明用的圓形光闌;在小開口徑時,係相干 、即σ值小的小σ光闌。 · 照明系統孔徑光闌板u i 制裝置來控制馬達等驅動裝置 光程上選取其中一個孔徑光闌 的旋轉,係藉由未圖示的控 11c’藉而在曝光用光el的 上述標線片遮板機構BL,其實際之配置面,係由標線 片R的圖案面之共軛面些微散焦的面,其包含始 ϋ# 4- 1 1 〇 U 疋私綠 ' &,其係具有既定形狀的開口部,用以規範標線 22 200423224 片R上之照明區域;以及可動標線片遮板113b,其係配置 於"亥固定標線片遮板的配置面附近之標線片R的圖案面的 共軛面,具有可變的開口部,可分別在對應於掃描方向及 與其正交的非掃描方向改變其位置及寬度。固定標線片遮 板113a的開口部,在位於投影光學系統pL的圓形視野内 之中央’形成直線伸展的細縫狀或矩形狀,其形成方向係 與掃描曝光時的標線片1^移動方向(γ軸方向)成為正交之χ 軸方向。 此時’掃描曝光在開始及終了係透過可動標線片遮板 113b更進一步局限其照明區域,以避免其他部分的曝光。 可動標線片遮板113b,係透過未圖示之驅動系統以未圖示 之控制系統來加以控制。 此處,簡要說明含光源101及照明單元ILlJ之照明系 統的作用,由光源101所射出的真空紫外域之光束(雷射光 束)’被光束路徑102中的光束整形光學系統21整形後, 射入照明單元ILU。射入照明單元ILU内的光束,穿透過 構成繞射光學單元106的繞射光學元件6a(或繞射光學元 件6b),經過中繼透鏡107,109及反射鏡1〇8,射入複眼 透鏡110。藉由該複眼透鏡11 〇轉換成強度(照度)分布大 致一致的曝光用光EL。又,穿透過配置於複眼透鏡丨丨〇的 射出面附近之照明孔徑光闌板Π1中的任一孔徑光闌後, 曝光用光源EL透過中繼透鏡112,以均一的照度,照明於 構成標線片遮板機構BL的固定標線片遮板U 3a。通過固 定標線片遮板113a的開口部之曝光用光el,通過可動標 200423224 線片遮板113b後,透過中繼透鏡114、f曲反射鏡n5及 聚焦透鏡116,以均一的照度,照明標線片r上之既定照 明區域(係以直線延伸;^ ‘ p 甲、X轴方向之細縫狀或矩形狀的照明 區域)。 此外,以真空紫外域的波長光作為曝光用光時,必須 要從其光程中排除氧、纟蒸氣、碳化氫系統等之氣體,亦 即對上述波長帶的光具強吸收性之氣體(以下,適當的稱 「吸收性氣體」)。因& ’本實施形態中m统外殼 m的内部係充滿其吸收力較吸收性氣體為弱的氣體,例 氮或氣1 n、氧等稀有氣體、或是該等之混合氣 體(以下,稱「低吸收性齑挪 、^ ,, m •叹性軋體」)。其結果,照明系統外殼 105内的吸收性氣體的濃度成為數ppm以下。 又,本實施形態中,光源1〇1及送光光學系统ι〇2的 内部光程’亦與上述照„、1G5同㈣充滿低吸收 性氣體。 照明單元ILU的曝光用光EL之射出$,係透過伸縮 如的密封機構(風箱)18設有作為第i光罩平台之照明系 :平台2。在該照明系統側平台2的下方,透過:投影 學系統PL間伸縮自如的密封機構(風箱)29設有作為第 光罩平台之投影系統側平台3^在該照明系統側平台2 投影系統側平台3之間’以一定間隔形成複數根(此處為 根)支持柱(spacer,間隔件)26a〜26d,(圖i中並未圖 支持:26c’ 26d’可參照4A、圖4B),投影系統側平 係藉由i设於無塵室地面之未圖示的支持構件,將上 24 支持為水平。 上述照明系統側平台2及投 由天然石、陶究、或不鏽鋼等材質所开心平台3’係分別 亦即照明系統側平台2的下面及投影 分別被施以研磨而成為1平口 3的上面) 又,平…的材質係天:石之平滑平面。 -表面塗布氟素樹脂等希子 蒸氣。 在表面吸附或脫離氧或水 在該等平台2,3中,拟#古国, 〇 ^成有圖1所示般的矩形開口部 ,3a,以作為供曝光用光束穿透的光穿透部。 ^述標線片載台RST,係配置在照明系統側平台2及 統側平台3之間,分別對上述平台保有既定間距, 片、=Γ广線片/可至少移動自如於γ轴方向。標線 口 _ 6’位置貧訊’係透過設於標線片載台m的移 鏡,經由圖1所示之標線片雷射干涉儀9,可怪常保有 例如0.5〜lnm的解析精度。標線片載台RST及標線片雷射 干涉儀9等之構成,將於梢後進一步詳述。 上述投影光學系統PL,係使用兩側為遠心縮小系統、 且其光軸具有共通的z軸方向、由複數枚透鏡元件(透鏡 )恤〜30K參照圖7)所構成之折射光學系統。該投影光學 系統PL的投影倍率々例如係"“戈1/5。如之前所述般, 當照明單7L ILU的曝光用光EL照射於標 標線片R的電路圖案中,受曝光用光EL照明的(相當於上 述照明區域)像,藉由投影光學系統pL而縮小轉印在晶圓 25 200423224 W上之曝光照射區域(shot)之一部分,形成電路圖案的縮 小像(部分倒立像)。 構成投影光學系統P L之透鏡3 0 a〜3 0 j中’例如,位 於最上部的透鏡3Oa,係如圖1所示般,由作為驅動機構 的壓電元件PZ來支持於3點。藉由該3個壓電元件pz, 使透鏡30a驅動於光軸方向(Z軸方向)及傾斜於XY平面的 方向。 如圖1所示般,投影光學系 供氣管路50的一端,及排氣管路51的一端。供氣管路5( 的另一端,則接至未圖示之低吸收性氣體(例如氦氣)的供 應I置。又’排氣管路51的另一端,連接至外部的氣體回 收裝置。故,來自氦氣供給裝置的高純度氦氣,透過氦氣 供給管路50,流向投影光學系統pL的鏡筒内部。此時, 鏡筒内的氣體透過排氣管路51回收至氣體回收裝置,進而 再被利用。再者,發明巾之所以使用氦氣作為其低吸收姓 亂體,除了與上述相同的理由,可由鏡筒内的光程排除氧 、水蒸氣、碳化氫系統氣體等對真空紫外域的光源具強效 收力的氣體,亦著眼於其極佳的冷卻效果。亦即,:實摊 形態中:由於係以真空紫外光為曝光用光EL,因而以:膨 脹係數㊅的榮;5來作為構成投影光學系統pL的透鏡材料。 因之,透鏡因吸收曝光用光乩而發生之溫度上昇, 化透鏡的成像特性。故而,最好 #曰 他低吸收性氣俨為佳的# ,較氮等其 汽内…/、 來作為投影光學系統PL的鐘 同内部之潔淨氣體。 月 26 200423224 :述晶圓載台w係配置於晶圓室40内。該晶圓4〇 係由與投影光學系統PL的鏡筒無鏠接合的間隔壁7】所包 覆,使其内部氣體與外部隔離。晶圓4〇的間隔壁?!係由 不鏽鋼(SUS)等脫氣性低的材料所形成。 ” 晶圓40之内,基座(⑹挪係透過複數個防振單元 :而:皮水平支持著。為避免因晶圓载台WST的移動而將振 動傳達至投影光學“ PL或標線m防振單元86且 二”等級之絕緣能力。再者,理所當然的,亦可根據於 =在#置内的-部分之半導體加速度計等振動感測器的 :出值’對基錢的振動主動控制,亦即所謂主動式防振 #置,來作為上述的防振單元86。 上述晶圓載台wst錢過晶圓保持具25以直空吸附等 方式來吸附晶圓W並加以保持,藉由例如線性馬達等所構 成之未圖示的驅㈣統,驅動自如於上述基座 XY2維方向。 瞧、二本實施形態所示,使用真空紫外域為其曝光波長之 1^置中,為避免氧氣等吸收性氣體吸收曝光用光,對 ^〜光予系統PL至晶ID w止的光程亦須置換成氮或稀 體0 ^ :圓室40的間隔壁71係如圖1所示般,分別連接至 供風官路41的一端,及排氣管43的一端,供氣管路41的 他立而’係連接曼去 _ … 较主禾圖不的低吸收性氣體之供給裝置,例如 氮氣之供驶吳 ^ 、、°表置。又,排氣管路43的他端係連接至外部的 氣體回收梦署。ν 、置 又’與上述相同地,在晶圓室40内常保氦 27 200423224 氣之流動。之所以採用氦氣作為其低吸收性氣體的理由, 以及回收後如何再利用氦氣,係與上述相同。 在上述日a圓至40的間隔壁71之+ Y側的側壁,設有 光穿透窗8 5。與此相同的,僅管圖示已予省略,在間隔壁 71的+ X側(圖1中的紙面深側)之側壁,亦同樣設有光穿 透窗。戎些光牙透窗之構成,係在形成於間隔壁7 1的窗部 (開口部),$裝用以阻隔該窗部的光穿透材料,而此處係 指一般的光學玻璃。此時,為避免在構成光穿透窗85的光 穿透構件之安裳部分發生漏氣現象,乃對安裝部位使用銦 或銅等金屬密封間、或使用氟素系樹脂施以 作業。又,作為上職«樹脂,最好是能使^80。= 施以2小時之加熱、脫氣處理之物。 在上述晶圓保持具25的+ γ側之端部,於χ軸方向延 伸由平面鏡所構成之移動鏡56Y。由配置於晶圓室4〇的外 部之Υ軸雷射干涉冑57Υ所發出的測長用雷射光,透過光 穿透窗85幾近垂直地投射於該具¥軸移動鏡56γ,复反射 光則透過光穿透窗85’經過γ轴雷射干涉儀57γ内部 測器之感光,可檢出以Υ軸雷射干涉物内部的灸昭; 之位置為基準時,Υ移動鏡56γ的位置、亦:兄 軸位置。 W的Υ a同樣的,料略圖示,在晶圓保持具25的+X側之# 部’於Y軸方向延設由平面鏡所構成之又移動鏡而 射干涉儀透過…動鏡以上述之同樣方法’ 私動鏡的位置、亦即晶圓W6U軸位置。上述2個雷射干 28 200423224 涉儀的檢測值(量測值)係供應至未圖示的控制裝置,控制 裝置一邊邊I測此等雷射干涉儀的檢測值、一邊透過晶圓 驅動系統來進行晶圓載台WST的位置控制。 如前所述,由於本實施形態之雷射干涉儀,亦即雷射 光源、稜鏡等光學構件及感測器等,係配置於晶圓室40的 外部,因此即使上述感測器等產生微量的吸收氣體,亦不 致對曝光造成不良影響。 又,上述投影光學系統PL的間隔壁所連接的供氣管路 50的他端,以及排氣管路51的他端,亦可分別連接至未 圖不之氦氣供應裝置,俾由氦氣供應裝置透過供氣管路 隨時將高純度氦氣供應至投影光學系統pL内,投影光學系 統PL的内部氣體則透過排氣管路51回到氦氣供給裝K ,以上揭方法來構成循環使甩氦氣之機制亦佳。此時,在 氦氣供應裝置中最好是能内建氣體精製裝置。如此,藉由 2體精製裝置的作用,即使氦氣在包含氦氣供應裝心投 影光學系統PL内部之循環路徑中,經長時間的循環使用後 ’仍能將投影光學系統PL内的氦氣以外的吸收性氣體(氧 、水蒸氣、有機物等)濃度控制在數ppm以下。又,此時, 亦可在投影光學系統PL内設置壓.片 、 卢^一x置&刀感測益、吸收性氣體濃 -感心寻感測器,根據該感測器之量測值,透過 之控制裝置,以決定該内建氣 θ 與停止。 、應裝置内之系的啟動 徑 同樣的 晶圓室40亦可採用與上述相 同的氦氣循環路 29 200423224 接著,根據圖2〜圖,詳述標線片載台RST的構成 '' 圖2係省略標線片載台RST的一部分之立體圖,圖3 係払線片載台RST之縱截面圖。又,圖4A係圖3的A—A 線截面圖’圖4B係圖3的B — B線截面圖。 軚線片載台RST,如前所述,被挾於照明系統側平台2 〜糸、、先側平台3間,分別以非接觸方式保持於平台2 3。此標線片載台RST,如圖2所示,具備標線片粗動載台 、及‘線片微動載台5,標線片微動載台係被標線片粗 動載〇 4圍於土z方向及_γ方向之三個方向所保持。 、,上述標線片粗動載台4,具備:上板部恤,係以數微 米之極小間隔配置於上述照明系統側平台2的下方;下板 部46c,係以數微米之極小間隔配置於投影系統側平台3 的土面;以及中間部46b,係位於上板部_與下板部術 間的位置以連結兩者。 q㈣丨用囬,透過支4 構件47a,47b配設有線性馬達RM1,趣的可動件他 48b(圖2中並未圖示支持構件…及可動件他,社夫日 圖4A)。該等可動件48a,傷經由與延展於= 子49a,49b之間的電磁相互作用,而驅動於”由方向, 此將標線片粗動載台4驅動於γ軸方向。 ° 1 又,上述定子49a,49b,亦可藉由支持平台2 3之 未圖示的架台來加以支持,然而,亦可在無塵室的地 上透過防振機構配設未圖示之支持機構,藉此 上 定子之支持物亦可。又,可動件.〇u ^ ^ 件48a,權的安裝位置並不 30 200423224 :限於上述下板部46c,亦可裳置於中間部46“ 線片粗動載台4係與此等可動件恤,概―體 ’‘ 而,繼產生的推力來進行加減速,因而,其安裝位置達( 南度方向的位置)最好是能與標線片粗動載台4整體的重、 位置一致。 版的重心 本實施形態中’照明系統側平台2及投 3分別對向於標線片粗動載…面,係分別平行於二; 片粗動載Μ的上面及底面。因此,即使標線片粗動^ 如上述般被線性馬達机讀驅動於Υ轴方向時,^ 2, 3及標線片粗動載台4間的微小間隔亦能大致保持一: 上述中間46b,如® 4Β所示,埋有由音圈馬達㈣ 構成之γ軸微致動器AC1,AC2、及χ軸微致動器似。;亥 些微致動器似〜AC3之可動件,係分別透過載台保持㈣ 42:: 42b,42c連接至標線片微動載台5。因而,藉由微致 動器AC1〜AC3的驅動,將標線片微動載台5微驅動於X軸 方向、Y軸方向、及ΘΖ方向(z軸旋轉之旋轉方向)。再者 ,本實施形態中為抑制微致動器AC1,AC2的溫度上昇,其 構成中,係使其一部分露出於中間部46b的外側,以利於 放熱。 又,標線片粗動載台4中,具有差動排氣型氣體靜壓 軸承,用以維持與照明系統側平台2及投影系統側平台3 間的既定間隙’亦具有差動排氣型氣體靜壓軸承用以維持 與標線片微動載台5間的既定間隙,惟此點將再詳述於後。 31 200423224 回到圖2,上述標線片微動载台5,具備底 Η 、以及固定於該底面構件55上面之間隔壁Μ。 上述底面構件55,如圖4B所示,係由把处 ,在其中央部附近形成矩形之曝光用開口' ,件構成 用開口 55…Y側形成虛擬照射用之照射用開口 ::: 大小大致等同㈣光之際該曝光用光EL照射於 二 明區域)大小。又’曝光用開口 55a的周邊部,設 有複數個(此處為4個)標線片保持機構53。 上述標線片保持機構53,係透過導入底面構件5 的真^線54等,連接至設於曝光裝置内之未圖示的真空 泵’當標線片R被載置於標線片保持機構53 二 空泵的作動,使標線片R被吸附保持於標線片保持機曰構Μ 。又’上述真空管線54係經由標線片粗動載台4,由 f體接頭等之氣體導入端子,導入標線片微動载台5的内 二。=、線片粗動載台4内的真空管線44係與連接於致動哭 寺之其他電氣配線一併被集束於配線I 39,連接至真心 。又’上述真空泵可設於曝光裝置内,亦可使用來自半導 體工廠的真空用管線、或使用減壓空氣用管線亦可。 所說明的真空泵亦與上述相同。 係圍繞於四方;以及 之圖3所示的矩形開 ’與通過曝光用光EL 55b、及兩開口 55a, 更要大上許多。藉由 上述間隔壁52,係由:側壁部, 頂板部,係具有設於側壁部上端中央 口 52a。矩形開口 52a,如圖3所示 的上述曝光用開口 55a、照射用開口 55b間的切除部分之合計面積相較, 32 200423224 間隔壁52及上述底面構件55,形成標線片之保持空間% 。又,頂板部的上端面,係如後述般形成對向的環狀凹槽 58, 59 。 、曰 又,在標線片微動載台5的保持空間SS的外側,於間 隔壁52的—X側面,如圖4B所示,設有平面反射鏡9U。 設在該一X側的標線片雷射干涉儀9c所發出的光束照射於 孩平面反射鏡91c,俾藉由標線片雷射干涉儀9c,持續檢 測標線片微動載台5(亦即標線片㈧的χ軸方向位置,可達 例如0.5〜lnm左右之解析能力。 再者,在間隔壁52的外側(保持空間SS的外側),於 底面構件55的+ γ側端部附近,透過安裂構件 104b(參日召’ …、Θ 2),配設有倒反射鏡9ia ㈣leCt〇r)’以作為反射構件。來自標線片雷射 ^義9a,9b之雷射光,分別照射於倒反射鏡91a,91b 击=由標線片雷射干涉儀9a,9b,分別檢出在該雷射光 向位置、射&塊:標線片微動載台5(亦即標線片_ Y軸方 個標線片::常保例如〇.5〜1nm的解析能力。又,根據2 ,:户線二·干Γ義9a,肋的檢出值之差與光束間的距離 便線片做勁载台5 (亦g炉令 之旋轉方向)旋轉(偏轉)"祕方面(z轴旋轉 :者’亦可對底面構件55的]側端 9ia,91卜 代上述平面反射鏡9lc、倒反射鏡 接著,根據圖 詳細說明設於標線片粗動载台4之 33 200423224 氣體靜壓軸承。 首先’說明形成標線片粗動载台4及投影系統側平台 3間的微小間隔之差動排氣型氣體靜壓軸承(以下,稱「第 1軸承」)。 在標線片粗動載台4之下板部46c的底面,從外緣部 之偏内側處形成供氣側環狀凹槽3卜在該供氣側環狀凹槽 31的外側形成排氣側環狀凹槽32。供氣㈣狀凹槽31 ^ 過標線片粗動載台4内所形成的供氣管路 37的-端,該供氣…另-端則連接至未圖示= 供應裝置。又,排氣側環狀凹槽32透過標線片粗動載台4Relatively speaking, the pattern of the reticle R is transmitted through the light side of the projection optical system PL. It is a step-and-scan type (p and SCan) projection exposure method, which is also called a scanning stepper. The exposure device 10 ° includes a light source 101 and an illumination unit ILU. The lighting system of the 1 > system 'uses illumination light for exposure (hereinafter referred to as "exposure: first" M to illuminate the reticle R; the reticle stage m, which is used to protect the reticle ... stage; projection optics, uniform hole, which is used to project the exposure light EL emitted by the reticle R on the wafer evaluation; and wafer stage m, which It is a stage for holding the wafer w. The above-mentioned light source 1G1 uses a round-out wavelength (the gas field emission light (f2 laser) of the vibrational wavelength η%). Also, the light source 10 can also be used, which belongs to a wavelength of about 12 〇m „~ 18_ Other light sources in the vacuum ultraviolet range, for example, a two-molecule laser with an output wavelength of 146nm is called a laser), a chlorine two-molecule laser (Ah laser) with an output of 126⑽, or a turn-out wavelength ArF excimer laser at 193 nm, etc. The light source 101 passes through a light transmission optical system (beam line) that has a beam shaping optical system 21 formed by optical elements such as a beam expander 103a, a cylindrical lens 103, and the like. 〇2, connected to the-end of the lighting system housing 105 constituting the lighting unit ILU. The actual setting of the light source 101 It is not a clean room that contains the lighting unit ILU, projection optical system, etc. 19 200423224, but other spaces with lower cleanliness, or public pipelines installed under the floor of the clean room. The lighting unit ILU is provided with: a lighting system housing 105; a diffractive optical unit 106, which is arranged in a predetermined positional relationship; relay lenses 107 and 109; a reflecting mirror 108; an optical integrator 11; an aperture light of the lighting system The diaphragm 111; the relay lenses 112 and 114; the reticle blind mechanism BL serving as the diaphragm of the field of view; the illumination optical system composed of the curved reflector 115 and the condenser 116. Furthermore, this embodiment The morphology uses an eye lens as the optical integrator 110. Therefore, in the following description, it may be appropriate to call it a "fly eye lens 110." The above-mentioned diffractive optical unit 106 is provided with two diffractive optical elements 6a, 6b. 'And a retainer 6c (refer to FIG. 9) for retaining the diffractive optical element 6a in a predetermined positional relationship. The retainer “is controlled by a control device (not shown) and a driver (not shown). Proceed Rotary or sliding drive, and then one of the diffractive optical elements 6a, 6b is selected, which is set on the optical path of the illumination light (laser light) emitted from the light source 101. As the above-mentioned diffractive optical element 6a ', its use The reason is that the incident illumination light is diffused in a predetermined angle range, and becomes a beam of a predetermined breadth: it is incident on the compound eye lens 110 _ incident surface that has been placed in the light money side. The real shape is also '% 中' diffraction The optical element 6a is mainly used in the known condition of the small alpha lighting described later. For a long time, another purpose of the diffractive optical element 6b is that it has a diffractive sub-pattern (signed, Fig. 9). A plurality of apertures 20 200423224, which are arranged on the exit-side focal plane of the fly-eye lens 110 and constitute the aperture stop plate lu of the lighting system, select aperture light such as a deformed illumination aperture described later having an opening at a predetermined distance from the optical axis. At the time of the diaphragm, the incident illumination light can be diffused in a wide range of angles, and the illumination beam can be focused to a position corresponding to the opening of the deformed illumination aperture with better efficiency. The compound eye lens of the above-mentioned optical integrator 丨 0 is the same as the pupil surface of the illumination optical system (the illumination light illuminated at each position on the reticle R, and the convergence surface of the main ray). It is arranged in a state to make the illuminance distribution of the illumination light of the reticle R uniform. The light (ultraviolet pulsed light) emitted from the fly-eye lens 110 is limited to the exposure light source EL. Moreover, the optical integrator 110 can not only use a fly-eye lens, but can also use a homogenizing member such as a glass ionization rod (a glass with a quadrangular prism, which uses the multiple internal reflections on its side to make the illumination uniform). use. Since the focal side of the exit side of the glass rod must be the same as the R pattern surface of the reticle, the reticle shield mechanism bl is arranged at the focal side of the exit side of the glass rod. It is closer to the common surface of the exit side focal plane on the #R side, and at this time, the diffractive optical element ^ is placed on the incident side focal plane of the glass rod, or it is closer to the light source. ι, of the: near the car surface of the focal side of the shooting side. Thus, in order to realize the above-mentioned positional relationship when using a glass rod, it is necessary to change the arrangement of the illumination unit, the mirror, or the reflector. ........., the implementation of the prisoner uses ultraviolet light with a wavelength shorter than 20- as the exposure light, so the optical component (synthetic quartz or fluorite, Dunhua bell "] Soil. Of course, the other lens materials 21 200423224 constituting the illumination optical system are also preferably materials that can also pass the exposure wavelength intact. The aperture diaphragm plate of the above-mentioned makeup system is arranged on the fly-eye lens 11 The disk-shaped member (that is, the aperture stop of the lighting system) is constituted by the disk-shaped material arranged in the focal plane of the emission side, which is approximately the same as that of the illumination optical system in this embodiment. The plate 11 1) includes, at approximately equal angular intervals, an alpha diaphragm made of, for example, a rainbow diaphragm, a belt lighting material, a belt-shaped aperture, and a plurality of deformed light sources (for example, two or four). ) Deformed-aperture apertures composed of eccentric openings, and / or diaphragms for virtual illumination, etc. In addition, only two of the holes in the picture! Are light only, that is, σ diaphragm j and virtual ones that are not shown in figure i 〇 The light used for irradiation is llb. As can be understood from FIG. 10 In the aperture for virtual illumination lib, there is a circular light-shielding portion, which is centered at 2 points with a predetermined distance in the center of the optical axis in the direction of soil γ (equivalent to the tz direction in FIG. 1), and other The part is 々 ·· ,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, 1. The opening diameter is continuously changed within the existing range. The σ diaphragm Ua, with a large opening diameter, is used for general lighting. At the small opening diameter, it is coherent, that is, a small σ diaphragm with a small σ value. · Aperture diaphragm plate of the lighting system controls the motor and other driving devices to select one of the aperture diaphragms in the optical path. The rotation of the reticle is based on the above-mentioned reticle masking mechanism BL for the exposure light el by the control 11c ′ (not shown). The actual arrangement surface is slightly conjugated to the conjugate surface of the pattern surface of the reticle R. A defocused surface, which includes ϋ # 4- 1 1 〇U 疋 私 绿 '& which has an opening of a predetermined shape to regulate the lighting area on the marking line 22 200423224 slice R; and a movable marking line Sheet mask 113b, which is a pattern of the reticle R arranged near the arrangement surface of the " Ha fixed reticle mask The conjugate surface has a variable opening, and its position and width can be changed in the non-scanning direction corresponding to the scanning direction and orthogonal to it. The opening of the fixed reticle shield 113a is located in the projection optical system pL. The center of the circular field of view forms a slender or rectangular shape that extends linearly, and its formation direction is the χ-axis direction that is orthogonal to the moving direction (γ-axis direction) of the reticle 1 during scanning exposure. 'Scanning exposure at the beginning and end is further limited by its movable reticle mask 113b to avoid exposure of other parts. The movable reticle mask 113b is not shown by a drive system (not shown). Control system to control. Here, the function of the illumination system including the light source 101 and the illumination unit IL1J is briefly described. The light beam (laser beam) in the vacuum ultraviolet range emitted by the light source 101 is shaped by the beam shaping optical system 21 in the beam path 102, Into the lighting unit ILU. The light beam entering the illumination unit ILU passes through the diffractive optical element 6a (or the diffractive optical element 6b) constituting the diffractive optical unit 106, passes through the relay lenses 107, 109, and the reflective mirror 108, and enters the fly-eye lens. 110. The fly-eye lens 110 converts the exposure light EL with a substantially uniform intensity (illumination) distribution. In addition, after passing through any aperture stop of the illumination aperture stop plate Π1 disposed near the exit surface of the fly-eye lens 丨 丨 0, the exposure light source EL passes through the relay lens 112 to illuminate the constituent target with uniform illumination. The reticle shutter mechanism BL fixes the reticle shutter U 3a. The exposure light el passing through the opening of the fixed reticle shield 113a passes through the movable target 200423224 reticle shield 113b, and then passes through the relay lens 114, the f-curve mirror n5, and the focusing lens 116 to illuminate with uniform illumination. The predetermined lighting area on the reticle r (extends in a straight line; ^ 'p A, the slit-shaped or rectangular lighting area in the X-axis direction). In addition, when using the light in the vacuum ultraviolet region as the exposure light, it is necessary to exclude gases such as oxygen, krypton vapor, and hydrocarbon systems from its optical path, that is, gases with strong absorption for the above-mentioned wavelength band light ( Hereinafter, it is appropriately called "absorptive gas"). Because & 'In the present embodiment, the internal system of the m-system casing m is filled with a gas having a weaker absorption capacity than the absorptive gas, such as nitrogen or gas 1 n, rare gases such as oxygen, or mixed gas (hereinafter, Called "low-absorptivity, ^ ,, m • sigh rolling"). As a result, the concentration of the absorbent gas in the lighting system case 105 becomes several ppm or less. In this embodiment, the internal optical path of the light source 101 and the light-transmitting optical system ι02 is also filled with a low-absorptive gas at the same time as the above-mentioned photo 1G5. The exposure light EL of the illumination unit ILU emits $ The telescopic sealing mechanism (air box) 18 is provided with the lighting system as the i-th photomask platform: platform 2. Below the lighting system-side platform 2, through: the telescopic sealing mechanism between the projection system PL (Wind box) 29 is provided with a projection system side platform 3 serving as a first mask platform, and a plurality of (here, root) support columns (spacers) are formed between the illumination system side platform 2 and the projection system side platform 3 at a certain interval. (Spacer) 26a ~ 26d, (not shown in figure i support: 26c '26d' can refer to 4A, 4B), the projection system side plane is an unillustrated support member located on the floor of the clean room by i The upper 24 is supported horizontally. The above lighting system side platform 2 and the happy platform 3 'cast by materials such as natural stone, ceramics, or stainless steel are respectively ground and the projection of the lighting system side platform 2 are ground and polished. Become the top of 1 flat mouth 3) Also, flat ... The material is sky: smooth surface of stone.-The surface is coated with fluorine resin and other steam. The surface absorbs or desorbs oxygen or water. In these platforms 2, 3, it is planned to be # 古国, 〇 ^ becomes as shown in Figure 1. The rectangular opening 3a serves as a light penetrating portion through which the exposure light beam passes. ^ The reticle stage RST is disposed between the lighting system side platform 2 and the system side platform 3, and holds the above platforms, respectively. The predetermined distance, film, = Γ wide line film / can move at least freely in the direction of the γ axis. Marking port _ 6 'Poor position' is through a moving mirror set on the marking sheet stage m, through the mirror shown in Figure 1. The reticle laser interferometer 9 may blame the resolution accuracy of 0.5 to 1 nm, for example. The configuration of the reticle stage RST and the reticle laser interferometer 9 will be further detailed later. The optical system PL is a refractive optical system that uses a telecentric reduction system on both sides and has a common z-axis direction on the optical axis, and is composed of a plurality of lens elements (lenses) (~ 30K (see FIG. 7)). This projection optical system The projection magnification of PL is, for example, "Ge 1/5. As described above, when the exposure light EL of the illumination unit 7L ILU is irradiated to the circuit pattern of the reticle R, the image illuminated by the exposure light EL (equivalent to the above-mentioned illumination area) is projected by the projection optical system pL And a part of the exposure shot transferred on the wafer 25 200423224 W is reduced to form a reduced image (partially inverted image) of the circuit pattern. Among the lenses 3 0 a to 3 0 j constituting the projection optical system PL, for example, the uppermost lens 3Oa is supported at three points by a piezoelectric element PZ as a driving mechanism as shown in FIG. With these three piezoelectric elements pz, the lens 30a is driven in the optical axis direction (Z-axis direction) and a direction inclined to the XY plane. As shown in Fig. 1, one end of the projection optical system air supply line 50 and one end of the exhaust line 51. The other end of the gas supply line 5 (is connected to a supply of a low-absorptive gas (such as helium), not shown. The other end of the exhaust line 51 is connected to an external gas recovery device. The high-purity helium gas from the helium gas supply device passes through the helium gas supply line 50 and flows into the lens barrel of the projection optical system pL. At this time, the gas in the lens barrel is recovered to the gas recovery device through the exhaust line 51, Furthermore, the reason why the invention towel uses helium as its low-absorptance surname, besides the same reason as above, the optical path in the lens barrel can exclude oxygen, water vapor, and hydrocarbon system gas from evacuating the vacuum. The light source in the ultraviolet region has a powerful retracting gas, and also focuses on its excellent cooling effect. That is, in the real form: because the vacuum ultraviolet light is used as the exposure light EL, so the expansion coefficient is ㊅ Rong; 5 as the lens material constituting the pL of the projection optical system. Therefore, the temperature rise of the lens due to absorption of light exposure exposure, and the imaging characteristics of the lens. Therefore, it is best #, More nitrogen Wait for its vapor ... /, as the clean gas inside the clock of the projection optical system PL. June 26 200423224: The wafer stage w is arranged in the wafer chamber 40. The wafer 40 is formed by the projection optical system. PL ’s lens barrel is joined by a partition wall 7] to isolate the internal gas from the outside. The partition wall of the wafer 40 is made of a material with low degassability such as stainless steel (SUS). " Within the wafer 40, the pedestal is supported by a plurality of anti-vibration units: and: the level is supported. In order to prevent the vibration of the wafer stage WST from transmitting vibrations to the projection optics "PL or marking m Vibration unit 86 and two "grade insulation capacity. Furthermore, as a matter of course, it can also actively control the vibration of the base money based on the value of the -in part of the -semiconductor accelerometer and other vibration sensors. The so-called active-type anti-vibration unit is used as the above-mentioned anti-vibration unit 86. The wafer stage wst passes through the wafer holder 25 to adsorb and hold the wafer W by means of direct air adsorption or the like, for example, by A drive system not shown, such as a linear motor, can drive freely. The XY2 dimension of the pedestal. As shown in this embodiment, the vacuum ultraviolet region is used to set the exposure wavelength to 1 ^. In order to avoid the absorption of exposure light by absorbent gases such as oxygen, the light is applied to the system PL to the crystal. The optical path of ID w must also be replaced with nitrogen or rare earth 0 ^: The partition wall 71 of the round chamber 40 is connected to one end of the air supply official road 41 and one end of the exhaust pipe 43 as shown in FIG. 1. In the air supply line 41, it is connected to the supply device of low absorption gas, such as the supply of nitrogen gas. The exhaust line 43 The other end is connected to the external gas recovery dream department. Ν, Zhiyou ', as described above, keeps the flow of helium 27 200423224 gas in the wafer chamber 40. The reason for using helium as its low-absorptive gas and how to reuse helium after recovery are the same as above. A light transmission window 85 is provided on the side wall on the + Y side of the partition wall 71 from a to 40 yen. Similarly, although the illustration has been omitted, a light transmission window is also provided on the side wall of the + X side of the partition wall 71 (the deep side of the paper surface in FIG. 1). The structure of some light transmission windows is formed in the window portion (opening) formed in the partition wall 71, and is used to block the light penetrating material of the window portion, and here refers to ordinary optical glass. At this time, in order to prevent air leakage from occurring in the safety part of the light-transmitting member constituting the light-transmitting window 85, a metal seal room such as indium or copper or a fluorine-based resin is used for the installation portion. Also, as the job «resin, it is best to make ^ 80. = Heated and degassed for 2 hours. A moving mirror 56Y composed of a flat mirror is extended at the end on the + γ side of the wafer holder 25 in the x-axis direction. The length measuring laser light emitted by the Υ-axis laser interference 胄 57Υ arranged outside the wafer chamber 40 passes through the light transmission window 85 and is projected almost perpendicularly on the ¥ -axis moving mirror 56γ. Through the light penetrating window 85 'through the light of the internal sensor of the gamma-axis laser interferometer 57γ, the moxibustion can be detected based on the position of the y-axis laser interferometer; when the position of the Υ-axis laser interferometer 56γ is used as a reference, : Brother axis position. W Υ a is the same, the material is shown in the figure, and the # part on the + X side of the wafer holder 25 is extended in the Y-axis direction by a moving mirror composed of a plane mirror and the interferometer passes through the moving mirror. In the same way, the position of the private mirror, that is, the position of the wafer W6U axis. The detection values (measured values) of the above two laser stems 28 200423224 are supplied to a control device (not shown). The control device measures the detection values of these laser interferometers while passing through the wafer drive system. The position of the wafer stage WST is controlled. As described above, since the laser interferometer of the present embodiment, that is, the optical components such as the laser light source, chirp, and the sensor are arranged outside the wafer chamber 40, even if the sensor or the like described above is generated, A small amount of absorbed gas will not adversely affect the exposure. In addition, the other end of the gas supply pipe 50 and the other end of the exhaust pipe 51 connected to the partition wall of the above-mentioned projection optical system PL may be respectively connected to a helium gas supply device (not shown), which is supplied by helium gas. The device supplies high-purity helium gas into the projection optical system pL at any time through the gas supply line, and the internal gas of the projection optical system PL is returned to the helium gas supply device K through the exhaust line 51. The above method is used to form a cycle to throw helium The mechanism of Qi is also good. In this case, it is preferable that a gas refining device be built in the helium gas supply device. In this way, with the function of the two-body refining device, even if helium is in the circulation path inside the projection optical system PL including the helium supply center, after a long period of cycle use, the helium in the projection optical system PL can still be used The concentration of other absorptive gases (oxygen, water vapor, organic matter, etc.) is controlled to a few ppm or less. Also, at this time, it is also possible to set a compression lens, a lens, a knife sensor, and an absorptive gas concentration-sensing sensor in the projection optical system PL. According to the measured value of the sensor , Through the control device to determine the built-in gas θ and stop. The same wafer chamber 40 with the same starting diameter as that in the device can also use the same helium circulation path 29 200423224. Next, the structure of the reticle stage RST will be described in detail based on Figs. A perspective view of a part of the reticle stage RST is omitted, and FIG. 3 is a longitudinal sectional view of the reticle stage RST. Fig. 4A is a cross-sectional view taken along the line A-A of Fig. 3 'Fig. 4B is a cross-sectional view taken along the line B-B of Fig. 3. The holographic film stage RST is held between the lighting system side platforms 2 to 糸, and the front side platform 3 as described above, and is held on the platform 23 in a non-contact manner, respectively. This reticle stage RST, as shown in FIG. 2, includes a reticle coarse motion stage and a 'line micro motion stage 5'. The reticle micro motion stage is surrounded by the reticle coarse motion. The three directions of the soil z direction and the _γ direction are maintained. The coarse motion stage 4 for the reticle is provided with an upper plate shirt arranged at a small interval of a few micrometers below the lighting system side platform 2 and a lower plate portion 46c arranged at a small interval of a few micrometers. The earth surface on the projection system side platform 3; and the middle portion 46b are located between the upper plate portion and the lower plate portion to connect the two. q㈣ 丨 Using back, through the support 4 members 47a, 47b is equipped with a linear motor RM1, interesting moving parts 48b (the supporting members are not shown in Figure 2 ... and moving parts, Figure 4A). The movable members 48a are driven in the direction of "via" by electromagnetic interaction with the extensions 49a, 49b. This drives the reticle coarse motion stage 4 in the direction of the γ axis. ° 1 Also, The above-mentioned stators 49a and 49b can also be supported by a rack (not shown) supporting the platform 23, however, a support mechanism (not shown) can also be provided on the floor of the clean room through an anti-vibration mechanism, thereby The support of the stator is also available. Also, the movable part. 〇u ^ ^ piece 48a, the right installation position is not 30 200423224: limited to the above lower plate portion 46c, or can be placed on the middle portion 46 "wire coarse motion stage The 4 series is similar to these movable shirts, and the body generates acceleration and deceleration following the generated thrust. Therefore, it is best to install it at a position (south direction) that can move coarsely with the reticles. 4 The overall weight and position are consistent. The center of gravity of the version In this embodiment, the ‘lighting system side platform 2 and cast 3 are respectively opposite the coarse moving load surface of the reticle, which are respectively parallel to the top and bottom surfaces of the coarse moving load M. Therefore, even if the reticle coarse movement ^ is driven by the linear motor in the direction of the y-axis as described above, the minute interval between ^ 2, 3 and the reticle coarse movement stage 4 can be maintained approximately one: the above-mentioned middle 46b As shown in ® 4B, γ-axis microactuators AC1, AC2, and χ-axis microactuators composed of a voice coil motor ㈣ are embedded. These micro-actuators are similar to the movable parts of ~ AC3, and are respectively connected to the reticle micro-motion stage 5 through the stage holders 42 :: 42b, 42c. Therefore, the micro-actuators AC1 to AC3 drive the reticle micro-movement stage 5 in the X-axis direction, the Y-axis direction, and the θZ direction (the rotation direction of the z-axis rotation). Furthermore, in this embodiment, in order to suppress the temperature rise of the microactuators AC1 and AC2, a part of the configuration is exposed outside the intermediate portion 46b to facilitate heat release. In addition, the reticle coarse motion stage 4 has a differential exhaust type gas static pressure bearing for maintaining a predetermined gap between the lighting system side platform 2 and the projection system side platform 3, and also has a differential exhaust type. The aerostatic bearing is used to maintain a predetermined gap with the reticle micro-movement stage 5, but this point will be described in detail later. 31 200423224 Returning to FIG. 2, the reticle micro-movement stage 5 includes a base Η and a partition wall M fixed on the bottom surface member 55. The bottom member 55, as shown in FIG. 4B, is formed by a handle and a rectangular opening for exposure in the vicinity of its central portion. When it is equal to the light, the exposure light EL is irradiated to the Erming area). Also, a plurality of (here, four) reticle holding mechanisms 53 are provided in the peripheral portion of the exposure opening 55a. The above-mentioned reticle holding mechanism 53 is connected to a vacuum pump (not shown) provided in the exposure device through the true line 54 and the like introduced into the bottom surface member 5 when the reticle R is placed on the reticle holding mechanism 53. The operation of the two air pumps causes the reticle R to be adsorbed and held on the reticle holding machine M. The above-mentioned vacuum line 54 is introduced into the inside of the reticle micro-moving stage 5 through a gas guide terminal of the reticle coarse moving stage 4 through a gas introduction terminal such as an f-body joint. = 、 The vacuum line 44 in the wire coarse motion stage 4 is bundled with wiring I 39 together with other electrical wiring connected to the actuary crying temple and connected to the heart. The above-mentioned vacuum pump may be installed in an exposure device, or a vacuum line from a semiconductor factory or a line for decompressed air may be used. The illustrated vacuum pump is also the same as described above. The rectangular opening shown in FIG. 3 and the light passing through the exposure light EL 55b and the two openings 55a are much larger. The partition wall 52 is provided with a side wall portion and a top plate portion having a central opening 52a provided at the upper end of the side wall portion. The rectangular opening 52a, as shown in FIG. 3, has a total area of the cutout portion between the exposure opening 55a and the irradiation opening 55b. 32 200423224 The partition wall 52 and the bottom surface member 55 form a reticle holding space%. The upper end surface of the top plate portion is formed with opposed annular grooves 58 and 59 as described later. On the outside of the holding space SS of the reticle micro-movement stage 5, on the side -X of the partition wall 52, as shown in Fig. 4B, a plane mirror 9U is provided. The light beam emitted by the reticle laser interferometer 9c provided on the X side is irradiated to the child plane mirror 91c, and the reticle microinterferometer 5c is continuously detected by the reticle laser interferometer 9c (also That is, the position of the reticle in the x-axis direction can reach, for example, a resolution of about 0.5 to 1 nm. Furthermore, the outside of the partition wall 52 (the outside of the holding space SS) is near the + γ side end of the bottom member 55. Through the safety cracking member 104b (Shenri call '..., Θ 2), a retro-reflective mirror 9ia ㈣leCtor) is provided as a reflecting member. The laser light from the reticle laser ^ 9a, 9b is irradiated to the retro-reflective mirrors 91a, 91b, respectively. = The reticle laser interferometers 9a, 9b respectively detect the position, emission, & Block: reticle micro-movement stage 5 (ie, reticle _ Y-axis square reticle :: often guarantee the resolution of, for example, 0.5 ~ 1nm. Also, according to 2 :: household line 2 · dry 9a, the difference between the detection value of the ribs and the distance between the beams will make the line sheet stiffen the stage 5 (also the direction of rotation of the furnace) rotation (deflection) " secret aspect (z-axis rotation: the person's can also be on the bottom surface) The side ends 9ia, 91 of the member 55, and the flat mirror 9lc and the inverted mirror described above are described in detail on the basis of the figure. 33 200423224 aerostatic bearing provided on the reticle coarse motion stage 4. First, the description of the formation of the reticle Differential exhaust type gas hydrostatic bearing (hereinafter referred to as "the first bearing") with a slight gap between the coarse motion stage 4 and the projection system-side platform 3. The plate portion under the reticle coarse motion stage 4 On the bottom surface of 46c, an air-supply-side annular groove 3 is formed from the inner side of the outer edge portion. An air-supply-side annular groove 3 is formed on the outside of the air-supply-side annular groove 31. 2. Air supply ㈣-shaped groove 31 ^ Pass the-end of the air supply line 37 formed in the coarse moving stage 4 of the reticle, and the air supply ... the other-end is connected to an unillustrated = supply device. Also, Exhaust-side annular groove 32 through reticle coarse movement stage 4
内所形成的排氣管路3 6連接至排夯其Q Q A 按主排軋官38的一端,該排氣 管38的另一端則連接至未圖示之真空泵。 有乳 因此,本實施形態中,由氣體供應裝置透過供氣 傳送而來的氮或稀有氣許擎 叙^ , ♦低騎性氣體,透過標線片粗 動載台4内所形成的供_总 卞 +山 的仏孔&路35而由供氣側環狀凹槽3] 贺出,且將排氣側環狀 t ^ ^ 僧dl 狀凹槽I排氣管路3Λ 的氣體’透過排氣側環 铆孔s路36、及排氣管38,以未圖 泵的吸力來進行排氣。复钍 之— ^ ^ f ,、、、、°果,可使得標線片粗動載A 4 以則、距離懸浮於投影系統側平台3,且可在 =4 之間隙内形成由内側柙 距離 的虛線箭頭),以阻止曰外立 側槽32之氣流(參照圖3 載台4的外钟入广氣體(氧、水蒸氣)由標線片粗動 j r 文入標線η 側)。藉以上所示方/ _載台4之内部(亦即開口仆 承。 / ,以下板部46c全體實質構成第1軸 34 200423224 4與照明系統側平台 靜壓軸承(以下稱為 接著,詳述使標線片粗動载台 間具氣密化功能之差動排氣型氣體 第2軸承」)。 =線片粗動載台4的上板部46a上面,於外緣 内側處形成供㈣觀凹槽27 的外側形成排氣側環狀凹槽28料狀凹槽27 禍菸綠u 、 價Μ供乳側環狀凹槽2Y係透 氣势粗^載口 4内所形成的供氣管路%連接至上述供 動二:一端。又,排氣側環狀凹槽28則透過標線片粗 :載:4::形成的排氣管…連接至上述排氣管:8 戈稀二二 氣體供應裝置透過供氣管37傳送來的氮 有氣體等低吸收性氣體,透過標線片粗動載 : 氣管路35而由供氣側環狀凹槽27喷出,且在排 槽28附近的氣體亦透過排氣側環狀凹槽28、 ::…及排氣管38,以未圖示之真空系的吸引力來 進行排氣。其結果,可在#始μ 平…… 粗動載台4及照明系統側 ° 持既定間距,且可在該既定間距内形成由内 側流向外測的氣流(參照圖3的虛線箭頭),因此,可阻止 外部氣體(氧、水蒸氣)由標線片粗動載台4 線片粗動載台4之内部(亦即開口 4“則)。如以上揭示二 ,以上板部46a全體實質構成第2軸承。 其次’說明形成於標線片粗動載台4之下板部46c及 標線片微動載台5之間的差動排氣型氣體㈣ 稱為「第3軸承」)。 在標線片粗動載台4的下板部46c上面,於開口牝的 35 200423224 外側形成供氣側環狀凹槽33, 更外側^、她〜 於^、亂側核狀凹槽33的 ^卜側开/成排氣側環狀凹槽34。供氣 過?成於標線片粗動載台4内的供氣管路35連L = …7的一端。又,排氣側環狀凹槽%係透 線片粗動载台4内的排氣管 於軚 -端。因此,由氣體供應裝置透過=上二^ ^ 或稀有氣體等低吸收性氣體,透過形成: :::的氮 …供氣管…供氣側環狀凹槽成:=_台 排氣側環狀凹槽34周邊 、出的㈣’在 34、排氣營狹〇礼肢’則透過排氣側環狀凹槽 引力A t及排氣f38’經由未― 匕處,只際上,由於環狀凹槽33 34 ^ 線片微動载台5的下端面,因狀 ,係近接標 ,受到槽……,一邊頂起標線二槽载=射, 於其周圍。亦即,受到由上述槽 ° -動 可使標線片微動載…以微小距起作用, 台4,進而達成近接配置(上浮支持):亡::標線片粗動載 槽34之間,因形成了由槽33流向> 槽33與 的虛線箭頭),故可免於外部氣體(氣:氣流(翏照圖3 動載台5的外部侵入標線片 7二氣:田標線片微 持標線“的空間之側)⑽揭示V,的内部(亦即用以保 構成第3細承。 以下板部46c實質 片微動载Μ月在&線片粗動載台4的上板部46a及標線 之間’具有氣密化作用之差動排氣型氣體靜 36 200423224 壓軸承(以下,稱為「第4軸承」)。 在標線片粗動载台4的上板部46a的下面 的外側形成供氣側環狀凹槽 ,於開口切 的更外側形成排氣側環㈣59、::、,側環狀凹槽58 過標―…所形 氣…-端。又,排氣侧環狀凹槽59透=接至上述供 片粗動載台4内的排氣管路%連接至二形成於標線 端。因此’來自氣體供應裝置透過供氣管管】之一 或稀有氣體等低吸收性氣體,透過形成專运而來的說 4内的供氣管路35而由供氣側環狀凹槽、5Γ=粗動載台 氣側環狀凹槽59周邊之氣體, 、出’且在排 排氣管路36、及排氣管38,經 乳:讀凹槽59、 來排氣。 …二泵的吸引力 貝際上,此處的環狀凹槽“的 於標線片微動载台5的上端面,# ’係'近接配置 及標線片粗動载台4的上板部46aJ^片微動载台5 環狀凹槽58及環狀凹槽μ之間形成了由;m’且在 之氣流(參照圖3的崖、線箭頭)。因而,可阻^L向槽59 、水蒸氣)由標線片微動载台5 外部氣體(氧 5之内部(亦即用以保持標線片只之 〜線片镟動载台 方法,藉上板部46a實質構成第4 .:二之側)。如所揭示 又’標線片粗動载台4及標線 動量’係藉線性馬達膽,題補償標線=口 5的相對移 置時的微量移動,具體而言僅有數"沒動載台4之位 右。因此,設於 37 兩者間的軸承(即箆 〜 片粗動載a 4對卜+、弟4軸承)的剛性無需過高,標線 僅須微量的氣體喷射量及吸:丨承量所進行之,氣)’有時 具充分與.里又,當近接配設的兩面 八兄刀/月動性及氣密性時, 4及標線片微動… 可不設標線片粗動載台 片㈣載台5間的軸承(即第3及第4轴承)。 稭以上說明之第丨〜第 ^ 弟4軸承,經由非接觸方式以支 符各載台,且可幾半宕入伽又 ^ ^ ^ 王 來自外部的氣體透過標線片 粗動載台4及照明系統側 ^ ee .κ 〇 2與技影糸統側平台3間的 間隙,以及標線片粗動載△ ρκ 口及軚線片微動載台5間的間 隙,k入標線片R的保持空間内。 此處,如圖3所示,佶用夕々_ H ^ ^ 使用之乳體供應機構,可將接至 線片粗動載台4之供韻答Q 7 ^ r,读、…η, 所流動的部分氮或稀有氣 月旦透過才示線片粗動載台4內夕八l+ a 991 Q〇lu 4内之分歧自供氣管路35的供氣 支吕221a,221b,從形成於产砼 取於铋線片粗動載台4的開口 4a 及開口 4b之側壁將氣體流入令 八忒開口内,以將氮或稀有氣體 i、、、Ό至保持空間SS内。而另__- 方面,使用之排氣機構,可 透過分岐自排氣管路36的排 旧排乳支管222a,222b,從開口 4a,4b的側壁,將保持空間、 寸二間SS网的氣體進行排放。藉由 以上揭示之氣體供應機構及氣體排氣機構,除具上述氣密 化效果,更利於在標線片的侔姓办 ^ ]保持空間内置換成對曝光用光 具低吸收性之氮或稀有氣以。再者,亦可將供氣支管 如,221b設置於供氣側環狀凹槽58, 33及開π 4a,4b 之間。 38 200423224 上述標線片R,如前所述,係由設於標線片載台防 標線片微動載台5)之曝光用開ϋ 55a附近的標線片保持機 構53,來加以吸附保持。該標線片R,如圖$所示,其中 央邛位之圖案區PA内,描繪著待轉印至晶圓w上的 案61。 圓 、私路圖案61,係移相式圖案,係由遮光部背景上排列 ,Y軸方向且以X軸方向為長邊之3〜5條程度的穿透圖案 、导斤構成。各穿透圖案,每隔一條根即反轉穿透部的穿透 光相位而構成移相式標線片圖案。又,將此圖案轉印至晶 圓^上後,肖f透圖t 61巾的穿透部與穿透部間所挾的遮 光邛’即成為電晶體的閘極。因此,目5的標線片中,被 轉印至晶圓W上之閘極方向(閘極圖案之長邊方向),係於 X車由方向一致。 接著,簡單說明以上述方法構成之曝光裝置100的曝 光動作。 首先,先設定各種曝光條件。本實施形態中,由於係 如上述般使用圖5所示之移相式標線片R來進行曝光,因 2用以照明於標線片R之曝光用光乩,從解析度及焦深考 量,以相干度(σ值)小的照明光,亦即對標線片之照明光 入射角範圍較小之照明光較佳…,使用移相式標線片 R以進仃曝光時,藉未圖示之控制裝置,將複眼透鏡11〇 2射出面附近的照明孔徑光闌板U1上的σ光圈Ua,設 疋於曝光用光EL的光程上,同時縮小該σ光圈的開口,俾 成為小σ之照明條件。又,控制裝置乃將繞射光學元件6a 39 200423224 設定於光程上’使穿透過的光束有較小發散角,作為對該 σ光圈11 a引導曝光用光EL之繞射光學元件。據此,將日尸 明光束對標線片R之數值孔徑設定為小。 之後’在未圖示的控制裝置的管理下,使用未圖示的 標線片對準系統、及未圖示之離軸對準感測器(〇ff — alignment sensor)等,俾進行標線片定位、定位感測器之 基礎線量測等既定準備作業。之後,在控制裝置的管Z下 ,以對準感測器對晶圓w進行增強型全晶圓對準(EGA、即 enhanced global alignment),完成後,求出取晶圓f上 複數個曝光照射區域之排列座標。 以上述方式,完成晶圓w的曝光準備動作後,藉由未 圖示之控制裝i,根據上述對_,,測晶圓'則χ 軸雷射干涉敍Υ軸雷射干涉儀57γ之量測值,—邊透過 晶圓驅動系統移動晶圓載台WST,使其到達為進行晶圓w 之第1曝光照射(第1個曝光照射區域)之開始加速位 描開始位置)。 接著控制裝置透過標線片驅動系統及晶圓驅動系統 ’使標線片載纟RST及晶圓载台WST開始朝γ軸方向掃描 、田兩载台RST,WST分別達到目標掃描速度時,即開始以 ^ 光^知、明標線片R的圖案區域,開始進行掃描曝光 金,j:t “曝光進行期間,由σ光㈤1 la射出的照明光 光里刀布呈圖6a所示之狀態(圖6A中,斜線區域即 係照明光束在立AA广丄、 、品域’即曝光用光的能量密度高的區域 40 200423224 )。此係由於使用》5之移相式標線片R來進行曝光時,其 照明狀磕係使照明光集令於光軸附近之小圓内(小π照明) 所致。再者,如圖1所示’標線片只及。光们ia之間有 彎曲反射鏡115,故圖6A中的Γ方向對應於圖】的z方向 Ο 、繼而,以紫外脈衝光逐次照明標線片"的相異圖案 區:或’完成對圖案區域全面之照明後,即完成對晶圓界上 之第1曝光照射區域的掃描曝光。據此,標線片R的電路 圖案即透過投影光學系統PL被縮小轉印於晶圓w上之第i =照射區域之光阻層。完成對此第1曝光照射區域之掃 :: 藉由未圖示之控制裝置,使晶圓載㈠ST以步 式移動於X軸方向(亦即進行曝光照射區域間的步進動 。-達弟2曝光點之曝光開始加速位置(掃描開始位置) 行η::、:以未圖示之控制裝置,對第2曝光照射區域進 仃同於上述之掃描曝光。 逆 以上述方式,反覆進 曝光,以及為& 口 w上曝光照射區域之掃描 將標線片,的曝光照射區域之步進動作,直至 曝光照射區域。2 α案依序轉印至晶圓w上之 辱光作苹後\ &肖晶圓w上所有曝光照射區域之 新的:Γ晶圓載…即進行晶圓交換,以換成 進行Γ二!=置透過未圖示之晶圓交換用機械手臂, 口载上的晶圓卸載及裝载新晶圓。. 41 200423224 又’在上述曝光動作P卩 I >. 勒作期間’由於形成於圖5 R之電路圖案,係其長邊方向 八聊万向一致、於γ細 向具有周期性的移相式桿魂Η 安 1 ^ ^ 、綠片圖案,故該穿透光會受 線片圖案之繞射作用,且社要,少机W ^ …、·。果,在投影光學系統PL内 光用光的能量分布’將如圖7所 + 叮丁 此圖7中,配置在将 影光學系統PL的光瞳面(係樟飧Η 两、你铩綠片R上各點所發出之 的主光線,收斂於1點的面,於此 π此邛分没有例如彩虹光闌 所構成之孔徑光閣63)30p附近的透鏡3〇c,㈣,心 30f,3Gg,3Gh #,如圖6B所示,係曝光用光集中(呈偏 置狀態)於離光軸既定距離之2個圓形區域的狀態。又,圖 6B中’賦予斜線的2個區域,係表示㈣用光的能量密:The exhaust pipe 36 formed in the inside is connected to one end of the row QQ A according to the main row 38, and the other end of the exhaust pipe 38 is connected to a vacuum pump (not shown). There is milk. Therefore, in this embodiment, the nitrogen or rare gas delivered by the gas supply device through the air supply is high, and the low-riding gas passes through the supply line formed in the coarse movement stage 4 of the reticle. The total 卞 + mountain hole of the mountain & the road 35 is fed by the gas-supply-side annular groove 3], and the gas on the exhaust-side annular t ^ ^ monk dl-shaped groove I exhaust pipe 3Λ is passed through The exhaust-side ring riveting hole s-path 36 and the exhaust pipe 38 are exhausted by suction of a pump (not shown). Fu Zhizhi — ^ ^ f ,,,,,, °, can make the reticle coarse dynamic load A 4 at a regular distance, suspended on the projection system side platform 3, and can form a distance from the inside 内 within the gap of = 4 (Dotted arrow) to prevent the airflow in the outer side groove 32 (refer to FIG. 3, the external clock into the gas (oxygen, water vapor) from the stage 4 coarsely moves the jr text into the eta side of the reticle). By the above-mentioned / _ the inside of the carrier 4 (that is, the opening bearing.) /, The following plate portion 46c substantially constitutes the first shaft 34 200423224 4 and the static pressure bearing of the lighting system side platform (hereinafter referred to as the next, details Differential exhaust type gas second bearing with air-tightening function between the reticle coarse moving stage "). = The upper part of the upper plate part 46a of the traverse coarse movement stage 4 is formed with a supply shaft inside the outer edge. The groove 27 on the outer side of the groove 27 is formed with an annular groove 28 on the exhaust side. A material groove 27 is provided. The annular groove on the milk supply side 2Y is a gas-supply pipeline formed in the carrier port 4. % Connected to the above-mentioned driver two: one end. Also, the exhaust-side annular groove 28 is thick through the reticle: load: 4 :: the exhaust pipe formed is connected to the above-mentioned exhaust pipe: 8 Gossier 22 The gas supply device transmits low-absorptive gases such as nitrogen through the gas supply pipe 37, and carries the coarse dynamic load through the reticle: The gas pipe 35 is ejected from the gas-supply-side annular groove 27, and The gas also passes through the annular grooves 28, ::, and the exhaust pipe 38 on the exhaust side, and is exhausted by a suction force of a vacuum system (not shown). As a result, # 始 μ Flat ... Coarse movement stage 4 and the side of the lighting system maintain a predetermined distance, and an airflow measured from the inside to the outside can be formed within the predetermined distance (refer to the dotted arrow in Fig. 3). Therefore, external air can be blocked (Oxygen, water vapor) is formed by the reticle coarse moving stage 4 (the opening 4 "). As disclosed above, the entire plate portion 46a substantially constitutes a second bearing. Next 'Describe a differential exhaust-type gas (referred to as a "third bearing") formed between the lower plate portion 46c of the reticle coarse motion stage 4 and the reticle micromotion stage 5.) On the lower plate portion 46c of the reticle coarse movement stage 4, an air-supply-side annular groove 33 is formed on the outside of the opening 35, 200423224, and further outside ^, her ~ ^, and chaotic side nuclear groove 33. ^ Bu side opening / groove exhaust side annular groove 34. The air supply is formed at one end of the gas supply line 35 in the coarse motion stage 4 of the reticle with L =… 7. In addition, the exhaust-side annular groove% is the exhaust pipe in the coarse-moving stage 4 of the diaphragm at the 軚 -end. Therefore, the gas supply device transmits = upper two ^ ^ or a rare gas such as a rare gas, and penetrates to form: :::: nitrogen ... supply pipe ... supply-side annular groove: = _ 台 exhaust side annular At the periphery of the groove 34, the ㈣ 'at 34, the exhaust battalion narrow and the ceremonial limbs' pass through the exhaust side annular groove gravity At and the exhaust f38' through the un-dagger, only occasionally, due to the ring The groove 33 34 ^ The lower end surface of the thread micro-movement stage 5 is close to the target due to the condition, and is subject to the slot ..., one side lifts the target line and the second slot loads = shoots around it. That is to say, subjecting the groove to the micro-movement of the reticle by the above-mentioned grooves ... acting at a small distance, the stage 4 can achieve a close configuration (upward support): death :: the reticle is coarsely moved between the loading slots 34, Due to the formation of a dashed arrow from slot 33 to slot 33, it is free from external air (gas: gas flow (see Figure 3 for the outside of the moving stage 5 to intrude into the marking strip 7) Second gas: field marking strip The side of the space of the micro-marking line "⑽ reveals the interior of V, (that is, used to ensure the formation of the third fine bearing. The substantial movement of the substantial part of the lower plate 46c is carried on the & coarse-movement stage 4 Between the plate portion 46a and the reticle, a differential exhaust type gas-static 36 200423224 pressure bearing (hereinafter referred to as a "fourth bearing") having a gas-tightening effect. The upper plate of the reticle rough movement stage 4 An air-supply-side annular groove is formed on the outer side of the lower portion of the portion 46a, and an exhaust-side annular ring 59, ::, is formed on the outer side of the opening cut. The annular groove 59 on the exhaust side is transparently connected to the exhaust pipe in the coarse feeding stage 4 described above. The exhaust pipe is connected to the second line at the end of the marked line. Tube] or a low-absorptive gas such as a rare gas, which is formed by a special gas supply pipe 35 in the 4 and is formed by a gas-supply-side annular groove, 5Γ = a coarse moving stage gas-side annular recess The gas around the tank 59 is exhausted through the exhaust pipe 36 and the exhaust pipe 38, and the breast: Read the groove 59 to exhaust.… The attraction of the two pumps, the ring here The upper end of the reticle micro-moving stage 5 is shaped like a "groove" on the upper end of the reticle coarse-moving stage 4 and the upper plate portion 46aJ of the reticle coarse-moving stage 5 is an annular groove 58 and a ring. The grooves are formed between the grooves μ; m ′ and the air flow (refer to the cliff and line arrows in FIG. 3). Therefore, ^ L to the groove 59, water vapor can be blocked) from the reticle micro-movement stage 5 outside air (The inside of oxygen 5 (that is, the method for holding the reticle only ~ the stub moving platform method, the upper plate portion 46a essentially constitutes the 4 :: 2 side). As disclosed, the `` reticle is thick The dynamic stage 4 and the momentum of the graticule are based on linear motors, and the compensation is for the slight movement when the graticule = the relative displacement of the port 5. Specifically, there are only a few " the position of the movable stage 4 is right. Therefore, set At 37 two The bearings between the bearings (that is, the rough moving load a 4 pairs of Bu +, brother 4 bearings) do not need to be too high, the marking line only needs a small amount of gas injection and suction: the bearing capacity is carried out, gas) 'Yes The time is fully compatible with the inner and outer sides. When the two-faced eight-knife knife / moon and air tightness are arranged close to each other, the 4 and the reticules are slightly moved ... There may be no coarse reversing of the reticles. Bearings (ie, 3rd and 4th bearings). The 4th ~ 4th brothers of the bearings described above are supported by non-contact methods on each carrier, and can be dropped into the halves from the outside. The gas passes through the coarse motion stage 4 of the reticle and the lighting system side ^ ee .κ 〇2 and the platform 3 side of the technical film system, and the coarse motion load of the reticle △ ρκ port and the micro motion stage 5 Between the gaps, k enters the holding space of the reticle R. Here, as shown in FIG. 3, the milk supply mechanism used by 々 々 H H ^ ^ can be used to answer the Q 7 ^ r of the supply to the coarse motion stage 4 of the thread, read,… η, Part of the flowing nitrogen or rare gas passes through the coarse movement stage 4 of the thread guide, and the divergence within the 4 l + a 991 Q0lu 4 is diverted from the gas supply branches 221a, 221b of the gas supply line 35, and is taken from the production unit. A gas is flowed into the openings of the openings 4a and 4b of the bismuth wire coarse-moving stage 4 to allow nitrogen or rare gases i,, and to be contained in the holding space SS. On the other hand, the exhaust mechanism used can pass through the old milk discharge branches 222a, 222b of the divergent self-exhaust pipe 36, and from the side walls of the openings 4a, 4b, the space will be maintained. The gas is vented. With the above-mentioned gas supply mechanism and gas exhaust mechanism, in addition to the above-mentioned air-tightening effect, it is more conducive to replacement in the space of the reticle ^] holding space with low-absorption nitrogen for exposure light or Rare gas. Furthermore, a gas supply branch pipe such as 221b may be provided between the gas-supply-side annular grooves 58 and 33 and the opening π 4a and 4b. 38 200423224 As mentioned above, the reticle R is adsorbed and held by the reticle holding mechanism 53 located near the exposure opening 55a on the reticle stage 5). . The reticle R, as shown in Fig. $, Depicts the case 61 to be transferred onto the wafer w in the central pattern area PA. The circle and private road pattern 61 is a phase-shifting pattern, which is composed of 3 to 5 penetrating patterns arranged on the background of the light-shielding part and having a length of 3 to 5 in the Y-axis direction and the X-axis direction as the long side. In each of the penetrating patterns, the phase of the penetrating light of the penetrating portion is inverted at every other root to form a phase-shift reticle pattern. In addition, after this pattern is transferred to the crystal circle ^, the transparent portion 肖 between the penetrating portion and the penetrating portion of the towel 61 becomes the gate of the transistor. Therefore, in the reticle of mesh 5, the gate direction (long side direction of the gate pattern) transferred to the wafer W is aligned with the X-axis direction. Next, the exposure operation of the exposure apparatus 100 configured as described above will be briefly described. First, set various exposure conditions. In this embodiment, as described above, the phase-shifting reticle R shown in FIG. 5 is used for exposure. Because 2 is used to illuminate the exposure light of the reticle R, the resolution and depth of focus are considered. It is better to use the illumination light with small coherence (σ value), that is, the illumination light with smaller incident angle range of the reticle. When using phase-shift reticle R for exposure, the The control device shown in the figure sets the σ aperture Ua on the iris aperture plate U1 near the exit surface of the fly-eye lens 1102 to the optical path of the exposure light EL, and at the same time reduces the opening of the σ aperture to become Small σ lighting conditions. The control device is a diffractive optical element 6a 39 200423224 set on the optical path 'so that the transmitted light beam has a small divergence angle as a diffractive optical element that guides the exposure light EL to the σ aperture 11 a. Based on this, the numerical aperture of the reticle bright beam alignment reticle R is set to be small. Afterwards, under the management of a control device (not shown), alignment is performed using an unillustrated reticle alignment system and an unillustrated off-axis alignment sensor (〇ff — alignment sensor). Film preparation, basic line measurement of positioning sensor, etc. After that, under the tube Z of the control device, the wafer w is subjected to enhanced global wafer alignment (EGA, ie, enhanced global alignment) with the alignment sensor. After completion, a plurality of exposures on the wafer f are obtained. Arrangement coordinates of the irradiation area. In the above-mentioned manner, after the exposure preparation operation for the wafer w is completed, the amount of the x-axis laser interference and the x-axis laser interferometer 57γ is measured by the control device i (not shown) according to the above-mentioned pair. Measured value—While moving the wafer stage WST through the wafer driving system, it reaches the start position of the acceleration tracing for the first exposure irradiation (the first exposure irradiation area) of the wafer w). Then the control device uses the reticle drive system and the wafer drive system to cause the reticle carrier 纟 and the wafer stage WST to start scanning in the γ-axis direction. When the two stages RST and WST reach the target scanning speed, that is, Beginning with the pattern area of the light-marked line R, scanning exposure gold is started, and j: t "During the exposure, the illumination light emitted by σ light ㈤1 la is in the state shown in Figure 6a ( In FIG. 6A, the oblique line area is the area where the illumination beam is wide, and the product area is the area where the energy density of the exposure light is high. (2004 200423224). This is because the phase-shifting reticle R of "5" is used to perform At the time of exposure, its illumination state is caused by the illumination light being concentrated in a small circle (small π illumination) near the optical axis. Furthermore, as shown in Figure 1, the reticle is only available. There is between the light ia The curved mirror 115, so the Γ direction in FIG. 6A corresponds to the z direction 0 in the figure. Then, the pulse pattern is used to sequentially illuminate the reticle " with different pattern areas: or 'After completing the full illumination of the pattern area , That is, the scanning exposure of the first exposure irradiation area on the wafer boundary is completed. Therefore, the circuit pattern of the reticle R is reduced and transferred through the projection optical system PL to the photoresist layer of the ith = irradiation area on the wafer w. The scan of the first exposure irradiation area is completed. The control device shown in the figure moves the wafer carrier ST in the X-axis direction in a stepwise manner (that is, the step between the exposure irradiation areas is performed.-The exposure start acceleration position (scanning start position) of Daddy 2 exposure point) Line η: :,: With the control device not shown, the second exposure irradiation area is scanned in the same way as above. Reverse the exposure in the manner described above, and mark the lines for scanning the exposure irradiation area on the & Step of the exposure irradiation area until the exposure irradiation area. 2 α case sequentially transferred to the wafer w shaming as the new \ All new exposure areas on the wafer w: Γ Wafer loading ... that is, wafer exchange, in exchange for Γ two! = Placement of unloaded wafers and loading of new wafers through a robotic arm for wafer exchange not shown. 41 200423224 Again ' During the above exposure operation P 动作 I >. Stroke period 'due to formation in Figure 5 R The circuit pattern is the same as the long-side direction. The phase-shifting pole-soul pattern is 1 ^ ^ in the γ fine direction, so the penetrating light will be diffracted by the line pattern. Role, and the main thing, less machine W ^, .... As a result, the energy distribution of light used in the projection optical system PL will be as shown in Figure 7 + Pupil plane (system of camphor 2. Second, the main light emitted from each point on your green sheet R converges to the 1-point surface, and here there is no aperture lighthouse 63 such as a rainbow diaphragm ) The lens 30c, ㈣, heart 30f, 3Gg, 3Gh # near 30p, as shown in FIG. 6B, is a state where the exposure light is concentrated (in an offset state) in two circular areas at a predetermined distance from the optical axis. . In addition, in FIG. 6B, the two regions given with slashes indicate the energy density of the light used:
高的區域。 X 因此4透鏡30c,30d,30e,斯,3〇g,識等透鏡 中’僅有受曝光用光照射的部分受到加熱,/亦即,呈現旋 轉非對稱之受熱現象。其結果,在透鏡3〇e,3〇山3〇e, 3〇f,30g,30h等透鏡中,僅有受加熱的部分產生體積膨 脹或折射率動,結果在該些透鏡3〇c〜3〇h造成旋轉非對 稱像差,甚至在投影光學系統PL造成旋轉非對稱像差。 因此’本實施形態之曝光裝置1 〇〇,為抑制在晶圓載 台WST上進行晶圓交換期間產生上述旋轉非對稱像差,係 對投影光學系統PL内的透鏡施以虛擬照射。 亦即,在晶圓载台WST上,於上述晶圓交換期間,將 妝明光照射於投影光學系統PL内,使得投影光學系統PL 内的光量分布,特別是該光瞳面3〇p附近之光量分布(曝光 42 200423224 用光的此置密度分布),呈現與圖6B反轉之分布(參照圖 8) ’據此’使投影光學系統PL的光瞳面30p附近之透鏡 30c〜30h等之旋轉非對稱之加熱(發熱)狀態,能儘可能的 轉變成旋轉對稱之加熱狀態。 具體而§ ’係往晶圓交換位置驅動晶圓載台WST,在 晶圓W脫離投影光學系統PL的曝光視野之狀態下,藉由控 制裝置’將上述照明系統孔徑光闌板111的虛擬照射用光 鬧1 lb设定於曝光用光el之光程上。為對應於該照明系統 孔徑光鬧板111之設定,控制裝置將繞射光學單元106中 的繞射光學元件置換成能賦予穿透光束更大發散角、由細 微間隙之繞射袼子所構成之繞射光學元件613(參照圖9)。 其結果’穿透過虛擬照射用光闌lib後的曝光用光EL,其 光量分布如圖8A所示。此時,因標線片r與虛擬照射用光 閣11 b之間同樣具有彎曲反射鏡丨丨5,故圖8a中的γ,方向 亦對應於圖1的Z方向。 又’以控制裝置來驅動標線片載台rST,將配置在曝 光用開口 55a之+ γ側附近之照射用開口 55b,定位成大致 與曝光用光之穿透位置一致,亦即,使照射用開口 55b的 中心與照明光學系統的光軸(與投影光學系統PL的光軸一 致)大致一致。此時,由於照射用開口 55b上不存在標線片 R ’曝光用光不受標線片r的遮光及繞射,逕入射至投影光 學系統PL。又,在投影光學系統pl的光瞳面3〇p附近, 形成圖8B所示般的光量分布。該圖8B的光量分布,與穿 透虛擬照射用光闌11 b後的曝光用光EL之光量分布(圖 43 200423224 8A),具有相似形狀。 以上述方式,藉由對投影光學系統pL照射曝光用光 EL(虛擬照射),使得投影光學系統pL内(特別是光瞳面 30p附近)的透鏡在圖8B中的虛線部分受到加熱而發熱。 因此,將晶圓w曝光時於光瞳面3〇1)附近之光量分布(參照 圖6B) ’與虛擬照射時於光瞳面3〇p附近之光量分布(參照 圖8B)予以合計後,即能使光瞳面3〇p附近之透鏡3〇c〜 30h等大致呈-致的加熱狀態(亦即成為旋轉對稱之加熱狀 態)’使其同樣的膨脹。據此,”效抑制投影光學系、統 PL内發生的旋轉非對稱像差。 此時,雖因虛擬照射的進行,增加照射於投影光學系 統PL的總光量,而增大投影光學系統孔之旋轉對稱像差 ,但在旋轉對稱像差之補償時,控制裝置可透過驅動機構 PZ將可動透鏡(本實施形態中為目1所*的透鏡3〇a)微驅 動於投衫光學系統PL的光軸方向,藉以修正像差。 以此方式結束虛擬照射及透鏡之驅動後,對新晶圓實 施一連串的曝光處理步驟。 、 之後,控制裝置在每一晶圓交換之時、或是交換既定 片數的晶圓之各個時間點,施以上述虛擬照射。 由以上之5兒明可知,本實施形態中,係藉由繞射光學 單元1 06及照明系統孔徑光闌板}丨丨,構成照明系統之照 明條件的變更機構,藉此變更將標線片R的圖案轉印於晶 圓W上時、以及透過照射用開口 55b將曝光用光照射於 才又衫光學系統PL時的照明條件。 44 200423224 如以上所評述者’若根據本實施形態之曝光裝置⑽ ’在移動自如地保持標線片R之標線片載台RST當中,形 =照射關口 55b,可使得曝光用光源el在未透過標線 片的狀態下逕穿透至投影光學系、统PL。因此,即可在標線 片/的圖案透過投影光學系統PL轉印至晶圓w上時(曝光 時)’構成投影光學系、统PL之透鏡,特別是光瞳面柳附 近的透鏡30c〜30h被局部(不均句的).加熱時 未進行曝光時’透過照射用開D55b將曝光用光_射於 透鏡30c〜30h’而能加熱透鏡3〇c〜3〇h中在上述曝光中 純加熱的部分,其結果,可緩和透鏡⑽〜識之加熱狀 態的不-致性。藉此,對於上述透鏡·〜3Qh因不均句加 熱造成之投影光學系統PL發生難以修正的像差,亦即並非 以光軸為中心之旋轉非對稱像差,乃具備抑制之效。此時 ,投影光學系統PL中雖發生旋轉對稱像差,但因曝光裝置 100具備驅動機構PZ俾使構成投影光學系統pL的透鏡3〇a 能驅動於投影光學系統PL之光軸方向(z軸方向),因此, 透過該驅動機構PZ來驅動投影光學系統PL内的透鏡3〇& ’即能容易的修正上述旋轉對稱像差。 又,曝光裝置1 〇 〇,具備:照明系統側平台2,係透過 既定間隙配置於標線片載台]rST的照明系統側,在其中一 部分配設有開口 2a,俾使曝光用光EL穿透,並以對向於 標線片載台RST的面作為標線片載台RST之移動導引面; 以及投影系統側平台3,係透過既定間隙配置於標線片載 台RST的投影光學系統pL側,在其中一部分配設有開口 45 200423224 3a’俾使曝光用光源el穿透,並以對向High area. X Therefore, among the 4 lenses 30c, 30d, 30e, 30g, 30g, and so on, only the portion irradiated with the exposure light is heated, that is, the heating phenomenon of asymmetric rotation is exhibited. As a result, among the lenses such as lenses 30e, 30s, 30e, 30f, 30g, and 30h, only the heated portion generates volume expansion or refractive index fluctuation. As a result, these lenses 30c ~ 30h causes a rotational asymmetric aberration, and even causes a rotational asymmetric aberration in the projection optical system PL. Therefore, 'the exposure apparatus 100 of this embodiment, in order to suppress the above-mentioned rotational asymmetrical aberration during wafer exchange on the wafer stage WST, performs virtual irradiation on the lens in the projection optical system PL. That is, on the wafer stage WST, during the above-mentioned wafer exchange, the bright light is irradiated into the projection optical system PL, so that the light amount distribution in the projection optical system PL, especially near the pupil plane 30p. The light quantity distribution (exposure 42 200423224 using this density distribution of light) shows a distribution reversed from that shown in FIG. 6B (refer to FIG. 8). “Based on this,” the lenses 30c ~ 30h near the pupil surface 30p of the projection optical system PL are displayed. The rotationally asymmetric heating (heating) state can be transformed into a rotationally symmetrical heating state as much as possible. Specifically, § 'the wafer stage WST is driven toward the wafer exchange position, and the wafer W is separated from the exposure field of the projection optical system PL by the control device' for the virtual irradiation of the aperture diaphragm plate 111 of the illumination system described above. The light disturbance 1 lb is set on the optical path of the exposure light el. In order to correspond to the setting of the aperture light board 111 of the illumination system, the control device replaces the diffractive optical element in the diffractive optical unit 106 with a diffractive tassel which can give a larger divergence angle to the penetrating light beam and has a fine gap. Diffractive optical element 613 (see FIG. 9). As a result, the light amount distribution of the exposure light EL after passing through the virtual aperture stop lib is shown in Fig. 8A. At this time, since the reticle r and the virtual illumination frame 11 b also have a curved mirror 5, the direction of γ in FIG. 8 a corresponds to the Z direction in FIG. 1. The control device drives the reticle stage rST to position the irradiation opening 55b arranged near the + γ side of the exposure opening 55a so as to approximately coincide with the penetration position of the exposure light, that is, to make the irradiation The center of the use opening 55b substantially coincides with the optical axis of the illumination optical system (which coincides with the optical axis of the projection optical system PL). At this time, since the reticle R 'does not exist on the irradiation opening 55b, the exposure light is not shielded or diffracted by the reticle r, and is incident on the projection optical system PL. Further, in the vicinity of the pupil plane 30p of the projection optical system pl, a light amount distribution as shown in FIG. 8B is formed. The light amount distribution of FIG. 8B has a similar shape to the light amount distribution of the exposure light EL after passing through the virtual illumination diaphragm 11b (FIG. 43 200423224 8A). In the manner described above, the projection optical system pL is irradiated with the exposure light EL (virtual irradiation), so that the lens in the projection optical system pL (especially near the pupil plane 30p) is heated by the dotted line in FIG. 8B to generate heat. Therefore, the light amount distribution (see FIG. 6B) 'near the pupil plane 30.1) when the wafer w is exposed and the light amount distribution (see FIG. 8B) near the pupil plane 30p during virtual irradiation are added up, That is, the lens 30 c ~ 30 h and the like near the pupil surface 30 p can be brought into a substantially uniform heating state (that is, a rotationally symmetric heating state), and the same expansion can be achieved. According to this, the "rotational asymmetric aberration occurring in the projection optical system and the system PL is effectively suppressed. At this time, although the total amount of light irradiated to the projection optical system PL is increased due to the progress of virtual irradiation, the aperture of the projection optical system is increased Rotationally symmetric aberrations, but when compensating for rotationally symmetric aberrations, the control device can micro-drive the movable lens (lens 30a * of the mesh 1 in this embodiment) to the projection optical system PL through the drive mechanism PZ. Optical axis direction to correct aberrations. After ending the virtual irradiation and lens driving in this way, a series of exposure processing steps are performed on the new wafer. After that, the control device exchanges each wafer or the predetermined At each time point of the number of wafers, the above-mentioned virtual irradiation is performed. It can be seen from the above 5 that in this embodiment, the diffractive optical unit 106 and the aperture diaphragm plate of the lighting system are used to form A mechanism for changing the lighting conditions of the lighting system, thereby changing the pattern when the pattern of the reticle R is transferred to the wafer W and when the exposure light is irradiated to the optical system PL through the irradiation opening 55b. Illumination conditions. 44 200423224 As described above, “If the exposure device according to this embodiment is used”, in the reticle stage RST holding the reticle R freely, the shape = irradiation gate 55b can make the light source for exposure El penetrates to the projection optical system and system PL without passing through the reticle. Therefore, when the reticle / pattern is transferred to the wafer w through the projection optical system PL (during exposure) ' The lenses constituting the projection optical system and the system PL, especially the lenses 30c ~ 30h near the pupil surface will be partially (uneven sentences). When the exposure is not performed when heating, the light for exposure is transmitted through the opening D55b. The lens 30c ~ 30h 'can heat the portion of the lens 30c ~ 30h that was heated purely during the above exposure, and as a result, the non-uniformity of the heating state of the lens can be reduced. As a result, for the above lens · ~ 3Qh Aberrations that are difficult to correct in the projection optical system PL caused by uneven sentence heating, that is, rotational asymmetric aberrations that are not centered on the optical axis, have the effect of suppression. At this time, in the projection optical system PL, Although rotationally symmetric aberrations occur, Since the exposure device 100 includes a driving mechanism PZ, the lens 30a constituting the projection optical system pL can be driven in the optical axis direction (z-axis direction) of the projection optical system PL. Therefore, the projection optical system PL is driven by the driving mechanism PZ. The inner lens 3 ′ can easily correct the above-mentioned rotationally symmetric aberration. The exposure device 100 includes an illumination system-side stage 2 and is arranged on a reticle stage through a predetermined gap] rST illumination On the system side, an opening 2a is provided in a part thereof to allow the exposure light EL to penetrate, and a surface facing the reticle stage RST is used as a movement guide surface of the reticle stage RST; and a projection system; The side stage 3 is arranged on the pL side of the projection optical system of the reticle stage RST through a predetermined gap, and an opening 45 200423224 3a 'is arranged in a part of the side so that the exposure light source el penetrates and faces
的面作為標線片载A RST > # & # 、知線片載台KST M m 口 RST之移動導引面 ㈣有間隔壁52,係圍繞於標 上線片載台 侧面之用囹、仏 莉D RST周圍(主要為The surface of the reticle is A RST ># &#, the moving guide surface of the reticle stage KST M m port RST is provided with a partition wall 52, which surrounds the side of the reticle stage. Around Lili D RST (mainly
Wit果。此π使標線片載台RST附近與其外部達成實質 千口 2’ 3所圍繞。因此,除了具有 RST全體時同等的对罢从^ ^ 土復盖&線片 ^ 的义果外,亦有助於裝置的小型化及_量 又’例如,在間隔壁52内的空間ss置換 的吸彳UM、之低吸收性氣料,除了與相隔壁覆: =質=τ’亦可降低標線“之周邊空間内的吸 ^度’另一方面亦可因氣體使用量的減少而具降低 成本之效。 因此能提南 又,因係以真空紫外光作為曝光用光虹, 投影光學系統PL之解析度。 光 承上所述,若使用曝光裝置100, 亦可達成裝置的小型化及輕樣化。 可貫現1¾精度之曝 又’曝光裝i 100具有照明系統之照明條件的變更機 構(106, m),以變更將圖案轉印至晶圓w上時、與透過 照射用開d 55b將曝光用《既照射至投影光學系統凡時 的照明條件。&時’藉由此變更.機構的使用,能進行根據 標線片R之圖案之照明條件的變更,與該照明條件下投影 光學系統PL之光瞳面附近之曝光用光EL之能量密度分佈 ,以及在虛擬照射時使投影光學系統pL的光瞳面附近產生 恰為相反之曝光用光EL之能量分布密度等照明條件之設定。 46 200423224 又,根據以曝光裝置100進行之曝光方法,係在未對 上述晶圓進行曝光(標線片R之圖案轉印)時,具體而t係 在交換晶圓時’在投影光學系統PL之像面上未配置晶圓w 之狀態下,以足可缓和曝光時投影光學系統PL内之透鏡 30c〜30h中因曝光用光EL的照射而造成之熱偏置狀態來 作為照明條件,在不透過標線片R的情況下,逕將曝光用 光EL照射至投影光學系統PL的虛擬照射。因此,即使在 標線片R的圖案轉印時,於構成投影光學系統pL的透鏡 3〇c〜3〇h中產生局部(不均句)加熱,仍可藉由虛擬照射的 處理’將透鏡3Gc〜3Gh等加熱成大致均句受熱的狀態。藉 此,避免透鏡30c〜30h等透鏡中因受到光學構件不均句加 熱,而造成投影光學系統PL發生難以補償的旋轉非對稱像 差,故可維持投影光學系統PL之良好成像特性,以實現高 精度的曝光。 又’本實施形態中,透過照射用開口咖戶斤進行之曝 光用光的虛擬照射,係與曝光步驟中所含的晶圓交換併行 ’因此’’幾乎不會因虛擬照射的進行而降低產能。 又’上述第1實施形態中,該照射用開口 55b及曝光 用開口…雖係分別(於曝光用開口的附近)形成,然其作 法不侷限於此,例如,亦可將曝 斗 ^ ^用開口的掃描方向之尺 寸拉長,使該曝光用開口的-部分兼作照射用開口之用。 再者,上述第1實施形態中, ^ -Λ 隹係採用圖案的長邊方 向亚排於同一方向之標線片R,鈇 Η …、本發明之應用不侷限於 此,使用一般之標線片圖案(亦 ^ ^ ' 兼具有以既定方向為 47 200423224 長邊方向之圖案、以及以2 $面内正交於既定方向之方向 ^圖案之長邊方向者),亦具良好效果。χ,曝純件不 。立;J σ值照明及移相式標線片的組合,用於照明光的 局部化程度大之變形照明時,亦具良效。 九亦即,將標線片圖案轉印於晶圓時在投影光學系統光 =面所形成之曝光用光的分布,於虛擬照射時,在投影光 :系統PL之光瞳面形成將該形狀之明暗反轉形狀之照明光 1分布即可。 、特別是,在σ值小的照明時,使用圖案之長邊方向並 ^於同S向之標線片的場合,由於在投影光學系統光瞳 面之曝光用光之光量分布具有最大的局部化,故本發明用 於該類曝光條件時最具效果。 又,上述第1實施形態中,係驅動構成投影光學系統 PL之透鏡30a〜3〇j中位於最上部的透鏡3〇&,使其驅動於 γ車方向藉以修正旋轉對稱像差,但本發明之應用不侷限 於此,亦可驅動其他透鏡以修正旋轉對稱像差,亦可在某 特定透鏡與鄰接該特定透鏡的透鏡之間,配置氣體室,藉 改變該氣體室的壓力以修正旋轉對稱像差。 曰 又,使用折反射光學系統作為投影光學系統pL時,將 構成杈衫光學系統的一部分之反射鏡元件朝光軸方向微量 移動,亦可修正旋轉對稱像差。 又上述第1實施形態中,係在照明系統側平台2及 投影系統側平台3形成開口作為光穿透部,然其應用不限 於此,亦可使用透明構件來構成平台全體,亦可藉透明構 48 200423224 件來構成曝光用光的穿透部分。 影光學系統及照明光學系二、透明構件亦可與投 (modified)石英。 、。樣使用螢石或改良 間SS中,不必然 設有其中的任一 此外,在標線片载台RST内的保持空 非得設有氣體供應機構及排氣機構兩者, 方者亦可。 又,上述第1實施形態中, 吸收性㈣,來作為差動排氣二乳或稀有氣體等低 ’然而,本發明不侷限於此,在直 吏用乳體 供應裝置之供氣量時,亦可採用空:等'的排氧量多於氣體 又,上述第1實施形態中’構成標線片粗動載台4之 上板部46a及下板部46c之間,雖係僅由中間部儀連社 i然本發明不偈限於此,亦可在標線片粗動載台4的 別方部(+γ側)’再加上維繫上板冑恤及下板部46c之 支持柱,以進一步提昇其剛性。 入,隹上返弟 ^ 土分袖承的氣體, 以及供應至標線片保持空間%内之氣體,最好是能 制於既定溫度㈣2rc),且已充分取出其中的粒: 機物、水蒸氣等異物者。 产此外,上述第1實施形態中的各軸承,雖係以具備供 氣側環狀凹槽及棑氣側環狀凹槽之雙重結構 丨行β钩具說明例 ’然而,其應用不侷限於此,若是採用具三重結構的槽, 由位於中間的槽來供應氣體,由挾中間槽的另2個槽來口 引氣體’亦能具有同樣的氣密化效果。又,無庸賢古的 49 200423224 若是形成二組上述雙重結構的槽,而成為四重構造之軸承 ,亦為適用之列。亦即,各軸承的槽數得任意安排。 又,在上述第1實施形態中,於虛擬照射時雖係採用 曝光用光,然而,在虛擬照射時亦可使用異於曝光用光之 域光源作為該虛擬照射用之能量束。該虛擬照射用之 月t* 3E束(例如為紅外線),分別透過開口 2a、開口切、開口 挪、開口 4b及開口 3a,且在未透過標線片R的條件下, 朝投影光學系統孔照射。此時,若在曝光用光的光程中設 有紅外線照射機構,其中具有在虛擬照射時插入光程中的 分束器,藉由該分束器使上述虛擬照射用之能量束(例如 為紅外線)透過上述各開口而照射至投影光學“孔亦宜 、。在上述應用例中,係在虛擬照射進行前,在曝光用光的 光知工間内插入上述分束器,其後透過分束器來射出紅外 線:此時’分束器之插入位置,可為投影光學系統pL與照 明早兀ILU之間,或是照明單元ILU内。 《第2實施形態》 。二下根據圖1U、圖11B,說明本發明之第2實施形態 。*处’對於與上述第1實施形態相同或相等的部分,係 賦予同-符號且簡略或省略其進一步說明。該第2實施形 恶之曝光裝置,其投影光學系統之構成與上述第^ : 態僅有些微差異,ι他邻八 貝乂 m 他口0刀之構成則相同。因此,為避免 複°兄 u下乃以其差異處為說明要點。 圖11A所示,係構成第2實施形態的曝 光學系統PL’的概略構成圖。 之杈如 50 200423224 如該圖11A所示,投影光學系統pL,係自其外部導入 光纖FB(特別是已在中空玻璃管的内面塗布鋁之光纖 日士— υ 守灵IV、上係如圖Π β所示,沿著透鏡外緣,以既定角度 間1^ ’分別對光學構件(例如透鏡3〇c,3〇d,30g)導入 稷數條光纖FBi〜FBn。此等光纖FB係連接至設在投影光學 系、、先PL外部之未圖示的紅外線照射源。此時,係藉由複 數铋光纖FB〗〜FBn與未圖示的紅外線照射源而構成紅外線 照射機構。 、 因本發明第2實施形態亦以I?2雷射光為曝光用光,因 此,構成投影光學系統PL,之透鏡3〇a〜3〇j係使用螢石。 係由構成紅外線照射機構之光纖Ρβ〗〜,將較易被 螢石透鏡所吸收之波長6〜1〇//m左右的紅外線照射至透鏡 (3〇c,30d,30g)。此時之紅外線照射源,例如,可使用含 硒化鉛硫黃、硒化鉛錫、碲化鉛錫等化合物半導體的半導 體雷射。 本第2實施形態之曝光裝置,係與上述第丨實施形態 同樣的方式,將標線片R的圖案轉印至晶圓w。又,未圖 不的控制機構,根據該曝光所用的標線片之圖案或照明條 件,計算出曝光用光在構成投影光學系統pL,的光學構件( 例如為透鏡30c,30d,30g)内之分布狀態,並根據所算出 的曝光用光之分布,預測出透鏡中(3〇c,3〇d,3〇g)應發生 的熱偏置狀態,且對應於該預測結果,從複數條光纖 FBn田中選取適當的光纖,由被選取的光纖對透鏡(3〇c, 30d,30g)照射紅外線。又,紅外線可照射於各透鏡(3〇c, 51 200423224 之任一面,或是 3Od,30g)之曝光用光源的入射面或射出面 照射於入射面及射出面之兩者。 ~丨·求旰,甸預測出具有圖 UB所示之發熱狀態時’即藉由_、ΡΒη以外的光纖提供 紅外線之照射,使發熱狀態趨近於旋轉對稱形狀。 又,藉由調整投影光學系統η内之可動透鏡的位置, 例如調整3〇a之光軸方向位置’以上述第1實施形態之相 同方法,修正投影光學系、統PL,的旋轉對稱像差。 如以上所揭示者,藉由太笙 〇 a , 稭由本弟2貫施形態之曝光裝置及 其曝光方法,將形成於標線片的圖案透過投影光學系統 PL’轉印於晶圓W上時(曝光時),即使構成投影光學系統 PL,的透鏡因曝光用光EL的照射而被局部(不均勻性)加孰 ,仍可藉紅外線照射機構’對於未受曝光用光源乩照射之 其他透鏡部分提供紅外線的照射予以加熱,其結果,可將 透鏡加熱成大致均-的狀態。藉此,對於因透鏡不均句加 熱而在投影光學系,统PL,發生難以修正的旋轉非對稱像差 現象,具有良好的抑制效果。此時,紅外線照射機構對透 ㈣加熱,在曝光中亦可進行,因此,與上述帛i實施形 態相較’更能確實地·抑制投影光學系統發生旋轉非對稱像 差。故而,可在曝光進行時維持投影光學系統的良好成像 特性,實現高精度之曝光。 又以紅外線加熱於透鏡,不同於藉接觸式加熱機構( …、原)所為之加熱或藉接觸式冷卻機構所為之冷卻,由於 未與透鏡接觸’因此不會因接觸於加熱或冷卻機構而導致 52 200423224 透鏡歪斜,又,亦不會發生送風進行冷卻時所產生之透鏡 振動。 再者,由上述之照明σ小的照明光束及移相式標線片 的組合所進行的曝光、或是照明光的局部性較嚴重的變升^ 照明,有時僅憑一次的曝光步驟尚無法形成(轉印)所有待 曝光的電路圖案。此時,可依既定照明條件,由既定桿線 片對1片晶圓進行曝光,完成後交換標線片,另變更為所 須的照明條件來曝光別的圖案(雙重曝光)於上述晶圓上, 以形成所期望之全部圖案。 在该雙重曝光的情況中’有可能在2次個別的曝光期 間改變投影光學系統内的曝光用光光程,使得吸收曝光用 光源所伴隨的材料發熱受到平均化的作用,然而,以2欠 曝光尚無法完全平均化的情況亦所在多有,因而,在此類 實施雙重曝光的情況時本發明仍能發揮極佳效果。 再者,上述各實施形態中,雖以h雷射、雷射、 Ar2雷射,ArF準分子雷射等真空紫外域的脈衝雷射光源, 作為所使用之光源,然其應用不在此限,使用Κβ準分子 雷射為其光源亦佳。又例如,上述各光源所輸出的真空紫 外域之雷射光並無特定侷限,以DFB半導體雷射、或是由 雷射光纖所振盪出的紅外域、或可視域之單一波長雷射光 ,例如,以摻雜铒(Er)(或铒與鏡(Yb)的雙方)的光纖放大 、放大使用非線性光學結晶將波長變換為高頻之紫 外光亦可。 例如若將單一波長雷射的振盪波長設定在1 · 5 1〜 53 200423224 1二範圍内的話,將產生波長為i89〜⑽⑽範圍内之 立丄门人°白波或是產生波長為151〜159nm範圍内之1〇 门人咱波。特別是,將振盪波長設定纟1.544〜1 553 " ::圍内時,將可得到波長為193〜194四範圍内之8倍高 次谐波,亦即# ArF準分子雷射幾乎同-波長的紫外光; 將振盈波長設定在U7〜1.58“範圍内時,將可得到波 長為157〜158nm範圍内之1〇倍高次諧波,亦即 幾乎同一波長的紫外光。 又,當振盪波長為1. 〇3〜1. 12# m範圍内時,可輸出 波長為147〜16〇nm範圍内之7倍高次諧波,特別是,當振 盪波長為1. 099〜1. 1〇6" m的範圍内時,可得到波長為 157〜158#m範圍内之7倍高次諧波’亦即與匕雷射:幾 為同一波長之紫外光。此時,單一波長振盪雷射光可採用 例如摻入鏡之光纖雷射。 又,投影光學系統PL之光源係ArF準分子雷射光源或 KrF準分子雷射光源時,大多僅是以折射光學元件(透鏡元 件)所構成的折射系統,然而在使用&雷射光源、A。雷射 光源等之際,主要係使用,如曰本專利特開平3一 了 號公報及對應之美國專利第5, 220, 454號公報中所揭示 折射光學元件及反射光學元件(凹面鏡或分束器)之組人 亦即所謂折反射系統(catadioptr ic),或是僅由反射朵與 ^ vj學 元件所構成之反射光學系統。不過,使用F2雷射光源時w 使用折射系統。 如前所述,使用折反射光學系統作為投影光學系统Wit fruit. This π enables the vicinity of the reticle stage RST to reach a substantial distance around its mouth 2 ′ 3. Therefore, in addition to having the same effect as ^ ^ 土 土 盖 & 线 片 ^, it also contributes to the miniaturization and quantity of the device. For example, the space ss in the partition wall 52 The replacement absorbing UM and the low-absorptive gas material, in addition to covering with the next wall: = quality = τ 'can also reduce the "absorption in the surrounding space" of the marking line. On the other hand, it can also reduce the amount of gas used. It has the effect of reducing the cost. Therefore, it can be used to raise the resolution of the projection optical system PL by using vacuum ultraviolet light as the exposure iris. As mentioned above, if the exposure device 100 is used, the device can also be achieved. Miniaturization and light-weighting. Exposure of 1¾ precision can be realized. The "exposure device i 100" has a mechanism (106, m) for changing the lighting conditions of the lighting system to change the pattern when it is transferred to the wafer w, and through The irradiation opening d 55b will be used to expose the lighting conditions of the projection optical system at all times. &Amp; Hour 'by this change. The use of the mechanism can change the lighting conditions according to the pattern of the reticle R, and Exposure near the pupil plane of the projection optical system PL under this lighting condition The lighting conditions such as the energy density distribution of the light EL, and the opposite of the energy distribution density of the exposure light EL are generated near the pupil plane of the projection optical system pL during virtual irradiation. 46 200423224 According to the exposure device The exposure method performed at 100 is when the wafer is not exposed (pattern transfer of the reticle R), specifically, when the wafer is exchanged, 'the wafer is not arranged on the image surface of the projection optical system PL. In the state of w, a thermal offset state caused by the exposure of the exposure light EL in the lenses 30c to 30h in the projection optical system PL during exposure can be used as a lighting condition, in the case where the reticle R is not transmitted. Next, the exposure light EL is irradiated to the projection optical system PL for virtual irradiation. Therefore, even when the pattern of the reticle R is transferred, the lenses 30c to 30h constituting the projection optical system pL are locally generated. (Uneven sentence) heating, the virtual irradiation treatment can still be used to heat the lens 3Gc ~ 3Gh to a state where the average sentence is heated. This prevents the lens 30c ~ 30h from being heated by the unevenness of the optical member. , As a result, it is difficult to compensate the rotational asymmetric aberration of the projection optical system PL, so it is possible to maintain the good imaging characteristics of the projection optical system PL to achieve high-precision exposure. Also, in this embodiment, it is performed through the opening opening for the user. The virtual irradiation of the exposure light is performed in parallel with the wafer exchange included in the exposure step, so `` there is almost no reduction in productivity due to the progress of the virtual irradiation. Also, in the above-mentioned first embodiment, the irradiation opening 55b And exposure openings are formed separately (near the exposure openings), but the method is not limited to this, for example, the size of the scanning direction of the exposure opening ^ ^ may be extended to make the exposure openings The-part doubles as an opening for irradiation. Furthermore, in the above-mentioned first embodiment, ^ -Λ 隹 is a reticle R, 鈇 Η, which uses the long sides of the pattern in the same direction. The application of the present invention is not limited to this, and a general reticle is used. The film pattern (also ^ ^ 'has both a pattern with a predetermined direction of 47 200423224 long side direction and a direction of the long side of the pattern with a direction orthogonal to the predetermined direction within 2 $ plane) also has good results. χ, exposed pure parts are not. The combination of J σ value lighting and phase-shifting reticle is also effective when used for deformation lighting with large localized illumination light. In other words, when the reticle pattern is transferred to the wafer, the light distribution of the exposure light formed on the projection optical system light = surface, and the shape is formed on the pupil surface of the projection light: system PL during virtual irradiation. It is sufficient to distribute the illumination light 1 in the shape of light-dark inversion. In particular, when lighting with a small σ value, when the long side of the pattern is used and the reticle in the same S direction is used, the light amount distribution of the exposure light on the pupil surface of the projection optical system has the largest local Therefore, the present invention is most effective when used in such exposure conditions. Furthermore, in the first embodiment described above, the lens 30a & located at the uppermost of the lenses 30a to 30j constituting the projection optical system PL is driven so as to correct the rotationally symmetric aberration by driving in the γ vehicle direction. The application of the invention is not limited to this, and other lenses can be driven to correct rotationally symmetric aberrations. A gas chamber can also be arranged between a specific lens and a lens adjacent to the specific lens, and the pressure of the gas chamber can be changed to correct the rotation. Symmetrical aberration. In other words, when a catadioptric optical system is used as the projection optical system pL, a mirror element constituting a part of the optical system of the shirt is moved slightly in the direction of the optical axis, and the rotationally symmetric aberration can be corrected. In the first embodiment described above, openings are formed in the illumination system-side platform 2 and the projection system-side platform 3 as light transmitting portions. However, its application is not limited to this, and a transparent member may be used to form the entire platform, or it may be transparent. Structure 48 200423224 pieces to constitute the penetrating portion of the exposure light. The shadow optical system and the lighting optical system 2. The transparent member can also be modified with quartz. . In the case of using fluorite or modified SS, it is not necessary to provide any of them. In addition, it is not necessary to provide both a gas supply mechanism and an exhaust mechanism in the reticle stage RST. In addition, in the first embodiment described above, the absorptive radon is low as a differential exhaust second milk or a rare gas. However, the present invention is not limited to this. When the air supply amount of the milk supply device is directly used, It can be used that the amount of oxygen exhausted is more than that of gas. In the above-mentioned first embodiment, the portion between the upper plate portion 46a and the lower plate portion 46c of the coarse reticle stage 4 is formed only by the middle portion. Yilian News Agency. The present invention is not limited to this, but the other part (+ γ side) of the coarse motion stage 4 of the reticle can be added with a support column that holds the upper plate shirt and the lower plate portion 46c. To further enhance its rigidity. The gas that is returned to the soil, and the gas that is supplied to the retention space of the reticle, should preferably be made at a predetermined temperature (2rc), and the pellets have been fully removed: organic matter, water Foreign objects such as steam. In addition, each bearing in the above-mentioned first embodiment has a double structure including an air-supply-side annular groove and a gas-supply-side annular groove. The β-hook description example is used. However, its application is not limited to Therefore, if a groove with a triple structure is used, the gas is supplied from the groove located in the middle, and the gas is introduced from the other two grooves of the middle groove of the 挟, which can also have the same air-tightening effect. In addition, Wu Yongxian's 49 200423224 is also applicable if it forms two sets of the above-mentioned double structure grooves and becomes a quadruple structure bearing. That is, the number of slots of each bearing can be arbitrarily arranged. In the first embodiment described above, although the exposure light is used during the virtual irradiation, a light source in a region different from the exposure light may be used as the energy beam for the virtual irradiation during the virtual irradiation. The beam t * 3E (for example, infrared rays) used for the virtual irradiation passes through the opening 2a, the opening cut, the opening, the opening 4b, and the opening 3a, respectively, and is directed toward the projection optical system without passing through the reticle R Irradiation. At this time, if an infrared irradiation mechanism is provided in the optical path of the exposure light, a beam splitter inserted into the optical path during virtual irradiation is provided, and the energy beam (for example, infrared rays) for the virtual irradiation is made by the beam splitter. Through the above-mentioned openings, the projection optical holes are also suitable. In the above application example, before the virtual irradiation is performed, the above-mentioned beam splitter is inserted in the exposure room of the exposure light, and is then emitted through the beam splitter. Infrared: At this time, the insertion position of the beam splitter can be between the projection optical system pL and the lighting early ILU, or in the lighting unit ILU. "Second Embodiment". The second description is based on Figure 1U and Figure 11B The second embodiment of the present invention. The "*" portion is the same as or equal to the first embodiment described above, and is given the same-symbol, and further description thereof is omitted or omitted. The exposure apparatus of the second embodiment has projection optics. The structure of the system is only slightly different from the above-mentioned ^: state, and the structure of the other swords is the same. Therefore, in order to avoid repetition, the differences are used as the main points. Figure 11A All This is a schematic configuration diagram of the exposure system PL 'constituting the second embodiment. The number is 50 200423224. As shown in FIG. 11A, the projection optical system pL is introduced from the outside into the optical fiber FB (especially the insulating glass). The inner surface of the tube is coated with aluminum fiber optics — υ Souling IV, the upper system is shown in Figure Π β, along the outer edge of the lens, the optical components (such as the lens 3c, 3d) (30g) Introduce several optical fibers FBi to FBn. These optical fibers FB are connected to an infrared radiation source (not shown) located outside of the projection optical system and first PL. At this time, a complex bismuth optical fiber FB is used. The FBn and an infrared radiation source (not shown) constitute an infrared irradiation mechanism. Since the second embodiment of the present invention also uses I? 2 laser light as the exposure light, a projection optical system PL is formed, and the lenses 30a to 3 〇j is using fluorite. It is the optical fiber Pβ that constitutes the infrared irradiation mechanism. It irradiates the lens with infrared rays with a wavelength of about 6 ~ 10 // m which is easier to be absorbed by the fluorite lens (30c, 30d, 30g). The infrared irradiation source at this time, for example, can use Semiconductor lasers for compound semiconductors such as lead sulfide, lead selenide, and lead telluride. The exposure device of the second embodiment is the same as that of the first embodiment, and the pattern of the reticle R is transferred. It is printed on the wafer w. Furthermore, a control mechanism (not shown) calculates the optical components (for example, the lens 30c, which constitutes the projection optical system pL, according to the pattern or illumination conditions of the reticle used for the exposure. 30d, 30g), and based on the calculated exposure light distribution, predict the thermal bias state that should occur in the lens (30c, 30d, 30g), and correspond to the prediction As a result, an appropriate optical fiber was selected from the plurality of optical fiber FBn fields, and the lens (30c, 30d, 30g) was irradiated with infrared rays by the selected optical fiber. In addition, infrared rays can be irradiated on either the surface of each lens (30c, 51 200423224, or 3Od, 30g). The incident surface or the emission surface of the light source for exposure is irradiated on both the incidence surface and the emission surface. ~ 丨 · Please, when Dian predicts that there is a heating state shown in Figure UB ', that is, infrared light is provided by optical fibers other than _ and PBn, so that the heating state approaches a rotationally symmetrical shape. In addition, by adjusting the position of the movable lens in the projection optical system η, for example, adjusting the position of the optical axis direction of 30a ', the rotational symmetric aberration of the projection optical system and the system PL is corrected in the same manner as in the first embodiment. . As disclosed above, the pattern formed on the reticle is transferred onto the wafer W through the projection optical system PL ′ by the exposure device and method of the method that is used in the form of Taisheng 0a. (At the time of exposure), even if the lens constituting the projection optical system PL is locally (non-uniformly) added by the exposure light EL, the infrared irradiation mechanism can still be used for other lenses that are not illuminated by the exposure light source 乩The infrared rays are partially provided and heated, and as a result, the lens can be heated to a substantially uniform state. This makes it possible to prevent asymmetrical aberrations that are difficult to correct in the projection optical system and the system PL due to the heating of the uneven sentence of the lens, which has a good suppression effect. In this case, the infrared irradiating mechanism can heat the transmission, and it can also be performed during exposure. Therefore, compared with the above-mentioned embodiment, the 'asymmetric aberration of the projection optical system can be suppressed more reliably. Therefore, it is possible to maintain good imaging characteristics of the projection optical system while the exposure is in progress, and realize high-precision exposure. Infrared heating to the lens is different from heating by the contact heating mechanism (..., original) or cooling by the contact cooling mechanism. Because it is not in contact with the lens, it will not be caused by contact with the heating or cooling mechanism. 52 200423224 The lens is skewed, and there is no lens vibration caused by air cooling. Furthermore, the exposure performed by the combination of the above-mentioned illumination beam with a small illumination σ and a phase-shift reticle, or the localization of the illumination light becomes more serious ^ Illumination sometimes depends on only one exposure step. Unable to form (transfer) all circuit patterns to be exposed. At this time, according to the predetermined lighting conditions, one wafer can be exposed from the predetermined rod and wire strips. After the reticle is exchanged, the other lighting conditions can be changed to expose another pattern (double exposure) on the wafer. To form all the desired patterns. In the case of this double exposure, it is possible that the optical path length of the exposure light in the projection optical system may be changed during two individual exposures, so that the heat generation of the material accompanying the absorption exposure light source may be averaged. There are many cases where the exposure cannot be fully averaged. Therefore, the present invention can still exert an excellent effect in the case of performing double exposure. In addition, in the above embodiments, although pulse laser light sources in the vacuum ultraviolet region, such as h laser, laser, Ar2 laser, and ArF excimer laser, are used as the light source, their applications are not limited thereto. It is also preferable to use a Kβ excimer laser as its light source. For another example, there is no specific limitation on the laser light in the vacuum ultraviolet region output by each of the above light sources. A DFB semiconductor laser, an infrared region oscillated by a laser fiber, or a single wavelength laser light in the visible region, for example, It is also possible to use erbium (Er) (or both erbium and mirror (Yb))-doped optical fibers to amplify and amplify and use non-linear optical crystals to convert the wavelength to high-frequency ultraviolet light. For example, if the oscillation wavelength of a single-wavelength laser is set in the range of 1.5 · 1 ~ 53 200423224 1 · 2, it will generate a Liemenmen ° white wave with a wavelength in the range of i89 ~ ⑽⑽ or a wavelength in the range of 151 ~ 159nm. Among the 10 people we wave. In particular, when the oscillation wavelength is set to 纟 1.544 ~ 1 553 ": within the range, 8 times higher harmonics with a wavelength in the range of 193 ~ 194 will be obtained, that is, the #ArF excimer laser is almost the same as- Ultraviolet light with a wavelength; When the vibrational wavelength is set within the range of U7 ~ 1.58 ", a harmonic wave of 10 times higher than the wavelength in the range of 157 ~ 158nm can be obtained, that is, ultraviolet light with almost the same wavelength. Also, when 1 099〜1. 1 When the oscillation wavelength is 1. 〇3 ~ 1. 12 # m range, the wavelength can be 7 times higher harmonics within the range of 147 ~ 160nm, especially when the oscillation wavelength is 1. 099 ~ 1. 1 〇6 " In the range of m, you can get 7 times higher harmonics in the range of 157 ~ 158 # m, that is, the same as the laser light: almost the same wavelength of ultraviolet light. At this time, a single wavelength oscillation mine For example, an optical fiber laser doped with a mirror can be used as the light. In addition, when the light source of the projection optical system PL is an ArF excimer laser light source or a KrF excimer laser light source, most of them are constituted by refractive optical elements (lens elements). Refraction systems, however, are mainly used when using & laser light sources, A. laser light sources, etc. The group of refractive optical elements and reflective optical elements (concave mirrors or beam splitters) disclosed in Japanese Patent Application Laid-Open No. 31 and corresponding US Patent No. 5,220,454 is also known as a refracting system ( catadioptr ic), or a reflective optical system consisting of a reflective element and a vj element. However, when using an F2 laser light source, a refractive system is used. As mentioned earlier, a refracting optical system is used as the projection optical system.
、、P L 54 200423224 上述透鏡,亦可照射 元件(例如凹面鏡、 時,上述紅外線的照射範圍可不限於 於折反射光學系統中所含的反射光學 分束器、稜鏡、或平面鏡等 再者,紅外線的照射對象為凹面鏡、平面鏡等反射鏡 之反射面日夺’希望使用的紅外線係在該反射面可被大幅吸 收的波長域’此點應不言自日月。例如,在反射面已塗布銘 ^ ’希望所使用的紅外線之波長,係對鋁的反射率低,亦 即吸收大之700〜900nm波長區間。 又,紅外線對反射鏡的照射面,並不偽限於其反射面 ’亦可對其背面或側面進行。此時亦與上述情況相同的, 因曝光用光的照射造成反射鏡發熱所導致之反射鏡變形, 可藉由紅外線的照射而予以相抵,以達成反射鏡的均熱化。 再者,照射於反射鏡的上述背面或側面之紅外線,亦 希望使用在該部分的吸收程度大的波長域。 此外,如前所述,以照射紅外線來加熱構成投影光學 系統的透鏡及反射鏡或稜鏡,在因曝光用光之吸收使該等 光學構件(光學7L件)發熱時,亦為了良好保持該投影光學 系統之成像狀態而進行。因Λ,只要有可能藉由將各光學 構件(透鏡、反射鏡、稜鏡等)的内部溫度分布設定成既定 關係,即可保持投影光學系統之良好成像狀態,此時,即 使所有光學構件之内部溫度未完全均熱化亦可。 亦即,當吸收曝光用光所造成的既定光學構件(透鏡、 反射鏡、稜鏡)内的溫度分布變動,嚴重影響投影光學系 、,先的成像性肖b打,可以免於為求均熱化而對該既定光學構 55 200423224 件照射紅外線,相對的,係代之以對其他的光學構件照射 紅外線’以求取投影光學系統全體之良好成像性能。 又’上述各實施形態中,對標線片載台RST構成之說 明例’係在照明系統側平台2及投影系統側平台3之間具 備標線片粗動載台4及標線片微動載台5,其中標線片微 動載台5係被該標線片粗動載台4圍於土z方向及一 γ方向 之三個方向而被保持於該狀態,然而,本發明之構成不侷 限於此。例如,亦可在標線片粗動載台4的~ Z方向之間 隔壁中,設有供標線片微動載台5插入的開口,標線片微 動载台5對於標線片粗動載台4及投影系統側平台3,係 么差動排氣之非接觸方式被支持著。&,當標線片微動載 5兼具有標線片粗動載台之功能時,亦可使投影系統側 平台或照明系統側平台的-部分構成覆於光罩周圍之間隔 阱田从t …,/…“…m、杈碉柯)亦需β 八:先源而區別之。使用ArF準分子雷射光源或μ ^ 刀子雷射光源時’可使用合成石英或螢石之雙方,但使用 2田射等真空紫外光源時,必須全部使用螢石。又,除壁 石1 卜二Γ可使用m氟储、及氟化料氟化物單晶 物“:':紹之複合氣化物結晶、鐘-錯-銘之複合氣化 力—鑭—㈣構成之氟化玻璃、摻氟的石英 氣且加Γ其且力口 t之石英破璃、含有0H基之石英玻璃,加 fl基之石英玻璃等改良石英。 再者,上述各實施形態中’雖係以步進掃描式等之掃 56 200423224 描型曝光裝置’作為適用本發明之說明例,然@,理所洛 然:,本發明之適用範圍不侷限於此。亦#,步進重複: 之縮小投影曝光裝置亦適用於本發明。 -再者’上述各實施形態的曝光裝4 100等本發明所揭 不之曝光裝置’其製造之時’係將複數片透鏡所構成之照 明兀件、投影光學系統組裝人曝光裝置本體,進行光學調 整’且將由多數機械元件所構成的晶圓載台(使用掃描型 時亦含標㈣載台)安裝於曝光裝置本體,且連接線路或 配管,安裝由照明系統側平台2、投影系統側平台3、及晶 圓室40所構成之間隔壁,連接氣體之配管,將未圖示之控 制裝置等控制系統統連接至各部&,且施以综合性調整( 電、動作確認等)來製造之。x,曝光裝置之製造 最好疋在/Jm_度及潔淨度受到管控之無塵室進行。 《元件製造方法》 以下祝明在微影步驟中使用上述曝光裝置丨〇〇之元 件製造方法的實施形態。 圖12所不’係元件(IC或LSI等半導體晶片、液晶面 板、CC一D、薄膜磁頭、微機器等)之製造例的流程圖。如圖 12所不瓜,百先,在步驟2〇1 (設計步驟)中,進行元件之 功能則生能設言十(例如半導體元件的電路設計等),以及具 迟力此之圖木的设汁。接著,在步驟別2(光罩製作步驟 )中,製作出含有設計電路圖案的光罩。另一方面,在步 •V 203(日日圓製造步驟)中,使时等材料以製造晶圓。 其人,在步驟204(晶圓處理步驟)中,使用已在步驟 57 200423224 201〜步驟203業已製備之光罩及晶圓,上μ 夂日日0,如後述般地藉微影 技術等在晶圓上形成實際電路等。接篓 接者,在步驟205(單元 裝步驟)中’使用在步驟2G4中處理的晶圓進行㈣的 。該步驟205中,視需要包含切割、結合、及 片)等製程。 θθ 所製 經以 最後,在步驟206(檢查步驟)中,對於步驟2〇5 成的元件,進行動作確認之測試、及耐久性等檢查。 上製程後而完成元件,加以出貨。 圖13所示’係對半導體元件中上述步驟咖的詳細产 程例。圖13中,步驟211(氧化步驟)係使晶圓表面氧化? 步驟212(CVD步驟)係在晶圓表面形成絕緣膜。步驟⑽ 形成電極步驟)係在晶圓上藉蒸鑛形成電極。步驟214(離 子植入步驟)係將離子植入晶圓内。以上步驟2ιι〜2“, 分別構成晶圓處理之各個階段的前處理製程,在各階段中 視所需處理選擇性實施。 又 在晶圓形成的各階段中,完成上述前處理製程,即如 下述般地實施後處理製程。該後處理製程的步驟,首先係 在步驟215(光阻形成步驟)將感光劑塗布於晶圓。接著在 乂驟216中(曝光步驟)中,藉由上述各實施形態中本發明 之曝光裝置及其曝光方法,將光罩的電路圖案轉印於晶圓 。転而’在步* 217(顯影步驟)中使已曝光的晶圓顯像, 在步驟刻步驟)中,以㈣將殘存光阻以外的部分( ,出構件)予以去除。又,在步驟219(光阻去除步驟),將 兀成钱刻後不需的光阻去除。 58 200423224 圓 經反覆實施該些前處理製程及後處理製程,而在晶 上形成多重電路。 ^ ^ 、上所揭示之本實施形態的元件製造方法,因 在…中的曝光製程中(步驟216)係使用上述各實施形態之 曝光叙置及其曝光方法,故可維持高精度的曝光,因而, 對於具有微細圖案的高集成精密元件,可提昇生產效能。 k來為進一步提昇c_m〇s—lsi的性能,所使 用的石夕晶圓,亦右命:古μ ^ 直於矽晶圓表面的軸與結晶軸的[111 ] 致者,亦即,使晶圓表面與結晶面之〈⑴〉面-致 的晶圓。 :如’在上述元件製程中,使用石夕晶圓表面與結晶面 :的::致的晶圓時’希使Μ。"晶體的電浏 =移:方向,與”晶的⑽]軸之方向或與其等價 ixr代表軸的指數順序已替換的心是符= 亦即,較佳之M0S電晶體的閘極 為〗20度間隔之 口茶《長邊刀向’雖 圖案之精产關# 因為描緣於標線片R的 ^槓度關係’微細圖案最 正方形)之邊,故實質上被侷限於同:方千:於標線 因此,為提昇C—M0S—LSI的性 於結晶面之<111>φ—致的晶圓時 ^晶圓表面 寻別疋在轉印閘極圖案 59 200423224 之曝光製程中,由於圖案的長邊方向並排於同一方向,因 ^光用光之吸收而使投影光學系統的旋轉非對稱發熱及像 差尤為顯著,因此,在上述第卜第2實施形態中分別實 施的虛擬照射、紅外線照射之效果,最為明顯。 再者’上述兀件製程中’無庸贅言的,亦可使用垂直 於表面的軸’與結晶轴之[110]軸大致一致,亦即使晶圓表 面―日日面之<1U>面—致之晶圓,此時,M0S電晶體的電 子及U (正孔)之移動方向,最好是能與石夕結晶之⑴轴 方向或其等價轴方向一致,俾利於電子及電洞的移動度。 因而,M0S電晶體的閉極圖案之長邊方向,最好是能與 [110]軸正交的[211]軸方向或其等價軸方向一致。如前所 j,有時使閘極圖案的方向並排於同—方向較佳,此時, 藉由上述虛擬照射、紅外線照射,亦同樣可形成高精度的 圖案。 再者,上述所指,晶圓表面為♦結晶之〈⑴〉面的晶圓 並非僅限於白知的塊狀(bulk)晶圓亦可為如I (Silicon ⑽Insulator,即絕緣物上有石夕)晶圓。使用s〇i晶圓時’ 其表面部分时’同樣指其表面與結晶之〈⑴〉面—致之晶 圓。 如以上之說明,本發明之曝光裝置及曝光方法,非常 適口在以月b里束恥明光},使形成於光罩的圖案透過投影 光學系統轉印至感光物體上時。X,本發明之元件製造方 法,適於微元件的製造。 60 200423224 【圖式簡單說明】 (一)圖式部分 f 1圖’係顯示帛1實施形態之曝光裝置的概略圖。 弟2圖,係顯示略去標線片載台及其附近之一 立體圖。 1刀的 第3圖,係標線片載台的縱截面圖。 弟4A,4B圖,4A係第3圖之A_A線截面圖 圖之B—B線截面圖。 第5圖,係顯示用於第i實施形態之曝光裝置之 片(移相標線片)的俯視圖。 '、、 一第6a,6B圖,6A係顯示從照明孔徑光闌射出之照明 光束的光量分布® ® 6b係暴員示投影光學系統内之透鏡中 曝光用光源偏置狀態的圖。 第7圖,係顯示曝光用光在投影光.學系統PL内的能量 分布圖。 第8A,8B圖,8A係虛擬照射時從照明孔徑光闌射出 之照明光束的光量分布圖;8B係虛擬照射時在投影光學系 統内之透鏡之曝光用光之狀態的圖。 第9圖,係顯示繞射光學單元的圖。 第10圖,係顯示照明孔徑光闌板的圖。 弟11A,11B圖’ 11A係顯示第2實施形態之投影光學 系統的構成圖;Π B係顯示導入投影光學系統内之光纖的 配置圖例。 第12圖,係用以說明本發明之元件製造方法的流程圖。 第13圖,係第12圖中之步驟204的具體流程示例。 61 200423224 )元件代表符號 3 2a,3a,4a,4b,55b 4 5 6a, 6b 6c 9,9c 11a lib 11c 18,29 21 25 26a〜26d 27, 31, 33, 58 28, 32, 34, 59 30a〜30j 35 36 37 38 照明系統側平台 投影系統側平台 開口部 標線片粗動載台 標線片微動載台 繞射光學元件 光學元件保持器 標線片雷射干涉儀 σ光闌 虛擬照射用光圈闌 驅動裝置 密封機構(風箱) 光束整形光學系統 晶圓保持具 支持柱 供氣側環狀凹槽 排氣側環狀凹槽 透鏡 供氣管路 排氣管路 供氣管 排氣管 39 配線束 62 200423224 40 41,50 43,51 42a, 42b, 42c 46a 46b 46c 47a 48a, 48b 49a, 49b 52 52a 53 54 55 55a 55b 56y 57 58, 59 61 63 71 晶圓室 供應管路 排氣管路 保持構件 上板部 中間部 下板部 支持構件 可動件 定子 間隔壁 矩形開口 標線片保持機構 真空管線 底面構件 曝光用開口 照射用開口 移動鏡 Y軸雷射干涉儀 環形凹槽 電路圖案 孔徑光闌 間隔壁 光穿透窗 63 85 200423224 86 防振單元 91c 平面反射鏡 91a, 91b 倒反射鏡 100 曝光裝置 101 光源 102 送光光學系統 103a 光束擴徑器 103b 柱面透鏡 104a, 104b 安裝構件 105 照明系統外殼 106 射光學單元 107, 109 中繼透鏡 108 反射鏡 110 光學積分器(複眼透鏡) 111 照明系統孔徑光闌板 112, 114 中繼透鏡 113a 固定標線片遮板 113b 可動標線片遮板 115 彎曲反射鏡 116 聚束器 221a, 221b 供氣支管 222a, 222b 排氣支管 ILU 照明單元 PL,PL, 投影光學系統 64 200423224 RST 標線片載台 WST 晶圓載台 EL 曝光用光源 RM1, RM2 線性馬達 AC1, AC2,AC3 微小致動器 PZ 壓電元件 SS 標線片保持空間 FB 光纖 PA 圖案區PL 54 200423224 The above lenses can also irradiate elements (for example, concave mirrors, the above-mentioned infrared irradiation range may not be limited to the reflective optical beam splitters, chirps, or flat mirrors included in the refracting optical system). The object of illumination is the reflective surface of a reflecting mirror such as a concave mirror or a flat mirror. The point that the infrared light that you want to use is in the wavelength range where the reflective surface can be greatly absorbed should be self-explanatory. For example, the reflective surface has been coated ^ 'I hope that the wavelength of the infrared rays used is low in reflectivity to aluminum, that is, in the wavelength range of 700 to 900 nm where the absorption is large. In addition, the irradiation surface of the mirror with infrared rays is not limited to its reflective surface.' It is performed on the back or side. At this time, as in the above case, the deformation of the mirror caused by the heating of the mirror caused by the exposure light can be offset by the irradiation of infrared rays to achieve the uniform heating of the mirror. In addition, it is also desirable to use infrared rays that irradiate the above-mentioned back surface or side surface of the mirror in a wavelength region that has a large degree of absorption in this part. As mentioned above, the lenses, mirrors, and grate that constitute the projection optical system are heated by irradiating infrared rays. When the optical components (optical 7L elements) are heated due to the absorption of exposure light, the projection optical system is also well maintained. The imaging state is performed. Because Λ, it is possible to maintain a good imaging state of the projection optical system as long as it is possible to set the internal temperature distribution of each optical member (lens, mirror, 稜鏡, etc.) to a predetermined relationship. Even if the internal temperature of all optical components is not completely heated, that is, when the temperature distribution changes in a given optical component (lens, reflector, ridge) caused by absorption of exposure light, it seriously affects the projection optical system. In order to obtain uniform projection, it is possible to avoid irradiating infrared rays on the given optical structure 55 200423224 pieces. Instead, irradiate infrared light to other optical components to obtain projection optics. The good imaging performance of the entire system. Also, in the above-mentioned embodiments, an example of the configuration of the reticle stage RST is shown on the lighting system side platform. A reticle coarse motion stage 4 and a reticle micromotion stage 5 are provided between 2 and the projection system side platform 3. The reticle micromotion stage 5 is surrounded by the reticle coarse motion stage 4 The three directions of the direction and a γ direction are maintained in this state, however, the configuration of the present invention is not limited to this. For example, a partition wall of the reticle coarse movement stage 4 in the ~ Z direction may be provided with There is an opening for the reticle micro-motion stage 5 to be inserted. The reticle micro-motion stage 5 is supported by the non-contact method of differential exhaust for the reticle coarse-motion stage 4 and the projection system side platform 3. & When the reticle micro-motion carrier 5 also has the function of the reticle coarse-motion stage, the-part of the projection system side platform or the lighting system side platform can also constitute a spaced Ikeda covered around the photomask. t…, /… “… m, Jiao Ke) also need β VIII: the difference between the first source. When using an ArF excimer laser light source or a μ ^ knife laser light source, both synthetic quartz and fluorite can be used. However, when using a vacuum ultraviolet light source such as 2 fields, all fluorite must be used. In addition, in addition to the wall stone 1 and the second Γ, m fluoride storage and fluoride single crystals of fluoride materials can be used: ": Shao's composite gaseous crystals, Zhong-zhao-ming's composite gasification force-lanthanum-scandium composition Fluorinated glass, Fluorine-doped quartz gas, Quartz glass with Γ added, Quartz glass with 0H group, Quartz glass with 0H group, Quartz glass with fl group, etc. Furthermore, in the above-mentioned embodiments, although The scanning exposure device of the step-scan type 56 200423224 is used as an illustrative example of applying the present invention, but @ , 理 所 洛 然:, the scope of application of the present invention is not limited to this. Also #, step repeat: The reduced projection exposure apparatus is also applicable to the present invention.-Furthermore, the exposure apparatus disclosed in the present invention such as the "exposure apparatus 4 100 of each of the above embodiments", "at the time of manufacture", is an illumination element composed of a plurality of lenses. 、 The projection optical system is assembled by the exposure device body to perform optical adjustments. And a wafer stage (including a standard stage when scanning type is used) composed of most mechanical components is installed on the exposure device body, and the connection line or piping is installed. By the lighting system side platform 2 The partition wall composed of the projection system side platform 3 and the wafer chamber 40 is connected to the gas piping, and control systems such as control devices (not shown) are connected to each department & comprehensively (electricity, motion (Confirmation, etc.) to manufacture. X, the exposure device is best manufactured in a clean room where / Jm_ degree and cleanliness are controlled. "Element Manufacturing Method" I wish to use the above exposure device in the lithography step. An embodiment of the method for manufacturing a device. Figure 12 is a flowchart of a manufacturing example of a device (such as a semiconductor wafer such as an IC or an LSI, a liquid crystal panel, a CC-D, a thin-film magnetic head, or a microcomputer). Don't worry, Baixian, in step 201 (design step), the function of the component can be set to ten (for example, the circuit design of semiconductor components, etc.), and the design of the map with the delay force. In step 2 (mask making step), a mask containing a design circuit pattern is produced. On the other hand, in step V 203 (Japanese yen manufacturing step), a time-honored material is used to manufacture a wafer. Person at step 204 (wafer processing In step), the mask and wafer that have been prepared in step 57 200423224 201 to step 203 are used, and the next day is 0, and the actual circuit is formed on the wafer by lithography technology as described later. Then, in step 205 (unit-packing step), the wafers processed in step 2G4 are used for ㈣. In step 205, processes such as cutting, bonding, and wafers are included as necessary. Θθ In step 206 (inspection step), the component completed in step 205 is tested for operation confirmation and durability inspection. After the process is completed, the component is completed and shipped. As shown in FIG. Example of the detailed production process of the above-mentioned step in the device. In FIG. 13, step 211 (oxidation step) is to oxidize the wafer surface? Step 212 (CVD step) is to form an insulating film on the surface of the wafer. Step ⑽ The electrode formation step) is to form an electrode by vaporizing ore on the wafer. Step 214 (ion implantation step) is implanting ions into the wafer. The above steps 2 to 2 "constitute the pre-processing processes of each stage of the wafer processing, and are selectively implemented in each stage depending on the required processing. In each stage of wafer formation, the above-mentioned pre-processing process is completed, as follows The post-processing process is generally performed. The steps of the post-processing process are firstly applying a photosensitizer to the wafer in step 215 (photoresist formation step). Then in step 216 (exposure step), the above-mentioned implementation is performed. In the form, the exposure device and the exposure method of the present invention transfer the circuit pattern of the photomask to the wafer. Then, 'the exposed wafer is developed in step * 217 (development step), and the step is engraved) In the process, ㈣ is used to remove the remaining photoresist (except the component), and in step 219 (photoresist removal step), the unnecessary photoresist is removed after being carved into a coin. 58 200423224 Round repeated implementation These pre-processing processes and post-processing processes form multiple circuits on the wafer. ^ ^ The device manufacturing method of the present embodiment disclosed above is used in the exposure process (step 216) in ... The exposure method and method of the exposure mode can maintain high-precision exposure. Therefore, for highly integrated precision components with fine patterns, production efficiency can be improved. K is to further improve the performance of c_m0s-lsi. The Shi Xi wafer used is also right-handed: the ancient μ ^ [111] is the same as the axis of the silicon wafer surface and the crystal axis, that is, the <⑴> plane of the wafer surface and the crystal plane is the same Wafer: such as 'In the above-mentioned device manufacturing process, when using the surface of the wafer and the crystal plane of Shixi ::: the same wafer', hope that M. " Electricity of the crystal = shift: direction, and "crystalline ⑽] the direction of the axis or its equivalent ixr represents the exponential order of the axis has been replaced by the heart symbol = that is, the gate electrode of the better M0S transistor 〖20-degree interval mouth tea "long side knife direction" Although the essence of the pattern产 关 # Because it is drawn on the edge of the reticle of the reticle R, the fine pattern is the most square), so it is essentially limited to the same: Fang Qian: On the reticle. Therefore, in order to improve the performance of C-M0S-LSI In the case of <111> φ-shaped wafers on the crystal plane ^ The wafer surface is identified by the transfer gate pattern 59 200423 In the exposure process of 224, because the long sides of the pattern are side by side in the same direction, the rotation asymmetric heating and aberration of the projection optical system are particularly significant due to the absorption of light. Therefore, in the second embodiment described above, The effects of virtual irradiation and infrared irradiation implemented in China are the most obvious. Furthermore, it is needless to say that in the above-mentioned manufacturing process, an axis perpendicular to the surface can also be used, which is approximately the same as the [110] axis of the crystal axis. At this time, the movement direction of the electrons and U (positive hole) of the M0S transistor should preferably be consistent with the y-axis direction or the equivalent axis direction of Shi Xi crystal, which is conducive to the movement of electrons and holes. degree. Therefore, the long side direction of the closed electrode pattern of the MOS transistor should preferably be the same as the [211] axis direction orthogonal to the [110] axis or its equivalent axis direction. As previously described, it is sometimes better to make the gate patterns side by side in the same direction. At this time, by the above-mentioned virtual irradiation and infrared irradiation, a high-precision pattern can also be formed. In addition, as mentioned above, the wafer whose surface of the wafer is a crystalline (结晶) surface is not limited to the bulk wafer of Bai Zhi. It can also be, for example, I (Silicon ⑽Insulator), that is, there is a stone on the insulator. ) Wafer. When using a soi wafer, 'the surface portion' also refers to the crystal circle between the surface and the <⑴> plane of the crystal. As explained above, the exposure device and exposure method of the present invention are very palatable when the pattern formed on the photomask is transferred to the photosensitive object through the projection optical system. X, the device manufacturing method of the present invention is suitable for manufacturing a micro device. 60 200423224 [Brief description of the drawings] (I) Schematic part f 1 Figure ′ is a schematic view showing an exposure apparatus of the first embodiment. Figure 2 is a perspective view showing one of the graticule stage and its vicinity omitted. Figure 3 of 1 knife is a longitudinal sectional view of a reticle stage. Figures 4A, 4B, 4A are the sectional views taken along line A_A in Figure 3, taken along line B-B. Fig. 5 is a plan view showing a sheet (phase-shifted reticle) used in the exposure apparatus of the i-th embodiment. Figures 6a, 6B, and 6A are diagrams showing the light quantity distribution of the illuminating light beam emitted from the illumination aperture stop ® ® 6b is a diagram showing the biased state of the light source for exposure in the lens in the projection optical system. Fig. 7 is a graph showing the energy distribution of the exposure light in the projection light science system PL. 8A and 8B, 8A is a light quantity distribution diagram of an illumination beam emitted from an illumination aperture stop during virtual irradiation; 8B is a diagram of a state of exposure light of a lens in a projection optical system during virtual irradiation. Fig. 9 is a diagram showing a diffractive optical unit. Fig. 10 is a diagram showing an iris diaphragm. Figures 11A and 11B '11A is a diagram showing the structure of a projection optical system according to the second embodiment; ΠB is a diagram showing an arrangement of optical fibers introduced into the projection optical system. Fig. 12 is a flowchart for explaining a method for manufacturing a device according to the present invention. FIG. 13 is a specific process example of step 204 in FIG. 12. 61 200423224) Element representative symbols 3 2a, 3a, 4a, 4b, 55b 4 5 6a, 6b 6c 9, 9c 11a lib 11c 18, 29 21 25 26a ~ 26d 27, 31, 33, 58 28, 32, 34, 59 30a ~ 30j 35 36 37 38 Illumination system side platform projection system side platform opening reticle coarse movement stage reticle micro movement stage diffraction optics optical element holder reticle laser interferometer σ diaphragm virtual irradiation Sealing mechanism (wind box) with diaphragm drive device Beam shaping optical system Wafer holder Supporting column Air supply side annular groove Exhaust side annular groove lens Air supply pipe Exhaust pipe Air supply pipe Exhaust pipe 39 Wiring Beam 62 200423224 40 41, 50 43, 51 42a, 42b, 42c 46a 46b 46c 47a 48a, 48b 49a, 49b 52 52a 53 54 55 55a 55b 56y 57 58, 59 61 63 71 Wafer chamber supply line Exhaust line Holding member Upper plate part Middle part Lower plate part Support member Movable stator Partition wall Rectangular opening reticle Retaining mechanism Vacuum line Bottom member Exposure opening Exposure opening Exposure moving mirror Y-axis laser interferometer Ring groove Circuit pattern Aperture stop Next door light Transmission window 63 85 200423224 86 Anti-vibration unit 91c Plane mirror 91a, 91b Inverted mirror 100 Exposure device 101 Light source 102 Light transmission optical system 103a Beam expander 103b Cylinder lens 104a, 104b Mounting member 105 Lighting system housing 106 Optical unit 107, 109 Relay lens 108 Reflector 110 Optical integrator (Flying lens) 111 Illumination aperture diaphragm 112, 114 Relay lens 113a Fixed reticle shield 113b Moveable reticle shield 115 Curved reflector 116 Concentrator 221a, 221b Air supply branch pipes 222a, 222b Exhaust branch pipes ILU Lighting unit PL, PL, projection optical system 64 200423224 RST reticle stage WST Wafer stage EL Exposure light source RM1, RM2 Linear motors AC1, AC2 , AC3 micro-actuator PZ piezoelectric element SS reticle holding space FB fiber PA pattern area
6565
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JP2002351336 | 2002-12-03 |
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TW92133809A TW200423224A (en) | 2002-12-03 | 2003-12-02 | Exposure system, exposure method, and device fabricating method |
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AU (1) | AU2003284540A1 (en) |
TW (1) | TW200423224A (en) |
WO (1) | WO2004051716A1 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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TWI386682B (en) * | 2004-12-17 | 2013-02-21 | Avago Tech Ecbu Ip Sg Pte Ltd | Method and system for generating substantially uniform speckle patterns |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
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US7903234B2 (en) | 2006-11-27 | 2011-03-08 | Asml Netherlands B.V. | Lithographic apparatus, device manufacturing method and computer program product |
SG143178A1 (en) * | 2006-11-27 | 2008-06-27 | Asml Netherlands Bv | Lithographic apparatus, device manufacturing method and computer program product |
NL2007498A (en) | 2010-12-23 | 2012-06-27 | Asml Netherlands Bv | Lithographic apparatus and method of modifying a beam of radiation within a lithographic apparatus. |
JP2022096141A (en) | 2020-12-17 | 2022-06-29 | キヤノン株式会社 | Exposure method, exposure device and manufacturing method of article |
ES2967699T3 (en) * | 2021-10-14 | 2024-05-03 | Ivoclar Vivadent Ag | Oven to heat a dental object |
ES2968215T3 (en) * | 2021-10-14 | 2024-05-08 | Ivoclar Vivadent Ag | Exposure device for exposing a dental object |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH09232213A (en) * | 1996-02-26 | 1997-09-05 | Nikon Corp | Projection aligner |
JPH09298143A (en) * | 1996-05-02 | 1997-11-18 | Hitachi Ltd | Exposure and device |
EP0823662A2 (en) * | 1996-08-07 | 1998-02-11 | Nikon Corporation | Projection exposure apparatus |
WO2000068980A1 (en) * | 1999-05-07 | 2000-11-16 | Nikon Corporation | Method and apparatus for exposure |
DE10000191B8 (en) * | 2000-01-05 | 2005-10-06 | Carl Zeiss Smt Ag | Project exposure system of microlithography |
JP3490068B2 (en) * | 2001-03-14 | 2004-01-26 | 株式会社半導体先端テクノロジーズ | Photomask storage device, projection exposure apparatus and projection exposure method |
-
2003
- 2003-12-02 TW TW92133809A patent/TW200423224A/en unknown
- 2003-12-02 WO PCT/JP2003/015436 patent/WO2004051716A1/en not_active Application Discontinuation
- 2003-12-02 AU AU2003284540A patent/AU2003284540A1/en not_active Abandoned
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI386682B (en) * | 2004-12-17 | 2013-02-21 | Avago Tech Ecbu Ip Sg Pte Ltd | Method and system for generating substantially uniform speckle patterns |
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AU2003284540A1 (en) | 2004-06-23 |
WO2004051716A1 (en) | 2004-06-17 |
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