TW497149B - An illumination optical apparatus - Google Patents

An illumination optical apparatus Download PDF

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Publication number
TW497149B
TW497149B TW090116870A TW90116870A TW497149B TW 497149 B TW497149 B TW 497149B TW 090116870 A TW090116870 A TW 090116870A TW 90116870 A TW90116870 A TW 90116870A TW 497149 B TW497149 B TW 497149B
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Taiwan
Prior art keywords
light
optical system
light source
illumination
optical
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TW090116870A
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Chinese (zh)
Inventor
Tanitsu Oasmu
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Nikon Corp
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    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70058Mask illumination systems

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
  • Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
  • Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Environmental & Geological Engineering (AREA)
  • Epidemiology (AREA)
  • Public Health (AREA)
  • Microscoopes, Condenser (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Optics & Photonics (AREA)

Abstract

The present invention effectively suppresses light quantity loss and securing a prescribed focus depth and is capable to improve the resolution of a projecting optical system to a prescribed pattern shape. The apparatus is provided with angle luminous flux forming means (4, 5) for converting luminous fluxes projected from a light source means (1) into luminous fluxes of various angle components to a reference optic axis (AX) and making them be incident on a first prescribed surface; irradiation field formation means (6, 7) for forming two irradiation fields which are eccentric almost symmetrical with respect to the reference optical axis on a second prescribed surface, based on the incident luminous fluxes of the various angle components; an optical integrator (8) for forming a bipolar secondary light source provided with the almost same light intensity distribution, based on the luminous fluxes from the formed two irradiation fields; and a light guide optical system (10) for guiding the luminous fluxes form the optical integrator to a surface (M) to be irradiated.

Description

4^7149 A7 _ B7 五、發明説明(1 ) 發明領域 本發明係有關照明光學裝置及具備該照明光學裝置的曝 光裝置,尤其是有關適用於以微影步驟製造半導體元件、 攝影元件、液晶顯示元件或薄膜磁頭等裝置之曝光裝置的 照明光學裝置。 先前之相關技藝 此種典型之曝光裝置係自光源射出之光束射入複眼透 鏡,在其後端之焦點面上形成包含許多光源像的二次光 源。二次光源射出的光束被配置於複眼透鏡後端焦點面附 近之孔徑光圈限制後,射入聚光鏡。孔徑光圈因應所需之 照明條件(曝光條件)將二次光源的形狀或大小限制在所需 的形狀或大小。 被聚光鏡聚光的光束重疊照明形成有指定圖案的掩膜。 穿透掩膜圖案的光線經由投影光學系統在晶圓上成像。如 此,掩膜圖案在晶圓上被投影曝光(複製)。另外,形成在 掩膜上的圖案被高積體化,將該微細圖案正確複製到晶圓 上時,晶圓上獲得均勻之照明分布爲不可或缺的條件。 m 近年來,藉由使配置在複眼透鏡射出端之孔徑光圈之孔 徑部(光穿透部)的大小改變,使複眼透鏡所形成之二次光 源的大小改變,且使照明之相關性β ( J値=孔徑光圈/投 影光學系統的瞳孔徑、或0*値=照明光學系統之射出端孔 徑數/投,影光學系統之射入端孔徑數)改變的技術受到矚 目。此外,藉由將配置在複眼透鏡之射出端之孔徑光圈的 孔徑部形狀設定成輪帶狀及四孔狀(亦即四極狀),將複眼 -4- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 4β7149 Α7 ______— Β7 五、發明説明(2 ) 透鏡所形成 < 二次光源的形狀限制在輪帶狀及四極狀,使 投影光學系統之焦點深度及解像力提高的技術受到矚目。 如上所述,先前技術由於係將二次光源的形狀限制在輪 帶狀及四極狀,進行變形照明(輪帶照明及四極照明),因 而複眼透鏡所形成之較大之二次光源射出的光束受到具有 輪帶狀及四極狀之孔徑部之孔徑光圈的限制。換言之,先 前技術之斡帶照明及四極照明時,自二次光源射出之光束 的相當部分被孔徑光圈遮蔽,而影響照明(曝光)。以致, 因孔徑光圈之光量損失,造成掩膜及晶圓上的亮度減低, 曝光裝置之通量亦減低的問題。此外,由於需要複製之圖 案也包含各種圖案形狀,因而需要不減少焦點深度而能使 投影光學系統對特定圖案形狀提高解像力的照明技術。 發明概述 本發明之目的在進行變形照明,其係用於有效抑制光量 損失且確保指定的焦點深度,同時使投影光學系統對特定 圖案形狀提高解像力。 爲求達到上述目的,本發明一種態樣之照明光學裝置係 用於照明掩膜,並使用在投影曝光裝置上,經由投影光學 系統,將上述掩膜上之圖案圖像複製到基板上,且具有: 光源機構’其係用於供應曝光波長的光束;二次光源形成 機構,其係用於依據上述光源機構射出之光束,在與上述 投影光學%系統之瞳孔共輛的照明瞳孔内,形成對某準光轴 概略對稱性偏移的兩個面光源;及變焦光學系纟充,其係用 於連續改變上述兩個面光源距上述基準光軸的距離、上述 -5- 本紙張尺度適用中國國家標準(CNS) Α4規格(210X297公釐) " -----^ 4p7149 A7 B7 五、發明説明(3 ) 兩個面光源之各個大小及自上述基準光軸估計上述兩個面 光源之角度的方位角。 圖式之簡要説明 圖1爲概略顯示具備本發明第一種實施形態之照明光學裝 置的曝光裝置構造圖。 圖2爲概略顯示圖1之微複眼4的構造圖。 圖3爲兩_極照明用之繞射光學元件6之作用的説明圖。 裝 圖4爲兩極照明用之繞射光學元件6之作用的説明圖,同 時顯示形成在複眼透鏡8之射入面上的兩極狀照射區域。 圖5爲概略顯示數個孔徑光圈配置成圓周狀之轉台的構造 圖。 圖6爲概略顯示自微複眼4至複眼透鏡8之射入面的構造 圖。且爲説明連續變焦透鏡(Afocal Zoom Lens ) 5之倍率及 變焦透鏡(Zoom Lens ) 7之焦點距離,與形成在複眼透鏡8 之射入面上之兩極狀照射區域大小及形狀的關係圖。 圖7爲概略顯示具備本發明第二種實施形態之照明光學裝 置之曝光裝置的構造圖。 m 圖8爲概略顯示第一種實施形態及第二種實施形態之類似 例的重要部分構造圖。 圖9爲獲得微型裝置之半導體裝置之方式的流程圖。 較佳之具體實施例詳述 本發明之典型實施形態,係在光源機構與光學積分器之 間的光程中配置有角度光束形成機構及照射區域形成機 構。具體而言,角度光束形成機構包含:散射光束形成元 -6- 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐) A7 —____ B7 五、發明説明(4 ) 件’其係用於將光源機構射出之概略平行的光束轉換成對 基準光軸以各種角度散射的光束;及連續變焦透鏡等光學 系統’其係將微複眼所形成之散射光束予以聚光,並導入 後述之光束轉換元件之繞射光學元件的繞射面上。因此, 自光源機構射出之概略平行的光束通過微複眼及連續變焦 透鏡後變成對基準光軸具有各種角度成分的光束,射入繞 射光學元件内。 另外’照射區域形成機構包含繞射光學元件的光束轉換 元件’其係用於將射入光束轉換成對基準光軸偏移的數個 (兩個)光束;及變焦透鏡的光學系統,其係依據繞射光學 元件所形成的數個(兩個)光束,在複眼透鏡之光學積分器 的射入面上形成對基準光軸偏移的數個照射區域。此處所 謂對基準光軸偏移的數個(兩個)照射區域,係指對基準光 轴概略對稱性偏移的兩個照射區域,亦即兩極狀照射區域 等。 如此,藉由微複眼及連續變焦透鏡構成的角度光束形成 機構,及由繞射光學元件及變焦透鏡構成之照射區域形成 機構的作用’在複眼透鏡的射入面上形成有兩極狀的照射 區域。因而在複眼透鏡的後端焦點面上形成有同樣兩極狀 的二次光源。此種由複眼透鏡所形成之二次光源射出的光 束被具有因應二次光源之大小及形狀之孔徑部的孔徑光圈 限制後,,重疊照明被照射面的掩膜。 如此,本發明可依據光源機構射出的光束,幾乎無光量 損失的形成兩極狀的二次光源。因而可有效抑制限制二次 -7- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 497149 A7 B7 五、發明説明(5 ) 光源射出之光束之孔徑光圈的光量損失,且確保指定的焦 點深度,同時使投影光學系統對特定圖案形狀提高解像力 來進行變形照明。亦即,依據兩極狀之二次光源的兩極照 明主要可對沿著一個方向的圖案形狀提高投影光學系統的 解像力。另外,當然亦可藉由使微複眼離開照明光程,有 效抑制光量損失來進行一般圓形照明。 此外,本發明之實施形態藉由使連續變焦透鏡的倍率改 變,可同時改變二次光源之外徑及輪帶比。再者,藉由使 變焦透鏡的焦點距離改變,可以不改變二次光源的輪帶比 而改變其外徑。因而,藉由適切改變連續變焦透鏡的倍率 與變焦透鏡的焦點距離,可使二次光源的外徑不改變而僅 改變其輪帶比。 如上所述,本發明之實施形態的照明光學裝置可有效抑 制限制二次光源之孔徑光圈的光量損失,來進行兩極照明 等之變形照明及一般圓形照明。此外,藉由使連續變焦透 鏡之倍率改變及使變焦透鏡之焦點距離改變的簡單操作, 可有效抑制孔徑光圈上的光量損失,同時使變形照明的參 數(受到限制之二次光源的大小及形狀)改變。 因此,安裝本發明實施形態之照明光學裝置的曝光裝置 可使變形照明的種類及參數適切改變,以獲得適於需要曝 光投影之微細圖案之投影光學系統的解像度及焦點深度。 因此可藉’由高度之曝光亮度及良好之曝光條件進行通量高 的良好投影曝光。此外,使用本發明實施形態之照明光學 裝置,將配置在被照射面上之掩膜的圖案曝光在感光性基 -8- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)4 ^ 7149 A7 _ B7 V. Description of the Invention (1) Field of the Invention The present invention relates to an illumination optical device and an exposure device provided with the same, and particularly to a semiconductor device, a photographic device, and a liquid crystal display suitable for manufacturing a lithographic step. Illumination optics for exposure devices such as devices or thin-film magnetic heads. Relevant prior art This type of typical exposure device is a light beam emitted from a light source into a fly-eye lens, and a secondary light source containing many light source images is formed on the focal plane at the rear end. The light beam emitted by the secondary light source is restricted by the aperture stop near the focal surface at the rear end of the fly-eye lens, and then enters the condenser. The aperture diaphragm limits the shape or size of the secondary light source to the required shape or size according to the required lighting conditions (exposure conditions). The light beam condensed by the condenser lens is superimposed and illuminated with a mask having a specified pattern. The light that penetrates the mask pattern is imaged on the wafer via a projection optical system. As such, the mask pattern is projected and exposed (replicated) on the wafer. In addition, the pattern formed on the mask is overprinted. When the fine pattern is correctly copied on the wafer, it is indispensable to obtain a uniform illumination distribution on the wafer. m In recent years, by changing the size of the aperture portion (light transmitting portion) of the aperture stop disposed at the exit end of the fly-eye lens, the size of the secondary light source formed by the fly-eye lens has been changed, and the correlation of illumination β ( J 値 = aperture aperture / pupil aperture of the projection optical system, or 0 * 値 = number of apertures at the exit end of the illumination optical system / throw, apertures at the entrance end of the shadow optical system) has attracted attention. In addition, by setting the shape of the aperture portion of the aperture stop at the exit end of the fly-eye lens into a belt shape and a four-hole shape (that is, a quadrupole shape), the compound eye -4- This paper size applies the Chinese National Standard (CNS) A4 size (210 X 297 mm) 4β7149 Α7 ______— Β7 V. Description of the invention (2) The shape of the lens formed by the secondary light source is limited to the belt shape and quadrupole shape, which improves the focal depth and resolution of the projection optical system Technology has attracted attention. As described above, in the prior art, because the shape of the secondary light source is limited to the shape of the belt and the quadrupole, and the deformation lighting (belt lighting and quadrupole lighting) is performed, the light beam emitted by the larger secondary light source formed by the fly-eye lens It is limited by the aperture stop with a ring-shaped and quadrupole-shaped aperture. In other words, in the ribbon illumination and quadrupole illumination of the prior art, a considerable portion of the light beam emitted from the secondary light source is blocked by the aperture diaphragm, which affects the illumination (exposure). Therefore, due to the loss of the light amount of the aperture diaphragm, the brightness on the mask and the wafer is reduced, and the throughput of the exposure device is also reduced. In addition, since the patterns to be reproduced also include various pattern shapes, there is a need for an illumination technology that enables the projection optical system to improve the resolution of a specific pattern shape without reducing the depth of focus. SUMMARY OF THE INVENTION The object of the present invention is to perform anamorphic lighting, which is used to effectively suppress the loss of light quantity and ensure a specified depth of focus, while making the projection optical system improve the resolution of a specific pattern shape. In order to achieve the above object, an aspect of the present invention is an illumination optical device for illuminating a mask, which is used on a projection exposure device, and the pattern image on the mask is copied to a substrate through a projection optical system, and The light source mechanism is used to supply a light beam with an exposure wavelength; the secondary light source forming mechanism is used to form a light beam emitted from the light source mechanism in the illumination pupil shared with the pupil of the projection optical% system. Two surface light sources that are roughly symmetrically offset from a quasi-optical axis; and a zoom optical system, which is used to continuously change the distance between the two surface light sources from the reference optical axis, and the above -5- paper size applies China National Standard (CNS) A4 specification (210X297 mm) " ----- ^ 4p7149 A7 B7 V. Description of the invention (3) Each size of the two surface light sources and the above two surface light sources are estimated from the above reference optical axis The azimuth of the angle. Brief Description of the Drawings Fig. 1 is a schematic view showing a structure of an exposure apparatus provided with an illumination optical apparatus according to a first embodiment of the present invention. FIG. 2 is a structural view schematically showing the micro compound eye 4 of FIG. 1. FIG. 3 is an explanatory diagram of the action of the diffractive optical element 6 for bipolar illumination. FIG. 4 is an explanatory view of the action of the diffractive optical element 6 for bipolar illumination, and also shows a bipolar irradiation area formed on the incident surface of the fly-eye lens 8. FIG. Fig. 5 is a schematic view showing a structure of a turntable in which a plurality of aperture diaphragms are arranged in a circle. FIG. 6 is a diagram schematically showing the structure of the entrance surfaces from the micro fly's eye 4 to the fly's eye lens 8. FIG. It is a diagram illustrating the relationship between the magnification of the continuous zoom lens (Afocal Zoom Lens) 5 and the focal distance of the zoom lens (Zoom Lens) 7 and the size and shape of the polarized irradiation area formed on the entrance surface of the fly-eye lens 8. Fig. 7 is a structural diagram schematically showing an exposure apparatus provided with an illumination optical apparatus according to a second embodiment of the present invention. m Fig. 8 is a structural diagram of an important part schematically showing a similar example of the first embodiment and the second embodiment. FIG. 9 is a flowchart of a method of obtaining a semiconductor device of a micro device. The preferred embodiment is described in detail. A typical embodiment of the present invention is an angular beam forming mechanism and an irradiation area forming mechanism arranged in the optical path between the light source mechanism and the optical integrator. Specifically, the angular beam forming mechanism includes: a scattered beam forming element-6- This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) A7 —____ B7 V. Description of the invention (4) pieces Converting the roughly parallel light beams emitted by the light source mechanism into light beams that scatter the reference optical axis at various angles; and optical systems such as continuous zoom lenses that converge the scattered light beams formed by the micro compound eyes and introduce them into later-described light beams The diffractive surface of the diffractive optical element of the conversion element. Therefore, the roughly parallel light beams emitted from the light source mechanism pass through the micro compound eye and the continuous zoom lens, and become light beams having various angular components with respect to the reference optical axis, and enter the diffractive optical element. In addition, the 'irradiation region forming mechanism includes a beam conversion element including a diffractive optical element', which is used to convert an incident beam into a plurality of (two) beams which are offset from a reference optical axis; According to several (two) light beams formed by the diffractive optical element, a plurality of irradiation areas offset from the reference optical axis are formed on the incident surface of the optical integrator of the fly-eye lens. The several (two) irradiated areas offset from the reference optical axis here refer to two irradiated areas that are roughly symmetrically offset from the reference optical axis, that is, polarized irradiated areas. In this way, the role of an angular beam forming mechanism composed of a micro fly eye and a continuous zoom lens, and an irradiation area forming mechanism composed of a diffractive optical element and a zoom lens, forms a bipolar irradiation area on the incident surface of the fly eye lens . Therefore, a secondary light source having the same bipolar shape is formed on the rear focal surface of the fly-eye lens. After the light beam emitted from such a secondary light source formed by the fly-eye lens is restricted by the aperture stop having an aperture portion corresponding to the size and shape of the secondary light source, a mask that illuminates the illuminated surface is superimposed. In this way, the present invention can form a bipolar secondary light source based on the light beam emitted from the light source mechanism with almost no loss of light quantity. Therefore, it can effectively restrain the limitation of the secondary -7. This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 497149 A7 B7 V. Description of the invention (5) The amount of light in the aperture of the light beam emitted by the light source is lost. And ensure the specified depth of focus, while enabling the projection optical system to improve the resolution of the specific pattern shape for deformation lighting. That is, the bipolar illumination based on the bipolar secondary light source mainly improves the resolution of the projection optical system for the pattern shape along one direction. In addition, of course, it is also possible to perform general circular lighting by keeping the micro compound eyes away from the illumination optical path and effectively suppressing the loss of light amount. In addition, according to the embodiment of the present invention, by changing the magnification of the continuous zoom lens, the outer diameter and the belt ratio of the secondary light source can be changed at the same time. Furthermore, by changing the focal length of the zoom lens, the outer diameter of the secondary light source can be changed without changing the wheel ratio of the secondary light source. Therefore, by appropriately changing the magnification of the continuous zoom lens and the focal distance of the zoom lens, the outer diameter of the secondary light source can be changed without changing its wheel ratio. As described above, the illumination optical device according to the embodiment of the present invention can effectively suppress the loss of the amount of light in the aperture stop of the secondary light source, and perform deformation illumination such as bipolar illumination and general circular illumination. In addition, with the simple operation of changing the magnification of the continuous zoom lens and changing the focal distance of the zoom lens, it is possible to effectively suppress the loss of light amount on the aperture stop, and at the same time, the parameters of the deformed illumination (the size and shape of the restricted secondary light source) )change. Therefore, the exposure device installed with the illumination optical device according to the embodiment of the present invention can appropriately change the type and parameters of the deformed illumination to obtain the resolution and focus depth of the projection optical system suitable for the fine pattern requiring exposure projection. Therefore, a good projection exposure with a high flux can be performed by using a high exposure brightness and good exposure conditions. In addition, using the illumination optical device according to the embodiment of the present invention, the pattern of the mask disposed on the illuminated surface is exposed on a photosensitive base. 8- This paper is in accordance with the Chinese National Standard (CNS) A4 specification (210 X 297 mm). )

裝 訂Binding

板上的曝光方法,由於可藉由良好的曝光條件進行投影 光,因此可製造良好的裝置。 ~、 以下參照附圖説明本發明的實施形態: 圖1爲概略顯7F具備本發明第一種實施形態之照明光學裝 置之曝光裝置的構造圖。圖丨中,分別將沿著感光性基板 I晶圓W的法線方向設定爲z軸,將晶圓面内之平行於圖i 紙面的方向設定爲γ軸,將晶圓面内,垂直於圖i紙面的方 向設定爲X軸。另外,圖i中的照明光學裝置設定成進行兩 極照明。 圖1的曝光裝置具備用於供應曝光光線(照明光線)的光源 1 ’如爲供應248 nm或193 nm波長光線的準分子雷射光源。 自光源1沿著Z方向射出之概略平行的光束具有沿著X方向 細長延伸的矩形剖面,射入由一對柱面透鏡2 a及2 b構成的 光束擴散器2。各柱面透鏡2a及2b在圖1紙面内(γζ平面内) 具有負折射力及正折射力,在包含光軸Αχ之與紙面垂直的 面内(XZ平面内)分別發揮平行平面板功能。因此,射入光 束擴散器2的光束在圖1的紙面内被擴大,被整形成具有指 定矩形剖面的光束。 通過整形光學系統之光束擴散器2之概略平行的光束被折 射鏡3向Y方向偏轉後,射入微複眼*内。如圖1及圖2所 不’微複眼4爲由緊密且縱橫排列之許多正六角形之具有 正折射力、的微小透鏡4 a構成的光學元件。通常,微複眼係 藉由在平行平面玻璃板上實施蝕刻處理,形成微小透鏡群 來構成。 -9-本紙張尺及·中國國家標準(CNS) A4規格(2iGχ撕公爱) 497149 A7 B7 五、發明説明(7 ) 此處’構成微複眼的各個微小透鏡比構成複眼透鏡之各 透鏡單元更微小。此外,微複眼與由相互隔離之透鏡單元 構成的複眼透鏡不同,許多微小透鏡係一體形成,並未相 互隔離。但是’微複眼與複眼透鏡相同之處在於具有正折 射力的透鏡要素採縱橫配置。另外,圖1及圖2中,爲求簡 化圖式,所設定之構成微複眼4之微小透鏡4 a的數量遠少 於實修數量。 因此,射入微複眼4的光束被許多微小透鏡二維分割,在 各微小透鏡的後端焦點面上分別形成一個光源(聚光點)。 形成在微複眼4後端焦點面上之許多光源射出的光束分別 形成具有正六角形狀剖面的散射光束,並射入連續變焦透 轉5。如此,微複眼4爲具有配置成平面狀(二維狀)之數個 單位光學元件(微小透鏡)的光學元件陣列,並構成散射光 束形成元件,將自光源1射出之概略平行的光束轉換成對 光軸AX以各種角度散射的光束。 另外,微複眼4對照明光程採可任意拆裝的構造。此外, 連續變焦透鏡5係採維持無焦點光學系統(Afocal系統),同 時,使倍率可在指定範圍連續改變的構造。此處,自微複 眼4的照明光程離開,係由依據控制系統2 1之指令操作的 第一驅動系統2 2來執行。此外,連續變焦透鏡5的倍率改 變則係由依據控制系統2 1之指令操作的第二驅動系統2 3來 執行。, 穿透連續變焦透鏡5的光束,射入兩^墨明用的繞射光學 元件(DOE ) 6。此時,自形成在微複眼4後端焦點面上之各 -10 - ^張尺度適用中國國家標準(CNS) A"^(21GX297涵 497149The exposure method on the board can produce a good device because it can project light under good exposure conditions. Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings: Fig. 1 is a schematic view showing a structure of an exposure device equipped with the illumination optical device of the first embodiment of the present invention in 7F. In the figure, the normal direction along the wafer W of the photosensitive substrate I is set as the z axis, and the direction in the wafer plane parallel to the paper plane in FIG. I is set as the γ axis. The wafer plane is perpendicular to The direction of the paper surface in figure i is set to the X axis. The illumination optical device in Fig. I is set to perform bipolar illumination. The exposure apparatus of FIG. 1 is provided with a light source 1 ′ for supplying exposure light (illumination light), such as an excimer laser light source for supplying light with a wavelength of 248 nm or 193 nm. A substantially parallel light beam emitted from the light source 1 in the Z direction has a rectangular cross section elongated along the X direction, and enters a beam diffuser 2 composed of a pair of cylindrical lenses 2 a and 2 b. Each of the cylindrical lenses 2a and 2b has a negative refractive power and a positive refractive power in the paper plane (in the γζ plane) in FIG. 1, and functions as parallel plane plates in planes (in the XZ plane) perpendicular to the paper plane including the optical axis Ax. Therefore, the light beam entering the light beam diffuser 2 is enlarged within the paper surface of Fig. 1 and is shaped into a light beam having a prescribed rectangular cross section. The roughly parallel light beams passing through the beam diffuser 2 of the shaping optical system are deflected in the Y direction by the refracting mirror 3 and then enter the micro compound eyes *. As shown in Figs. 1 and 2, the micro compound eye 4 is an optical element composed of a plurality of regular hexagonal micro lenses 4a having positive refractive power and arranged in a vertical and horizontal direction. Generally, a micro compound eye is formed by performing an etching process on a parallel plane glass plate to form a micro lens group. -9-The paper ruler and Chinese National Standard (CNS) A4 specification (2iGχ tear public love) 497149 A7 B7 V. Description of the invention (7) Here, 'the micro lenses constituting the micro compound eye are more than the lens units constituting the compound eye lens Even smaller. In addition, unlike the fly-eye lens, which is composed of lens units that are isolated from each other, many micro-lenses are integrally formed and are not isolated from each other. However, the 'micro-eye' is similar to the fly-eye lens in that the lens elements having a positive refractive power are arranged vertically and horizontally. In addition, in FIG. 1 and FIG. 2, for the sake of simplicity, the number of the micro lenses 4 a constituting the micro compound eye 4 is set to be much smaller than the number of actual repairs. Therefore, the light beam entering the micro compound eye 4 is two-dimensionally divided by a plurality of microlenses, and a light source (condensing point) is formed on the rear focal surface of each microlens. The light beams emitted from a plurality of light sources formed on the focal surface at the rear end of the micro compound eye 4 respectively form scattered light beams having a regular hexagonal cross-section, and enter the continuous zoom lens 5. In this way, the micro compound eye 4 is an optical element array having a plurality of unit optical elements (microlenses) arranged in a planar shape (two-dimensional shape), and constitutes a scattered beam forming element, and converts a roughly parallel light beam emitted from the light source 1 into Light beams scattered at various angles with respect to the optical axis AX. In addition, the micro-complex eye 4 can be arbitrarily disassembled and assembled. In addition, the continuous zoom lens 5 has a structure that maintains a focus-free optical system (Afocal system) and allows the magnification to be continuously changed within a specified range. Here, the light path length of the illumination from the micro-eye 4 is executed by the first driving system 22 which operates according to the instruction of the control system 21. In addition, the magnification change of the continuous zoom lens 5 is performed by the second driving system 23, which operates in accordance with a command of the control system 21. The light beam that has passed through the continuous zoom lens 5 is incident on two diffractive optical elements (DOE) 6 for Mo Ming. At this time, each of the -10-^ scales formed on the focal plane at the rear end of the micro compound eye 4 applies the Chinese National Standard (CNS) A " ^ (21GX297 涵 497149

光原射出的散射光束保持正六角形狀的剖面,4 妓 光學,,的繞射面上。亦即,連續變焦透鏡5二^^ 彳交崎焦點面與繞射光學元件6之繞射面予以光學性共軛 連結。因而聚光在繞射光學元件6之繞射面上一點的光束 孔I數k連續變焦透鏡5的倍率而改變。 通常,繞射光學元件的構造係在玻璃基板上形成具有概 略曝光光線(照明光線)之波長間距的階差,具有將射入光 束繞射成所需角度的作用。具體而言,兩極照明用的繞射 光學疋件6如圖3(a)所示,將平行於光軸人乂之垂直射入的 細光束轉換成依據指定之射出角行進的兩個光束。換言 之,沿著光軸ΑΧ垂直射入之細光束以光軸Αχ爲中心的等 角度,沿奢特定的兩個方向繞射,形成兩個細光束。進一 步詳述’垂直射入繞射光學元件6的細光束轉換成兩個光 束’將通過平行於繞射光學元件6之後面之兩個光束之通 過中心點連線部分的中心,位於繞射光學元件6的射入軸 線上。如此,繞射光學元件6構成光束轉換元件,用於將 射入光束轉換成兩個光束。 因此,如圖3 (b)所示,粗的平行光束對繞射光學元件6 垂直射入時,配置於繞射光學元件6後方之透鏡3 1的焦點 位置上也形成有兩個點像(點狀的光源像)3 2。亦即,繞射 光學元件6在遠場(或夫朗和費繞射區域)上形成兩點狀的光 強度分布、。此外,透鏡3 1則將形成在遠場(或夫朗和費繞 射區域)上的兩點狀光強度分布形成在其後端焦點面上。 此時,如圖3 ( c )所示,將射入繞射光學元件6之粗平行光 -11 - 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公I)The scattered light beam emitted by the light source maintains a regular hexagonal cross section, 4 prosthetics, and a diffraction surface. That is, the focal plane of the continuous zoom lens 52 and the diffraction plane of the diffractive optical element 6 are optically conjugated. Therefore, the magnification of the continuous zoom lens 5 is changed by condensing the light beam aperture I at a point on the diffraction surface of the diffractive optical element 6. Generally, the structure of a diffractive optical element is formed on a glass substrate with a step having a wavelength interval of approximately exposure light (illumination light), and has a function of diffracting an incident light beam into a desired angle. Specifically, as shown in FIG. 3 (a), a diffraction optical element 6 for bipolar illumination converts a thin light beam that is perpendicularly incident to a human axis parallel to the optical axis into two light beams that travel at a specified exit angle. In other words, the thin light beams that are perpendicularly incident along the optical axis AX are diffracted in two specific directions at equal angles with the optical axis AX as the center to form two thin beams. Further details, 'the thin beam perpendicularly incident on the diffractive optical element 6 is converted into two beams' will pass through the center of the line connecting the two points of the two beams parallel to the rear surface of the diffractive optical element 6, which is located in the diffractive optical The injection axis of the element 6. In this way, the diffractive optical element 6 constitutes a light beam conversion element for converting the incident light beam into two light beams. Therefore, as shown in FIG. 3 (b), when a thick parallel light beam is incident perpendicularly to the diffractive optical element 6, two point images are also formed at the focal position of the lens 31 disposed behind the diffractive optical element 6. Point-like light source image) 3 2. That is, the diffractive optical element 6 forms a two-point light intensity distribution in the far field (or the Fraunhofer diffraction region). In addition, the lens 31 forms a two-point light intensity distribution formed on the far field (or the Fraunhofer diffraction region) on the rear focal plane. At this time, as shown in FIG. 3 (c), the coarse parallel light that is incident on the diffractive optical element 6 -11-This paper size applies to the Chinese National Standard (CNS) A4 specification (210X 297 male I)

装 m 497149 A7 B7 五、發明説明(9 ) 束對光抽A X傾斜時,形成在透知^ 1之焦點位置上的兩個 圖像移動。亦即,射入繞射光學元件6之粗平行光束沿著 指定面傾斜時,形成在透鏡3 1之焦點位置上的兩個點像3 3 不改變其大小,其中心沿著指定面向傾向光束之另一端移 動。 如上所述’自形成在微複眼4之後焦點面之各光源射出 的散射光_束保持正六角形狀剖面的會聚在繞射光學元件6 的繞射面上。換言之,具有各種角度成分之光束雖射入繞 射光學元件6上,但是其射入角度受到正六角錐狀之光束 範圍的限制。因此,如圖4 ( a)所示,將垂直射入繞射光學 元件6之光束形成之兩點狀圖像4 0爲中心,以對應於正六 角錐狀之光束範圍之各稜線之最大角度射入的光束,將兩 點狀圖像4 1〜4 6形成在透鏡3 1的焦點位置。實際上,由於 具有被正六角錐狀之光束範圍限制之許多角度成分的無限 數量光束射入繞射光學元件6内,因此,無限數量之兩點 狀圖像在透鏡31的焦點位置上重疊,整體形成如圖4(b)所 不的兩極狀照射區域0 另外,繞射光學元件6對照明光程採可任意拆裝的構造, 且採可轉換成八極照明用之繞射光學元件6〇、變形四極照 明用之繞射光學元件6 1及一般圓形照明用之繞射光學元件 6 2的構造。有關八極照明用之繞射光學元件6 〇、變形四極 照明用之、繞射光學元件6 1及一般圓形照明用之繞射光學元 件6 2的構造及作用如後述。此處’兩極照明用之繞射光取 元件6、八極照明用之繞射光學元件60、變形四極照明: -12 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 497149 A7 --------Β7 五、發明説明(1〇 ) I'繞射光學το件6 1與一般圓形照明用之繞射光學元件6 2間 的轉換’係由依據控制系統2丨之指令操作的第三驅動系統 2 4來執行。 再度參…、圖1 ’牙透繞射光學元件6的光束射入變焦透鏡 7。此時t變焦透鏡7具有與圖3所示之透鏡”相同的作 用此外’作爲光學積分器之複眼透鏡8之射入面被固定 在夂二透韓7之後端焦點面的附近。因此,穿透繞射光學 π件6的光束在變焦透鏡7之後端焦點面上與複眼透鏡8的 射入面上,形成對圖4 ( b )所示之光軸Α χ對稱性偏移的兩 個照射區域’亦即兩極狀照射區域。該兩極狀照射區域的 大小(兩極狀照射區域之外接圓的直徑)隨變焦透鏡7的焦點 距離而改變。如此,變焦透鏡7之繞射光學元件ό與複眼透 鏡8之射入面連結成實質上之傅里葉轉換的關係。另外, 變焦透鏡7之焦點距離的改變係由依據控制系統〕〗之指令 操作的第四驅動系統2 5來執行。 複眼透鏡8將具有正折射力之許多透鏡單元採緊密且縱橫 排列來構成。另外,構成複眼透鏡8的各透鏡單元具有與 需要在掩膜上形成之照射區域形狀(或是需要在晶圓上形成 之曝光區域的形狀)類似的矩形剖面。此外,構成複限透鏡 8之各透鏡單元的射入面形成向射入端凸起的球面狀,射 出面形成向射出端凸起的球面狀。 因此,射入複眼透鏡8之光束被許多透鏡單元二維分割, 在光束射入之各透鏡單元的後端焦點面上分別形成^光 源。如此,在複眼透鏡8之後端焦點面上形成有光強度分 -13-Installation m 497149 A7 B7 V. Description of the invention (9) When the beam is tilted to the light extraction A X, the two images formed at the focal position of the transparence ^ 1 move. That is, when a thick parallel light beam incident on the diffractive optical element 6 is inclined along a specified surface, the two point images 3 3 formed at the focal position of the lens 31 are not changed in size, and the center thereof is inclined along the specified plane. Move the other end. As described above, 'the scattered light beam emitted from each light source formed on the focal plane after the micro compound eye 4 converges on the diffraction surface of the diffractive optical element 6 while maintaining a regular hexagonal cross section. In other words, although a light beam having various angular components is incident on the diffractive optical element 6, the angle of incidence is limited by the range of the light beam having a regular hexagonal cone shape. Therefore, as shown in FIG. 4 (a), the two-point image 40 formed by the light beams that are perpendicularly incident on the diffractive optical element 6 is used as the center, and the maximum angle of each edge line corresponding to the regular hexagonal cone-shaped beam range is projected The incoming light beam forms two dot-like images 4 1 to 4 6 at the focal position of the lens 31. Actually, since an infinite number of light beams having many angular components limited by the beam range of a regular hexagonal cone is incident into the diffractive optical element 6, an infinite number of two-point images overlap at the focal position of the lens 31, and A bipolar irradiation area 0 as shown in Fig. 4 (b) is formed. In addition, the diffractive optical element 6 adopts a structure in which the illumination light path can be detached arbitrarily, and adopts a diffractive optical element 6 which can be converted into eight-pole illumination. Structures of the diffractive optical element 61 for anamorphic quadrupole illumination and the diffractive optical element 62 for general circular illumination. The structures and functions of the diffractive optical element 60 for octapole illumination, the diffractive optical element 61 for quaternary illumination, and the diffractive optical element 62 for general circular illumination are described later. Here 'diffractive light extraction element for bipolar illumination 6, diffractive optical element 60 for octapolar illumination, deformed quadrupole illumination: -12 This paper size applies to China National Standard (CNS) A4 (210X 297 mm) 497149 A7 -------- B7 V. Description of the invention (1〇) I 'Diffraction optics το 6 1 and the diffractive optical element 6 2 for general circular lighting conversion is based on the control system 2 丨The third driving system 24 executes the command operation. Once again ... Fig. 1 'The light beam of the diffracting optical element 6 enters the zoom lens 7. At this time, the t-zoom lens 7 has the same function as the lens shown in FIG. 3. In addition, the entrance surface of the fly-eye lens 8 as an optical integrator is fixed near the focal surface of the rear end of the second transparent lens 7. Therefore, wear The light beam passing through the diffractive optical π member 6 forms two irradiations on the focal plane at the rear end of the zoom lens 7 and the entrance plane of the fly-eye lens 8 to the optical axis A χ as shown in FIG. 4 (b). The 'area' is a polarized irradiation area. The size of the polarized irradiation area (the diameter of the circle outside the polarized irradiation area) changes with the focal distance of the zoom lens 7. Thus, the diffractive optical element of the zoom lens 7 and the compound eye The incident surfaces of the lens 8 are connected in a substantially Fourier transform relationship. In addition, the change in the focal distance of the zoom lens 7 is performed by a fourth driving system 25 that operates according to a command of the control system]. Fly-eye lens 8 A plurality of lens units having a positive refractive power are arranged closely and arranged vertically and horizontally. In addition, each lens unit constituting the fly-eye lens 8 has a shape corresponding to an irradiation area to be formed on a mask (or needs to be formed on a wafer). The shape of the exposed area formed) is similar to a rectangular cross section. In addition, the entrance surface of each lens unit constituting the complex lens 8 is formed into a spherical shape convex toward the entrance end, and the exit surface is formed into a spherical shape convex toward the exit end. Therefore, the light beam incident on the fly-eye lens 8 is two-dimensionally divided by many lens units, and a light source is formed on the rear focal plane of each lens unit where the light beam is incident. In this way, light is formed on the rear focal plane of the fly-eye lens 8. Intensity points

497149 A7 _ B7 五、發明説明(11 ) 布與射入複眼透鏡8之光束所形成之照射區域相同的兩極 狀面光源(以下稱「二次光源」)。自形成在複眼透鏡8之後 端焦點面上之兩極狀二次光源射出的光束,射入配置在其 附近的孔徑光圈9。該孔徑光圈9被支撑在可沿平行於光軸 AX之指定軸線四周旋轉的轉台(旋轉板:圖1上未顯示) 上。 圖5爲I略顯示數個孔徑光圈配置成圓周狀之轉台的構造 圖。如圖5所示,轉台基板400上,具有圖上斜線所示之透 光£域的八個孔徑光圈沿著圓周方向設置。轉台基板4〇〇 的構造採可通過其中心點〇,平行於光軸Αχ的軸線四周旋 轉。因此’藉由使轉台基板4 0 〇旋轉,可將從八個孔徑光 圈中選出的一個孔徑光圈固定在照明光程中。另外,轉台 基板400的旋轉係由依據控制系統2 1之指令操作的第五驅 動系統2 6來執行。 在轉台基板400上形成有輪帶比不同之三個兩極孔徑光圈 401,403及405。此處之兩極孔徑光圈4〇1在具有r11/r21 之輪帶比的輪帶狀區域内具有對其中心對稱性配置的兩個 圓形穿透區域。兩極孔徑光圈403在具有γ12/γ22之輪帶比 的輪帶狀區域内具有對其中心對稱性配置的兩個圓形穿透 區域。兩極孔徑光圈405在具有rl3/r21之輪帶比的輪帶狀 區域内具有對其中心對稱性配置的兩個圓形穿透區域。 此外,轉台基板400上形成有輪帶比不同之三個八極孔徑 光圈 402,404 及 406。 再者,於轉台基板4〇〇上形成有大小(孔徑)不同之兩個圓 -14-497149 A7 _ B7 V. Description of the invention (11) The polar surface light source (hereinafter referred to as "secondary light source") having the same polarized area as the irradiation area formed by the light beam incident on the fly-eye lens 8 is used. A light beam emitted from a bipolar secondary light source formed on the focal end surface behind the fly-eye lens 8 enters an aperture stop 9 disposed in the vicinity thereof. The aperture diaphragm 9 is supported on a turntable (rotating plate: not shown in Fig. 1) that can rotate around a specified axis parallel to the optical axis AX. FIG. 5 is a schematic view showing a structure of a turntable in which a plurality of aperture diaphragms are arranged in a circle. As shown in FIG. 5, on the turntable substrate 400, eight aperture apertures having a light transmission range shown by diagonal lines in the figure are provided along the circumferential direction. The structure of the turntable substrate 400 can rotate around its axis parallel to the optical axis Ax through its center point 0. Therefore, by rotating the turntable substrate 400, one aperture stop selected from the eight aperture stops can be fixed in the illumination path. In addition, the rotation of the turntable substrate 400 is performed by a fifth drive system 26 which operates in accordance with a command of the control system 21. On the turntable substrate 400, three bipolar aperture diaphragms 401, 403, and 405 having different wheel ratios are formed. The bipolar aperture stop 401 here has two circular penetration regions symmetrically arranged at its center in a belt-shaped region having a belt-ratio of r11 / r21. The bipolar aperture diaphragm 403 has two circular penetration regions arranged symmetrically to its center in a wheel-belt region having a wheel-belt ratio of γ12 / γ22. The bipolar aperture diaphragm 405 has two circular penetration regions arranged symmetrically to its center in a belt-like region having a belt-ratio of rl3 / r21. In addition, three octopole apertures 402, 404, and 406 having different wheel ratios are formed on the turntable substrate 400. Furthermore, two circles having different sizes (apertures) are formed on the turntable substrate 400. -14-

A7 ______ B7 五、發明説明(U ^ --- 形孔徑光圈407及408。此處之圓形孔徑光圈4〇7具有2^ ,小的圓形穿透區域,圓形孔徑光圈4〇8具有Μ丄大小的 圓形穿透區域。 此外,在轉台基板400上形成有輪帶比不同之三個便行四 極孔後光圈409〜411,因受紙面限制,其構成另行圖示。 因此,藉由從三個輪帶孔徑光圈4〇1,4〇3及4〇5中選擇 個雨極孔;f二光圈,固足在照明光程内,可正確限制(規定) 具有一個不同輪帶比之兩極狀的光束,進行輪帶比不同之 三種兩極照明。 再者’藉由從兩個圓形孔徑光圈4〇7及4〇8中選擇一個圓 形孔徑光圈,固定在照明光程内,可進行σ値不同的兩種 一般圓形照明。 圖1中’由於在複眼透鏡8之後端焦點面上形成有兩極狀 的一次光源’因此’係使用自三個兩極孔徑光圈1,403 及405中選出之一個兩極孔徑光圈9。但是,圖5所示之轉 台的構造僅爲範例,所配置之孔徑光圈的種類及數量並不 受限制。此外’並不限定於轉台方式的孔徑光圈,亦可在 照明光程内固定安裝可適切變更透光區域大小及形狀的孔 徨光圈。再者,亦可設置彩虹光圈,使圓形孔徑連續改 變’來取代兩個圓形孔徑光圈407及408。 穿透具有兩極狀孔徑部(透光部)之孔徑光圈9之二次光源 射出的光、線接受導光光學系統之聚光光學系統1 0的聚光作 用後,重疊性的均勻照明形成有指定圖案的掩膜Μ。穿透 掩膜Μ圖案的光束通過投影光學系統PL,在感光性基板之 -15- 本紙張尺度適用中國國家標準…^^) Α4規格(210X297公釐) 497149A7 ______ B7 V. Description of the invention (U ^ --- shaped aperture diaphragms 407 and 408. Here the circular aperture diaphragm 407 has 2 ^, a small circular penetration area, and the circular aperture diaphragm 408 has A circular penetrating area of the size of 丄. In addition, three portable quadrupole apertures 409 to 411 with different wheel ratios are formed on the turntable substrate 400. Due to paper restrictions, the composition is shown separately. Therefore, borrow Choose a rain pole hole from the three wheel aperture apertures 40.1, 4.03, and 4.05; f two apertures, fixed in the light path, can be properly restricted (specified). Have a different wheel ratio The two pole-shaped beams are illuminated by three types of poles with different wheel-to-belt ratios. Furthermore, 'a circular aperture stop is selected from two circular aperture stops 407 and 408 and fixed in the illumination path. Two kinds of general circular illumination with different σ 値 can be performed. In Fig. 1, 'because a bipolar primary light source is formed on the focal surface behind the fly-eye lens 8', therefore, three bipolar apertures 1,403 and 405 are used. One of the two-pole aperture diaphragms 9 is selected. However, the structure of the turntable shown in FIG. 5 It is only an example, and the type and number of the aperture diaphragms are not limited. In addition, it is not limited to the aperture diaphragm of the turntable method. It can also be fixed in the illumination path to change the size and shape of the light transmission area.徨 Aperture. In addition, a rainbow aperture can be set to continuously change the circular aperture 'to replace the two circular aperture apertures 407 and 408. It penetrates the aperture aperture 9 having a bipolar aperture portion (light transmitting portion) twice After the light and line emitted from the light source receive the light-concentrating effect of the light-concentrating optical system 10 of the light-guiding optical system, the overlapping uniform illumination forms a mask M of a specified pattern. The light beam penetrating the pattern of the mask M passes through the projection optical system. PL, -15 on the photosensitive substrate. This paper size applies Chinese national standards ... ^^) Α4 size (210X297 mm) 497149

晶圓w上形成掩膜圖案的圖I。如此,在與投影光學系統 PL〈光抽ΑΧ垂直的平面(χγ平面)内,藉由平面驅動控制 曰3圓W並進行統一曝光或掃描曝光,掩膜Μ的圖案逐次被 曝光在晶圓W的各曝光區域上。 另外,統一曝光時,係依據所謂之步進及反覆方式,對 晶圓的各曝光區域統一曝光掩膜圖案。此時,掩膜Μ上之 照射區域_的形狀爲接近正方形的矩形,複眼透鏡8之各透 鏡單元的剖面形狀亦爲接近正方形的矩形。另外,於掃描 曝光時,係依據所謂之步進及掃瞄方式,使掩膜及晶圓對 投影光學系統相對移動,並對晶圓之各曝光區域掃描曝光 掩膜圖案。此時’掩膜Μ上之照射區域的形狀爲短邊與長 邊比例爲1 : 3的矩形,而複眼透鏡8之各透鏡單元的剖面 形狀亦爲與其類似的短形。 圖ό爲概略顯示自微複眼4至複眼透鏡8之射入面的構造 圖,説明連續變焦透鏡5之倍率及變焦透鏡7之焦點距離, 與形成在複眼透鏡8之射入面上之兩極狀照射區域大小及 形狀的關係圖。圖6中在配置於微複眼4之光軸ΑΧ上之微 小透鏡中心,沿著光軸ΑΧ射入的光線70,沿著光軸ΑΧ被 射出。微複眼4的尺寸(對應於正六角行之外接圓之直徑的 尺寸)a由焦點距離爲f 1的微小透鏡構成。光線7 0穿透連續 變焦透鏡5後,沿著光軸A X射入繞射光學元件6。 繞射光學元件6依據沿著光軸AX垂直射入之光線70,形 成以對光軸A X成#角度射出的光線7 0 a。自繞射光學元件 6以角度Θ射出的光線7 0 a穿透焦點距離f 2之變焦透鏡7, -16- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 497149 A7 B7 五、發明説明(14 ) 到達複眼透鏡8的射入面。此時’複眼透鏡8之射入面上之 光線7 0 a的位置具有距光袖A X爲y的南度。另外,平行於 光軸AX射入配置在微複眼4之光軸AX上之微小透鏡最上 端的光線7 1,以對光軸A X成角度t射出。該光線7 1穿透倍 率爲m之連續變焦透鏡5後,以對光軸AX成角度t,射入繞 射光學元件6。 以對光#AX成角度t’射入繞射光學元件6的光線7 1,轉 換成包含以對光軸AX成角度(Θ + t’)射出之光線71a的各 種光線。以對光軸AX成角度(Θ + t’),自繞射光學元件6 射出之光線7 1 a穿透變焦透鏡7,在複眼透鏡8的射入面上 達到距光輛AX爲(y + b)的南度。再者,平行於光轴AX射 入配置於微複眼4之光軸A X上之微小透鏡之最下端的光線 72以對光軸AX成角度ί射出。該光線72穿透連續變焦透鏡 5後,以對光軸ΑΧ成角度t,射入繞射光學元件6。 以對光軸AX成角度t’射入繞射光學元件6的光線72,轉 換成包含以對光軸AX成角度(β -t’)射出之光線72a(圖上 未顯示)的各種光線。以對光軸A X成角度(θ -1 ’),自繞射 光學元件6射出之光線7 2 a穿透變焦透鏡7,在複眼透鏡8的 射入面上達到距光軸AX爲(y-b)的高度。 如此,自形成於微複眼4之後端焦點面附近之各光源射出 之散射光束到達複眼透鏡8之射入面的範圍,爲在圖4(b) 所示的兩、極狀照射區域中,以距光軸ΑΧ爲y高度作中心, 具有寬度2b的範圍。亦即,如圖6(b)所示,形成在複眼透 鏡8之射入面之兩極狀照射區域,與形成在複眼透鏡8之後 -17- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 497149 A7Figure I of a mask pattern is formed on the wafer w. In this way, in a plane (χγ plane) perpendicular to the projection optical system PL <optical pumping AX, by plane driving control of 3 circles W and performing unified exposure or scanning exposure, the pattern of the mask M is sequentially exposed on the wafer W On each exposed area. In addition, in the case of uniform exposure, the mask pattern is uniformly exposed on each exposure area of the wafer according to the so-called step and repeat method. At this time, the shape of the irradiation area _ on the mask M is a rectangle close to a square, and the cross-sectional shape of each lens unit of the fly-eye lens 8 is also a rectangle close to a square. In addition, during the scanning exposure, the mask and the wafer are moved relative to the projection optical system according to the so-called step and scan method, and the exposed mask patterns are scanned and exposed for each exposed area of the wafer. At this time, the shape of the irradiated area on the 'mask M is a rectangle with a short side to long side ratio of 1: 3, and the cross-sectional shape of each lens unit of the fly-eye lens 8 is similarly short. FIG. 6 is a structural diagram schematically showing the entrance surface of the fly-eye lens 4 to the fly-eye lens 8, illustrating the magnification of the continuous zoom lens 5 and the focal distance of the zoom lens 7, and the polar shape formed on the entrance surface of the fly-eye lens 8. The relationship between the size and shape of the irradiation area. In FIG. 6, at the center of the microlens disposed on the optical axis AX of the micro compound eye 4, the light rays 70 incident along the optical axis AX are emitted along the optical axis AX. The size of the micro compound eye 4 (the size corresponding to the diameter of the circle outside the regular hexagonal line) a is composed of a minute lens having a focal distance f 1. The light 70 passes through the continuous zoom lens 5 and enters the diffractive optical element 6 along the optical axis A X. The diffractive optical element 6 forms a light beam 7 0 a which is emitted at an angle of # with respect to the optical axis A X based on the light rays 70 incident perpendicularly along the optical axis AX. The light 7 emitted by the self-diffractive optical element 6 at an angle Θ 7 a a zoom lens 7 penetrating the focal distance f 2, -16- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 497149 A7 B7 V. Description of the invention (14) It reaches the entrance surface of the fly-eye lens 8. At this time, the position of the light ray 70a on the incident surface of the 'Flying Eye Lens 8 has a south degree from the optical sleeve AX to y. In addition, light rays 71, which enter the uppermost end of the microlenses arranged on the optical axis AX of the micro compound eye 4 in parallel to the optical axis AX, are emitted at an angle t to the optical axis AX. The light beam 71 passes through the continuous zoom lens 5 with a magnification of m and enters the diffractive optical element 6 at an angle t with respect to the optical axis AX. The light ray 71, which is incident on the diffractive optical element 6 at an angle t 'to the light #AX, is converted into various types of light including the light 71a which is emitted at an angle (Θ + t') to the optical axis AX. At an angle (Θ + t ') to the optical axis AX, the light 7 1 a emitted from the self-diffractive optical element 6 penetrates the zoom lens 7 and reaches the entrance plane of the fly-eye lens 8 from the optical axis AX as (y + b) South. In addition, the light rays 72 entering the lowermost end of the microlenses arranged on the optical axis A X of the micro compound eye 4 parallel to the optical axis AX are emitted at an angle to the optical axis AX. The light 72 passes through the continuous zoom lens 5 and enters the diffractive optical element 6 at an angle t with respect to the optical axis AX. The light rays 72 entering the diffractive optical element 6 at an angle t 'with respect to the optical axis AX are converted into various light rays including light rays 72a (not shown in the figure) emitted at an angle (β -t') with respect to the optical axis AX. At an angle (θ -1 ′) to the optical axis AX, the light 7 2 a emitted from the self-diffractive optical element 6 penetrates the zoom lens 7, and reaches the entrance surface of the fly-eye lens 8 from the optical axis AX as (yb) the height of. In this way, the range of the scattered light beams emitted from the light sources near the focal plane behind the micro-fly eye 4 to the entrance surface of the fly-eye lens 8 is in the two, polar irradiation areas shown in FIG. 4 (b). The distance from the optical axis AX is centered at a height of y and has a range of a width 2b. That is, as shown in FIG. 6 (b), the polarized irradiation area formed on the entrance surface of the fly-eye lens 8 and the rear area of the fly-eye lens 8 are formed. -17- This paper applies the Chinese National Standard (CNS) A4 specification ( 210X 297 mm) 497149 A7

五、發明説明(15 ) 端焦點面上之兩極狀的二次光源,具有距光軸A X之中心高 度y,且具有寬度2b。 此處,自微複眼4射出角度t及射入繞射光學元件6的角度 t ’,由下列公式(1 )及(2 )表示: t = a/ (2-fl) (1) t’=t/m = a/(2 - fl .m) ( 2 ) 此外,,極狀之二次光源的衷心高度y、最高高度(y + b) 及最低南度(y-b),由下列公式(3)〜(5)表示: y = f2 · sin θ ( 3 ) y + b = f2(sin β + sint,) (4) y — b = f2 ( sin &lt;9 - sint,) (5) 因此,被兩極狀之二次光源内徑0 i與外徑0 〇所限制之 輪帶比A由下列公式(6 )表示。此處,如圖6 (b )所示,内押 0i爲在内接於正六角形之面光源之一對圓(相當於孔後光 圈9之孔徑部)上内接之圓的直徑。此外,外徑0 〇爲外隹 於該一對圓之圓的直徑。 A = 0i/0〇 = 2(y — b)/(2(y + b)) 二(sin &lt;9 - sint 丨)/(sin θ + sint’)5. Description of the invention (15) The bipolar secondary light source on the focal end surface has a height y from the center of the optical axis A X and has a width 2b. Here, the exiting angle t of the self-micro compound eye 4 and the angle t ′ entering the diffractive optical element 6 are expressed by the following formulas (1) and (2): t = a / (2-fl) (1) t '= t / m = a / (2-fl .m) (2) In addition, the sincere height y, the highest height (y + b), and the lowest south degree (yb) of the polar secondary light source are given by the following formula (3 ) ~ (5) represent: y = f2 · sin θ (3) y + b = f2 (sin β + sint,) (4) y — b = f2 (sin &lt; 9-sint,) (5) Therefore, The wheel ratio A, which is limited by the inner diameter 0 i and the outer diameter 0 of the bipolar secondary light source, is expressed by the following formula (6). Here, as shown in FIG. 6 (b), the inscribed 0i is the diameter of the circle inscribed on a pair of circles (equivalent to the aperture portion of the aperture 9 behind the hole) in a regular hexagonal surface light source. In addition, the outer diameter 0 is the diameter of a circle that lies outside the pair of circles. A = 0i / 0〇 = 2 (y — b) / (2 (y + b)) two (sin &lt; 9-sint 丨) / (sin θ + sint ’)

Msin θ - sin(a/(2 · fl · m)))/(sin $ + sin((a/ (2 · fl · m))) (6) 此外,兩極狀之二次光源的外徑0 〇由下巧公式(7 )表 示: - 0〇 = 2(y + b) = 2 · f2(sin θ + sint1) =2 · f2(sin θ + sin(2/(a · f 1 · m))) (7、Msin θ-sin (a / (2 · fl · m))) / (sin $ + sin ((a / (2 · fl · m))) (6) In addition, the outer diameter of the bipolar secondary light source is 0 〇 is represented by the following formula (7):-0〇 = 2 (y + b) = 2 · f2 (sin θ + sint1) = 2 · f2 (sin θ + sin (2 / (a · f 1 · m) )) (7,

裝 訂 -18-Binding -18-

497149 A7497149 A7

五、發明説明(16 ) 如此,參照公式(2 )〜(6 ),當連續變焦透鏡5之倍率m改 變時,可知兩極狀之二次光源中心高度y不改變,僅其寬 度2 b改變。亦即,藉由使連續變焦透鏡5的倍率m改變, 可以同時改變兩極狀之二次光源的大小(外徑0 〇)及其形狀 (輪帶比A)。 此外’參照公式(3 )〜(7 ),當變焦透鏡7的焦點距離f 2改 變時,可_知兩極狀之二次光源的輪帶比A不改變,而中心 向度y及其寬度2b同時改變。亦即,藉由使變焦透鏡7之焦 點距離f2改變,可以不改變兩極狀之二次光源的輪帶比 A,而改變其外徑0 〇。依據上述,藉由使連續變焦透鏡5 之倍率m與變焦透鏡7之焦點距離f2適切改變,可以不使兩 極狀之二次光源之外徑0 〇改變,而僅改變其輪帶比A。 此外,如圖6(b)所示,將形成之對光軸AX對稱性偏移之 兩個正六角形的面光源作爲二次光源,距各面光源之光軸 AX的距離y、各面光源之大小(寬度)2b、及自光軸AX估 計各面光源之角度,亦即方位角Φ,隨連續變焦透鏡5之 倍率m及變焦透鏡7之焦點距離f 2的改變而連續改變。因 而,使用兩極照明用之繞射光學元件6時,可以依據自光 源1射出之光束,幾乎無光量損失的形成兩極狀的二次光 源’因此可有效抑制限制二次光源之光束之孔徑光圈9的 光量損失,.來進行兩極照明。 其次説玥,使微複眼4自照明光程離開,同時在照明光程 中設定圓形照明用之繞射光學元件6 2以取代繞射光學元件 6,6 0或6 1,所獲得之一般圓形照明。此時,沿著光轴 -19- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 497149 A7 ___B7 五、發明説明(17 ) A X ’具有矩形剖面之光束射入連續變焦透鏡5。射入連續 變焦透鏡5的光束,因應其倍率被放大或縮小,原具有矩 形剖面的光束沿著光軸AX,自連續變焦透鏡5射出,並射 入繞射光學元件6 2 〇 此處之圓形照明用的繞射光學元件6 2具有將射入之矩形 光束轉換成圓形光束的功能。因此,由繞射光學元件62所 形成之圓歩光束穿透變焦透鏡7,在連續變焦透鏡8的射入 面上形成以光軸A X爲中心的圓形照射區域。因而也在複眼 透鏡8的後端焦點面上形成有以光軸a X爲中心的圓形二次 光源。此時,藉由使變焦透鏡7的焦點距離改變,可以適 切改變圓形之二次光源的外徑。 另外,對應於微複眼4自照明光程離開與將圓形照明用之 繞射光學元件6 2 s又足在照明光程上,自兩極孔徑光圈9、 八極孔徑光圈9a或變形四極孔徑光圈9b轉換成圓形孔徑光 圈9c。圓形孔徑光圈9c爲從兩個圓形孔徑光圈407及40 8選 出的一個圓形孔徑光圈,具有對應於圓形之二次光源大小 的孔徑部。如此,藉由使微複眼4自照明光程離開,且使 用圓形照明用的繞射光學元件6 2,可以依據自光源1射出 的光束’幾乎無光量損失的形成圓形的二次光源,可有效 抑制限制二次光源之光束之孔徑光圈中的光量損失,來進 行一般圓形照明。 以下,县體説明第一種實施形態之照明的轉換操作等。 首先’依據步進及反覆方式或步進及掃描方式,藉由鍵盤 等輸入機構20,將需要依序曝光之各種掩膜的相關資訊等 -20- ^張尺度適财目^^⑽)A4祕(21G X 297公釐) 497149 A7 B7 五、發明説明(18 ) 輸入控制系統21内。控制系統21將各種掩膜相關之最適切 線寬(解像度)、焦點深度等資訊記憶在内部的部分記憶體 内,因應輸入機構2 0的輸入,供應適切的控制信號至第一 驅動系統2 2〜第五驅動系統2 6。 亦即,依據最適切之解像度及焦點深度進行兩極照明 時,第二驅動系統2 4依據控制系統2 1的指令,將兩極照明 用的繞射_光學元件6固定在照明光程中。繼續,第二驅動 系統2 3依據控制系統2 1的指令,設定連續變焦透鏡5的倍 率,第四驅動系統2 5依據控制系統2 1的指令,設定變焦透 鏡7的焦點距離,在複眼透鏡8的後端焦點面上,獲得具有 所需大小(外徑)及形狀(輪帶比)的兩極狀二次光源。此 外,由於在有效抑制光量損失的狀態下,限制兩極狀的二 次光源’因此’第五驅動系統2 6依據控制系統2 1的指令, 使轉台旋轉,將所需的兩極孔徑光圈固定在照明光程中。 如此,可依據光源1的光束,幾乎無光量損失的形成兩極 狀的一次光源’因此可在限制二次光源射出之光束之孔徑 光圈中幾乎無光量損失的進行兩極照明。依據兩極狀之二 次光源的兩極照明可在確保指定之焦點深度下,使投影光 學系統P L對主要沿著一定方向的圖案形狀提高解像力。 再者,必要時,藉由以第二驅動系統2 3使連續變焦透鏡 5的倍率改變,以第四驅動系統2 5使變焦透鏡7的焦點距離 改變’可、適切改變形成在複眼透鏡8之後端焦點面上之兩 極狀之一次光源的大小及輪帶比。此時,轉台因應兩極狀 之--次光源之大小及輪帶比的改變而旋轉,選出具有所需 -21 - 本紙張尺度適财國@家標準(CNS) A4規格(21GX297公$V. Description of the invention (16) So, referring to formulas (2) to (6), when the magnification m of the continuous zoom lens 5 is changed, it can be seen that the center height y of the secondary secondary light source does not change, but only its width 2b changes. That is, by changing the magnification m of the continuous zoom lens 5, the size (outer diameter 0) of the bipolar secondary light source and its shape (belt ratio A) can be changed at the same time. In addition, with reference to the formulas (3) to (7), when the focal distance f 2 of the zoom lens 7 is changed, it can be seen that the belt ratio A of the bipolar secondary light source does not change, and the central direction y and its width 2b Change at the same time. That is, by changing the focal point distance f2 of the zoom lens 7, it is possible to change the outer diameter 0 of the secondary polarized light source without changing its belt ratio A. According to the above, by appropriately changing the magnification m of the continuous zoom lens 5 and the focal distance f2 of the zoom lens 7, it is possible to change only the wheel belt ratio A without changing the outer diameter 0 of the bipolar secondary light source. In addition, as shown in FIG. 6 (b), the two regular hexagonal surface light sources formed symmetrically offset from the optical axis AX are used as secondary light sources, the distance y from the optical axis AX of each surface light source, and each surface light source The size (width) 2b and the angle of each surface light source estimated from the optical axis AX, that is, the azimuth angle Φ, change continuously with the change in the magnification m of the continuous zoom lens 5 and the focal distance f 2 of the zoom lens 7. Therefore, when the diffractive optical element 6 for bipolar illumination is used, a bipolar secondary light source can be formed based on the light beam emitted from the light source 1 with almost no light loss. Therefore, it is possible to effectively suppress the aperture stop 9 that restricts the beam of the secondary light source. The amount of light is lost, for bipolar illumination. Secondly, let ’s say that the micro compound eye 4 is separated from the illumination optical path, and a diffractive optical element 62 for circular illumination is set in the illumination optical path to replace the diffractive optical element 6, 60 or 61, and the obtained general Circular lighting. At this time, along the optical axis -19- this paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 497149 A7 ___B7 V. Description of the invention (17) AX 'A beam with a rectangular cross section enters a continuous zoom Lens 5. The light beam incident on the continuous zoom lens 5 is enlarged or reduced according to its magnification. The light beam having a rectangular cross section along the optical axis AX exits from the continuous zoom lens 5 and enters the diffractive optical element 6 2. Here the circle The diffractive optical element 62 for shape illumination has a function of converting an incident rectangular light beam into a circular light beam. Therefore, a round chirped light beam formed by the diffractive optical element 62 penetrates the zoom lens 7 and forms a circular irradiation area centered on the optical axis A X on the incident surface of the continuous zoom lens 8. Therefore, a circular secondary light source centered on the optical axis a X is also formed on the rear focal surface of the fly-eye lens 8. At this time, by changing the focal distance of the zoom lens 7, the outer diameter of the circular secondary light source can be appropriately changed. In addition, corresponding to the micro compound eye 4 leaving the optical path of the illumination and using the diffractive optical element 6 2 s for circular illumination, it is sufficient to illuminate the optical path. 9b is converted into a circular aperture stop 9c. The circular aperture stop 9c is a circular aperture stop selected from two circular aperture stops 407 and 408, and has an aperture portion corresponding to the size of a circular secondary light source. In this way, by leaving the micro compound eye 4 away from the illumination optical path and using the diffractive optical element 62 for circular illumination, a circular secondary light source can be formed based on the light beam 'emitted from the light source 1 with almost no loss of light amount, It can effectively suppress the loss of light amount in the aperture stop that restricts the light beam of the secondary light source for general circular lighting. In the following, the prefecture will explain the lighting conversion operation and the like of the first embodiment. First of all, according to the step and repeat method or step and scan method, through the keyboard and other input mechanisms 20, the relevant information of the various masks that need to be sequentially exposed will be disclosed. -20- ^ 张 标定 财 目 ^^ ⑽) A4 Secret (21G X 297 mm) 497149 A7 B7 V. Description of the invention (18) Enter the control system 21. The control system 21 stores information such as the optimal line width (resolution) and depth of focus of various masks in some internal memories, and supplies appropriate control signals to the first drive system 2 according to the input of the input mechanism 20. ~ Fifth drive system 2 6. That is, when performing bipolar illumination based on the most appropriate resolution and focal depth, the second drive system 24 fixes the diffraction_optical element 6 for bipolar illumination in the light path of the illumination according to the instruction of the control system 21. Continuing, the second driving system 23 sets the magnification of the continuous zoom lens 5 according to the instruction of the control system 21, and the fourth driving system 25 sets the focus distance of the zoom lens 7 according to the instruction of the control system 21, and sets the focus distance of the zoom lens 7 On the rear focal plane, a bipolar secondary light source with the required size (outer diameter) and shape (belt ratio) is obtained. In addition, because the bipolar secondary light source is restricted in a state where the loss of light quantity is effectively suppressed, the fifth drive system 2 6 rotates the turntable according to the instructions of the control system 21 and fixes the required bipolar aperture diaphragm to the lighting. Light path. In this way, the bipolar primary light source 'can be formed with almost no light loss depending on the light beam of the light source 1, and thus the bipolar illumination can be performed with almost no light loss in the aperture stop which restricts the light beam emitted from the secondary light source. The bipolar illumination based on the bipolar secondary light source can make the projection optical system PL to improve the resolution of the pattern mainly along a certain direction while ensuring the specified focal depth. Furthermore, when necessary, the magnification of the continuous zoom lens 5 is changed by the second driving system 23, and the focal distance of the zoom lens 7 is changed by the fourth driving system 25. The change can be made appropriately after the fly-eye lens 8. The magnitude and wheel ratio of the two-pole primary light source on the end focus surface. At this time, the turntable was rotated in response to changes in the size of the bipolar light source and the ratio of the wheel and belt, and was selected to have the required -21-this paper size is suitable for financial countries @ 家 标准 (CNS) A4 size (21GX297)

大小及輪帶比之兩極孔徑光圈 此’可在兩極狀之二次光源的 量損失的使兩極狀之二次光源 進行多種兩極照明。 ,並固定在照明光程中。如 形成及其限制中,幾乎無光 的大小及輪帶比適切改變來 此外’依據最適切之解德命 卜 度及焦點深度進行一般圓形照 明時,第一驅動系統2 2依據柝 佩k制系統2 1的指令,使微複眼 4自照明光程中離開。此外一 - r 罘二驅動系統24依據控制系The diameter and aperture ratio of the two-pole aperture diaphragm This' allows the two-pole-shaped secondary light source to perform a variety of two-pole illumination at the loss of the amount of the two-pole-shaped secondary light source. , And fixed in the light path. For example, in the formation and its limitation, the size of almost no light and the ratio of the wheel belt change appropriately. In addition, when performing general circular lighting based on the most appropriate solution power and depth of focus, the first drive system 2 2 is based on the 柝 佩 k The command of the control system 21 causes the micro compound eye 4 to leave from the illumination path. Besides one-r r drive system 24 according to the control system

裝 統21的指令’將一般圓形照明用之繞射光學元件62固定在 …、明光私中。、繼、續’第二驅動系統23依據控㈣系統2 ^的指 令,設定連續變焦透鏡5的倍率,第四驅動系統25依據控 制系統2i的指令,設定變焦透鏡7的焦點距離,在複眼透 4¾ 8 i後端焦點面上獲得具有所需大小(外徑)的圓形二次 源。 癱 此外,爲求在有效抑制光量損失的狀態下限制圓形的二 次光源,第五驅動系統2 6依據控制系統2 i的指令使轉台旋 轉,將所需之圓形孔徑光圈固定在照明光程中。另外,使 用可使圓形孔徑連續性改變的彩虹光圈時,第五驅動系統 2 6依據棱制系統2 1的指令設定彩虹光圈的孔徑。如此,可 依據光源1射出的光束,幾乎無光量損失的形成圓形二次 光源,因此可有效抑制限制二次光源之光束之孔徑中的光 量損失,來進行一般圓形照明。 再者’功要時,可藉由以第四驅動系統2 5使變焦透鏡7 的焦點距離改變,來適切改變形成在複眼透鏡8之後端焦 點面上之圓形二次光源的大小。此時,轉台因應圓形二次 -22- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 497149 A7 B7 五、發明説明(2〇 ) 光源的大小旋轉,選出具有所需大小之孔徑部的圓形孔徑 光圈,並固定在照明光程中。如此,可在圓形之二次光源 的形成及其限制中,有效抑制光量損失,使値適切改變 來進行多種的一般圓形照明。 如上所述,上述第一種實施形態可有效抑制因限制二次 光源之孔徑光圈的光量損失,進行兩極照明等的變形照明 及一般圓f照明。再者,藉由使連續變焦透鏡的倍率改變 及使變焦透鏡的焦點距離改變的簡單操作,可有效抑制孔 徑光圈的光量損失,使變形照明及一般圓形照明的參數改 變。因此,可使變形照明之種類及參數適切改變,獲得適 於曝光投影之微細圖案之投影光學系統的解像度及焦點深 度。因此可依據高度曝光亮度及良妤的曝光條件,進行通 量高的良好投影曝光。 圖7爲概略顯示具備本發明第二種實施形態之照明光學裝 置之曝光裝置的構造圖。第二種實施形態具有與第一種實 施形態類似的構造。但是,第一種實施形態中係在折射鏡 3與連續變焦透鏡5之間配置有微複眼4,且在連續變焦透 鏡5與變焦透鏡7之間配置有繞射光學元件6 ( 6 0〜6 2 ),而 第二種實施形態則是在折射鏡3與連續變焦透鏡5之間配置 有繞射光學元件6(60,61),且在連續變焦透鏡5與變焦透 鏡7之間配置有微複眼4。亦即,第一種實施形態與第二種 實施形態啲基本差異處僅爲微複眼及繞射光學元件的配置 位置相反。另外,第二種實施形態與第一種實施形態不同 之處爲沒有圓形照明用的繞射光學元件。 -23- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐)The command of the device 21 'fixes the diffractive optical element 62 for general circular lighting in the bright light. Continue, follow, continue 'The second drive system 23 sets the magnification of the continuous zoom lens 5 in accordance with the instructions of the control system 2 ^, and the fourth drive system 25 sets the focus distance of the zoom lens 7 in accordance with the instructions of the control system 2i, and transmits through the compound eye A circular secondary source with the required size (outer diameter) is obtained on the focal surface of the 4¾ 8 i rear end. In addition, in order to limit the circular secondary light source while effectively suppressing the loss of light, the fifth drive system 26 rotates the turntable according to the instructions of the control system 2 i, and fixes the required circular aperture diaphragm to the illumination light. Process. In addition, when using a rainbow aperture that can change the continuity of the circular aperture, the fifth drive system 26 sets the aperture of the rainbow aperture according to the instruction of the prism system 21. In this way, a circular secondary light source can be formed based on the light beam emitted from the light source 1 with almost no loss of light amount. Therefore, it is possible to effectively limit the loss of light amount in the aperture of the light beam of the secondary light source for general circular lighting. Moreover, when the function is important, the size of the circular secondary light source formed on the focal point surface of the rear end of the fly-eye lens 8 can be appropriately changed by changing the focal distance of the zoom lens 7 by the fourth driving system 25. At this time, the turntable should respond to the circular quadratic 22- This paper size applies the Chinese National Standard (CNS) A4 specification (210X 297 mm) 497149 A7 B7 V. Description of the invention (20) The size of the light source is rotated and selected to have the required The circular aperture stop of the small and large aperture section is fixed in the illumination path. In this way, in the formation and limitation of the circular secondary light source, it is possible to effectively suppress the loss of light quantity, and appropriately change the chirp to perform a variety of general circular lighting. As described above, the first embodiment described above can effectively suppress the loss of light due to the limitation of the aperture stop of the secondary light source, and perform deformation lighting such as bipolar lighting and general circular f lighting. Furthermore, the simple operation of changing the magnification of the continuous zoom lens and changing the focal distance of the zoom lens can effectively suppress the loss of the light amount of the aperture diaphragm, and change the parameters of anamorphic lighting and general circular lighting. Therefore, the types and parameters of the anamorphic illumination can be appropriately changed, and the resolution and focal depth of the projection optical system suitable for exposure and projection of a fine pattern can be obtained. Therefore, a good projection exposure with high flux can be performed according to the high exposure brightness and good exposure conditions. Fig. 7 is a structural diagram schematically showing an exposure apparatus provided with an illumination optical apparatus according to a second embodiment of the present invention. The second embodiment has a structure similar to that of the first embodiment. However, in the first embodiment, a micro fly eye 4 is arranged between the refraction lens 3 and the continuous zoom lens 5, and a diffractive optical element 6 (60 to 6 is arranged between the continuous zoom lens 5 and the zoom lens 7). 2), and the second embodiment is that a diffractive optical element 6 (60, 61) is arranged between the refraction lens 3 and the continuous zoom lens 5, and a micro lens is arranged between the continuous zoom lens 5 and the zoom lens 7. Compound eyes 4. That is, the basic difference between the first embodiment and the second embodiment is only that the positions of the micro compound eyes and the diffractive optical elements are opposite. The second embodiment differs from the first embodiment in that there is no diffractive optical element for circular illumination. -23- This paper size applies to China National Standard (CNS) A4 (210X 297mm)

裝 497149 A7 B7 五、發明説明(21 ) 如上所述,第一種實施形態之微複眼4及連續變焦透鏡5 構成角度光束形成機構,其係將光源1射出之光束轉換成 對光軸AX具有各種角度成分的光束,並使其射入繞射光學 元件6(60,61)的繞射面上。此時微複眼4構成散射光束形 成元件,其係將光源1射出之概略平行的光束轉換成以對 光軸A X成各種角度散射的光束。此外,繞射光學元件 6 ( 6 0,6 1_)及變焦透鏡7構成照射區域形成機構,其係依據 具有各種角度成分的射入光束,將對光軸A X對稱性偏移的 數個(兩個)照射區域形成在複眼透鏡8的射入面上。此時, 繞射光學元件6(60,6 1)構成光束轉換元件,其係將射入 光束轉換成數個(兩個)光束。 反之,第二種實施形態之繞射光學元件6(60,61)與連 續變焦透鏡5係構成光束形狀轉換機構,其係將光源1射出 之光束轉換成對光軸AX偏移的數個(兩個)光束,自這些光 束射出的光線自對光軸AX傾斜的方向射入微複眼4的射入 面。此時,繞射光學元件6(60,61)構成光束轉換元件, 其係將光源1射出之概略平行的光束轉換成數個(兩個)光 束。此外,微複眼4及變焦透鏡7係形成照射區域形成機 構,其係依據斜向射入的光束,在複眼透鏡8的射入面上 形成對光軸AX對稱性偏移的數個(兩個)照射區域。此時, 微複眼4係構成波面分割元件,其係波面分割射入光束, 形成許多咣源。 如此,第一種實施形態與第二種實施形態之微複眼4及縫 射光學元件6(60,61)的配置位置相反。但是,第—種實 -24- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)497149 A7 B7 V. Description of the invention (21) As mentioned above, the micro compound eye 4 and the continuous zoom lens 5 of the first embodiment form an angle beam forming mechanism, which converts the light beam emitted from the light source 1 into the optical axis AX having Light beams of various angle components are made to enter the diffraction surfaces of the diffractive optical element 6 (60, 61). At this time, the micro compound eye 4 constitutes a scattered light beam forming element, which converts a substantially parallel light beam emitted from the light source 1 into a light beam scattered at various angles with respect to the optical axis A X. In addition, the diffractive optical element 6 (6 0, 6 1_) and the zoom lens 7 constitute an irradiation area forming mechanism, which are based on a plurality of angle components (2) which are symmetrically shifted from the optical axis AX based on the incident light beam having various angular components. (A) The irradiation area is formed on the incident surface of the fly-eye lens 8. At this time, the diffractive optical element 6 (60, 61) constitutes a light beam conversion element which converts the incident light beam into several (two) light beams. Conversely, the diffractive optical element 6 (60, 61) and the continuous zoom lens 5 of the second embodiment form a beam shape conversion mechanism, which converts the light beam emitted from the light source 1 into a number of shifts to the optical axis AX ( (2) Light beams, and the light rays emitted from these light beams are incident on the entrance surface of the micro compound eye 4 from a direction inclined to the optical axis AX. At this time, the diffractive optical element 6 (60, 61) constitutes a light beam conversion element which converts a substantially parallel light beam emitted from the light source 1 into several (two) light beams. In addition, the micro fly's eye 4 and the zoom lens 7 form an irradiation area forming mechanism. Based on the light beam incident obliquely, a plurality of (two are symmetrically offset from the optical axis AX are formed on the incident surface of the fly eye lens 8). ) Irradiated area. At this time, the micro compound eye 4 system constitutes a wavefront division element, and the wavefront divides the incident light beam to form many chirped sources. As described above, the arrangement positions of the micro compound eyes 4 and the slit optical elements 6 (60, 61) of the first embodiment and the second embodiment are opposite. However, Article No. -24- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)

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497149 A7 _ B7 ____ 五、發明説明(22 ) 施形態之自微複眼4至變焦透鏡7的部分光學系統,與第二 種實施形態之自繞射光學元件6 ( 6 0,6 1 )至變焦透鏡7之部 分光學系統在光學上等效。因此,第一種實施形態之自微 複眼4至複眼透鏡8之部分光學系統與第二種實施形態之自 繞射光學元件6 ( 6 0,6 1 )至複眼透鏡8之部分光學系统,在 構成二次光源形成機構上,其係依據光源1射出之光束, 在與投影光學系統P L之瞳孔共軛的照明瞳孔内,形成對光 軸A X對稱性偏移的數個面光源相同。 以下,針對與第一種實施形態的差異處,簡單説明第二 種實施形態。第二種實施形態之連續變焦透鏡5將繞射光 學元件6與微複眼4的射入面構成光學性之概略共輛^連結。 此外,變焦透鏡7將微複眼4之後端焦點面與複眼透鏡8之 射入面連結成實質上之傅里葉轉換的關係。因此,穿透兩 極照明用之繞射光學元件6的光線在連續變焦透鏡5的瞳孔 面上形成如圖3 (b )所示的兩個點像。 這兩個點像射出的光線穿透連續變焦透鏡5形成平行光, 自對光軸A X傾斜的方向射入微複眼4的射入面。因而,第 二種實施形態與第一種實施形態同樣的,在變焦透鏡7之 後端焦點面及在複眼透鏡8的射入面上形成有如圖4 (b)所 示之對光軸AX對稱性偏移的兩個照射區域,亦即兩極狀的 照射區域。繼續,在複眼透鏡8的後端焦點面上,依據光 源1射出的光束’幾乎無光量損失的形成有兩極狀的二次 光源。此外’配置在複眼透鏡8之後端焦點面附近的孔徑 光圈9中也幾乎不產生光量損失。而有關藉由使連續變焦 -25- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 497149 A7 B7 五、發明説明(23 ) 透鏡5之倍率及變焦透鏡7的焦點距離適切改變,可以改變 兩極狀之二次光源的大小及形狀(輪帶比),則與第一種實 施形態相同。 圖8爲概略顯示第一種實施形態及第二種實施形態之類似 例的重要部分構造圖。圖8之類似例具有與第一種實施形 態及第二種實施形態類似的構造。但是基本差異僅爲,第 一種實施弗態及第二種實施形態係使用波面分割型的複眼 透鏡’作爲光學積分器。圖8之類似例則是使用内面反射 型的棒狀光學積分器。另外,圖8中比第一種實施形態及 第二種實施形態的變焦透鏡7還省略了光源端的要素及驅 動控制關係之要素等的圖式。以下針對與第一種實施形態 及第二種實施形態的差異處來説明類似例。 類似例中’對應於使用棒狀積分器8 a來取代複眼透鏡 8,在變焦透鏡7與棒狀積分器8 a之間的光程中附設聚光鏡 7 a,故置成像光學系統i 〇 a來取代聚光光學系統丄〇,同 時,省略用於限制二次光源的孔徑光圈。此處,由變焦透 鏡7與炙光鏡7 a所構成的合成光學系統,在對應於第一種 實施形態之類似例中,將繞射光學元件6(6〇〜62)的繞射面 與2狀積分器8a的射入面連結成光學性概略共軛,在對應 於第二種實施形態的類似例中,將微複眼4之後端焦點面 與棒狀積分器8a之射入面連結成光學性概略共耗。此外, 成像光學系統1〇a將棒狀積分器8a之射出面與掩膜乂連結 成光學性的概略共軛。 棒狀積分器8a爲由石英玻璃及螢石等玻璃材料構成的内 -26- 297^57 巧張尺度適财國國 497149 A7 B7 五、發明説明(24 面反射型玻璃棒,利用内部與外部之界面,亦即内面的全 反射,通過聚光點,在射入面上,沿著平行面形成因應内 面反射數之數量的光源圖像。此時所形成之光源圖像大部 分爲虛像,而僅中心(聚光點)的光源圖像爲實像。亦即, 射入棒狀積分器8 a的光束被内面反射沿著角度方向分割, 通過聚光點,在其射入面上,沿著平行面,形成由許多光 源圖像構成的二次光源。 經棒狀積分器8 a在其射入端所形成之二次光源射出的光 束在其射出面上重疊後,穿透成像光學系統1 〇 a,均勻照 明形成有指定圖案的掩膜Μ。如上所述,成像光學系統 l〇a將棒狀積分器8a的射出面與掩膜Μ(或晶圓W)連結成 光學性概略共軛。因此,在掩膜Μ上形成有與棒狀積分器 8 a之剖面形狀類似之矩形的照射區域。因而,類似例也與 第一種實施形態及第二種實施形態同樣的,可有效抑制光 量損失,來進行兩極照明等的變形照明及一般的圓形照 明。 上述各種實施形態之曝光裝置藉由使用照明光學裝置來 照明掩膜(照明步驟),使用投影光學系統將形成在掩膜上 之複製用圖案掃描曝光在感光性基板上(曝光步驟),可以 製造微型裝置(半導體元件、攝影元件、液晶顯示元件、薄 膜磁頭等)。以下,參照圖9之流程圖來説明藉由使用圖1 所示之第一實施形態的曝光裝置或圖7所示之第二實施形 態的曝光裝置,在感光性基板之晶圓等上形成指定電路圖 案,獲得半導體裝置等微型裝置時的一種方法。 -27- 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公釐)497149 A7 _ B7 ____ 5. Description of the invention (22) Part of the optical system from the micro compound eye 4 to the zoom lens 7 of the application mode, and the self-diffractive optical element 6 (60, 6 1) to the zoom of the second embodiment Part of the optical system of the lens 7 is optically equivalent. Therefore, part of the optical system from the micro fly eye 4 to the fly eye lens 8 in the first embodiment and part of the optical system from the self-diffractive optical element 6 (60, 6 1) to the fly eye lens 8 in the second embodiment are in The secondary light source forming mechanism is the same as several surface light sources that are symmetrically offset from the optical axis AX in the illumination pupil conjugated to the pupil of the projection optical system PL based on the light beam emitted from the light source 1. The differences from the first embodiment will be briefly described below. The continuous zoom lens 5 of the second embodiment connects the diffractive optical element 6 and the entrance surface of the micro-complex eye 4 to form an optical outline. In addition, the zoom lens 7 connects the focal surface at the rear end of the micro fly eye 4 and the incident surface of the fly eye lens 8 into a substantially Fourier transform relationship. Therefore, the light passing through the diffractive optical element 6 for polarized illumination forms two spot images on the pupil surface of the continuous zoom lens 5 as shown in FIG. 3 (b). The light emitted from these two point images penetrates the continuous zoom lens 5 to form parallel light, and enters the incident surface of the micro compound eye 4 from a direction inclined to the optical axis A X. Therefore, in the second embodiment, similar to the first embodiment, a symmetry with respect to the optical axis AX as shown in FIG. 4 (b) is formed on the focal surface at the rear end of the zoom lens 7 and on the incident surface of the fly-eye lens 8. The two irradiated regions that are offset, that is, polarized irradiated regions. Continuing, on the rear focal plane of the fly-eye lens 8, a bipolar secondary light source is formed with almost no light loss depending on the light beam 'emitted from the light source 1. In addition, the aperture diaphragm 9 disposed near the focal plane of the rear end of the fly-eye lens 8 hardly causes a loss of light amount. With regard to the continuous zoom-25- this paper size applies the Chinese National Standard (CNS) A4 specification (210X 297 mm) 497149 A7 B7 V. Description of the invention (23) The magnification of lens 5 and the focal distance of zoom lens 7 are appropriate The change can change the size and shape (wheel ratio) of the bipolar secondary light source, which is the same as the first embodiment. Fig. 8 is a structural diagram showing the essential parts of a similar example of the first embodiment and the second embodiment. The similar example of Fig. 8 has a structure similar to that of the first embodiment and the second embodiment. However, the basic difference is only that the first embodiment and the second embodiment use a wavefront split type fly-eye lens' as an optical integrator. A similar example in Fig. 8 uses a rod-shaped optical integrator of the internal reflection type. In addition, in FIG. 8, the elements of the light source side and the elements of the drive control relationship are omitted from the zoom lens 7 of the first embodiment and the second embodiment. Hereinafter, similar examples will be described with respect to differences from the first embodiment and the second embodiment. In the similar example, 'corresponding to the use of a rod-shaped integrator 8 a instead of the fly-eye lens 8, a condenser 7 a is attached to the optical path between the zoom lens 7 and the rod-shaped integrator 8 a, so the imaging optical system i 〇a is provided. Instead of condensing optical system 丄 〇, at the same time, the aperture stop for limiting the secondary light source is omitted. Here, in a similar example corresponding to the first embodiment, the composite optical system composed of the zoom lens 7 and the glare lens 7 a is formed by diffractive surfaces of the diffractive optical element 6 (60-62) and The incident surface of the two-shaped integrator 8a is connected to form an optically conjugate. In a similar example corresponding to the second embodiment, the rear focal surface of the micro compound eye 4 and the incident surface of the rod-shaped integrator 8a are connected to each other. Optical properties are generally consumed. In addition, the imaging optical system 10a connects the exit surface of the rod integrator 8a and the mask 掩 to form an optically approximate conjugate. The rod-shaped integrator 8a is made of glass materials such as quartz glass and fluorite. -26- 297 ^ 57 Kojima scale suitable country 497149 A7 B7 5. Description of the invention (24-sided reflective glass rod, using the inside and outside The interface, that is, the total reflection of the inner surface, passes through the condensing point and forms a light source image corresponding to the number of internal surface reflections along the parallel plane on the incident surface. Most of the light source images formed at this time are virtual images. The light source image at only the center (condensing point) is a real image. That is, the light beam incident on the rod integrator 8 a is reflected by the inner surface and divided along the angular direction. The secondary light source composed of many light source images is formed on the parallel plane. The light beam emitted by the secondary light source formed by the rod integrator 8 a at its entrance end is superimposed on its exit surface and penetrates the imaging optical system. 10a, uniformly illuminate the mask M with a specified pattern. As described above, the imaging optical system 10a connects the exit surface of the rod integrator 8a and the mask M (or the wafer W) to form an optical outline. Therefore, a rod-shaped product is formed on the mask M. The rectangular irradiation area of the cross section of the device 8a is similar. Therefore, similar examples are also the same as the first embodiment and the second embodiment, which can effectively suppress the loss of light amount, and perform deformation lighting such as bipolar lighting and general Circular illumination. The exposure apparatus of the various embodiments described above uses the illumination optical device to illuminate the mask (illumination step), and uses a projection optical system to scan and expose the copy pattern formed on the mask on the photosensitive substrate (exposure step ), Micro devices (semiconductor elements, photographic elements, liquid crystal display elements, thin-film magnetic heads, etc.) can be manufactured. Hereinafter, the exposure apparatus of the first embodiment shown in FIG. 1 or FIG. 7 will be described with reference to the flowchart of FIG. 9. The exposure apparatus of the second embodiment shown is a method for forming a predetermined circuit pattern on a wafer or the like of a photosensitive substrate to obtain a micro device such as a semiconductor device. -27- This paper is in accordance with China National Standard (CNS) A4 Specifications (210X297 mm)

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497149 A7 _B7 五、發明説明(25~~^ ' 首先’在圖9的步骤301中,於一批晶圓上蒸鍍有金屬 膜。其次在步驟302中,於該批晶圓上的金屬膜上塗敷有 光阻。之後,於步驟303中,使用圖i或圖7所示之曝光裝 置,掩膜上之圖案圖像經由其投影光學系統(投影光學模 組),被依序曝光複製到該批晶圓上的各照射區域。之後, 於步驟3 04中’進行該批晶圓上的光阻顯像後,於步驟3〇5 中,藉由在該批晶圓上,將光阻圖案作爲掩膜進行蝕刻, 在各晶圓上之各照射區域形成對應於掩膜上之圖案的電路 圖案。之後,再藉由形成上層的電路圖案等,製造出半導 體元件等的裝置。採用上述的半導體裝置製造方法,可獲 得良好通量之具有極微細電路圖案的半導體裝置。 另外,上述各實施形態可採用將作爲光束轉換元件的繞 射光學元件6 ( 6 1〜6 2 )以轉台方式固定在照明光程中的構 造。此外,亦可利用一般的滑動機構進行上述繞射光學元 件6(6 1〜62)的拆裝及轉換。 此外,上述各實施形態係將構成微複眼4之微小透鏡的形 狀設定成正六角形。此因圓形之微小透鏡無法緊密排列, 會產生光量損失,因而選擇接近圓形之多角形的正六角 形。但是,構成微複眼4之各微小透鏡的形狀並不限定於 此,例如亦可使用包含矩形的其他適切形狀。此外,上述 各實施形態係將構成微複眼4之微小透鏡的折射力爲正折 射力,不過該微小透鏡的折射力亦可爲負値。 再者,上述第一種實施形態係使用連續變焦透鏡5,不過 亦可採用以焦點變焦透鏡(Focal Zoom Lens)來取代連續變 -28- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 497149 A7 B7 説明)~ 一 焦透鏡,在微複眼4之前方配置繞射光學元件,將矩形光 束轉換成圓形光束的構造。此外,上述各實施形態係使用 一個複眼透鏡8,不過使用兩個複眼透鏡之雙複眼方式亦 可適用於本發明。再者,上述第一種實施形態於進行一般 圓形照明時,係將繞射光學元件6 2固定在照明光程中,不 過亦可省略該繞射光學元件6 2。 此外、,Λ述各種實施形態係使用微複眼4作爲散射光束形 成元件,不過,必要時亦可使用複眼透鏡及繞射光學元件 等。再者,上述各種實施形態係使用繞射光學元件作爲光 束轉換元件6 ( 6 1〜6 2 ),不過並不限定於此,例如,亦可使 用微複眼及微小棱柱透鏡等折射光學元件。而有關本發明 中可以利用之繞射光學元件的詳細説明揭示於美國專利第 5,850,300號公報等。 此外,上述各種實施形態係以具備照明光學裝置之投影 曝光裝置爲例來説明本發明,當然本發明亦可適用於用於 均勻照明掩膜以外之被照射面的一般照明光學裝置。 另外,上述各種實施形態之導光光學系統的構造,係藉 由聚光光學系統1 0將形成在孔徑光圈9位置上之二次光源 射出的光線予以聚光,重疊性的照明掩膜,不過亦可在聚 光光學系統10與掩膜Μ之間配置照射區域光圈(Mask Blind) 及將該照射區域光圈圖像形成在掩膜Μ上的轉像(Relay)光 學系統。呲時,導光光學系統由聚光光學系統1 〇與轉像光 學系統構成,聚光光學系統1 〇將形成在孔徑光圈9之位置 上之二次光源射出的光線予以聚光,重疊性照明照射區域 -29- 本紙張尺度相巾目时標準(CNS) A视格(21GX 297公釐y 497149 A7 B7 五、發明説明(27 ) 光圈,轉像光學系統將照射區域光圈的孔徑部圖像形成在 掩膜Μ上。以上説明,各種實施形態的類似例均同。 此外’上述各種實施形態係集合數個要素透鏡形成複眼 透鏡8 ’不過亦可將其作爲微複眼。所謂微複眼,係指採 用餘刻等方法在透光性基板上將數個微小透鏡面設置成矩 陣狀者。有關形成數個光源像方面,複眼透鏡與微複眼之 間在功能占實質上並無差異,不過就可使一個要素透鏡(微 小透鏡)之孔徑大小形成極小,可大幅降低製造成本,及可 使光軸方向的厚度及薄等方面而言,微複眼較爲優異。 再者’上述各種實施形態係在複眼透鏡8之後端焦點面附 近配置用於限制二次光源之光束的孔徑光圈9。但是亦可 採用省略孔徑光圈的配置,使二次光源之光束完全不受限 制的構造。 例如,將上述之複眼透鏡8作爲微複眼時,將構成複眼透 叙之各透鏡單元剖面積設定成極小的情況下,可採省略孔 徑光圈的配置,使二次光源之光束完全不受限制的構造。 此外,上述各種實施形態因係使用KrF準分子雷射(波 長:248 nm)及ArF準分子雷射(波長:193 nm)等波長在 180 nm以上的曝光光線作爲光源,因此繞射光學元件可以 石英玻璃形成。另外,使用2〇〇 nm以下之波長作爲曝光光 線時,如在使用供應眞空紫外區波長之曝光光線的h雷射 (波長:157 nm)的情況下,亦可以螢石、摻雜有氟之石英 玻璃、掺雜有氟及氫之石英玻璃、構造指定溫度在12〇〇 κ 以下,且OH基濃度在1〇〇〇 ppm以上之石英玻璃、構造指 -30 - 本紙張尺度適用中國國家標準(CNS) A4規格(210X297公爱) 497149 A7 B7 五、發明説明(28 ) 定溫度在1200 K以下,且氫分子濃度在1 X 1017 molecules/cm3以上之石英玻璃、構造指定溫度在1200 K以 下,且氯濃度在50 ppm以下之石英玻璃、及構造指定溫度 在1200 K以下,且氫分子濃度在1 xlO17 molecules/cm3以 上,且氯濃度在50 ppm以下之石英玻璃群中選出的材料來 形成繞射光學元件。 另外,有關構造指定溫度在1200 K以下,且OH基濃度在 1000 ppm以上之石英玻璃,如本專利申請人於日本專利第 2770224號公報中所揭示,有關構造指定溫度在1200 K以 下,且氫分子濃度在1 X 1017 molecules/cm3以上之石英玻 璃、構造指定溫度在1200 K以下,且氣濃度在50 ppm以下 之石英玻璃、及構造指定溫度在1200 K以下,且氫分子濃 度在1 X 1 0 17 molecules/cm3以上,且氯濃度在50 ppm以下 之石英玻璃,則如本專利申請人於日本專利第293613 8號公 報中所揭示。 如以上説明,本發明之各種實施形態的照明光學裝置可 有效抑制因限制二次光源造成孔徑光圈之光量損失,來進 行兩極照明等之變形照明及一般圓形照明。因而可確保指 定之焦點深度,使投影光學系統對特定圖案形狀提高解像 力。此外,藉由使連續變焦透鏡之倍率改變,及使變焦透 鏡之焦點距離政變的簡單操作,可有效抑制孔徑光圈的光 量損失,使變形照明的參數改變。 因此,安裝本發明各種實施形態之照明光學裝置的曝光 裝置,使變形照明之種類及參數適切改變,可獲得適於需 -31 - 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)497149 A7 _B7 V. Description of the invention (25 ~~ ^ 'First' In step 301 of FIG. 9, a metal film is vapor-deposited on a batch of wafers. Second, in step 302, the metal film on the batch of wafers A photoresist is applied on the surface. Then, in step 303, the exposure device shown in FIG. I or FIG. 7 is used, and the pattern image on the mask is sequentially exposed and copied through its projection optical system (projection optical module). Each illuminated area on the batch of wafers. After that, the photoresist development on the batch of wafers is performed in step 304, and then in step 305, the photoresist is applied on the batch of wafers. The pattern is etched as a mask, and a circuit pattern corresponding to the pattern on the mask is formed in each irradiated area on each wafer. Then, a device such as a semiconductor element is manufactured by forming an upper circuit pattern and the like. Using the above The method for manufacturing a semiconductor device can obtain a semiconductor device having an extremely fine circuit pattern with a good flux. In addition, in each of the above embodiments, the diffractive optical element 6 (6 1 to 6 2), which is a light beam conversion element, can be used in a turntable manner. Fixed in the light path In addition, the above-mentioned diffractive optical element 6 (6 1 to 62) can be disassembled and converted by using a general sliding mechanism. In addition, in each of the above embodiments, the shape of the micro lens constituting the micro compound eye 4 is set Regular Hexagon. Because circular micro lenses cannot be arranged closely, light loss will occur. Therefore, a regular hexagon that is close to a circular polygon is selected. However, the shape of each micro lens constituting the micro compound eye 4 is not limited to this, for example Other suitable shapes including rectangles can also be used. In addition, in the above embodiments, the refractive power of the microlenses constituting the micro compound eye 4 is positive, but the refractive power of the microlenses may also be negative. The first embodiment uses a continuous zoom lens 5. However, a focal zoom lens (Focal Zoom Lens) can also be used instead of the continuous variable -28- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) ) 497149 A7 B7 Description) ~ A focal lens with a diffractive optical element in front of the micro compound eye 4 to convert a rectangular beam into a circular beam. In addition, each of the above embodiments uses one fly-eye lens 8, but the double-eye method using two fly-eye lenses is also applicable to the present invention. Moreover, in the first embodiment described above, when performing general circular illumination, the diffractive optical element 62 is fixed in the optical path of the illumination, but the diffractive optical element 62 may be omitted. In addition, although the various embodiments described above use the micro fly eye 4 as a scattered light beam forming element, a fly eye lens, a diffractive optical element, etc. may be used if necessary. The various embodiments described above use diffractive optical elements as the light beam conversion elements 6 (6 1 to 6 2). However, the present invention is not limited to this. For example, refractive optical elements such as a micro compound eye and a micro prism lens may be used. A detailed description of the diffractive optical element that can be used in the present invention is disclosed in U.S. Patent No. 5,850,300 and the like. In addition, the various embodiments described above take the projection exposure device provided with the illumination optical device as an example to explain the present invention. Of course, the present invention can also be applied to a general illumination optical device for uniformly illuminating an illuminated surface other than a mask. In addition, the structures of the light-guiding optical systems of the various embodiments described above are based on a condensing optical system 10 for condensing light emitted from a secondary light source formed at a position of the aperture stop 9 at an overlapping lighting mask. An optical region diaphragm (Mask Blind) and a relay optical system for forming an image of the illuminated region diaphragm on the mask M may be disposed between the condenser optical system 10 and the mask M. At first, the light guide optical system is composed of a condensing optical system 10 and an image transfer optical system. The condensing optical system 10 focuses the light emitted by the secondary light source formed at the position of the aperture stop 9 and overlaps the illumination. Irradiation area-29- The standard of this paper standard (CNS) A viewing frame (21GX 297 mm y 497149 A7 B7) V. Description of the invention (27) Aperture, the image of the aperture part of the aperture of the irradiated area by the transfer optical system It is formed on the mask M. As described above, the similar examples of the various embodiments are the same. In addition, the above-mentioned various embodiments are formed by combining a plurality of element lenses to form a fly-eye lens 8. Refers to those who set a few micro lens surfaces in a matrix on a light-transmitting substrate by means such as intaglio. Regarding the formation of several light source images, there is virtually no difference in function between the compound eye lens and the micro compound eye, but The size of the aperture of an element lens (micro lens) can be made extremely small, manufacturing costs can be greatly reduced, and the thickness and thinness in the optical axis direction can be made. Micro compound eyes are excellent. Furthermore, in the above-mentioned various embodiments, an aperture stop 9 for restricting the light beam of the secondary light source is arranged near the focal surface at the rear end of the fly-eye lens 8. However, a configuration in which the aperture stop is omitted may be adopted so that the light beam of the secondary light source is not affected at all For example, when the compound eye lens 8 described above is used as a micro compound eye, and the cross-sectional area of each lens unit constituting the compound eye is set to be extremely small, the configuration of the aperture stop can be omitted to make the beam of the secondary light source completely. The structure is not limited. In addition, the various embodiments described above use KrF excimer laser (wavelength: 248 nm) and ArF excimer laser (wavelength: 193 nm) as exposure light with a wavelength of 180 nm or more. Therefore, the diffractive optical element can be formed of quartz glass. In addition, when using a wavelength below 200 nm as the exposure light, such as when using an h laser (wavelength: 157 nm) that supplies exposure light with a wavelength in the hollow ultraviolet region, Can also be fluorite, quartz glass doped with fluorine, quartz glass doped with fluorine and hydrogen, the specified temperature of the structure is below 12,000 k, and the OH group concentration Quartz glass above 1000ppm, structure index -30-This paper size applies Chinese National Standard (CNS) A4 specification (210X297 public love) 497149 A7 B7 V. Description of the invention (28) The fixed temperature is below 1200 K, Quartz glass with a hydrogen molecule concentration of 1 X 1017 molecules / cm3 or more, a quartz glass with a structure designation temperature of 1200 K or less and a chlorine concentration of 50 ppm or less, and a structure designation temperature of 1200 K or less, and a hydrogen molecule concentration of 1 Materials selected from quartz glass group with xlO17 molecules / cm3 or more and chlorine concentration below 50 ppm to form diffractive optical elements. In addition, as for the quartz glass with a specified structure temperature of 1200 K or less and an OH group concentration of 1,000 ppm or more, as disclosed by the applicant of this patent in Japanese Patent No. 2770224, the specified temperature of the structure is 1200 K or less, and hydrogen Quartz glass with a molecular concentration of 1 X 1017 molecules / cm3 or more, quartz glass with a structural designation temperature of 1200 K or less and a gas concentration of 50 ppm or less, and a structural designation temperature of 1200 K or less with a hydrogen molecular concentration of 1 X 1 Quartz glass above 0 17 molecules / cm3 and chlorine concentration below 50 ppm is disclosed in Japanese Patent No. 293613 8 by the applicant of this patent. As described above, the illumination optical device according to various embodiments of the present invention can effectively suppress the loss of the light amount of the aperture stop caused by the limitation of the secondary light source, and perform deformed illumination such as bipolar illumination and general circular illumination. Therefore, the specified focal depth can be ensured, and the projection optical system can improve the resolution of a specific pattern shape. In addition, by changing the magnification of the continuous zoom lens and the simple operation of changing the focal distance of the zoom lens, it is possible to effectively suppress the light amount loss of the aperture diaphragm and change the parameters of the distortion illumination. Therefore, by installing the exposure device of the illumination optical device of various embodiments of the present invention, the types and parameters of the anamorphic illumination are appropriately changed to obtain the suitable requirements. -31-This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297) (Mm)

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497149 A7 B7 五、發明説明(29 要曝光投影之微細圖案之投影光學系統的解像度及焦點深 度。因而可依據高度曝光亮度及良好的曝光條件進行通量 高的良好投影曝光。此外,使用本發明之照明光學裝置, 將配置在被照射面上之掩膜圖案曝光在感光性基板上的曝 光方法,可依據良好之曝光條件進行投影曝光,因此可製 造良好的微型裝置。 -32- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)497149 A7 B7 V. Explanation of the invention (29 Resolution and focal depth of the projection optical system for exposing the fine pattern of the projection. Therefore, a good projection exposure with high flux can be performed according to the high exposure brightness and good exposure conditions. In addition, the invention is used For the illumination optical device, an exposure method in which a mask pattern arranged on an illuminated surface is exposed on a photosensitive substrate can perform projection exposure according to good exposure conditions, so that a good micro device can be manufactured. -32- This paper size Applicable to China National Standard (CNS) A4 (210 X 297 mm)

Claims (1)

497149497149 1. 一種照明光學裝置,其係用於照明掩膜,並使用在投影 曝光裝置上,經由投影光學系統,將上述掩膜上之圖案 圖像複製到基板上, 其特徵爲具有:光源機構,其係用於供應曝光波長的 光束; 二次光源形成機構,其係用於依據上述光源機構射出 之光束’在與上述投影光學系統之瞳孔共軛的照明瞳孔 内’形成對基準光軸概略對稱性偏移的兩個面光源;及 變焦光學系統,其係_用於連續改變上述兩個面光源距 上述基準光軸的距離、上述兩個面光源之各個大小及自 上述基準光軸估計上述兩個面光源之角度的方位角。 2 ·如申請專利範圍第1項之照明光學裝置,其中上述變焦 光學系統具備兩個變焦光學系統。 3 ·如申請專利範圍第2項之照明光學裝置,其中上述二次 光源形成機構具備光束轉換元件,其係用於將射入光束 轉換成兩個光束。 4 ·如申請專利範圍第3項之照明光學裝置,其中上述光束 轉換元件可與其他光束轉換元件交換。 5 .如申請專利範圍第i項之照明光學裝置,其中上述二次 光源形成機構具備: 角度光束形成機構,其係用於將自上述光源機構射出 之光束、轉換成對基準光轴具有各種角度成分的光束,射 入第一指定面; 、 照射區域形成機構,其係用於依據具有射入上述第一- -33- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公董) 4971491. An illumination optical device, which is used to illuminate a mask and is used on a projection exposure device to copy a pattern image on the mask onto a substrate via a projection optical system, which is characterized by having a light source mechanism, It is used to supply a light beam with an exposure wavelength; a secondary light source forming mechanism is used to form a roughly symmetrical reference optical axis based on the light beam emitted by the light source mechanism 'in an illumination pupil conjugated with the pupil of the above-mentioned projection optical system' Two surface light sources that are shifted in a linear manner; and a zoom optical system for continuously changing the distance between the two surface light sources from the reference optical axis, the respective sizes of the two surface light sources, and estimating the above from the reference optical axis The azimuth of the angle of the two area light sources. 2 · The illumination optical device according to item 1 of the patent application range, wherein the above-mentioned zoom optical system is provided with two zoom optical systems. 3. The illumination optical device according to item 2 of the patent application, wherein the above-mentioned secondary light source forming mechanism is provided with a light beam conversion element for converting an incident light beam into two light beams. 4 · The illumination optical device according to item 3 of the patent application, wherein the above-mentioned beam conversion element can be exchanged with other beam conversion elements. 5. The illumination optical device according to item i of the patent application scope, wherein the secondary light source forming mechanism includes: an angle beam forming mechanism for converting a light beam emitted from the light source mechanism into various angles with respect to the reference optical axis The component beam is incident on the first designated surface; and the irradiation area forming mechanism is used to comply with the above-mentioned first--33- This paper size is applicable to the Chinese National Standard (CNS) A4 specification (210 X 297) ) 497149 指定面之上述各種角度成分的光束,將對基準光軸概略 對稱性偏移的兩個照射區域形成在第二指定面上;及 光子積刀器’其係用於依據形成在上述第二指定面上 之上述兩個照射區域射出的光束,形成具有與上述兩個 照射區域概略相同光度分布的兩極狀二次光源; 還具備導光光學系統,其係用於將上述光學積分器射 出之光束導向上述被照射面。 6 ·如申請|利範圍第5項之照明光學裝置,其中上述角度 光束形成機構具有:散射光束形成元件,其係用於將上 述光源機構射出之概略平行的光束轉換成對上述基準光 軸以各種角度散射的光束;及第一光學系統,其係用於 將藉由上述散射光束形成元件所形成的教射光束予以聚 光,射入上述第一指定面。 7 .如申請專利範圍第6項之照明光學裝置,其中上述第一 光學系統具有第一變焦光學系統,其係不使形成爲上述 二次光源之數個面光源的中心高度改變,而使其寬度改 變, 該第一變焦光學系統構成上述變焦光學系統的至少一 部分。 8 .如申請專利範圍第7項之照明光學装置’其中上述散射 光束形成元件具有光學元件陣列,其具有排列成平面狀 的數個、單位光學元件, -上述第一變焦光學系統具有連續變焦透鏡’其係將上 述光學元件陣列形成之上述光源機構射出之光束的數個 -34- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 497149The light beams of the above-mentioned various angle components on the designated surface form two irradiation areas that are roughly symmetrically offset from the reference optical axis on the second designated surface; and a photon accumulator is used to form the second designated The light beams emitted from the two irradiated areas on the surface form a bipolar secondary light source having approximately the same light distribution as the two irradiated areas; and a light guide optical system for emitting the light from the optical integrator. Guide to the illuminated surface. 6 · The illumination optical device according to item 5 of the application, wherein the angle beam forming mechanism has a scattered beam forming element for converting a substantially parallel light beam emitted by the light source mechanism into a reference beam axis. Light beams scattered at various angles; and a first optical system for condensing a teaching light beam formed by the scattered light beam forming element and incident on the first designated surface. 7. The illumination optical device according to item 6 of the patent application, wherein the first optical system has a first zoom optical system, which does not change the center heights of the surface light sources formed as the secondary light sources, so that The width is changed, and the first zoom optical system constitutes at least a part of the above-mentioned zoom optical system. 8. The illumination optical device according to item 7 of the scope of the patent application, wherein the scattered light beam forming element has an optical element array having a plurality of unit optical elements arranged in a flat shape,-the first zoom optical system has a continuous zoom lens 'It is the number of light beams emitted by the above-mentioned light source mechanism formed by the above-mentioned optical element array -34- This paper size applies to China National Standard (CNS) A4 specification (210 X 297 mm) 497149 聚光點與上述第一指定面連結成光學性概略共扼。 9 ·如申請專利範圍第5項之照明光學裝置,其中上述照射 區域形成機構具有光束轉換元件,其係配置在上述第一 指定面附近,用於將射入光束轉換成數個光束;及第二 光學系統,其係用於將上述光束轉換元件射出之光束導 入上述第二指定面。 10·如申請專利範圍第9項之照明光學裝置,其中上述光束 轉換元件將對上述基準光軸偏移之數個照射區域形成在 遠場上, 上述第二光學系統使形成在上述遠場的上述數個照射 區域形成在上述第二指定面上。 11. 如申請專利範圍第9項之照明光學裝置,其中上述第二 光學系統具有第二變焦光學系統,其係用於保持類似形 狀,使形成上述二次光源之數個面光源的外徑改變, 該第二變焦光學系統構成上述變焦光學系統的至少一 部分。 12. 如申請專利範圍第1 1項之照明光學裝置,其中上述光束 轉換元件具有繞射光學元件,其構造爲對照明光程可任 意拆裝’且繞射面被固定在上述第一指定面上, 上述第二變焦光學系統將上述繞射光學元件的繞射面 與上述第二指定面連結成實質上之傅里葉轉換的關係。 13. 如申请、專利範圍第i項之照明光學裝置,其中上述二次 光源形成機構具備: 光束形狀轉換機構,其係用於將上述光源機構射出之 -35-The light-condensing point is connected to the first predetermined surface to form a general optical conjugate. 9 · The illumination optical device according to item 5 of the application, wherein the above-mentioned irradiation area forming mechanism has a light beam conversion element which is arranged near the first designated surface for converting the incident light beam into several light beams; and the second The optical system is configured to guide a light beam emitted from the light beam conversion element to the second designated surface. 10. The illumination optical device according to item 9 of the scope of patent application, wherein the light beam conversion element forms a plurality of irradiated areas offset from the reference optical axis in the far field, and the second optical system makes the light field formed in the far field The plurality of irradiation areas are formed on the second designated surface. 11. The illumination optical device according to item 9 of the application, wherein the second optical system has a second zoom optical system, which is used to maintain a similar shape and change the outer diameter of the surface light sources forming the secondary light source. The second zoom optical system constitutes at least a part of the zoom optical system. 12. For the illumination optical device according to item 11 of the scope of patent application, wherein the above-mentioned beam conversion element has a diffractive optical element, which is configured to be detachable to the illumination optical path 'and the diffractive surface is fixed on the first specified surface The second zoom optical system connects the diffraction surface of the diffractive optical element and the second designated surface into a substantially Fourier transform relationship. 13. For example, the illumination optical device according to item i of the patent scope, wherein the secondary light source forming mechanism includes: a beam shape conversion mechanism for emitting the light source mechanism described above -35- 光束轉換成對基準光軸偏移的兩個光束,上述兩個光束 射出的光線自對上述基準光軸傾斜的方向射入第一指定 面; 照射區域形成機構,其係用於依據射入上述第一指定 面之上述傾斜方向的光束,將對上述基準光軸概略對稱 性偏移的兩個照射區域形成在第二指定面上;及 光學積分器,其係用於依據形成在上述第二指定面上 ,上述兩個照射區域射出的光束,形成具有與上述兩個 照射區域概等之光度分布的兩極狀二次光源, 還具備導光光學系統,其係用於將上述光學積分器射 出之光束導入上述掩膜。 14·如申請專利範圍第1 3項之照明光學裝置,其中上述光束 形狀轉換機構具有:光束轉換元件,其係用於將上述光 源機構射出之概略平行的光束轉換成數個光束;及第三 光學系統,其係用於將上述光束轉換元件射出之光束導 入上述第一指定面。 15.如申請專利範圍第1 4項之照明光學裝置,其中上述光束 轉換元件將對上述基準光軸偏移之數個光束形成在遠 場, 上述第三光學系統使形成在上述遠場之上述數個光束 形成在該瞳孔面上。 16·如申請、專利範圍第丨4項之照明光學裝置,其中上述第三 光學系統具有第三變焦光學系統,其係用於不使形成上 述一’人光源之數個面光源的中心高度改變,而使其寬度 -36- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公董) A B c D 497149 々、申請專利範圍 改變, .該第三變焦光學系統構成上述變焦光學系統的至少一 部分。 17. 如申請專利範圍第1 6項之照明光學裝置,其中上述光束 轉換元件具有繞射光學元件,其構造對照明光程可任意 拆裝, 上述第三變焦光學系統具有連續變焦透鏡,其係將上 述繞射羌學元件之繞射面與上述第一指定面連結成光學 性概略共軛。 18. 如申請專利範圍第1 3項之照明光學裝置,其中上述照射 區域形成機構具有:波面分割元件,其係用於波面分割 射入上述第一指定面的光束,形成許多光源;及第四光 學系統,其係用於將藉由上述波面分割元件所形成之許 多光源射出的散射光束予以聚光,並導入上述第二指定 面。 19. 如申請專利範圍第1 8項之照明光學裝置,其中上述第四 光學系統具有第四變焦光學系統,其係用於保持類似形 狀,使形成上述二次光源之數個面光源的外徑改變, 該第四變焦光學系統構成上述變焦光學系統的至少一 部分。 20. 如申請專利範圍第1 9項之照明光學裝置,其中上述波面 分割元件之射入面配置在上述第一指定面附近,且具有 光學元件陣列,其係具有排列成平面狀的數個單位光學 元件, -37- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)The light beam is converted into two light beams which are offset from the reference optical axis, and the light rays emitted by the two light beams are incident on the first designated surface from a direction inclined to the reference optical axis; The light beam in the oblique direction on the first designated surface forms two irradiation areas that are roughly symmetrically offset from the reference optical axis on the second designated surface; and an optical integrator for forming on the second designated surface according to The light beams emitted from the two irradiated areas on the designated surface form a bipolar secondary light source having a light distribution similar to that of the two irradiated areas, and further include a light guide optical system for emitting the optical integrator. The light beam is guided into the above mask. 14. The illumination optical device according to item 13 of the scope of patent application, wherein the beam shape conversion mechanism has: a beam conversion element for converting roughly parallel light beams emitted by the light source mechanism into a plurality of light beams; and third optical A system for guiding a light beam emitted from the light beam conversion element to the first designated surface. 15. The illumination optical device according to item 14 of the scope of patent application, wherein the light beam conversion element forms a plurality of light beams shifted from the reference optical axis in a far field, and the third optical system causes the light beam formed in the far field to be formed. Several light beams are formed on the pupil surface. 16. According to the application, the illumination optical device according to item 4 of the patent, wherein the third optical system has a third zoom optical system, which is used to not change the center heights of the surface light sources forming the one human light source. The width of this paper is -36- This paper size is in accordance with Chinese National Standard (CNS) A4 (210 X 297 public directors) AB c D 497149 々 The scope of patent application is changed. The third zoom optical system constitutes the above-mentioned zoom optical system At least part of it. 17. For the illumination optical device according to item 16 of the patent application, wherein the above-mentioned beam conversion element has a diffractive optical element, and its structure can be arbitrarily detached and attached to the illumination optical path, and the third zoom optical system has a continuous zoom lens, The diffractive surface of the diffractive magnetic element is connected to the first predetermined surface to form an optically rough conjugate. 18. The illuminating optical device according to item 13 of the scope of patent application, wherein the above-mentioned irradiation area forming mechanism has: a wavefront division element for wavefront division of the light beam incident on the first specified surface to form a plurality of light sources; and a fourth An optical system is used for condensing the scattered light beams emitted from a plurality of light sources formed by the wave surface division element and introducing the scattered light beams into the second specified surface. 19. The illumination optical device according to item 18 of the scope of patent application, wherein the fourth optical system has a fourth zoom optical system, which is used to maintain a similar shape so that the outer diameters of the surface light sources forming the secondary light source described above Alternatively, the fourth zoom optical system constitutes at least a part of the above-mentioned zoom optical system. 20. The illumination optical device according to item 19 of the scope of patent application, in which the incident surface of the wave-surface dividing element is arranged near the first specified surface and has an optical element array having a plurality of units arranged in a flat shape. Optical components, -37- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm) 497149 8 8 8 8 A B c D 六、申請專利範圍 上述第四變焦光學系統將上述光學元件陣列之上述射 入面與上述第二指定面連結成光學性概略共軛的關係。 21. —種曝光裝置,其特徵爲具備:申請專利範圍第1至2 0 項中任一項之照明光學裝置;及投影光學系統,其係將 設定在上述被照射面之掩膜圖案投影曝光在感光性基板 上。 22. —種微型裝置的製造方法,其特徵爲包含:曝光步驟, 其係藉南申請專利範圍第2 1項之曝光裝置,將上述掩膜 圖案曝光在上述感光性基板上;及顯像步驟,其係將上 述曝光步驟所曝光之上述感光性基板予以顯像。 -38- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)497149 8 8 8 8 A B c D 6. Scope of patent application The fourth zoom optical system connects the above-mentioned incident surface of the above-mentioned optical element array and the above-mentioned second specified surface into an optically roughly conjugated relationship. 21. An exposure device comprising: an illumination optical device according to any one of claims 1 to 20 of a patent application scope; and a projection optical system for projecting and exposing a mask pattern set on the surface to be irradiated On a photosensitive substrate. 22. A method for manufacturing a micro device, comprising: an exposure step for exposing the mask pattern on the photosensitive substrate by using the exposure device of the Nanning Patent Application No. 21; and an imaging step; It develops the photosensitive substrate exposed by the exposure step. -38- This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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