TW200405426A - Diffractive optical device, illuminating optical apparatus, exposure apparatus and exposure method - Google Patents

Diffractive optical device, illuminating optical apparatus, exposure apparatus and exposure method Download PDF

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Publication number
TW200405426A
TW200405426A TW92120383A TW92120383A TW200405426A TW 200405426 A TW200405426 A TW 200405426A TW 92120383 A TW92120383 A TW 92120383A TW 92120383 A TW92120383 A TW 92120383A TW 200405426 A TW200405426 A TW 200405426A
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Taiwan
Prior art keywords
diffractive optical
optical element
basic
complementary
light
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TW92120383A
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Chinese (zh)
Inventor
Akihiro Goto
Naonori Kita
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Nippon Kogaku Kk
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Publication of TW200405426A publication Critical patent/TW200405426A/en

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    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70058Mask illumination systems
    • G03F7/70091Illumination settings, i.e. intensity distribution in the pupil plane or angular distribution in the field plane; On-axis or off-axis settings, e.g. annular, dipole or quadrupole settings; Partial coherence control, i.e. sigma or numerical aperture [NA]
    • G03F7/70108Off-axis setting using a light-guiding element, e.g. diffractive optical elements [DOEs] or light guides
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0927Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0938Using specific optical elements
    • G02B27/0944Diffractive optical elements, e.g. gratings, holograms
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/42Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect
    • G02B27/4233Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having a diffractive element [DOE] contributing to a non-imaging application
    • G02B27/425Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having a diffractive element [DOE] contributing to a non-imaging application in illumination systems
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings
    • G02B5/1814Diffraction gratings structurally combined with one or more further optical elements, e.g. lenses, mirrors, prisms or other diffraction gratings
    • G02B5/1819Plural gratings positioned on the same surface, e.g. array of gratings
    • 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
    • G03F7/7015Details of optical elements
    • G03F7/70158Diffractive optical elements

Abstract

The present invention is related to a kind of illuminating optical apparatus, which is used to illuminate papillary face to form a substantially uniform four-pole shape diffractive optical device such that it is capable of suppressing optical loss when conducting excellent four-pole illumination. The present invention is related to the illumination apparatus used for illuminating the illuminated faces (13, 15). In order to form the secondary light source having four-pole shape light intensity distribution on the illuminating light papillary face, a diffractive optical device (61) used for converting the incident light into four light beams is provided. In the diffractive optical device, the same numbers of the first basic diffractive optical device, the second basic diffractive optical device, the first compensative optical device, and the second compensative optical device are closely arranged.

Description

200405426 玫、發明說明: 【發明所屬之技術領域】 本發明,係關於繞射光學元件、照明光學裝置、曝光裝 置及曝光方法’尤其是關於非㈣合用於以微影製程製造半導體 元件、攝影元件、液晶顯示元件、薄膜磁頭等微元件之曝光裝置 的照明光學元件。 【先前技術】 典型的此種曝光裝置,從光源射出之光束係射入複眼 透鏡,在其後側焦點面形成由多數個光源像構成的二次光 源。來自二次光源之光束,透過孔徑光閑(配置在複眼透 鏡之後側焦點面附近)加以限難,射人聚焦透鏡。孔_ 光闌根期望之照明條件(曝光條件),將二次光源之形㈣ 大小限制成期望之形狀或大小。 被聚焦透鏡聚光之光束,重疊照明形成有既定圖案之 光罩。透射過光罩圖案之光,透過投影光學系統成像在晶 圓上。如此,在晶圓上投影曝光(轉印)出光罩圖案。又, 形成在光罩之圖案被高積體化,為將此微細圖案正確的轉 的孔徑部(光透射部)之大小’來變化以複眼透鏡形成 近年來,藉由改變複眼透鏡射出側所配置之孔徑光爲 次光源之大小,以變化照明之相干#童 诉数σ (σ值=孔徑光 闌直徑/投影光學系統之光瞳面直徑 或σ值=照明光學 200405426 系統射出側孔徑數/投影光學系統入射側孔徑數)的技術 文到到各界注目。此外,將複眼透鏡射出側所配置之孔徑 光闌的孔徑部形狀設定成環帶狀、或4孔狀(即4極狀), 來將以複眼透鏡形成之二次光源形狀限制成4極狀,以提 昇投影光學系統之焦點深度及解析力之技術亦受到各界注 目° 如前所述,習知技術,係將二次光源之形狀限制成環 帶狀或4極狀來進行變形照明(環帶照明或4極照明),因 :係將來自以複眼透鏡形成之二次光源之光束,以具有環 帶狀或4極狀孔徑部之孔徑光闌來加以限制。換言之,習 知技術之環帶照明A 4極照明中,來自二次光源之光束的 相當部分被孔徑光闌遮蔽,對照明(曝光)無任何助益。其 結果,因孔徑光闌之光量損《,而使得在光罩及晶圓上之 照度低,導致曝光裝置之效率亦低。 本毛明有鑑於上述情事’其目的在提供一種繞射光与 元件’例如係用於照明光學裝置,能在照明光瞳面形成, 質上均一之4極狀的照度分佈等。又,本發明之另… ’係提供一種照明来璺梦罢 ^ ^ 一 裡'、、、月九子裝置’其係使用能在照明光曈面开 成貫貝上均 一之 4極狀夕\ ι 另之…、度刀佈等的繞射光學元件,名 抑制光量損失之同時,亦能良 月b艮好進仃4極照明等多極照明 。此外,本發明之爯—θ Μ ^ " 旦 _ 、,係提供一種使用能在抑制矢 里損失之同時,亦能自杯;隹/ 光與梦罟..^ 丁極照明等多極照明的照明 光予’置’在光罩之最佳昭明 錢b , 、、月條件下’將光罩圖案忠實的 轉㉟先性基板上的曝光裝置以及曝光方法。 200405426 【發明内容】 為解決前述課題,本案第1發明提供一種繞射光學元 件’其特徵在於,具備: 第1基本繞射光學元件,其具有沿第1方向之直線光 栅圖案; 第2基本繞射光學元件,其具有沿不同於前述第1方 向之第2方向之直線光栅圖案; 第1補全繞射光學元件,其對前述第丨基本繞射光學 元件所產生之光振幅,具有產生具第丨相位差之光振幅的 圖案;以及 第2補全繞射光學元件,其對前述第2基本繞射光學 件所產生之光振幅,具有產生具第2相位差之光振幅的 圖案; 如述第1基本繞射光學元件、前述第2 :件、前述第1補全繞射光學元件與前述第 學元件,係大致緊密排列。 本案第2發明提供一種繞射光學元 旲備: 基本繞射光學 2補全繞射光 其特徵在於, 撫闻第1基本繞射光學元件’其具有沿第1方向之直線光 撕圖案; 6第2基本繞射光學元件,其具有沿不同於前述第1方 向之第2方向之直線光柵圖案;以及 單純透射部’係實質上無偏向作用者; 200405426 前述第1基本繞射光學元件、前述第2基本繞射光學 兀件與前述單純透射部係大致緊密排列。 本案第3發明提供一種照明光學裝置,係用來照明被 照射面,其特徵在於: 為了在照明光瞳面形成具有4極狀強度分佈的二次光 源’具備用來將入射光束轉換為4個光束之第1發明的繞 射光學元件。 本案第4發明係提供一種照明光學裝置,其特徵在於 ,具備: 光源機構,係用來供應光束; 角度光束形成機構,係將來自前述光源裝置之光束轉 換成具有相對光軸之各種角度成份的光束,以射入第1既 定面; 照野形成機構,其包含繞射光學元件,以根據射入前 述第1既定面之前述具有各種角度成份的光束,而在第2 既定面上形成4極狀之照野; 光學積分器,係根據來自前述第2既定面上所形成之 前述4極狀照野的光束,來形成具有與前述4極狀照野大 致相同光強度分佈的4極狀二次光源;以及 導光光學系統,係用來將來自前述光學積分器之光束 導向被照射面; 前述繞射光學元件,具備複數個第1基本繞射光學元 件與複數個第2基本繞射光學元件,該第1基本繞射光學 元件具有沿第1方向的直線光柵,而該第2基本繞射光學 200405426 :件具有沿不同於前述第i方向之第2方向的直線光柵, 則述複數個第1基本繞射光學元件與前述複數個第2基本 繞射光學元件,係大致緊密排列。 本案第5發明提供一種照明光學裝置,係用來照明被 照射面,其特徵在於: 為了在照明光瞳面形成具有2極狀強度分佈之二次光 源,具備用來將入射光束轉換為2個光束的繞射光學元件 , 則述繞射光學元件,具有沿既定方向之直線光栅圖案 勺複數個基本繞射光學元件,與對前述基本繞射光學元件 所產生之光振幅,具有產生具既定相位差之光振幅之圖案 的複數個補全繞射光學元件; · 則述複數個基本繞射光學元件與前述複數個補全繞射 光學元件,係大致緊密排列。 本案第6發明提供一種照明光學裝置,係用來照明被 照射面,其特徵在於: 為了在照明光瞳面形成具有3極狀強度分佈之二次光 源,具備用來將入射光束轉換為3個光束的繞射光學元件 刖述繞射光學元件,具有沿既定方向之直線光栅圖案 的複數個基本繞射光學元件,與實質上無偏向作用的複數 個單純透射部; 刚述複數個基本繞射光學元件與前述複數個單純透射 部,係大致緊密排列。 200405426 本案第7發明提供一種照明光學裝置,係用來照明被 照射面,其特徵在於: 為了在照明光瞳面形成具有8極狀強度分佈的二次光 源,具備用來將入射光束轉換為8個光束的繞射光學元件 前述繞射光學元件,具備: 第1基本繞射光學元件,其具有沿第丨方向之直線光 栅圖案; 第 栅圖案 第 柵圖案 第 栅圖案 2基本繞射光學元件,其具有沿第2方向之直線光 則述第2方向與前述第1方向大致正交; 3基本繞射光學元件,其具有沿第3方向之直線光 月’J述第3方向與前述第1方向大致成45度;以及 4基本繞射光學元件,其具有沿第4方向之直線光 ,刖述第4方向與前述第】方向大致成45度、且與 前述第3方向大致正交; 述第1第4基本繞射光學元件係大致緊密排列。 :案帛8發明提供一種照明光學裝置,係用來照明被 …射面,其特徵在於,具備: 光源機構,係用來供應光束; 換成具有相對光:機構,係將來述光源裝置之光束轉 定面;以及 <各種角度成份的光束’以射入第1既 ’系野形成機構’其包含繞射光學 述第1既宁品> 1 以根據射入前 則述具有各種角度成份的光束,在第2既 200405426 疋面上形成複數極狀之照野; 前述繞射光學元件,係將具有既定繞射光學元件圖案 之複數個基本繞射光學元件予以緊密排列而構成; 刚述角度光束形成機構,具有由複數個光學元件構成 之光學構件; 刚述繞射光學元件,係被定位成對應前述光學構件之 各光學元件的要素光束中,合計包含4個以上之基本繞射 光學元件或補全繞射光學元件。 本案第9發明係提供一種照明光學裝置,其特徵在於(_ ,具備: 光源機構,係用來供應光束; 角度光束形成機構,係將來自前述光源裝置之光束轉 換成具有相對光軸之各種角度成份的光束,以射入第丨既 定面;200405426 Description of the invention: [Technical field to which the invention belongs] The present invention relates to a diffractive optical element, an illumination optical device, an exposure device, and an exposure method ', and more particularly to a non-coupling method for manufacturing a semiconductor device and a photographic device by a lithography process. Optical elements for exposure devices of micro-elements such as liquid crystal display elements, thin-film magnetic heads, etc. [Prior art] In a typical exposure device of this type, a light beam emitted from a light source is incident on a fly-eye lens, and a secondary light source composed of a plurality of light source images is formed on a rear focal plane. The light beam from the secondary light source passes through the aperture light (located near the focal plane behind the fly-eye lens) to limit the difficulty and hit the focusing lens. Hole_ The desired lighting conditions (exposure conditions) of the diaphragm root limit the size of the secondary light source to the desired shape or size. The light beam focused by the focused lens is superimposed to form a mask with a predetermined pattern. The light transmitted through the mask pattern is imaged on the wafer by the projection optical system. In this way, a mask pattern is projected and exposed (transferred) on the wafer. In addition, the pattern formed on the photomask is highly integrated, and the size of the aperture portion (light transmitting portion) for correct rotation of the fine pattern is changed to form a fly-eye lens. In recent years, the fly-eye lens has been changed by changing the position of the fly-eye lens. The configured aperture light is the size of the secondary light source, in order to change the coherence of the illumination. # 童 告 数 σ (σ value = aperture diaphragm diameter / pupil plane diameter of the projection optical system or σ value = illumination optics 200405426 system exit side aperture number / The number of apertures on the incident side of the projection optical system has attracted attention from all walks of life. In addition, the shape of the aperture portion of the aperture stop arranged on the exit side of the fly-eye lens is set to be a ring shape or a 4-hole shape (that is, a 4-pole shape) to limit the shape of the secondary light source formed by the fly-eye lens to a 4-pole shape The technology to improve the depth of focus and resolution of the projection optical system has also attracted attention from all walks of life. As mentioned earlier, the conventional technology is to limit the shape of the secondary light source to the shape of an endless belt or a 4-pole to deform the illumination (ring (With illumination or 4-pole illumination), because the beam from the secondary light source formed by the fly-eye lens is restricted by an aperture stop with an annular zone or a 4-pole aperture. In other words, in the circular lighting A 4 pole lighting of the conventional technology, a considerable portion of the light beam from the secondary light source is blocked by the aperture stop, which does not contribute to the illumination (exposure). As a result, the light amount of the aperture stop is reduced, resulting in low illuminance on the reticle and wafer, resulting in low efficiency of the exposure device. In view of the above-mentioned circumstances, Ben Maoming aims to provide a diffracted light and element, for example, which is used for illumination optical devices, can be formed on the illumination pupil surface, and has a uniform 4-pole illuminance distribution in quality. In addition, another aspect of the present invention ... 'provides a kind of lighting to dream ^ ^ one mile' ,,, and moon nine sub-devices' which uses a uniform 4-pole-shaped eve on the light surface of the lighting \ ι In addition, the diffractive optical elements such as ..., dagger cloth, etc., while suppressing the loss of light quantity, can also be used for multi-pole lighting such as 4-pole lighting. In addition, the 爯 —θ Μ ^ " once in the present invention, provides a method that can suppress the loss of the sagittal and also can self-cup; 杯 / light and nightmare .. ^ multi-pole lighting such as Dingji lighting Under the conditions of the best light source of the mask, the exposure light and the exposure device and method for faithfully turning the mask pattern on the aforesaid substrate are provided. 200405426 [Summary of the Invention] In order to solve the foregoing problem, the first invention of the present invention provides a diffractive optical element, which includes: a first basic diffractive optical element having a linear grating pattern along a first direction; and a second basic diffractive optical element. The diffractive optical element has a linear grating pattern along a second direction different from the first direction. The first complementary diffractive optical element has a light amplitude to the light amplitude generated by the first basic diffractive optical element. A pattern of the light amplitude of the second phase difference; and a second complementary diffractive optical element having a pattern of generating the light amplitude of the second phase difference from the light amplitude generated by the second basic diffractive optical element; The first basic diffractive optical element, the second component, the first complementary diffractive optical element, and the first element are substantially closely aligned. The second invention of this case provides a diffractive optical element preparation: the basic diffractive optics 2 complements the diffracted light, and is characterized in that the first basic diffractive optical element 'features a linear light tearing pattern along the first direction; 2 A basic diffractive optical element having a linear grating pattern in a second direction different from the first direction; and a simple transmission portion is a person having substantially no deflection; 200405426 The first basic diffractive optical element, the first 2 The basic diffractive optical element is arranged approximately closely with the aforementioned simple transmission system. The third invention of the present invention provides an illumination optical device for illuminating the illuminated surface, which is characterized in that: in order to form a secondary light source having a quadrupole intensity distribution on the illumination pupil surface, the device is provided for converting incident light beams into four The diffractive optical element of the first invention of the light beam. The fourth invention of the present case is to provide an illumination optical device, comprising: a light source mechanism for supplying a light beam; and an angular beam forming mechanism for converting a light beam from the light source device into various angle components with respect to an optical axis. The light beam is incident on the first predetermined surface; the light field forming mechanism includes a diffractive optical element to form four poles on the second predetermined surface according to the aforementioned light beam having various angular components incident on the first predetermined surface. An optical integrator, based on the light beam from the aforementioned 4-pole illumination field formed on the second predetermined surface, to form a 4-pole II having a light intensity distribution substantially the same as that of the aforementioned 4-pole illumination field A secondary light source; and a light-guiding optical system for guiding a light beam from the optical integrator to the illuminated surface; the diffractive optical element includes a plurality of first basic diffractive optical elements and a plurality of second basic diffractive optical elements; Element, the first basic diffractive optical element has a linear grating in a first direction, and the second basic diffractive optical element 200405426 has a For the linear gratings in the second direction, the plurality of first basic diffractive optical elements and the plurality of second basic diffractive optical elements are arranged closely together. The fifth invention of the present invention provides an illumination optical device for illuminating the illuminated surface, which is characterized in that: in order to form a secondary light source having a bipolar intensity distribution on the illumination pupil surface, the method is provided for converting the incident light beam into two A diffractive optical element of a light beam, the diffractive optical element has a plurality of basic diffractive optical elements with a linear grating pattern along a predetermined direction, and the light amplitude generated by the basic diffractive optical element has a predetermined phase. The plurality of complementary diffractive optical elements of the pattern of the difference light amplitude are described. The plurality of basic diffractive optical elements and the aforementioned plurality of complementary diffractive optical elements are arranged approximately closely. The sixth invention of the present invention provides an illumination optical device for illuminating the irradiated surface, which is characterized in that: in order to form a secondary light source with a three-pole intensity distribution on the illumination pupil surface, it is provided to convert the incident light beam into three A diffractive optical element of a light beam describes a diffractive optical element having a plurality of basic diffractive optical elements having a linear grating pattern along a predetermined direction, and a plurality of simple transmission portions having substantially no deflection effect; the plurality of basic diffractions just described The optical elements are arranged approximately closely to the plurality of simple transmission portions. 200405426 The seventh invention of the present invention provides an illumination optical device for illuminating the illuminated surface, which is characterized in that: in order to form a secondary light source with an 8-pole intensity distribution on the illumination pupil surface, the method is provided for converting the incident light beam into 8 The above-mentioned diffractive optical element of each light beam includes: a first basic diffractive optical element having a linear grating pattern along the first direction; a second grid pattern, a second grid pattern, and a second grid optical element, It has linear light along the second direction, and the second direction is substantially orthogonal to the first direction. 3 Basic diffractive optical element, which has a straight line of light along the third direction. The third direction is the first direction. Approximately 45 degrees; and 4 basic diffractive optical elements having linear light along a fourth direction, the fourth direction is substantially 45 degrees to the first direction, and is substantially orthogonal to the third direction; The first and fourth basic diffractive optical elements are arranged approximately closely. The invention of case 8 provides an illumination optical device for illuminating the illuminated surface, which is characterized by having: a light source mechanism for supplying a light beam; a light source mechanism having a relative light: mechanism for a light beam of a light source device described below The plane of conversion; and < the light beam of various angle components' is incident on the first both 'system forming mechanism', which contains diffractive optics, and the first conventional product > The beam of light forms a complex polar field on the second surface of 200405426; the aforementioned diffractive optical element is formed by closely arraying a plurality of basic diffractive optical elements with a predetermined pattern of diffractive optical elements; just described The angle beam forming mechanism has an optical member composed of a plurality of optical elements; the diffractive optical element just described is a beam of elements that is positioned to correspond to each of the optical elements of the aforementioned optical member, and includes a total of 4 or more basic diffraction optics Element or complementary diffractive optical element. The ninth invention of this case is to provide an illumination optical device, characterized by (_, having: a light source mechanism for supplying a light beam; an angular beam forming mechanism for converting a light beam from the light source device into various angles with respect to an optical axis A component beam to be incident on the first predetermined surface;

照野形成機構,其包含繞射光學元件,以根據射入前 述第1既定面之前述具有各種角度成份的光束,而在第2 既定面上形成複數極狀之照野; 光學積分器,係根據來自前述第2既定面上所形成之 前述複數極狀照野的光束,來形成具有與前述複數極狀照 野大致相同光強度分佈的複數極狀二次光源;以及 導光光學系統,係用來將來自前述光學積分器之光束 導向被照射面; 前述繞射光學元件,係將具有大致正方形外形、且具 有既定繞射光學元件圖案之複數個基本繞射光學元件予以 12 緊密排列而構成; 前述照野形成機構,具有配置在前述繞射光學元件盘 前述光學積分器間之光程中的光學系統; 〃 义設構成前述複數極狀二次光源之各面光源的大小為必 月'J述基本繞射光學元件一邊的長度為L、光束之中心波 長為;I、前述光學系統之焦距為f時,滿足以下條件 L> 2· 5xf X λ / 0。 .本案第10發明係提供一種折射光學元件,其特徵在於 其產生與第1發明或第2發明之繞射光學元件、或第 5發明或帛6發明之照明光學裝置中之繞射光學元件大致 相同的光振幅。 本案第11發明係提供一種照明光學裝置,係帛來照明 被照射面,其特徵在於: 為了在照明光瞳面形成具有既定強度分佈的二次光源 /、備用來將入射光束轉換既定截面形狀之光束之第10發 明之繞射光學元件。 义 本案第12發明提供一種曝光裝置,其特徵在於,具備 第3、9發明或第丨丨發明之照明光學裝置·,以及 杈〜光學系統,係用來將配置在前述被照射面之光罩 之圖案投影曝光至感光性基板。 本案第13發明係提供一種曝光方法,其特徵在於: 係透過第3〜9發明或第11發明之照明光學裝置來照 13 200405426 明光罩,將被照明之前述光罩上形成之圖案之像投影曝光 至感光性基板上。 【實施方式】 根據所附圖式說本發明之實施形態。第丨圖,係概略 顯示具備本發明各實施形態之照明光學裝置之曝光裝置之 構成的圖。圖i中’係分別設定沿感光性基板之晶圓15之 法線方向為Z軸、於晶圓15面内與第J圖紙面平行之方向 為γ軸、於晶圓15面内與第1圖紙面垂直之方向為χ軸。(籲 第1圖之曝光裝置,作為供應曝光用光(照明光)之光 源1,係使用供應193ηπι波長之光的ArF準分子雷射光源( 供應248mn波長之光的KrF準分子雷射光源)。從光源i沿 方向射出之平行光束,具有沿X方向細長延伸之矩形截 面,射入整形光學系統2。整形光學系統2,係由例如在第 1圖之紙面内具有負屈光力之透鏡與具有正屈光力之透鏡 所構成。 透過整形光學系統2,被整形成具有既定矩形截面光 束之平行光束,被f折豸3偏向至γ方向後,射入繞射光 學兀件4。一般來說,繞射光學元件係藉由在玻璃基板上 形成段差(具有曝光用光(照明光)之波長程度的節距)而構 成,具有將入射光束繞射至期望角度的作用。具體而言, 繞射光學元件4係一發散光束形成元件,其具有將射入之 矩形平行光束加以繞射,而在遠場(far field)形成圓形光 束的功能。 14 200405426 因此’透過繞射光學元件4而繞射之光击 ^ 不 入射至作 為第1變倍光學系統之無焦點變焦透鏡5, 、。 升尤曈面形 成圓形光束。來自此圓形光束之光,從無焦點變焦透鏡$ 射出,而射入複數極照明(2極照明、4極照明、8極照^月) 用之繞射光學元件6。無焦點變焦透鏡5,其能一邊維持作 為發散光束形成元件之繞射光學元件4與複數極照明用之 繞射光學元件6的光學共軛關係,一邊在既定範圍内連續 變化倍率。不過,如第丨圖所示,繞射光學元件6,係= 與繞射光學元件4光學共軛之位置些微的偏於光源側。 如此,光束從對光軸AX大致對稱之斜方向射入繞射光 學元件6。亦即,繞射光學元件4與無焦點變焦透鏡5構 成一角度光束形成機構,以將來自光源丨之光束轉換成對 光軸AX具有各種角度成份之光束,使其射入繞射光學元件 6之入射面(第丨既定面)。繞射光學元件6,其具有在射入 平行光束時,將此光束繞射而在遠場形成以光軸Αχ為中心 之多極狀光束的功能。關於繞射光學元件之詳細構成及作 用’留待後述。 透過繞射光學元件6之光束,再透過作為第2變倍光 學系統之可變焦透鏡7,照明作為光學積分器之微透鏡陣 列(或複眼透鏡)8。又,可變焦透鏡7,係將繞射光學元件 6與微透鏡陣列8之後側焦點面連結成大致光學共軛。換 吕之’可變焦透鏡7,係將繞射光學元件6與微透鏡陣列8 之入射面實質上連結成傅立業變換的關係。 因此,透過繞射光學元件6之光束,在可變焦透鏡7 200405426 之後側焦點面(進而在微透鏡陣列8之入射面),形成依據 繞射光學元件4之圓形分佈與繞射光學元件6本身之多極 點狀分佈的捲積(convolution)之光強度分佈,亦即形成以 光軸AX為中心之複數極狀照野。如前所述,繞射光學元件 6與可變焦透鏡7構成為一種照野形成機構,以根據射入 繞射光學元件6入射面(第1既定面)之具有各種角度成份 之光束’來將以光軸AX為中心之複數極狀照野形成在微透 鏡陣列8之入射面(第2既定面)上。此複數極狀照野之寬 度(外徑與内徑差的1/2),係依存於無焦點變焦透鏡5之(參 倍率而變化,其全體之大小,依存於可變焦透鏡7之焦距 而變化。 被透鏡陣列8,係由縱橫且緊密排列之多數個具有正 屈光力之微小透鏡構成的光學元件。構成微透鏡陣列8之 各微小透鏡,具有與光罩13上待形成之照野形狀(進而與 晶圓15上待形成之曝光區域的形狀)相似的矩形截面。一A light field forming mechanism includes a diffractive optical element to form a plurality of polar light fields on a second predetermined surface according to the aforementioned light beams having various angular components incident on the first predetermined surface; an optical integrator, a system Forming a complex polar secondary light source having a light intensity distribution substantially the same as that of the complex polar field according to the light beams from the complex polar field formed on the second predetermined surface; and a light-guiding optical system, It is used to guide the light beam from the optical integrator to the irradiated surface. The aforementioned diffractive optical element is formed by closely arraying a plurality of basic diffractive optical elements having a substantially square shape and a predetermined pattern of diffractive optical elements. The aforementioned field forming mechanism has an optical system arranged in the optical path between the aforementioned optical integrator of the diffractive optical element disk; 设 the size of each surface light source constituting the aforementioned plurality of polar secondary light sources is required; The length of one side of the basic diffractive optical element is L, and the center wavelength of the beam is: I. When the focal length of the optical system is f, the following Piece L > 2 · 5xf X λ / 0. The tenth invention of the present case is to provide a refractive optical element, which is characterized in that it is roughly equivalent to the diffractive optical element of the first or second invention, or the diffractive optical element of the illumination optical device of the fifth or sixth invention. Same light amplitude. The eleventh invention of the present invention is to provide an illumination optical device for illuminating the illuminated surface, which is characterized in that: in order to form a secondary light source with a predetermined intensity distribution on the illumination pupil surface, and reserve it to convert the incident beam into a predetermined cross-sectional shape The diffractive optical element of the tenth invention of the light beam. The twelfth invention of the present invention provides an exposure device, which is provided with the illumination optical device of the third, ninth, or ninth invention, and an optical system, and is a photomask arranged on the illuminated surface. The pattern is projected and exposed on a photosensitive substrate. The thirteenth invention of the present case is to provide an exposure method, characterized in that the illumination optical device of the third to ninth inventions or the eleventh invention is used to illuminate the 13 200405426 bright light mask, and project the image of the pattern formed on the illuminated light mask. Exposure to a photosensitive substrate. [Embodiment] An embodiment of the present invention will be described based on the drawings. Fig. 丨 is a diagram schematically showing the configuration of an exposure device provided with the illumination optical device according to each embodiment of the present invention. In Figure i, 'Z' is set along the normal direction of the wafer 15 of the photosensitive substrate as the Z axis, and the direction parallel to the J-th drawing plane in the plane of the wafer 15 is the γ axis, and in the plane of the wafer 15 and the first The vertical direction of the drawing surface is the χ axis. (The exposure device shown in Figure 1 is used as the light source 1 for the exposure light (illumination light). It is an ArF excimer laser light source that supplies light with a wavelength of 193 ηm (a KrF excimer laser light source that supplies light with a wavelength of 248 mn)) The parallel light beam emitted from the light source i in the direction has a rectangular cross section that extends slenderly in the X direction and enters the shaping optical system 2. The shaping optical system 2 is formed by, for example, a lens having negative refractive power on the paper surface of FIG. It is composed of a lens with positive refractive power. It passes through the shaping optical system 2 and is shaped into a parallel beam with a predetermined rectangular cross-section. After being deflected by the f-fold 3 to the γ direction, it enters the diffractive optical element 4. Generally, the The diffractive optical element is formed by forming a step on the glass substrate (having a pitch of about the wavelength of the exposure light (illumination light)), and has the function of diffracting the incident light beam to a desired angle. Specifically, the diffractive optics Element 4 is a divergent beam forming element, which has the function of diffracting an incident rectangular parallel beam and forming a circular beam in the far field. 14 2004054 26 Therefore, the light diffracted by passing through the diffractive optical element 4 is not incident on the focus-free zoom lens 5 which is the first variable magnification optical system. A circular beam is formed on the ascending surface. From this circular beam Light is emitted from the non-focusing zoom lens $, and is injected into the multiple pole illumination (2 pole illumination, 4 pole illumination, 8 pole illumination) for the diffractive optical element 6. The non-focus zoom lens 5, which can be maintained as The optical conjugate relationship between the diffractive optical element 4 of the divergent beam forming element and the diffractive optical element 6 for the complex pole illumination continuously changes the magnification within a predetermined range. However, as shown in FIG. 丨, the diffractive optical element 6 , = The position of the optical conjugate with the diffractive optical element 4 is slightly biased toward the light source side. In this way, the light beam enters the diffractive optical element 6 from an oblique direction substantially symmetrical to the optical axis AX. That is, the diffractive optical element 4 An angle beam forming mechanism is formed with the non-focus zoom lens 5 to convert the light beam from the light source 丨 into a light beam having various angular components with respect to the optical axis AX, so that it enters the incident surface (the predetermined surface of the diffractive optical element 6) ). Diffraction The optical element 6 has a function of diffracting the beam when it enters a parallel beam, and forming a multipolar beam centered on the optical axis Ax in the far field. The detailed structure and function of the diffractive optical element will be described later. The light beam passing through the diffractive optical element 6 passes through the zoom lens 7 as the second variable magnification optical system to illuminate the micro lens array (or fly-eye lens) 8 as an optical integrator. The zoom lens 7 is The diffractive optical element 6 and the rear focal plane of the microlens array 8 are connected to form an optical conjugation. In another aspect, the 'zoomable lens 7' connects the diffractive optical element 6 and the incident surface of the microlens array 8 into a substantially fu The relationship between the industry transformation. Therefore, the beam passing through the diffractive optical element 6 forms a circular distribution according to the circular distribution of the diffractive optical element 4 and the focal plane behind the variable lens 7 200405426 (and then the incident surface of the microlens array 8). The light intensity distribution of the convolution of the multiple pole-like distribution of the diffractive optical element 6 itself, that is, the formation of a complex polar field with the optical axis AX as the center. As described above, the diffractive optical element 6 and the variable-focus lens 7 constitute a field formation mechanism, which is based on the light beams having various angle components that are incident on the incident surface (the first predetermined surface) of the diffractive optical element 6. A plurality of polar illumination fields centered on the optical axis AX are formed on the incident surface (the second predetermined surface) of the microlens array 8. The width of this complex polar field (1/2 of the difference between the outer diameter and the inner diameter) depends on the focal length of the non-focus zoom lens 5 (the reference magnification varies, and its overall size depends on the focal length of the zoom lens 7). The lens array 8 is an optical element composed of a plurality of tiny lenses with positive refractive power arranged vertically and horizontally. Each tiny lens constituting the microlens array 8 has a shape of a field to be formed on the mask 13 ( Furthermore, it has a rectangular cross section similar to the shape of the exposed area to be formed on the wafer 15.)

般而έ,彳政透鏡陣列,係例如對平行平面玻璃板施以蝕刻 形成微小透鏡群而構成。 此處,構成微透鏡陣列之各微小透鏡,較構成複眼透 鏡之各透鏡兀件還要微小。又,微透鏡陣列,與由彼此隔 絕之透鏡元件構成之覆眼透鏡不同處在於,多數個微小透 鏡並未彼此隔絕而形成為一體。然而,具有正屈光力之透 鏡元件縱橫配置之點,則微透鏡陣列與複眼透鏡相同。又 ,第1圖中,為求圖面之清晰,所顯示之構成微透鏡陣列 之微小透鏡數量’遠低於實際數量。 16 200405426 因此,射入微透鏡陣列8之光束被多數個微小透鏡2 維分割,而在微透鏡陣列8之後側焦點面,形成與照野(藉 由射入微透鏡陣列8之入射光束所形成者)具有大致相同光 強度分佈之二次光源,亦即形成由以光軸Αχ為中心之複數 個實質的面光源所構成之複數極狀二次光源。如上述般, 微透鏡陣列8構成為一光學積分器,以根據來自在該入射 面(第2既定面)上形成之複數極狀照野的光束,用來形成 具有與複數極狀照野大致相同光強度分佈之複數極狀二次 光源。 | 來自微透鏡陣列8後側焦點面所形成之複數極狀二次 光源之光束,視需要以孔徑光闌(具有複數極狀之光透射 部)加以限制,在受到聚光光學系統9之聚光作用後,重疊 照明於作為照明視野光闌之光罩遮簾丨〇。透過光罩遮簾Μ 之矩形開口部(光透射部)之光束,在受到成像光學系統 (11a,lib)之聚光作用後,重疊照明於光罩13。此處,成 像光學系統(11a,lib)係將光罩遮簾1〇與光罩13連結成 大致光學共軛,於光罩13上,透過成像光學系統⑴a,| 11 b)而形成光罩遮簾1 〇之矩形開口部之像。 光罩13,係被支持在能2維移動之光罩載台(未圖示) 上。透射過光罩13之圖案的光束,透過投影光學系統Η ’在感光性基板之晶圓15上形成光罩圖案之像。晶圓15 ’被支持在能2維移動之晶圓載台(未圖示)上。以此方式 ’在與投影光學系統14之光軸AX正交之平面(χγ平面)内 一邊2維驅動控制晶圓15,一邊進行一次全面曝光或掃描 17 200405426 曝光,而在晶圓15 次曝光 之各曝光區域將光罩13 之圖案予以逐 又,—次全面曝光,係根據 咐⑽方式,將 進重複(响 此時,在光里η 光於晶圓之各曝光區域。 上之照明區域形狀為接讲 微透鏡陣列8之各朽… 為接近正方形之矩形’ 矩形。另—* “小透鏡之截面形狀亦為接近正方形之 蔣㈣固 、先罩及曰曰圓相對投影光學系統移動、同時 ,0案掃描曝光於晶圓之各曝光區域。此時,在光罩 13上之照明區域形狀係短邊與長邊例如為1 : 3之矩形, 微透鏡陣列8 f t 之各彳政小透鏡之截面形狀亦係與此相似之矩 形0 各實施形態中,繞射光學元件6,具備各種複數極照 明用(能對照明光程進行交換)的繞射光學元件6ι〜64。又 ,亦可取代作為發散光束形成元件之繞射光學元件4,而 使用由縱橫且緊密排列之多數個正六角形微小透鏡(例如 透鏡元件)所構成之微透鏡陣列(或複眼透鏡)。此時,在微 透鏡陣列8之入射面,形成依據正六角形與多極點的捲積 之光強度分佈,亦即形成以光軸AX為中心之複數極狀照野 ’於微透鏡陣列8之後側焦點面,形成以光軸AX為中心之 複數個實質面光源所構成之複數極狀的二次光源。 《第1實施形態》 第2圖,係概略顯示第1實施形態之4極照明用繞射 光學元件中所含之基本繞射光學元件及補全繞射光學元件 200405426 之構成的圖。又,第3圖係第2圖之各光學元件的截面圖 。第4圖,係概略顯示第i實施形態之4極照明用繞射光 學元件中所含之4種區塊之構成的圖。又,第5圖係概略 顯示第1實施形態之4極照明用繞射光學元件之全體構成 的圖。此外,f 6圖係用以說明第!實施形態之4極照明 用繞射光學元件之基本作用的圖。In general, the lens array is formed by, for example, etching a parallel flat glass plate to form a micro lens group. Here, each micro lens constituting the micro lens array is smaller than each lens element constituting the fly-eye lens. A microlens array is different from an eye-closing lens composed of lens elements isolated from each other in that a plurality of microlenses are not integrated with each other. However, the point where the lens elements with positive refractive power are arranged vertically and horizontally, the microlens array is the same as the fly-eye lens. In addition, in Fig. 1, for the sake of clarity of the drawing, the number of micro lenses' constituting the micro lens array is shown to be much lower than the actual number. 16 200405426 Therefore, the light beam entering the microlens array 8 is two-dimensionally divided by a plurality of microlenses, and the focal plane behind the microlens array 8 forms and illuminates the field (formed by the incident light beam entering the microlens array 8). (1) Secondary light sources having approximately the same light intensity distribution, that is, a plurality of polar secondary light sources formed by a plurality of substantial surface light sources centered on the optical axis Ax. As described above, the microlens array 8 is configured as an optical integrator for forming a light beam having a shape substantially equal to that of the complex polar field based on the light beams from the complex polar field formed on the incident surface (second predetermined surface). Multiple polar secondary light sources with the same light intensity distribution. The light beam from the multiple polar secondary light source formed by the focal plane on the rear side of the micro lens array 8 is limited by the aperture stop (with a multiple polar light transmitting portion) as needed, and is condensed by the condenser optical system 9 After the light is applied, the light is superimposed on a mask shade serving as a diaphragm of the illumination field. The light beam that has passed through the rectangular opening portion (light transmitting portion) of the mask M is subjected to the condensing action of the imaging optical system (11a, lib), and is then superimposed and illuminated on the mask 13. Here, the imaging optical system (11a, lib) connects the photomask blind 10 and the photomask 13 into a substantially optical conjugate, and the photomask 13 passes through the imaging optical system ⑴a, | 11 b) to form a photomask. Image of the rectangular opening of the shade 10. The photomask 13 is supported on a photomask stage (not shown) capable of two-dimensional movement. The light beam transmitted through the pattern of the mask 13 passes through the projection optical system ’'to form an image of a mask pattern on the wafer 15 of the photosensitive substrate. The wafer 15 'is supported on a wafer stage (not shown) that can be moved in two dimensions. In this way, while performing a two-dimensional driving control scan of the wafer 15 in a plane (χγ plane) orthogonal to the optical axis AX of the projection optical system 14, a full exposure or scan 17 200405426 exposure is performed, and 15 exposures are made on the wafer Each exposure area will repeat the pattern of the mask 13 one by one, a full exposure, which will be repeated according to the command (at this time, the light is exposed to each exposure area of the wafer in the light. The shape of the illuminated area on the In order to talk about the decay of the micro lens array 8 ... It is a rectangle close to a square 'rectangle. In addition— * "The cross-sectional shape of the small lens is also close to the shape of Jiang Yangu, the first cover and the circle are moved relative to the projection optical system, at the same time Scanning and exposure are performed on each exposed area of the wafer. At this time, the shape of the illuminated area on the mask 13 is a rectangular with short sides and long sides, for example, 1: 3, and each small lens of the microlens array 8 ft. The cross-sectional shape is similar to the rectangular shape. In each embodiment, the diffractive optical element 6 is provided with various diffractive optical elements 6 to 64 for various polar lighting (can exchange the optical path of the illumination). Instead of the diffractive optical element 4 as a divergent beam forming element, a microlens array (or fly-eye lens) composed of a plurality of regular hexagonal microlenses (such as lens elements) arranged closely and horizontally is used. At this time, in the microlens The incident surface of the array 8 forms a light intensity distribution based on the convolution of regular hexagons and multiple poles, that is, a plurality of polar field fields with the optical axis AX as the center is formed at the focal surface behind the microlens array 8 to form light. A plurality of polar secondary light sources constituted by a plurality of substantially planar light sources with the axis AX as the center. [First Embodiment] Fig. 2 is a schematic view showing the inclusion of a diffractive optical element for 4-pole illumination in the first embodiment. Figures of the basic diffractive optical element and complementary diffractive optical element 200405426. Fig. 3 is a cross-sectional view of each optical element of Fig. 2. Fig. 4 is a diagram showing a 4-pole of an i-th embodiment. FIG. 5 is a diagram showing the configuration of four types of blocks included in the diffractive optical element for illumination. FIG. 5 is a diagram schematically showing the entire configuration of the diffractive optical element for 4-pole illumination according to the first embodiment. In addition, f 6 For graphics The figure explaining the basic operation of the diffractive optical element for quadrupole illumination according to the first embodiment.

且參照第2圖可知,帛!實施形態之繞射光學元件61, 八備/σ X方向之直線光柵圖案的第1基本繞射光學 疋件Α卜沿Ζ方向之直線光栅圖案的第2基本繞射光學元 件Β卜將第1基本繞射光學元件…之凸面與凹面予以反 轉:得的第i補全繞射光學元件Α2,以及將第2基本繞射 與于π件Β1之凸面與凹面予以反轉所得的第2補全繞射光 學元件Β2。也就是說,第2基本繞射光學元件βι,具有將 :1基本繞射光學元件A1之圖案、於χζ平面順圖中反時 :童方向旋轉90度所得之圖案。又,第2補全繞射光學元件 2 ’具有將第!補全繞射光學元件Α2之圖案、於χζ平面 順圖中反時鐘方向旋轉90度所得之圖案。 第2圖中,斜線部係代表凸面、非斜線部(空白部)係 ._面亦即’各光學元件Α1,Α2,β1及,如第3 =不,具有凸面與凹面反覆構成之2元型繞射光學元件 =,該凸面及凹面之寬度w(以及凸面及凹面之節距p(= =於各光學70件全體係一定,其全體具一邊長度為L(L ::二、為整數)之正方形外形。又,斜線部表示凸面、非 ’、、’、部(空白部)表示凹面的記號’於其他相關之第1〇圖及 19 200405426 弟2 3圖中亦同。 因此,第1補全繞射光學元件A2,其對第丨基本繞射 光予元件所產生之光振幅,具有產生具1/2波長(18〇度) 相位差之光振幅的圖案。又,第2補全繞射光學元件B2, 其對第2基本繞射光學元件所產生之光振幅,具有產生具 1/2波長(180度)相位差之光振幅的圖案。進一步的,各 光學凡件Al,A2,B1及B2之凸面與凹面之段差(凸部與凹And referring to Figure 2, we can see, oh! The diffractive optical element 61 of the embodiment, the first basic diffractive optical element of the linear grating pattern in the Haze / σ X direction, and the second basic diffractive optical element in the linear grating pattern in the Z direction. The convex and concave surfaces of the basic diffractive optical element are reversed: the i-th complementary diffractive optical element A2 obtained, and the second complement obtained by inverting the second basic diffraction and the convex and concave surfaces of the π member B1. Full diffraction optical element B2. In other words, the second basic diffractive optical element βι has a pattern obtained by rotating the pattern of the: 1 basic diffractive optical element A1 in the χζ plane in the reverse direction of the child's direction: 90 degrees. The second complementary diffractive optical element 2 ′ has a first! The pattern obtained by completing the pattern of the diffractive optical element A2 and rotating it 90 ° counterclockwise in the χζ plane in the figure. In FIG. 2, the oblique line represents a convex surface, and the non-slanted portion (blank portion) is a ._ surface, that is, each optical element A1, A2, β1, and, as in 3 = No, a two-element structure having a convex surface and a concave surface repeatedly. Type diffractive optical element =, the width w of the convex and concave surfaces (and the pitch p and convex p and concave surface p (=) are fixed in the entire system of each 70 optical components, and the length of one side of the whole is L (L :: two, is an integer) ) Square shape. Moreover, the oblique line part indicates convex, non- ',,', part (blank part) indicates the concave symbol 'in the other related figures 10 and 19 200405426. The same is true for the second and third figures. Therefore, the first 1 Complementary diffractive optical element A2, which has a pattern for generating the amplitude of light with a phase difference of 1/2 wavelength (18 °) for the first diffracted light element, and a second complement The diffractive optical element B2 has a pattern for generating a light amplitude with a phase difference of 1/2 wavelength (180 degrees) for the light amplitude generated by the second basic diffractive optical element. Further, each optical element Al, A2 , The difference between convex and concave surfaces of B1 and B2 (convex and concave

部間之高度尺寸)d,係根據下式(1)來設定,以使繞射效率 為最佳,亦即相位差為又/2。 d=A/{2(nl — n2)} ···(〇 此處,λ係照明光(曝光用光)之波長、亦即使用波長 ,nl係繞射光學元件6(61〜64)之玻璃基板於使用波長之 折射率,n2係照明光程環境氣息之形成媒體於使用波長之 折射率。具體而言,設使用波長λ為i 93nm、玻璃基板之 折射率為1.5、料媒體之空氣或惰性氣體 時,段差d係設定成193酿左右。The height dimension d) of the parts is set according to the following formula (1) to optimize the diffraction efficiency, that is, the phase difference is / 2. d = A / {2 (nl — n2)} (... here, λ is the wavelength of the illumination light (exposure light), that is, the used wavelength, and nl is the wavelength of the diffractive optical element 6 (61 ~ 64) The refractive index of the glass substrate at the wavelength of use, n2 is the refractive index of the medium at the wavelength of the light used to form the ambient atmosphere of the illumination. Specifically, let us use the wavelength λ of 93nm, the refractive index of the glass substrate at 1.5, and the air of the material In the case of an inert gas, the step d is set to about 193.

又,各光學元件A1,A2, B1及们之凸面及凹面之 距P ’係視對繞射光學元件6(61〜64)待設定之期望的繞 角0,根據下式(2)來設定。 ^ sine/ ··· (1) 備 本 參照第4圖可知’第!實施形態之繞射光學元件具 4種類的區塊C1〜C4。又,帛i區塊π中,8個第】基 繞射光學元件Μ肖8個第2基本繞射光學元件Μ,: X方向及Z方向之兩方向交互排列。又,第2區塊a中 20 200405426 元LI第1基本繞射光學元件A1與8個第2補全繞射光學 係^ X方向及z方向之兩方向交互排列。 ,外,第3區塊C3中,8個第!補全繞射光學元件A2 ”固第2基本繞射光學元件B1,係沿χ方向及z方向之 2向交互排列。又,第4區塊C4中,8個第U本補全 先予…2與8個第2補全繞射光學元件Β2,係沿χ方 向:ζ方向之兩方向交互排列。以此方式,各區塊ci〜以 ,皆具有正方形之外形,彼此大小相同。 參照第5圖可知,帛1實施形態之繞射光學元件6卜 係由縱橫且緊密排狀多數個區塊G1〜C4所構成。此處, 各區塊C1〜C4彼此大致為同數,於繞射光學元件61之矩 形有效區域(有效直徑)61 a之全體隨機排列。 第1圖之曝光裝置中,在複數極照明用繞射光學元件 6之位置設置第1實施形之繞射光學元件6丨,將平行光束 射入此繞射光學元件61時,即能在微透鏡8之入射面獲得 如弟6圖所示之4點狀光強度分佈。此處,挾著光軸Αχ卜 X方向之2點狀光強度分佈,係藉由第1基本繞射光學元 件A1及第1補全繞射光學元件A2之作用而形成。又,挟 者光轴AX沿Z方向之2點狀光強度分佈,係藉由第2灵本 繞射光學元件B1及第2補全繞射光學元件B2之作用而形 成0 第7圖,係用以說明第1實施形態中,於微透鏡陣列 之入射面形成4極狀照野之原理的圖。又,第8圖,係顯 示第1實施形態中,於微透鏡陣列之入射面形成之4極狀 21 200405426 照野的圖。此外,第9圖,係顯示在第1實施形態中使用 微透鏡陣列來作為發散光束形成元件時,於作為光學積分 器之微透鏡陣列之入射面形成之4極狀照野的圖。又,第 7圖中,係顯示取代作為發散光束形成元件之繞射光學元 件4,而使用微透鏡陣列4的狀態。 第7圖中,作為發散光束形成元件,由於係使用由正 六角形之微小透鏡所構成之微透鏡陣列4,因此於其後側 焦點面形成多數光源。又,來自多數個光源之光,於無焦 點變焦透鏡5之光瞳面形成六角形(正六角形之光強度分佈 )之光束。又,使用繞射光學元件4來作為發散光束形成元 件時’如前所述,在無焦點變焦透鏡5之光瞳面,係形成 圓形(圓形之光強度分佈)之光束。 來自無焦點變焦透鏡5之光瞳面所形成之成六角形或 圓形光強度分佈之光,從無焦點變焦透鏡5射出,成為具 有各種角度成分之光束射入繞射光學元件61。當具有各種 角度成分之聚光光束射入繞射光學元件61時,例如平行於 光軸AX之光、線al,在通過繞射光學元件61 |,即往對光 軸繞射角度未圖示)之方向前進。又,例如, :有軸為±1:角度之光、線以,心,在通過繞射光學元 《,則往對光軸繞射角度±(θ 士±t)側未 圖示)之方向前進。 之後,光線a 1,a 2, 鏡7,到達微透鏡陣列8 陣列4a中,與光線ai a3,透過具有焦距f之可變焦透 之入射面。另一方面,於微透鏡 a2,a3通過不同微小透鏡元件之 22 200405426 光線bl,b2,b3’亦透過繞射光學元件61及可變焦透鏡7 而在微透鏡陣列8之入射面到達與光線&1,a2,a3相同之 區域。換言之’在微透鏡陣列8之入射面,相同區域係被 光線al〜a3與光線bl〜b3重疊照明。 如上述般,當平行光束射入繞射光學元件Η時,在微 透鏡陣列8之入射面係形成如第6圖所示之4點狀光強度 分佈。然而,實際上,射入繞射光學元件61的並非是平行 光束,而是具有被錐狀體(微透鏡陣列4a時為正六角形錐 狀體、繞射光學元件4時為圓錐體)之光束範圍所限定之角 度成分的光束。如前所述,在微透鏡陣列8之入射面,係 如第8圖或第9圖所示,形成由4點狀光強度分佈與圓形 或正六角形光束之捲積所構成的4極狀照明分佈(照野)。 其結果’在微透鏡陣列8之後側焦點面(照明光瞳面) ’形成具有與4極狀照野大致相同光強度分佈之4極狀二 人光源。此處,4極狀二次光源,係由4個圓形或正六角 形之實質的面光源,亦即由挾著光軸AX於X方向對稱配置 之2個面光源、與挾著光軸AX於Z方向對稱配置之2個面 光源所構成。如此,在第1實施形態中,藉由繞射光學元 件之作用,於照明光瞳面形成實質上均勻的4極狀二次 光源。 第1實施形態中,可藉由改變無焦點變焦透鏡5之倍 率 在構成4極狀二次光源之各面光源中心與光軸A)(之距 離不變的情形下,僅使各面光源之大小(4極狀二次光源之 卜接圓半控一 4極狀二次光源之内接圓半徑)變化。另一方Further, the distance P 'between the convex and concave surfaces of each optical element A1, A2, B1, and their respective convex angles and concave surfaces P' depends on the desired winding angle 0 to be set for the diffractive optical element 6 (61 to 64), and is set according to the following formula (2) . ^ sine / ··· (1) Prepare this book Refer to Figure 4 The diffractive optical element of the embodiment has four types of blocks C1 to C4. Also, in the 帛 i block π, the eighth basic diffraction optical elements M and the eight second basic diffraction optical elements M are alternately arranged in two directions: the X direction and the Z direction. Also, in the second block a, 20 200405426 yuan LI, the first basic diffractive optical element A1, and eight second complementary diffractive optical systems ^ are alternately arranged in two directions: the X direction and the z direction. In addition, in the third block C3, 8th! The complementary diffractive optical element A2 is a second basic diffractive optical element B1, which is arranged alternately in two directions of the χ direction and the z direction. In addition, in the fourth block C4, eight U-th completions are given in advance ... The 2 and 8 second complementary diffractive optical elements B2 are alternately arranged along two directions of the χ direction and the ζ direction. In this way, each block ci to y has a square shape and is the same size as each other. It can be seen from FIG. 5 that the diffractive optical element 6 of the first embodiment is composed of a plurality of blocks G1 to C4 that are arranged vertically and closely in a row. Here, the blocks C1 to C4 are approximately the same as each other, and are diffractive The entire rectangular effective area (effective diameter) 61 a of the optical element 61 is randomly arranged. In the exposure device of FIG. 1, the diffractive optical element 6 of the first embodiment is provided at the position of the diffractive optical element 6 for multiple polar illumination. When a parallel light beam is incident on the diffractive optical element 61, a 4-point light intensity distribution as shown in Fig. 6 can be obtained on the incident surface of the microlens 8. Here, the optical axis Aχ and the X-direction Two-point light intensity distribution, which is based on the first basic diffractive optical element A1 and the first complementary diffracted light It is formed by the function of the element A2. The two-point light intensity distribution of the optical axis AX along the Z direction is formed by the action of the second spirit diffraction optical element B1 and the second complementary diffraction optical element B2. Formation 0 FIG. 7 is a diagram for explaining the principle of forming a 4-pole field on the incident surface of the microlens array in the first embodiment. Also, FIG. 8 is a diagram showing the microstructure in the first embodiment. A diagram of the four poles 21 200405426 formed by the incident surface of the lens array. In addition, FIG. 9 shows the micro-lens array used as the divergent beam forming element in the first embodiment. A diagram of a quadrupole field formed by the incident surface of the lens array. In addition, FIG. 7 shows a state where the microlens array 4 is used instead of the diffractive optical element 4 as a divergent beam forming element. FIG. 7 As the divergent beam forming element, since a micro lens array 4 composed of regular hexagonal micro lenses is used, a plurality of light sources are formed on the rear focal plane. In addition, light from a plurality of light sources is used in a non-focus zoom lens 5 Pupil plane formation An angular beam (a regular hexagonal light intensity distribution). When the diffractive optical element 4 is used as the divergent beam forming element, as described above, the pupil surface of the non-focus zoom lens 5 is circular (circular). Shaped light intensity distribution). The light from the hexagonal or circular light intensity distribution formed by the pupil surface of the non-focus zoom lens 5 is emitted from the non-focus zoom lens 5 and becomes a beam with various angle components. Enter the diffractive optical element 61. When a condensed light beam having various angle components enters the diffractive optical element 61, for example, light parallel to the optical axis AX, the line al passes through the diffractive optical element 61 | The axis diffraction angle is not shown). For example, if the axis is ± 1: the angle of the light, line, and center passes through the diffractive optical element ", then the angle of diffraction to the optical axis is ± ( θ ±± t) side). After that, the light rays a 1, a 2, and the mirror 7 reach the micro lens array 8 array 4 a and the light rays ai a3 pass through an incident surface with a focal length f and a variable focal length. On the other hand, the microlenses a2 and a3 pass through the different microlens elements 22 200405426. The light b1, b2, and b3 'also pass through the diffractive optical element 61 and the variable lens 7 and reach the light plane at the incident surface of the microlens array 8. ; 1, a2, a3 same area. In other words, on the incident surface of the microlens array 8, the same area is illuminated by light rays al ~ a3 and light rays b1 ~ b3 overlapping. As described above, when a parallel light beam enters the diffractive optical element Η, a 4-point light intensity distribution as shown in Fig. 6 is formed on the incident surface of the microlens array 8. However, in fact, it is not a parallel light beam that enters the diffractive optical element 61, but a light beam having a cone (a regular hexagonal cone in the microlens array 4a and a cone in the diffractive optical element 4). Beams with angular components defined by the range. As described above, on the incident surface of the microlens array 8, as shown in FIG. 8 or FIG. 9, a 4-pole shape composed of a convolution of a 4-point light intensity distribution and a circular or regular hexagonal beam is formed. Lighting distribution (photofield). As a result, a quadrupole dipole light source having a light intensity distribution approximately the same as that of the quadrupole illumination field is formed on the side focal plane (illumination pupil plane) behind the microlens array 8. Here, the quadrupole secondary light source is composed of four substantially circular or regular hexagonal surface light sources, that is, two surface light sources arranged symmetrically in the X direction by the optical axis AX and the optical axis AX. It consists of two surface light sources arranged symmetrically in the Z direction. As described above, in the first embodiment, a substantially uniform quadrupole secondary light source is formed on the illumination pupil surface by the action of the diffractive optical element. In the first embodiment, by changing the magnification of the non-focus zoom lens 5, the distance between the center and the optical axis A of each surface light source constituting the quadrupole secondary light source can be changed. The size (the radius of the inscribed circle of the 4-pole secondary light source and the half radius of the inscribed circle of the 4-pole secondary light source) is changed.

23 200405426 面可藉由改變可變焦透冑7之焦距,來變化上述距離及 大小雙方’使4極狀二次光源全體相似的放大或縮小。 又’上述第1實施形態,於各區塊C1〜C4中,係於橫 方向及縱方向分別配置4個光學元件,但不限於此,二般 來說,可在橫方向及縱方向分別配置η個(G2)光學心 來構成各區塊C1〜C4°如第1實施形態般’將4種類之光 學兀件(Al,A2,Bl,B2)加以區塊化並隨機排列之方式, 與規則排列各光學元件(Al,A2, B1,B2)之情形相較,無 論在實驗及模擬計算上,皆已證實較有利於降低因相干雜% 訊所造成之照度不均現象。 《第2實施形態》 第1實施形態中,係藉由繞射光學元件61之作用,來 形成由挾著光軸AX於X方向對稱配置之2個面光源、與挾 著光軸AX於Z方向對稱配置之2個面光源所構成的十字形 4極狀二次光源。相對於此,第2實施形態中,則係藉由23 200405426 The surface can be enlarged or reduced similarly to the entire quadrupole secondary light source by changing both the above distance and size by changing the focal length of the zoom lens 7. Also, in the above-mentioned first embodiment, four optical elements are respectively arranged in the horizontal direction and the vertical direction in each of the blocks C1 to C4. η (G2) optical cores to constitute each block C1 ~ C4 ° as in the first embodiment, a method of 'blocking and randomly arranging 4 types of optical elements (Al, A2, Bl, B2) and Compared with the case where the optical elements (Al, A2, B1, B2) are arranged regularly, both in experiments and simulation calculations, it has been proved that it is more beneficial to reduce the uneven illumination caused by the coherent noise. << Second Embodiment >> In the first embodiment, two surface light sources arranged symmetrically with the optical axis AX in the X direction and the optical axis AX in the Z direction are formed by the action of the diffractive optical element 61. A cross-shaped quadrupole secondary light source composed of two surface light sources arranged symmetrically in the direction. In contrast, in the second embodiment,

繞射光學兀件62之作用,來形成由挾著光軸Αχ、相肖X 軸於45度方向對稱配置之4個面光源所構成的χ形4極狀| 二次光源。以下,著眼於與第1實施形態之相異處,來說 明第2實施形態。 第1 〇圖’係概略顯示第2實施形態之4極照明用繞射 光學兀件中所含之基本繞射光學元件及補全繞射光學元件 之構成的圖。又’第1丨圖,係概略顯示第2實施形態之4 極照明用繞射光學元件中所含之4種區塊之構成的圖。又 ’第12圖’係概略顯示第2實施形態之4極照明用繞射光 24 200405426 學兀件之全體構成的圖。此外,第丨3圖,係用以說明第2 實施形態之4極照明用繞射光學元件之基本作用的圖。 由第10圖可知,第2實施形態之繞射光學元件Μ, 具備··沿著對+ X方向繞+ γ軸(以圖中順時鐘方向為正角 落)45度方向之直線光柵圖案的第丨基本繞射光學元件w ,沿著對+ Z方向繞—γ軸45度方向之直線光栅圖案的第 2基本繞射光學元件E卜將第!基本繞射光學元件di之凸 面與凹面予以反轉所得的第1補全繞射光學元件D2,以及 將第2基本繞射光學元件E1之凸面與凹面予以反轉所得的· 苐2補全繞射光學元件μ。 也就是說,第2基本繞射光學元件E1,具有將第丨基 本繞射光學元件D1之圖案、於XZ平面順圖中反時鐘方向 走轉9 G度所得之圖案。又,第2補全繞射光學元件μ, 具有將第1補全繞射光學元件D2之圖案、力χζ平面順圖 :反時鐘方向旋轉9〇度所得之圖案。第2實施形態中亦與 第1實施形態同樣的,具有凸面與凹面反覆構成之2元型· 凡射光予兀件圖案’該凸面及凹面之寬度w於各光學元件, 王體係一疋,其全體具一邊長度為L(L=mP: m為整數)之 正方形外形。 參照第11圖可知,第1實施形態之繞射光學元件62 ”備4種類之區塊F1〜F4。又,第i區塊Fi中,g個第 1二本:繞射光學元件D1與9個第2基本繞射光學元件, 、著^ X方向成45度的2個方向交互排列。又,第2區 Α 2中,9個第1基本繞射光學元件D1與9個第2補全 25 200405426 繞射光學元件E2,係沿著與χ方向成45度的2個方向交 互排列。 此外’第3區塊F3中,9個第1補全繞射光學元件D2 與9個第2基本繞射光學元件E1,係沿著與X方向成45 度的2個方向交互排列。又,第4區塊f4中,9個第1補 全繞射光學元件D2與9個第2補全繞射光學元件E2,係 /口著與X方向成45度的2個方向交互排列。如此,各區塊 F1〜F4 ’彼此具有相同大小。 參照第12圖可知,第2實施形態之繞射光學元件62 % ,係由縱橫且緊密排列之多數個區塊F1〜F4所構成。此處 各區塊C1〜C4彼此大致為同數,於繞射光學元件62之 矩形有效區域(有效直徑)62a之全體隨機排列。此時,為 避免在有效區域62a中產生間隙,多數個區塊C1〜C4係以 既定之邊(margin)配置。 第1圖之曝光裝置中,在複數極照明用繞射光學元The function of the diffractive optical element 62 forms a χ-shaped quadrupole-shaped | secondary light source composed of 4 area light sources arranged symmetrically with respect to the optical axis Ax and the phase X axis at 45 degrees. Hereinafter, the second embodiment will be described focusing on differences from the first embodiment. Fig. 10 'is a diagram schematically showing the configuration of a basic diffractive optical element and a complementary diffractive optical element included in the diffractive optical element for quadrupole illumination of the second embodiment. FIG. 1 ′ is a diagram schematically showing the configuration of four types of blocks included in the diffraction optical element for quadrupole illumination according to the second embodiment. Fig. 12 is a diagram schematically showing the overall configuration of the diffracted light for quadrupole illumination of the second embodiment. FIG. 3 is a diagram for explaining the basic operation of the diffractive optical element for quadrupole illumination according to the second embodiment. It can be seen from FIG. 10 that the diffractive optical element M of the second embodiment includes a first linear grating pattern of 45 degrees in a direction of +45 along the pair + X direction (the clockwise direction is a positive corner in the figure).丨 Basic diffractive optical element w, the second basic diffractive optical element E of the linear grating pattern that is wound along the + Z direction—45 axis in the γ axis direction! The first complementary diffractive optical element D2 obtained by inverting the convex and concave surfaces of the basic diffractive optical element di, and the 苐 2 complementary winding obtained by inverting the convex and concave surfaces of the second basic diffractive optical element E1. Emitting optical element μ. That is to say, the second basic diffractive optical element E1 has a pattern obtained by rotating the pattern of the first basic diffractive optical element D1 by 9 G degrees in the counterclockwise direction in the XZ plane. The second complementary diffractive optical element μ has a pattern obtained by rotating the pattern of the first complementary diffractive optical element D2 and the force χ ζ plane: 90 ° counterclockwise. The second embodiment is the same as the first embodiment, and has a two-element structure with a convex surface and a concave surface. Wherever the light beams to the element pattern, the width of the convex surface and the concave surface is in each optical element. It has a square shape with one side length L (L = mP: m is an integer). Referring to FIG. 11, it can be seen that the diffractive optical element 62 ″ of the first embodiment has four types of blocks F1 to F4. In the i-th block Fi, there are g first and second copies: diffractive optical elements D1 and 9 The second basic diffractive optical elements are arranged alternately in two directions at 45 degrees to the X direction. In addition, in the second area A 2, 9 first basic diffractive optical elements D1 and 9 second completions 25 200405426 Diffractive optical element E2 is alternately arranged in two directions that are 45 degrees from the χ direction. In addition, in the third block F3, nine first complementary diffractive optical elements D2 and nine second basic The diffractive optical element E1 is alternately arranged in two directions at 45 degrees to the X direction. In the fourth block f4, nine first complementary diffractive optical elements D2 and nine second complementary diffractive elements are arranged. The diffractive optical element E2 is alternately arranged in two directions at 45 degrees to the X direction. In this way, the blocks F1 to F4 'have the same size as each other. Referring to FIG. 12, it can be seen that the diffractive optics of the second embodiment The element 62% is composed of a plurality of blocks F1 to F4 arranged vertically and horizontally. The blocks C1 to C4 are approximately the same number as each other, and the rectangle of the diffractive optical element 62 The entire effective area (effective diameter) 62a is randomly arranged. At this time, in order to avoid a gap in the effective area 62a, most of the blocks C1 to C4 are arranged with a predetermined margin. In the exposure device of FIG. 1, Diffractive optics for complex pole illumination

6之位置設置第2實施形之繞射光學元件62,將平行夫 射入此繞射光學元件62日夺,即能在微透鏡8之人射面獲 如第13圖所示之X形4點狀光強度分佈。此處,挾著二 AX、沿對+ X方向繞+ γ軸(以圖中順時鐘方向為正角落 度方向之2點狀光強度分佈’係藉由帛1基本繞射光學 :D1及帛1補全繞射光學元件D2之作用而形成。又, “光軸AX化對+ z方向繞+ γ轴一 45度方向之2 =分佈’係藉由第2基本繞射光學元件E1及第2補全 射光學元件E2之作用而形成。 26 200405426 因此,第2實施形態中,於微透鏡陣列8之入射面, 係如第14圖或第15圖所示,形成由X形4點狀光強度分 佈一圓形或正六角形光束之捲積所構成之4極狀照明分佈( …、野)。其結果,於微透鏡陣列8之後側焦點面(照明光瞳 面)形成具有與4極狀照野大致相同光強度分佈之χ形4極 狀一次光源。以此方式,第2實施形態亦與第丨實施形態 同樣的,藉由繞射光學元件62之作用,於照明光瞳面形成 貫質上均勻的4極狀二次光源。 又,第2實施形態亦與第i實施形態同樣的,可藉由% 改k無焦點變焦透鏡5之倍率,在構成4極狀二次光源之 各面光源中心與光軸AX之距離不變的情形下,僅使各面光 源之大小變化。另一方面,可藉由改變可變焦透鏡7之焦 距,來變化上述距離及大小雙方,使4極狀二次光源全體 相似的放大或縮小。進一步的,各區塊π〜F4之光學元件 排列方法,亦與第1實施形態同樣的,可作各種的變形例 〇 《第3實施形態》 9 第1實施形態係藉由繞射光學元件61之作用,來形成 十字形4極狀二次光源,第2實施形態則係藉由繞射光學 元件62之作用來形成X形4極狀二次光源。相對於此,第 3實施形態,則係藉由繞射光學元件61與繞射光學元件 之共同作用’來形成8極狀二次光源。以下,著眼於與第 1實施形態及第2實施形態之相異處,來說明第3實施形 態。 27 200405426 第3實施形態中,8極照明用繞射光學元件63,具備 :第1實施形態之4極照明用繞射光學元件61中所含之4 種光學元件(Al,A2,Bl,B2)、以及與第2實施形態之4 極照明用繞射光學元件62中所含之4種光學元件(Dl,D2, El, E2)類似之(Dl,,D2,,ΕΓ,E2,)。又,第3實施形態 之繞射光學元件63,具備包含區塊C1〜C4與F1,〜F4,的4 種區塊DQ1〜DQ4。 第16圖,係顯示第3實施形態之基本繞射光學元件及 補全繞射光學元件(Dl,,D2,,ΕΓ,E2,)之構成的概念圖。 如以下之記述,為了與區塊C1〜C4合成,正方形交界與直 線繞射光栅之圖案係被圖案化成具有45度之傾斜。第! 7 圖’係顯示以光學元件(Dl,,D2,,ΕΓ,E2,)構成之區塊 F1’〜F4’之構成的概念圖。第18圖,係藉由組合區塊C1〜 C4與區塊F1’〜F4’來構成合成區塊DQ1〜DQ4的概念圖。 第19圖’係顯示將多數之合成區塊DQ1〜DQ4縱橫緊密排 列所構成之第3實施形態之繞射光學元件63之構成的概念 圖。此處,各合成區塊DQ1〜DQ4,彼此大致為同數,於繞 射光學元件6 3之矩形有效區域全體隨機配置。 第1圖之曝光裝置中,在複數極照明用繞射光學元件 6之位置設置第3實施形之繞射光學元件63,將平行光束 射入此繞射光學元件63時,即能在微透鏡8之入射面獲得 第2 0圖所示之8點狀光強度分佈。此處,挟著光轴μ 沿X方向之2點狀光強度分佈,係由第丨基本繞射光學元 件A1及第1補全繞射光學元件A2之作用而形成。又,挾 200405426 之2點狀光強度分佈 2補全繞射光學 著光軸ΑΧ沿z方向 射光學元件B1及第 係由第2基本繞 兀件B2之作用而形成A diffractive optical element 62 of the second embodiment is set at the position of 6 and a parallel husband is injected into the diffractive optical element 62 to obtain an X-shaped 4 as shown in FIG. 13 on the projection surface of the micro lens 8. Spot light intensity distribution. Here, the two-point light intensity distribution along the pair AX, around the + X direction + the γ axis (the clockwise direction in the figure is the positive corner direction direction 'is based on 帛 1 basic diffraction optics: D1 and 帛1 is formed by complementing the action of the diffractive optical element D2. Also, "the optical axis AX is paired with + z-direction winding + γ-axis in a 45-degree direction 2 = distribution 'is obtained by the second basic diffractive optical element E1 and the first 2 It is formed by complementing the action of the radiating optical element E2. 26 200405426 Therefore, in the second embodiment, the incident surface of the microlens array 8 is formed as shown in FIG. 14 or FIG. Light intensity distribution A 4-pole illumination distribution (..., field) formed by the convolution of a circular or regular hexagonal beam. As a result, a side focal plane (illumination pupil plane) behind the microlens array 8 is formed with 4 poles. The χ-shaped 4-pole primary light source having substantially the same light intensity distribution in the field of illumination. In this way, the second embodiment is also formed on the illumination pupil surface by the action of the diffractive optical element 62 in the same manner as the first embodiment. A quadrupole secondary light source that is uniform in quality. The second embodiment is the same as the i-th embodiment. By changing the magnification of the k-focusless zoom lens 5 by%, only the size of each surface light source is changed while the distance between the center of each surface light source and the optical axis AX constituting the quadrupole secondary light source is not changed. On the other hand, by changing the focal length of the variable-focus lens 7, both the distance and the size can be changed, so that the entire quadrupole secondary light source can be similarly enlarged or reduced. Further, the optical element arrangement method of each block π to F4, Similar to the first embodiment, various modifications can be made. "Third embodiment" 9 The first embodiment forms a cross-shaped quadrupole secondary light source by the action of the diffractive optical element 61. In the second embodiment, an X-shaped quadrupole secondary light source is formed by the action of the diffractive optical element 62. In contrast, in the third embodiment, the diffractive optical element 61 and the diffractive optical element are used in common. Action 'to form an 8-pole secondary light source. The third embodiment will be described focusing on the differences from the first embodiment and the second embodiment. 27 200405426 In the third embodiment, an 8-pole lighting coil is used. Radiation optical element 63 including: The four types of optical elements (Al, A2, Bl, B2) included in the diffractive optical element 61 for 4-pole illumination according to the embodiment, and the four types of optical elements included in the diffractive optical element 62 for 4-pole illumination according to the second embodiment. This optical element (Dl, D2, El, E2) is similar to (Dl ,, D2 ,, Γ, E2,). The diffractive optical element 63 of the third embodiment includes blocks C1 to C4 and F1, Four blocks DQ1 to DQ4 of ~ F4. Fig. 16 shows the structure of the basic diffractive optical element and the complementary diffractive optical element (Dl ,, D2,, Γ, E2,) of the third embodiment. Conceptual map: As described below, in order to combine with the blocks C1 to C4, the pattern of the square boundary and the linear diffraction grating is patterned to have a 45-degree tilt. Number! Fig. 7 is a conceptual diagram showing the composition of blocks F1 'to F4' composed of optical elements (Dl ,, D2 ,, EΓ, E2,). FIG. 18 is a conceptual diagram of the synthesized blocks DQ1 to DQ4 by combining blocks C1 to C4 and blocks F1 'to F4'. Fig. 19 'is a conceptual diagram showing the structure of a diffractive optical element 63 according to a third embodiment in which a plurality of synthesized blocks DQ1 to DQ4 are arranged closely and vertically. Here, the respective synthetic blocks DQ1 to DQ4 are approximately the same number as each other, and are randomly arranged in the entire rectangular effective area of the diffractive optical element 63. In the exposure apparatus shown in FIG. 1, a diffraction optical element 63 according to the third embodiment is provided at the position of the diffraction optical element 6 for multiple pole illumination. When a parallel light beam is incident on the diffraction optical element 63, the microlens The 8-point incident plane obtains the 8-point light intensity distribution shown in FIG. 20. Here, the two-point light intensity distribution along the X direction along the optical axis µ is formed by the action of the first basic diffraction optical element A1 and the first complementary diffraction optical element A2. In addition, the two-point light intensity distribution of 挟 200405426 2 Complementary Diffraction Optics The optical element B1 and the first system are aligned with the optical axis A × in the z direction and are formed by the action of the second basic diffraction element B2

立再者,挾著光軸AX、沿對+ X方向繞+ ¥軸(以圖中順 時鐘方向為正角幻45度方向之2點狀光強度分佈,係藉 由第i基本繞射光學元件D1’及第i補全繞射光學元件二 :作用而形成。又’挾著光車4 AX、沿對+ z方向繞+ γ軸 :45度方向之2點狀光強度分佈,係藉由帛2基本繞射光 學兀件E1’及第2補全繞射光學元件E2,之作用而形成。 因此,第3實施形態中,於微透鏡陣列8之入射面, 係如第21圖或第22圖所示,形成由8點狀光強度分佈與 圓形或正六角形光束之捲積所構成之8極狀照明分佈(照野 )。其結果,於微透鏡陣列8之後側焦點面(照明光瞳面)形 成具有與8極狀照野大致相同光強度分佈之8極狀二次光 源。以此方式,第3實施形態,藉由繞射光學元件63之作In addition, the two-point light intensity distribution around the optical axis AX, along the pair + X direction + + axis (the clockwise direction in the figure is a positive angle of 45 degrees, is based on the i-th basic diffraction optics) Element D1 'and the i-th complementary diffractive optical element 2: function and are formed. It is also held by the light car 4 AX, along the pair + z direction around + γ axis: a 2-point light intensity distribution in the direction of 45 degrees. It is formed by the function of the 帛 2 basic diffractive optical element E1 ′ and the second complementary diffractive optical element E2. Therefore, in the third embodiment, the incident surface of the microlens array 8 is as shown in FIG. 21 or As shown in FIG. 22, an 8-pole illumination distribution (illumination field) formed by a convolution of an 8-point light intensity distribution and a circular or regular hexagonal beam is formed. As a result, a focal surface behind the microlens array 8 ( An illumination pupil surface) forms an 8-pole secondary light source having approximately the same light intensity distribution as the 8-pole illumination field. In this way, the third embodiment uses the operation of the diffractive optical element 63

用’於照明光瞳面形成實質上均勻的8極狀二次光源。 又’第3實施形態,可藉由改變無焦點變焦透鏡5之 倍率,在構成8極狀二次光源之各面光源中心與光軸AX之 距離不變的情形下,僅使各面光源之大小變化。另一方面 ’可藉由改變可變焦透鏡7之焦距,來變化上述距離及大 小雙方,使8極狀二次光源全體相似的放大或縮小。 《第4實施形態》 第1實施形態及第2實施形態,係藉由繞射光學元件 61或62之作用,來形成4極狀二次光源。相對於此,第4 29 200405426 實施形態,則係藉由繞射光學元件64之作用,來形成2極 狀二次光源。以下,著眼於與第1實施形態及第2實施形 態之相異處,來說明第4實施形態。 第23圖,係概略顯示第4實施形態之2極照明用繞射 光學元件中所含之基本繞射光學元件及補全繞射光學元件 之構成的圖。又,第24圖,係概略顯示第4實施形態之2 極照明用繞射光學元件之全體構成的圖。此外,第25圖, 係用以說明第4實施形態之各光學元件之隨機配置的圖。It is used to form a substantially uniform 8-pole secondary light source for the illumination pupil surface. In the third embodiment, by changing the magnification of the non-focus zoom lens 5, when the distance between the center of each surface light source and the optical axis AX of the 8-pole secondary light source is unchanged, only the Size changes. On the other hand, by changing the focal length of the variable focus lens 7, both the above distance and the size can be changed, so that the entire 8-pole secondary light source can be similarly enlarged or reduced. [Fourth Embodiment] The first embodiment and the second embodiment form a quadrupole secondary light source by the action of the diffractive optical element 61 or 62. In contrast, the fourth 29th 200405426 embodiment forms a bipolar secondary light source by the action of the diffractive optical element 64. Hereinafter, the fourth embodiment will be described focusing on differences from the first embodiment and the second embodiment. Fig. 23 is a diagram schematically showing a configuration of a basic diffractive optical element and a complementary diffractive optical element included in the diffractive optical element for bipolar illumination of the fourth embodiment. Fig. 24 is a diagram schematically showing the entire configuration of a diffractive optical element for bipolar illumination according to the fourth embodiment. In addition, Fig. 25 is a diagram for explaining the random arrangement of the optical elements of the fourth embodiment.

第1實施形態及第2實施形態中,若設基本繞射光學 元件(Al,Bl,Dl,E1)所產生之光束相位為〇相位的話, 則補全繞射光學元件(A2,B2,D2,E2)所產生之光束相位 即為7Γ相位。換言之,補全繞射光學元件(A2,B2, E2),係被設定成其所產生之光振幅,對基本繞射光學元件 (Al,Bl,Dl,E1)所產生之光振幅具有π的相位差。相對 於此’第4實施形態則係設定成,設基本繞射光學元件〇 1 所產生之光束相位為〇相位的話,則第1〜第3補全繞射 光學元件G2〜G4所產生之光束相位,分別為冗/ 2相位、| 7Γ相位、3 7Γ / 2相位。 此時,基本繞射光學元件G1,例如具有與第丨實施形 態之基本繞射光學元件Α1相同之圖案。又,第2補全終射 光學元件G3,例如具有與第丨實施形態之補全繞射光學一 件Α2相同之圖案(將基本繞射光學元件Μ加以反轉之圖= )。此外,為簡化說明,第23圖中所顯示的,係減少基本 繞射光學元件及補全繞射光學元件中所含凹 口丨刀〈條數 30 200405426 的狀態。實際上,光學元件之外形,最好是能設定成以一 對凹凸作為1節距份,包含5節距以上之凹凸圖案。 另方面,相位差為π / 2之第1補全繞射光學元件 G2,係將基本繞射光學元件G1之圖案,移動凹凸圖案之節 距P的1/4而獲得。又,相位差為3疋/ 2之第3補全繞 射光學元件G4,係將基本繞射光學元件以之圖案,移動 3P/4而獲得。亦即,第3補全繞射光學元件G4 ,具有將 第1補全繞射光學元件G2在相位上反轉之圖案。此外,各 光學元件G1〜G4,冑具有正方形之外形(交界)、彼此具有% 大致相同的大小。 第4實施形中,基本繞射光學元件G1及第1〜第3補 全繞射光學元件G2〜G4分別產生之光束強度分佈(光的發 散方向及強度)雖然相同,但僅有規定該強度分佈之光振 幅的相位部分不同。如此,藉由隨機混合強度分佈相同且 相位彼此相異之4種光束,即能大幅降低規則的干涉雜訊 〇 參照第24圖可知,第4實施形態之繞射光學元件64 I ’係由縱橫且緊密排列之多數個基本繞射光學元件與第 1補全繞射光學元件G2與第2補全繞射光學元件G3與第3 補全繞射光學元件G4所構成。又,各元件G1〜G4彼此大 致為同數,於繞射光學元件64之矩形有效區域(有效直徑 )64a之全體隨機配置。 各元件G1〜G4之隨機配置,係如第2 5圖所示,使(3, 2,1,0)隨基數序列之〇對應基本繞射光學元件gi、1對 31 200405426 應第1補全繞射光學元件G2、2對應第2補全繞射光學元 件G3、3對應第3補全繞射光學元件G4,以製作隨機數表 。此處,作為隨機數序列,係選擇分別包含大致同數之〇 〜3之數字者來使用。然後,根據所作成之隨機數表來排 列各元件G1〜G4之圖案,而獲得如第24圖所示之繞射光 學元件64之構成。In the first and second embodiments, if the phase of the light beam generated by the basic diffractive optical element (Al, Bl, Dl, E1) is zero phase, the diffractive optical element (A2, B2, D2) is completed. The phase of the beam produced by E2) is the 7Γ phase. In other words, the complementary diffractive optical element (A2, B2, E2) is set to the amplitude of the light it generates, and the Phase difference. In contrast to this, the fourth embodiment is set such that if the phase of the light beam generated by the basic diffractive optical element 〇1 is 0 phase, the light beams generated by the first to third complementary diffractive optical elements G2 to G4 are The phases are redundant / 2 phase, | 7Γ phase, and 3 7Γ / 2 phase, respectively. At this time, the basic diffractive optical element G1 has, for example, the same pattern as the basic diffractive optical element A1 of the first embodiment. The second complementary final optical element G3 has, for example, the same pattern as the complementary diffractive optical element A2 of the first embodiment (a figure in which the basic diffractive optical element M is inverted =). In addition, in order to simplify the explanation, the state shown in FIG. 23 is to reduce the number of notches included in the basic diffractive optical element and complete the diffractive optical element <number of strips 30 200405426. In fact, it is desirable that the outer shape of the optical element can be set to have a pair of irregularities as one pitch and include an uneven pattern of 5 pitches or more. On the other hand, the first complementary diffractive optical element G2 with a phase difference of π / 2 is obtained by shifting the pattern of the basic diffractive optical element G1 by 1/4 of the pitch P of the concave-convex pattern. The third complementary diffractive optical element G4 having a phase difference of 3 疋 / 2 is obtained by moving the basic diffractive optical element in a pattern by 3P / 4. That is, the third complementary diffractive optical element G4 has a pattern in which the first complementary diffractive optical element G2 is inverted in phase. In addition, each of the optical elements G1 to G4 has a shape other than a square (boundary), and has approximately the same size as each other. In the fourth embodiment, although the light beam intensity distributions (direction and intensity of light divergence) generated by the basic diffractive optical elements G1 and the first to third complementary diffractive optical elements G2 to G4 are the same, only the intensity is specified. The phase portions of the distributed light amplitudes are different. In this way, by randomly mixing four kinds of light beams with the same intensity distribution and different phases, the regular interference noise can be greatly reduced. Referring to FIG. 24, it can be seen that the diffractive optical element 64 I 'of the fourth embodiment is formed by vertical and horizontal directions. A plurality of basic diffraction optical elements, a first complementary diffraction optical element G2, a second complementary diffraction optical element G3, and a third complementary diffraction optical element G4, which are closely arranged, are formed. Each of the elements G1 to G4 has approximately the same number as each other, and is randomly arranged in the entire rectangular effective area (effective diameter) 64a of the diffractive optical element 64. The random arrangement of each element G1 ~ G4 is shown in Fig. 25, so that (3, 2, 1, 0) corresponds to the basic diffractive optical element gi, 1 pair 31 with the cardinal sequence 0 200405426 should be completed first The diffractive optical elements G2 and 2 correspond to the second complementary diffractive optical element G3 and 3 correspond to the third complementary diffractive optical element G4 to make a random number table. Here, as the random number sequence, those having numbers of approximately 0 to 3 are selected and used. Then, the patterns of the elements G1 to G4 are arranged according to the created random number table, and the structure of the diffractive optical element 64 shown in Fig. 24 is obtained.

第1圖之曝光裝置中,在複數極照明用繞射光學元件 6之位置設置第4實施形之繞射光學元件6 4,將平行光束 射入此繞射光學元件64時,即能在微透鏡8之入射面獲得 如第26圖所示之2點狀光強度分佈。因此,第4實施形態 中,於微透鏡陣列8之入射面,係如第27圖或第28圖所 示’形成由2點狀光強度分佈與圓形或正六角形光束之捲 積所構成之2極狀照明分佈(照野)。In the exposure device of FIG. 1, the fourth embodiment of the diffractive optical element 64 is provided at the position of the diffractive optical element 6 for multiple-pole illumination. When a parallel light beam is incident on this diffractive optical element 64, the The incident surface of the lens 8 obtains a two-point light intensity distribution as shown in FIG. 26. Therefore, in the fourth embodiment, as shown in FIG. 27 or 28, the incident surface of the microlens array 8 is formed by a convolution of a two-point light intensity distribution and a circular or regular hexagonal beam. 2Polar illumination distribution (illumination field).

其結果,於微透鏡陣列8之後側焦點面(照明光瞳面) 办成具有與2極狀照野大致相同光強度分佈之2極狀二次 光源。如此,第4實施形態,藉由繞射光學元件64之作用 ’於照明光瞳面形成實質上均勻的2極狀二次光源。 第4實施形態中,可藉由改變無焦點變焦透鏡5之倍 率,在構成2極狀二次光源之各面光源中心與光軸AX之距 離不變的情形下,僅使各面光源之大小變化。另一方面, 可藉由改變可變焦透鏡7之焦距,來變化上述距離及大小 雙方,使2極狀二次光源全體相似的放大或縮小。 又,第4實施形態中,由於基本繞射光學元件G1具有 與第1實施形態之基本繞射光學元件A1相同的圖案,因此 32 200405426 挾著光軸ΑΧ於X方向形成對稱的2極狀二次光源。缺而 在基本繞射光學元件G1具有與第i實施形態之基本结 學元件B&quot;目同的圖案時,可挾著光軸AUZ方向:成對 稱的2極狀二次光源。再者,本繞射光學元件^具有與第 2實施形態之基本繞射光學元件M或π相同的圖案時, 可挾著光幸“X、在對X方向成45度之方向形成對稱的2 極狀二次光源。 又,第4實施形態,雖係針對基本繞射光學元件與補 全繞射光學元件合計共4種相位隨機配置之情形作了說明 ,但並不限於此,可進一步增加相位種類(進一步增加補 全繞射光學元件之種類數),來進行更為均勻的照明。一 般來說,對1個基本繞射光學元件設定相位不同的複數個 補全繞射光學元件時,為提昇降低干涉雜訊之效果,最好 是能大致以等間隔變化相位差。As a result, a side focus surface (illumination pupil surface) behind the microlens array 8 is a bipolar secondary light source having a light intensity distribution approximately the same as that of the bipolar field. As described above, in the fourth embodiment, a substantially uniform bipolar secondary light source is formed on the illumination pupil surface by the action of the diffractive optical element 64 '. In the fourth embodiment, by changing the magnification of the non-focus zoom lens 5, when the distance between the center of each surface light source and the optical axis AX constituting the bipolar secondary light source is not changed, only the size of each surface light source can be made. Variety. On the other hand, by changing the focal length of the variable-focus lens 7, both the above-mentioned distance and size can be changed, so that the entirety of the bipolar secondary light source can be similarly enlarged or reduced. In addition, in the fourth embodiment, the basic diffractive optical element G1 has the same pattern as the basic diffractive optical element A1 of the first embodiment, so 32 200405426 forms a symmetrical two-pole dipole in the X direction around the optical axis AX. Secondary light source. When the basic diffractive optical element G1 has the same pattern as the basic structure element B &quot; of the i-th embodiment, the optical axis can be oriented in the direction of the optical axis AUZ: a pair of bipolar secondary light sources. In addition, when the present diffractive optical element ^ has the same pattern as the basic diffractive optical element M or π of the second embodiment, it is possible to hold a light beam "X, and form symmetrical two poles at a direction of 45 degrees to the X direction." In the fourth embodiment, the case where the basic diffraction optical element and the complementary diffraction optical element are randomly arranged in a total of four phases has been described, but it is not limited to this, and the phase can be further increased. Type (further increase the number of types of complementary diffractive optical elements) for more uniform illumination. In general, when a plurality of complementary diffractive optical elements with different phases are set for one basic diffractive optical element, To improve the effect of reducing interference noise, it is best to change the phase difference at approximately equal intervals.

如第1實施形悲〜第3實施形態般’補全繞射光學元 件為1種時,最好是能對基本繞射光學元件使補全繞射光 學元件之相位偏移7Γ,藉由基本繞射光學元件與補全繞射 光學元件之隨機排列,可達成最低限之隨基相位效果。此 時’具有補全繞射光學元件之種類少、圖案化較輕鬆的優 點。又’複數種補全繞射光學元件之設定方法,亦可適用 於上述第1實施形態〜第3實施形態。 如上述般,在照明光瞳面形成複數極狀之二次光源時 ,較為理想的是,構成二次光源之各面光源的光強度分佈 為高頂帽(top-hat)狀。然而,實際上,會因繞射而在周邊 33 2⑻405426 (邊緣)發生光強度緩緩降低的現象。特 (Llne/,之繞射的影響㈣,需盡可能的降= 於先^70件本㈣期性之—次光所造成的周邊變 子 亦即’例如第工實施形態之繞射元件(區塊 4圖所示,係…之週期性配置。 =As in the first embodiment to the third embodiment, when there is only one type of complementary diffractive optical element, it is preferable to shift the phase of the complementary diffractive optical element by 7Γ to the basic diffractive optical element. The random arrangement of the diffractive optical element and the complementary diffractive optical element can achieve the minimum effect of the base phase. In this case, '' has the advantages of fewer types of complementary diffractive optical elements and easier patterning. Also, a plurality of setting methods of the complementary diffractive optical element can be applied to the first to third embodiments described above. As described above, when a plurality of polar secondary light sources are formed on the illumination pupil surface, it is preferable that the light intensity distribution of each surface light source constituting the secondary light source is top-hat. However, in practice, a phenomenon that the light intensity gradually decreases in the periphery 33 2⑻405426 (edge) due to diffraction. (Llne /, the influence of diffraction, you need to reduce as much as possible = before ^ 70 pieces of this period-the peripheral variables caused by the secondary light, that is, for example, the diffraction element of the first embodiment ( Figure 4 shows the periodic configuration of ...

照明成份,係負責Z方向照明成份之繞射元件=向: 即,例如就X方向來看B1要素完全沒有任何幫助,就2方 向來看AU素完全沒有任何幫助。換句話說,例如僅就X 方向來考量的話,可將C1元件視㈣部分被完全遮光的 圖案。因此,例如就X方向考量時,C1元件係作用為,且 有L大小之A1圖案與具有L大小之遮光部分的_對,以 2L之週期配置的黑白型繞射元件,本質上會產生因此造成 的附加繞射成份。此點就Z方向而言亦完全相同。 由於此種附加繞射成份係周邊變暗的主要因素,因此 必須將其壓抑至一定值以下。此處,第29圖,係以示意方 式顯示構成複數極狀二次光源之各面光源光強度輪廓的圖 。該圖中,假設沒有附加繞射成份時僅有以M所示之主成 份成為最後的面光源分佈,但實際上,以s所示之附加繞 射成份會產生繞射份之移動而重疊於主成份M,成為真邊 變暗的主要因素。此外,該圖中,s係例示附加繞射成份 之+ 1次成份,實際上亦產生一1次成份及高次成份。然而 ,關於高次成份之幫助小,因此,此處僅考慮丨次成份即 足夠。又’由於繞射光係對稱產生,因此此處僅考慮絕對 值(例如僅考慮+ 1次成份)即可。 34 200405426 附加性繞射成份s(+1次成份)之繞射角Θι,可假言λ 性的考!以上述原理之2L為節距的黑白繞射元件,以下列 基本式(3a)來加以預估。 2Lsin6&gt; != λ ··· (3a) 此處,;I係照明光波長。再者,若設可變焦透鏡7之 焦距為f的話’因附加性繞射成份所造成之偏移量&amp; 以下式(3b)算出。 △ x= fsin0 1= f λ / (2L) …(3b)The lighting component is the diffractive element responsible for the lighting component in the Z direction = direction: That is, for example, the B1 element in the X direction is not helpful at all, and the AU element in the 2 direction is not at all helpful. In other words, for example, considering only the X direction, a pattern in which the C1 element is completely shielded from view can be used. Therefore, for example, when considering the X direction, the C1 element functions as a black-and-white diffractive element with a L-sized A1 pattern and a L-shaped light-shielding portion. A black-and-white diffractive element arranged at a period of 2L will essentially produce this. Caused by additional diffraction components. This point is also exactly the same in terms of the Z direction. Since this additional diffractive component is the main factor for the surrounding darkening, it must be suppressed below a certain value. Here, Fig. 29 is a diagram schematically showing a light intensity profile of each surface light source constituting a plurality of polar secondary light sources. In this figure, it is assumed that when there is no additional diffractive component, only the main component indicated by M becomes the final surface light source distribution, but in fact, the additional diffractive component indicated by s will cause the diffraction component to move and overlap with The principal component M becomes the main factor for the darkening of the true edge. In addition, in the figure, s is an example of the + 1st component of the additional diffraction component. In fact, a 1st component and a higher-order component are also generated. However, the help on high-order components is small, so it is sufficient to consider only high-order components here. Since the diffracted light is generated symmetrically, only the absolute value (for example, only the + 1st order component) is considered here. 34 200405426 The diffraction angle Θι of the additional diffraction component s (+1 order component) can be hypothesized. The black-and-white diffractive element based on the above-mentioned 2L pitch is estimated by the following basic formula (3a). 2Lsin6 &gt;! = Λ ··· (3a) Here, I is the wavelength of the illumination light. In addition, if the focal length of the variable focus lens 7 is set to f ', the amount of shift due to the additional diffraction component will be calculated by the following formula (3b). △ x = fsin0 1 = f λ / (2L)… (3b)

二》上式(3b)中,fsin^係代入式(3a)所預估之數來加以 計算。此偏移量越小,附加性繞射成份的影響越小。 △ X之容許量,只要是在原來主成份Μ之面光源大小必(直 徑)之1/5以下的話,即能進行良好的照明。此條件,以 下式(3c)定義之。 f λ /(2L)&lt; φ /5 ... (3c) 又,各實施形悲中,為了使複數極狀二次光源之照度 對比良好,最好是能將繞射光學元件6(61〜64)定位成構 成作為發散光束形成元件之繞射光學元件4所對應的要素 光束中,至少包含4個光學元件。又,在使用微透鏡陣列 4a來作為發散光束形成元件時,亦最好是能將繞射光學元 件6(61〜64)定位成各光學要素(各微小透鏡要素)所對應 的要素光束中,至少包含4個光學元件。 又,上述第1實施形態〜第3實施形態中,具備於繞 射光學元件全體隨機排列之複數個區塊,各區塊中2種光 學元件同數交互排列。此排列方法中,由於導入了部分的 35 200405426 規則性,因此能在加強方向性(directivity)之同時、實現 實質上不會發生干涉雜訊程度之因隨機相位效果所帶來之 照度不均的平均化。 不過,並不限於上述排列方法,在第1實施形態〜第 3實施形態中亦能與第4實施形態同樣的,將各光學元件 於繞射光學元件全體隨機排列。又,繞射光學元件具備複 數個£塊’於各區塊中隨機排列多數之光學元件亦可。此 時’各種光學元件以彼此大致為同數者較佳。又,繞射光 學元件具備複數種區塊,各種區塊之各個的隨機排列形態 不同者較佳。 其次,參照第1實施形態,具體說明部分隨機配置。 第34圖,係概略顯示為了以微影法製造繞射光學元件所使 用之光罩之構成的圖。又,第35圖,係顯示使用第34圖 之光罩,在玻璃基板上製成之繞射光學元件的圖。參照第 34圖可知,於光罩中央,例如以EB描繪方式,形成有2 個區塊圖案AAP1及AAP2。 一在區塊圖案AAP1内,分別各有1〇〇個第j至第4區部 凡件Cl,C2,C3,C4,於區塊全體隨機排列。區塊圖莽 ΑΑΡ1之隨機排列規貝丨卜例如係使用與帛25 $相同之隨招 數序列同樣的’區塊圖案AAP2内,亦隨機分別配置有 100個第1至第4區塊元件C1 LZ,C3,C4。不過,區均 圖案AAP2隨機排列之規則,盥 (he塊圖案AAP1之隨機排列 圖案不同。亦即,區塊圖幸A AP9 2么^ ” AAP2 ’係使用與區塊圖案AAP] 所使用之隨機數序列不同排 〜的隧機數序列,來進行隨機 36 200405426 排列。 在光罩周邊,繪有3個對準標記am。對準標記⑽,係 將區塊圖案AAP1及區塊圖案AAP2以縮小投影曝光方式曝 光至塗有光阻之玻璃基板上時的位置基準。此外,於^罩 上,繪有一對切斷用引導圖案(引導窗)(^。切斷用引導窗 GP,係用來標示用以將繞射光學元件切斷成既定形狀的切 斷線。 又,於光罩上,作為用來控制線寬及蝕刻深度之控制 用規則圖案,例如形成有線與空間圖案Ls。亦即,圖案^ ,係内部包含線寬2μιη左右之直線狀線與空間圖案的測試 圖案,在區塊圖案ΑΑΡ1與ΑΑΡ2之曝光前後,將此圖案^ 印在繞射光學元件之有效直徑外側,用於線寬控㈣ 深度控制。 ^ 第35圖所示之繞射光學元件,係使用第34圖之光 ’對區塊圖案刪與峨彼此交錯的進行4χΐ2次的曝 光後,予以顯影及蝕刻所得者。以此方式製成之繞射光學 元件’於其有效直徑全體元件並非隨機配置,而係所^ 部分隨機配置。此種部分隨機配置,由於在彼此排列:里 之各區塊内元件為隨機配置’以及準分子雷射之干涉性有 限,因此=揮既定的光學性能。又,能以一片標線片原 板(光罩)簡單、且便宜的製造繞射光學元件。 ’、 又’為了針對干涉雜訊達成較高的降低效果, 區塊圖案ΑΑΡ1與ΑΑΡ2外,最好是能再適當準備ΑΑΡ3 Α綱,…等内部隨機排列相異之其他區塊圖案。然後,將 200405426 所有的區塊依序曝光至繞射光學元件 々杂 精由顯影及蝕刻 之實施,即能製造如第5圖所示之於有 心孓有效直控全體元件 C2,C3,C4隨機排列之繞射光學元件。In "2" above formula (3b), fsin ^ is calculated by substituting the estimated value in formula (3a). The smaller this offset, the smaller the effect of the additional diffraction component. As long as the allowable amount of △ X is less than 1/5 (diameter) of the surface light source of the original main component M, good lighting can be achieved. This condition is defined by the following formula (3c). f λ / (2L) &lt; φ / 5 ... (3c) In each embodiment, in order to make the illuminance contrast of the multiple polar secondary light sources good, it is better that the diffractive optical element 6 (61 ~ 64) The element beam corresponding to the diffractive optical element 4 as the divergent beam forming element is positioned so as to include at least four optical elements. When using the microlens array 4a as the divergent beam forming element, it is also preferable that the diffractive optical element 6 (61 to 64) can be positioned as an element beam corresponding to each optical element (each microlens element). Contains at least 4 optical elements. The first to third embodiments described above include a plurality of blocks randomly arranged in the entire diffractive optical element, and two types of optical elements in each block are alternately arranged in the same number. In this arranging method, because part of the 35 200405426 regularity is introduced, it is possible to enhance the directivity while realizing the non-uniformity of the illuminance unevenness caused by the random phase effect that does not substantially interfere with the noise level. Averaging. However, the present invention is not limited to the above-mentioned arrangement method. In the first to third embodiments, as in the fourth embodiment, each optical element can be randomly arranged over the entire diffractive optical element. Further, the diffractive optical element may include a plurality of optical elements in which a plurality of £ blocks are randomly arranged in each block. In this case, it is preferable that the various optical elements are approximately the same as each other. In addition, the diffractive optical element has a plurality of types of blocks, and it is preferable that the random arrangement of each of the various blocks is different. Next, a partial random arrangement will be specifically described with reference to the first embodiment. Fig. 34 is a diagram schematically showing a configuration of a photomask used for manufacturing a diffractive optical element by a lithography method. Fig. 35 is a view showing a diffractive optical element made on a glass substrate using the photomask of Fig. 34. Referring to FIG. 34, it can be seen that two block patterns AAP1 and AAP2 are formed in the center of the mask, for example, in the EB drawing method. First, in the block pattern AAP1, there are 100 jth to 4th section parts, respectively. Each piece Cl, C2, C3, C4 is randomly arranged in the whole block. The random arrangement of the block diagram AAP1, for example, uses the same 'block pattern AAP2 as the same sequence of tricks as $ 25 $, and 100 random first to fourth block elements C1 LZ are also randomly arranged. , C3, C4. However, the rules of random arrangement of the area average pattern AAP2 are different. The random arrangement pattern of the block pattern AAP1 is different. That is, the block map is A AP9 2? ^ "AAP2 'is used in random with the block pattern AAP]. The sequence of the number of tunnels in different rows ~ is randomly arranged. 2004200426. There are 3 alignment marks am drawn around the mask. The alignment mark ⑽ is to reduce the block pattern AAP1 and the block pattern AAP2. Position reference when projecting to a photoresist-coated glass substrate by projection exposure method. In addition, a pair of cutting guide patterns (guide windows) (^. Cutting guide windows GP) are drawn on the cover. Marking is used to cut the diffractive optical element into a predetermined shape. Also, on the photomask, as a regular pattern for controlling the line width and etching depth, for example, forming a line and space pattern Ls. That is, The pattern ^ is a test pattern containing linear lines and space patterns with a line width of about 2 μm. The pattern ^ is printed on the outside of the effective diameter of the diffractive optical element before and after the block pattern AAP1 and AAP2 are exposed. line Wide control ㈣ Depth control. ^ The diffractive optical element shown in Figure 35 is obtained by using the light of Figure 34 to perform 4 × 区块 2 exposures of the block pattern and the staggered pattern, and then develop and etch it. The diffractive optical element made in this way is not randomly arranged in its effective diameter, but all the elements are randomly arranged. This kind of random arrangement is due to the arrangement of each other: the elements in each block are randomly arranged. 'And the interference of excimer lasers is limited, so it has a predetermined optical performance. Moreover, it is possible to manufacture a diffractive optical element with a reticle original plate (reticle) simply and cheaply. The noise achieves a high reduction effect. In addition to the block patterns AAP1 and ΑAP2, it is best to prepare ΑΑΡ3 Α 纲, and other random block patterns with different internal random arrangements. Then, all the blocks in 200405426 are divided according to Sequential exposure to diffractive optical elements is performed by development and etching, that is, as shown in Fig. 5, it is possible to directly control all elements C2, C3, and C4 randomly arranged around the core as shown in Figure 5.射 optical components.

此外,若無法將所有的區塊圖案皆配置在第34圖之光 罩上時’在其他之1個或複數個光罩上騎剩餘的區塊圖 案,依序交換光罩以將所有區塊圖案曝光至玻璃基板上, 亦能製造繞射光學元件。又’上述以第34圖、第Μ圖為 例所說明之部㈣機配置*成的繞射光學元件圖案化方法 ’並不限於第1實施形態’而能適用於本發明之所有實施 形態。亦即’在各實施形態中’可製造與第34圖相同之繞 射光學元件之光罩,而使用該光罩來製造與第35圖相同2 部分隨機目案化之繞射光學元件。χ,本發明&lt;所有實施 形態中,作業將繞射光學元件圖案化之基板材料,可使用 例如合成石英、水晶、螢石等。 此外,上述各實施形態及變形例中,可將直線光柵圖In addition, if it is not possible to arrange all the block patterns on the mask in Fig. 34, ride the remaining block patterns on one or more other masks, and sequentially exchange the masks to place all the blocks. The pattern is also exposed on a glass substrate, and a diffractive optical element can also be manufactured. Also, "The above-mentioned method of patterning the diffractive optical element using the configuration of the partial machine illustrated in Fig. 34 and Fig. M as an example" is not limited to the first embodiment and can be applied to all embodiments of the present invention. That is, "in each embodiment", a mask of the same diffractive optical element as that shown in Fig. 34 can be manufactured, and this mask can be used to manufacture a diffractive optical element that is randomized into two parts as in Fig. 35. χ, in all embodiments of the present invention, a substrate material for patterning a diffractive optical element is used, and synthetic quartz, crystal, fluorite, etc. can be used. In addition, in each of the above embodiments and modifications, a linear raster image

案之週期(節距)p設定成〇.1μιη〜25〇μιη程度,將基本繞射 光學元件及補全繞射光學元件有效直徑之面積設定成7帅 Χ5μιη〜1〇〇〇μιηΧΐ〇〇〇μιη程度,將繞射光學元件之有效直 徑内基本繞射光學元件及補全繞射光學元件之數量設為約 10個以上。 又,第1圖所示之曝光裝置,為形成複數極狀二次光 源係使用波面分割型光學積分器之微透鏡陣列8,但亦可 取代此微透鏡陣列8而使用内面反射型光學積分器之棒狀 積分器。第30圖,係概略顯示於第}圖之曝光裝置中,取 38 200405426 代微透鏡陣列而使用棒狀積分器時之主要部構成的圖。 參照第30圖可知,因庫 因應取代锨透鏡陣列δ而配置棒狀 積刀盗81,在可變焦透鏡7與棒狀積分器Μ間之光 1輸入透鏡82,在棒狀積分器81與聚光光學系統9間 之光程中配置了中繼透鏡83。此處,第30_示 對應第1圖之微透鏡陣列8之人射面,第3〇圖所示之^ 則對應第1圖之微透鏡陣列8之射出面。 棒狀積分器8卜係由石英玻璃或榮石等之玻璃材質所 構成之内面反射型玻璃棒,利用内部與外部之交界 利用在内面之全反射’通過聚光點沿著與棒入射面平行 面’形成對應内面反射數之數量的光源。此處,所形成之 先源雖幾乎皆為虛像,但僅中心(聚光點)光源為實像。亦 即射入棒狀積分器81之光束因内面反射而被分割於角声 方向’通過聚光點沿著與棒入射面平行之面,形成由多數 光源構成之二次光源。 因此,通過繞射光學元件6(61〜64)之光束纟a面來 錢數極狀之照野後,透過“⑽_聚光在棒狀❹f = 之入射面81a附近。如此,來自二次光源(藉由棒狀 81在其人射面形成之複數極狀之二次光源)之光束 ,在其射出面81b重疊後,透過中繼透鏡83及聚光光學系 統9,而重疊照明形成有既定圖案之標線片(光罩)13。 ' 、又,亦可取下中繼透鏡83及聚光光學系統9,將棒狀 積分器81之射出面81b設在標線片13附近。或者,亦可 取下可變焦透鏡7及輸入透鏡82,將棒狀積分器81之入 39 200405426 射面81a设在繞射光學元件6(61〜64)之射出面附近,且 將棒狀積分器81之射出面81b設在標線片13附近。 又’亦可在第1圖所示之曝光裝置中,在光源1與作 為發散光束形成元件之繞射光學元件4間之光程中,附設 例如日本專利特開平9-205060號公報、特開平M-125585 波公報、特開2000-277421號公報等所揭示之光延遲系統 。以下’簡單說明在彎折鏡3與繞射光學元件4間之光程 中附設光延遲系統之情形。 此時’透過整形光學系統2及彎折鏡3被變換成期望 截面形狀之光束,射入由全反射鏡與部分反射鏡所構成之 光延遲系統。光延遲系統中,透射過部分反射鏡之部分光 束射入繞射光學元件4,而被部分反射鏡所反射之其他光 束則射入全反射鏡。被全反射鏡反射之光束射入部分反射 、兄透射過邛为反射鏡之部分光束射入繞射光學元件4, 被部分反射鏡反射之其他光束則射入全反射鏡。 如此,光延遲系統,藉由在全反射鏡與部分反射鏡間 反稷進仃之多重反射,將入射光束依序轉換成被延遲的多 數個光束群。其結果,^能藉由光延遲系統之作用,降低 j晶圓共軛面之干涉雜訊。又,關於光延遲系統進一步的 评細構成及作用,可參照例如特開平9 — 2〇5〇6〇號公報、特 開平10-125585號公報、特開2〇〇〇_277421號公報。 又,上述各實施形態中 件圖案,但並不限於此,刃 案或多元型繞射光學元件。 T ’雖係使用2元型繞射光學元 亦可使用閃耀型繞射光學元件圖 。以下,參照第31A圖〜第31c 200405426 圖對閃耀型繞射光學元件圖案、多元型繞射光學元件、 以及2元型繞射光學元件作一般性的說明。 、第31A圖係將閃耀型繞射光學元件於其周期方向截面 :以切斷的截面圖,第31B圖係將多元型繞射光學元件於 其周期方向截面加以切斷的截面圖,帛⑽圖係將2元型 繞射光學元件於其周期方向截面加以切斷的截面圖。來昭 第3U圖可知,閃耀型繞射光學元件之切斷面為錯齒狀*、,、、 產生鋸齒狀階之節距P係以式(2)定義之。 又,截面之深度dG,若設基板之折射率為n,配置基 板之氣體的折射率為1的話,係以下式(5 )定義。 d〇= Λ / (η- 1) …⑸ 使用具有此種閃耀型繞射光學元件之基本繞射光學元 件及補全繞射光學㈣是可能的。此時,基本繞射光學元 件及補全繞射光學元件之圖案並非是凸面與凹面之2元型 ’而係截面形狀於高度方向變化之圖帛。在此種高度方向 相異之圖案之製作時’可使用透射率漸漸變化的灰度光罩 (gray scale musk) ° 參照第31B圖可知,多元型繞射光學元件之切斷面, 係使第31A圖之鑛齒狀近似於L層⑽3)之階梯型形狀。 此外,各層之交界處,可藉由將節距p之範圍依據各層之 階(step)區域加以L分割即能容易的規定。第3ΐβ圖,係 顯示L=8之8元相位型繞射光學元件的情形。截面之深度 dL,若設基板折射率為n、配置基板之氣體的折射率為i 的話,係以下式(6)定義。 41 200405426The period (pitch) p of the project is set to the range of 0.1 μm to 25 μm, and the area of the effective diameter of the basic diffractive optical element and the complementary diffractive optical element is set to 7 handsome × 5 μιη to 100 μm μ ×× 〇〇〇〇 μιη, the number of basic diffractive optical elements and complementary diffractive optical elements within the effective diameter of the diffractive optical element is set to about 10 or more. The exposure device shown in FIG. 1 is a microlens array 8 using a wavefront division type optical integrator to form a complex polar secondary light source. However, an internal reflection type optical integrator may be used instead of the microlens array 8. Rod integrator. Fig. 30 is a diagram schematically showing the structure of the main parts when the rod integrator is used in the exposure device shown in Fig.} And a microlens array of 2004200426 is used. Referring to FIG. 30, it can be seen that the rod-shaped product knife 81 is arranged because the library replaces the 锨 lens array δ. The light 1 between the zoom lens 7 and the rod integrator M is input to the lens 82, and the rod integrator 81 and the condenser A relay lens 83 is arranged in the optical path between the optical optical systems 9. Here, Fig. 30_ corresponds to the emission surface of the microlens array 8 of Fig. 1, and ^ shown in Fig. 30 corresponds to the emission surface of the microlens array 8 of Fig. 1. The rod integrator 8 is a reflective glass rod made of glass material such as quartz glass or sapphire. It uses the boundary between the inside and the outside and uses the total reflection on the inside. The planes form a number of light sources corresponding to the number of reflections of the inner plane. Here, although the first sources formed are almost all virtual images, only the central (condensing point) light source is a real image. That is, the light beam incident on the rod integrator 81 is divided into the angular sound direction due to the internal reflection. The secondary light source composed of a plurality of light sources is formed along the plane parallel to the incident surface of the rod through the condensing point. Therefore, after the polarized light field is transmitted through the light beam 面 a side of the diffractive optical element 6 (61 ~ 64), the light beam passes through "⑽_ and is focused near the incident surface 81a of the rod-shaped ❹f =. Thus, from the secondary The light beams (multiple polar secondary light sources formed by the rod-shaped 81 on its projection surface) are superimposed on the emission surface 81b and then transmitted through the relay lens 83 and the condenser optical system 9 to form overlapping illumination. A reticle (photomask) 13 with a predetermined pattern. Also, the relay lens 83 and the condensing optical system 9 may be removed, and the exit surface 81b of the rod integrator 81 may be provided near the reticle 13. Or, The zoom lens 7 and the input lens 82 can also be removed, and the rod-shaped integrator 81 can be inserted into the 200404026. The emission surface 81a is set near the emission surface of the diffractive optical element 6 (61 to 64). The emission surface 81b is provided in the vicinity of the reticle 13. In the exposure apparatus shown in FIG. 1, the optical path between the light source 1 and the diffractive optical element 4 which is a divergent beam forming element may be provided with, for example, Japan. Patent Publication No. 9-205060, Patent Publication No. M-125585, Patent Publication No. 2000-277421, etc. Revealed optical delay system. The following is a brief description of the case where an optical delay system is attached to the optical path between the bending mirror 3 and the diffractive optical element 4. At this time, the transmission optical shaping system 2 and the bending mirror 3 are transformed into expectations. The light beam with a cross-sectional shape enters a light delay system composed of a total reflection mirror and a partial reflection mirror. In the light delay system, a part of the light beam transmitted through the partial reflection mirror enters the diffraction optical element 4 and is reflected by the partial reflection mirror. The other light beams are incident on the total reflection mirror. The light beams reflected by the total reflection mirror are incident on the partial reflection, and the part of the beam transmitted through the mirror is incident on the diffractive optical element 4. The other beams reflected by the partial reflection mirror are incident. In this way, the optical delay system converts the incident beam into a plurality of delayed beam groups in sequence by multiple reflections that are reflected between the total mirror and the partial mirror. As a result, With the effect of the optical delay system, the interference noise of the conjugate surface of the j wafer is reduced. For further details on the composition and effect of the optical delay system, refer to, for example, Japanese Patent Application Laid-Open No. 9-2050 Japanese Patent Application Publication No. 10-125585 and Japanese Patent Application Publication No. 2000-277421. In addition, the pattern in each of the above embodiments is not limited to this, and it is a blade or multi-element diffractive optical element. T ′ Although it is a two-element diffractive optical element, the blazed type diffractive optical element diagram can also be used. Hereinafter, referring to FIGS. 31A to 31c 200405426, the blazed type diffractive optical element pattern, multi-element diffractive optical element, and 2 The elementary diffractive optical element is generally described. Figure 31A is a cross-section of the blazed type diffractive optical element in its periodic direction: in a cut-away cross-sectional view, Figure 31B is a multi-type diffractive optical element A cross-sectional view in which a periodic cross section is cut. A hologram is a cross-sectional view in which a binary diffractive optical element is cut in a periodic cross section. It can be seen from Fig. 3U that the cut surface of the flare-type diffractive optical element is staggered * ,,,, and the pitch P that generates the zigzag order is defined by Equation (2). The depth dG of the cross section is defined by the following formula (5) if the refractive index of the substrate is n and the refractive index of the gas in which the substrate is disposed is 1. d〇 = Λ / (η-1)… ⑸ It is possible to use a basic diffractive optical element having such a blazed type diffractive optical element and a complementary diffractive optical ㈣. At this time, the pattern of the basic diffractive optical element and the complementary diffractive optical element is not a two-element pattern of convex and concave surfaces ′, but is a diagram in which the cross-sectional shape changes in the height direction. In the production of such patterns with different height directions, 'a gray scale musk with gradually decreasing transmittance can be used.' Referring to FIG. 31B, it can be seen that the cut surface of the multi-element diffractive optical element is the first The dentate shape of Figure 31A is similar to the stepped shape of L layer⑽3). In addition, the boundary of each layer can be easily specified by dividing the range of the pitch p according to the step area of each layer by L division. Figure 3ΐβ shows the case of an 8-element phase-type diffractive optical element with L = 8. The depth dL of the cross section is defined by the following formula (6) if the refractive index of the substrate is n and the refractive index of the gas in which the substrate is disposed is i. 41 200405426

dT η- 1) } (6) λ (L- 1)/ { 使用具有此種多元型繞射光學元件之基本繞射光學元 件及補全繞射光學元件是可能的。此時,基本繞射光學元 件及補全繞射光學元件之圖案並非是凸面與凹面之2元型 ,而係截面形狀為階梯形、於高度方向變化之圖案。在此 種高度方向相異之圖案之製作時,可使用透射率步進且多 階段變化的灰度光罩。 參照第31C圖可知,2元型繞射光學元件之切斷面, 係近似於第31Β圖之階梯型而L=2時之形狀。亦即,2元 型繞射光學元件之切斷面,如第31c圖所示,係於厚度廿 方向以凸區域部分與凹區域部分之2種段差所示之矩形圖 案。各矩形區域之交界處,可藉由ρ/2來加以定義。又, 截面之M d2,若設基板折射率為η、配置基板之氣體的 折射率為1的話,係以下式(7)定義。 (7) 己2= λ / { 2 (η- 1) } 又’上各實施形態及變形例中’實現了具備基本繞射 先學疋件之繞射光學元件(該基本繞射光學元件,呈 圖案(將直線光栅狀繞射光學元件圖案根據既定方位' 以設定之圖案)緊密排列所得之圖案)。然而, 口 此繞射光學元件相同光學性能之光學構件,亦可實備 基本折射元件之折射光學元件(該基本折射元件,呈: 稜鏡狀折射面(根據既定方位角力口以設定者二 所得之折射面圖案)。 -雄排列 具體而言,可實現將閃耀型繞射光學元件的繞射角置 42 換為微折射元件(微稜 _ ό 專)之折射元件的折射角。可蔣+ 種折射元件緊密排列 斤射角了將此 —入^ 匕a既疋方位角成份。不過,作a 兀王的折射元件加以緊密排列 … 恭“Q、旦 J的δ舌,由於在玻璃蝕刻時的 化。木將波長份相位差視為等價之段差構造,來進行圖案 =折射光學元件之製造,係在進行基本折射元件之 ^將忒圖案轉換成微折射元件製造用之光罩(灰 度光罩等)圖案,將該光罩圖案曝光至塗有光阻之玻璃基t 板,再進行顯影及蝕刻。 生接著,簡單說明各實施形態之繞射光學元件典型的製 化=序。首先,根據從既定光源至最後段(最靠近光罩側) 之光學積分器(各實施形態中為微透鏡陣列8)中所含之中 繼透鏡之焦距與光束有纟直徑肖光源波長與發散光束形成 凡件之發散角的關係,設定直線光栅狀繞射光學元件之節 距。然後,依照期望之照明方式設定既定方位角,且設定 基本繞射光學元件之有效直徑。此時,係將基本繞射光學| 元件之有效直徑設定成要素光束(對應構成發散光束形成 凡件之各光學要素)中包含複數個基本繞射光學元件或補 全繞射光學元件。 其次’將直線光栅狀繞射光學元件設定於既定方位角 ’以設定基本繞射光學元件之圖案。進一步的,設定1個 或複數個補全繞射光學元件之圖案,其所產生之強度分佈 與基本繞射光學元件相同、且相位與基本繞射光學元件不 43 200405426 同。並設定將以此方式所得之基本繞射光學元件與1種或 複數種補全繞射光學元件,分別大致同數統合於有效直徑 内之繞射光學元件的圖案。 此時’係將基本繞射光學元件及補全繞射光學元件之 排列位置予以隨機化(全體隨機或部分隨機)。對以此方式 圖案化之繞射光學元件進行波動光學模擬,將基本繞射光 學元件之節距及補全繞射光學元件之相位及該相位之種類 等加以最佳化。接著’ A照被最佳化之繞射光學元件之圖 案製造標線片(光罩),使用此標線片將圖案轉印至塗有光% 阻之玻璃基板。之後,進行顯影製程、蚀刻製程、及形成 AR(反射防止)層之製程。 上述各實施形恶’係使用具有此種2元型繞射光學元 件圖案之基本繞射光學元件及補全繞射光學元件。此時, 可使用所謂之黑白型(僅透射部與遮光部)光罩。又,作將 、、凡射光學7L件圖案化之基板之材料,可使用例如合成石英 、水晶、螢石等。 《第5實施形態》 第1實施形態係藉由繞射光學元件61之作用來形成 由挾著光軸AX於X方向對稱配置之2個面光源、與挾著光 軸AXH方向對稱配置之2個面光源所構成的十字形4極 狀照明分佈(二次光源)。相對於此,帛5實施形態,則係 藉由採用區塊元件Cld〜C4d(對繞射光學元件61中所含之 區塊元件C1〜C4附加新的單純透射部),來形成在第丄實 把形%之4極外於光轴上加上J極的5極狀照明分佈。亦 44 200405426 即,第5實施形態係光軸上亦有強度分佈之5極照明的實 施形態。以下,著眼於與第1實施形態之相異處,來說明 第5實施形態。 第36圖,係顯示第5實施形態中,於微透鏡陣列之入 射面形成之5極狀照野的圖。又,第37圖,係用以說明第 5實施形態之5極照明用繞射光學元件之基本作用的圖。 第38圖,係概略顯示第5實施形態之5極照明用繞射光學 元件之全體構成的圖。此外,第39圖,係概略顯示第5實 施形態之5極照明用繞射光學元件中所含之區塊元件之構| 成的圖。 如第38圖所示,第5實施形態之5極照明用繞射光學 元件1〇〇,係由縱橫且緊密排列之多數個區塊元件cid〜 C4d所構成。區塊元件Cld〜C4d,皆具有長方形之外形(交 界),彼此具有大致相同的大小。又,區塊元件cld〜c4d 中各種類大致包含同數,於繞射光學元件丨〇〇之矩形有效dT η- 1)} (6) λ (L-1) / {It is possible to use a basic diffractive optical element and a complementary diffractive optical element with such a multi-type diffractive optical element. At this time, the pattern of the basic diffractive optical element and the complementary diffractive optical element is not a two-element type of convex surface and concave surface, but a pattern in which the cross-sectional shape is stepped and changes in the height direction. In the production of such patterns with different height directions, a gray mask with a step change in transmittance and a multi-step change can be used. Referring to FIG. 31C, it can be seen that the cut surface of the 2-element diffractive optical element is similar to the stepped shape of FIG. 31B and L = 2. That is, as shown in Fig. 31c, the cut surface of the two-dimensional diffractive optical element is a rectangular pattern shown in the thickness 廿 direction with two steps between the convex region portion and the concave region portion. The boundary of each rectangular area can be defined by ρ / 2. The M d2 of the cross section is defined by the following formula (7) if the refractive index of the substrate is η and the refractive index of the gas in which the substrate is disposed is 1. (7) 2 = λ / {2 (η- 1)} and in the above embodiments and modifications, a diffractive optical element (the basic diffractive optical element, A pattern (a pattern obtained by closely aligning a linear grating-shaped diffractive optical element pattern with a set orientation according to a predetermined orientation). However, an optical component with the same optical properties of this diffractive optical element can also be used to prepare a refractive optical element of a basic refractive element (the basic refractive element is: a 折射 -shaped refractive surface (according to a given azimuth force and the set two) (Refracting surface pattern). -Specifically, the male angle can be achieved by changing the diffraction angle of the blazed diffractive optical element to 42 for the refractive angle of the refractive element of the micro-refractive element (micro-edge). 可 蒋 + This kind of refraction elements are closely arranged at the angle of incidence. This means that the azimuth component is included. However, the refraction elements for the king are closely arranged ... Respectively "Q, Dan J's δ tongue, because during glass etching, Wood regards the wavelength phase difference as the equivalent step structure to produce the pattern = refractive optical element, which is performing the basic refractive element ^ converting the chirped pattern into a photomask for the manufacture of micro-refractive elements (gray Photomask, etc.) pattern, and expose the photomask pattern to a glass-based t-plate coated with photoresist, and then develop and etch. Next, a brief description of the typical fabrication of the diffractive optical element of each embodiment is given. First, according to the focal length of the relay lens included in the optical integrator (microlens array 8 in each embodiment) from the predetermined light source to the final stage (closest to the mask side), the beam has the diameter of the light source and the wavelength of the light source. The divergent beam forms the relationship between the divergence angles of all parts, and sets the pitch of the linear grating-shaped diffractive optical element. Then, the predetermined azimuth angle is set according to the desired illumination method, and the effective diameter of the basic diffractive optical element is set. At this time, the Set the effective diameter of the basic diffractive optics | element to the element beam (corresponding to each optical element constituting the divergent beam forming common element) contains a plurality of basic diffractive optical elements or complementary diffractive optical elements. Secondly, The diffractive optical element is set at a predetermined azimuth angle to set the pattern of the basic diffractive optical element. Further, the pattern of one or more complementary diffractive optical elements is set, and the intensity distribution and the basic diffractive optical element produced by the pattern are set. The same, and the phase is different from the basic diffractive optical element 43 200405426. And set the basic diffractive optical element to be obtained in this way The pattern of one or more types of complementary diffractive optical elements is approximately the same as the pattern of the diffractive optical elements integrated within the effective diameter. At this time, 'the arrangement position of the basic diffractive optical element and the complementary diffractive optical element is used. Randomize (random or partially random). Perform wave optical simulations on the diffractive optical elements patterned in this way, the pitch of the basic diffractive optical elements, and the phase of the diffractive optical elements and the types of the phases. Optimize, etc. Then 'A according to the pattern of the optimized diffractive optical element to make a reticle (reticle), use this reticle to transfer the pattern to a glass substrate coated with% light resistance. After that The development process, the etching process, and the process of forming the AR (reflection prevention) layer are performed. Each of the above embodiments uses a basic diffractive optical element having such a binary diffractive optical element pattern and a complementary diffractive optical element. element. In this case, a so-called black-and-white (only transmissive portion and light-shielding portion) mask can be used. In addition, as a material for patterning the 7L pieces of the optical lens, synthetic quartz, crystal, fluorite, etc. can be used. << Fifth Embodiment >> The first embodiment forms two surface light sources arranged symmetrically in the X direction by the optical axis AX and two arranged symmetrically in the direction of the optical axis AXH by the action of the diffractive optical element 61. Cross-shaped 4-pole illumination distribution (secondary light source) composed of individual surface light sources. On the other hand, in the fifth embodiment, the block elements Cld to C4d are used (a new simple transmission part is added to the block elements C1 to C4 included in the diffractive optical element 61) to form the third block. The 4 poles of the shape% are added to the 5-axis illumination distribution of the J pole on the optical axis. Ye 44 200405426 That is, the fifth embodiment is an implementation form of 5-pole illumination that also has an intensity distribution on the optical axis. Hereinafter, the fifth embodiment will be described focusing on differences from the first embodiment. Fig. 36 is a diagram showing a 5-pole field formed on the incident surface of the microlens array in the fifth embodiment. Fig. 37 is a diagram for explaining the basic operation of the diffractive optical element for 5-pole illumination according to the fifth embodiment. Fig. 38 is a diagram schematically showing the entire configuration of a diffractive optical element for 5-pole illumination according to the fifth embodiment. Fig. 39 is a diagram schematically showing the structure of a block element included in the diffractive optical element for 5-pole illumination according to the fifth embodiment. As shown in Fig. 38, the diffractive optical element 100 for 5-pole illumination of the fifth embodiment is composed of a plurality of block elements cid to C4d arranged vertically and horizontally. The block elements Cld to C4d each have a rectangular outer shape (boundary) and have approximately the same size as each other. In addition, the various types of block elements cld ~ c4d include the same number, which is valid for the rectangular shape of the diffractive optical element.

區域(有效直徑)l00a之全體隨機配置、或在將全體分割成 若干個區塊之區塊中隨機配置。 —如第39圖所示,區塊元件Cld〜C4d,分別包含第 形〜中況明之區塊C丨〜C4。例如,區塊元件d d係 -實轭形怨之區塊C1的X方向相鄰配置單純透射部Η :::同樣的,區塊元件C2d係在區塊。2的叉方向相鄰 dl cf射部H的元件。而區塊元件⑶,C4d則係分別 。 的X方向相鄰配置補全單純透射部Hd的元 45 200405426 此處,單純透射部Η及補全單純透射部Hd之目的在於 使入射光單純的透射而直線前進,一般來說,並不在元件 Η及&quot;牛Hd内。卩進行特別微細之圖案化。亦即,單純透射 部H,得、原封不動的留下用纟形成繞射光學元件之玻璃基 板表面的單純平面部分。又,補全單純透射部Hd,係將形 成繞射光學元件之玻璃基板,在元件Hd之有效直徑内㈣ 至以式(1)所示深度d為止的平面部分。The entire area (effective diameter) 100a is randomly arranged, or randomly arranged in a block that divides the whole into several blocks. -As shown in Fig. 39, the block elements Cld ~ C4d include blocks C 丨 ~ C4, respectively, which are shaped from the middle to the middle. For example, the block element d d is a real yoke-shaped block C1 adjacent to the X direction in which a simple transmission part is arranged Η ::: Similarly, the block element C2d is in a block. The cross direction of 2 is adjacent to the element of dl cf emitter H. The block components ⑶ and C4d are respectively. The element 45 that complements the simple transmission part Hd is arranged adjacent to the X direction. 200405426 Here, the purpose of the simple transmission part Η and the completion of the simple transmission part Hd is to make the incident light transmit straight and go straight. Generally, it is not on the element. Within &quot; Bull Hd.特别 Specially fine patterning. That is, the simple transmission portion H leaves a purely flat portion of the surface of the glass substrate on which the diffractive optical element is formed by the ytterbium. In addition, the completion of the simple transmission portion Hd is a flat portion of the glass substrate on which the diffractive optical element is formed, within the effective diameter of the element Hd to a depth d shown in the formula (1).

由於兀件Η及Hd之表面係單純平面狀,因此射入元件 Η及Hd之光,除若干的繞射外皆單純的透射而直線前進。 不^透射過單純透射部Η之光束與透射過補全單純透射 邠Hd之光束’對應段差d而有又/ 2之光程差。亦即,單 純透射部Η係不對玻璃面進行特別加卫的部分,補全單純 透射部Hd則係相對單純透射部Η,僅將玻璃單純的、且均 勻的加以蝕刻既定光程差的元件。 &amp;又,在4極成份之發散角(繞射角不同於第丨實施 形心時可就對應之發散角0,根據式(2)來設定區塊C1 〜C4内所含之元件Α1,Α2, β1,β2之節距,將元^及Since the surfaces of the element Η and Hd are purely planar, the light entering the element Η and Hd, except for a few diffractions, are simply transmitted and proceed straight. The light beam that does not pass through the simple transmission part 与 and the light beam that passes through the complementary simple transmission 邠 Hd ′ corresponds to a step difference d and has an optical path difference of / 2. That is, the simple transmission part Η is a part that does not particularly guard the glass surface, and the complementary simple transmission part Hd is a relatively simple transmission part Η, which is only a simple and uniformly etched glass with a predetermined optical path difference. &amp; At the divergence angle of the 4-pole component (diffraction angle is different from the centroid of the first implementation, the corresponding divergence angle 0 can be set according to equation (2) to set the component A1 contained in the blocks C1 to C4 The pitch of Α2, β1, β2, will be ^ and

Hd組合於其中來設定期望之區塊元件Cld〜C4d,而形成對 應之繞射光學元件。 如以上之說明,使用繞射光學元件100之第5實施形 悲係藉由透射過區塊C1〜C4之光而生成具有既定發散角 之4極成份’同時藉由透射過件Η及Hd之光而生成在光轴 附近/、有強度之i極成份,藉由此等4極成份肖1極成份 之合成即能進行如第36圖所示之5極照明。 习 46 200405426 亦即,將第5實施形態之繞射光學元件ι〇。定位在照 並射入平行光束時,即會在微透鏡陣歹&quot;之入射面 弟37圖所示’形成由十字形4點狀光強度分佈與光轴 附近1點狀光強度分佈所構成之合計5點狀光強度分佈。 然而’與帛1實施形態同樣的,實際上,射人繞射光學元 牛〇的並非疋平仃光束,而係射入具有以錐體形狀(在微 透鏡陣列4a時為正六角錐體形、在繞射光學元件4時則為 圓錐體形)之光束範圍規定之角度成份的光束。如此,在 Μ透鏡陣列8之入射面,如第36圖所示,形成由5點狀光 強度分佈與圓形(或正六角形)光束之捲積所構成之5極狀 照明分佈(照野)。 其結果,微透鏡陣列8之後側焦點面(照明光瞳面), 形成具有與5極狀照野大致相同光強度分佈之5極狀二次 光源。此處,5極狀二次光源,係由5個圓形(或正六角形 )實質的面光源,亦即由挾著光軸ΑΧ於X方向對稱配置之 2個面光源、與挾著光軸^於2方向對稱配置之2個面光 源,以及配置在光軸附近之丨個面光源所構成。如此,在 第5實施形態中,藉由繞射光學元件丨〇〇之作用,於照明 光瞳面形成實質上均勻的5極狀二次光源。 又,第5實施形態與第丨實施形態同樣的,可藉由改 變無焦點變焦透鏡5之倍率’在構成5極狀二次光源之各 面光源中心與光轴AX之距離不變的情形下,僅使各面光源 之大小(4極狀二次光源之外接圓半徑一 4極狀二次光源之 内接圓半徑、以及光軸上1極狀二次光源之直經)變化。另 47 200405426 一方面,可藉由改變可變焦透鏡7之焦距,來變化上述距 離及大小雙方,使5極狀二次光源全體相似的放大或縮小 〇 此外,第5實施形態中,作為區塊元件Cld〜C4d之變 形例,亦可使用如第40圖所示之區塊元件nd〜C4d。區 塊凡件Cld,係將區塊C1及單純透射部H以平行於χ軸之 直線大致對半切斷,如第40圖所示的彼此交互穿插之構成 。區塊元件C2d與區塊元件Cld相同。區塊元件C3d,則 係將區塊C3及補全單純透射部Hd大致對半切斷成與χ軸$ 平行之直線,如第40圖所示的彼此交互穿插構成。使用包 含區塊元件Cld〜C4d(具有上述配置)之繞射光學元件,能 提昇4極照明與光軸附近1極照明成份之照明平衡。同樣 的,將區塊元件Cld〜C4d之内部圖案進一步予以細分化, 將對應4極成份之C1〜C4元件圖案加以細分化後之細分化 要素、與對應光軸附近1極成份之H,Hd區域加以細分化 後之細分化要素,彼此予以不同排列或隨機配置所得之新 的區塊元件,使用此區塊元件即能更進一步的提昇4極照H 明與光軸附近1極照明成份之照明平衡。 又,第5實施形態中,最好是能將區塊C1,C2與單純 透射部Η設定成具有相同面積,將區塊C3,C4與補全單純 透射部Hd設定成具有相同面積。 《第6實施形態》 第2實施形悲係藉由繞射光學元件6 2之作用,來形成 由挾著光軸AX、沿相對+ X方向繞+ γ軸+ 45度方向之 48 200405426 個面光源,與挾著光軸AX、沿相對+ z方向繞+ γ軸一45 度方向之2個面光源所構成的X形4極狀照明分佈(二次光 源)。相對於此,第6實施形態,則係藉由採用區塊元件 Fid〜F4d(對繞射光學元件62中所含之區塊元件F1〜F4附 加新的單純透射部),來形成在第2實施形態之4極外於光 軸上加上1極的5極狀照明分佈。以下,著眼於與第2實 施形態之相異處,來說明第6實施形態。 第41圖,係顯示第6實施形態中,於微透鏡陣列之入 射面形成之5極狀照野的圖。第42圖,係用以說明第6實% 施形態之5極照明用繞射光學元件之基本作用的圖。第43 圖係概略顯示弟6實施形態之5極照明用繞射光學元件 之全體構成的圖。又,第44圖,係概略顯示第6實施形態 之5極照明用繞射光學元件中所含之區塊元件之構成的圖Hd is combined therein to set desired block elements Cld to C4d, thereby forming corresponding diffractive optical elements. As described above, the fifth embodiment using the diffractive optical element 100 generates a 4-pole component having a predetermined divergence angle by transmitting light passing through the blocks C1 to C4, and by transmitting through the element Η and Hd. Light is generated near the optical axis and has an i-pole component with intensity. By combining the 4-pole component and the 1-pole component, the 5-pole illumination shown in FIG. 36 can be performed. Xi 46 200405426 That is, the diffractive optical element ι0 of the fifth embodiment is used. When it is positioned and irradiated into a parallel beam, it will be formed on the incident surface of the microlens array as shown in Figure 37. It consists of a cross-shaped 4-point light intensity distribution and a 1-point light intensity distribution near the optical axis. The total is a 5-point light intensity distribution. However, 'same as the embodiment of 帛 1, in fact, it is not the 疋 flat 仃 beam that radiates the diffracted optical element. Instead, it is incident with a cone shape (in the microlens array 4a, a regular hexagonal cone shape, in the When the diffractive optical element 4 is in the shape of a cone, a light beam having an angular component specified in the light beam range is used. In this way, as shown in FIG. 36 on the incident surface of the M lens array 8, a 5-pole illumination distribution (illumination field) formed by a convolution of a 5-point light intensity distribution and a circular (or regular hexagonal) light beam is formed. . As a result, the focus surface (illumination pupil surface) on the rear side of the microlens array 8 forms a 5-pole secondary light source having a light intensity distribution approximately the same as that of the 5-pole illumination field. Here, the five-pole secondary light source is composed of five circular (or regular hexagonal) surface light sources, that is, two surface light sources symmetrically arranged in the X direction by the optical axis AX and the optical axis. ^ Two surface light sources arranged symmetrically in two directions, and one surface light source arranged near the optical axis. As described above, in the fifth embodiment, a substantially uniform 5-pole secondary light source is formed on the illumination pupil surface by the action of the diffractive optical element. Moreover, the fifth embodiment is the same as the first embodiment. By changing the magnification 'of the non-focus zoom lens 5', the distance between the center of the light source of each plane constituting the 5-pole secondary light source and the optical axis AX is not changed. , Only the size of each surface light source (the outer radius of the quadrupole secondary light source and the inner radius of the quadrupole secondary light source and the straight path of the one-pole secondary light source on the optical axis) are changed. 47 200405426 On the one hand, by changing the focal length of the variable focus lens 7, both the above distance and size can be changed, so that the entire 5-pole secondary light source can be similarly enlarged or reduced. In addition, in the fifth embodiment, it is used as a block. As a modification of the elements Cld to C4d, block elements nd to C4d as shown in FIG. 40 can also be used. Each block Cld is formed by cutting the block C1 and the simple transmission part H approximately in half in a straight line parallel to the x-axis, as shown in Fig. 40. The block element C2d is the same as the block element Cld. The block element C3d is formed by cutting the block C3 and the complementary simple transmission portion Hd approximately in half into a straight line parallel to the x-axis $, and is interspersed with each other as shown in FIG. 40. The use of diffractive optical elements containing block elements Cld ~ C4d (with the above configuration) can improve the lighting balance of 4-pole lighting and 1-pole lighting components near the optical axis. Similarly, the internal patterns of the block elements Cld ~ C4d are further subdivided, the subdivided elements corresponding to the C1 ~ C4 element patterns corresponding to the 4-pole component, and the H, Hd corresponding to the 1-pole component near the optical axis. After the area is subdivided, the subdivided elements are arranged in different or randomly arranged new block components. Using this block component can further enhance the 4-pole illumination H and the 1-pole illumination component near the optical axis. Lighting balance. In the fifth embodiment, it is preferable that the blocks C1 and C2 can be set to have the same area as the simple transmission portion ,, and the blocks C3 and C4 can be set to have the same area as the complementary simple transmission portion Hd. << Sixth Embodiment >> The second embodiment is formed by the action of the diffractive optical element 62 to form 48 200405426 planes with the optical axis AX in the relative + X direction and + γ axis + 45 degrees. The light source is an X-shaped quadrupole illumination distribution (secondary light source) composed of two surface light sources that are oriented along the optical axis AX and around 45 degrees in the + z direction relative to the + axis. In contrast, the sixth embodiment is formed in the second embodiment by using block elements Fid to F4d (a new simple transmission part is added to the block elements F1 to F4 included in the diffractive optical element 62). The fourth pole of the embodiment has a five-pole illumination distribution in which one pole is added to the optical axis. Hereinafter, the sixth embodiment will be described focusing on differences from the second embodiment. Fig. 41 is a diagram showing a 5-pole field formed on the incident surface of the microlens array in the sixth embodiment. Fig. 42 is a diagram for explaining the basic function of the diffractive optical element for 5-pole illumination in the sixth embodiment. Fig. 43 is a diagram schematically showing the overall configuration of a diffractive optical element for 5-pole illumination according to the sixth embodiment. Fig. 44 is a diagram schematically showing a configuration of a block element included in a diffractive optical element for 5-pole illumination according to a sixth embodiment.

如第43圖所示,第6實施形態之5極照明用繞射光學 元件101’係由縱橫且緊密排列之多數個區塊元件Fld〜 F4d所構成。區塊元件Fid〜F4d,分別具有第43圖或第 44圖所示之外形(交界),彼此具有大致相同的大小。又, 區塊元件Fid〜F4d中各種類大致包含同數,於繞射光學元 件1 0 1之矩形有效區域(有效直徑)1 〇 1 a之全體隨機配置、 或在將全體分割成若干個區塊之區塊中隨機配置。 如第44圖所示,區塊元件Fid〜F4d,分別包含第2 貫施形悲中說明之區塊F1〜F 4。例如,區塊元件F1 d係在 第2實施形態之區塊f 1的X方向相鄰配置單純透射部η的 49 200405426 元,。同樣的,區塊元件F2d係在區塊⑺的义方向相鄰配 置早純透射部Η的元件。而區塊元件㈣,_則係分別在 區塊F3’ Η的X方向相鄰配置補全單純透射部此的元件 。此處’第6實施形態之單純透射部H及補全單純透射部As shown in Fig. 43, the diffractive optical element 101 'for 5-pole illumination according to the sixth embodiment is composed of a plurality of block elements Fld to F4d arranged vertically and horizontally. The block elements Fid to F4d have the outer shapes (junctions) shown in Fig. 43 or 44, respectively, and have approximately the same size as each other. In addition, the various types of the block elements Fid to F4d include almost the same number, and are randomly arranged in the entire rectangular effective area (effective diameter) 1 〇1 a of the diffractive optical element 1 01, or the whole is divided into several areas Blocks are randomly allocated in blocks. As shown in FIG. 44, the block elements Fid to F4d include blocks F1 to F4 described in the second embodiment. For example, the block element F1 d is 49 200405426 yuan, in which the simple transmission portion η is adjacently arranged in the X direction of the block f 1 of the second embodiment. Similarly, the block element F2d is an element in which the early pure transmission part Η is arranged adjacent to the sense direction of the block ⑺. The block elements ㈣, _ are elements arranged in the X direction of the block F3 '相邻 to complete the simple transmission part. Here 'in the sixth embodiment, the simple transmission portion H and the complementary simple transmission portion H

Hd,與第5實施形態之單純透射部h及補全單純透射部貼 相較,雖然交界線之形狀相異,但钱刻深度d之設定及元 件之作用效果是相同的。 又,在4極成份之發散角(繞射角)θ不同於第2實施 形態時’可就對應之發散角Θ,根據式⑵來設定區塊η % 〜F4内所含之元件D1,叹E1,E2之節距’將元件η及 Hd組合於其中來設定期望之區塊元件Fid〜,而形 應之繞射光學元件。 如以上之說明’使用繞射光學元件101之第6實施形 態’係藉由透射過區塊F1〜F4之光而生成具有既定發散角 之4極成份’同時藉由透射過件Η及Hd之光而生成在光轴 附近具有強度之1極成份’藉由此等4極成份與!極成份 之合成即能進行如第41圖所示之5極照明。 f :即’將第6實施形態之繞射光學元件m定位在照 明光紅並射入平仃光束時’即會在微透鏡陣列8之入射面 士第42圖所不’形成由χ形4點狀光強度分佈與光軸附 近1點狀光強度分佈所構成之合計5點狀光強度分佈。缺 而,與第2實施形態同樣的,實際上,射入繞射光學元件 101的並非疋平仃光束,而係射入具有以錐體形狀(在微透 鏡陣列4a時為正六角錐體形、在繞射光學元件4時則為圓 50 200405426 錐體形)之光束範圍規定之角度成份的光束。如此,在微 透鏡陣列8之入射面’如第41圖所示’形成由5點狀強 度分佈與圓形(或正六角形)光束之捲積所構成之 明分佈(照野)。 ' …其結果’微透鏡陣列8之後側焦點面(照明光瞳面), 形成具有肖5極狀照野大致相同光強度分佈之5極狀二次 光源。此處’ 5極狀二次光源,係由5個圓形(或正六角形 )實質的面光源,φ即由挾著光軸Αχ、沿相對+ χ方向繞+ Υ軸+ 45度方向之2個面光源、挾著光軸ΑΧ、沿相對+ ζ 方向繞+ Υ軸-45度方向之2個面光源、以及以及配置在 光軸附近之1個面光源所構成。如此,在第6實施形態中 ,藉由繞射光學元件101之作用,於照明光瞳面形成實質 上均勻的5極狀二次光源。 又,第6實施形態與第2實施形態同樣的,可藉由改 變無焦點變焦透鏡5之倍率,在構成5極狀二次光源之各 面光源中心與光軸ΑΧ之距離不變的情形下,僅使各面光源 之大小(4極狀二次光源之外接圓半徑—4極狀二次光源之 内接圓半徑、以及光轴上1極狀二次光源之直徑)變化。另 一方面,可藉由改變可變焦透鏡7之焦距,來變化上述距 離及大小雙方,使5極狀二次光源全體相似的放大或縮小 此外,第6實施形態中,作為區塊元件Fid〜F4d之變 形例,可使用將對應第44圖之Fid〜F4d中所含4極成份 之F1〜F4之元件圖案,細分成以Dl,D2,El,E2所示之 51 200405426 被區分的要素,或將對應光軸附近1極成份之Η及Hd區域 加以細分化後之被區分的要素,分別將各要素予以排列成 第45圖所示之彼此不同排列的新的區塊元件,來提昇4極 照明與光軸附近1極照明成份之照明平衡。同樣的,將區 塊元件Fid〜F4d之内部圖案進一步予以細分化,將對應4 極成份之F1〜F 4元件圖案加以細分化後之細分化要素、與 對應光軸附近1極成份之H,Hd區域加以細分化後之細分 化的要素’彼此予以不同排列或隨機配置所得之新的區塊 元件,使用此區塊元件即能更進一步的提昇4極照明與光 轴附近1極照明成份之照明平衡。又,第6實施形態中, 最好是能將區塊Fl,F2與單純透射部η設定成具有相同面 積’將區塊F3,F4與補全單純透射部jjd設定成具有相同 面積。 《第7實施形態》 第4實施形態係藉由繞射光學元件64之作用,來形成 由挾著光軸AX於X方向對稱配置之2極狀照明分佈(二次 光源)。相對於此,第7實施形態,則係藉由採用元件gH 〜G4d(對繞射光學元件64中所含之元件G1〜G4附加新的 單純透射部),來形成在第4實施形態之2極外於光軸上加 上1極的3極狀照明分佈。以下,著眼於與第4實施形熊 之相異處,來說明第7實施形態。 &quot; 第46圖,係顯示第7實施形態中,於微透鏡陣列之入 射面形成之3極狀照野的圖。第47圖,係用以說明第7實 施形態之3極照明用繞射光學元件之基本作用的圖。第w 52 200405426 圖’係概略顯示第7實施形態之3極照明用繞射光學元件 之全體構成的圖。又,第49圖,係概略顯示第7實施形態 之3極照明用繞射光學元件中所含之區塊元件之構成的圖 〇 如第48圖所示,第7實施形態之3極照明用繞射光學 元件102,係由縱橫且緊密排列之多數個元件Gld〜G4d所 構成。元件Gld〜G4d,皆具有長方形之外形(交界),彼此 具有大致相同的大小。又,元件Gld〜G4d中各種類大致包 含同數,於繞射光學元件102之矩形有效區域(有效直徑| )102a之全體隨機配置、或在將全體分割成若干個區塊之 區塊中隨機配置。 如第49圖所示,元件Gld〜G4d,分別包含第4實施 形態中說明之元件G1〜G4。例如,元件Gld係在第4實施 形態之元件G1的X方向相鄰配置單純透射部H的元件。同 樣的元件G2d係在元件G2的X方向相鄰配置單純透射部 Η的元件。而元件G3d,G4d則係分別在元件G3,以的χ 方:相鄰配置補全單純透射部肋的元件。此處,第7實施f 形態之單純透射部H及補全單純透射部Hd,具有與第5實 施幵八%之單純透射部H及補全單純透射部Μ相同之構成及 作用。 &amp;又,在2極成份之發散角(繞射角)θ不同於第4實施 〜每可就對應之發散角0,根據式(2)來設定元件G1 〜G4之節距’將元件H A Hd組合於其中來設定期望之元 件Gld〜G4d,而形成對應之繞射光學元件。Hd is compared with the simple transmission part h and the complementary simple transmission part of the fifth embodiment. Although the shape of the boundary line is different, the setting of the money-cut depth d and the effect of the elements are the same. In addition, when the divergence angle (diffraction angle) θ of the 4-pole component is different from the second embodiment, the component D1 included in the block η% to F4 can be set according to Equation 之 with respect to the corresponding divergence angle θ. The pitch of E1 and E2 is a combination of the elements η and Hd to set a desired block element Fid ~, and it is shaped as a diffractive optical element. As described above, the "sixth embodiment using the diffractive optical element 101" is to generate a 4-pole component having a predetermined divergence angle by transmitting light passing through the blocks F1 to F4, and transmitting the Η and Hd Light generates a 1-pole component with an intensity near the optical axis. The composition of the polar components enables 5-pole illumination as shown in Figure 41. f: That is, when the diffractive optical element m of the sixth embodiment is positioned at the illumination light red and enters the flat beam, it will be formed on the incident surface of the microlens array 8 as shown in Figure 42. A total of five-point light intensity distributions composed of the point-shaped light intensity distribution and the one-point light intensity distribution near the optical axis. However, in the same way as the second embodiment, in fact, what is incident into the diffractive optical element 101 is not a chirped chirped beam, but is incident in a cone shape (a hexagonal pyramid shape in the microlens array 4a, in When diffracting the optical element 4, it is a light beam with an angular component specified by the beam range of the circle 50 (200405426 cone). In this way, as shown in FIG. 41, the incident surface of the microlens array 8 is formed with a bright distribution (illumination field) composed of a convolution of a 5-point intensity distribution and a circular (or regular hexagonal) light beam. '... As a result', the focal surface (illumination pupil surface) on the rear side of the microlens array 8 forms a 5-pole secondary light source having substantially the same light intensity distribution as the 5-pole illumination field. Here, the 5-pole secondary light source is composed of 5 circular (or regular hexagonal) surface light sources. Φ is defined by the direction of the optical axis Αχ, and the relative + χ direction around + Υ axis + 45 degrees. A surface light source, two surface light sources oriented along the optical axis AX, two +45 directions around the + + axis, and one surface light source arranged near the optical axis. As described above, in the sixth embodiment, a substantially uniform five-pole secondary light source is formed on the illumination pupil surface by the action of the diffractive optical element 101. The sixth embodiment is the same as the second embodiment. By changing the magnification of the non-focus zoom lens 5, the distance between the center of the light source and the optical axis AX of each surface constituting the 5-pole secondary light source is not changed. Only the size of each surface light source (the radius of the outer circle of the 4-pole secondary light source—the radius of the inner circle of the 4-pole secondary light source and the diameter of the 1-pole secondary light source on the optical axis) are changed. On the other hand, by changing the focal length of the variable-focus lens 7, both the above-mentioned distance and size can be changed, so that the entire five-pole-shaped secondary light source can be similarly enlarged or reduced. In addition, in the sixth embodiment, as the block element Fid ~ For the modification of F4d, the element patterns corresponding to the four-pole components F1 to F4 contained in Fid to F4d in Fig. 44 can be subdivided into 51 200405426 divided by D1, D2, El, and E2. Or the subdivided elements corresponding to the Η and Hd regions corresponding to the 1-pole component near the optical axis are divided into different elements, and the elements are respectively arranged into new block elements arranged differently from each other as shown in FIG. 45 to improve 4 The lighting balance between the polar lighting and the lighting component near the optical axis. Similarly, the internal patterns of the block elements Fid ~ F4d are further subdivided, and the subdivided elements corresponding to the F1 ~ F 4 element patterns corresponding to the 4-pole component and the H corresponding to the 1-pole component near the optical axis are subdivided. The subdivided elements after subdividing the Hd region are new block elements obtained by differently arranging or randomly disposing each other. Using this block element can further enhance the 4-pole lighting and the 1-pole lighting component near the optical axis. Lighting balance. Further, in the sixth embodiment, it is preferable that the blocks Fl, F2 and the simple transmission part η can be set to have the same area ', and the blocks F3, F4 and the complementary simple transmission part jjd can be set to have the same area. [Seventh Embodiment] The fourth embodiment forms a bipolar illumination distribution (secondary light source) symmetrically arranged in the X direction by the optical axis AX by the action of the diffractive optical element 64. In contrast, the seventh embodiment is formed in the second embodiment according to the second embodiment by using the elements gH to G4d (adding a new simple transmission portion to the elements G1 to G4 included in the diffractive optical element 64). A 3-pole illumination distribution with one pole added to the optical axis outside the pole. Hereinafter, the seventh embodiment will be described focusing on differences from the fourth embodiment. &quot; Fig. 46 is a diagram showing a three-pole field formed on the incident surface of the microlens array in the seventh embodiment. Fig. 47 is a diagram for explaining the basic operation of the diffractive optical element for 3-pole illumination according to the seventh embodiment. W 52 200405426 Fig. 'Is a diagram schematically showing the overall configuration of a diffractive optical element for 3-pole illumination according to a seventh embodiment. Fig. 49 is a diagram schematically showing the configuration of a block element included in the diffraction optical element for 3-pole illumination according to the seventh embodiment. As shown in Fig. 48, for the 3-pole illumination according to the seventh embodiment The diffractive optical element 102 is composed of a plurality of elements Gld to G4d arranged vertically and closely. The elements Gld to G4d each have a rectangular outer shape (boundary) and have approximately the same size as each other. In addition, the various types of the elements Gld to G4d include approximately the same number, and are randomly arranged in the entire rectangular effective area (effective diameter |) 102a of the diffractive optical element 102, or randomly in a block that divides the whole into several blocks. Configuration. As shown in Fig. 49, the elements Gld to G4d include the elements G1 to G4 described in the fourth embodiment, respectively. For example, the element Gld is an element in which the simple transmission portion H is disposed adjacent to each other in the X direction of the element G1 of the fourth embodiment. The same element G2d is an element in which the simple transmission portion 配置 is arranged adjacent to the X direction of the element G2. The elements G3d and G4d are respectively located on the element G3, and the x-squares are: adjacently arranged elements that complete the ribs of the simple transmission part. Here, the simple transmission portion H and the complementary simple transmission portion Hd in the seventh embodiment f have the same configuration and function as those of the simple transmission portion H and the complementary simple transmission portion M in the fifth embodiment. &amp; In addition, the divergence angle (diffraction angle) θ of the 2-pole component is different from that in the fourth embodiment. Each divergence angle corresponding to 0 can be set according to Equation (2). Hd is combined therein to set desired elements Gld to G4d, and corresponding diffraction optical elements are formed.

53 200405426 &amp;如:上之說明,使用繞射光學元件102之第7實施形 久藉由透射過元件G1〜G4之光而生成具有既定發散角 和成伤同時藉由透射過件Η及Hd之光而生成在光軸 附近具有強度之1極成份,藉由此等2極成份肖!極成份 之曰成即犯進行如第4 6圖所示之沿X方向之3極照明。 亦即’將第7實施形態之繞射光學元件102定位在照 明光耘並射入平行光束時,即會在微透鏡陣列8之入射面 ,如第47圖所示,形成由挾著光軸Αχ於χ方向對稱配置 之2點狀光強度分佈與光軸附近1點狀光強度分佈所構成 之合計5點狀光強度分佈。然而,與第4實施形態同樣的 ’實際上,射入繞射光學元件102的並非是平行光束,而 係射入具有以錐體形狀(在微透鏡陣列4a時為正六角錐體 形、在繞射光學元件4時則為圓錐體形)之光束範圍規定之 角度成份的光束。如此,在微透鏡陣列8之入射面,如第 46圖所示’形成由3點狀光強度分佈與圓形(或正六角形) 光束之捲積所構成之3極狀照明分佈(照野)。 其結果,微透鏡陣列8之後側焦點面(照明光瞳面), 形成具有與3極狀照野大致相同光強度分佈之3極狀二次 光源。此處,3極狀二次光源,係由3個圓形(或正六角形 )實貝的面光源,亦即由挟者光轴AX於X方向對稱配置之 2個面光源、與配置在光軸AX附近之1個面光源所構成。 如此,在第7實施形態中,藉由繞射光學元件1 〇 2之作用 ,於照明光瞳面形成實質上均勻的3極狀二次光源。 又,第7實施形態與第4實施形態同樣的,可藉由改 54 200405426 變無焦點變焦透鏡5之倍率,在構成3極狀二次光源之各 面光源中心與光軸AX之距離不變的情形下,僅使各面光源 之大小(2極狀二次光源之外接圓半徑_2極狀二次光源之 内接圓半徑、以及光軸上丨極狀二次光源之直徑)變化。另 一方面,可藉由改變可變焦透鏡7之焦距,來變化上述距 離及大小雙方,使3極狀二次光源全體相似的放大或縮小 〇 此外’第7實施形態中,亦與第5及第6實施形態同 樣的’可作為元件Gld〜G4d之變形例,將元件Gld〜G4d 之内部圖案予以細分化,將對應2極成份之G1〜G4元件圖 案加以細分化後之細分化要素、與對應光軸附近1極成份 之Η及Hd區域加以細分化後之細分化的要素,彼此予以不 同排列或隨機配置所得之新的元件,使用此元件來提升2 極照明與光軸附近1極照明成份之照明平衡。又,第7實 施形態中,最好是能將元件Gl,G2與單純透射部Η設定成 具有相同面積,將元件G3,G4與補全單純透射部Hd設定 成具有相同面積。 《第8實施形態》 第50圖,係顯示第8實施形態中,於微透鏡陣列之入 射面形成之9極狀照野的圖。又,第51圖,係用以說明第 8實施形態之9極照明用繞射光學元件之基本作用的圖。 如前所述,第3實施形態,係藉由第1實施形態之繞射光 學元件61之作用與第2實施形態之繞射光學元件62之作 用的合成,來形成8極狀照明分佈(二次光源)。同樣的, 55 200405426 第8實施形態,可藉由第5實施形態之繞射光學元件1〇〇 之作用與第6實施形態之繞射光學元件1 〇1之作用的合成 ’來形成第51圖所示之由9點狀光強度分佈與圓形(或正 六角形)光束之捲積所構成之9極狀照明分佈,亦即形成第 50圖所示之9極狀照明分佈。 此外,上述各實施形態及變形例中,雖係使用含直線 光柵圖案之繞射光學元件,但作為與此種繞射光學元件具 有相同光學性能之光學構件,亦可使用與繞射光學元件產 生大致相同光振幅之折射光學元件。 又,關於上述繞射光學元件之各實施形態及變形例中 ,雖係使用2元型繞射光學元件圖案,但並不限於此,與 第1至第4實施形態同樣的,亦可使用閃耀型繞射光學元 件圖案或多元型繞射光學元件圖案。 除此之外,就第i至第4實施形態及其變形例所說明 之技術内容’亦可適用於第5至帛8實施形態及其變形例53 200405426 &amp; As explained above, the seventh embodiment of the use of the diffractive optical element 102 is used to generate light with a predetermined divergence angle and wound by transmitting light passing through the elements G1 to G4, and transmitting through the element H and Hd. The light produces a 1-pole component with an intensity near the optical axis, and thus waits for the 2-pole component to appear! The polar component is used to illuminate the 3-pole illumination along the X direction as shown in Figure 46. That is, when the diffractive optical element 102 of the seventh embodiment is positioned on the illumination light beam and enters a parallel beam, it will be formed on the incident surface of the microlens array 8 as shown in FIG. 47 to form a beam axis A total of five-point light intensity distributions composed of the two-point light intensity distribution in which χ is symmetrically arranged in the χ direction and the one-point light intensity distribution near the optical axis. However, it is the same as the fourth embodiment. 'Actually, it is not a parallel beam that enters the diffractive optical element 102. Instead, it has a cone shape (a regular hexagonal cone shape in the microlens array 4a, a diffraction When the optical element 4 is in the shape of a cone, it is a light beam with an angular component specified by the beam range. In this way, as shown in FIG. 46, the incident surface of the microlens array 8 is formed into a three-pole illumination distribution (illuminated field) formed by a convolution of a three-point light intensity distribution and a circular (or regular hexagonal) light beam. . As a result, the rear focal surface (illumination pupil surface) of the microlens array 8 forms a tripolar secondary light source having a light intensity distribution approximately the same as that of the tripolar illumination field. Here, the tripolar secondary light source is a surface light source composed of three circular (or regular hexagonal) solid shells, that is, two surface light sources symmetrically arranged in the X direction by the optical axis AX of the person, and One surface light source near the axis AX. As described above, in the seventh embodiment, a substantially uniform tripolar secondary light source is formed on the illumination pupil surface by the action of the diffractive optical element 102. The seventh embodiment is the same as the fourth embodiment. By changing 54 200405426 to change the magnification of the non-focus zoom lens 5, the distance between the center of the light source and the optical axis AX of each surface constituting the three-pole secondary light source is not changed. In the case of the light source, only the size of each surface light source (the radius of the outer circle of the 2-pole secondary light source and the radius of the inner circle of the polar secondary light source and the diameter of the polar secondary light source on the optical axis) are changed. On the other hand, by changing the focal length of the variable-focus lens 7, both the distance and the size can be changed, so that the entire three-pole secondary light source can be similarly enlarged or reduced. In addition, the seventh embodiment is also similar to the fifth and fifth embodiments. In the same manner as the sixth embodiment, as a modification of the elements Gld to G4d, the internal patterns of the elements Gld to G4d can be subdivided, and the subdivided elements of the G1 to G4 element patterns corresponding to the two-pole components can be subdivided into Corresponding to the subdivided elements of the 极 and Hd regions of the 1-pole component near the optical axis, new elements obtained by differently arranging or randomly arranging each other, using this element to enhance 2-pole illumination and 1-pole illumination near the optical axis Lighting balance of ingredients. In the seventh embodiment, it is preferable that the elements G1, G2 and the simple transmission portion Η can be set to have the same area, and the elements G3, G4 and the complementary simple transmission portion Hd can be set to have the same area. [Eighth Embodiment] Fig. 50 is a diagram showing a 9-pole field formed on the incident surface of the microlens array in the 8th embodiment. Fig. 51 is a diagram for explaining the basic operation of the diffractive optical element for 9-pole illumination according to the eighth embodiment. As described above, the third embodiment forms an 8-pole illumination distribution by combining the effects of the diffractive optical element 61 of the first embodiment and the functions of the diffractive optical element 62 of the second embodiment (2 Secondary light). Similarly, 55 200405426 in the eighth embodiment, the combination of the function of the diffractive optical element 100 in the fifth embodiment and the function of the diffractive optical element 100 in the sixth embodiment can be used to form FIG. 51. The 9-pole illumination distribution formed by the convolution of a 9-point light intensity distribution and a circular (or regular hexagonal) beam is shown, that is, the 9-pole illumination distribution shown in FIG. 50 is formed. In addition, although the diffractive optical element including a linear grating pattern is used in each of the above embodiments and modifications, as an optical member having the same optical performance as this diffractive optical element, it can also be produced using a diffractive optical element. Refractive optical element with approximately the same light amplitude. In addition, in each of the above-mentioned embodiments and modification examples of the diffractive optical element, although a two-element diffractive optical element pattern is used, it is not limited to this. Similar to the first to fourth embodiments, a sparkle may be used. Type diffractive optical element pattern or multi-type diffractive optical element pattern. In addition, the technical contents described in the i-th to the fourth embodiments and their modifications are also applicable to the fifth to the eighth embodiments and their modifications.

上述各實施形態中之曝光褒置,可藉由照明光 =月,標線片X照明製程),使用投影光學軸 成=罩之轉印關案㈣至感光性基板(曝光製程), 以製造微7L件(半導體元件、攝 一 .¾ og . ^ 〜兀件、,夜日日顯示元件 4膑磁頭4)。以下,參照第 圓之机%圖,來說明使 上述各實施形態之曝光裝置將 美始夕曰尤疋電路圖案形成於感光 土板之日日0 4,以獲得作為微 的一例。 卩之+導體兀件時之方 56 200405426 膜。於L於弟32圖之步驟30卜在1批晶圓上蒸鍍金屬 布光八人之步驟302巾’在該1批晶圓上之金屬膜上塗 =。之後,於步驟30”,使用上述各實施形態之曝 尤我置’透過投影光學糸 ^ ^ 元予糸統將先罩上圖案之像,依序曝光 该、&quot;比晶圓上之各曝光照射區域。之後,於步驟 ’進㈣1批晶圓上之光阻之顯影後,在該1批晶 固上將光阻圖案作為光罩進行敍刻,而在各晶圓上之各曝 先照射區域形成對應光罩上圖案之電路圖帛。之後,進一 t形成上層之電路圖案等,來製造半導體元件等之元件。 若使用上述半導體S件之製造方法,π能以良好的效率( 產旎)得到具有極微細之電路圖案的半導體元件。 又,上述各實施形態之曝光裝置,亦可藉由在板(玻璃 基板)上形成既定圖案(電路圖案、電極圖案等),來獲得作 為微元件之液晶顯示元件。以下,參照第33圖之流程圖, 說明此方法之一例。第33圖中,圖案形成步驟4〇1,係使 用上述各實施形態之曝光裝置將光罩圖案轉印曝光至感光 性基板(塗有光阻之玻璃基板等),亦即實施所謂之光微影 製程。藉由此光微影製程,在感光性基板上形成包含多數 電極等之既定圖案。之後,曝光後之基板,經顯影、蝕刻 、光阻剝離等各製程,在基板上形成既定圖案,而移至次 一彩色濾光片形成步驟402。 接著,於彩色濾光片形成步驟402中,形成對應 R(Red)、G(Green)、B(Blue)3點之組多數排列成矩陣狀, 或將R、G、B之3條條狀濾光片組複數排列於水平方向的 200405426 彩色濾光片。然後,在彩色濾光片形成步驟4〇2後,進行 單元胞組裝步驟403。單元胞組裝步驟403中,係使用在 圖案形成步驟401中所得之具有既定圖案的基板,及在彩 色濾光片形成步驟402中所得之彩色濾光片等,來組裝液 晶面板(液晶單元胞)。單元胞組裝步驟403中,例如,係 在圖案形成步驟401中所得之具有既定圖案的基板、與在 彩色濾光片形成步驟402中所得之彩色濾光片之間注入液 晶,以製造液晶面板(液晶單元胞)。 之後,於模組組裝步驟404中,安裝使組裝成之液晶t 面板(液晶單元胞)進行顯示動作的電氣電路、背光等各零 件’而元成液晶顯不兀件。The exposure settings in each of the above embodiments can be manufactured by using illumination light = month, reticle X illumination process), and using a projection optical axis to form a cover to the photosensitive substrate (exposure process) to manufacture Micro 7L pieces (semiconductor element, photo. ¾ og. ^ ~ Element, night and day display element 4 膑 head 4). In the following, referring to the diagram of the circle, the explanation will be made on the day when the exposure apparatus of each of the above embodiments formed the U.S.A. and U.S. circuit pattern on the light-sensitive clay plate as an example.卩 之 + Conductor element when it is 56 200405426 Film. In step 30 of FIG. 32, the metal is vapor-deposited on a batch of wafers. Step 302 of eight people is coated on the metal film on the batch of wafers. After that, in step 30 ", the exposure of each of the above embodiments is used, and the image of the pattern is first masked by the projection system, and the exposures are sequentially exposed. Irradiate the area. After the development of the photoresist on one batch of wafers in step ', the photoresist pattern is engraved on the batch of crystal solids, and each exposure on each wafer is irradiated first. The circuit pattern 电路 corresponding to the pattern on the photomask is formed in the area. Then, the circuit pattern of the upper layer is further formed to manufacture components such as semiconductor elements. If the above-mentioned manufacturing method of the semiconductor S-piece is used, π can be produced with good efficiency. A semiconductor element having an extremely fine circuit pattern is obtained. In addition, the exposure apparatus of each of the above embodiments can also be obtained as a micro-element by forming a predetermined pattern (circuit pattern, electrode pattern, etc.) on a plate (glass substrate). A liquid crystal display element. Hereinafter, an example of this method will be described with reference to the flowchart in FIG. 33. In FIG. 33, the pattern forming step 401 is performed by using the exposure device of each of the above embodiments to mask the photomask. The pattern is transferred to a photosensitive substrate (such as a glass substrate coated with a photoresist), which is a so-called photolithography process. By this photolithography process, a predetermined pattern including a plurality of electrodes is formed on the photosensitive substrate. After that, the exposed substrate is subjected to various processes such as development, etching, and photoresist peeling to form a predetermined pattern on the substrate, and then moves to the next color filter forming step 402. Next, in the color filter forming step 402 Among them, the groups corresponding to the three points of R (Red), G (Green), and B (Blue) are mostly arranged in a matrix, or a plurality of three strip filter groups of R, G, and B are arranged in a horizontal direction. 200405426 Color filter. Then, after the color filter forming step 4202, a cell assembly step 403 is performed. In the cell assembly step 403, a substrate having a predetermined pattern obtained in the pattern forming step 401 is used. And the color filters obtained in the color filter formation step 402 to assemble a liquid crystal panel (liquid crystal cell). In the cell assembly step 403, for example, the pattern obtained in the pattern formation step 401 has a predetermined pattern. Liquid crystal is injected between the substrate and the color filter obtained in the color filter forming step 402 to manufacture a liquid crystal panel (liquid crystal cell). Then, in the module assembly step 404, the assembled liquid crystal t is installed. The panel (liquid crystal cell) performs various operations such as electrical circuits, backlights, etc., and the element becomes a liquid crystal display element.

又,上述各實施形態中,作為光源丨,雖係使用供應 193nm波長之光的ArF準分子雷射光源(或供應248nm波長 之光的KrF準分子雷射光源),但並不限於此,亦可使用供 應供應157nm波長之光的F2雷射光源、或供應g線 (436nm)及i線(365nm)之光的水銀燈等。使用水銀燈時, 光源1 ’係具有水銀燈與橢圓鏡與準直透鏡之構成。 又,上述實施形態中,雖係以具備照明光學裝置之投 影曝光裝置為例來說明本發明,但顯而易見的,本發明亦 月b適用於用來照明光罩以外之被照射面的一般照明光學裝 置。 如以上之說明,本發明之繞射光學元件,例如可用於 照明光學裝置’在照明光瞳面形成實質上均一之複數極狀 (4極狀、8極狀、2極狀)照度分佈。又,本發明之照明光 58 200405426 子虞置可使用在照明光瞳面形成實質上均一之複數極狀 …、度刀佈的、、凡射光學元件,在抑制光量損失之同時進行良 好的各種複數極明。 此外’女裝有本發明之照明光學裝置之曝光裝置及使 用本發明之照明光學裝置之曝光方法,可使用能在抑制光 里相失之同時進行良好的各種複數極明的照明光學装置, 在對光罩之最佳的照明條件下,將光罩圖案忠實的轉印至 感光性基板上。進一步的,本發明中,可使用能將光罩圖 案忠實的轉印至感光性基板上之本發明的曝光裝置及曝光t 方法’製造良好的微元件。 【圖式簡單說明】 (一)圖式部分 第1圖’係概略顯示具備本發明各實施形態之照明光 學裝置之曝光裝置之構成的圖。In each of the above embodiments, although the light source 丨 is an ArF excimer laser light source (or a KrF excimer laser light source that supplies 248 nm light), it is not limited to this. An F2 laser light source that supplies light with a wavelength of 157 nm, or a mercury lamp that supplies light with g-line (436 nm) and i-line (365 nm) can be used. When a mercury lamp is used, the light source 1 'has a structure including a mercury lamp, an elliptical mirror, and a collimating lens. In the above embodiment, the present invention has been described using a projection exposure apparatus provided with an illumination optical device as an example. However, it is obvious that the present invention is also applicable to general illumination optics for illuminating an illuminated surface other than a photomask Device. As described above, the diffractive optical element of the present invention can be used in, for example, an illumination optical device 'to form a substantially uniform plural polar shape (4-pole shape, 8-pole shape, 2-pole shape) on the illumination pupil surface. In addition, the illumination light 58 200405426 of the present invention can be used to form a substantially uniform plural polar shape on the pupil surface of the illumination .... The plural is extremely clear. In addition, 'women have the exposure device of the illumination optical device of the present invention and the exposure method using the illumination optical device of the present invention, and it is possible to use various kinds of extremely bright illumination optical devices that can perform good simultaneous suppression of phase loss in light. Under the optimal lighting conditions of the photomask, the photomask pattern is faithfully transferred to the photosensitive substrate. Further, in the present invention, an exposure device and an exposure method of the present invention that can faithfully transfer a mask pattern onto a photosensitive substrate can be used to produce a good micro-device. [Brief description of the drawings] (I) Schematic part Fig. 1 'is a diagram schematically showing the configuration of an exposure device provided with an illumination optical device according to each embodiment of the present invention.

第2圖,係概略顯示第1實施形態之4極照明用繞射 光學TL件中所含之基本繞射光學元件及補全繞射光學元件 之構成的圖。 第3圖,係第2圖之各光學元件的截面圖。 第4圖,係概略顯示第1實施形態之4極照明用繞射 光學疋件中所含之4種區塊之構成的圖。 第5圖,係概略顯示第1實施形態之4極照明用繞射 光學70件之全體構成的圖。 第6圖,係用以說明第1實施形態之4極照明用繞射 59 200405426 光學元件之基本作用的圖。 第7圖,係用以說明第1實施形態中,於微透鏡陣列 之入射面形成4極狀照野之原理的圖。 第8圖,係顯示第1實施形態中,於微透鏡陣列之入 射面形成之4極狀照野的圖。 第9圖,係顯示在第1實施形態中使用微透鏡陣列來 作為發散光束形成元件時,於作為光學積分器之微透鏡陣 列之入射面形成之4極狀照野的圖。Fig. 2 is a diagram schematically showing the configuration of a basic diffractive optical element and a complementary diffractive optical element included in the diffractive optical TL element for quadrupole illumination of the first embodiment. FIG. 3 is a cross-sectional view of each optical element in FIG. 2. Fig. 4 is a diagram schematically showing a configuration of four types of blocks included in the diffraction optical element for quadrupole illumination of the first embodiment. Fig. 5 is a diagram schematically showing the entire configuration of 70 diffractive optics for quadrupole illumination of the first embodiment. Fig. 6 is a diagram for explaining the basic operation of the diffraction element for quadrupole illumination 59 200405426 of the first embodiment. Fig. 7 is a diagram for explaining the principle of forming a quadrupole field on the incident surface of the microlens array in the first embodiment. Fig. 8 is a diagram showing a quadrupole field formed on the incident surface of the microlens array in the first embodiment. Fig. 9 is a diagram showing a quadrupole field formed on the incident surface of a microlens array as an optical integrator when a microlens array is used as a divergent beam forming element in the first embodiment.

第1 〇圖,係概略顯示第2實施形態之4極照明用繞射 光學元件中所含之基本繞射光學元件及補全繞射光學元件 之構成的圖。 第11圖,係概略顯示第2實施形態之4極照明用繞射 光學元件中所含之4種區塊之構成的圖。 第12圖’係概略顯示第2實施形態之4極照明用繞射 光學元件之全體構成的圖。Fig. 10 is a diagram schematically showing the configuration of a basic diffractive optical element and a complementary diffractive optical element included in the diffractive optical element for quadrupole illumination of the second embodiment. Fig. 11 is a diagram schematically showing the configuration of four types of blocks included in the diffractive optical element for quadrupole illumination of the second embodiment. Fig. 12 'is a diagram schematically showing the entire configuration of a diffractive optical element for quadrupole illumination according to the second embodiment.

第13圖’係用以說明第2實施形態之4極照明用繞射 光學元件之基本作用的圖。 第14圖,係顯示第2實施形態中,於微透鏡陣列之入 射面形成之4極狀照野的圖。 第15圖,係顯示在第2實施形態中使用微透鏡陣列來 作為發散光束形成元件時,於作為光學積分器之微透鏡陣 列之入射面形成之4極狀照野的圖。 第1 6圖,係顯示第3實施形態之基本繞射光學元件及 補全繞射光學元件(Dl,,D2,,El,,E2,)之構成的概念圖。 60 200405426 第17圖’係顯示以光學元件(D1,,D2,,ΕΓ,E2,)構 成之區塊F1,〜F4,之構成的概念圖。 第18圖’係藉由組合區塊C1〜C4與區塊F1,〜F4,來 構成合成區塊DQ1〜DQ4的概念圖。 第19圖’係顯示將多數之合成區塊DQ1〜DQ4縱橫緊 密排列所構成之第3實施形態之繞射光學元件63之構成的 概念圖。Fig. 13 'is a diagram for explaining the basic operation of the diffractive optical element for quadrupole illumination according to the second embodiment. Fig. 14 is a diagram showing a quadrupole field formed on the incident surface of the microlens array in the second embodiment. Fig. 15 is a diagram showing a quadrupole field formed on the incident surface of a microlens array as an optical integrator when a microlens array is used as a divergent beam forming element in the second embodiment. FIG. 16 is a conceptual diagram showing the configuration of the basic diffractive optical element and the complementary diffractive optical element (D1, D2, El, E2,) in the third embodiment. 60 200405426 Fig. 17 is a conceptual diagram showing the composition of blocks F1, ~ F4, composed of optical elements (D1 ,, D2 ,, Γ, E2,). Fig. 18 'is a conceptual diagram of the synthesized blocks DQ1 to DQ4 by combining blocks C1 to C4 and blocks F1 to F4. Fig. 19 'is a conceptual diagram showing the structure of a diffractive optical element 63 according to a third embodiment in which a plurality of synthesized blocks DQ1 to DQ4 are arranged closely and vertically.

第20圖’係用以說明第3實施形態之8極照明用繞射 光學元件之基本作用的圖。 第21圖’係顯示第3實施形態中,於微透鏡陣列之入 射面形成之8極狀照野的圖。 第22圖’係顯示在第3實施形態中使用微透鏡陣列來 作為發散光束形成元件時,於作為光學積分器之微透鏡陣 列之入射面形成之8極狀照野的圖。Fig. 20 'is a diagram for explaining the basic operation of the diffractive optical element for 8-pole illumination according to the third embodiment. Fig. 21 'is a diagram showing an eight-pole field formed on the incident surface of the microlens array in the third embodiment. Fig. 22 'is a diagram showing an octopole field formed on the incident surface of a microlens array as an optical integrator when a microlens array is used as a divergent beam forming element in the third embodiment.

第2 3圖,係概略顯示第4實施形態之2極照明用繞射 光學元件中所含之基本繞射光學元件及補全繞射光學元件 之構成的圖。 第24圖,係概略顯示第4實施形態之2極照明用繞射 光學元件之全體構成的圖。 第25圖,係用以說明第4實施形態之各光學元件之隨 機配置的圖。 第2 6圖,係用以說明第4實施形態之2極照明用繞射 光學元件之基本作用的圖。 第27圖,係顯示第4實施形態中,於微透鏡陣列之入 61 200405426 射面形成之2極狀照野的圖。 、第28圖’係顯不在第4實施形態中使用微透鏡陣列來 作為發散光束形成元件時,於作為光學積分器之微透鏡陣 列之入射面形成之2極狀照野的圖。 第29圖,係以不意方式顯示構成複數極狀二次光源之 各面光源光強度輪廓的圖。 第30圖,係概略顯示於第丨圖之曝光裝置中,取代微 透鏡陣列而使用棒狀積分器時之主要部構成的圖。 第31A圖,係將閃耀型繞射光學元件於其周期方向截$ 面加以切斷的截面圖。 第31B圖,係將多元型繞射光學元件於其周期方向截 面加以切斷的截面圖。 第31C圖,係將2元型繞射光學元件於其周期方向截 面加以切斷的截面圖。 第32圖,係作為微元件之半導體元件之製造方法的流 程圖。Fig. 23 is a diagram schematically showing the configuration of a basic diffractive optical element and a complementary diffractive optical element included in the diffractive optical element for bipolar illumination of the fourth embodiment. Fig. 24 is a diagram schematically showing the entire configuration of a diffractive optical element for bipolar illumination of the fourth embodiment. Fig. 25 is a diagram for explaining the random arrangement of each optical element in the fourth embodiment. Fig. 26 is a diagram for explaining the basic operation of the diffractive optical element for bipolar illumination of the fourth embodiment. Fig. 27 is a diagram showing a bipolar field formed on the entrance surface of the microlens array 61 200405426 in the fourth embodiment. Fig. 28 'shows a bipolar field formed on the incident surface of a microlens array as an optical integrator when a microlens array is not used as a divergent beam forming element in the fourth embodiment. Fig. 29 is a diagram showing the light intensity profile of each surface light source constituting a plurality of polar secondary light sources by accident. Fig. 30 is a diagram schematically showing the configuration of the main parts when the rod integrator is used instead of the micro lens array in the exposure apparatus shown in Fig. 丨. FIG. 31A is a cross-sectional view of a flare-type diffractive optical element cut along a periodic plane. Fig. 31B is a cross-sectional view of a multi-element diffractive optical element cut in a periodic cross-section. Fig. 31C is a cross-sectional view of a binary diffractive optical element cut in a periodic cross-section. Fig. 32 is a flowchart of a method of manufacturing a semiconductor device as a micro device.

第33圖’係作為微元件之液晶顯不元件之製造方法的 流程圖。 第34圖,係概略顯示為了以微影法製造繞射光學元件 所使用之光罩之構成的圖。 第35圖,係顯示使用第34圖之光罩,在玻璃基板上 製成之繞射光學元件的圖。 第3 6圖,係顯示第5實施形態中,於微透鏡陣列之入 射面形成之5極狀照野的圖。 62 200405426 第37圖,係用以說明第5實施形態之5極照明用繞射 光學元件之基本作用的圖。 第38圖,係概略顯示第5實施形態之5極照明用繞射 光學元件之全體構成的圖。 第39圖,係概略顯示第5實施形態之5極照明用繞射 光學元件中所含之區塊元件之構成的圖。 第40圖,係概略顯示第5實施形態之5極照明用繞射 光學元件中所含之區塊元件之變形例的圖。 第41圖,係顯示第6實施形態中,於微透鏡陣列之入$ 射面形成之5極狀照野的圖。 第42圖,係用以說明第6實施形態之5極照明用繞射 光學元件之基本作用的圖。 第43圖,係概略顯示第6實施形態之5極照明用繞射 光學元件之全體構成的圖。Fig. 33 'is a flowchart of a method for manufacturing a liquid crystal display device as a micro-device. Fig. 34 is a diagram schematically showing a configuration of a photomask used for manufacturing a diffractive optical element by a lithography method. Fig. 35 is a view showing a diffractive optical element made on a glass substrate using the mask of Fig. 34. Fig. 36 is a diagram showing a 5-pole field formed on the incident surface of the microlens array in the fifth embodiment. 62 200405426 Fig. 37 is a diagram for explaining the basic operation of the diffractive optical element for 5-pole illumination according to the fifth embodiment. Fig. 38 is a diagram schematically showing the entire configuration of a diffractive optical element for 5-pole illumination according to a fifth embodiment. Fig. 39 is a diagram schematically showing the configuration of a block element included in the diffractive optical element for 5-pole illumination according to the fifth embodiment. Fig. 40 is a diagram schematically showing a modification of the block element included in the diffractive optical element for 5-pole illumination according to the fifth embodiment. Fig. 41 is a diagram showing a 5-pole field formed on the entrance surface of the microlens array in the sixth embodiment. Fig. 42 is a diagram for explaining the basic operation of the diffractive optical element for 5-pole illumination according to the sixth embodiment. Fig. 43 is a diagram schematically showing the entire configuration of a diffractive optical element for 5-pole illumination according to a sixth embodiment.

第44圖,係概略顯示第6實施形態之5極照明用繞射 光學元件中所含之區塊元件之構成的圖。 第45圖,係概略顯示第6實施形態之5極照明用繞射 光學元件中所含之區塊元件之變形例的圖。 第46圖,係顯示第7實施形態中,於微透鏡陣列之入 射面形成之3極狀照野的圖。 第47圖’係用以說明第7實施形態之3極照明用繞射 光學元件之基本作用的圖。 第48圖,係概略顯示第7實施形態之3極照明用繞射 光學元件之全體構成的圖。 06 63 200405426 第49圖,係概略顯示第7實施形態之3極照明用繞射 光學元件中所含之區塊元件之構成的圖。 第50圖,係顯示第8實施形態中,於微透鏡陣列之入 射面形成之9極狀照野的圖。 第51圖,係用以說明第8實施形態之9極照明用繞射 光學元件之基本作用的圖。 (二)元件代表符號 1 光源 2 整形光學系 3, 12 彎折鏡 4, 6, 61, 62, 63, 100, 101, 5 無焦點變焦 7 可變焦透鏡 8 微透鏡陣列 9 聚光光學系 10 光罩遮簾 11a,lib 成像光學系 13 光罩 14 投影光學系 15 晶圓 Al,D1 第1基本繞 Bl,El 第2基本繞 A2, D2 第1補全繞 B2, E2 第2補全繞 統 102 繞射光學元件 透鏡 統 統 統 射光學元件 射光學元件 射光學元件 射光學元件 64 200405426 al〜a3 光線Fig. 44 is a diagram schematically showing the configuration of a block element included in the diffractive optical element for 5-pole illumination according to the sixth embodiment. Fig. 45 is a diagram schematically showing a modification of the block element included in the diffractive optical element for 5-pole illumination according to the sixth embodiment. Fig. 46 is a diagram showing a three-pole field formed on the incident surface of the microlens array in the seventh embodiment. Fig. 47 'is a diagram for explaining the basic operation of the diffractive optical element for 3-pole illumination according to the seventh embodiment. Fig. 48 is a diagram schematically showing the entire configuration of a diffractive optical element for 3-pole illumination according to a seventh embodiment. 06 63 200405426 Fig. 49 is a diagram schematically showing the configuration of a block element included in the diffraction optical element for 3-pole illumination according to the seventh embodiment. Fig. 50 is a diagram showing a nine-pole field formed on the incident surface of the microlens array in the eighth embodiment. Fig. 51 is a diagram for explaining the basic operation of a diffractive optical element for 9-pole illumination according to the eighth embodiment. (II) Symbols for component 1 Light source 2 Plastic optics 3, 12 Bending mirrors 4, 6, 61, 62, 63, 100, 101, 5 Non-focus zoom 7 Zoom lens 8 Micro lens array 9 Condensing optics 10 Photomask curtain 11a, lib Imaging optics 13 Photomask 14 Projection optics 15 Wafer Al, D1 First basic winding Bl, El Second basic winding A2, D2 First complementary winding B2, E2 Second complementary winding System 102 Diffractive Optical Element Lens System All Optical Element Optical Element Optical Element Optical Element 64 200405426 al ~ a3 Light

Cld〜C4d,Fid〜F4d,Gld〜G4d 區塊元件 DQ1〜DQ4 合成區塊 G1 〜G4 元件 Η 單純透射部 Hd 補全單純透射部 ΑΧ 光軸 65Cld ~ C4d, Fid ~ F4d, Gld ~ G4d Block elements DQ1 ~ DQ4 Synthetic blocks G1 ~ G4 elements

Claims (1)

^00405426 拾、申請專利範圍: 1 · 一種繞射光學元件,其特徵在於,具備: 第1基本繞射光學元件,其具有沿第丨方向之直線光 柵圖案; 第2基本繞射光學元件,其具有沿不同於該第丨方向 之第2方向之直線光栅圖案; 第1補全繞射光學元件,其對該第丨基本繞射光學元 件所產生之光振幅,具有產生具帛&quot;目位差之光振幅的圖 案;以及 | 第2補全繞射光學元件,其對該第2基本繞射光學元 件所產生之光振幅,具有產生具第2相位差之光振幅的圖 案; 上該第1基本繞射光學元件、該第2基本繞射光學元件 :该第1補全繞射光學元件與該第2補全繞射光學元件, 係大致緊密排列。 2 · —種繞射光學元件,其特徵在於,具備: 第1基本繞射光學元件’其具有沿第1方向之直線光f 柵圖案; 第2基本繞射光學元件,其具有沿不同於該第丨方向 之第2方向之直線光栅圖案;以及 單純透射部,係實質上無偏向作用者; ::第1基本繞射光學元件、該第2基本繞射光學元件 與該單純透射部係大致緊密排列。 3·如申請專利範圍第2項之繞射光學元件,其中,進 66 200405426 一步具備; 第1補全繞射光學元件,其對該第1基本繞射光學元 牛斤產生之光振巾田’具有產生具帛i相位差之光振幅的圖 案; 第2補全繞射光學元件,其對該第2基本繞射光學元 件所產生之光振幅,具有產生具帛2相位差之光振幅的圖 案,以及 補全單純透射部,其對該單純透射部所產生之光振幅 ,具有產生具第5相位差之光振幅的圖案。 4 ·如申請專利範圍帛!項之繞射光學元件,其中,該 第5相位差大致為1/2波長。 5·如申請專利範圍帛卜4項中任一項之繞射光學元 件’其中,該第1相位差與該第2相位差大致為1/2波長 Ο 6·如申請專利範圍帛1〜4項中任-項之繞射光學元 件其中,δ亥繞射光學凡件,具備:複數個該第丄基本繞 射光學元件、複數個該帛2基本繞射光學元件、複數個該 第1補全繞射光學元件與複數個該第2補全繞射光學元件 0 7·如申請專利範圍第6項之繞射光學元件,其中,該 複數個第1基本繞射光學元件、該複數個帛2基本繞射^ 學元件、該複數個第丨補全繞射光學元件與該複數個第2 補全繞射光學元件,彼此大致為同數。 8·如申請專利範圍第6項之繞射光學元件,其中,該 67 200405426 複數個第^基本繞射光學元件、該複數個第2基本繞射光 學凡件、該複數個第工補全繞射光學元件與該複數個第2 補全繞射光學元件,係於該繞射光學元件之全體隨機排列 〇 9如申睛專利範圍第6項之繞射光學元件,其中兮 繞射光學元件具備複數個區塊,各區塊中,該複數個第; 基本㈣光學元件、該複數個第2基本繞射光學元件、該^ 00405426 Patent application scope: 1 · A diffractive optical element, comprising: a first basic diffractive optical element having a linear grating pattern along the first direction; a second basic diffractive optical element, which It has a linear grating pattern along a second direction different from the first direction. The first complementary diffractive optical element has a light amplitude generated by the first basic diffractive optical element. A pattern of the difference in light amplitude; and | a second complementary diffractive optical element having a pattern of generating a light amplitude with a second phase difference to the light amplitude generated by the second basic diffractive optical element; 1 basic diffractive optical element and the second basic diffractive optical element: the first complementary diffractive optical element and the second complementary diffractive optical element are arranged approximately closely. 2. A diffractive optical element, comprising: a first basic diffractive optical element having a linear light f-gate pattern along a first direction; and a second basic diffractive optical element having a shape different from that The linear grating pattern in the second direction and the second direction; and the simple transmission part, which is substantially free of deflection; :: The first basic diffraction optical element, the second basic diffraction optical element, and the simple transmission part are roughly the same Closely arranged. 3. If the diffractive optical element of the second item of the scope of the patent application is applied, it is provided in a step of 66 200405426; The first complementary diffractive optical element is a light vibration field produced by the first basic diffractive optical element. 'Has a pattern that produces a light amplitude with a phase difference of 帛 i; a second complementary diffractive optical element which has a light amplitude of the second basic diffractive optical element which has a light amplitude with a phase difference of 帛 2 The pattern and the simple transmission part are complementary, and the light amplitude generated by the simple transmission part has a pattern that generates a light amplitude with a fifth phase difference. 4 · If the scope of patent application is 帛! In the diffractive optical element, the fifth phase difference is approximately 1/2 wavelength. 5. If the scope of patent application is diffractive optical element according to any one of 4 items, wherein the first phase difference and the second phase difference are approximately 1/2 wavelength. 0 6 If the scope of patent application is 帛 1 ~ 4 Any of the terms-the diffractive optical element of the term, wherein the delta diffractive optical element includes: a plurality of the first basic diffractive optical element, a plurality of the second basic diffractive optical element, and a plurality of the first supplement The full diffractive optical element and the plurality of second complementary diffractive optical elements 0 7 · As the diffractive optical element of the sixth item of the patent application scope, wherein the plurality of first basic diffractive optical elements, the plurality of 帛2 The basic diffraction element, the plurality of complementary diffractive optical elements, and the plurality of second complementary diffractive optical elements are substantially the same as each other. 8. If the diffractive optical element according to item 6 of the scope of patent application, the 67 200405426 plurality of ^ th basic diffractive optical elements, the plurality of second basic diffractive optical elements, and the plurality of first complementary diffractive elements The diffractive optical element and the plurality of second complementary diffractive optical elements are randomly arranged in the entirety of the diffractive optical element. 9 The diffractive optical element as described in item 6 of the patent scope, wherein the diffractive optical element has A plurality of blocks, in each block, the plurality of first; the basic ㈣ optical element, the plurality of second basic diffractive optical elements, the 複數個第1補全繞射光學元件與該複數個第2補全繞射光 學元件,係隨機排列。 、 I 〇 ·如申請專利範圍第9項之繞射光學元件,其各區 塊中’該複數㈣i基本繞射光學元件、該複數個第 本繞射光學元件、該複數個第1補全繞射光學元件與該複 數個第2補全繞射光學元件,彼此大致為同數。 II ·如申請專利範圍第9項之繞射光學元件,其中, 該繞射光學元件具備複數種類之區塊,各種類之每—區塊 f 之卩返機排列形態皆不同。 12·如巾請專利範圍第6項之繞射光學元件,其 具備: 、 Λ第1基本繞射光學元件與該第2基本繞射光學元件 大致同數交互排列的複數個第1區塊; X第1基本繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第2區塊; /第1補全繞射光學元件與該帛2基本繞射光學元件 大致同數交互排列的複數個第3區塊;以及 68 200405426 該第1補全繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第4區塊。 13 ·如申請專利範圍第12項之繞射光學元件,其中, 該繞射光學元件具備複數個中區塊,各中區塊中,該複數 個第1區塊、該複數個第2區塊、該複數個第3區塊與該 複數個第4區塊,係大致同數隨機排列。The plurality of first complementary diffraction optical elements and the plurality of second complementary diffraction optical elements are arranged at random. 1. I. If the diffractive optical element of item 9 in the scope of patent application, in each block, the 'the complex ㈣i basic diffractive optical element, the plurality of first diffractive optical elements, and the plurality of first complementary windings The diffractive optical element and the plurality of second complementary diffractive optical elements are substantially the same as each other. II. For example, the diffractive optical element according to item 9 of the scope of patent application, wherein the diffractive optical element has a plurality of types of blocks, each of which has a different arrangement pattern for each block f. 12. If a diffractive optical element according to item 6 of the patent is requested, it includes: a plurality of first blocks that are arranged alternately in the same number as the first basic diffractive optical element and the second basic diffractive optical element; X a plurality of second blocks in which the first basic diffractive optical element and the second complementary diffractive optical element are arranged in substantially the same number alternately; / the first complementary diffractive optical element and the 帛 2 basic diffractive optical element are roughly A plurality of third blocks arranged in the same number alternately; and a plurality of fourth blocks arranged in the same number in the first complementary diffraction optical element and the second complementary diffraction optical element. 13 · The diffractive optical element according to item 12 of the patent application scope, wherein the diffractive optical element has a plurality of middle blocks, and among the middle blocks, the plurality of first blocks and the plurality of second blocks The plurality of third blocks and the plurality of fourth blocks are randomly arranged in substantially the same number. 14 ·如申請專利範圍第13項之繞射光學元件,其中, 該繞射光學元件具備複數種類之中區塊,各種類之每一中 區塊之隨機排列形態皆不同。 15 ·如申請專利範圍第12項之繞射光學元件,其中, 該繞射光學元件含大致同數的複數個第1〜第4區塊,且 各區塊於該繞射光學元件全體係隨機排列。14. The diffractive optical element according to item 13 of the patent application scope, wherein the diffractive optical element has a plurality of types of middle blocks, and the random arrangement of each of the blocks in each class is different. 15 · If the diffractive optical element according to item 12 of the patent application scope, wherein the diffractive optical element contains a plurality of first to fourth blocks of approximately the same number, and each block is randomized in the entire system of the diffractive optical element arrangement. 16·如申請專利範圍第丨〜4項中任一項之繞射光學元 件’其中’㈣1基本繞射光學元件、該第2基本繞射光 學元件、該第1補全繞射光學元件、以及該第2補全繞射 光學元件,具有大致正方形之外形。 17·如申請專利範圍第16項之繞射光學元件,直中, 該第1方向與該具有大致正方形之外形的繞射光學元件之 一邊大致平行,該帛2方向與該具有大致正方形之外形的 繞射光學元件之另一邊大致平行。 18 ·如申請專利範圍第 件,其中,該直線光栅圖案 案、閃耀型繞射光學元件圖 圖案中之任意一種圖案。 1〜4項中任一項之繞射光學元 ’具有2元型繞射光學元件圖 案、以及多元型繞射光學元件 69 200405426 •一種照明光學系統,係用來照明被照射面,其特 徵在於: 為了在照明光瞳面形成具有4極狀強度分佈的二次光 源’具備用來將入射光束轉換為4個光束之申請專利範圍 第1至第18項中任一項之繞射光學元件。 20 ·如申請專利範圍第19項之照明光學裝置,其中, 進一步具備: ' 光源機構,係用來供應光束; 角度光束形成機構,係將來自該光源裝置之光束轉換 成具有相對光軸之各種角度成份的光束,以射入第1既定 面;以及 ^照野形成機構,其包含繞射光學元件,以根據射入該 第1既定面之該具有各種角度成份的光束,而在第2既定 面上形成4極狀之照野; 該角度光束形成機構,具有由複數個光學元件構成之 之各光 射光學 该繞射光學元件,係被定位成對應該光學構件 予元件的要素光束中,合計包含4個以上之基本鈐 凡件或補全繞射光學元件。 · —種照明光學裝置,其特徵在於,具備: 光源機構,係用來供應光束; 角度光束形成機構,係將來自該光源裝置之光束轉換 成具有相對光軸之各種角度成份的光束, 、 而· A射入第1既定 200405426 照野形成機構,其包含繞射光學元件,以根據射入該 第1既定面之該具有各種角度成份的光束,而在第2既定 面上形成4極狀之照野; 光學積分器,係根據來自該第2既定面上所形成之該 4極狀照野的光束,來形成具有與該4極狀照野大致相同 光強度分佈的4極狀二次光源;以及 導光光學系統’係用來將來自該光學積分器之光束導 向被照射面; 該繞射光學元件,具備複數個第丨基本繞射光學元件 與複數個第2基本繞射光學元件,該第丨基本繞射光學元 件具有沿第1方向的直線光柵,而該第2基本繞射光學元 件具有沿不同於該第丨方向之第2方向的直線光柵,該複 數個第1基本繞射光學元件與該複數個第2基本繞射光學 元件,係大致緊密排列。 22 ·如申請專利範圍第21項之照明光學裝置,其中, 该複數個第1基本繞射光學元件與該複數個第2基本繞射 光學元件,係大致同數交互排列。 23 ·如申請專利範圍第21或22項之照明光學裝置, 其中,該繞射光學元件,具備·· 複數個第1補全繞射光學元件,其對該第i基本繞射 光學7L件所產生之光振幅,具有產生具第1相位差之光振 幅的圖案;以及 複數個第2補全繞射光學元件,其對該第2基本繞射 光學元件所產生之光振幅’具有產生具第2相位差之光振 200405426 幅的圖案; 口亥複數個第1基本繞射光學元件、該複數個第2基本 繞^光學元件、該複數個第i補全繞射光學元件與該複數 個第2補全繞射光學元件,係大致緊密排列。 24 ·如申請專利範圍第23項之照明光學裝置,其中, X第1相位差與s亥第2相位差大致為1 /2波長。 25·如申請專利範圍第23項之照明光學裝置,其中, d m數個第1基本繞射光學元件、該複數個第2基本繞射 光學元件、該複數個第丨補全繞射光學元件與該複數個第^ 2補全繞射光學元件,彼此大致為同數。 26 ·如申請專利範圍第23項之照明光學裝置,其中, 該複數個第1基本繞射光學元件、該複數個第2基本繞射 光學元件、該複數個第i補全繞射光學元件與該複數個第 2補全繞射光學元件,係於該繞射光學元件之全體隨機排 列。 27 ·如申請專利範圍第23項之照明光學裝置,其中,, 該繞射光學元件具備複數個區塊,各區塊中,該複數個第| 1基本繞射光學元件、該複數個帛2基本繞射光學元件、 該複數個第1補全繞射光學元件與該複數個第2補全繞射 光學元件,係隨機排列。 A 28 ·如申請專利範圍第27項之照明光學裝置,其各區 塊中’該複數個第i基本繞射光學元件、該複數個第2: 本繞射光學元件、該複數個第!補全繞射光學元件與該複 數個第2補全繞射光學元件,彼此大致為同數。 72 月專利乾圍弟27項之照明光學裝置,其中, 该繞射光學元彳來1 #+ _ ^ 牛/、備複數種類之區塊,各種類之每一區塊 之Ik機排列形態皆不同。 3〇 ·如申請專利範圍第23項之照明光學裝置,其中, 具備: ^第1基本繞射光學元件與該第2基本繞射光學元件 大致同數父互排列的複數個第1區塊; °亥第1基本繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第2區塊; A第1補全繞射光學元件與該第2基本繞射光學元件 大致同數又互排列的複數個第3區塊·,以及 4第1補全繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第4區塊。 31 ·如申請專利範圍第3〇項之照明光學裝置,其中, 该繞射光學元件具備複數個中區塊,各中區塊中,該複數 個第1區塊、該複數個第2區塊、該複數個第3區塊與該 複數個第4區塊,係大致同數隨機排列。 32 ·如申請專利範圍第31項之照明光學裝置,其中, 4繞射光學元件具備複數種類之中區塊,各種類之每一中 區塊之隨機排列形態皆不同。 33 ·如申請專利範圍第30項之照明光學裝置,其中, 該繞射光學元件含大致同數的該複數個第1〜第4區塊, 且各區塊於該繞射光學元件全體係隨機排列。 3 4 ·如申晴專利範圍第21或2 2項之照明光學裝置, 73 200405426 其中’该帛1基本繞射光學元件、該第2基本繞射光學元 件、該第1補全繞射光學元件、以及該帛2補全繞射光學 元件,具有大致正方形之外形。 35·如申請專利範圍第34項之照明光學裝置,其中, 忒第1方向與該具有大致正方形之外形的繞射光學元件之 一邊大致平行,該第2方向與該具有大致正方形之外形的 繞射光學元件之另一邊大致平行。 36·如申請專利範圍第21或22項之照明光學裝置, 其中’ 3亥角度光束形成機構具備由複數個光學元件構成之$ 光學構件; 該繞射光學元件,係被定位成對應該光學構件之各光 學元件的要素光束中,合計包含4個以上之基本繞射光學 元件或補全繞射光學元件。 37 ·如申請專利範圍第35項之照明光學裝置,其中, $亥照野形成機構’具有配置在該繞射光學元件與該光學積 分器間之光程中的光學系統; 設構成該4極狀二次光源之各面光源的大小為必、具· 有4大致正方形外形之該基本繞射光學元件一邊的為 L、光束之中心波長為λ、該光學系統之焦距為f時二足 以下條件 、 L&gt; 2· 5xf X 入 / 0。 38 · -種照明光學裝置,係用來照明被照射面,其特 於: z、 為了在照明光曈面形成具冑2極&amp;強度分佈之二次光 74 200405426 源,具備用來將入射光束轉換為2個光束的繞射光學元件 該繞射光學元件,具有沿既定方向之直線光柵圖案的 複數個基本繞射光學元件,與對該基本繞射光學元件所產 生之光振幅,具有產生具既定相位差之光振幅之圖案的複 數個補全繞射光學元件; 忒複數個基本繞射光學元件與該複數個補全繞射光學 元件,係大致緊密排列。 39 · 一種照明光學裝置,係用來照明被照射面,其特$ 徵在於: 為了在照明光瞳面形成具有3極狀強度分佈之二次光 源,具備用來將入射光束轉換為3個光束的繞射光學元件 , 忒繞射光學元件,具有沿既定方向之直線光栅圖案的 複數個基本繞射光學元件,與實質上無偏向作用的複數個 單純透射部; 孩複數個基本繞射光學元件與該複數個單純透射部,| 係大致緊密排列。 40 ·如申請專利範圍第39項之照明光學裝置,其中, 進一步具備: 複數個補全繞射光學元件,其對該基本繞射光學元件 所產生之光振幅’具有產生具既定相位差之光振幅的圖案 ;以及 補全單純透射部,其對該單純透射部所產生之光振幅 75 200405426 ’具有產生具第5相位差之光振幅的圖案。 41 ·如申請專利範圍第40項之照明光學裝置,其中, 該第5相位差大致為1 / 2波長。 42 ·如申請專利範圍第38〜41項中任一項之照明光學 裝置’其中’該既定相位差大致為1 / 2波長。 43 ·如申請專利範圍第38〜41項中任一項之照明光學 裝置’其中’該複數個基本繞射光學元件與該複數個補全 繞射光學元件’彼此大致為同數。 44 ·如申請專利範圍第38〜41項中任一項之照明光學 裝置’其中’該複數個基本繞射光學元件與該複數個補全 繞射光學元件,於該繞射光學元件全體係隨機排列。 4 5 ·如申睛專利範圍第3 8〜41項中任一項之照明光學 裝置,其中,該繞射光學元件具備複數個區塊,各區塊中 ,該複數個基本繞射光學元件與該複數個補全繞射光學元 件,係大致同數隨機排列。 46 ·如申請專利範圍第45項之照明光學裝置,其中, 4繞射光學7L件具備複數種類之區塊,各種類之每一區塊 ,孩複數個基本繞射光學元件與該複數個補全繞射光學元 件之隨機排列形態皆不同。 女申明專利範圍第3 8〜41項中任一項之照明光學 表置〃中忒基本繞射光學元件與該補全繞射光學元件 ,具有大致正方形之外形。 η 48·如申請專利範圍第38〜41項中任一項之照明光學 破置其中,该直線光栅圖案,具有2元型繞射光學元件 76 200405426 圖案、閃耀型繞射光學元件圖案、以及多元型繞射光學元 件圖案中之任意一種圖案。 49 · 一種照明光學系統,係用來照明被照射面,其特 徵在於: 為了在照明光瞳面形成具有8極狀強度分佈的二次光 源’具備用來將入射光束轉換為8個光束的繞射光學元件 方向之直線光16. If the diffractive optical element according to any one of items 1-4 of the patent application 'wherein': ㈣1 basic diffractive optical element, the second basic diffractive optical element, the first complementary diffractive optical element, and The second complementary diffractive optical element has a substantially square outer shape. 17. If the diffractive optical element according to item 16 of the patent application scope, the first direction is substantially parallel to one side of the diffractive optical element having a substantially square outer shape, and the 帛 2 direction is substantially parallel to the substantially square external shape. The other side of the diffractive optical element is substantially parallel. 18 · According to the patent application, any one of the linear grating pattern scheme and the blaze-type diffractive optical element pattern pattern. The diffractive optical element of any one of items 1 to 4 has a two-element diffractive optical element pattern and a multi-type diffractive optical element 69 200405426 • An illumination optical system for illuminating the illuminated surface, which is characterized in that : In order to form a secondary light source with a quadrupole intensity distribution on the illumination pupil surface, it is provided with a diffractive optical element according to any of claims 1 to 18 of the patent application scope for converting an incident light beam into four light beams. 20 · The illumination optical device according to item 19 of the patent application scope, further comprising: 'a light source mechanism for supplying a light beam; an angular beam forming mechanism for converting a light beam from the light source device into various types having a relative optical axis The light beam with the angle component is incident on the first predetermined surface; and the illumination field forming mechanism includes a diffractive optical element to transmit the light beam with various angle components into the first predetermined surface according to the light beam having various angle components incident on the first predetermined surface. A quadrupole-shaped light field is formed on the surface; the angle beam forming mechanism has a plurality of light emitting optics composed of a plurality of optical elements, and the diffractive optical element is positioned in the element beam corresponding to the optical element and the element, In total, it contains more than 4 basic ordinary pieces or complementary diffractive optical elements. -An illumination optical device, comprising: a light source mechanism for supplying a light beam; an angular beam forming mechanism for converting a light beam from the light source device into a light beam having various angular components relative to an optical axis, and · A shot into the first predetermined 200405426 photofield formation mechanism, which includes diffractive optical elements to form a 4-pole-shaped beam on the second predetermined surface based on the light beams having various angular components incident on the first predetermined surface. Photofield; an optical integrator that forms a quadrupole secondary light source with approximately the same light intensity distribution as the quadrupole field according to the light beam from the quadrupole field formed on the second predetermined surface ; And the light-guiding optical system 'is used to guide the light beam from the optical integrator to the illuminated surface; the diffractive optical element includes a plurality of first basic diffractive optical elements and a plurality of second basic diffractive optical elements, The second basic diffractive optical element has a linear grating in a first direction, and the second basic diffractive optical element has a linear grating in a second direction different from the first direction The plurality of first basic diffractive optical elements and the plurality of second basic diffractive optical elements are substantially closely arranged. 22. The illumination optical device according to item 21 of the patent application scope, wherein the plurality of first basic diffraction optical elements and the plurality of second basic diffraction optical elements are arranged in approximately the same number alternately. 23 · If the illuminating optical device according to item 21 or 22 of the scope of patent application, wherein the diffractive optical element is provided with a plurality of first complementary diffractive optical elements, the 7th basic diffractive optical element The generated light amplitude has a pattern that generates a light amplitude with a first phase difference; and a plurality of second complementary diffractive optical elements, which have a generated light amplitude to the second basic diffractive optical element. 2 patterns of phase-shifted optical vibrations of 200,405,426; a plurality of first basic diffraction optical elements, the plurality of second basic diffraction optical elements, the plurality of i-th complementary diffraction optical elements, and the plurality of first 2 Complement the diffractive optical elements, which are roughly arranged closely. 24. The illumination optical device according to item 23 of the patent application, wherein the first phase difference between X and second phase is approximately 1/2 wavelength. 25. The illumination optical device according to item 23 of the scope of patent application, wherein the dm number of the first basic diffractive optical elements, the plurality of second basic diffractive optical elements, the plurality of first complementary diffractive optical elements, and The plurality of second complementary diffraction optical elements are substantially the same as each other. 26. The illumination optical device according to item 23 of the scope of patent application, wherein the plurality of first basic diffractive optical elements, the plurality of second basic diffractive optical elements, the plurality of i-th complementary diffractive optical elements, and The plurality of second complementary diffractive optical elements are randomly arranged on the entirety of the diffractive optical elements. 27. The illumination optical device according to item 23 of the patent application scope, wherein the diffractive optical element has a plurality of blocks, and in each block, the plurality of | 1 basic diffractive optical elements, the plurality of 帛 2 The basic diffractive optical element, the plurality of first complementary diffractive optical elements, and the plurality of second complementary diffractive optical elements are arranged randomly. A 28 · If the illumination optical device of the 27th scope of the patent application, in each of the blocks, the plurality of ith basic diffractive optical elements, the plurality of second diffractive optical elements: the diffractive optical element, the plurality of first! The complementary diffractive optical element and the plurality of second complementary diffractive optical elements are substantially the same as each other. The 72-year patent for the lighting optical device of 27 items, among which, the diffractive optical element 彳 来 1 # + _ ^ cattle, multiple types of blocks, the arrangement of the Ik machine of each block of each type is different. 30. The illumination optical device according to item 23 of the scope of patent application, which comprises: ^ a plurality of first blocks of the first basic diffractive optical element and the second basic diffractive optical element arranged substantially in the same order; ° The first and second basic diffractive optical elements and the second complementary diffractive optical element are arranged alternately in the same number of the second block; A the first complementary diffractive optical element and the second basic diffractive optical element A plurality of third blocks that are approximately the same number and are aligned with each other, and a plurality of fourth blocks in which the first complementary diffraction optical element and the second complementary diffraction optical element are arranged in substantially the same number alternately. 31. The illumination optical device according to claim 30 of the patent application scope, wherein the diffractive optical element is provided with a plurality of middle blocks, and among the middle blocks, the plurality of first blocks and the plurality of second blocks The plurality of third blocks and the plurality of fourth blocks are randomly arranged in substantially the same number. 32. If the illumination optical device according to item 31 of the patent application scope, wherein the 4-diffractive optical element has a plurality of types of middle blocks, the random arrangement of each of the blocks in each class is different. 33. The illumination optical device according to item 30 of the scope of patent application, wherein the diffractive optical element includes the plurality of first to fourth blocks having substantially the same number, and each block is randomly arranged in the entire system of the diffractive optical element. arrangement. 3 4 · For example, the illumination optics of item 21 or 22 of Shen Qing's patent scope, 73 200405426, where the 帛 1 basic diffractive optical element, the second basic diffractive optical element, and the first complementary diffractive optical element And the 帛 2 complementary diffractive optical element has a substantially square outer shape. 35. The illumination optical device according to item 34 of the patent application, wherein the first direction is substantially parallel to one side of the diffractive optical element having a substantially square outer shape, and the second direction is substantially parallel to the light having a substantially square outer shape. The other side of the radiation optical element is substantially parallel. 36. If the illumination optical device according to item 21 or 22 of the patent application scope, wherein the '30 -degree angle beam forming mechanism includes an optical member composed of a plurality of optical elements; the diffractive optical element is positioned to correspond to the optical member The elementary beam of each optical element includes a total of four or more basic diffractive optical elements or complementary diffractive optical elements. 37. The illumination optical device according to item 35 of the scope of patent application, wherein the $ 海 照 野 formation mechanism has an optical system arranged in the optical path between the diffractive optical element and the optical integrator; The size of each surface light source of the secondary secondary light source is required. The basic diffractive optical element with 4 approximately square shape is L on one side, the center wavelength of the beam is λ, and the focal length of the optical system is f. Conditions, L &gt; 2.5xf X in / 0. 38 ·-An illumination optical device, which is used to illuminate the irradiated surface, and has the following characteristics: z. In order to form a secondary light with a 2-pole &amp; intensity distribution on the illumination light surface 74 200405426 source, which is used to A diffractive optical element that converts a light beam into two light beams. The diffractive optical element has a plurality of basic diffractive optical elements having a linear grating pattern along a predetermined direction, and a light amplitude generated by the basic diffractive optical element. A plurality of complementary diffractive optical elements having a pattern of light amplitude with a predetermined phase difference; (2) A plurality of basic diffractive optical elements and the plurality of complementary diffractive optical elements are arranged approximately closely. 39 · An illumination optical device is used to illuminate the illuminated surface. Its characteristics are as follows: In order to form a secondary light source with a 3-pole intensity distribution on the illumination pupil surface, it is provided with a function to convert the incident beam into 3 beams. Diffractive optical element, chirped diffractive optical element, having a plurality of basic diffractive optical elements having a linear grating pattern along a predetermined direction, and a plurality of simple transmitting portions having substantially no deflection effect; a plurality of basic diffractive optical elements The | are approximately closely aligned with the plurality of simple transmission portions. 40. The illumination optical device according to item 39 of the patent application scope, further comprising: a plurality of complementary diffractive optical elements having light amplitudes' of the light generated by the basic diffractive optical element to generate light with a predetermined phase difference. A pattern of amplitude; and a simple transmission portion that complements the light amplitude 75 200405426 of the simple transmission portion with a pattern that generates a light amplitude with a fifth phase difference. 41. The illumination optical device according to claim 40, wherein the fifth phase difference is approximately 1/2 wavelength. 42. The illumination optical device according to any one of claims 38 to 41 of the scope of the patent application, wherein the predetermined phase difference is approximately 1/2 wavelength. 43. The illumination optical device ′ according to any one of claims 38 to 41 of the patent application scope, wherein ‘the plurality of basic diffractive optical elements and the plurality of complementary diffractive optical elements ′ are substantially the same as each other. 44 · If the illumination optical device according to any one of claims 38 to 41 of the application scope 'wherein' the plurality of basic diffractive optical elements and the plurality of complementary diffractive optical elements are randomized in the entire system of the diffractive optical elements arrangement. 4 5 · The illumination optical device according to any one of items 38 to 41 in the patent scope of Shenyan, wherein the diffractive optical element has a plurality of blocks, and in each block, the plurality of basic diffractive optical elements and the The plurality of complementary diffractive optical elements are arranged at substantially the same random number. 46. For example, the illumination optical device according to item 45 of the scope of patent application, in which 4L optical 7L pieces have a plurality of types of blocks, each type of each block, a plurality of basic diffractive optical elements and the plurality of supplements The random arrangement of full-diffraction optical elements is different. The female claimed that the scope of patents for any one of the 38 to 41 patents for illumination optics, including the central diffractive optical element and the complementary diffractive optical element, has a roughly square shape. η 48 · If the illumination optics of any one of items 38 to 41 of the scope of patent application is broken, the linear grating pattern has a two-element diffractive optical element 76 200405426 pattern, a blaze-type diffractive optical element pattern, and multiple elements. Any one of the patterns of the diffractive optical element pattern. 49 · An illumination optical system for illuminating the illuminated surface, characterized in that: to form a secondary light source with an 8-pole intensity distribution on the illumination pupil surface, it is provided with a winding for converting an incident light beam into 8 light beams; Linear light in the direction of the optical element 该繞射光學元件,具備: 第1基本繞射光學元件,其具有沿第 柵圖案; 第2基本繞射光學元件,其具有沿第2方向之直線光 柵圖案,該第2方向與該第丨方向大致正交; 第3基本繞射光學元件,其具有沿第3方向之直線光 柵圖案,該第3方向與該第}方向大致成45度;以及 第4基本繞射光學元件,其具有沿第4方向之直線光 柵圖案,該第4方向與該第1方向大致成45度、且與該第 3方向大致正交; 该第1〜第4基本繞射光學元件係大致緊密排列。 50 ·如申凊專利範圍第項之照明光學裝置,其中, 該繞射光學元件進一步具備·· 第1補全繞射光學元件,其對該第丨基本繞射光學元 件所產生之光振幅,具有產生具第丨相位差之光振幅的圖 案; 第2補全繞射光學元件,其對該第2基本繞射光學元 77 200405426 件所產生之光振幅,具有產生具第2相位差之光振幅的圖 案; 第3補全繞射光學元件,其對該第3基本繞射光學元 件所產生之光振幅,具有產生具第3相位差之光振幅的圖 案;以及 第4補全繞射光學元件,其對該第4基本繞射光學元 件所產生之光振幅,具有產生具第4相位差之光振幅的圖 案; 該第1〜第4基本繞射光學元件與該第丨〜第4補全繞 射光學元件,係大致緊密排列。 51 ·如申請專利範圍第50項之照明光學裝置,其中, 該第1相位差、該第2相位差、該第3相位差及該第4相 位差,大致為1 / 2波長。 52 ·如申請專利範圍第50或51項之照明光學裝置, 其中,該繞射光學元件,具備複數個該第丨〜第4基本綍 射光學元件與複數個該第丨〜第4補全繞射光學元件。' 53 ·如申請專利範圍第52項之照明光學裝置,其中, 該複數個第丨〜第4基本繞射光學元件與該複數個第1〜第 4補全繞射光學元件,彼此大致為同數。 54 ·如申請專利範圍第52項之照明光學裝置,其中 該複數個第1〜第4基本繞射光學元件與該複數個第1〜第 4補全繞射光學元件,係於該繞射光學元件之全體隨^排 列。 55 ·如申請專利範圍第52項之照明光學裝置,其中 78 200405426 忒繞射光學兀件具備複數個區塊,各區塊中,該複數個第 1〜第4基本繞射光學元件與該複數個第H 4補全繞射 光學元件,係隨機排列。 56 ·如申睛專利範圍帛55工員之照明光學裝f ,其各區 塊中4複數個第1〜第4基本繞射光學元件與該複數個 第1〜第4補全繞射光學元件,彼此大致為同數。 57如申a月專利範圍第55項之照明光學裝置,其中, 該繞射光學it件具備複數種類之區塊,各種類之每一區塊 之隨機排列形態皆不同。 58如申4專利範圍第52項之照明光學裝置,其中, 具備: 省第1基本繞射光學元件與該第2基本繞射光學元件 大致同數交互排列的複數個第1區塊; 忒第1基本繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第2區塊;The diffractive optical element includes: a first basic diffractive optical element having a pattern along a first grid; a second basic diffractive optical element having a linear grating pattern in a second direction; the second direction and the first The directions are substantially orthogonal; a third basic diffractive optical element having a linear grating pattern along a third direction, the third direction being approximately 45 degrees from the} direction; and a fourth basic diffractive optical element having a along A linear grating pattern in a fourth direction, the fourth direction being approximately 45 degrees from the first direction and being substantially orthogonal to the third direction; the first to fourth basic diffractive optical elements are approximately closely arranged. 50 · The illumination optical device according to the first item of the patent scope of the application, wherein the diffractive optical element further includes a first complementary diffractive optical element, which has an amplitude of light generated by the first basic diffractive optical element, It has a pattern that generates a light amplitude with a second phase difference; a second complementary diffractive optical element that generates a light amplitude to the second basic diffraction optical element 77 200405426 and has a light that has a second phase difference A pattern of amplitude; a third complementary diffractive optical element having a pattern for generating a light amplitude with a third phase difference to the third basic diffractive optical element; and a fourth complementary diffractive optical element Element having a pattern of light amplitude generated by the fourth basic diffractive optical element to generate a light amplitude with a fourth phase difference; the first to fourth basic diffractive optical elements and the fourth to fourth supplements Full-diffraction optics are roughly closely spaced. 51. The illumination optical device according to Claim 50 of the application, wherein the first phase difference, the second phase difference, the third phase difference, and the fourth phase difference are approximately 1/2 wavelengths. 52. The illumination optical device according to the 50th or 51st scope of the application for a patent, wherein the diffractive optical element includes a plurality of the fourth to fourth basic diffractive optical elements and a plurality of the fourth to fourth complementary windings.射 optical components. '53 · If the illumination optical device according to item 52 of the patent application scope, wherein the plurality of first to fourth basic diffractive optical elements and the plurality of first to fourth complementary diffractive optical elements are substantially the same as each other number. 54. The illumination optical device according to item 52 of the application, wherein the plurality of first to fourth basic diffraction optical elements and the plurality of first to fourth complementary diffraction optical elements are attached to the diffractive optics. The whole of the components is arranged with ^. 55 · If the illumination optical device according to item 52 of the patent application scope, 78 200405426 The diffractive optical element has a plurality of blocks, and in each block, the plurality of first to fourth basic diffractive optical elements and the complex number The H-th complementary diffractive optical elements are arranged randomly. 56 · If the patent scope of Shenjing 帛 55 workers ’lighting optics f, each of the four first to fourth basic diffractive optical elements and the plurality of first to fourth complementary diffractive optical elements in each block, They are roughly the same number. 57 For example, the illumination optical device of the 55th scope of the patent application, wherein the diffractive optical it has a plurality of types of blocks, and the random arrangement of each block of each type is different. 58 The illumination optical device according to item 52 in the scope of patent No. 4, including: a plurality of first blocks arranged in the same number as the first basic diffractive optical element and the second basic diffractive optical element; 1 a plurality of second blocks arranged substantially alternately with the basic complementary diffractive optical element and the second complementary diffractive optical element; 4第1補全、繞射光學元件與該第2基本繞射光學元件 大致同數交互排列的複數個第3區塊; 。亥第1補全繞射光學元件與該第2補全繞射光學元件 大致同數交互排列的複數個第4區塊; A第3基本繞射光學元件與該第4基本繞射光學元件 大致同數交互排列的複數個第5區塊; 汶第3基本繞射光學元件與該第4補全繞射光學元件 大致同數交互排列的複數個第6區塊; 。亥第3補全繞射光學元件與該第4基本繞射光學元件 79 200405426 大致同數交互排列的複數個第7區塊;以及 4第3補全繞射光學元件與該第4補全繞射光學元件 大致同數又互排列的複數個第8區塊。 59 ·如申請專利範圍第58項之照明光學裝置,其中, 該繞射光學元件具備複數個中區塊,各中區塊中,該複數 個第1〜f 8區i免,係大致同數隨機排列。 60 ·如申請專利範圍第59項之照明光學裝置,其中, &quot;玄、凡射光予元件具備複數種類之中區塊,各種類之每一中 區塊之隨機排列形態皆不同。 61 ·如申請專利範圍第58項之照明光學裝置,其中, 该繞射光學元件含大致同數的該複數個第1〜第8區塊, 且各區塊於該繞射光學元件全體係隨機排列。 62 · —種照明光學裝置,係用來照明被照射面,其特 徵在於,具備·· 光源機構,係用來供應光束; 角度光束形成機構,係將來自該光源裝置之光束轉換 成具有相對光軸之各種角度成份的光束,以射入第1既定 面;以及 照野形成機構,其包含繞射光學元件,以根據射入該 第1既定面之該具有各種角度成份的光束,在第2既定面 上形成複數極狀之照野; 該繞射光學元件,係將具有既定繞射光學元件圖案之 複數個基本繞射光學元件予以緊密排列而構成; 該角度光束形成機構,具有由複數個光學元件構成之 200405426 光學構件; 該繞射光學元件,係被定位成對應該光學構件之各光 學7L件的要素光束中,合計包含4個以上之基本繞射光學 元件或補全繞射光學元件。 · —種照明光學裝置,其特徵在於,具備: 光源機構,係用來供應光束; 角度光束形成機構,係將來自該光源裝置之光束轉換4 a plurality of third blocks in which the first complementary, diffractive optical element and the second basic diffractive optical element are arranged in approximately the same number alternately; A plurality of fourth blocks in which the first complementary diffractive optical element and the second complementary diffractive optical element are arranged in substantially the same number alternately; A third basic diffractive optical element and the fourth basic diffractive optical element are roughly A plurality of fifth blocks arranged alternately in the same number; a plurality of sixth blocks arranged alternately in the same number as the third basic diffraction optical element and the fourth complementary diffraction optical element; The third complementary diffraction optical element and the fourth basic diffraction optical element 79 200405426, a plurality of seventh blocks arranged in approximately the same number; and the fourth third complementary diffraction optical element and the fourth complementary diffraction optical element There are a plurality of eighth blocks of the same number of optical elements arranged in parallel. 59. The illumination optical device according to item 58 of the scope of patent application, wherein the diffractive optical element has a plurality of middle blocks, and in each of the middle blocks, the plurality of first to f-th regions i are free, which are approximately the same number. Randomly arranged. 60. For example, the illumination optical device of the 59th scope of the application for a patent, wherein the &quot; Xuan and Fanguang elements have a plurality of types of middle blocks, and the random arrangement of each of the blocks in each class is different. 61. The illumination optical device according to item 58 of the scope of patent application, wherein the diffractive optical element includes the plurality of first to eighth blocks of approximately the same number, and each block is randomized in the entire system of the diffractive optical element. arrangement. 62 · — An illumination optical device for illuminating the illuminated surface, which is provided with a light source mechanism for supplying a light beam; an angular beam forming mechanism for converting a light beam from the light source device into a light having a relative light The light beams of various angular components of the axis are incident on the first predetermined surface; and the illumination field forming mechanism includes a diffractive optical element so that the light beams of various angular components incident on the first predetermined surface are incident on the second surface. A plurality of polar fields are formed on a predetermined surface; the diffractive optical element is formed by closely arranging a plurality of basic diffractive optical elements having a predetermined diffractive optical element pattern; the angle beam forming mechanism includes a plurality of 200405426 optical component composed of optical elements; the diffractive optical element is positioned to correspond to the elementary beam of each optical 7L piece of the optical component, and contains a total of 4 or more basic diffractive optical elements or complementary diffractive optical elements . · An illumination optical device, comprising: a light source mechanism for supplying a light beam; an angular beam forming mechanism for converting a light beam from the light source device 成具有相對光軸之各種角度成份的光束,以射入第1既定 面; 照野形成機構,其包含繞射光學元件,以根據射入該 第1既定面之該具有各種角度成份的光束,而在第2既定 面上形成複數極狀之照野; 光學積分器,係根據來自該第2既定面上所形成之該 複數極狀照野的光束,來形成具有與該複數極狀照野大致 相同光強度分佈的複數極狀二次光源;以及 導光光學系統 向被照射面; 係用來將來自該光學積分器之光束導Forming a light beam having various angle components relative to the optical axis so as to be incident on the first predetermined surface; a field forming mechanism including a diffractive optical element for according to the light beam having various angle components entering the first predetermined surface, A plurality of polar fields are formed on the second predetermined surface. The optical integrator is based on the light beams from the plurality of polar fields that are formed on the second predetermined surface. Multiple polar secondary light sources with approximately the same light intensity distribution; and a light-guiding optical system toward the illuminated surface; used to guide the light beam from the optical integrator 该繞射光學元件,係將具有大致正方形外形、且具有 既疋繞射光學元件圖案之複數個基本繞射光學元件予以緊 密排列而構成; 該照野形成機構,具有配置在該繞射光學元件與該光 學積分器間之光程中的光學系統; 设構成該複數極狀二次光源之各面光源的大小為必、 該基本繞射光學元件-邊的長度|L、光束之中心波長為 81 200405426 A、該光學系統之焦距為f時,滿足以下條件 L&gt;2.5xfx 又/ 0 。 64· —種折射光學元件,其特徵在於·· 其產生與申請專利範圍第】〜18項中任n繞射光 學兀件、或申請專利範圍第38〜48項中任一項之照明光風 裝置中之繞射光學元件大致相同的光振幅。 65 · -種照明光學裝置,係用來照明被照射面, 徵在於·· 八特The diffractive optical element is constituted by closely arranging a plurality of basic diffractive optical elements having a substantially square shape and a pattern of existing diffractive optical elements; the light field forming mechanism is provided with the diffractive optical element; The optical system in the path length between the optical integrator and the optical integrator; Suppose that the size of each surface light source constituting the complex polar secondary light source is required, the length of the basic diffractive optical element-side | L, and the center wavelength of the light beam are 81 200405426 A. When the focal length of this optical system is f, the following condition L &gt; 2.5xfx / 0 is satisfied. 64 · —A kind of refractive optical element, which is characterized by its production and application of any of the n-diffractive optical elements in the scope of the application] ~ 18, or an illumination light wind device in any of the scope of the application of the patent in 38 ~ 48 The diffractive optical elements are approximately the same light amplitude. 65 ·-a kind of lighting optics, which is used to illuminate the illuminated surface, characterized by ... 為了在照明《瞳面形成具有既$強度分佈%二次光源 ,具備用來將入射光束轉換既定截面形狀之光束之申請專 利範圍第64項之折射光學元件。 66 · —種曝光裝置,其特徵在於,具備: 申請專利範圍第19〜63項中任一項、或第65項之照 明光學裝置;以及 f 投影光學系統,係用來將配置在該被照射面之光罩之 圖案投影曝光至感光性基板。 67 · —種曝光方法,其特徵在於: 係透過申請專利範圍第19〜63項中任一項、或第65 項之照明光學裝置來照明光罩,將被照明之該光罩上形成 之圖案之像投影曝光至感光性基板上。 拾壹、囷式·· 如次頁 82In order to form a secondary light source with an existing intensity distribution% on the pupil surface of the illumination, a refracting optical element according to the application patent No. 64 for converting an incident beam into a beam having a predetermined cross-sectional shape is provided. 66 · An exposure device, comprising: an illumination optical device according to any one of claims 19 to 63 or 65 in the scope of patent application; and an f projection optical system for arranging the light to be irradiated The pattern of the face mask is projected and exposed on the photosensitive substrate. 67 · — An exposure method, characterized in that: the photomask is illuminated through the illumination optical device of any of the patent application scopes 19 to 63 or 65, and the pattern formed on the photomask to be illuminated The image is projected and exposed on a photosensitive substrate. Picking up, 囷 style ... as next page 82
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TWI407246B (en) * 2005-10-07 2013-09-01 V Technology Co Ltd Photomask and exposure method using same
TWI466748B (en) * 2010-12-28 2015-01-01 Qmc Co Ltd Laser processing apparatus

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WO2020153504A1 (en) * 2019-01-25 2020-07-30 大日本印刷株式会社 Diffractive optical device, illumination apparatus, projection apparatus, projection display apparatus, and method for manufacturing element diffractive optical device

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