JPH0817720A - Projection exposure device - Google Patents

Projection exposure device

Info

Publication number
JPH0817720A
JPH0817720A JP6170378A JP17037894A JPH0817720A JP H0817720 A JPH0817720 A JP H0817720A JP 6170378 A JP6170378 A JP 6170378A JP 17037894 A JP17037894 A JP 17037894A JP H0817720 A JPH0817720 A JP H0817720A
Authority
JP
Japan
Prior art keywords
optical system
reflecting
optical element
projection
exposure apparatus
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP6170378A
Other languages
Japanese (ja)
Inventor
Kazuo Ushida
一雄 牛田
Koichi Matsumoto
宏一 松本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nikon Corp
Original Assignee
Nikon Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nikon Corp filed Critical Nikon Corp
Priority to JP6170378A priority Critical patent/JPH0817720A/en
Publication of JPH0817720A publication Critical patent/JPH0817720A/en
Pending legal-status Critical Current

Links

Classifications

    • 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
    • G03F7/70216Mask projection systems
    • G03F7/70233Optical aspects of catoptric systems, i.e. comprising only reflective elements, e.g. extreme ultraviolet [EUV] projection systems
    • 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
    • G02B27/0025Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration
    • G02B27/0037Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration with diffracting elements
    • G02B27/0043Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration with diffracting elements in projection exposure systems, e.g. microlithographic systems
    • 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
    • G02B27/4205Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having a diffractive optical element [DOE] contributing to image formation, e.g. whereby modulation transfer function MTF or optical aberrations are relevant
    • G02B27/4222Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having a diffractive optical element [DOE] contributing to image formation, e.g. whereby modulation transfer function MTF or optical aberrations are relevant in projection exposure systems, e.g. photolithographic systems
    • 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
    • G02B27/4272Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having plural diffractive elements positioned sequentially along the optical path
    • G02B27/4277Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect having plural diffractive elements positioned sequentially along the optical path being separated by an air space
    • 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
    • G03F7/70216Mask projection systems
    • G03F7/70316Details of optical elements, e.g. of Bragg reflectors, extreme ultraviolet [EUV] multilayer or bilayer mirrors or diffractive optical elements

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)

Abstract

(57)【要約】 【目的】 反射型の縮小投影露光装置を構築し、透過屈
折レンズを用いることができないような短波長域におい
ても使用できる投影光学系を提供すること。 【構成】 光源手段からの光束をマスクに照射すること
により投影光学系を介して前記マスクのパターンを感光
基板上へ露光する投影露光装置であって、前記投影光学
系は、曲面上の反射面を持つ複数の反射部材と、少なく
とも一つの回折光学素子とを含むもの。前記回折光学素
子が、反射部材の反射面に形成されているもの。
(57) [Summary] [Object] To construct a reflection type reduction projection exposure apparatus and to provide a projection optical system which can be used even in a short wavelength region where a transmission refraction lens cannot be used. A projection exposure apparatus that exposes a pattern of the mask onto a photosensitive substrate through a projection optical system by irradiating a light beam from a light source means on the mask, wherein the projection optical system has a curved reflecting surface. Including a plurality of reflecting members having at least one diffractive optical element. The diffractive optical element is formed on the reflecting surface of a reflecting member.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、例えばマスクに形成さ
れた所定のパターンを感光基板上に投影露光するために
使用される反射型の投影露光装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a reflection type projection exposure apparatus used for projecting a predetermined pattern formed on a mask onto a photosensitive substrate.

【0002】[0002]

【従来の技術】従来からICやLSI等の半導体素子や
これに類する液晶素子、薄膜直ヘッド等の微細パターン
を有する部材の製造工程においては、所定のパターンの
転写露光を伴ういわゆるリソグラフィ工程が応用されて
いる。ここでは、所定の回路パターン等を有するマスク
から、投影光学系を介してシリコンウエハ等の感光基板
上にこのパターンを露光投影して転写する工程が行なわ
れる。
2. Description of the Related Art Conventionally, a so-called lithographic process involving transfer exposure of a predetermined pattern has been applied to a manufacturing process of a semiconductor device such as an IC or an LSI, a liquid crystal device similar thereto, a member having a fine pattern such as a thin film direct head. Has been done. Here, a step of exposing and projecting this pattern from a mask having a predetermined circuit pattern or the like onto a photosensitive substrate such as a silicon wafer via a projection optical system is performed.

【0003】また、半導体素子の集積度が上り、パター
ンの微細化が進むに従い、この種の装置の投影系の倍率
としては、縮小倍率のものが一般的になってきている。
この理由は、もし等倍であるとすると、フォトマスク上
のパターンを投影されるべきパターンと同じ寸法で作成
しなくてはならず、フォトマスク作成に困難をきたすた
めである。また、フォトマスクの欠陥やゴミ等の管理も
困難が予想される点である。
Further, as the degree of integration of semiconductor elements increases and the miniaturization of patterns progresses, a reduction magnification is generally used as the magnification of the projection system of this type of apparatus.
The reason for this is that if the same size is used, the pattern on the photomask must be formed with the same size as the pattern to be projected, which makes it difficult to form the photomask. Further, it is expected that it will be difficult to manage defects and dust on the photomask.

【0004】このようなパターンの転写露光に用いられ
る投影露光装置の投影光学系には高度な解像力が要求さ
れるが、光学系の分解能は使用する光束の波長に関連す
ることから、この種の光学系に使用する光束の短波長化
が進んでいる。今日に至るまでの短波長化の経緯を見る
と、水銀ランプの輝線スペクトルであるg線(λ=43
6nm)、i線(λ=365nm)と進んできて、Kr
−Fエキシマレーザー(λ=248nm)を用いる露光
装置が商業ベースで利用できる状況になってきている。
そして、Ar−Fエキシマレーザー(λ=193nm)
を用いる露光装置が研究されている。
The projection optical system of the projection exposure apparatus used for the transfer exposure of such a pattern is required to have a high resolution, but since the resolution of the optical system is related to the wavelength of the light flux used, this type of The wavelength of the light flux used in the optical system is becoming shorter. Looking at the history of shorter wavelengths up to today, the g-line (λ = 43
6 nm), i-line (λ = 365 nm), Kr
An exposure apparatus using a −F excimer laser (λ = 248 nm) is becoming commercially available.
And Ar-F excimer laser (λ = 193 nm)
An exposure apparatus using is used.

【0005】ところで、いわゆる半導体集積回路では、
従来のICやLSIから近年のVLSI、ULSI等へ
の移行の様に更なる高集積化が進んでおり、要求される
解像力(分解能)も更に高くなってきている。このた
め、投影光学系は縮小型のものが用いられているが、従
来より短波長の光束を用いる等の手段により、これらの
高集積化の要請に対処する必要性が生じており、例えば
2 レーザ(157μm)やX線等の利用化が研究され
ている。
By the way, in a so-called semiconductor integrated circuit,
With the recent shift from conventional ICs and LSIs to VLSIs, ULSIs, and the like, higher integration is progressing, and the required resolution (resolution) is also becoming higher. For this reason, a projection type optical system is used, but there is a need to cope with the demand for higher integration by means such as using a light flux having a shorter wavelength than in the past. Utilization of 2 lasers (157 μm) and X-rays has been studied.

【0006】しかしながら、従来の屈折レンズを用いた
投影光学系では、透過率等の問題から充分な結像特性が
得られない問題があり、従来の光学素子や補正手段のみ
では、短波長化による更なる高集積化の要請には充分に
応じられないのが実状であった。また、反射部材のみを
用いた投影光学系も実用化されているが、球面鏡等の反
射特性の問題から、微細パターン転写に有効な縮小型の
投影光学系の構築が極めて難しく、実用的な光学系が構
築できない問題があった。
However, a conventional projection optical system using a refracting lens has a problem that sufficient imaging characteristics cannot be obtained due to a problem such as transmittance, and a conventional optical element or a correction means alone causes a short wavelength. The reality is that we cannot fully meet the demand for higher integration. In addition, although a projection optical system using only a reflecting member has been put into practical use, it is extremely difficult to construct a reduction type projection optical system effective for transferring a fine pattern because of the problem of the reflection characteristics of a spherical mirror, etc. There was a problem that the system could not be constructed.

【0007】このように、縮小倍率を持ち、かつ短波長
化(による高解像度化)を目的とする技術開発の流れの
中で、どのような投影光学系(あるいは投影露光装置)
が今までに実現しているかを概観してみる。
As described above, in the flow of technological development for the purpose of reducing the wavelength and shortening the wavelength (increasing the resolution), what kind of projection optical system (or projection exposure apparatus)
Let's take a quick look at what has happened so far.

【0008】古くから、そして、現在に至るまで使用さ
れている光学系の形態として、最も一般的に利用されて
いるものが屈折光学系である。この屈折光学系は、St
ep−and−Repeat System(いわゆる
ステッパー方式の投影露光装置)に用いられているもの
であり、光軸上に複数の屈折部材を配置して縮小倍率を
達成すると共に結像諸収差を補正したものである。ここ
で、屈折部材とは、光軸まわりに回転対称な曲面により
構成される、いわゆるレンズである。
As a form of an optical system that has been used for a long time and up to the present, the most commonly used form is a refractive optical system. This refraction optical system is
It is used in an ep-and-Repeat System (so-called stepper type projection exposure apparatus), and a plurality of refracting members are arranged on the optical axis to achieve reduction magnification and to correct various imaging aberrations. Is. Here, the refraction member is a so-called lens configured by a curved surface that is rotationally symmetrical about the optical axis.

【0009】一方、従来の屈折部材を用いない投影光学
系としては、一番容易には反射面のみにより構成する反
射光学系が考えられるが、この種の反射光学系では、等
倍の結像倍率を実現できることが知られている。その例
は、いわゆるオフナー(Offner)の光学系として
知られているものであり、具体的構成は、特公昭57−
51083号に開示されている。しかしながら、反射面
のみで構成される縮小倍率の投影光学系は、まだ見出さ
れていないのである。
On the other hand, as a conventional projection optical system which does not use a refracting member, a reflection optical system composed of only a reflection surface can be considered most easily. It is known that magnification can be realized. An example thereof is known as a so-called Offner optical system, and its specific configuration is described in JP-B-57-
No. 51083. However, a reduction-magnification projection optical system composed of only a reflecting surface has not yet been found.

【0010】[0010]

【発明が解決しようとする課題】上記の如き従来の技術
においては、投影光学系を構成する光学系内に屈折部材
が必須であったが、短波長域では、屈折部材としてのガ
ラス材料の透過率が極めて悪くなるという難点が周知で
ある。
In the prior art as described above, a refraction member was indispensable in the optical system constituting the projection optical system, but in the short wavelength region, the glass material as the refraction member is transmitted. It is well known that the rate is extremely poor.

【0011】具体的には、Kr−Fエキシマレーザーの
波長(λ=248nm)から、Ar−Fエキシマレーザ
ーの波長(λ=193nm)の領域においては、既に一
般の光学ガラスを用いることができないため、石英ある
いは螢石ガラスといった特殊なガラス材料により、光学
系内の屈折部材を構成している。
Specifically, since a general optical glass cannot be used in the range of the wavelength of the Kr-F excimer laser (λ = 248 nm) to the wavelength of the Ar-F excimer laser (λ = 193 nm). The refracting member in the optical system is made of a special glass material such as quartz or fluorite glass.

【0012】仮に、当該波長領域での透過率の悪いガラ
ス材料等を屈折部材に用いると、透過光量が少なくなっ
て露光装置の性能が悪化し、露光作業のスループットを
悪化させるのみならず、透過しない分の光量は屈折部材
を構成するガラス材料に吸収されるので、光学系全体が
ここで発生する熱による熱変形や屈折率変化等の問題か
ら性能劣化を受けるという点が重大な問題として挙げら
れる。
If a glass material or the like having a poor transmittance in the wavelength range is used for the refraction member, the amount of transmitted light is reduced, the performance of the exposure apparatus is deteriorated, and not only the throughput of the exposure operation is deteriorated, but also the transmission work. Since the amount of light that is not absorbed is absorbed by the glass material that constitutes the refraction member, the serious problem is that the entire optical system suffers from performance deterioration due to problems such as thermal deformation and refractive index change due to heat generated here. To be

【0013】そこで、短波長化というトレンドの延長上
に、縮小投影露光装置を考えると、屈折部材を必要とす
る前述のような技術では、ArFエキシマレーザー(λ
=193nm)あたりが短波長化の限界であり、更なる
短波長化、例えばF2 レーザー(λ=157nm)等を
光源とする縮小投影露光装置は、構成し得ないことにな
ってしまう。
In view of the extension of the trend of shortening the wavelength, therefore, considering a reduction projection exposure apparatus, the ArF excimer laser (λ
= 193 nm) is the limit for shortening the wavelength, and a further reduction in wavelength, for example, a reduction projection exposure apparatus using a F 2 laser (λ = 157 nm) as a light source cannot be configured.

【0014】一方、反射光学系のみで正確なパターンの
露光転写が行える縮小型の光学系を構築することは、反
射特性のみの限界から従来の技術では不可能であり、一
部に屈折部材を利用したものが実現化されているが、屈
折部材(内の透過光路が長い)が大きく、短波長の光束
を利用することができないものとなっている。
On the other hand, it is impossible to construct a reduction type optical system capable of performing accurate exposure and transfer of a pattern only by the reflection optical system, because it is impossible with the conventional technique due to the limit of the reflection characteristic only. Although the one using it has been realized, the refracting member (in which the transmitted optical path is long) is large, and the light flux of short wavelength cannot be used.

【0015】例えば、米国SVGL社よりマイクラスキ
ャン(Micrascan)の商品名で出されている露
光装置は、Step−and−Scan System
というコンセプトのものであるが、この装置では、投影
光学系に反射屈折光学系が用いられている。この反射屈
折光学系では、複数枚の反射面と、複数個の屈折部材に
より構成されているものである。
[0015] For example, an exposure apparatus that is issued by SVGL, Inc. under the trade name of Micrascan is a Step-and-Scan System.
In this device, a catadioptric optical system is used as the projection optical system. In this catadioptric optical system, a plurality of reflecting surfaces and a plurality of refracting members are used.

【0016】本発明は、上記の問題点に鑑みてなされた
ものであり、一般的な屈折部材を用いることができない
ような短波長域においても使用することができる縮小型
の投影光学系を構築し、当該光学系を搭載する縮小型の
投影露光装置を提供することを目的とするものである。
The present invention has been made in view of the above problems, and constructs a reduction type projection optical system that can be used even in a short wavelength region where a general refracting member cannot be used. However, it is an object of the present invention to provide a reduction type projection exposure apparatus having the optical system.

【0017】[0017]

【課題を解決するための手段】上記目的を達成すべく、
本願請求項1に記載した発明では、光源手段からの光束
をマスクに照射することにより投影光学系を介して前記
マスクのパターンを感光基板上へ露光する投影露光装置
において、前記投影光学系が、曲面状の反射面を持つ複
数の反射部材と、少なくとも一つの回折光学素子とを含
むことを特徴とする投影露光装置を提供する。
In order to achieve the above object,
In the invention described in claim 1 of the present application, in the projection exposure apparatus, which exposes the pattern of the mask onto the photosensitive substrate through the projection optical system by irradiating the mask with the light flux from the light source means, the projection optical system comprises: A projection exposure apparatus including a plurality of reflecting members having curved reflecting surfaces and at least one diffractive optical element.

【0018】請求項2に記載した発明では、請求項1に
記載した投影露光装置において、前記回折光学素子が、
前記反射部材の反射面に形成されていることを特徴とす
るものである。
According to a second aspect of the invention, in the projection exposure apparatus according to the first aspect, the diffractive optical element is
It is characterized in that it is formed on the reflecting surface of the reflecting member.

【0019】請求項3に記載した発明では、請求項1又
は2に記載した投影露光装置において、前記複数の反射
部材の内の少なくとも二つが、夫々の反射面の曲率中心
位置が互いに異なる位置になるように配設されており、
投影光学系全体として縮小光学系を構成することを特徴
とするものである。
According to a third aspect of the invention, in the projection exposure apparatus according to the first or second aspect, at least two of the plurality of reflecting members are located at positions where the respective centers of curvature of the reflecting surfaces are different from each other. It is arranged so that
A feature is that a reduction optical system is configured as the entire projection optical system.

【0020】[0020]

【作用】本発明は上記のように構成されているため、反
射部材と回折光学素子により投影光学系を構成するもの
としているので、反射部材による光路の偏向作用に加え
て回折素子による光路の偏向作用を組み合わせること
で、所定のパターンの投影(転写)を行うものとなって
いる。
Since the present invention is configured as described above, the projection optical system is constituted by the reflecting member and the diffractive optical element. Therefore, in addition to the deflecting action of the optical path by the reflecting member, the deflection of the optical path by the diffractive element is performed. By combining the actions, a predetermined pattern is projected (transferred).

【0021】ここで、回折光学素子は、光の回折作用を
利用して光路の偏向を行なわせる光学素子であり、近年
この種の投影露光装置等に用いる光学素子として注目さ
れている。この回折光学素子によれば、短波長の光束の
光路をも任意に偏向させることが可能である。
Here, the diffractive optical element is an optical element that deflects the optical path by utilizing the diffracting action of light, and has recently been attracting attention as an optical element used in a projection exposure apparatus of this type. According to this diffractive optical element, it is possible to arbitrarily deflect the optical path of a light flux having a short wavelength.

【0022】更に、いわゆる屈折レンズとは異なる波長
−偏向特性を示すことから、屈折レンズとの組合せによ
る新たな収差補正手段等が注目されているが、反射特性
の補正にも応用可能であることが、本発明者らの研究で
明らかになった。
Further, since it exhibits a wavelength-deflection characteristic different from that of a so-called refraction lens, new aberration correction means or the like by combining with a refraction lens is drawing attention, but it can also be applied to correction of reflection characteristics. However, it became clear in the study of the present inventors.

【0023】回折光学素子としては、例えばフレネルゾ
ーンプレート等が良く知られているが、一般的なフレネ
ルゾーンプレートは光透過性の基板上に同心円状の遮光
部材を設けた構造のものであり、透過領域からの光束の
回折作用を利用して所定位置に光束を集光させるものが
一般的である。
As the diffractive optical element, for example, a Fresnel zone plate or the like is well known, but a general Fresnel zone plate has a structure in which a concentric light shielding member is provided on a light transmissive substrate, Generally, the light beam is condensed at a predetermined position by utilizing the diffraction effect of the light beam from the transmission region.

【0024】ゾーンプレートを含む回折光学素子の構造
は、上記のような透過部と遮光部によるもののみでは無
く、透過特性(屈折率、透過距離等)が異なる領域を段
階的に設けたものや、基板内部に屈折率分布による透過
特性の異なる部分を設けたもの等が知られている。前者
の代表的なものは、いわゆるバイナリーオプティカルエ
レメント(BOE)であり後者の代表的なものは、いわ
ゆるホログラムオプティカルエレメント(HOE)であ
る。
The structure of the diffractive optical element including the zone plate is not limited to the structure of the transmitting portion and the light shielding portion as described above, but may be one in which regions having different transmission characteristics (refractive index, transmission distance, etc.) are provided stepwise. It is known that the substrate is provided with a portion having different transmission characteristics due to the refractive index distribution. The former representative is a so-called binary optical element (BOE), and the latter representative is a so-called hologram optical element (HOE).

【0025】BOEは、リソグラフィの工程を利用して
光透過性部材に階段状の表面形状を形成し(反射部材の
表面に形成しても良い)、透過距離を部分的に異ならし
めることにより回折作用を生じさせるものであり、フレ
ネルゾーンプレートの作用効果を持つ構成のものを図2
に例示する。BOEは、その製造方法から微細な任意の
パターンを高精度でかつ自由に構築できる利点があり、
その応用分野が特に注目されている。(写真工業、19
94年、3月号94頁)
In the BOE, a stepwise surface shape is formed on the light transmissive member (may be formed on the surface of the reflective member) by using a lithography process, and the transmission distance is partially made different to diffract. Fig. 2 shows a configuration that produces the action and has the action and effect of the Fresnel zone plate.
For example. BOE has an advantage that a fine arbitrary pattern can be constructed with high accuracy and freely from its manufacturing method.
Its field of application is of particular interest. (Photo industry, 19
(March 1994, p. 94)

【0026】これらのBOE等の高度な回折光学素子に
よれば、生じさせる回折光も従来良く知られた一点への
集束作用を有するもののみならず、任意の光波面を所望
の光波面に変換すること、光発散機能を有すること、光
集束機能と光束分離機能等を複合させること等の自由な
回折作用を生じさせることが可能である。
According to these sophisticated diffractive optical elements such as BOE, the diffracted light to be generated is not only the one which has the well-known well-known focusing function, but also any light wavefront is converted into a desired light wavefront. By doing so, it is possible to generate a free diffraction action such as having a light diverging function and combining a light focusing function and a light beam separating function.

【0027】さらに、BOEは薄くて軽量であり、量産
が容易であること、製造が容易で高い回折作用が得られ
ること、光利用率が高いこと、深紫外領域の光束でも光
路の偏向が可能であること等から、投影光学系の光学部
材としての応用が研究されてきた。
Furthermore, BOE is thin and lightweight, easy to mass-produce, easy to manufacture and high in diffractive action, high in light utilization rate, and capable of deflecting an optical path even in a light beam in the deep ultraviolet region. Therefore, the application of the projection optical system as an optical member has been studied.

【0028】ところで、回折光学素子の振る舞いは、
W.C.Sweattの論文(J.Opt.Soc.A
m.vol.69,No.3,p.486(197
9))によると、厚さ無限小、屈折率無限大の屈折レン
ズと等価である。
By the way, the behavior of the diffractive optical element is as follows.
W. C. Sweatt's paper (J. Opt. Soc. A.
m. vol. 69, No. 3, p. 486 (197)
According to 9)), it is equivalent to a refractive lens having an infinitely small thickness and an infinite refractive index.

【0029】従って、縮小倍率で反射型の投影光学系に
おいて、屈折部材の担っていた役割を、回折光学素子に
負わせることにより、反射面と回折光学素子のみで縮小
倍率の投影光学系を実現することが可能となるのであ
る。
Therefore, in the projection optical system of the reduction type with the reduction magnification, the role of the refracting member is assigned to the diffractive optical element, so that the projection optical system of the reduction magnification is realized only by the reflecting surface and the diffractive optical element. It becomes possible to do it.

【0030】本発明においては、縮小型の投影光学系を
反射部材と、回折光学素子で構成するので、通常、一般
的な透過型の屈折部材が使用できないとされる短波長域
においても、縮小型の投影露光装置を実現することがで
きる。
In the present invention, since the reduction type projection optical system is composed of the reflection member and the diffractive optical element, reduction is achieved even in a short wavelength region where a general transmission type refraction member cannot be used. A mold type projection exposure apparatus can be realized.

【0031】ここで、本発明にかかる反射型の縮小投影
露光装置における構成上の制約として以下のようなこと
がある。まず第1に、回折光学素子は使用する光の波長
幅に応じた分散を有している。これは、波長により回折
角が異なってくることに起因している。このため、近軸
域で話をすれば、回折光学素子としては、パワー(又は
回折角)をゼロ(焦点距離、無限大)に近い状態にする
のが望ましい。
Here, there are the following restrictions on the structure of the reflection type reduction projection exposure apparatus according to the present invention. First of all, the diffractive optical element has a dispersion according to the wavelength width of the light used. This is because the diffraction angle varies depending on the wavelength. Therefore, speaking in the paraxial region, it is desirable for the diffractive optical element to have a power (or diffraction angle) close to zero (focal length, infinity).

【0032】しかし、このことは回折光学素子が平行平
板と等価であることを意味するわけではない。回折光学
素子は、近軸域ではパワーをゼロに形成しても、他の部
分において光路を簡易かつ任意に偏向できるので、容易
に任意非球面と同等の効果を持たせた回折光学素子が構
築できるのである。
However, this does not mean that the diffractive optical element is equivalent to a parallel plate. Since the diffractive optical element can easily and arbitrarily deflect the optical path in other parts even if the power is formed to be zero in the paraxial region, it is easy to construct a diffractive optical element that has the same effect as an arbitrary aspherical surface. You can do it.

【0033】第2に、このような回折光学素子の有して
いる分散特性を考慮すると、使用する光束の波長域が小
さいことが好ましく、このような光束を生じさせる光源
としては波長幅の小さいものが適していることが理解さ
れる。従って、光源としてはレーザーが望ましい。
Secondly, considering the dispersion characteristics of such a diffractive optical element, it is preferable that the wavelength range of the light beam used is small, and a light source for producing such a light beam has a small wavelength width. It will be appreciated that one is suitable. Therefore, a laser is desirable as the light source.

【0034】第3に、先に述べた様に、回折光学素子
は、屈折率無限大と等価となるのであるから、ペッツバ
ール(Petzval)和への寄与はゼロである。故
に、光学系全体としては、回折光学素子を除いた光学部
材、好ましくは反射部材だけでペッツバール和の補正が
なされていなければならない。そのため、複数の反射部
材の各々の曲面状の反射面としては、凸面と凹面の両方
を用いなければならないこととなる。
Thirdly, as described above, since the diffractive optical element is equivalent to infinite refractive index, its contribution to the Petzval sum is zero. Therefore, the Petzval sum must be corrected only by the optical member excluding the diffractive optical element, preferably by the reflecting member, as the entire optical system. Therefore, both the convex surface and the concave surface must be used as the curved reflecting surface of each of the plurality of reflecting members.

【0035】即ち、これらを勘案すると、発振波長帯域
の狭い光源(短波長のレーザ等)を用い、複数の反射部
材が凸面と凹面の反射面を持つものを組み合わせてペッ
ツバール和が補正されるものであれば良く、これにより
希望する倍率に設計された光学系を構築すると共に、投
影像に歪み等を生じさせる収差や反射偏向光等を回折光
学素子で部分的な光路の偏向等を行い、正確な投影像が
得られるように光路の偏向を行うように設計すること
で、反射型の縮小投影光学系並びにこれを利用した投影
露光装置が構築できる。
That is, taking these into consideration, a Petzval sum is corrected by using a light source having a narrow oscillation wavelength band (a laser having a short wavelength or the like) and combining a plurality of reflecting members having convex and concave reflecting surfaces. As long as this is done, an optical system designed to have a desired magnification is constructed, and at the same time, the diffractive optical element partially deflects aberrations and reflected deflected light that cause distortion in the projected image, By designing to deflect the optical path so that an accurate projected image can be obtained, a reflection type reduction projection optical system and a projection exposure apparatus using the same can be constructed.

【0036】ここで、回折光学素子は例えばBOEのよ
うに薄い光透過性基板上に構築された回折パターンから
なるものであれば、投影光学系の光路中に透過部材とし
て配しても、ここでの透過光量の減少はほとんど問題と
ならない程度である。また、反射型の基板上に回折パタ
ーンを構築することで反射型の回折光学素子を構築する
ことも可能である。このため、投影光学系の光路上に反
射型の回折光学素子を設けることで、光学部材の透過に
伴う光量減少も問題は生じない投影光学系が構築でき
る。
If the diffractive optical element has a diffraction pattern constructed on a thin light transmissive substrate such as BOE, it may be arranged as a transmissive member in the optical path of the projection optical system. The decrease in the amount of transmitted light at 10 is not a problem. It is also possible to construct a reflective diffractive optical element by constructing a diffraction pattern on a reflective substrate. Therefore, by providing the reflection type diffractive optical element on the optical path of the projection optical system, it is possible to construct a projection optical system in which there is no problem in reducing the amount of light due to the transmission of the optical member.

【0037】次に、請求項2に記載した発明では、反射
部材の曲面状の反射面に回折光学素子を形成している
が、言い換えると回折光学素子と反射部材とを一体に構
成したものであり、投影光学系を構成する部材点数が減
少する利点がある。
In the second aspect of the invention, the diffractive optical element is formed on the curved reflecting surface of the reflecting member. In other words, the diffractive optical element and the reflecting member are integrally formed. There is an advantage that the number of members constituting the projection optical system is reduced.

【0038】このような一体型の反射回折光学素子は、
反射鏡の表面に回折パターンを形成することで構築でき
る。例えば、反射面上にBOE等の製造工程を応用し
て、光透過性部材の積層パターンを形成する等の方法で
容易に製造できる。
Such an integrated reflection diffractive optical element is
It can be constructed by forming a diffraction pattern on the surface of the reflecting mirror. For example, it can be easily manufactured by a method such as applying a manufacturing process such as BOE on the reflecting surface to form a laminated pattern of light transmitting members.

【0039】また、請求項3に記載した発明では、前記
複数の反射部材の内の少なくとも二つが、夫々の反射面
の曲率中心位置が互いに異なる位置になるように配設さ
れているので、これらの反射部材の反射作用により投影
像が変倍される。即ち、本発明における投影光学系の変
倍作用は、反射部材の曲面反射作用や、回折光学素子の
回折偏向作用により変倍するものでも良いが、少なくと
も反射部材の曲率中心が同一であればそれらの間での変
倍作用は生じずに等倍となる。
Further, in the invention described in claim 3, since at least two of the plurality of reflecting members are arranged such that the respective centers of curvature of the reflecting surfaces are different from each other, these are provided. The projected image is magnified by the reflecting action of the reflecting member. That is, the zooming action of the projection optical system in the present invention may be performed by the curved reflecting action of the reflecting member or the diffractive deflection action of the diffractive optical element, but at least if the centers of curvature of the reflecting members are the same. There is no scaling effect between the two, and the magnification becomes equal.

【0040】本発明のように、反射部材の曲率中心を異
ならしめることにより、これらの間での反射偏向作用で
投影像は変倍される。ただし、このような曲面の反射の
みでは投影像に歪みが生ずるので、回折光学素子により
投影像の歪みを打ち消すように光路を修正する偏向作用
を持たせている。
As in the present invention, by making the centers of curvature of the reflecting members different, the projected image is magnified by the reflection and deflection action between them. However, since the projection image is distorted only by the reflection of such a curved surface, the diffractive optical element is provided with a deflecting action for correcting the optical path so as to cancel the distortion of the projection image.

【0041】[0041]

【実施例】以下、実施例を通じ本発明をさらに詳しく説
明する。図1は、本発明の一実施例に係る投影光学装置
の主要部を示すものであり、フォトマスク1は、図示し
ない照明光学系より射出される露光光により透過照明さ
れ、フォトレジストが塗布されたウエハからなる感光性
基板2の上に、フォトマスク1の所定のパターンの像を
形成するものである。ここでは、光源手段としてAr−
Fレーザー(λ=193nm)を使用している。
The present invention will be described in more detail with reference to the following examples. FIG. 1 shows a main part of a projection optical apparatus according to an embodiment of the present invention. A photomask 1 is transmissively illuminated by exposure light emitted from an illumination optical system (not shown) and coated with a photoresist. The image of the predetermined pattern of the photomask 1 is formed on the photosensitive substrate 2 made of a wafer. Here, as the light source means Ar-
An F laser (λ = 193 nm) is used.

【0042】フォトマスク1を透過した光束は、凹曲面
の反射面を持つ反射鏡11により反射され、凸曲面の反
射面を持つ反射鏡12に導かれ、更にここで反射され
て、凹曲面の反射面を持つ反射鏡13に導かれる。反射
鏡13で反射された光束は、透過型の回折光学素子21
に入射し、ここで光路が一部偏向されて凹曲面の反射面
とその表面に回折パターン22が形成された回折反射鏡
14に導かれ、ここで反射回折されて感光性基板2上に
マスク1のパターンの像が縮小変倍されて投影される。
なお、これらの反射面の曲率中心位置はすべてが一致す
るということがないように配置されている。
The light flux that has passed through the photomask 1 is reflected by a reflecting mirror 11 having a concave curved reflecting surface, guided to a reflecting mirror 12 having a convex curved reflecting surface, and further reflected here to have a concave curved surface. It is guided to the reflecting mirror 13 having a reflecting surface. The light beam reflected by the reflecting mirror 13 is transmitted through the diffractive optical element 21.
The light path is partially deflected and guided to a diffractive reflecting mirror 14 having a concave curved reflecting surface and a diffractive pattern 22 formed on the reflecting surface, where it is reflected and diffracted to form a mask on the photosensitive substrate 2. The image of the pattern No. 1 is reduced and scaled and projected.
The positions of the centers of curvature of these reflecting surfaces are arranged so that they do not all coincide.

【0043】ここで、回折光学素子21は、例えば石英
ガラス基板上に形成された透過部材からなる回折パター
ンを有する回折光学素子である。なお、石英ガラス基板
自体をエッチング処理して回折パターンを形成したもの
であっても良い。
Here, the diffractive optical element 21 is a diffractive optical element having a diffraction pattern made of, for example, a transmissive member formed on a quartz glass substrate. The quartz glass substrate itself may be etched to form a diffraction pattern.

【0044】また、この回折光学素子21は、透過型の
ものを使用しているが、いわゆるBOE等の製造方法に
よれば基板自体は非常に薄いもので構築できるので、屈
折レンズを用いる場合と異なって、透過率(透過光量の
減少)、及び熱(光の吸収)もほとんど問題とならな
い。なお、回折光学素子21を平面反射部材上に設けた
回折パターンを有するものとしここで光路を折り曲げて
光学系を構成することも可能であり、この場合には透過
素子を用いずに投影光学系が構築できる。
Although the diffractive optical element 21 is of a transmissive type, the substrate itself can be constructed with a very thin one according to a manufacturing method such as so-called BOE. Differently, the transmittance (decrease in the amount of transmitted light) and the heat (absorption of light) are hardly problems. It is also possible that the diffractive optical element 21 has a diffraction pattern provided on a flat reflecting member, and the optical path is bent here to form an optical system. In this case, the projection optical system is used without using a transmissive element. Can be built.

【0045】一方、回折反射鏡14も同様に反射鏡の表
面に透過部材又は反射部材の積層構造を有する回折パタ
ーンが形成された一種の回折光学素子である。前述した
ようにBOE等の回折光学素子は、回折パターンを平面
上のみならず曲面上にも形成できるものであり、さらに
透過部材のみならず反射面上にも形成することが可能で
ある。
On the other hand, the diffractive reflecting mirror 14 is also a kind of diffractive optical element in which a diffractive pattern having a laminated structure of a transmissive member or a reflective member is formed on the surface of the reflective mirror. As described above, the diffractive optical element such as BOE can form the diffraction pattern not only on the flat surface but also on the curved surface, and can be formed not only on the transmitting member but also on the reflecting surface.

【0046】次に、本実施例の投影光学系の基本的倍率
は、大旨、反射面(反射鏡11、12、13、回折反射
鏡14)だけで決められている。即ち、3個の凹曲面と
1個の凸曲面の反射(偏向)作用により、反射面のみで
構成される縮小倍率の投影光学系が構築されている。
Next, the basic magnification of the projection optical system of this embodiment is basically determined only by the reflecting surface (reflecting mirrors 11, 12, 13 and the diffractive reflecting mirror 14). That is, a projection optical system with a reduced magnification composed of only reflecting surfaces is constructed by the reflection (deflection) action of three concave curved surfaces and one convex curved surface.

【0047】縮小倍率としては、現行トレンドとして
は、1/4〜1/5倍が適正であるとされている。ま
た、フォトマスク面と感光性基板の間の結像関係は、円
環状スリット領域にて行ない、フォトマスクと感光性基
板を縮小の結像倍率比で沿うほうをスキャンする構成と
するのが好ましい。さらに、回折光学素子(21、2
2)は、いわゆる屈折面における屈折作用のアナロジー
でいえば、非球面の効果を有するものであり、上記のよ
うに反射鏡で構成される変倍光学系の収差補正の機能を
有している。
As a reduction trend, it is said that 1/4 to 1/5 times is appropriate as the current trend. Further, it is preferable that the image formation relationship between the photomask surface and the photosensitive substrate is performed in the annular slit region, and the photomask and the photosensitive substrate are scanned along the reduced imaging magnification ratio. . Further, the diffractive optical element (21, 2)
2) has the effect of an aspherical surface in terms of the so-called analogy of the refracting action on the refracting surface, and has the function of correcting the aberration of the variable power optical system configured by the reflecting mirror as described above. .

【0048】即ち、投影光学系の基本倍率は回折光学素
子以外の反射面により定められているので、回折光学素
子は収差補正に寄与する構成とされている。ここで、収
差とは球面収差、コマ収差、非点収差、像面湾曲、歪曲
収差等であり、回折光学素子を複数枚用いる場合は、そ
の配置構成により補正対象となる収差が決まる。
That is, since the basic magnification of the projection optical system is determined by the reflecting surface other than the diffractive optical element, the diffractive optical element is configured to contribute to aberration correction. Here, the aberrations include spherical aberration, coma aberration, astigmatism, field curvature, distortion aberration, etc. When a plurality of diffractive optical elements are used, the aberration to be corrected is determined by the arrangement configuration.

【0049】例えば、全景の瞳面付近に配される場合
は、球面収差、コマ収差、非点収差、像面湾曲、歪曲収
差の順に収差補正の効果が大きい。また、像面(中間像
を含む)の付近に配される場合は、これとは逆に歪曲収
差、像面湾曲、非点収差、コマ収差、球面収差の順に収
差補正の効果が大きい。
For example, when it is arranged near the pupil plane of the whole view, the effect of aberration correction is large in the order of spherical aberration, coma, astigmatism, field curvature, and distortion. In the case of being arranged near the image plane (including the intermediate image), on the contrary, the effect of aberration correction is large in the order of distortion, field curvature, astigmatism, coma and spherical aberration.

【0050】図1に示す実施例においては、回折光学素
子21の付近に中間像が形成されるので回折光学素子2
1により主に歪曲収差、像面湾曲、非点収差の収差補正
を行ない、瞳面付近に位置する回折光学素子22が球面
収差、コマ収差、非点収差の補正を主に行なう構成とし
ている。
In the embodiment shown in FIG. 1, since an intermediate image is formed near the diffractive optical element 21, the diffractive optical element 2
1, the distortion correction, the field curvature, and the astigmatism are mainly corrected, and the diffractive optical element 22 located near the pupil surface mainly corrects the spherical aberration, the coma, and the astigmatism.

【0051】従って、本実施例では上記のように反射型
の縮小投影光学系を用いた露光装置が構築でき、その投
影像は歪みのない微細なパターンが再現されている。ま
た、基本設計を更なる短波長(F2 レーザー(λ=15
7nm)等)に合わせて、露光装置を構築することも可
能であり、従来より高精度な微細パターンの転写露光が
行えるものとなる。
Therefore, in this embodiment, an exposure apparatus using the reflection type reduction projection optical system can be constructed as described above, and the projected image reproduces a fine pattern without distortion. In addition, the basic design is based on an even shorter wavelength (F 2 laser (λ = 15
It is also possible to construct an exposure apparatus in accordance with (7 nm) and the like), and transfer exposure of a fine pattern with higher accuracy than ever can be performed.

【0052】なお、本実施例では、回折光学素子を2つ
として、図1に示したような位置に配置したが、これは
本実施例における反射鏡の配置構成から生ずる収差補正
の都合により決定されたものであり、これに限定される
ものでは無い。同じ反射鏡の配置構成においても、異な
る位置に異なる構成の回折光学素子を異なる個数設けて
も良い。
In this embodiment, two diffractive optical elements are arranged at the positions shown in FIG. 1. However, this is determined by the aberration correction caused by the arrangement of the reflecting mirrors in this embodiment. However, the present invention is not limited to this. Even with the same arrangement of reflecting mirrors, different numbers of diffractive optical elements having different configurations may be provided at different positions.

【0053】また、各反射面の配置も図1に示す構成に
限定されるものではない。必要とする倍率等に合わせて
設計された光学系の構成に合わせて、任意の個数にて、
任意の位置に配置することが可能である。いずれの場合
にも、本発明の要旨を逸脱していない範囲で、反射鏡並
びに回折光学素子を組み合わせて、適正な倍率で正確な
投影像が得られるように種々の構成を設計すれば良い。
The arrangement of the reflecting surfaces is not limited to the arrangement shown in FIG. Depending on the configuration of the optical system designed according to the required magnification, etc., in any number,
It can be arranged at any position. In any case, various configurations may be designed by combining a reflecting mirror and a diffractive optical element within a range not departing from the gist of the present invention so that an accurate projected image can be obtained at an appropriate magnification.

【0054】[0054]

【発明の効果】以上説明したとおり、本発明によれば、
回折光学素子を利用することで反射型の縮小投影光学系
が容易に構築できるので、投影光学装置としての応用範
囲が広がる利点がある。
As described above, according to the present invention,
Since the reflection type reduction projection optical system can be easily constructed by using the diffractive optical element, there is an advantage that the range of application as the projection optical device is widened.

【0055】特に、従来不可能であった透過屈折部材を
用いずに、主に反射部材のみで変倍(縮小型)投影光学
系が実現できるので、短波長域における転写露光が可能
となる。即ち、一般に屈折部材を用いることができない
とされている短波長領域においても使用可能な縮小投影
光学系を実現することができることとなる。言うまでも
無く、使用光束の短波長化は、投影光学系の解像力の向
上を意味するものであるので、短波長域の光束を利用し
た更なる微細パターンの高精度の転写露光が可能とな
る。
In particular, a variable-magnification (reduction type) projection optical system can be realized mainly by a reflecting member without using a transmissive-refractive member, which has heretofore been impossible. Therefore, transfer exposure in a short wavelength region becomes possible. That is, it is possible to realize a reduction projection optical system that can be used even in a short wavelength region where it is generally considered that a refraction member cannot be used. Needless to say, shortening the wavelength of the used light flux means improving the resolution of the projection optical system, so that it is possible to perform highly precise transfer exposure of a fine pattern using a light flux in the short wavelength range. .

【0056】さらに、本発明は、いわゆるフォトリソグ
ラフィにて用いられる縮小投影光学系を搭載する投影露
光装置のみならず、いわゆるX線リソグラフィにおける
露光装置としても適用できる。即ち、X線も電磁波の一
種であり、反射部材における反射はスネルの法則(入射
角=反射角)に従い、回折光学素子における回折現象も
光と同様に認められるためである。従って、本発明を応
用することにより、X線を利用した等倍もしくは変倍の
投影光学系も構築できる。
Furthermore, the present invention can be applied not only as a projection exposure apparatus equipped with a reduction projection optical system used in so-called photolithography but also as an exposure apparatus in so-called X-ray lithography. That is, X-rays are also a type of electromagnetic wave, and the reflection on the reflecting member follows Snell's law (incident angle = reflection angle), and the diffraction phenomenon in the diffractive optical element is recognized as in light. Therefore, by applying the present invention, it is also possible to construct a projection optical system of equal magnification or variable magnification using X-rays.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の一実施例に係る投影露光装置の主要構
成を示す概略説明図である。
FIG. 1 is a schematic explanatory diagram showing a main configuration of a projection exposure apparatus according to an embodiment of the present invention.

【図2】バイナリーオプティカルエレメント(回折光学
素子)の一例の概略構成を示す説明図である。
FIG. 2 is an explanatory diagram showing a schematic configuration of an example of a binary optical element (diffractive optical element).

【符号の説明】[Explanation of symbols]

1:フォトマスク 2:感光性基板 11、13:凹反射鏡 12:凸反射鏡 14:回折反射鏡 21:透過型の回折光学素子 22:反射型の回折光学素子(反射鏡の上に設けられた
回折パターン)
DESCRIPTION OF SYMBOLS 1: Photomask 2: Photosensitive substrate 11, 13: Concave reflecting mirror 12: Convex reflecting mirror 14: Diffractive reflecting mirror 21: Transmissive diffractive optical element 22: Reflective diffractive optical element (provided on the reflective mirror Diffraction pattern)

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 光源手段からの光束をマスクに照射する
ことにより、投影光学系を介して前記マスクのパターン
を感光基板上へ露光する投影露光装置において、 前記投影光学系は、曲面上の反射面を持つ複数の反射部
材と、少なくとも一つの回折光学素子とを含むことを特
徴とする投影露光装置。
1. A projection exposure apparatus that exposes the pattern of the mask onto a photosensitive substrate through a projection optical system by irradiating the mask with a light beam from a light source means, wherein the projection optical system is a reflection on a curved surface. A projection exposure apparatus comprising a plurality of reflecting members each having a surface and at least one diffractive optical element.
【請求項2】 前記回折光学素子が、前記反射部材の反
射面に形成されていることを特徴とする請求項1に記載
した投影露光装置。
2. The projection exposure apparatus according to claim 1, wherein the diffractive optical element is formed on a reflecting surface of the reflecting member.
【請求項3】 前記複数の反射部材の内の少なくとも二
つは、夫々の反射面の曲率中心位置が互いに異なる位置
になるように配設されており、投影光学系全体として縮
小光学系を構成することを特徴とする請求項1又は2に
記載した投影露光装置。
3. At least two of the plurality of reflecting members are arranged such that the respective centers of curvature of their reflecting surfaces are different from each other, and constitute a reduction optical system as a whole of the projection optical system. The projection exposure apparatus according to claim 1 or 2, wherein
JP6170378A 1994-06-30 1994-06-30 Projection exposure device Pending JPH0817720A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6170378A JPH0817720A (en) 1994-06-30 1994-06-30 Projection exposure device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6170378A JPH0817720A (en) 1994-06-30 1994-06-30 Projection exposure device

Publications (1)

Publication Number Publication Date
JPH0817720A true JPH0817720A (en) 1996-01-19

Family

ID=15903832

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6170378A Pending JPH0817720A (en) 1994-06-30 1994-06-30 Projection exposure device

Country Status (1)

Country Link
JP (1) JPH0817720A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999045580A1 (en) * 1998-03-06 1999-09-10 Nikon Corporation Exposure device and method of manufacturing semiconductor device
WO1999052004A1 (en) * 1998-04-07 1999-10-14 Nikon Corporation Projection exposure apparatus and method, and reflection refraction optical system
US6829099B2 (en) 2000-03-31 2004-12-07 Canon Kabushiki Kaisha Projection optical system and projection exposure apparatus
JP2012182492A (en) * 2008-05-20 2012-09-20 Gigaphoton Inc Mirror for extreme ultra violet, manufacturing method for mirror for extreme ultra violet, and extreme ultraviolet light source device

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1999045580A1 (en) * 1998-03-06 1999-09-10 Nikon Corporation Exposure device and method of manufacturing semiconductor device
US6583856B1 (en) 1998-03-06 2003-06-24 Nikon Corporation Exposure apparatus and fabrication method of semiconductor device using the same
JP4333035B2 (en) * 1998-03-06 2009-09-16 株式会社ニコン EXPOSURE APPARATUS AND METHOD FOR MANUFACTURING SEMICONDUCTOR DEVICE USING THE APPARATUS
WO1999052004A1 (en) * 1998-04-07 1999-10-14 Nikon Corporation Projection exposure apparatus and method, and reflection refraction optical system
US6707616B1 (en) 1998-04-07 2004-03-16 Nikon Corporation Projection exposure apparatus, projection exposure method and catadioptric optical system
US6829099B2 (en) 2000-03-31 2004-12-07 Canon Kabushiki Kaisha Projection optical system and projection exposure apparatus
JP2012182492A (en) * 2008-05-20 2012-09-20 Gigaphoton Inc Mirror for extreme ultra violet, manufacturing method for mirror for extreme ultra violet, and extreme ultraviolet light source device
JP2012212904A (en) * 2008-05-20 2012-11-01 Gigaphoton Inc Extreme-ultraviolet light mirror, manufacturing method of the same and extreme-ultraviolet light source device

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