WO2005006414A1 - 集光光学系、光源ユニット、照明光学装置および露光装置 - Google Patents
集光光学系、光源ユニット、照明光学装置および露光装置 Download PDFInfo
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- WO2005006414A1 WO2005006414A1 PCT/JP2004/010053 JP2004010053W WO2005006414A1 WO 2005006414 A1 WO2005006414 A1 WO 2005006414A1 JP 2004010053 W JP2004010053 W JP 2004010053W WO 2005006414 A1 WO2005006414 A1 WO 2005006414A1
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- Prior art keywords
- light source
- mirror
- plasma
- light
- source unit
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Classifications
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70058—Mask illumination systems
- G03F7/7015—Details of optical elements
- G03F7/70175—Lamphouse reflector arrangements or collector mirrors, i.e. collecting light from solid angle upstream of the light source
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0033—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
- G02B19/0047—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70008—Production of exposure light, i.e. light sources
- G03F7/70033—Production of exposure light, i.e. light sources by plasma extreme ultraviolet [EUV] sources
Definitions
- the present invention relates to a condensing optical system, an illumination optical device, and an exposure device. More specifically, the present invention relates to an exposure apparatus suitable for manufacturing a microdevice such as a semiconductor device by photolithography using EUV light (extreme ultraviolet light) having a wavelength of about 550 nm. It relates to an optical optical system.
- EUV light extreme ultraviolet light
- An exposure apparatus for manufacturing a semiconductor device projects and transfers a circuit pattern formed on a mask onto a photosensitive substrate such as a wafer coated with a resist via a projection optical system.
- LPP Laser Produced Plasma
- a DPP discharge Produced Plasma
- a DPP discharge Produced Plasma light source that applies a voltage between the electrodes while the target material is present on or between the electrodes and converts the target material into plasma to obtain EUV light.
- the DPP light source and the LPP light source are collectively referred to as "plasma light source”.
- EUV light is isotropically emitted from a plasma light source. That is, the plasma light source can be regarded as a point light source.
- the size (diameter) of the plasma light source is on the order of 50 to 500 ⁇
- FIG. 1 shows an example of a conventional condensing optical system.
- the converging mirror 2 has a spheroidal reflecting surface. When the plasma light source 1 is arranged at a first focal point (hereinafter, referred to as a first focal point) of the elliptical surface, the converging mirror 2 reflects the light.
- the EUV light thus collected is converged on a second focal point (hereinafter, referred to as a second focal point) of the ellipsoid to form a light source image 3.
- a second focal point On a plane passing through the second focal point of the converging mirror 2 and perpendicular to the optical axis (hereinafter referred to as a second focal plane), an aperture for blocking light beams directly incident from the EUV light source 1 without being condensed. 7 is arranged.
- An illumination optical system is arranged downstream of the stop 7.
- a part of the EUV light diverging isotropically from the plasma light source 1 is condensed by a converging mirror 2 having a spheroidal reflecting surface, like the conventional converging mirror shown in FIG. To form a light source image 3 on the second focal plane.
- a converging mirror 2 having a spheroidal reflecting surface, like the conventional converging mirror shown in FIG.
- another part of the EUV light is reflected by an auxiliary focusing mirror 4 having a spherical reflecting surface centered on the position of the plasma light source 1 and is once collected at the same position as the plasma light source 1. After that, the light is reflected by the converging mirror 2 and formed at the same position as the light source image 3.
- a real image by the condensing mirror 2 of the plasma light source 1 and a real image by an optical system combining the auxiliary condensing mirror 4 and the condensing mirror 2 are formed in a superimposed manner.
- the luminous flux diverging from the plasma light source 1 can be guided to the light source image 3 in a larger solid angle range, so that the amount of light guided to the illumination optical system increases.
- Condensing optics based on this concept have already been put to practical use in projector condensing optics, etc.
- Plasma used as an EUV light source generally strongly absorbs EUV light.
- Plasma intensity EUV light of a specific wavelength is generated by the transition of electrons between energy levels unique to atoms. It generates light when transitioning to a lower energy level and absorbs light of the same wavelength when transitioning to a higher energy level. Therefore, light generated from the plasma is essentially greatly absorbed by the plasma.
- EUV light reflected by the auxiliary focusing mirror 4 and returned to the position of the EUV light source 1 is absorbed by the plasma. Because it cannot be reached. Therefore, the total amount of collected EUV light does not increase.
- the present invention has been made in view of the above problems, and has been achieved by reflecting light from an auxiliary condensing mirror.
- Condensing optics are configured so that EUV light is not absorbed by plasma, the total amount of EUV light to be collected is increased, and this condensing optical system is applied to EUV lithography equipment to greatly improve throughput.
- the purpose is to aim.
- the present invention uses the following means.
- the condensing optical system of the present invention is a light source unit for EUV light
- a plasma light source that emits EUV light that emits EUV light
- a condensing mirror having a spheroidal reflecting surface and the plasma light source placed at a first focal point (elliptical focal point); and a spherical reflecting surface having a spherical center corresponding to the position of the plasma light source. And an auxiliary focusing mirror arranged so as to be shifted.
- the spherical center of the auxiliary focusing mirror is displaced from the position of the plasma light source, the image of the plasma light source formed by the auxiliary focusing mirror is not included in the plasma. It is not formed at the light source position. Therefore, the EUV light reflected by the auxiliary condenser mirror can be prevented from being absorbed by the plasma.
- the spherical center position of the auxiliary condensing mirror passes through the first focal point of the condensing mirror and is perpendicular to the optical axis (coinciding with the axis of the ellipse).
- First focus of elliptical mirror It is also preferable that the distance from the optical axis is greater than or equal to the radius of the plasma light source.
- the spherical center of the auxiliary condensing mirror is shifted by the radius of the plasma light source or more, the image position of the plasma light source formed by the auxiliary condensing mirror is Are not formed at the position of the plasma light source with a deviation of more than the radius. Therefore, it is possible to more reliably prevent EUV light reflected by the auxiliary condensing mirror from being absorbed by the plasma.
- the auxiliary converging mirror is constituted by a plurality of mirrors having different spherical center positions.
- the auxiliary condensing mirror is constituted by a plurality of mirrors having different spherical centers, the number of light source images formed on an incident surface of an optical integrator described later is reduced. , The uniformity of the illuminance on the mask surface after passing through the illumination optical system is improved.
- a condensing mirror comprising a condensing mirror having a spheroidal reflecting surface and an auxiliary condensing mirror having a spherical surface having a spherical center at a first focal point of the condensing mirror.
- R the radius of the auxiliary focusing mirror
- the duration of the pulse light of the plasma light source is t
- the speed of light is c
- R> (tXc) / 2 must be satisfied. Is also preferred.
- the condensing optical system when the plasma light source is placed at the position of the first focal point, the reciprocating distance from the plasma light source to the auxiliary condensing mirror becomes longer than the pulse light of the plasma light source.
- the EUV light reflected by the auxiliary converging mirror 2 returns to the position of the plasma light source, the plasma becomes longer than the distance (t X c), which is the product of the energy of the duration (t) and the speed of light (c). Will disappear and EUV light will not be absorbed by the plasma.
- the light source unit includes the plasma light source that emits EUV light at the first focal point of the light-collecting optical system.
- the reciprocating distance from the light source to the auxiliary converging mirror is determined by the distance (tXc) which is the product of the duration (t) of the pulse light of the plasma light source and the speed of light (c).
- the distance (tXc) which is the product of the duration (t) of the pulse light of the plasma light source and the speed of light (c).
- the converging mirror is divided into a partial mirror near the plasma light source and a partial mirror far from the plasma light source, and only the partial mirror near the plasma light source is detachably replaceable. It is also preferred.
- the reflection surface is affected by the radiant heat from the plasma light source
- an illumination optical device of the present invention includes the above light source unit and an illumination optical system for guiding EUV light from the light source unit to a mask.
- the EUV light from the light source unit can be supplied without substantial loss of light amount, and a mask on which a predetermined pattern is formed under favorable illumination conditions using an optical integrator. Can be illuminated.
- the exposure apparatus of the present invention provides an illumination optical device for illuminating a reflective mask on which a predetermined pattern is formed, and a mask arranged on a surface to be illuminated by the illumination optical device.
- the exposure apparatus includes a driving device that relatively moves the mask stage and the wafer stage relative to the projection optical system at a speed corresponding to the reduction ratio. And the above-mentioned illumination optical device.
- the EUV light reflected by the auxiliary condenser mirror is not absorbed by the plasma by slightly shifting the spherical center position of the auxiliary condenser mirror from the plasma light source position.
- much more EUV light can be efficiently collected than before.
- by applying the light source unit whose light-collecting efficiency has been greatly increased to the exposure apparatus it is possible to significantly improve the throughput.
- the reciprocating distance from the plasma light source to the auxiliary condensing mirror is made longer than the distance which is the product of the duration of the laser light of the plasma light source and the speed of light, thereby increasing the plasma.
- the EUV light emitted from the light source is reflected by the auxiliary focusing mirror and returns, the plasma is extinguished, and the EUV light reflected by the auxiliary focusing mirror is not absorbed by the plasma.
- much more EUV light can be efficiently collected than before.
- by applying a light source unit having such a large increase in light collection efficiency to an exposure apparatus it is possible to significantly improve throughput.
- Garden 1 is a view showing a conventional light-collecting optical system.
- Garden 2 is a diagram showing a condensing optical system using a conventional auxiliary condensing mirror.
- Garden 3 is a view showing a condensing optical system according to an embodiment of the present invention.
- [Garden 4] is a view showing an example of an auxiliary focusing mirror.
- Garden 5 is a view showing an example of an auxiliary condenser mirror.
- FIG. 6 is a view showing a modification of the light collecting mirror according to the present invention.
- Garden 7 is a view showing a condensing optical system using an auxiliary condensing mirror according to the present invention.
- Garden 8 is a diagram showing an example of an EUV exposure apparatus using the condensing optical system according to the present invention.
- Garden 9 is a view showing an example of an EUV exposure apparatus using the condensing optical system according to the present invention.
- FIG. 3 shows a light source unit according to an embodiment of the present invention.
- the plasma light source 1 has a first focal point (an elliptical shape) of a condenser mirror 2 having a spheroidal reflecting surface.
- the auxiliary focusing mirrors 4a and 4b are arranged so that their spherical centers Ca and Cb are shifted from the position of the plasma light source 1 by ⁇ 0.25 mm in the direction perpendicular to the optical axis OA.
- a part of the EUV light emitted from the plasma light source 1 is reflected by the condenser mirror 2 to form a light source image 3 on an elliptical second focal plane.
- the other part of the EUV light emitted from the light source 1 is reflected by the auxiliary condensing mirrors 4a and 4b, and is separated from the plasma light source 1 by ⁇ 0.50 mm in a direction perpendicular to the optical axis OA.
- Light source images 5a and 5b are formed at shifted positions. Since the size (diameter) of the plasma light source 1 is about 500 ⁇ , the light source images 5a and 5b can be prevented from being absorbed by the plasma without overlapping with the plasma position.
- the light source images 5a and 5b are reflected by the converging mirror 2 to form light source images 6a and 6b on an elliptical second focal plane.
- a stop 7 for removing stray light is provided on the second focal plane of the ellipse, and the light source images 3, 6a, 6b are formed side by side on the openings provided in the stop 7.
- An illumination optical system (described later) is provided downstream of the stop 7, and the luminous flux diverging from the light source images 3, 6a, 6b is introduced there.
- the diaphragm 7 can also serve as a vacuum partition for performing differential exhaust between the light source unit and the portion where the illumination optical system and the like are arranged.
- an optical integrator for dividing a light beam diverging from a light source to form a plurality of light source images is used.
- an optical integrator By using an optical integrator, the intensity distribution of the illumination light irradiated on the mask can be made uniform.
- the light-collecting optical system of the light source unit since a plurality of light source images 3, 6a, and 6b are formed by the light-collecting optical system, these can be used as a part of the function of the optical integrator. I can do it.
- FIG. 3 shows a view from the side, but when viewed from the direction of the optical axis OA, the auxiliary focusing mirrors 4a-4d are actually divided into four parts as shown in FIG. 4 (a). Therefore, five light source images 3, 6a-6d are formed on the focal plane as shown in Fig. 4 (b). Since the number of light source images formed on the entrance surface of the optical integrator increases, the illuminance uniformity on the exit surface of the optical integrator improves.
- the auxiliary focusing mirrors 4a and 4h may be divided into eight parts. This
- FIG. 6 is a side view of a modification of the condenser mirror 2 shown in FIG. As shown in Figure 6, It can also be divided into two parts, a partial mirror 2a near and at the position of plasma and a partial mirror 2b at a position far from and away from the plasma.
- the reflective surface is likely to be severely damaged due to the effects of radiant heat from the plasma light source 1 and EUV light irradiation heat, and it is necessary to remove and replace only the partial mirror 2a. It is desirable that the configuration be replaceable.
- FIG. 7 shows a light source unit according to an embodiment of the present invention.
- the plasma light source 1 in the plasma light source 1, light (non-EUV light) emitted from the laser light source LS is condensed through the through hole of the lens 12 and the converging mirror 2.
- the plasma light source 1 is disposed at a first focal point of a condenser mirror 2 having a spheroidal reflecting surface.
- An auxiliary focusing mirror 4 having a spherical reflecting surface centered on this position is arranged.
- a part of the EUV light emitted from the plasma light source 1 is reflected by the focusing mirror 2 to form a light source image 3 on an elliptical second focal plane.
- Another part of the EUV light emitted from the plasma light source 1 is reflected by the auxiliary focusing mirror 4 to form a light source image 3 at the same position as the plasma light source 1.
- the distance from the plasma light source 1 to the auxiliary converging mirror 2 was 4 Ocm.
- a laser plasma light source (LPP) was used as the plasma light source, and the duration of the plasma light source was 2 ns.
- the EUV light emitted from the plasma light source 1 travels a distance of 80 cm before being reflected by the auxiliary focusing mirror 2 and returning to the position of the plasma light source 1, so that a time of 2.7 ns is required.
- the duration of the pulse light of the plasma light source is 2 ns, even if the light is generated at the beginning of the pulse, the plasma is already extinguished when it is reflected by the auxiliary focusing mirror 2 and returns to the position of the plasma light source 1. are doing. Therefore, EUV light cannot be absorbed by plasma.
- the luminous flux traveling from this light source image is reflected by the condensing mirror 12 and falls on the second focal plane of the ellipse.
- a light source image 3 is formed. That is, at the position of the light source image 3, the real image by the condensing mirror 2 of the plasma light source 1 and the real image by the optical system combining the auxiliary converging mirror 4 and the converging mirror 2 are at the same position at different times. It is formed.
- a stop 7 for removing stray light is provided on the focal plane of the ellipse, and the light source image 3 is formed on an opening provided in the stop 7.
- An illumination optical system (not shown) is provided downstream of the stop, and a luminous flux diverging from the light source image 3 is introduced into the illumination optical system.
- the diaphragm 7 can also serve as a vacuum partition for performing differential evacuation between the light source unit and a portion where the illumination optical system and the like are arranged.
- FIG. 8 shows a light source unit according to a first embodiment of the present invention, and an illumination optical system using a rod-type optical integrator (Japanese Patent Application No. 2000-068114) by the present applicant. 1 shows an embodiment of an EUV exposure apparatus.
- FIG. 8 is a diagram showing a schematic configuration of a first projection exposure apparatus according to the present embodiment.
- the projection exposure apparatus is roughly divided into a light source unit LU, an illumination optical system IU, and a projection optical system PL. Power is composed. These are placed in a chamber filled with a force that is placed in the chamber in a vacuum state, at least a gas (such as helium) that absorbs little at least the used wavelength.
- a gas such as helium
- the laser light source LS is slightly tilted with respect to the optical axis OA so that direct laser light (non-EUV light) does not enter the illumination optical system IU downstream of the second focal point CP of the condenser mirror 2. It is desirable to be located.
- a gas ejected from a gas nozzle 14 with a high-pressure gas such as a xenon (Xe) force forms a gas target 13.
- the gas target 13 obtains energy from the condensed laser light, turns it into plasma, and emits EUV light.
- the gas target 13 is positioned at the first focal point of the condenser mirror 2. Therefore, EUV light emitted from the plasma light source 1 is focused on the second focal point CP of the focusing mirror 2.
- the auxiliary focusing mirror 4 is composed of two mirrors, the center of which is perpendicular to the optical axis OA rather than the position of the plasma light source 1.
- the illumination optical system IU is composed of an opticanole integrator 10 and an imaging system including a concave mirror M2 and a convex mirror M3.
- the optical integrator 10 is arranged such that the incident end face 10F is located near the second focal point CP of the condenser mirror 2, and the light reflected by the inner wall surface of the optical integrator 10 and passed therethrough is emitted. Emitted from end face 10B.
- the light emitted from the emission end face 10 B of the optical integrator 10 is reflected by the concave mirror M 2, reflected by the convex mirror M 3, further reflected by the concave mirror M 2, and reflected by the reflection type mask R. Lighting.
- the device pattern surface of the mask R and the emission end surface 10B of the optical integrator 10 have a conjugate relationship. As described with reference to FIG. 2, the exit end face 10B is uniformly illuminated in the plane, so that the mask R plane is also uniformly illuminated.
- the projection optical system PL includes, in order from the mask R side, a concave mirror M4, a convex mirror M5, a concave mirror M6, and a concave mirror M7.
- the concave mirror M4, the concave mirror M6 and the concave mirror M7 are formed in an aspherical shape. For example, this configuration is disclosed in JP-A-9-251097.
- the light reflected by the reflective mask R forms a device pattern on the resist-coated wafer W via the projection optical system PL. Since the illumination area of the mask R is smaller than the area of the device pattern of the mask, the mask R and the wafer W are synchronously scanned to expose the entire device pattern, as shown by the arrows in FIG. After the entire device pattern is exposed, the wafer is stepped to the next exposure area. This operation is repeated, that is, a plurality of device patterns are formed on the entire wafer by the step-and-scan method.
- the light source unit according to the present embodiment has the same configuration as that of the light source unit shown in FIG. 8 of the third embodiment, and the description of the overlapping parts will be omitted.
- the EUV light collected at the second focal point CP of the collection mirror 2 is guided to a pair of fly-eye mirrors 16a and 16b via a collimator mirror 15.
- a fly-eye mirror disclosed by the present applicant in Japanese Patent Application Laid-Open No. H11-312638 can be used.
- the related description in JP-A-11-312638 can be referred to.
- a substantial surface light source having a predetermined shape is formed near the reflection surface of the second fly-eye mirror 16b, that is, near the emission surface of the optical integrator 16.
- the light from the substantial surface light source is deflected by the plane reflecting mirror 17, and then forms an elongated arc-shaped illumination area on the mask R via a field stop (not shown). Of illuminated mask
- the light from the pattern forms an image of the mask pattern on the wafer W via the projection optical system PL.
- the projection optical system PL is composed of six mirrors in order from the mask R side. For example, this configuration is disclosed in JP-A-11-312638.
- the plasma light source 1 is disposed at the first focal point (elliptical focal point) of the condenser mirror 2 having a spheroidal reflection surface as the condenser optical system, and
- the mirrors 4a and 4b have their spheres perpendicular to the optical axis OA more than the position of the plasma light source 1.
- the focusing optical system which is not limited to this is a focusing mirror having a spheroidal reflecting surface and an auxiliary focusing mirror comprising a spherical surface having a spherical center at a first focal point of the focusing mirror.
- R the radius of the auxiliary focusing mirror
- the duration of the pulse light of the plasma light source is t
- the speed of light is c
- R> (t X c) Z2 is satisfied. It can also be arranged so that
- an LPP type light source is used as the plasma light source.
- the power S is not limited to this, and a DPP type light source can also be used.
- the EUV light reflected by the auxiliary condenser mirror is not absorbed by the plasma by shifting the spherical center position of the auxiliary condenser mirror slightly from the position of the plasma light source. .
- much more EUV light can be efficiently collected than before.
- by applying a light source unit having such a large increase in light collection efficiency to an exposure apparatus it is possible to significantly improve throughput.
- the reciprocating distance from the plasma light source to the auxiliary converging mirror is made longer than the distance that is the product of the duration of the pulse light of the plasma light source and the speed of light, so that the light from the plasma light source is emitted.
- the plasma is extinguished, and the EUV light reflected by the auxiliary focusing mirror is not absorbed by the plasma.
- much more EUV light can be efficiently collected than before.
- by applying a light source unit having such a large increase in light collection efficiency to an exposure apparatus it is possible to significantly improve throughput.
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
- X-Ray Techniques (AREA)
Abstract
Description
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Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
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AT04747519T ATE448565T1 (de) | 2003-07-14 | 2004-07-14 | Lichtquelleneinheit, optische beleuchtungsvorrichtung und belichtungsvorrichtung |
EP04747519A EP1650786B1 (en) | 2003-07-14 | 2004-07-14 | Light source unit, illumination optical apparatus and exposure apparatus |
KR1020067000854A KR101139051B1 (ko) | 2003-07-14 | 2004-07-14 | 집광 광학계, 광원 유닛, 조명 광학 장치 및 노광 장치 |
DE602004024073T DE602004024073D1 (de) | 2003-07-14 | 2004-07-14 | Lichtquelleneinheit, optische Beleuchtungsvorrichtung und Belichtungsvorrichtung |
US11/327,339 US7385212B2 (en) | 2003-07-14 | 2006-01-09 | Collector optical system, light source unit, illumination optical apparatus, and exposure apparatus |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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JP2003-196194 | 2003-07-14 | ||
JP2003196194A JP4120502B2 (ja) | 2003-07-14 | 2003-07-14 | 集光光学系、光源ユニット、照明光学装置および露光装置 |
Related Child Applications (1)
Application Number | Title | Priority Date | Filing Date |
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US11/327,339 Continuation-In-Part US7385212B2 (en) | 2003-07-14 | 2006-01-09 | Collector optical system, light source unit, illumination optical apparatus, and exposure apparatus |
Publications (1)
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WO2005006414A1 true WO2005006414A1 (ja) | 2005-01-20 |
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PCT/JP2004/010053 WO2005006414A1 (ja) | 2003-07-14 | 2004-07-14 | 集光光学系、光源ユニット、照明光学装置および露光装置 |
Country Status (7)
Country | Link |
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US (1) | US7385212B2 (ja) |
EP (2) | EP1975983B1 (ja) |
JP (1) | JP4120502B2 (ja) |
KR (1) | KR101139051B1 (ja) |
AT (2) | ATE545150T1 (ja) |
DE (1) | DE602004024073D1 (ja) |
WO (1) | WO2005006414A1 (ja) |
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DE102006056035A1 (de) * | 2006-11-28 | 2008-05-29 | Carl Zeiss Smt Ag | Beleuchtungsoptik für die EUV-Projektions-Mikrolithographie, Beleuchtungssystem mit einer derartigen Beleuchtungsoptik, Projektionsbelichtungsanlage mit einem derartigen Beleuchtungssystem, Verfahren zur Herstellung eines mikrostrukturierten Bauteils sowie durch das Verfahren hergestelltes mikrostrukturiertes Bauteil |
US7728988B2 (en) * | 2008-01-24 | 2010-06-01 | Raytheon Company | Method and apparatus for testing conic optical surfaces |
US7872245B2 (en) * | 2008-03-17 | 2011-01-18 | Cymer, Inc. | Systems and methods for target material delivery in a laser produced plasma EUV light source |
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JP5841655B2 (ja) * | 2010-03-18 | 2016-01-13 | ギガフォトン株式会社 | チャンバ装置および極端紫外光生成装置 |
US8587768B2 (en) | 2010-04-05 | 2013-11-19 | Media Lario S.R.L. | EUV collector system with enhanced EUV radiation collection |
DE102010028655A1 (de) | 2010-05-06 | 2011-11-10 | Carl Zeiss Smt Gmbh | EUV-Kollektor |
DE102011084266A1 (de) | 2011-10-11 | 2013-04-11 | Carl Zeiss Smt Gmbh | Kollektor |
KR101877468B1 (ko) * | 2011-12-29 | 2018-07-12 | 삼성전자주식회사 | 광원 장치 및 광 생성 방법 |
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- 2004-07-14 EP EP08007239A patent/EP1975983B1/en active Active
- 2004-07-14 WO PCT/JP2004/010053 patent/WO2005006414A1/ja active Application Filing
- 2004-07-14 EP EP04747519A patent/EP1650786B1/en active Active
- 2004-07-14 KR KR1020067000854A patent/KR101139051B1/ko active IP Right Grant
- 2004-07-14 AT AT04747519T patent/ATE448565T1/de not_active IP Right Cessation
- 2004-07-14 DE DE602004024073T patent/DE602004024073D1/de active Active
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Also Published As
Publication number | Publication date |
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KR101139051B1 (ko) | 2012-04-30 |
EP1650786A1 (en) | 2006-04-26 |
EP1975983B1 (en) | 2012-02-08 |
EP1650786B1 (en) | 2009-11-11 |
KR20060058678A (ko) | 2006-05-30 |
ATE545150T1 (de) | 2012-02-15 |
US20060120429A1 (en) | 2006-06-08 |
EP1975983A2 (en) | 2008-10-01 |
EP1650786A4 (en) | 2007-09-05 |
JP2005032972A (ja) | 2005-02-03 |
EP1975983A3 (en) | 2008-10-08 |
ATE448565T1 (de) | 2009-11-15 |
US7385212B2 (en) | 2008-06-10 |
DE602004024073D1 (de) | 2009-12-24 |
JP4120502B2 (ja) | 2008-07-16 |
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