WO1998059364A1 - Aligneur de projection, son procede de fabrication, procede d'exposition dudit aligneur et procede de fabrication de composants au moyen de l'aligneur - Google Patents
Aligneur de projection, son procede de fabrication, procede d'exposition dudit aligneur et procede de fabrication de composants au moyen de l'aligneur Download PDFInfo
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- WO1998059364A1 WO1998059364A1 PCT/JP1998/002840 JP9802840W WO9859364A1 WO 1998059364 A1 WO1998059364 A1 WO 1998059364A1 JP 9802840 W JP9802840 W JP 9802840W WO 9859364 A1 WO9859364 A1 WO 9859364A1
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- Prior art keywords
- exposure
- mask
- projection
- optical system
- exposure apparatus
- Prior art date
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Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/027—Making masks on semiconductor bodies for further photolithographic processing not provided for in group H01L21/18 or H01L21/34
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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
- G03F7/70066—Size and form of the illuminated area in the mask plane, e.g. reticle masking blades or blinds
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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
- G03F7/70216—Mask projection systems
- G03F7/70241—Optical aspects of refractive lens systems, i.e. comprising only refractive elements
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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
- G03F7/70483—Information management; Active and passive control; Testing; Wafer monitoring, e.g. pattern monitoring
- G03F7/7055—Exposure light control in all parts of the microlithographic apparatus, e.g. pulse length control or light interruption
- G03F7/70558—Dose control, i.e. achievement of a desired dose
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
Definitions
- the present invention relates to a projection exposure apparatus used for transferring a mask pattern onto a substrate via a projection optical system in a lithographic process for manufacturing a semiconductor element, a liquid crystal display element, or a thin film magnetic head, for example.
- the present invention relates to a method for manufacturing the projection exposure apparatus, an exposure method using the projection exposure apparatus, and a method for manufacturing a circuit device using the projection exposure apparatus.
- an exposure apparatus that handles the lithographic process (typically consisting of a resist coating process, an exposure process, and a resist development process) for manufacturing semiconductor devices Is required to further improve resolution, transfer fidelity, and the like.
- lithographic process typically consisting of a resist coating process, an exposure process, and a resist development process
- reduction projection optics with a projection magnification of 1Z5 times from the reticle to the wafer is mainly used as i-light with a wavelength of 365 nm out of the emission lines of mercury discharge lamps as illumination light for exposure.
- a step-and-repeat type reduction projection exposure apparatus (stepper) using a system is often used.
- the projection optics of the reduced projection optics has to be prevented from becoming extremely large with the increase in the size (chip size) of the circuit devices formed on the wafer.
- the transmittance of the projection optical system to the illumination light for exposure is short.
- the surface of the wafer is determined from the amount of illumination light branched in the illumination optical system and the transmittance.
- Exposure was calculated.
- the exposure time is controlled so that the integrated value of the calculated exposure amount becomes a predetermined value.
- the calculated exposure amount is a constant value. The output of the light source or the scanning speed was controlled so that
- this Ar r excimer laser light source When this Ar r excimer laser light source is used as an exposure light source, there are several oxygen absorption bands in the wavelength band of the spontaneous oscillation state of the ultraviolet pulse light. It is necessary to narrow the band to a wavelength avoiding the band. Furthermore, the illumination light path from the exposure light source to the reticle should be in an environment in which oxygen is not contained as much as possible in the projection light path from the reticle to the wafer. That is, most of those illumination light paths and the projection light path should be inert gas ( It is also necessary to replace with nitrogen gas or helium gas.
- An example of a projection exposure apparatus using such an ArF excimer laser light source is disclosed in, for example, U.S. Pat. No. 5,559,584 (Japanese Unexamined Patent Application Publication No. No. 6-260 386).
- the practical optical glass material having a desired transmittance to ultraviolet pulse light (wavelength 2 about 5 O nm or less) from an excimer laser light source as described above, at present, quartz (Si0 2) and E Only two of them are known, fluorite (fluorite: CaF 2 ).
- quartz Si0 2
- fluorite fluorite: CaF 2
- magnesium fluoride and lithium fluoride are also known, but in order to use them as optical glass materials for projection exposure equipment, it is necessary to solve the problems of workability and durability. is there.
- the projection optical system mounted on the projection exposure apparatus In addition to the W (refraction) system, a catadioptric system (catadioptric system) composed of a combination of a refraction optical element (lens element) and a reflection optical element (especially a concave mirror) is also used.
- a catadioptric system composed of a combination of a refraction optical element (lens element) and a reflection optical element (especially a concave mirror) is also used.
- refractive optical elements transmiss
- two types of glass materials, quartz and fluorite are used as refractive optical elements. I have no choice.
- the optical element is a refractive optical element or a reflective optical element
- a multilayer film such as an anti-reflection film or a protective layer is deposited on the surface thereof, and the optical element is manufactured so that its performance as a single element is in a predetermined state.
- the performance that should be particularly noted here is how large the absolute value of the transmittance of the single lens element or the absolute value of the reflectance of the single reflective optical element can be obtained.
- both the light incident surface and the light exit surface are coated with an anti-reflection film or the like so as to maximize the transmittance.
- a precise imaging optical system such as a projection optical system
- 20 to 30 lens elements are used to satisfactorily correct various aberration characteristics, and the transmittance of each lens element is 100. Even if it is slightly lower than%, the transmittance of the whole projection optical system becomes considerably small (the attenuation rate of the whole projection optical system becomes considerably large). Even in a projection optical system including several reflecting optical elements, when the reflectance of each reflecting optical element is low, the transmittance of the entire projection optical system is low, and the attenuation factor of the entire projection optical system is considerably large.
- the projection optical system has 25 lens elements that form the imaging optical path, and if the individual transmittance of each lens element is 96%, the transmittance ⁇ of the entire projection optical system is about 36%. ( ⁇ 0.96 25 ⁇ 1 0 0).
- the transmittance of the projection optical system is low, should the intensity (energy) of illumination light for exposing the circuit pattern image of the reticle onto the wafer be increased, or should a more sensitive ultraviolet resist be used? If the countermeasures are not taken, the throughput will decrease due to the increase in the exposure time. Therefore, as a countermeasure that can be realized on the projection exposure apparatus side, it is conceivable to prepare a higher output excimer laser light source.
- illumination light in the ultraviolet wavelength range such as KrF excimer laser light or ArF excimer laser light
- the optical element in the projection optical system or the coating material of the optical element for example, an anti-reflection film
- Such phenomena are caused by impurities contained in the gas (air, nitrogen gas, etc.) existing in the space in the projection optical path or the illumination optical path, and organic substances generated from adhesives for fixing the optical element to the lens barrel.
- Substance molecules or impurities for example, water molecules, hydrocarbon molecules, or other substances that diffuse illumination light
- the inner wall of the lens barrel painted surface for anti-reflection, etc.
- Such a variation in transmittance changes the exposure dose to be given on the wafer from an appropriate value, and the transfer fidelity of a fine pattern having a design line width of about 0.25 to 0.18 im transferred on the wafer. May deteriorate.
- a conventional projection exposure apparatus as disclosed in, for example, Japanese Patent Application Laid-Open No. 2-135,723 (U.S. Pat. No. 5,191,374), an optical path in an illumination optical system is not disclosed. The light intensity of the illumination light is detected at a predetermined position, and the intensity (energy per pulse) of the pulse light from the excimer laser light source is adjusted based on the detected light intensity so that an appropriate exposure can be obtained.
- the fluctuation of the transmittance of the illumination optical system and the projection optical system after the portion in the illumination optical path for detecting the intensity of the illumination light for controlling the exposure amount is not taken into account at all. Exposure control could not be performed.
- the present invention provides a projection exposure apparatus that prevents deterioration of control accuracy of an exposure amount due to illuminance fluctuation (or pulse energy fluctuation) on a substrate caused by transmittance fluctuation of a projection optical system.
- the first object is to provide a manufacturing method.
- a second object of the present invention is to provide an exposure method that can obtain good exposure amount control accuracy using such a projection exposure apparatus.
- a third object of the present invention is to provide a method of manufacturing a circuit device capable of forming a circuit pattern on a substrate with high transfer fidelity by using such a projection exposure apparatus.
- the projection exposure apparatus is a projection exposure apparatus that irradiates a pattern formed on a mask with a predetermined exposure energy beam and projects an image of the pattern of the mask onto a substrate via a projection optical system.
- the attenuation rate variation is a function of a total incident energy value incident on the projection optical system via the mask. Based on the transmittance of the mask, it is possible to calculate the total incident energy incident on the projection optical system via the mask.
- the projection exposure apparatus may perform relative scanning between the exposure energy beam and the mask to project an image of a pattern of the mask onto the substrate. Using the relative position information between the exposure energy beam and the mask, the total incident energy incident on the projection optical system via the mask can be calculated.
- the relative position information is an optical characteristic of the mask according to a relative position between the exposure energy beam and the mask.
- the optical characteristics of the mask include the transmittance characteristics of the mask.
- An incident energy measuring system for measuring the total incident energy incident on the projection optical system via the mask may be further provided.
- an emission energy measurement system for measuring emission energy from the projection optical system may be further provided. Further, based on the measurement results of the incident energy measurement system and the emission energy measurement system, The variation in the attenuation rate may be obtained.
- An exposure control system for controlling an exposure amount given on the substrate based on the fluctuation of the attenuation rate may be further provided.
- the attenuation rate characteristic storage system may include, in addition to the attenuation rate of the projection optical system with respect to the total incident energy, the projection optical system with respect to an elapsed time after the irradiation of the exposure energy beam to the projection optical system is stopped.
- the variation of the attenuation rate may be stored.
- An energy beam having a wavelength in the ultraviolet region is used as the exposure energy beam.
- the change in the transmittance of the lens element largely affects the optical characteristics of the projection optical system PL.
- the attenuation rate fluctuates due to the change in the transmittance of the lens element.
- a power dioptric system a catadioptric system
- the change in the reflectance of the reflective optical element in addition to the change in the transmittance of the lens element causes the optical change of the projection optical system PL. This greatly affects the characteristics, and the attenuation factor of the projection optical system PL fluctuates due to the change in the transmittance of the lens element and the change in the reflectance of the reflective optical element.
- the attenuation rate of the projection optical system PL is used.
- the change in the attenuation factor of the projection optical system PL means the change in the transmittance in the case of the projection optical system PL using a dioptric system (refractive system). In the case of the used projection optical system PL, this means a change in transmittance and a change in reflectance.
- the fluctuation of the attenuation rate of the projection optical system is stored as a function of the energy value of the total incident energy incident on the projection optical system, and the exposure is started at the time of actual exposure, that is, the irradiation of the exposure energy beam is started.
- the attenuation rate of the projection optical system can be estimated with high accuracy almost in real time. it can. Therefore, by controlling the exposure amount so as to offset the change in the attenuation rate, the exposure amount due to the illuminance variation (or pulse energy variation) on the substrate caused by the variation in the attenuation rate of the projection optical system can be controlled. Control accuracy can be prevented from deteriorating.
- the attenuation rate characteristic storage system stores the variation of the attenuation rate of the projection optical system with respect to the elapsed time after stopping the irradiation of the exposure energy beam.
- a stage system for moving the mask and the substrate may be provided, and the mask and the substrate may be synchronously scanned with respect to the projection optical system via the stage system during exposure.
- the present invention is applied to a scanning exposure type projection exposure apparatus.
- the scanning speed may be controlled.
- the method of manufacturing a projection exposure apparatus is directed to a projection exposure apparatus that irradiates a pattern formed on a mask with a predetermined exposure energy beam and projects an image of the pattern of the mask onto a substrate via a projection optical system.
- the exposure method of the present invention is an exposure method of irradiating a pattern formed on a mask with a predetermined exposure energy beam, and projecting an image of the pattern of the mask onto a substrate via a projection optical system. Calculating the attenuation rate variation of the projection optical system according to the total incident energy incident on the projection optical system; andbased on the total incident energy value incident on the projection optical system via the mask and the attenuation rate variation. Determining the attenuation factor of the projection optical system.
- a method of manufacturing a circuit device is a circuit device for manufacturing a predetermined circuit device by projecting an image of a pattern of a mask onto a substrate via a projection optical system.
- FIG. 1 is a schematic configuration diagram showing a projection exposure apparatus used in an embodiment of the present invention.
- FIG. 2 is a partial function showing a state in which the dose monitor 32 is moved to the exposure area of the projection optical system PL in order to measure the transmittance (attenuation rate) of the projection optical system PL in the embodiment of the present invention. It is a block diagram including a block diagram.
- FIG. 3 is a flowchart showing the transmittance (attenuation) measurement operation and the exposure operation of the projection optical system PL according to the first embodiment of the present invention.
- FIG. 4 is a flowchart showing a transmission (attenuation) measurement operation and an exposure operation of the projection optical system PL according to the second embodiment of the present invention.
- FIG. 5 is a flowchart showing a transmission (attenuation) measurement operation and an exposure operation of the projection optical system PL according to the third embodiment of the present invention.
- FIG. 6 is a diagram showing an example of a change in the transmittance (attenuation) of the projection optical system PL after the stop of the irradiation of the ultraviolet pulse light measured in the third embodiment.
- FIG. 7 is a flowchart showing an example of a process for forming a circuit pattern in the third embodiment.
- FIG. 1 shows a schematic configuration of the projection exposure apparatus of the present embodiment.
- the ultraviolet pulse light IL as the exposure light narrowed at a wavelength of 193 nm from the ArF excimer laser light source 1 is shown.
- the light passes through a beam matching unit (BMU) 3 including a moving mirror and the like, and enters a variable attenuator 6 serving as an optical attenuator through a light-shielding pipe 5.
- BMU beam matching unit
- Exposure control unit for controlling the amount of exposure on the resist on the wafer 30 0 Force A / F Excimer Laser light source 1 Start and stop light emission, and control the output determined by the oscillation frequency and pulse energy, and variably reduce The extinction ratio for the ultraviolet pulse light in the optical device 6 is adjusted stepwise or continuously.
- the present invention is also applicable to a case where r F excimer laser light having a wavelength of 248 nm or other laser light having a wavelength of about 250 nm or less is used as the exposure light.
- the ultraviolet pulse light IL passed through the variable attenuator 6 is incident on the fly-eye lens 11 via a beam shaping optical system including lens systems 7A and 7B arranged along a predetermined optical axis.
- the fly-eye lens 11 has one stage.
- fly-eye lenses may be arranged in two stages in series.
- An aperture stop system 12 of an illumination system is arranged on the exit surface of the fly-eye lens 11.
- a circular aperture stop for normal illumination, an aperture stop for deformed illumination composed of a plurality of eccentric small apertures, an aperture stop for annular illumination, and the like are arranged to be switchable.
- the ultraviolet pulse light IL emitted from the fly-eye lens 11 and passing through a predetermined aperture stop in the aperture stop system 12 is incident on a beam splitter 8 having a high attenuation factor and a low reflectance.
- the ultraviolet pulse light reflected by the beam splitter 8 enters an integrator sensor 9 composed of a photoelectric detector, and a detection signal of the integrator sensor 9 is supplied to an exposure control unit 30.
- the transmittance and reflectance of the beam splitter 8 are measured with high precision in advance and stored in the memory of the exposure control unit 30.
- the exposure control unit 30 detects the integration sensor 9
- the configuration is such that the amount of incident ultraviolet pulse light IL to the projection optical system PL and the integrated value thereof can be monitored indirectly from the signal.
- a beam splitter 8A is arranged in front of the lens system 7A, and the beam splitter 8A is arranged.
- the reflected light from A may be received by the photoelectric detector 9A, and the detection signal of the photoelectric detector 9A may be supplied to the exposure control unit 30.
- the ultraviolet pulse light IL transmitted through the beam splitter 8 enters the fixed illumination field stop (fixed blind) 15 A in the reticle blind mechanism 16 via the condenser lens system 14.
- the fixed blind 15A has a circular shape of the projection optical system PL as disclosed in, for example, Japanese Patent Application Laid-Open No. Hei 4-19613 (US Pat. No. 5,473,410). It has an opening arranged so as to extend in a linear slit shape or a rectangular shape (hereinafter, collectively referred to as “slit shape”) in the center perpendicular to the scanning exposure direction at the center of the field of view.
- a movable blind 15 B for changing the width of the illumination visual field in the scanning exposure direction is provided separately from the fixed blind 15 A, and the movable blind 15 B is provided.
- the scanning movement stroke of the reticle stage is reduced, and the width of the light-shielding band of the reticle R is reduced.
- the information on the aperture ratio of the movable blind 15 B is also supplied to the exposure control unit 30, and the value obtained by multiplying the incident light amount obtained from the detection signal of the integrator sensor 9 by the aperture ratio is used for the projection optical system PL. This is the actual amount of incident light.
- the ultraviolet pulse light IL shaped into a slit with the fixed blind 15 A of the reticle blind mechanism 16 is passed through the imaging lens system 17, the reflection mirror 18, and the main condenser lens system 19, and then becomes a reticle.
- An illumination area similar to the slit-shaped opening of the fixed blind 15 A is radiated on the circuit pattern area of R with a uniform intensity distribution. That is, the arrangement surface of the opening of the fixed blind 15A or the opening of the movable blind 15B is different from the pattern surface of the reticle R by the combined system of the imaging lens system 17 and the main condenser lens system 19. It is almost conjugate.
- the image of the circuit pattern in the illumination area of the reticle R is converted into a predetermined projection magnification ⁇ ( ⁇ is, for example, 1/4, 1Z5, etc.) through a bilateral telecentric projection optical system PL.
- ⁇ is, for example, 1/4, 1Z5, etc.
- the light is transferred to a slit-shaped exposure area of the resist layer on the wafer W arranged on the image plane of the projection optical system PL.
- the exposure region is located on one of a plurality of shot regions on the wafer.
- the projection optical system PL of this example is a dioptric system (refractive system), but it is needless to say that a catadioptric system (reflective system) can also be used.
- the Z axis is taken parallel to the optical axis AX of the projection optical system PL
- the X axis is taken in the scanning direction (in this case, the direction parallel to the paper in Fig. 1) in a plane perpendicular to the Z axis
- the scanning direction is orthogonal In the non-scanning direction (Vertical direction) and the Y axis.
- the reticle R is held by suction on the reticle stage 20 mm, and the reticle stage 2 OA can move at a constant speed in the X direction on the reticle base 20 B and can finely move in the X, Y, and rotation directions. It is mounted as follows.
- the two-dimensional position and rotation angle of reticle stage 2 OA (reticle R) are measured in real time by a laser interferometer in drive control unit 22.
- the drive motors such as linear motor and voice coil motor
- Stage 2 Controls the scanning speed and position of the OA.
- the wafer W is sucked and held on the Z tilt stage 24Z via the wafer holder WH, and the Z tilt stage 24Z moves two-dimensionally along the XY plane parallel to the image plane of the projection optical system PL.
- the XY stage 24 is fixed on the XY, and the Z tilt stage 24 Z and the XY stage 24 XY constitute the wafer stage 24.
- the Z tilt stage 24 Z controls the focus position (position in the Z direction) and the tilt angle of the wafer W, and the surface of the wafer W is controlled by an autofocus method and an auto-leveling method.
- the XY stage 24XY performs uniform scanning of the wafer W in the X direction and stepping in the X and Y directions.
- the two-dimensional position and rotation angle of the Z tilt stage 24Z (wafer W) are measured in real time by a laser interferometer in the drive control unit 25. Based on this measurement result and the control information from the main control system 27, the drive motor (such as a linear motor) in the drive control unit 25 controls the scanning speed and position of the XY stage 24XY.
- the rotation error of wafer W is corrected by rotating reticle stage 2OA via main control system 27 and drive control unit 22.
- the main control system 27 sends various information such as the movement position, movement speed, movement acceleration, and position offset of the reticle stage 20A and the XY stage 24XY to the drive control units 22 and 25. Then, at the time of scanning exposure, the reticle R is scanned in the + X direction (or —X direction) at the speed Vr through the reticle stage 2 OA with respect to the illumination area of the ultraviolet pulse light IL. The wafer W is moved in the X direction (or + X direction) with respect to the exposure area of the pattern image of the reticle R via the stage 24XY. The scanning is performed at the speed) 3 * V r (] 3 is the projection magnification from the reticle R to the wafer W).
- the main control system 27 performs control for synchronizing the movement of each blade of the movable blind 16 B provided in the reticle blind mechanism 16 with the movement of the reticle stage 2 OA during scanning exposure. Do. Further, the main control system 27 sets various exposure conditions for scanning and exposing the resist in each shot area on the wafer W with an appropriate exposure amount, and executes the optimal exposure sequence in cooperation with the exposure control unit 30. I do. That is, when a command to start scanning exposure to one shot area on the wafer W is issued from the main control system 27 to the exposure control unit 30, the exposure control unit 30 receives the ArF excimer laser light source 1. At the same time, the integral value of the amount of light incident on the projection optical system PL via the integrator sensor 9 is calculated.
- the integrated value is reset to 0 at the start of scanning exposure.
- the exposure control unit 30 sequentially calculates the transmittance (attenuation rate) of the projection optical system PL from the integrated value of the incident light amount, as described later, and performs scanning exposure according to the transmittance (attenuation rate). Control the output of the ArF excimer laser light source 1 (oscillation frequency and pulse energy) and the dimming rate of the variable dimmer 6 so that the appropriate exposure can be obtained at each point of the resist on the wafer W to be subsequently processed. I do. Then, at the end of the scanning exposure to the shot area, the emission of the ArF excimer laser light source 1 is stopped.
- an irradiation amount monitor 32 composed of a photoelectric detector is installed near the wafer holder WH on the Z tilt stage 24 Z in this example, and a detection signal of the irradiation amount monitor 32 is also supplied to the exposure control unit 30. Have been.
- the irradiation amount monitor 32 has a light receiving surface large enough to cover the entire exposure area of the projection optical system PL, and drives the XY stage 24 XY to cover the light receiving surface of the exposure area of the projection optical system PL. By setting the position, the amount of ultraviolet pulse light IL that has passed through the projection optical system PL can be measured.
- the transmittance (attenuation rate) of the projection optical system PL is measured using the detection signals of the integration overnight sensor 9 and the irradiation amount monitor 32.
- the irradiation amount monitor 32 an uneven illuminance sensor having a pinhole-shaped light receiving portion for measuring the light amount distribution in the exposure area may be used.
- the ArF excimer laser light source 1 since the ArF excimer laser light source 1 is used, the variable dimmer 6, the lens systems 7A and 7B, the fly-eye lens 11 and the main condenser lens A sub-chamber 35 is provided for shutting off each illumination light path up to the W system 19 from the outside air, and the entirety of the sub-chamber 35 is provided with a dry nitrogen gas (O2) having an extremely low oxygen content through a pipe 36. N 2 ).
- dry nitrogen gas is supplied to the entire space inside the lens barrel of the projection optical system PL (space between a plurality of lens elements) via the pipe 37.
- the supply of the dry nitrogen gas does not need to be performed so frequently after the air has been completely replaced once.
- the transmittance caused by the adhesion of water molecules and hydrocarbon molecules from various substances (glass materials, coating materials, adhesives, paints, metals, ceramics, etc.) existing in the optical path to the surface of the optical element Considering the fluctuation, it is necessary to remove the impurity molecules by using a chemical filter and an electrostatic filter while forcing the temperature-controlled nitrogen gas to flow in the optical path.
- a transmittance (attenuation rate) measuring system of the projection optical system PL in the projection exposure apparatus of the present embodiment with reference to FIG.
- the XY stage 2 4 XY is driven and the light-receiving surface of the dose monitor 32 is exposed to the exposure area of the projection optical system PL.
- the pulse light emission of the ArF excimer laser light source 1 is started, and a part of the ultraviolet pulse light IL incident on the beam splitter 8 is reflected, and is incident on the integer sensor 9 as the ultraviolet pulse light IL1. I do.
- the ultraviolet pulse light IL 2 that has passed through the projection optical system PL enters the irradiation amount monitor 32, and the detection signal of the integrator sensor 9 and the detection signal of the irradiation amount monitor 32 are controlled in parallel by exposure control. Unit 30.
- the detection signal of the integrator sensor 9 is supplied to a peak hold (P / H) circuit 61 and an analog / digital converter (hereinafter referred to as “AD C”) 62 in the exposure control unit 30.
- the incident energy E i is directly supplied to the transmittance (attenuation) calculator 63 and the incident light amount integrating unit 64 as incident energy E i.
- the direct transmittance (attenuation rate) calculation unit 63, the incident light amount integration unit 64, and the transmittance (attenuation rate) calculation unit 67 and the control unit 69 described later are each executed by a microprocessor. It represents functions on software, but it goes without saying that each of those functions may be implemented by hardware.
- the detection signal of the irradiation dose monitor 32 is supplied to the transmittance (attenuation) calculator 63 as the transmission energy Eo via the peak hold circuit 65 and the ADC 66 in the exposure control unit 30 directly.
- the rate (attenuation rate) T is supplied to the transmittance (attenuation rate) calculator 67.
- the incident light amount integration unit 64 calculates the total incident energy e by integrating (accumulating) the incident energy E i for each incident ultraviolet pulse light, and calculates the transmittance (attenuation rate) of the calculated total incident energy e. Supply to part 67.
- the total incident energy e is reset to 0 immediately before the start of pulse emission.
- the transmittance (attenuation rate) calculation unit 67 calculates a function of the incident total energy e to which the supplied transmittance (attenuation rate) T is supplied (a second-order or higher-order function or an exponential function, etc.) T (e ) And store this function T (e) in memory 68.
- the transmittance (attenuation rate) calculation unit 67 substitutes the total incident energy e supplied from the incident light amount integration unit 64 into the function T (e) read out from the memory 68 to obtain the current projection.
- the transmittance (attenuation rate) T (now) of the optical system PL is obtained, and this transmittance (attenuation rate) T (now) is supplied to the control unit 69.
- the incident energy Ei from the ADC 62 is also supplied to the control unit 69, and the control unit 69 uses the incident energy Ei and the transmittance (attenuation rate) T (now).
- the output of the ArF excimer laser light source 1 and the transmittance of the variable dimmer 6 are controlled so that the exposure amount of the ultraviolet pulse light at each point of the resist on the wafer W becomes an appropriate exposure amount.
- the change in the transmittance (attenuation rate) of the projection optical system PL is measured, and the scanning exposure is performed while controlling the exposure amount based on the measurement result, with reference to the flowchart in FIG. I will explain.
- the measurement of the transmittance (attenuation rate) is performed, for example, at the start of the operation of the projection exposure apparatus or at the start of the exposure operation.
- step 101 of FIG. 3 the light receiving surface of the irradiation amount monitor 32 is set to the exposure area of the projection optical system PL, and the total aperture of the fixed blind 15A and the movable blind 15B is set.
- the rate is set to 100%.
- the reticle R is removed from the reticle stage 2 OA, Scanning of reticle stage 20 A is not performed. Then, pulse emission of the ArF excimer laser light source 1 is started.
- the exposure control unit 30 shown in FIG. 2 takes in the output signals of the integration sensor 9 and the dose monitor 32 in parallel to actually enter the projection optical system PL.
- Incident energy E i corresponding to the energy that is transmitted
- transmitted energy E o corresponding to the energy that actually passes through the projection optical system PL.
- the incident light amount integration section 64 should use a sample hold circuit 'instead of the peak hold circuits 61 and 65 and sequentially integrate the detection signals at a predetermined sampling rate.
- the direct transmittance (attenuation) calculator 63 may calculate the transmittance (attenuation) T at predetermined time intervals.
- the transmittance (attenuation rate) calculation unit 67 in the exposure control unit 30 sets each of the measurement intervals so as to be sufficiently short with respect to the exposure time of one shot. Import the total incident energy e and the transmittance (attenuation rate) T at the measurement time.
- step 105 the transmittance (attenuation rate) calculation section 67 calculates the transmittance (attenuation rate) T (e) of the projection optical system PL as a function of a series of total incident energy—e. It is stored in memory 68. This is equivalent to storing the state of the change of the transmittance (decay rate) of the projection optical system PL with respect to the incident energy Ei.
- the function of the transmittance (decay rate) T (e) is used in step 109 during scanning exposure.
- a step-and-scan projection exposure apparatus is used.
- the exposure control can be performed using both the scanning speed and the light amount control of the exposure light source (including the dimming rate control of the variable dimmer 6).
- a predetermined exposure amount determined from the resist sensitivity and the like is applied to the point during the time when the point passes through the slit-like exposure area by the projection optical system PL.
- the scanning speed of the wafer stage 24 and the light amount of the exposure light source are controlled as described above.
- E is the reference value of the output per unit time of the ArF excimer laser light source 1 (that is, the oscillation frequency X pulse energy). [W]. Further, hereinafter, the output is a value multiplied by the dimming rate in the variable dimmer 6. Then, the initial attenuation rate of the projection optical system PL is T0, the area of the slit-shaped exposure area is S [cm 2 ], the length of the exposure area in the scanning direction is L [mm], and the resist sensitivity is I [JZ cm]. 2 ], the initial value Vw of the scanning speed of the wafer stage 24 during scanning exposure. [mmZ sec] is as follows.
- Vw 0 (Yes. ⁇ T 0 ) (I ⁇ S) (1)
- scanning is performed while maintaining the relative positional relationship between the reticle R and the wafer W so that the wafer stage 24 has the scanning speed.
- step 106 of FIG. 3 the reticle R is placed on the reticle stage 2OA as shown in FIG. 1, and the resist is applied to the wafer holder WH on the wafer stage 24.
- the loaded wafer W is loaded.
- scanning of the reticle stage 20A and the wafer stage 24 is started, and when the scanning is synchronized, A r
- the pulse emission of the F excimer laser light source 1 is started, and the capture of the detection signal of the integration sensor 9 into the exposure control unit 30 is also started.
- the movable blind 15B gradually opens, and transfer of the pattern image of the reticle R to the shot area on the wafer W is started.
- the information on the total aperture ratio of the fixed blind 15A and the movable blind 15B is supplied to the incident light amount integration section 64 of FIG.
- step 107 the incident energy E i is measured for each pulse emission via the integrator sensor 9, peak hold circuit 61, and ADC 62 in FIG. 2, and this incident energy E i is sequentially measured. It is supplied to the incident light quantity integration section 64. So in step 108 following this, the incident light amount integration unit 64 integrates the energy obtained by multiplying the incident energy E i supplied for each pulse emission by the aperture ratio at that time and calculates the total incident energy e up to that point. Then, the total incident energy e from the start of the exposure is supplied to the transmittance (attenuation rate) calculation unit 67.
- the transmittance (attenuation) calculator 67 calculates the total incident energy e into a function T (e) (ie, transmittance data) representing the transmittance (attenuation) read from the memory 68. Then, at a predetermined time interval, the current transmittance (attenuation rate) T (now) of the projection optical system PL is calculated, and the calculated transmittance (attenuation rate) T (now) is supplied to the control unit 69. I do.
- the frequency of this calculation should be sufficiently short for the exposure time of one shot. That is, the transmittance (attenuation) of the projection optical system PL is repeatedly calculated a plurality of times during the exposure time of one shot, and the current transmittance (attenuation) is always obtained almost in real time.
- the control section 69 controls the output of the ultraviolet pulse light IL based on the supplied transmittance (attenuation rate) T (now).
- the wafer W of the ultraviolet pulsed light IL The illuminance (energy per unit time, per unit area) on the surface (wafer surface) should be constant. That is, the Ar F excimer laser light source is designed to offset the change in the transmittance (attenuation) T (now) of the projection optical system PL (inversely proportional to the transmittance (attenuation) T (now)).
- the value of the transmittance (attenuation rate) T (now) of the projection optical system PL at a certain time point t thus obtained is T
- the initial transmittance (attenuation rate) of the projection optical system PL is T.
- the reference value (initial value) of the output of Ar F excimer laser light source 1 is E.
- the target output of the ArF excimer laser light source 1 for keeping the illuminance of the ultraviolet pulse light IL on the wafer surface constant is E (where E, is obtained as follows.
- the control unit 69 adjusts the output of the ArF excimer laser light source 1 (oscillation frequency) so that the output of the ultraviolet pulse light IL passing through the variable dimmer 6 becomes the target output Et obtained from the equation (2). , And pulse energy) or the dimming rate in the variable dimmer 6.
- the operation returns to steps 107 to 110 to calculate the transmittance (attenuation) of the projection optical system PL at predetermined time intervals.
- the calculation of the target output E of the pulsed light IL ( and the output control of the ArF excimer laser light source 1) are performed.
- the operation shifts from step 111 to step 112.
- the emission of the ArF excimer laser light source 1 is stopped, and after the exposure for one shot is completed (step 113), the exposure operation for the next shot area is started (step 114)
- the transmittance (attenuation) of the projection optical system PL is assumed to have almost recovered to the initial transmittance (attenuation) in step 106, and the transmittance (attenuation) is assumed. ) Is started.
- the transmittance (attenuation rate) of the projection optical system PL is measured in almost real time based on the integrated value of the incident energy to the projection optical system PL measured via the integrator sensor 9. Since the output of the ArF excimer laser light source 1 is controlled based on the measurement result so that the illuminance of the ultraviolet pulse light IL on the wafer surface is constant, the transmittance of the projection optical system PL ( Even when the (attenuation rate) changes, the entire surface of each shot area on the wafer W can be exposed with an appropriate exposure amount.
- the output of the ArF excimer laser light source 1 is controlled according to the transmittance (attenuation rate) of the projection optical system PL.
- the exposure light source The output of E. If is constant, the transmittance (attenuation rate) T of the projection optical system PL. And the scanning speed Vw Q of the wafer stage 24 are in a proportional relationship. Therefore, when the transmittance (attenuation rate) T (now) of the projection optical system PL changes, the output of the exposure light source is fixed, and the output is proportional to the transmittance (attenuation rate) T (now).
- the scanning speed of the wafer stage 24 may be controlled. However, this control can be performed in a range where the scanning speed does not reach the upper limit determined by the stage system.
- the projection exposure apparatus shown in Fig. 1 is used, but the method of measuring the change in transmittance (attenuation) of the projection optical system PL is different. Therefore, the operation of measuring the change in the transmittance (attenuation) of the projection optical system PL and the scanning exposure operation in this example will be described with reference to the flowchart of FIG.
- the reticle R to be actually exposed is used and the reticle R is scanned in the same manner as in the actual exposure.
- the total amount of light incident on the projection optical system PL during scanning of the reticle R from the start of scanning to a certain arbitrary position is set to be the same at the time of measurement and at the time of scanning exposure.
- Vm Ve.
- the transmitted energy Eo measured via the irradiation amount monitor 32 is obtained by multiplying the incident light amount by the pattern transmittance of the reticle R and the transmittance (attenuation) of the projection optical system PL.
- the pattern transmittance is known from the design data of the reticle R as a function of the position X of the reticle R, and the object to be determined is the transmittance (attenuation) of the projection optical system PL.
- the pattern transmittance (transmittance) of the reticle R is determined by the position X
- the transmittance (attenuation) T of the projection optical system PL can be obtained from the following equation. More precisely, the pattern transmittance function TR (X) is multiplied by the total aperture ratio of the fixed blind 15A and the movable blind 15B.
- step 121 of FIG. 4 the light receiving surface of the irradiation amount monitor 32 is set in the exposure area of the projection optical system PL (see FIG. 2), the reticle R is placed on the reticle stage 2OA, and the reticle Stage 2 OA moves to the scanning start position.
- design data (reticle data) of the reticle R is called from the host computer (not shown) by the main control system 27 in FIG. 1, for example, and the pattern transmittance corresponding to the position X of the reticle R in the scanning direction is read. TR (X) is calculated.
- step 123 the scanning of the reticle stage 2OA (reticle R) is started and the emission of the ArF excimer laser light source 1 is started by the command of the main control system 27 as in the actual exposure. .
- the reticle R is scanned in the + direction or the 1X direction to the scanning end position.
- step 124 the position X of the reticle stage 20A measured via the drive control unit 22 is supplied to the main control system 27, and the pulse is emitted via the INTEGRA sensor 9 every pulse emission.
- the incident energy E i measured is directly supplied to the transmittance (attenuation) calculation unit 63 and the incident light amount integration unit 64, and the transmitted energy E o measured via the irradiation amount monitor 32 is directly calculated. Transmittance (attenuation rate) Supplied to the calculator 63.
- the main control system 27 calculates the current pattern transmittance TR (X) from the position X of the reticle stage 2OA in a cycle shorter than the pulse emission cycle, and directly calculates the calculated result as the transmittance.
- the incident light amount integration unit 64 integrates (accumulates) the value obtained by multiplying the incident energy E i by the pattern transmittance TR (X) for each pulse emission, calculates the total incident energy e, and calculates the transmittance (attenuation rate).
- Is supplied to the calculation unit 67 and the direct transmittance (attenuation) is calculated by the calculation unit 63 by substituting the incident energy E i and the transmitted energy E o into the equation (4) to obtain the transmittance (attenuation) of the projection optical system PL.
- Rate) T is calculated, and the calculation result is supplied to the transmittance (attenuation rate) calculation unit 67.
- step 125 Until the measurement is completed in the next step 126, that is, until the reticle scale moves to the scanning end position, the operation of step 125 is repeated at a predetermined time interval. 7, the transmittance (attenuation rate) calculation unit 67 calculates the transmittance (attenuation rate) T of the projection optical system PL as a function T (e) of the total incident energy e, and this function T ( e) is stored in the memory 68.
- step 128 scanning of the reticle R and the wafer W is started in step 128 as shown in FIG. 1 in the same manner as in step 106 of FIG.
- Light emission of the F excimer laser light source 1 is started.
- step 129 the position X of the reticle R is measured by the drive control unit 22 at a predetermined cycle, and the incident energy E i is measured by the integrator sensor 9 every pulse emission.
- the pattern transmittance TR (X) calculated from the position X of the reticle R is supplied to the incident light amount integration unit 64 of FIG.
- the value obtained by multiplying the energy E i by the pattern transmittance TR (X) is integrated to calculate the total incident energy e, and the calculation result is supplied to the transmittance (attenuation) calculator 67.
- the transmittance (attenuation rate) calculation unit 67 substitutes the total incident energy e into the function T (e) stored in the memory 68 in step 127 to substitute the current projection optical system PL
- the transmittance (attenuation rate) T (now) is calculated, and the calculation result is supplied to the control unit 69.
- step 131 the control section 69 cancels the fluctuation of the transmittance (attenuation rate) of the projection optical system PL in the same manner as in step 110, so that the illuminance of the ultraviolet pulse light IL on The output of the ArF excimer laser light source 1 or the dimming rate of the variable dimmer 6 is controlled so that Subsequent steps 132 to 135 are the same as steps 111 to 114, and the scanning exposure for the shot area and the preparation for exposure to the next shot area are performed.
- the pattern transmittance of the reticle is also taken into consideration, the fluctuation of the transmittance (attenuation) of the projection optical system PL during actual scanning exposure can be detected with higher accuracy. Therefore, the control accuracy of the exposure amount is also improved.
- the reticle R is assumed to be scanned in an arbitrary direction when the transmittance (attenuation) is measured, but a function T (e) representing the transmittance (attenuation) of the projection optical system PL depending on the scanning direction. ) May change slightly. Therefore, the functions Tl (e) and T2 (e) are obtained for each scanning direction, and the functions Tl (e) and T2 (e) are used depending on the scanning direction during scanning exposure. You may. Accordingly, even when the reticle pattern transmittance is not symmetric or the reticle substrate itself is not symmetrical, the exposure amount control is performed with high accuracy.
- the projection exposure apparatus shown in Fig. 1 is used, but in this example, the fluctuation of the transmittance (attenuation rate) of the projection optical system PL after the stop of the irradiation of the ultraviolet pulse light IL is also measured. That is, in the first and second embodiments, the simple assumption is made that the transmittance (attenuation rate) of the projection optical system PL returns to the initial state immediately after stopping the irradiation of the ultraviolet pulse light IL. In addition, the change in the transmittance (attenuation rate) of the projection optical system PL was determined by considering only the irradiation for each scanning exposure.
- the transmittance may not be sufficiently restored to the initial state after the end of the exposure of a certain shot and before the start of the exposure of the next shot.
- a large change in transmittance is required because a large amount of exposure is required, and it is difficult for the transmittance to recover to the initial state between shots.
- the stepping time between shots is shortened to improve the throughput of the device, the recovery of the transmittance between shots may become insufficient. It is necessary to consider the transmittance (attenuation rate) fluctuation of
- steps 141 to 145 of FIG. 5 similarly to steps 101 to 105 of the first embodiment (steps 121 to 155 of the second embodiment). 27), the change in the transmittance (attenuation) of the projection optical system PL during irradiation with the ultraviolet pulsed light IL is measured, and the transmittance (attenuation) T as a function of the total incident energy e is measured. (e) is obtained and stored in the memory 68.
- steps 147 to 150 a change in the transmittance (attenuation rate) of the projection optical system PL without irradiation is measured and expressed as a function of elapsed time.
- step 146 the emission of the ArF excimer laser light source 1 is stopped in a state where the projection optical system PL is irradiated with the exposure amount obtained by adding a predetermined margin to the assumed maximum exposure amount, for example. I do. Then, the elapsed time t from the stop of light emission is measured in step 147, and the light of the minimum pulse number is instantaneously emitted to the ArF excimer laser light source 1 in Fig. 2 at predetermined time intervals in step 148.
- the transmittance (attenuation rate) T is supplied to the transmittance (attenuation rate) calculation unit 67. This measurement of the attenuation rate is repeated a predetermined number of times, and when the measurement is completed, the operation shifts from step 149 to step 150, and the transmittance (attenuation rate) calculation section 67 calculates the transmittance of the projection optical system PL.
- the transmittance (attenuation rate) T is approximated as a function T (t) of the elapsed time t from the stop of the emission of the ultraviolet pulse light IL, and this function T (t) is stored in the memory 68.
- T (t) a function of the quadratic or higher order of the elapsed time t with an undetermined coefficient in advance, or an exponential function can be used.
- the curve 70 C in Fig. 6 shows the transmission of the projection optical system PL after the irradiation of the ultraviolet pulse light IL was stopped.
- the horizontal axis in Fig. 6 is the elapsed time t (hour) since the irradiation was stopped, and the vertical axis is the transmittance (decay rate).
- T (relative value).
- Curve 7 OA indicates the incident energy E i (relative value) instantaneously supplied for the measurement of the attenuation rate
- curve 70 B indicates the transmittance measured corresponding to the incident energy E i. It shows over energy E o (relative value).
- the transmittance (attenuation rate) T of the projection optical system PL recovers once and then gradually decreases.
- the memory 68 stores a function T (t) of the elapsed time t approximating the curve 70C.
- the main control system 27 in FIG. 1 irradiates the transmittance (attenuation rate) calculator 67 in FIG. 2 with the ultraviolet pulse light IL, or during stepping between shots, for example.
- Information indicating whether irradiation of the ultraviolet pulse light IL has been interrupted is supplied.
- the transmittance (attenuation rate) calculation unit 67 may determine whether irradiation is being performed based on the presence or absence of the incident energy E i from the ADC 62. In this way, in step 1 51 of FIG. 5, the transmittance (attenuation rate) calculation unit 67 determines whether or not the ultraviolet pulse light IL is being irradiated.
- step 52 the total incident energy e from the incident light amount integration unit 64 is taken in at a predetermined time interval, and in step 1553, this total incident energy e and stored in the memory 68 in step 144.
- T (e) the current transmittance (attenuation) T (now) of the projection optical system PL is obtained.
- step 154 the output of the ultraviolet pulse light IL is controlled so as to cancel the change in the transmittance (attenuation rate) T (now) in the same manner as in step 110 of FIG. Until the scanning exposure is completed at 55, the operations of steps 152 to 154 are repeated.
- step 155 the scanning exposure is completed, and in step 159, when exposure to one shot area is completed, it is determined in step 165 whether exposure to all shot areas is completed. If the exposure has not been completed, the flow returns to step 151. In this case, since the wafer stage 24 is stepping to move the next shot area to the scanning start position and the irradiation of the ultraviolet pulse light IL has been interrupted, the operation is performed from step 15 1 to step 1 The process proceeds to step 56, where the transmittance (attenuation rate) calculation unit 67 firstly receives the total incident energy supplied from the incident light amount integration unit 64 at that time.
- the transmissivity (attenuation rate) TA of the current projection optical system PL is calculated from the energy e and the function T (e) stored in step 145.
- the transmittance (attenuation rate) calculation unit 67 stores the elapsed time t from the interruption of the irradiation of the ultraviolet pulse light IL and the time in step 150. From the function T (t) obtained, the current transmittance (attenuation rate) TB of the projection optical system PL is calculated.
- the transmittance (attenuation rate) calculation unit 67 calculates the current The actual transmittance (attenuation rate) T (now) of the projection optical system PL is calculated.
- the initial value of the transmittance (attenuation) of the projection optical system PL is calculated by the equation (5).
- Exposure amount control is performed as a fixed value. In this way, scanning exposure is performed on each shot area, and when the exposure on all shot areas is completed in step 160, the exposure operation ends in step 161.
- the fluctuation of the transmittance (attenuation rate) of the projection optical system PL when the irradiation of the ultraviolet pulse light IL is interrupted between shots is taken into consideration, so that higher accuracy is achieved.
- the exposure amount to each shot area on the wafer W is controlled.
- step 171 of FIG. 7 the reticle R is loaded on the reticle stage 20A of FIG.
- step 172 a metal film is vapor-deposited on the wafer to be exposed (wafer), and in step 173, a resist is applied on the metal film on the wafer W.
- the wafer is loaded on the wafer stage 24 of the apparatus.
- Step 174 similarly to the operations in Steps 151 to 161 in FIG.
- the change in the transmittance (attenuation) of the projection optical system PL is canceled out, that is, the ultraviolet pulse on the wafer W is canceled.
- the pattern image of the reticle R is exposed to each shot area on the wafer W by a scanning exposure method while controlling the amount of the ultraviolet pulse light IL so that the illuminance of the light IL is constant.
- the resist on the wafer W is developed, and in Step 176, the metal film on the wafer W is etched using the resist pattern as a mask, and then the resist pattern is removed.
- a desired circuit pattern is formed in each shot area on the wafer W.
- the wafer W moves to a process of forming a circuit pattern of the next layer.
- the desired circuit pattern is formed with high transfer fidelity in each shot area on the wafer W. You.
- the present invention is applied to a step 'and' scan type projection exposure apparatus.
- the present invention is applied to a case where exposure is performed by a step and repeat type projection exposure apparatus (stepper).
- stepper for example, in a process corresponding to steps 110 and 111 in FIG. 3, the exposure time is controlled so that the integrated exposure amount to the shot area on the wafer becomes a predetermined value. Is controlled.
- the change in the attenuation rate of the projection optical system from the start of exposure of the exposure energy beam shows a substantially constant change amount in accordance with the irradiation amount, and the change in the attenuation rate is determined in advance. Measured and memorized.
- the change in the attenuation rate of the projection optical system is estimated from the amount of exposure energy beam incident on the projection optical system, and the exposure amount is controlled in accordance with the change in the attenuation rate.
- the attenuation rate characteristic storage system stores, in addition to the rate of change of the attenuation rate of the projection optical system with respect to the total incident energy, the attenuation rate of the projection optical system with respect to the elapsed time after the interruption of the exposure energy beam irradiation.
- the arithmetic system stores the two types of change rates of the attenuation rate stored in the attenuation rate characteristic storage system, the output of the incident energy integration system, and the time elapsed after the irradiation of the exposure energy beam was interrupted.
- a constant illuminance can be obtained on a substrate surface, for example, in accordance with a change in attenuation factor of a projection optical system.
- the exposure method of the present invention by using a scanning exposure type projection exposure apparatus, when measuring the change in the attenuation rate of the projection optical system, the attenuation rate in a state where the mask is actually used is measured. This prevents erroneous measurement of the change in the attenuation factor of the projection optical system due to the change in the amount of incident energy due to the difference in the pattern density of the mask, thereby improving the exposure amount control accuracy.
- a circuit pattern can be formed on a substrate with high transfer fidelity using the projection exposure apparatus of the present invention.
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP98929682A EP1017086A4 (en) | 1997-06-25 | 1998-06-25 | PROJECTION ALIGNMENT DEVICE, METHOD FOR PRODUCING THE ALIGNMENT DEVICE, EXPOSURE METHOD USING THE ALIGNMENT DEVICE, AND METHOD FOR PRODUCING CIRCUITING ARRANGEMENTS USING THE ALIGNMENT DEVICE |
AU79334/98A AU7933498A (en) | 1997-06-25 | 1998-06-25 | Projection aligner, method of manufacturing the aligner, method of exposure using the aligner, and method of manufacturing circuit devices by using the aligner |
US10/042,345 US20020061469A1 (en) | 1997-06-25 | 2002-01-11 | Projection apparatus, method of manufacturing the apparatus,method of exposure using the apparatus, and method of manufacturing circuit devices by using the apparatus |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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JP9/168406 | 1997-06-25 | ||
JP9168406A JPH1116816A (ja) | 1997-06-25 | 1997-06-25 | 投影露光装置、該装置を用いた露光方法、及び該装置を用いた回路デバイスの製造方法 |
Related Child Applications (1)
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US46922999A Continuation | 1997-06-25 | 1999-12-22 |
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WO1998059364A1 true WO1998059364A1 (fr) | 1998-12-30 |
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ID=15867540
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/JP1998/002840 WO1998059364A1 (fr) | 1997-06-25 | 1998-06-25 | Aligneur de projection, son procede de fabrication, procede d'exposition dudit aligneur et procede de fabrication de composants au moyen de l'aligneur |
Country Status (6)
Country | Link |
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US (1) | US20020061469A1 (ja) |
EP (1) | EP1017086A4 (ja) |
JP (1) | JPH1116816A (ja) |
KR (1) | KR20010020502A (ja) |
AU (1) | AU7933498A (ja) |
WO (1) | WO1998059364A1 (ja) |
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Also Published As
Publication number | Publication date |
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KR20010020502A (ko) | 2001-03-15 |
US20020061469A1 (en) | 2002-05-23 |
AU7933498A (en) | 1999-01-04 |
EP1017086A4 (en) | 2004-06-02 |
EP1017086A1 (en) | 2000-07-05 |
JPH1116816A (ja) | 1999-01-22 |
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