The present invention relates generally to optical elements, and more particularly to a renewable optical element that may be reused after it deteriorates.
Along with recent demands on smaller and lower profile electronic devices, fine semiconductor devices to be mounted onto these electronic devices have been increasingly demanded. For example, a design rule for a mask pattern requires an extensive formation of the image with a size of a line and space (“L & S”) of 0.1 μm or less, which will predictably shift to a formation of circuit patterns of 80 nm or less in the future. L & S denotes an image projected onto a wafer in exposure with equal line and space widths, and serves as an index of exposure resolution.
A projection exposure apparatus as a typical exposure apparatus for fabricating semiconductor devices, generally has an illumination apparatus that includes a light source such as laser and an illumination optical system for illuminating a reticle (mask), and a projection optical system that is located between the mask and an object to be exposed. Recent years have required smaller resolution to transfer a finer circuit pattern, and attempted to improve the resolution using a shorter wavelength. An exposure light source has recently been shifted from KrF excimer laser (with a wavelength of approximately 248 nm) and ArF excimer laser (with a wavelength of approximately 193 nm) to F2 excimer laser (with a wavelength of approximately 157 nm). Practical use of extreme ultraviolet (“EUV”) light with a wavelength of 5 to 20 nm has also been promoted. When the EUV light is used as exposure light, no transmission and refraction-type materials are usable, and optical systems need to include only reflection-type or catoptric optical elements, i.e., mirrors. The catoptric optical element in an exposure apparatus using EUV light includes a grazing-incidence total-reflection mirror and a multilayer mirror.
A real part of the refractive index is slightly smaller than 1 in the EUV region, and generates total reflection for EUV light enters a surface with a narrow grazing angle. A grazing-incidence total-reflection mirror may usually maintain its reflectance higher than several scores of percentage for obliquely incident light within several degrees from the surface, but its degree of freedom in design is small.
A multilayer mirror that alternately forms or layers two kinds of materials having different optical constants is used for a mirror for EUV light with an incident angle close to normal incidence. The multilayer mirror reflects EUV light with a specific wavelength when receiving EUV light. The wavelength A of the reflected EUV light is approximately expressed by Bragg's equation below where θ is an incident angle and d is a coating cycle:
2·d·cosθ=λ (1)
Efficiently reflected EUV light is one within a narrow bandwidth around λ that satisfies the equation 1, and the bandwidth is about 0.6 to 1 nm.
For example, a condenser mirror as a first mirror for efficiently taking in EUV light emitted isotropically from a light source (a plasma) is made of a spheroid or paraboloid of revolution with a concave curvature viewed from the light source (the plasma). A sufficiently smooth substrate is necessary to avoid lowered reflectance, and a relationship between reflectance R and surface roughness σ of the substrate is given by the equation below by using the wavelength λ, the incident angle θ, and reflectance Ro without surface roughness:
R=Rc exp[−(4πσ·cosθ/λ)2] (2)
When the light with a wavelength of 13 nm enters a multilayer mirror with normal incidence or at an angle θ of 0° and the degradation of reflectance due to the surface roughness is within 5% or less, Equation 2 requires the surface roughness σ=0.2 nm. Thus, the substrate needs a precisely polished curved surface.
A multilayer is formed on this substrate. Evaporation is a major coating method that evaporates several types of materials, rotates a holder that supports the substrate, and passes it over an evaporation source. The evaporation has a difficulty in uniformly coating as the substrate's offset from a flat surface or curvature becomes large. In addition, the EUV light incident upon the first mirror has different incident angles depending upon locations, and requires a thickness distribution. Disadvantageously, a fabrication of a multilayer mirror with a large curvature is very difficult.
Debris is a critical problem for an EUV light source. The debris is particles scattering from the light source. A debris source depends upon a light source system. For example, a target or a supply nozzle is an emission source for a laser plasma light source. Debris disadvantageously sticks to a multilayer or collides with the multilayer, destroying its multilayer structure and lowering its reflectance. Of course, the mirror reflectance lowers due to deteriorations with time, and contamination by impurities inside a vacuum chamber.
A deteriorated mirror should be exchanged so as to always ensure adequate reflectance for exposure with high exposure performance such as throughput. The first mirror in particular is easily subject to debris and deterioration. As discussed, a multilayer mirror is complicated and difficult to fabricate, and a precisely polished substrate is often expensive. Therefore, an exchange of a deteriorated multilayer mirror with a new multilayer mirror is not preferable because an exposure apparatus user incurs increased running cost for an apparatus and thus large economical burden.
Accordingly, it is an exemplary object of the present invention to easily form a multilayer mirror with a large curvature, and to provide an optical element whose deteriorated mirror is made reusable, and a light source unit and an exposure apparatus having the same.
An optical element of one aspect of the present invention includes plural multilayer mirrors, wherein the multilayer mirrors are renewable. The optical element may have a concave shape, and serves to condense incident light. The multilayer mirror may have a dividable side along a line having an equal incident light angle to the optical element.
The multilayer mirror may form a release layer and a multilayer in this order on a substrate, and the release layer may be soluble in a solution that is less reactive with the substrate. The release layer may dissolve in the solution at a speed 1000 times or more than the substrate.
The multilayer mirror may form a buffer layer and a multilayer in this order on a substrate, and the multilayer may be soluble in etchant that is less reactive with the buffer layer. The buffer layer may dissolve in the etchant at a speed equal to or less than 1/1000 of a solution velocity of the multilayer.
The multilayer mirror may form a buffer layer and a multilayer in this order on a substrate, and the multilayer may be removable by a dry etching process that is less reactive with the buffer layer. The buffer layer may be removed by the dry etching process at a speed equal to or less than 1/1000 of a removal velocity of the multilayer.
The multilayer mirror may form a buffer layer, a release layer, and a multilayer in this order on a substrate, and the release layer may be soluble in a solution that is less reactive with the buffer layer. The release layer may dissolve in the solution at a speed 1000 times or more than that of the buffer layer.
The multilayer mirror is designed to reflect EUV light (with a wavelength of 5 to 20 nm). It may have a protective layer for protecting the multilayer mirror on its surface.
A light source unit of another aspect of the present invention includes a light source that generates light, and the above optical element that includes plural multilayer mirrors, and condenses the light generated from the light source, wherein the multilayer mirror is renewable. The light may be EUV light (with a wavelength of 5 to 20 nm).
An exposure apparatus of another aspect of the present invention includes the above optical element for introducing-light from a light source to an object to be exposed. The exposure apparatus may further include an illumination optical system that includes the optical element at a first stage, the illumination optical system using light that has passed the optical element to illuminate a reticle (mask), and a projection optical system for projecting a pattern formed on the reticle onto the object. The light may be EUV light (with a wavelength of 5 to 20 nm).
An exposure apparatus of still another aspect of the present invention includes the above light source, an illumination optical system that uses light from the light source unit to illuminate a reticle (mask), and a projection optical system for projecting a pattern formed on the reticle onto an object to be exposed.
A device fabrication method of another aspect of this invention includes the steps of exposing a plate by using the above exposure apparatus, and performing a predetermined process for the exposed object. Claims for a device fabrication method for performing operations similar to that of the above exposure apparatus cover devices as intermediate and final products. Such devices include semiconductor chips like an LSI and VLSI, CCDs, LCDs, magnetic sensors, thin film magnetic heads, and the like.
Other objects and further features of the present invention will become readily apparent from the following description of the preferred embodiments with reference to accompanying drawings.
With reference to accompanying drawings, a description will now be given of an exposure apparatus 10 that uses an optical element 100 of one aspect according to the present invention. In each figure, the same reference numeral indicates a corresponding member. Here,
The inventive exposure apparatus 10 uses EUV light with a wavelength of 5 to 20 nm, for example, a wavelength of 13.4 nm as illumination light for exposure. The exposure apparatus 10 forms an arc or ring image surface, and exposes the whole area on the mask by scanning the mask and the wafer at a speed ratio of a reduction ratio. Any other method is applicable. Referring to
The EUV light source 210 of this embodiment employs, for example, a laser plasma light source. The laser plasma light source generates high temperature plasma 215 by irradiating a exciting pulse laser beam 110 generated from a pulse laser (not shown) via a condensing lens 214 onto a target material that is supplied in a vacuum chamber 280 by a target supply unit, which includes, for example, a supply nozzle 130 for jetting droplets as a target material, and an exhausting section 140 for collecting unused droplets. It uses the EUV light with a wavelength of about 13.4 nm as the light source 210, which has been irradiated from the plasma. The target material may use a metallic thin film, an inert gas, a liquid-drop, etc., and the target supply unit may use a gas jet and so on. The pulse laser 211 is usually driven with a higher repetitive frequency, such as several kHz, for increased average intensity of radiated EUV. An alternative embodiment may use a discharge plasma light source, which emits gas around an electrode in the vacuum chamber 280, applies pulse voltage to the electrode to cause discharge, generates high temperature plasma, and uses EUV light with a wavelength of, for example, about 13.4 nm radiated from it.
The optical element 100 shown in detail in
The multilayer 112 alternately forms or layers two kinds of materials of different optical constants (e.g., molybdenum (Mo)/silicon (Si)). For example, a molybdenum layer is about 2 nm thick, a silicon layer is about 5 nm thick, and the number of layers is about 20 pairs of layers. A sum of thickness of two kinds of materials is called a coating cycle. In the above example, the coating cycle is 2 nm+5 nm=7 nm. A multilayer 112 accumulating about 20 pairs of layers (each thickness of one pair of layers is about 7 nm) exhibits almost 70% of reflectance in the EUV region.
The protective layer (not shown) located below is made of SiO2 with a thickness of 30 nm to 50 nm and used to protect aluminum of the release layer 114. The release layer 114 is made of aluminum with a thickness of 100 nm. The protective layer is not necessarily needed. The substrate 118 is a (ceramic) glass plate fabricated with a good surface precision for reflectance, etc. A curved surface is so precisely polished with surface roughness σ=0.2 nm that the degradation of reflectance may be within 5% due to the surface roughness when light with a wavelength of about 13 nm enters the multilayer mirror with normal incidence or at θ=0°.
A thickness d of the multilayer 112 satisfies above Equation 1 with the wavelength λ of reflected light and incident angle θ. Since the use wavelength for the exposure apparatus 10 is fixed, a film thickness needs to change depending on incident angles θ. The optical element 100 needs to have a film thickness distribution along an axis A that connects focal points of an ellipsoid to each other. A difference in the film thickness distribution becomes large according to having large curvature. The evaporation is a major coating method that evaporates several kinds of materials, rotates the holder 330 that supports the substrate 118, and passes it over the evaporation source 320.
A difference in film thickness distribution which individual mirrors need may be small by dividing the optical element 100 perpendicular to the axis A that connects focal points of an ellipsoid or a line with an equal light incident angle θ. A subdivision into plural pieces, for example, as in a dotted line parallel to the axis A, would realize a flat surface as shown in
A description will now be given of a spheroidal mirror of a size shown in
The EUV light source 210 generates debris and the EUV light from the target 213 and the discharge electrode. Debris sticks to the multilayer 112 or collides with the multilayer 112, destroying its multilayer structure and lowering its reflectance. The mirror reflectance lowers due to deteriorations with time, and contamination of the multilayer 112 by impurities inside a vacuum chamber 280. The first mirror or optical element 100 with deteriorated reflectance should be replaced, but the precisely polished substrate 118 is preferably reused in the multilayer 112.
The instant embodiment removes the multilayer 112 and coats it again, after picking up the optical element 100 and dividing into respective mirrors 110, thereby reusing the substrate 118. Advantageously, a subdivision of plural multilayer mirrors 110 facilitates coating and removal of the multilayer. One exemplary multilayer removal method etches the release layer 114 between the substrate 118 and the multilayer 112, and removes the multilayer 112, as disclosed in “Repair of high performance multilayer coatings”, SPIE1547 (1991). This method would increase an area of the release layer 114 to be exposed to a solution as the optical element 100 is divided, and a removal of the multilayer finishes in a shorter time. When the multilayer 112 uses Mo/Si, the release layer 114 uses aluminum with a thickness of 100 nm, the protective layer uses SiO2 with a thickness of 30 nm to 50 nm, and the etchant includes hydrochloric acid and copper sulfate, it takes about four hours to etch the release layer 114 with a diameter of 50 mm without damaging the substrate 118.
An individual multilayer mirror 110 in the divisible first mirror or optical element 100 in the above embodiment may be a multilayer mirror 110a that includes, as shown in
An individual multilayer mirror 110 in a divisible first mirror or optical element 100 may be a multilayer mirror 110b that includes, as shown in
Germanium, chrome, etc. are effective materials for the release layer 114a. Carbon is suitable for the buffer layer 116a. The release layer 114a made of germanium is quickly etched in a sodium hydroxide solution at room temperature. The release layer 114a made of chrome is etched in a TFM-type etchant. After the release layer 114a is removed, carbon is selectively removed in the dry etching process, e.g., low temperature plasma ozone etching.
An individual multilayer mirror 110 in the divisible first mirror 100 may be a multilayer mirror 110c that includes, as shown in
The divisible first mirror or optical element 100 may use a multilayer mirror 110c, as shown in
The illumination optical system 220 propagates the EUV light to illuminate a reticle (mask) 230. The illumination optical system 220 includes, as shown in
The projection optical system 250 is a catoptric reduction projection optical system including plural mirrors 251 to 256, especially suitable for the EUV light having a wavelength, for example, of 13.4 nm, for reducing and projecting a pattern on the mask 230 onto an object W.
The reticle stage 260 and the wafer stage 270 each include a mechanism for scanning synchronously at a speed ratio in proportion to a reduction ratio. Here, “X” is a scan direction in the reticle 230 surface or the object W surface, “Y” is a direction perpendicular to it, and “Z” is a direction perpendicular to the reticle 230 surface or the object W surface.
The reticle 230 forms a desired pattern and is held on a reticle chuck (not shown) on the reticle stage 260. The reticle stage 260 has a mechanism for moving in the direction X, and a fine adjustment mechanism in the directions X, Y, Z, and rotational directions around each axis for positioning the reticle 230. A position and orientation of the reticle stage 260 are measured by a laser interferometer, and controlled based on the measurement results. While the instant embodiment uses a catoptric reticle for the reticle 230, a transmission type reticle are also usable.
The instant embodiment uses a wafer as the object to be exposed W, but it may include a liquid crystal plate and a wide range of other objects to be exposed. Photoresist is applied onto the object W. A photoresist application step includes a pretreatment, an adhesion accelerator application treatment, a photo-resist application treatment, and a pre-bake treatment. The pretreatment includes cleaning, drying, etc. The adhesion accelerator application treatment is a surface reforming process so as to enhance the adhesion between the photoresist and a base (i.e., a process to increase the hydrophobicity by applying a surface active agent), through a coat or vaporous process using an organic film such as HMDS (Hexamethyl-disilazane). The pre-bake treatment is a baking (or burning) step, softer than that after development, which removes the solvent.
An object to be exposed W is held onto the wafer stage 270 by a wafer chuck (not shown). Similar to the reticle stage 260, the wafer stage 270 has a mechanism for moving in the direction X, and a fine adjustment mechanism in the directions X, Y, Z, and rotational directions around each axis for positioning the object W. The position and orientation of the wafer stage 270 are measured by a laser interferometer, and controlled based on the measurement results.
The alignment detection optical system 240 measures a positional relationship between the position of the reticle 230 and the optical axis of the projection optical system 250, and a positional relationship between the position of the object W and the optical axis of the projection optical system 250, and sets positions and angles of the reticle stage 260 and the wafer stage 270 so that a projected image of the reticle 230 may be positioned in place on the object W. A focus detection optical system (not shown) measures a focus position in the direction Z on the object W surface, and control over a position and angle of the wafer stage 270 may always maintain the wafer surface at an imaging position of the projection optical system 250 during exposure.
Once a scan exposure finishes on the object W, the wafer stage 270 moves stepwise in the directions X and Y to the next start position for scan exposure, and the reticle stage 260 and the wafer stage 270 synchronously scan in the direction X at a speed ratio in proportion to the reduction ratio of the projection optical system.
While the reduced projected image of the reticle 230 is formed on the object W, a synchronous scan between them is repeated in a step-and-scan manner. A pattern on the reticle 230 is thus transferred onto the entire area on the object W.
A space in which the EUV light propagates and the optical element for receiving the EUV light is located should be maintained under a certain pressure or lower, in order to prevent gas from absorbing the EUV light, and remnant carbons and other molecules from adhering to the optical element. The light source, the illumination optical system 220, the projection optical system 250, the reticle 230, the object W, etc. are housed in the vacuum chamber 280, which is exhausted of air for a certain degree of vacuum.
In exposure, the illumination optical system 220 uses the EUV light emitted from the EUV light source 210 and condensed by the first mirror or optical element 100 to illuminate the mask 230 and images a pattern on the mask 230 surface onto the object W surface, such as a wafer, to which resist is applied. The present embodiment forms an arc or ring image surface, and exposes the entire area on the mask by scanning the mask and wafer at the speed ratio of the reduction ratio.
While the instant embodiment uses an optical element as one aspect of the present invention for the first mirror 100, the present invention is not limited to this embodiment. The optical element as one aspect of the present invention is applicable to another optical element in the illumination optical system 220 other than the first mirror 100 and an optical element in the projection optical system 250. In this case, a surface shape of the optical element may be formed as a paraboloid of revolution rather than a spheroid.
The exposure apparatus does not limit the light source unit to one in the instant embodiment. The light source unit may use, for example, a Z pinch method as one discharge method, a plasma focus, a capillary discharge, a hollow cathode triggered Z pinch, etc.
Referring now to
Further, the present invention is not limited to these preferred embodiments, and various variations and modifications may be made without departing from the scope of the present invention.
Thus, the present invention divides an optical element having a large curvature, and facilitates formations and removals of a multilayer and a protective layering. This allows the multiple coating or the protective layering to be exchanged when the reflectance of the mirror reduces, recovering the reflectance to its initial state.
Number | Date | Country | Kind |
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2002-142454 | May 2002 | JP | national |
This is a divisional of prior application Ser. No. 10/439,711, filed May 16, 2003, now pending. The prior application is incorporated herein by reference in its entirety. This application claims the right of priority under 35 U.S.C. §119 based on Japanese Patent Application No. 2002-142454, filed on May 17, 2002, which is hereby incorporated by reference herein in its entirety as if fully set forth herein.
Number | Date | Country | |
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Parent | 10439711 | May 2003 | US |
Child | 11733583 | Apr 2007 | US |