Synthetic imaging technique

Abstract: An optical system wherein a mask pattern occurring at a predetermined period is imaged with a period less than the predetermined period. Spatial filter means are disposed within the optical system for permitting only the two positive and negative first orders of light from an illumination source diffracted by the mask pattern to pass therethrough.

Description: The present invention is directed to an afocal optical system according to the preamble of claim 1. One type of data storage media utilize optical disks. In this type of data storage photolithographic techniques are utilized to form circular or spiral patterns on glass disks in much the same way as integrated circuits are formed on silicon wafers. The patterns consist of lines and spaces on which data may be permanently or temporarily stored. In the latter case the lines and or spaces may be formed of sensitive material on which lasers may be used to read, write or erase and rewrite. More conventional read, write and rewrite techniques such as magnetic read-write heads may also be used. A very important feature of such memory disks is the density at which data may be stored thereon. The storage density is a function of the closeness at which discrete lines and spaces are formed on the disks. In US-A-4293186 a catadioptric optical imaging system is shown comprising a convex mirror and a concave mirror with said mirrors being arranged with their centres of curvature along a system axis. Such a system has been devised in order to obtain a well corrected imaging system suitable for photolithography employed for the manufacture of integrated circuits. In order to provide good correction resulting in a high resolution, the optical system comprises two meniscus lenses for balancing the effects of the variation in the Petzval sum due to the variation in colour. From JP-A-6141150 a refractive optical system is known comprising a light source, a collimator lens to illuminate a phase grating disposed on a reticle, a first Fourier transform lens, a spatial filter in the Fourier transform plane of said first lens and a second Fourier transform lens for forming an image of the phase grating on the wafer having a pitch higher than the pitch of the phase grating on the reticle. FR-A-2582415 discloses an optical apparatus for spatial filtering comprising a parabolic concave mirror and a reflection filter at a focal position of said parabolic concave mirror, said reflection filter acting as a spatial frequency filter. It is the object of the present invention to provide an optical system capable of patterning an optical storage medium with high resolution. The foregoing object is solved according to the invention with an afocal optical system according to claim 1. In the present invention an illumination source projects light through a mask positioned at the object plane of an imaging optical system such as a projection mask aligner. In a typical projection mask aligner of the type disclosed in U.S. Patent Nos. 3,748,015; 4,293,186 and 4,011,011 the pattern of the mask would be projected or imaged on the target, e.g., a wafer or optical disk without change in the image. The number of lines and spaces, on the mask pattern would be reproduced on the optical disk without a change in the period. In normal practice the newest model of the Micralign Model 600 projection mask aligners of the type manufactured by the Perkin-Elmer Corporation of Norwalk, Connecticut is capable of forming high contrast (modulation) images of repetitive patterns such as groups of lines and spaces, concentric circles or spirals with the same mask (Λ m ) and image (Λ i ) period as small as Λm = Λ i = λ/NA = 2.2 um where the Model 600 has a numerical aperatue of NA = 0.167. The wave length is λ = 365 nm. the image can be used to expose a light sensitive coating on a glass disk to meet the specific requirements of an optical disk. This small period approaches the practical limits of photolithography. Repetitive patterns of smaller period, 1.7 to 1.3 um, can be imaged only under ideal conditions because of the low contast image. In addition, the depth of focus is very limited. In the present invention the image differs significantly from the mask pattern: the image period is one half the mask period, i.e., the previous 2.2 um period is imaged as a high contrast 1.1 um period image. In addition this image has a large depth of focus. To carry out this invention means are provided within the optics of the projection system to block out all orders of light diffracted by the mask pattern except for the desired positive and negative first orders. In a practical embodiment the invention comprises an off-axis system comprising a concave and convex mirror arranged to have their centers of curvature coincident or nearly on the optical axis. An illumination source projects light of controlled coherence through a mask disposed at one conjugate to image the pattern at the other conjugate point of the system. Obscuration means are provided at the convex mirror (system pupil)to block all orders of light diffracted by the mask pattern except the two first orders from reaching the target, e.g., the optical disk. This results in an image of the mask pattern having half its period. It should be remembered that in the system described the mask and wafer must be scanned past the annular area of good correction as described, e.g., in U.S. Patent No. 4,011,011 in order to fully expose the optical disk. In another embodiment the optical system is purely refractive, e.g., as in step and repeat projection mask aligner. Here again, obscuration means are used to block all light diffractd by the mask pattern except the first order. In both cases careful selection of parameters are necessary for optimum performance, e.g., illumination, spatial and spectral coherence, object mask pattern and optical imaging system stop should be carefully selected in a coordinated manner. Unequal lines and spaces may be made by the appropriate exposure selection. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 illustrates in schematic form a first embodiment of the present invention utilizing an off axis optical system; and Fig. 2 illustrates in schematic form another embodiment of the present invention utilizing an on axis optical system. DESCRIPTION Referring to Fig. 1 there is shown an off axis afocal optical system 10 comprising concave mirror 11 and convex mirror 12. Concave mirror 11 and convex mirror 12 are arranged so that their centers of curvature are nearly coincident on the optical axis of the system. The mirror surfaces of concave mirror 11 and convex mirror 12 face each other. The radius of curvature of convex mirror 12 is smaller than that of concave mirror 10 so that rays of light from object point 0 are reflected from concave mirror 11 to convex mirror 12 and thence to concave mirror 11 and therefrom to image point I. This arrangement produces a well corrected image of the object within an annular ring concentric to the optical axis which is highly useful in the microlithography art as described in the above mentioned patents. The term "nearly coincident" is used inasmuch as it has been shown that if the centers of curvature are permitted to deviate a little from coincidence, the width of the ring of well corrected imagery is increased and is still within acceptable microlithography standards. By placing obscurations 13 as shown at or on the convex mirror 12 an image of a mask 15a patterned with concentric or spiral circles having a period A placed at the object point and properly illuminated by a source 14 will project an image of the pattern to the image point I having a period ½ A. An optical disk 15b placed at the image point thus would be exposed to a pattern with lines and spaces half the period of those on the mask. Appropriate processing, e.,g. developing and etching will then provide an optical disk having a storage capacity four times that normally possible. The obscurations function as a spatial filter and block all orders of diffracted light through the mask except the two first orders, i.e., the zero order and second and greater orders of light are blocked. This results in the phenomena of halving the period of the lines and spaces projected onto a target disposed at the image plane I. Thus, on processing a photoresist coated glass disk results in an optical disk with double the number of lines and spaces possible through conventional techniques and, thus, allowing up to four times the storage capacity. Table 1 lists the basic system parameters referred to the image. The desired diffracted orders are transmitted through the unobstructed pupil between N₁ and N₂. Table 2 gives the basic relationships for this imaging technique. The relationships must hold for all variables i.e., over all image period ranges and wavelengths used. Fig. 2 illustrates an on axis refractive optical system embodying the concept of the reflective off axis optical system of Fig. 1. The optical system of Fig. 2 comprises a spectrally filtered light source 16 of controlled area (or a laser), collimating lens 17, a mask 18 disposed at the object plane of the system, imaging lenses 19 and 20, and an optical disk 21 disposed at the image plane of the system. The optical disk 21 is coated with a light sensitive material. A spatial filter 22 is disposed between lenses 19 and 20 at the (pupil) focal plane of lens 19. The spatial filter 22 is essentially a stop having an opaque center portion 22a and an opaque outer annular portion 22b which together form an annular opening 22c. The mask 18 is patterned the same as mask 15a of the system of Fig. 1, i.e., with concentric or spiral rings having period Λ m . The pattern may be composed of transparent spaces and opaque lines or of alternating phase differences in an all transparent phase mask or a combination. Upon illumination of the mask 18 its pattern is imaged at the image plane onto optical disk 21. As in the case of the system of Fig. 1 the imaged pattern has a period which is one half that of the mask pattern. Thus, after appropriate processing, e.g., developing and etching the memory capacity of the optical disk 21 is up to four times that ordinarily expected from the mask 18. Other modifications of the invention are possible in light of the above description which should not be interpreted as placing limitations on the invention beyond those set forth in the Claims which follow:

Claims: An afocal optical system for projecting a well corrected ring field off axis image comprising; at least one concave (11) and convex (12) mirror, having their centres of curvature on a common optical axis; a mask (15a) having a pattern formed thereon disposed at a first conjugate point (0) of the system; an illumination source (14) disposed relative to said mask (15a) and said mirrors (11, 12) for imaging the pattern at a second conjugate point (I) of the system characterised in that; the said at least one concave (11) and convex (12) mirror have their centres of curvature nearly coincident on said common optical axis; said mask (15a) has a pattern with concentric or spiral circles having a period; means (13), disposed at said convex mirror (12), for blocking zero order and second and above orders of light caused by diffraction of light by the mask pattern from said illumination source (14); and an optical disk (15b) placed at the second conjugate point (I) whereby the image found at the second conjugate point has a period one-half that of the period of said mask (15a). A system according to claim 1 wherein said circular rings are formed by transparent and opaque areas. A system according to claim 1 wherein said circular rings are formed by alternating phase differences in thickness of an all transparent mask. A system according to claim 3 wherein said means for blocking is a spatial filter.

Inventors: KREUZER JUSTIN L, KREUZER, JUSTIN L.
Applicants: SVG LITHOGRAPHY SYSTEMS INC, SVG LITHOGRAPHY SYSTEMS, INC.
Application year: 1989
Main classification: G03F7
IPC codes: G03F7, G02B17