Method for fine-line interferometric lithography

In microelectronic processing, the method of producing complex, two-dimensional patterns on a photosensitive layer with dimensions in the extreme submicron range. A photosensitive layer is first exposed to two beams of coherent radiation to form an image of a first interference pattern on the surface of the layer. The layer is subsequently exposed to one or more interference pattern(s) that differ from the first interference pattern in some way, such as by varying the incident angle of the beams, the optical intensity, the periodicity, rotational orientation, translational position, by using complex amplitude or phase masks in one or both of the coherent beams, or a combination of the above. Desired regions of the complex pattern thus produced are isolated with a further exposure of the photosensitive layer using any conventional lithography.

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Claims

1. In microelectronic processing, the method of producing a two-dimensional complex pattern on a photosensitive layer said pattern containing structures with dimensions in the extreme submicron range, comprising the steps of:

a) exposing the photosensitive layer for a first time to two beams of coherent radiation which form an image of a first interference pattern on the surface of said layer;
b) exposing the photosensitive layer for at least one subsequent time to two beams of coherent radiation which form an image of at least one subsequent interference pattern, such that said subsequent interference pattern or patterns referenced to the photosensitive layer are each different from the first pattern;
c) isolating desired regions of said complex pattern with a further exposure of the photosensitive layer using any conventional lithography.

2. The method of claim 1 wherein the photosensitive layer is rotated between exposures such that each subsequent interference pattern differs in rotational orientation relative to said first interference pattern.

3. The method of claim 1 wherein the photosensitive layer is translated between exposures such that each subsequent interfere pattern is offset from said first interference pattern.

4. The method of claim 1 wherein the photosensitive layer is both rotated and translated between exposures such that each subsequent interference pattern different from said first interference pattern in both rotational orientation and in translational position.

5. The method of claim 1 wherein at least one of said beams of the second or subsequent exposures of the photosensitive layer is varied in amplitude such that each subsequent interference pattern differs from said first interference pattern.

6. The method of claim 1 wherein at least one of said beams of the second or subsequent exposures of the photosensitive layer is varied in phase such that each subsequent interference pattern differs from said first interference pattern.

7. The method of claim 1 wherein at least one of said beams of the second or subsequent exposures of the photosensitive layer is varied in phase and amplitude such that each subsequent interference pattern differs from said first interference pattern.

8. The method of claim 1 wherein the periodicity of the interference pattern of at least one said second or subsequent exposures of the photosensitive layer is varied such that each subsequent interference pattern differs from said first interference pattern.

9. In microelectronic processing, the method of producing a single isolated line of extreme submicron dimensions on a photosensitive layer comprising the steps of:

a) exposing the photosensitive layer for a first time to two beams of coherent radiation such that an image of an interference pattern is formed on said layer;
b) isolating a portion of a single line within said interference pattern by a second exposure of the photosensitive layer using conventional optical lithography.

10. In microelectronic processing, a method of producing interdigitated structures on a photosensitive layer, comprising the steps of:

a) exposing a defined area of the photosensitive layer with a first interference pattern, having a period p1, said defined area being bounded by two side edges approximately parallel to the lines of constant exposure dose and by top and bottom edges approximately perpendicular to the lines of constant exposure dose;
b) exposing a second defined area containing the top edge of the first defined area with a second interference pattern of period p2 equal to twice p1 and with lines of constant exposure parallel to those of the first interference pattern, said second interference pattern being positioned relative to the first interference pattern such that every other unexposed region of the first exposure pattern within the second defined area is exposed;
c) exposing a third defined area containing the bottom edge of the first defined area with a third interference pattern of period p2 equal to twice p1 and with lines of constant exposure parallel to those of the first interference pattern, said third interference pattern being positioned relative to the first and second interference patterns such that every other unexposed region of the first exposure pattern within the third defined area is exposed, said unexposed regions being connected to unexposed regions alternate to those exposed in step b.

11. The method of claim 10 wherein the second and third exposures of steps b and c are replaced by a single second exposure of period p2 equal to twice p1 and with lines of constant exposure parallel to those of the first interference pattern, and further, in which both interfering beams of the second exposure pass through a mask with two transparent holes that map the second exposure into two areas at the photosensitive layer containing said top edge and said bottom edge, respectively, there further being a net phase shift of 1/2 period between the two resulting interference patterns at the photosensitive layer caused by optical path length differences in the transparent mask areas, said interference patterns being disposed to simultaneously expose every other unexposed region of said first exposure within the illuminated areas..Iadd.

12. An apparatus for producing a two-dimensional complex pattern on a photosensitive layer, said pattern containing structures with dimensions in the extreme submicron range, comprising:

a movable table;
a wafer positioned on said movable table, said wafer having a surface; and,
a source of coherent radiation which forms subsequent images of interference patterns on said surface of said wafer, said source providing at least two beam paths, said radiation having an amplitude, phase, angle, intensity and periodicity..Iaddend..Iadd.13. The apparatus of claim 12, wherein said table communicates with a means for rotation and a means for translation..Iaddend..Iadd.14. The apparatus of claim 12, wherein said

wafer has a photosensitive layer and a substrate..Iaddend..Iadd.15. The apparatus of claim 12, wherein said source has a means for varying the amplitude of said radiation, a means for varying the phase of said radiation, a means for varying the angle of said radiation, a means for varying the optical intensity of said radiation and a means for varying the periodicity of said interference pattern..Iaddend..Iadd.16. The apparatus of claim 12, further comprising a means for dividing said coherent radiation into said beam paths, each of said beam paths having coherent radiation of essentially equal intensity at said wafer, thereby assuring a high contrast exposure..Iaddend..Iadd.17. The apparatus of claim 12, further comprising a phase-amplitude mask, said mask

intercepting at least one of said beam paths..Iaddend..Iadd.18. A method for producing a two-dimensional complex pattern on a photosensitive layer, with dimensions in the extreme submicron range, in a stepwise manner by reducing the field aperture to increase the source coherence..Iaddend.

Referenced Cited
U.S. Patent Documents
3591252 July 1971 Lu
4375315 March 1, 1983 Lacombat
4402571 September 6, 1983 Cowan
4796038 January 3, 1989 Allen
4859548 August 22, 1989 Heise
4997747 March 5, 1991 Yoshida
5142132 August 25, 1992 Macdonald
5208123 May 4, 1993 Ramsbottom
5448332 September 5, 1995 Sakakibara
Other references
  • Zhou: "Precise Periodicity Control in the Fabrication of Holographic Gratings" in Appl. Optics,20(8), Apr. 1981, pp. 1270-1272.
Patent History
Patent number: RE35930
Type: Grant
Filed: Apr 22, 1996
Date of Patent: Oct 20, 1998
Assignee: the University of New Mexico (Albuquerque, NM)
Inventors: Steven R. J. Brueck (Albuquerque, NM), Saleem Zaidi (Albuquerque, NM), An-Shyang Chu (Albuquerque, NM)
Primary Examiner: Kathleen Duda
Law Firm: Snell & Wilmer L.L.P.
Application Number: 8/635,565