Suppressing Ghost Diffraction in E-Beam-Written Gratings
- Created on Friday, 01 May 2009
The degree of periodicity of stitching errors is reduced.
A modified scheme for electron-beam (E-beam) writing used in the fabrication of convex or concave diffraction gratings makes it possible to suppress the ghost diffraction heretofore exhibited by such gratings. Ghost diffraction is a spurious component of diffraction caused by a spurious component of grating periodicity as described below. The ghost diffraction orders appear between the main diffraction orders and are typically more intense than is the diffuse scattering from the grating. At such high intensity, ghost diffraction is the dominant source of degradation of grating performance.
The pattern of a convex or concave grating is established by electron- beam writing in a resist material coating a substrate that has the desired convex or concave shape. Unfortunately, as a result of the characteristics of electrostatic deflectors used to control the electron beam, it is possible to expose only a small field — typically between 0.5 and 1.0 mm wide — at a given fixed position of the electron gun relative to the substrate. To make a grating larger than the field size, it is necessary to move the substrate to make it possible to write fields centered at different positions, so that the larger area is synthesized by “stitching” the exposed fields.
Even though the mechanical stage used to position the substrate can be very accurate (positioning error of ≈ 20 nm or less), field-stitching errors occur, causing underexposures or overexposures that manifest themselves, after development of the resist, as increases or decreases in grating thickness along the field boundaries. Because all the fields are of the same size, the stitching errors form another grating that has a period equal to the field size. Hence, the light scattered from the field boundaries adds coherently: this is ghost diffraction.
The modified scheme for electron-beam writing is based on the concept of reducing the degree of periodicity of the stitching errors. In this scheme, the overall grating area is divided into sub-areas within which the grating patterns are written in differently sized fields. For a typical convex or concave grating, the sub-areas are most easily defined as annular areas that correspond to equal-height slices through the substrate (see figure). Hence, the grating pattern in each annulus is written with a different field size.
The ghost order intensities are proportional to the square of the scattering amplitudes. Hence, if N different field sizes are used, the intensity of ghost diffraction can be expected to be reduced to approximately N–2 times the intensity obtained with a single field size.
To test this concept, two nominally identical gratings were fabricated. The pattern of the first grating was written by stitching together fields of the same size over its entire area, while the pattern of the second grating was established by use of four different field sizes. Whereas the ghost diffraction from the first grating was clearly noticeable, the intensity of ghost diffraction from the second grating was so low as to be undetectable against the diffuse-scattering background.
This work was done by Daniel Wilson and Johan Backlund of Caltech for NASA’s Jet Propulsion Laboratory.
In accordance with Public Law 96-517, the contractor has elected to retain title to this invention. Inquiries concerning rights for its commercial use should be addressed to:
Innovative Technology Assets Management
Mail Stop 202-233
4800 Oak Grove Drive
Pasadena, CA 91109-8099
Refer to NPO-41302, volume and number of this NASA Tech Briefs issue, and the page number.
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