1. Field of the Invention
This invention relates to the field of electron beam lithography and more specifically to a method of correcting for proximity effects in exposure patterns.
2. Description of the Related Art
In the field of electron beam lithography it is necessary to correct for the background dose effect of back scattered electrons. The pattern in the electron-sensitive resist is defined by the dose of the finely focussed incident electron beam at the various points of the pattern on the surface. Most of the electrons pass into the bulk of the substrate and scatter. A fraction of the scattered electrons come back to the surface and exit. As they exit they also provide a background dose to parts of the pattern that are distant from the incident beam. At any given point, the cumulative effect of this background, from all the other points that receive an incident dose, can create an improper exposure. The resist will not develop properly and shapes will have the wrong dimensions. The only methods available for compensation are to change the incident dose (current per area) or to modify the shape dimensions. This is proximity effect correction or PEC. The correction depends upon the dose given the other shapes or points in proximity to the point being corrected.
The traditional PEC takes into account the actual shapes in the pattern (which includes their density and critical dimensions) and the range of the back scattered electrons. The background dose from back scattered electrons decreases exponentially from the primary beam. This exponential dependence is best determined empirically. It increases with the incident electron energy and is inversely related to the atomic number of the substrate. Most early electron beam patterning systems used relatively low electron beam energy, for example 10 keV. The backscatter range was the same order as the patterns being reproduced, with shapes 1 .mu.m or larger. In this case the background dose varies from the interior to the exterior edges of each shape. To achieve proper exposure Jones, U.S. Pat. No. 4,520,269, and Meiri et al., U.S. Pat. No. 5,313,068, show how to divide the shapes into smaller features so that the edges can be given a higher dose than the interiors. The purpose is to get the dose correct at the edge so as to achieve the proper position of the developed resist.
Most of the PEC methods apply Mihir Parikh's method of self-consistency (M. Parikh, J. Appl. Phys. 50(6) June 1979 p. 4371). This method requires the following
Desired dose (K)=Incident Dose (C)+Backscatter (S)
or EQU K=C+S
to be achieved. The desired dose gives the proper resist exposure. It is found by process experiments. The incident dose is the only parameter under direct control. The backscatter dose must be calculated by integrating all the incident doses at proximal points, taking into account the exponential decrease of the backscatter dose with distance. After the backscatter is calculated, the incident dose is changed to achieve the desired dose. Unfortunately, this changes the backscatter calculation. Thus, iterative calculations must be performed until the incident dose changes insignificantly with each iteration. There has been much work and invention to achieve this calculation. Watson, U.S. Pat. No. 5,736,281, changed a factor so that the equation became EQU K=1/2C+S
This change improves the exposure of isolated shapes where the backscatter dose is very low.
The precalculated doses are best applied to vector or vector/shaped electron beam systems that allow dose variations with each shape, or subdivision of a shape, written. Raster scan systems such as the Etec Systems MEBES can not achieve these graded levels of exposure. Each pixel is either on or off during a single pass. Thus the incident dose can not be modulated over a range of values for each pixel. Four overlaying passes of the raster can be used to write the pattern while turning on or off individual pixels to achieve pixel doses of 0, 0.25, 0.50, 0.75, or 1.0 (S. Ma, M. Parikh, and W. Ward, J. Vac. Sci. 19(4), Nov/Dec 1981 p. 1275). Four passes reduce the throughput to 25%, a significant disadvantage. This coarse five-level control is often insufficient for PEC.
The GHOST method can also be applied with raster scan (G. Owen, P. Rissman, and M. Long, J. Vac. Sci. B3 (1) Jan/Feb 1985, p. 153). The GHOST method requires two passes, for a throughput cut in half. It works by making the background dose uniform throughout the pattern. This means that an isolated shape, that would have had low background and therefore high contrast, ends up with lowered contrast. Such isolated shapes could be the most critical and are thus degraded.
The concept of making the backscatter background dose more uniform is partially achieved by employing electron beam energies above 50 keV. The backscatter exponential range is then greater than 10 .mu.m, much larger than the pattern shapes that are much less than 1 .mu.m. Thus the PEC does not vary within a shape and the shape partitioning of Meiri et al., U.S. Pat. No. 5,313,068, is not necessary. This is recognized in Ashton et al., U.S. Pat. No. 5,051,598, which used a coarse grid (greater than the shapes) to calculate PEC. Several adjacent shapes within the grid could have the same correction.
None of these PEC techniques seek to reduce the backscatter dose background when large or densely packed shapes exist near shapes with fine features. At high beam energy, the dose in the center of the large or densely packed shapes contributes background to the fine shapes that may be 1 to 5 .mu.m distant. This lowers the contrast for the shapes with fine features and decreases process latitude. A large process latitude is highly desirable for the use of electron beam lithography processes in industry, for example the semiconductor industry. Therefore, there is a need for PEC techniques that can offer an improvement in process latitude, preferably without impacting throughput.
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