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Asymmetric fluid-structure dynamics in nanoscale imprint lithography

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

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Figure 6.6 shows that the force due to the squeeze film pressure follow thesame trend for the simulation and the experiments. The maximum force <strong>in</strong> theexperimental data was 1.75 lbs. The maximum force <strong>in</strong> the simulation was 1.35lbs. The relative difference between the two results is 23%, which is quitesignificant. This discrepancy could be due to several possibilities.First, compliance estimates for the mechanical system contribute todifference <strong>in</strong> the actual and expected forces. In the actual setup, there are certa<strong>in</strong>compliances that are not modeled, for example, the substrate is modeled as rigid,however, the chuck, which holds the chromium substrate has compliance.Second, there existed some topography due to macroscopic scratches on thechromium substrate. S<strong>in</strong>ce chromium is a fairly soft material, ma<strong>in</strong>ta<strong>in</strong><strong>in</strong>g aclean, flat surface was extremely difficult. The third cause relates to the previous<strong>in</strong> that there were particles observed on the substrate and template surfaces underthe magnification of a microscope. These particles could not be elim<strong>in</strong>ated due tohandl<strong>in</strong>g of these components. The comb<strong>in</strong>ed effects of all these factors are notfully understood and more research is needed <strong>in</strong> this area.4000380036003400film thickness, nm32003000280026002400220020000 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1time, sFigure 6.7 Average film thicknesses from simulation results (solid l<strong>in</strong>e) andexperimental results (circles). Correlation set.88

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