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Asymmetric fluid-structure dynamics in nanoscale imprint lithography

Asymmetric fluid-structure dynamics in nanoscale imprint lithography

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when measur<strong>in</strong>g th<strong>in</strong> layers <strong>in</strong> the range of about 300 to 400 nm. Figure 6.15illustrates the case when a false peak masks the true peak. The differencebetween 6.14a and 6.14b is that the number of zeros used to pad the FFT has been<strong>in</strong>creased by a power of two. This stretches the FFT out and the spectral leakageis <strong>in</strong>creased, however, note that the <strong>in</strong>dex at the maximum of the FFT has nowbeen approximately doubled. Spectral leakage is the smear<strong>in</strong>g of energy acrossthe FFT doma<strong>in</strong>, which results <strong>in</strong> wider peaks. This doubles the resolution s<strong>in</strong>ce apeak at an FFT <strong>in</strong>dex of 200.5, which cannot be resolved <strong>in</strong> 6.14a, is now equal toa peak at an FFT <strong>in</strong>dex of 401 <strong>in</strong> 6.14b, for example.y g18magnitude of the FFT1614121086False peakTrue peak4200 1000 2000 3000 4000 5000 6000 7000 8000 9000FFT <strong>in</strong>dexFigure 6.15 False signal mask<strong>in</strong>g the true signal <strong>in</strong> FFT6.5.3 Template/Substrate DeformationThe template and substrate can be deformed when us<strong>in</strong>g setscrews toconstra<strong>in</strong> their positions. The setscrews cause local stress concentrations that areundesirable. This leads to possible bow<strong>in</strong>g of the template and substrate. Tom<strong>in</strong>imize the effect of stress concentrations on the bow<strong>in</strong>g of the template andsubstrate, flat alum<strong>in</strong>um plates were placed between the setscrews and the quartzpieces.98

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