Surface Roughness of Thorium in addition to Thorium Oxide in addition to its Effect on Optical Properties in the Extreme Ultraviolet Why the Extreme Ultraviolet Roughness Roughness Characterization of Roughness

Surface Roughness of Thorium in addition to Thorium Oxide in addition to its Effect on Optical Properties in the Extreme Ultraviolet Why the Extreme Ultraviolet Roughness Roughness Characterization of Roughness www.phwiki.com

Surface Roughness of Thorium in addition to Thorium Oxide in addition to its Effect on Optical Properties in the Extreme Ultraviolet Why the Extreme Ultraviolet Roughness Roughness Characterization of Roughness

Nordstrand, Dave, Features Writer has reference to this Academic Journal, PHwiki organized this Journal Surface Roughness of Thorium in addition to Thorium Oxide in addition to its Effect on Optical Properties in the Extreme Ultraviolet Niki Farnsworth R. Steven Turley Why the Extreme Ultraviolet Roughness Why do we care

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Roughness Roughness affects the way a surface reflects. Characterization of Roughness The easiest way to characterize roughness is to measure it directly. ATOMIC FORCE MICROSCOPY Our Data RMS roughness of 4.3 nm over a 1000x1000nm length scale. Peak roughness at horizontal length scales on the order of 50 nm.

Too Good to be True It wouldn’t be interesting physics research if it were this simple. Problem: What happens when the tip size is on the order of the horizontal length scales of our roughness Too Good to be True Now what Do AFM measurements tell us anything about the surface How accurate are the RMS roughnesses it reports How accurate are the power spectral densities it reports

Solution: Model it Different types of rough surfaces Change horizontal length scales Change correlation length Change magnitudes Different types of tips Change tip shape Change tip size Solution: Model it Assumptions: Horizontal length scale = 20 nm. Magnitude is a Gaussian of width 1nm around zero. Tip shape is a parabola. Changing Tip Sizes

Changing Tip Sizes tip width = 10 nm tip width = 15 nm tip width = 20 nm tip width = 30 nm Changing Tip Sizes Changing Tip Sizes

Changing Tip Sizes tip width = 10 nm Changing Tip Sizes tip width = 15 nm Changing Tip Sizes tip width = 20 nm

Changing Tip Sizes tip width = 30 nm Comparing to Our Data dx = 20 nm, tip width = 30 nm Comparing to Our Data The horizontal length scales of our surface roughness are approximately 2/3 the size of our tip. The real RMS roughness of our surface could be up to 2.7 times that measured by the AFM (up to 11.6 nm).

How Does this Affect Reflectance Data Conclusions The discrepancy in the roughness measured by the tip in addition to the actual roughness of the surface could be different by as much as 7.3 nm. Failure to take this difference into account could change our calculated reflectance by up to 35%. This discrepancy could be fatal to our calculation of optical constants as long as that material. Acknowledgements Dr. R. Steven Turley Dr. David D. Allred The BYU Thin Films Group Physics in addition to Astronomy Department Funding Rocky Mountain NASA Space Grant

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