Abstract

The range and straggle of boron in KTFR are measured and found to be in excellent agreement with the theoretical values of Lindhard, Scharff and Schiøtt for projected range, R p , and straggling, Δ R p , (depth of peak and width of assumed Gaussian distribution) if an empirical correction is made to the electronic stopping power using the results of Ormrod and Duckworth. A probable deviation from a Gaussian distribution approximation is found in this experiment for the fraction of ions which penetrate shallowly ( x 《 R p , where x is the depth) but a good fit to the Gaussian assumption is seen for the deeply penetrating ions ( x 《 R p ). From the results, curves are constructed which give the thickness of KTFR necessary to stop a given fraction of incident ions so a photoresist thickness sufficient for masking purposes may be chosen.

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