Abstract
Calculations of $\ensuremath{\alpha}$-particle stopping cross sections based on the theories of Lindhard et al. using the Hartree-Fock-Slater atomic-charge distribution provide generally good agreement with previously obtained experimental results. In particular, the calculations are helpful in understanding the structure which results when, for fixed energy of the $\ensuremath{\alpha}$ particle, the stopping cross section is plotted against the atomic number of the stopping medium.
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