The energy loss associated with the passage of typical heavy ions through various gases has been measured as a function of gas thickness. The ions enter an absorber cell with initial energies of about 10 MeV/amu, held fixed by a magnetic analyzer; the final energy of the ions is determined by analyzing the emergent beam with a magnetic spectrograph. Range-energy curves are obtained for He, C, and Ar ions in H₂, N₂, and Ar and for C ions in CH₄ and He. Over-all accuracy is about 1%. The mean ionization potentials of H₂, N₂, and Ar are determined to be 18.3±{}2.6, 79±{}7, and 190±{}17 eV, respectively. From the stopping power for C and Ar ions relative to that for He ions, their fractional effective charge is computed. Plots of the square of the fractional effective charge as a function of the ratio of the velocity of an ion to that of its own first K electron are in agreement with similar plots for heavy ions in aluminum and oxygen, with one exception, the case of Ar ions in H₂.
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Martin et al. (1962) studied this question.