Abstract
The ranges of ThC" α-recoil
atoms have been redetermined at pressures of hydrogen, argon, and air from 10-3
to 30 mm, by collection on a silver plate mounted 3 mm from a platinum source
plate. The collector was maintained at a positive potential of 300 V to prevent
collection of ions which migrate by diffusion. A similar method is used for
RaA, with a (gaseous) radon source.
Previous work is critically discussed in
terms of the corrections necessary to allow for (i) geometrical features, and
(ii) range straggling. Values of the mean range calculated both from previous
work and from the present work are plotted against the recoil energy. Both the
Fl�gge-Zimens recoil-range equation and the stopping power equation are shown
to be unsatisfactory, and to rest on arguments which are subject to serious
objection on both experimental and theoretical grounds. The recent Bohr
treatment of collisions between recoil atoms and gaseous atoms is In much
better agreement with the unobjectionable experimental data available.
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