1984
DOI: 10.1139/p84-089
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Mean excitation energies for stopping powers in various materials composed of elements hydrogen through argon

Abstract: The basic model of Lindhard and Scharff, known as the local plasma model, is utilized to study the effects of the chemical and physical state of the medium on its stopping power. Unlike previous work with the local plasma model, in which individual electron shifts in the plasma frequency were estimated empirically, the Pines correction derived for a degenerate Fermi gas is shown herein to provide a reasonable estimate even on the atomic scale. Thus, the model is moved to a completely theoretical base requiri… Show more

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Cited by 6 publications
(1 citation statement)
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“…Some of these theoretical models such as the MOCA14 (Wilson et al 1984; Charlton et al 1985) and PITS (Stewart et al 2002; Mainardi et al 2004) codes, consider the stochastics of ion tracks in evaluating frequency distributions, but have been limited to dealing with maximum energies of 5 MeV amu −1 and have not been extended to high atomic number and energy ions. A deterministic model of frequency distributions for total energy deposited in small volumes similar to DNA molecules from high-energy ions of interest for cancer therapy and other applications has been developed (Cucinotta and Dicello 2000).…”
Section: Particle Physicsmentioning
confidence: 99%
“…Some of these theoretical models such as the MOCA14 (Wilson et al 1984; Charlton et al 1985) and PITS (Stewart et al 2002; Mainardi et al 2004) codes, consider the stochastics of ion tracks in evaluating frequency distributions, but have been limited to dealing with maximum energies of 5 MeV amu −1 and have not been extended to high atomic number and energy ions. A deterministic model of frequency distributions for total energy deposited in small volumes similar to DNA molecules from high-energy ions of interest for cancer therapy and other applications has been developed (Cucinotta and Dicello 2000).…”
Section: Particle Physicsmentioning
confidence: 99%