1982
DOI: 10.1016/0029-554x(82)90482-7
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Effective charges of ions and the stopping power of dense media

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Cited by 92 publications
(22 citation statements)
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“…was obtained by removing the nuclear stopping power component from their experimental measurements. The analytical model by Heredia-Avalos and co-workers [48] employs the dielectric response formulation using a Mermin-type dielectric function [49] together with a modified Brandt-Kitagawa model [50,51] for the effective charge state of the proton. The dielectric function was obtained by fitting to the experimental spectrum of the energy loss function in the optical limit (q = 0).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…was obtained by removing the nuclear stopping power component from their experimental measurements. The analytical model by Heredia-Avalos and co-workers [48] employs the dielectric response formulation using a Mermin-type dielectric function [49] together with a modified Brandt-Kitagawa model [50,51] for the effective charge state of the proton. The dielectric function was obtained by fitting to the experimental spectrum of the energy loss function in the optical limit (q = 0).…”
Section: Resultsmentioning
confidence: 99%
“…In addition to this mass-density effect, the velocity dependence of the charge state has also been widely studied, and various theoretical descriptions exist in the literature. The commonly used Brandt-Kitagawa theory [50,51], for example, models the charge state as a function of the scaled velocity based on the Thomas-Fermi model. Clearly, an important aspect in applying the linear response theory formalism for calculating stopping power is the question of whether the use of an effective charge for the swift ion can better represents the electronic stopping power curve.…”
Section: Hementioning
confidence: 99%
“…[6][7][8][9][10][11][12] If a SHI with energy E enters a target and its initial charge q init is lower than the mean equilibrium one in the target bulk ͗q͘ ͑can be calculated, e.g., using formulas given in Ref. [6][7][8][9][10][11][12] If a SHI with energy E enters a target and its initial charge q init is lower than the mean equilibrium one in the target bulk ͗q͘ ͑can be calculated, e.g., using formulas given in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…The summation is performed over all the possible charge states q of the projectile, characterized by the Fourier transform ρ q (k) of its electronic density, which is described by the Brandt-Kitagawa model [57,58]. φ q are the equilibrium charge state fractions of the projectile, which depend on its energy and the target nature; we have used in this work a parametrization to experimental data [59].…”
Section: Theoretical Energy Loss Calculationsmentioning
confidence: 99%