Universal fit formula for electronic stopping of all ions in carbon and silicon

Konac, G.; Klatt, Ch.; Kalbitzer, S.

doi:10.1016/s0168-583x(98)00453-4

Cited by 47 publications

(10 citation statements)

References 18 publications

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“…2, along with Konac et al's fit on experimental data [27] and data from the PSTAR database [28]. The results from this work's calculation are close to the published data in the 50 keV-100 MeV range, with less than 10% difference.…”

Section: Incident Protonssupporting

confidence: 81%

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Geant4 physics processes for microdosimetry simulation: Very low energy electromagnetic models for protons and heavy ions in silicon

Valentin

Raine

Gaillardin

et al. 2012

Nuclear Instruments and Methods in Physics Research Section B:

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Section: Incident Protonssupporting

confidence: 81%

“…Calculated proton stopping power (red solid line) compared to the Konac et al's fit on experimental data[27] and to the data from the PSTAR database[28]. (For interpretation of the references to colour in this figure legend, the reader is referred to the web version of this article.…”

mentioning

confidence: 99%

Geant4 physics processes for microdosimetry simulation: Very low energy electromagnetic models for protons and heavy ions in silicon

Valentin

Raine

Gaillardin

et al. 2012

Nuclear Instruments and Methods in Physics Research Section B:

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“…Solid curves indicate the present calculations. The experimental data are shown as letters and the other theoretical calculations are shown as dashed curves TRIM90-TRIM98 [24], KO98 [64]. Figure 3b shows the stopping power for carbon incident on nickel as a function of projectile energies.…”

mentioning

confidence: 99%

Effective stopping charges and stopping power calculations for heavy ions

Gümüş

Köksal

2002

Radiation Effects and Defects in Solids

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In this study the model suggested by Sugiyama has been developed and applied for the calculation of the stopping powers for nonrelativistic heavy ions in various target materials. Sugiyama's model has been expanded to low and high energy regions in our work. Analytical expressions are obtained in the modified BB stopping power formula for the effective charge and effective mean excitation energies. In the modified LSS formula, a quasi-molecule criterion has been applied to both the projectiles and the target atoms. Electronic excitation contribution, S e0 , and quasi-molecule contribution, S ei , to stopping power were found for a wide energy region. It is observed that in intermediate energy region both contributions have maxima. The stopping power due to excitation-ionization in the intermediate and higher energy region is found to be dominant, whereas quasi-molecule contribution is dominant in the lower energy region. The calculated results of stopping power are in good agreement with experimental data for various ions and targets within a few percent in a wide projectile energy range.

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“…In Fig. 5, the electronic energy loss data used in TRIM 98 are compared with those of the corresponding universal stopping power formula proposed by the Heidelberg group [15], which was empirically obtained from data at E > 10 keV/amu. Although these estimates are only validated for energies above 120 keV for carbon, 280 keV for silicon and 400 keV for argon ions, a comparison might be instructive.…”

Section: Openup (July 2007)mentioning

confidence: 99%