In this page you can find the available values for the electronic stopping power of H ions (in 10-15eV cm2/atom), plotted versus equivalent proton energy. The data reference codes are explained in the list of all data references , and the curve designations in the list of stopping power tables and programs.
At present, data and graphs are available for the following targets (to download all the experimental data for Helium Ions click here):
Ions | Target | Graph | Files | Comments |
He Ions |
Acetylene |
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He Ions |
Ag |
SRIM13 and ICRU49 do not describe the low energy data by Gö13. Change of slope at 3 keV, the velocity constant changes (see Gö13). |
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He Ions |
Air |
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He Ions |
Al, versus v |
For He in Al, stopping is velocity-proportional, but with different slopes in two different regions, indicating charge exchange between He and Al atoms |
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He Ions |
Al |
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He Ions |
Al2O3 |
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He Ions |
Ar |
In agreement with Chu’s and Besenbacher’s measurements, Z03 (SRIM2003) predicts no gas-solid difference. Excellent agreement of Z03 and ICRU 49 with the data |
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He Ions |
Au |
Pe81 data are too high compared to many others |
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He Ions |
Au, versus v |
There is an indication of a stopping threshold similar to the case of H ions in Au. The theory by Zeb12 shows a change of steepness there. |
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He Ions |
B |
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He Ions |
Be |
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He Ions |
Bi |
Good agreement of Z03 with the data |
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He Ions |
Butane |
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He Ions |
C |
Pe81 data are too high compared to many others |
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He Ions |
Ca |
Large discrepancy between Eppacher measurement and Z03 |
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He Ions |
CF4 |
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He Ions |
CO2 |
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He Ions |
CCl4 liquid, vapor |
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He Ions |
Co |
Excellent agreement of Z03 with the data |
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He Ions |
Cr |
The second graph shows the low energy data by Sp98 better; reevaluated Sp98 data are shown by circles (cf. remarks for Mo) |
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He Ions |
Cu |
The second graph shows the low energy data by Sp98 better; reevaluated Sp98 data are shown by circles (cf. remarks for Mo) |
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He Ions |
Cyclohexane liquid, vapor |
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He Ions |
Cyclopropane |
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He Ions |
Dy |
Good agreement of Z03 with most of the data |
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He Ions |
Ethane |
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He Ions |
Ethyl alcohol liquid |
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He Ions |
Ethyl alcohol liquid, vapor |
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He Ions |
Ethylene |
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He Ions |
Fe |
Good agreement of the curves (except for Z99) with most of the data |
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He Ions |
Formvar |
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He Ions |
GaSb |
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He Ions |
Ge |
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He Ions |
H2 |
Good agreement between Z12, ICRU 49 and the data. |
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He Ions |
H2S |
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He Ions |
Havar |
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He Ions |
He |
Excellent agreement between curves and data (except for Hb72) |
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He Ions |
Heptane liquid, vapor |
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He Ions |
Hexane liquid, vapor |
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He Ions |
HfO2 |
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He ions |
Hydroxy apatite |
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He Ions |
InN |
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He Ions |
Kapton, Polyimide |
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He Ions |
KCl, versus v |
The new Mk09 data show an (extrapolated) threshold |
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He Ions |
Kr |
Good agreement of Z03 and ICRU 49 with the data |
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He Ions |
LiF, versus v |
The new Mk09 data show a threshold at v = 0.1 a.u. (250 eV/u) |
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He Ions |
Methane |
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He Ions |
Methyl alcohol liquid, vapor |
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He Ions |
Mg |
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He Ions |
Mo |
The Sp98 data are exceptional in that they go down as far as 0.01 keV (see the second graph). But these values are based on an evaluation of measured ranges for 5 - 100 keV He ions, taking the energy dependence from TRIM 95. We re-evaluated the Sp98 data by a comparison with Monte Carlo ranges from SRIM 2003 (circles). |
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He Ions |
Mylar |
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He Ions |
N2 |
Excellent agreement between curves and the data |
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He Ions |
Nb2O5 |
Excellent agreement between curves and data |
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He Ions |
Ne |
Excellent agreement between curves and data |
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He Ions |
Ni |
Excellent agreement of Z03 with the data above 20 keV. See also remark for Mo. |
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He Ions |
O2 |
Excellent agreement between Z03, ICRU 49 and data |
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He Ions |
Pb |
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He Ions |
Pentane liquid, vapor |
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He Ions |
3-Pentanone vapor |
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He Ions |
Polycarbonate |
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He Ions |
Polypropylene |
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He Ions |
Polystyrene |
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He Ions |
Polysulfone |
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He Ions |
Propane |
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He Ions |
Propyl alcohol vapor |
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He Ions |
Propylene |
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He Ions |
Propylene oxide vapor |
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He Ions |
Pt |
Good agreement between Z03 and the data. At low energy, stopping is proportional to velocity, but the velocity constant changes at 4 keV (Gö13). |
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He Ions |
Se |
Fair agreement of Z03 with the data, except for Co83 |
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He Ions |
SF6 |
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He Ions |
Si |
The ICRU 49 curve appears slightly low at the maximum |
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He Ions |
SiC |
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He Ions |
SiO2 |
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He Ions |
SiO2, versus v |
Contrary to the hydrogen data, the helium data do not show a threshold |
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He Ions |
Sn |
Good agreement of SRIM13 with the data except for Ep94a |
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He Ions |
Ta |
Excellent agreement of Z03 with the data |
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He Ions |
Ta2O5 |
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He Ions |
Ti |
Good agreement of the curves with the data (except for Gt62) |
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He Ions |
TiO2 |
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He Ions |
V |
Excellent agreement of Z03 with the data |
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He Ions |
Vyns |
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He Ions |
W |
Good agreement |
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He Ions |
Water |
GarM09 curve reproduces the data quite well |
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He Ions |
Water |
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He Ions |
Water vapor |
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He Ions |
Xe |
Excellent agreement of Z03 with the data; ICRU 49 fits less well at 2000 keV |
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He Ions |
Y |
Fair agreement of Z03 with the data, except for Ep94a at low energy |
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He Ions |
Zn |
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He Ions |
ZnO |
Only one set of data |
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He Ions |
ZnTe |
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He Ions |
Zr |
Good agreement of Z03 with the scant data |
Click here to see the complete list of data for helium ions available in the files. The list was brought up to date in 2007. In this list, every line corresponds to one data file. The targets are ordered alphabetically. The headings in the list have the following meaning:
M | Mass Number of Projectile |
Eq. Energy | Equivalent Proton Energy, i.e., energy of a proton of equal speed |
Error | Error in percent. "e" means estimate. |
Ref. | Reference Code, see list of all data references |
Meas. |
Number of measurement within the publication (you don’t need that!)/p> |
Method | Method of measurement according to classification by Paul, Semrad and Seilinger, Table 5 |
Ag. | State of aggregation (s: solid; g: gaseous). G: graphite (as opposed to amorphous carbon) |
File | File designation: the file name Al.005, e.g., means file number 5 for hydrogen ions on Al. |
See also: H. Paul, D. Semrad and A. Seilinger, " Reference stopping cross sections for hydrogen and helium ions in selected elements", Nucl. Instr. Methods in Phys. Res. B61 (1991) 261.