In the present work, we report experimental results of He stopping power into Al2O3 films by using both transmission and Rutherford backscattering techniques. We have performed measurements along a wide energy range, from 60 to 3000 key, covering the maximum stopping range. The results of this work are compared with previously published dap-, showing a good agreement for the high-energy range, but evidencing discrepancies in the low-energy region. The existing theories follow the same tendency: good theoretical-experimental agreement for higher energies, but they failed to reproduce previous and present results in the low energy regime. On the other hand it is interesting to note that the semi-empirical SRIM code reproduces quite well the p...
The electronic stopping power, S, of HfO2 films for proton and alpha particle beams has been measure...
AbstractThe p¯ stopping power in helium from 1 keV kinetic energy is evaluated. Contrary to the effe...
The stopping powers of CaF2 and MoO3 for O-16 and F-19 were measured with heavy-substrate Rutherford...
In the present work, we report experimental results of He stopping power into Al2O3 films by using b...
The electronic stopping cross section (SCS) of Al2O3 for proton beams is studied both experimentally...
The electronic stopping cross section (SCS) of Al2O3 for proton beams is studied both experimentally...
The energy-loss straggling of zirconia (ZrO2) and alumina (Al2O3) has been experimentally determined...
Includes bibliographical references (leaves 61-63)Stopping, powers Tor 20-1 50 keV hydrogen and heli...
We report the results of an experimental-theoretical study on the stopping power of ZrO2 films for s...
Stopping powers of Al film for Si ions (0.8-6.4 MeV) have been measured with Rutherford backscatteri...
The electronic stopping power, S, of HfO₂ films for proton and alpha particle beams has been measure...
The stopping cross section, ε, of light ions in solids determines the accuracy of depth distribution...
Abstract. Stopping cross sections of TiO2 films were measured for H and He ions in the energy interv...
Stopping cross sections of TiO2 films were measured for H and He ions in the energy intervals200−150...
none46noThe stopping power in helium from 1 keV kinetic energy is evaluated. Contrary to the effect...
The electronic stopping power, S, of HfO2 films for proton and alpha particle beams has been measure...
AbstractThe p¯ stopping power in helium from 1 keV kinetic energy is evaluated. Contrary to the effe...
The stopping powers of CaF2 and MoO3 for O-16 and F-19 were measured with heavy-substrate Rutherford...
In the present work, we report experimental results of He stopping power into Al2O3 films by using b...
The electronic stopping cross section (SCS) of Al2O3 for proton beams is studied both experimentally...
The electronic stopping cross section (SCS) of Al2O3 for proton beams is studied both experimentally...
The energy-loss straggling of zirconia (ZrO2) and alumina (Al2O3) has been experimentally determined...
Includes bibliographical references (leaves 61-63)Stopping, powers Tor 20-1 50 keV hydrogen and heli...
We report the results of an experimental-theoretical study on the stopping power of ZrO2 films for s...
Stopping powers of Al film for Si ions (0.8-6.4 MeV) have been measured with Rutherford backscatteri...
The electronic stopping power, S, of HfO₂ films for proton and alpha particle beams has been measure...
The stopping cross section, ε, of light ions in solids determines the accuracy of depth distribution...
Abstract. Stopping cross sections of TiO2 films were measured for H and He ions in the energy interv...
Stopping cross sections of TiO2 films were measured for H and He ions in the energy intervals200−150...
none46noThe stopping power in helium from 1 keV kinetic energy is evaluated. Contrary to the effect...
The electronic stopping power, S, of HfO2 films for proton and alpha particle beams has been measure...
AbstractThe p¯ stopping power in helium from 1 keV kinetic energy is evaluated. Contrary to the effe...
The stopping powers of CaF2 and MoO3 for O-16 and F-19 were measured with heavy-substrate Rutherford...