Stopping powers of gases for heavy ions (O, Ar, Kr, Xe) at intermediate energy (20–100 MeV/u). Vanishing of the gas—solid effect☆
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Measurement of the stopping power for <sup>16</sup>O in <sup>4</sup>He gas
2016, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsThe stopping powers and energy straggling of heavy ions in polymer foils
2014, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :The CAB model becomes less accurate when the significant effect of the physical state of the investigated materials is expected, which is not our case, we are not studying gaseous targets or targets containing heavier constituents. As an indication, it has been observed in previous experiments that for light ions values of stopping powers are up to 20% larger in vapour than in the solid phase, whereas for heavier ions the opposite has been reported, that is, values of the stopping powers are then up to 20% lower in gases than in solids [14–17]. The program MSTAR [18] was used for stopping power predictions and a model of calculation Bragg's rule is included in this simulation.
A new stopping power parameterization for 0.1-15 MeV/nucleon heavy and superheavy ions in solids and gases
2010, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsEnergy loss of energetic <sup>40</sup>Ar, <sup>84</sup>Kr, <sup>197</sup>Au and <sup>238</sup>U ions in mylar, aluminum and isobutane
2010, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
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Experiment performed at the GANIL National Facility in Caen (France).