Stopping powers of gases for very heavy ions
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Cited by (15)
Accurate simultaneous lead stopping power and charge-state measurements in gases and solids: Benchmark data for basic atomic theory and nuclear applications
2023, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsZ<inf>2</inf> structure and gas-solid effect in the stopping of slow ions
2007, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsGas-solid effect in mean charge and slowing down of uranium ions at 60.2 and 200 MeV/u
2006, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Here we see a gas–solid effect for the lighter materials and no effect for the heavier. This is in contrast to previous experiments [2,3]. One has to note that the experimental stopping cross sections are non-equilibrium stopping cross sections.
Empirical stopping power tables for ions from <inf>3</inf>Li to <inf>18</inf>Ar and from 0.001 to 1000 MeV/nucleon in solids and gases
2003, Atomic Data and Nuclear Data TablesExperimental studies of heavy-ion slowing down in matter
2002, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsAn empirical approach to the stopping power of solids and gases for ions from <inf>3</inf>Li to <inf>18</inf>Ar
2001, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :This is also seen as an increased “effective charge” for H2 and He in Fig. 7 of [30]. It has been explained [31] as due to the fact that electron capture by the projectile becomes inhibited (and, hence, the ionic charge becomes enhanced) when the projectile velocity exceeds that of the fastest target electron. In the following, we treat solid and gaseous targets separately.4
Work performed at the GANIL national facility, Caen, France.
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