Experimental studies of heavy-ion slowing down in matter
H Geissel, H Weick, C Scheidenberger… - Nuclear Instruments and …, 2002 - Elsevier
Measurements of heavy-ion slowing down in matter differ in many aspects from experiments
with light particles like protons and α-particles. An overview of the special experimental …
with light particles like protons and α-particles. An overview of the special experimental …
C− generation by charge exchange with non-metallic gas for positive ion mass spectrometry
B Cui, S Peng, K Li, T Ma, W Wu, A Zhang, Y Dong… - Vacuum, 2024 - Elsevier
Carbon positive ion mass spectrometry technology (C-PIMS) is a new type of mass
spectrometry technology using the opposite charge exchange process of accelerator mass …
spectrometry technology using the opposite charge exchange process of accelerator mass …
[PDF][PDF] The FLUKA radiation transport code and its use for space problems
A Ferrari, J Ranft, PR Sala - Physica Medica, 2001 - fluka.org
FLUKA is a multiparticle transport code capable of handling hadronic and electromagnetic
showers up to very high energies (100 TeV), widely used for radioprotection and detector …
showers up to very high energies (100 TeV), widely used for radioprotection and detector …
Energy loss and straggling of MeV heavy ions in polypropylene absorber foils
Energy loss and straggling of Li, C and O ions have been measured in varying thicknesses
of polypropylene absorber foils. These measured values have been compared with those …
of polypropylene absorber foils. These measured values have been compared with those …
Energy loss straggling for α-particles in varying thicknesses of Al, Ti and Ni metallic foils
The energy loss straggling for α-particles, in the fractional energy loss limits (ΔE/E)~ 10–
75%, has been measured in varying thicknesses of Aluminum, Titanium and Nickel metallic …
75%, has been measured in varying thicknesses of Aluminum, Titanium and Nickel metallic …
Energy loss straggling of α-particles in Tb, Ta and Au metallic foils
The energy loss straggling of 5.486 MeV α-particles in Tb, Ta and Au metallic foils (varying
thicknesses∼ 4.20–16.00 mg/cm 2) is measured, in the fractional energy loss limits …
thicknesses∼ 4.20–16.00 mg/cm 2) is measured, in the fractional energy loss limits …
[HTML][HTML] Energy loss and straggling of α-particles in Ag and Sn metallic foils
Energy loss and straggling in Ag and Sn metallic foils for α-particles, using 241 Am source,
are measured. The measured energy loss values are compared with the predicted values …
are measured. The measured energy loss values are compared with the predicted values …
Heavy ion energy loss straggling data from time of flight stopping force measurements
M Msimanga, CA Pineda-Vargas, CM Comrie… - Nuclear Instruments and …, 2012 - Elsevier
The accuracy of heavy ion beam analytical techniques such as Heavy Ion-Elastic Recoil
Detection Analysis (HI-ERDA) depends on, among other factors, the accuracy of basic ion …
Detection Analysis (HI-ERDA) depends on, among other factors, the accuracy of basic ion …
Stopping of 236 keV–3.019 MeV protons in mylar and polypropylene films
S Damache, S Ouichaoui, A Belhout, A Medouni… - Nuclear Instruments and …, 2004 - Elsevier
The stopping powers of polypropylene and mylar polymers for protons have been accurately
measured over the energy intervals Ep=(0.352–3.009) MeV and Ep=(0.236–3.019) MeV …
measured over the energy intervals Ep=(0.352–3.009) MeV and Ep=(0.236–3.019) MeV …
Energy loss straggling of Li, C and O ions in mylar and polycarbonate absorber foils
Measurements of energy loss straggling for Li, C and O ions in varying thicknesses of mylar
(C10H8O4) and polycarbonate (C16H14O3) absorber foils in the energy range∼ 3.0–6.0 …
(C10H8O4) and polycarbonate (C16H14O3) absorber foils in the energy range∼ 3.0–6.0 …