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Stopping Cross Sections of Some Hydrocarbon Gases for 40-250 keV Protons and Helium Ions
74
Citations
13
References
1963
Year
Heavy Ion PhysicHydrocarbon GasesExperimental Nuclear PhysicsNuclear PhysicsPhysicsCross SectionsNatural SciencesEngineeringParticle PhysicsHigh-energy Nuclear ReactionGas DynamicAtomic PhysicsLepton-nucleon ScatteringChemistryStopping Cross SectionsIncident ProtonsNuclear Astrophysics40-250 Kev Protons
The stopping cross sections of air, He, C${\mathrm{H}}_{4}$, ${\mathrm{C}}_{2}$${\mathrm{H}}_{2}$, ${\mathrm{C}}_{2}$${\mathrm{H}}_{4}$, ${\mathrm{C}}_{3}$${\mathrm{H}}_{8}$, ${(\mathrm{C}{\mathrm{H}}_{2})}_{3}$, and ${\mathrm{C}}_{3}$${\mathrm{H}}_{6}$ have been measured for protons in the energy range 40 to 250 keV. The stopping cross sections of ${\mathrm{C}}_{2}$${\mathrm{H}}_{4}$ and ${\mathrm{C}}_{3}$${\mathrm{H}}_{8}$ were also measured for helium ions. The data are in good agreement with previous experimental work, and have standard deviations between 1.5 and 4%. They clearly demonstrate the failure of the Bragg rule of additivity for proton energies less than 150 keV. The helium-ion data indicate that the effect of chemical binding on stopping cross sections is unlikely to be any greater for incident helium ions than for incident protons at the same energy.
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