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Charge Exchange Cross Sections of Hydrogen Particles in Gases at High Energies
202
Citations
13
References
1958
Year
Cross SectionEngineeringNuclear PhysicsElectron LossChemistryHydrogen ParticlesElectron PhysicHeavy Ion PhysicCross SectionsElectron SpectroscopyPlasma SimulationIon EmissionHigh-energy Nuclear ReactionPhysicsAtomic PhysicsHydrogenParticle Beam PhysicsHydrogen TransitionNatural SciencesProton TransferApplied PhysicsHigh Energies
Measurements are reported of the cross section for electron loss (${\ensuremath{\sigma}}_{01}$) and electron capture (${\ensuremath{\sigma}}_{10}$) for hydrogen atoms and ions traversing gases of hydrogen, helium, nitrogen, and argon. The kinetic energy of the particles was from 250 kev-1 Mev. Cross sections for electron loss were determined by measuring the attenuation of a neutral monatomic hydrogen beam in a gas cell in which a transverse electric field was present. The cross section for electron capture was measured by determining the fraction of the beam in each charge state after passing through a "thick" gas target. The fraction of the neutral component to the charge-one component is equal to the ratio of the cross sections for electron capture to electron loss. The velocity dependence of the cross section does not follow a strict power law. In hydrogen the cross section decreases approximately as ${v}^{\ensuremath{-}10}$, while for heavier target gases the velocity dependence is smaller, being ${v}^{\ensuremath{-}3.7}$ for argon at energies greater than 500 kev. The electron loss cross section has a $\frac{1}{{v}^{2}}$ dependence for gases of hydrogen and helium and a $\frac{1}{v}$ dependence for nitrogen and argon target gases.
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