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- W1990223750 abstract "The total cross section for the single-electron-capture reaction, ${mathrm{H}}^{+}$+ Arensuremath{rightarrow}H+${mathrm{Ar}}^{+}${(Ne)3${mathit{s}}^{1}$3${mathit{p}}^{6}$${;}^{2}$S}, has been measured at energies from 100 to 800 keV. The cross section is tentatively identified with the cross section for capture directly from the 3s single-electron orbital of Ar. A clear indication of a structure in the functional dependence of the cross section on energy is seen. It is suggested that the structure is caused by one of the two radial nodes of the 3s wave function. The cross sections for the simul- taneous charge transfer and ionization reactions, ${mathrm{H}}^{+}$+Arensuremath{rightarrow}${mathrm{H}}^{+}$+${mathrm{Ar}}^{2+}${(Ne)3${mathit{s}}^{1}$3${mathit{p}}^{5}$${;}^{1}$P and $^{3}mathrm{}}$, ${mathrm{H}}^{+}$+Arensuremath{rightarrow}H+${mathrm{Ar}}^{3+}${(Ne)3${mathit{s}}^{1}$3${mathit{p}}^{4}$${;}^{4}$P${,}^{2}$D, and $^{2}$P}, and ${mathrm{H}}^{+}$+Arensuremath{rightarrow}H+${mathrm{Ar}}^{4+}${(Ne)3${mathit{s}}^{1}$3${mathit{p}}^{3}$${;}^{3}$D}, were also measured within the energy region 100--800 keV. The energy dependence of these cross sections is different from that found for the pure single-electron-capture reaction. The reason for this is, most likely, that the transfer and ionization reactions are influenced by electron capture from the L shell, followed by Coster-Kronig and Auger transitions. It is not known at present whether multielectron transitions due to dynamic electron correlation or multiple interactions with the projectile are important for the present collision systems. If so, the interpretation of the reactions will require a more thorough theoretical analysis." @default.
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- W1990223750 date "1991-08-01" @default.
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- W1990223750 title "Electron capture from Ar by fast protons: Capture from theM1subshell" @default.
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- W1990223750 doi "https://doi.org/10.1103/physreva.44.1604" @default.
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