1997
DOI: 10.1088/0953-4075/30/23/012
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Excitation of autoionizing states of helium by 100 keV proton impact: theory and experiment

Abstract: A joint theoretical and experimental study of the excitation of the autoionizing (2s 2 ) 1 S, (2p 2 ) 1 D and (2s2p) 1 P states of helium by 100 keV proton impact is presented for the first time. The role of the three-body Coulomb interaction in the final state between the ejected electron, the scattered proton and the recoil helium ion is emphasized. Calculations have been carried out with inclusion of the three-body Coulomb interaction and within an expansion of a two-electron excitation amplitude in powers … Show more

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Cited by 25 publications
(70 citation statements)
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“…Therefore, comparing the calculation results for two-electron excitation with available experimental data (electron spectra or resonance parameters) requires not only an adequate theoretical description of the double excitation itself, but also a realistic description of the direct ionization, including the interference of resonant and direct ionization. Moreover, Coulomb interaction in the final state (CIFS) between the scattered charged particle, the ejected electron, and the recoil ion considerably influences the resonance profiles [5][6][7][8]. Under the conditions of strong CIFS the shapes of the resonant lines can be very different from the familiar Fano's one [5,7] complicating the comparison of experimental and theoretical results, and hence the description of three-body Coulomb interaction of charged particles must be as accurate as the description of twoelectron excitation [8].…”
mentioning
confidence: 99%
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“…Therefore, comparing the calculation results for two-electron excitation with available experimental data (electron spectra or resonance parameters) requires not only an adequate theoretical description of the double excitation itself, but also a realistic description of the direct ionization, including the interference of resonant and direct ionization. Moreover, Coulomb interaction in the final state (CIFS) between the scattered charged particle, the ejected electron, and the recoil ion considerably influences the resonance profiles [5][6][7][8]. Under the conditions of strong CIFS the shapes of the resonant lines can be very different from the familiar Fano's one [5,7] complicating the comparison of experimental and theoretical results, and hence the description of three-body Coulomb interaction of charged particles must be as accurate as the description of twoelectron excitation [8].…”
mentioning
confidence: 99%
“…Moreover, Coulomb interaction in the final state (CIFS) between the scattered charged particle, the ejected electron, and the recoil ion considerably influences the resonance profiles [5][6][7][8]. Under the conditions of strong CIFS the shapes of the resonant lines can be very different from the familiar Fano's one [5,7] complicating the comparison of experimental and theoretical results, and hence the description of three-body Coulomb interaction of charged particles must be as accurate as the description of twoelectron excitation [8]. The theoretical excitation cross sections reported in this paper are part of our complete calculation [8] where all these problems are solved.…”
mentioning
confidence: 99%
“…The role of the three-body Coulomb interaction in the ¢nal state between the ejected electron, the scattered proton, and the recoil helium ion is emphasized. 165 Mutual neutralization rates for H 3 O (H 2 O) n 0^3 OH À (H 2 O) m 0^3 have been determined using a new type of apparatus providing electrostatically merged ion beams. A pronounced enhancement of the rate is observed with clustering, which is interpreted as a change from electron transfer at small cluster size to proton transfer with more clustering.…”
Section: Gasesmentioning
confidence: 99%
“…Under these conditions information about the population of the doubly excited states can be obtained by the analysis of the energy spectra of the ejected electron, the dierent autoionizing states appearing as resonances. The theoretical interpretation of these experimental spectra is dicult, because of the interference of the direct and resonant ionization processes, and the three-body Coulomb interaction in the ®nal state between the scattered projectile, ejected electron and the residual ion [29].…”
Section: Introductionmentioning
confidence: 99%
“…Very recently, the complete theoretical description of the resonant ionization processes at intermediate projectile energies (100 keV/amu) performed by Godunov et al [29] made possible for Moretto-Capelle et al [37] to extract double excitation cross sections from their experimental spectra of the ejected electron, obtained with a high-resolution spectrometer. These cross sections not only complete the experimental data of Giese et al [36] to lower energies, but are stated to be more exact, making sense for the comparison of dierent theoretical results with the experiment.…”
Section: Introductionmentioning
confidence: 99%