1994
DOI: 10.1103/physreva.50.3117
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Auger electron emission following double electron capture in 150-keVNe10++He collisions

Abstract: The method of projectile electron spectroscopy was used to measure the Ne'+ Auger decay of the configurations 3lnl' and 4lnl. ' (n~4) created by double electron capture in 150-keV Ne' ++He collisions. Auger yields were evaluated to convert the experimental cross sections for Auger-electron emission into the corresponding cross sections for double electron capture. It is found that the cross sections attributed to the configurations 3lnl' follow a n ' law, while the excitation of the configurations 4lnl' is rat… Show more

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Cited by 30 publications
(10 citation statements)
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“…At the conclusion of the time propagation for each trajectory, the binding energies of the electrons were examined to determine whether a SEC or MEC event had occurred. For the MCLZ method, the multichannel probability approach of Janev et al (1983) was adopted with radial couplings estimated for monoelectronic transitions following Olson & Salop (1976) and dielectronic transitions following Fremont et al (1994). Further details concerning the MCLZ and CTMC methods as well as final-state-selective results will be presented in a later paper.…”
Section: Theoretical Considerationsmentioning
confidence: 99%
“…At the conclusion of the time propagation for each trajectory, the binding energies of the electrons were examined to determine whether a SEC or MEC event had occurred. For the MCLZ method, the multichannel probability approach of Janev et al (1983) was adopted with radial couplings estimated for monoelectronic transitions following Olson & Salop (1976) and dielectronic transitions following Fremont et al (1994). Further details concerning the MCLZ and CTMC methods as well as final-state-selective results will be presented in a later paper.…”
Section: Theoretical Considerationsmentioning
confidence: 99%
“…Elaborate quantum multistate close coupling calculations [2] give precise cross sections for production of either configurations. Contributions of single capture followed by transfer excitation and of other dielectronic interactions for populating asymmetrical configurations [3][4][5] depend on collision systems and impact energies. In the case of primary population into ͑n, n 0 ͒ symmetrical configurations which are strongly mixed with (low n 1 , high n 2 ) Rydberg states, the transfer from the former to the latter by autotransfer to Rydberg states (ATR) is very efficient [6,7].…”
mentioning
confidence: 99%
“…Ne 10+ +He is a collision system that received much attention, but without reaching consensus. Several experimental reports argued in favor of correlated double capture and correlated transfer excitation [49][50][51], while others stressed the importance of auto-transfer to Rydberg states [43,[52][53][54][55]; whereas a theoretical study [56] found that both auto-transfer to Rydberg states and static configuration interaction populate the (3, n) Rydberg series. The debate continued in more recent work involving other collision systems [57,58].…”
Section: Introductionmentioning
confidence: 99%