2002
DOI: 10.1016/s1387-3806(01)00515-2
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Calculated electron impact cross sections for the K-shell ionization of Fe, Co, Mn, Ti, Zn, Nb, and Mo atoms using the DM formalism

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Cited by 45 publications
(31 citation statements)
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“…The characteristic or line radiation exhibits a quasi-threshold dependence on the intensity, as it increases more rapidly after a delayed onset. The collisional ionization cross section for the 2s electron (whose vacancy results in L-shell photon emission) peaks at energies well above those measured in the experiments here, approximately three times its binding energy [27], which is shown by the dotted line in Fig. 3.…”
Section: Target Materialssupporting
confidence: 48%
“…The characteristic or line radiation exhibits a quasi-threshold dependence on the intensity, as it increases more rapidly after a delayed onset. The collisional ionization cross section for the 2s electron (whose vacancy results in L-shell photon emission) peaks at energies well above those measured in the experiments here, approximately three times its binding energy [27], which is shown by the dotted line in Fig. 3.…”
Section: Target Materialssupporting
confidence: 48%
“…For high incident energies from several keV, relativistic effects affect the EI ionization cross sections considerably. In the DM model 18, relativistic effects are included via a multiplying factor to the nonrelativistic DM model 4, and this provides a good description of the electron impact K‐shell ionization of atoms with a wide range of Z values 19–21. In the BEA model, the relativistic kinematics is absent.…”
Section: Introductionmentioning
confidence: 99%
“…where r 1s is the radius of maximum radial density of Cu 1s-shell from the tables of Desclaux [57], g 1s is a weighting factor, E 1s is the binding energy of 1s electrons, and the functions f , F are those in reference [56].…”
Section: Numerical Modelmentioning
confidence: 99%