1972
DOI: 10.1088/0022-3727/5/12/313
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Noble metal ion bombardment of polycrystalline metal surfaces

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Cited by 4 publications
(2 citation statements)
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“…The neutralized ions have small excitation energies (less than the target work-functions) and relatively large target/atom attractive forces. Neutralization is likely then to be predominantly by resonance transitions involving no electron ejection, just as in the case of noble metal ions (Burrow and Burtt 1972), and electron ejection coefficients of less than 1 % would be expected.…”
Section: Potential Ejectionmentioning
confidence: 99%
“…The neutralized ions have small excitation energies (less than the target work-functions) and relatively large target/atom attractive forces. Neutralization is likely then to be predominantly by resonance transitions involving no electron ejection, just as in the case of noble metal ions (Burrow and Burtt 1972), and electron ejection coefficients of less than 1 % would be expected.…”
Section: Potential Ejectionmentioning
confidence: 99%
“…The Fermi energies and work-functions (Yasui et a1 1970, Anderson and McCaffrey 1969, Mattheiss 1965, probably the dipole polarizabilities, and therefore the attractive van der Waals forces between the sputtered ions and the targets, increase with atomic number (Burrow and Burtt 1972). Ions sputtered from the vanadium target will thus be subject to recombination transitions nearest to the target and the ion current will be subject to the greatest attenuation (Burrow and Burtt 1972). Molybdenum ions will be subject to less attenuation and tungsten ions even less.…”
Section: L Sputtered Target Ionsmentioning
confidence: 99%