1982
DOI: 10.1051/jphys:01982004302027900
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Calcul exact de la fonction de distribution des ions incidents sur une cible dans le cas d'un plasma de pulvérisation

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Cited by 7 publications
(4 citation statements)
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“…(1) where a i s in cm2, and the ion energy E is in eV. Chouan and Collobert (1982) use a similar expression for a. (Strictly speaking it is the relative velocity of the colliding ion and atom which enters in the cross-section, but we shall assume that the atom is at rest before the collision.)…”
Section: Energy Distributions Of Ions and Neutralsmentioning
confidence: 99%
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“…(1) where a i s in cm2, and the ion energy E is in eV. Chouan and Collobert (1982) use a similar expression for a. (Strictly speaking it is the relative velocity of the colliding ion and atom which enters in the cross-section, but we shall assume that the atom is at rest before the collision.)…”
Section: Energy Distributions Of Ions and Neutralsmentioning
confidence: 99%
“…The expression in equation (6a) was derived by Davis and Vanderslice (1963) and also by Chouan and Collobert (1982). Except for the contribution of the primary ions to the energy distribution (the first term in equations ( 4a) and (6a), corresponding to those ions that do not collide in the dark space), and for L/A 3 1, the ion distributions peak at low energies and decrease monotonically with increasing ion energy.…”
Section: B ( L E ) = (L/~ae)(e/e)-''~~xp[-l(e/e~)~'~/a]mentioning
confidence: 99%
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