Titlebook: Ionization of Solids by Heavy Particles; Raúl A. Baragiola Book 1993 Springer Science+Business Media New York 1993 collision.condensed mat

Chemotherapy

Inner Shell Target Ionization by the Impact of N6+, O7+ and Ne9+ on Pt(110)(GANIL), Caen, were used to study the ion-induced electron emission (IEE) from a single crystal Pt(110) surface. Mass and charge selected beams of N., O. and Ne. with currents of 150nA, 60nA and 15nA are obtained. The IEE spectra are measured with an electrostatic analyzer with an energy resolution

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Studies on Slow Particle-Induced Electron Emission from Clean Metal Surfaces by Means of Electron Emelated electron emission statistics e.g. rather precise measurements of electron emission yields and a separation of (as long as remaining mutually independent) potential and kinetic contributions to the latter can be obtained..We discuss the shape of electron statistics for slow singly charged ion-

Intercept

Z1 and Z2 Oscillations in the Energy Loss of Slow Ions: Inhomogeneous Electron Gas Modelsolids. Both Z1 (ion atomic number) and Z2 (target atomic number) oscillations in the stopping power are calculated using a self-consistent (non-perturbative) description of the screening of the ion charge in an inhomogeneous electron gas, representing the core and the outer electrons of target atoms

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Aviary

Symmetric and Asymmetric Collisions in Auger Electron Emission from Al, Mg, Si, and MgxAl1-X, Targetbroad feature which are assigned to atomic-like L23MM and bulk-like L.VV transitions respectively.. Hole in the inner L-shell is produced in collisions between projectile and target atoms (asymmetric or p-t collisions) or between two alike target atoms in the collisional cascade (symmetric or t-t co

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Confound

Electron Ejection Induced by Fast Projectilesse models may be applied for the prediction of the primary electron flux in solids, as far as insulators or innershells of conductors are concerned. From comparisons of experimental data and theoretical results one may derive the limits of perturbation theory or classical collision theories. It will

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Statistics of Heavy Particle-Induced Electron Emission from a Foilnge of 10–200 keV. The absolute probabilities .., .., .. of the emission of ., .′(= 0, 1…) numbers ot electrons in forward (.), and/or backward (.′) direction from the foil have been derived. Using the Monte Carlo approach the processes of internal secondary electron production and transport were si

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Incident and Exit Charge State Dependence of Secondary Electron Emission from a Carbon Foil by the Projectile ion itself comes close to the state of equilibrium through the charge exchange process with target atoms. Primary electrons produced in the direct ionization of target atoms by the projectile ion give birth to “secondary” electrons through a cascade process. Plasmons also decay into electr

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