Monte Carlo simulation of low-energy electron trajectories and energy lossin ZnS phosphor powders

Citation
Ap. Greeff et Hc. Swart, Monte Carlo simulation of low-energy electron trajectories and energy lossin ZnS phosphor powders, SURF INT AN, 31(6), 2001, pp. 448-456
Citations number
26
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
SURFACE AND INTERFACE ANALYSIS
ISSN journal
01422421 → ACNP
Volume
31
Issue
6
Year of publication
2001
Pages
448 - 456
Database
ISI
SICI code
0142-2421(200106)31:6<448:MCSOLE>2.0.ZU;2-A
Abstract
During electron beam irradiation of ZnS phosphor powders, a non-luminescent ZnO layer is formed on the powder due to electron-beam-stimulated surface reactions. As the thickness of the oxide layer increases, the energy loss i n the ZnS bulk decreases with a subsequent degradation in cathodoluminescen ce. Using the Monte Carlo technique, the trajectories of low-energy electro ns were simulated in a ZnS phosphor powder with a ZnO overlayer of varying thickness based on recent models describing the energy loss and scattering angles of low-energy electrons in a solid. A diffusion interface between th e ZnO layer and ZnS bulk was simulated by varying the concentration of O an d S atoms in the interface. Modelling the interface in this way describes t he electron trajectories and energy loss in the interface region, because a sharp interlace between two dissimilar layers very seldom exists. In the e nergy-loss profiles the transition between ZnO and ZnS corresponds to a sha rp increase in energy loss due to the increased rate of energy loss of elec trons in ZnS. The diffusion interface has a smoothing effect on this sudden increase. From the electron trajectory data and corresponding energy loss, energy loss profiles were determined indicating the cumulative distributio n of all the electron energy losses as a function of the interaction volume depth and thickness of the ZnO layer. When a distribution of incident angl es is used, the profile differs from the typical energy-loss profile seen a t normal incident angles. As the thickness of the ZnO layer increases, the total energy loss in the solid decreases due to the increase in the backsca ttering coefficient of electrons in ZnO. Copyright (C) 2001 John Wiley & So ns, Ltd.