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Electron beam charging of insulators with surface layer and leakage currents

N. CornetCentre Sciences des Matériaux et des Structures 1 , Ecole Nationale Supérieure des Mines, 158 cours Fauriel, F-42023 Saint-Etienne Cedex 2, FranceD. GoeuriotCentre Sciences des Matériaux et des Structures 1 , Ecole Nationale Supérieure des Mines, 158 cours Fauriel, F-42023 Saint-Etienne Cedex 2, FranceC. Guerret-PiécourtLaboratoire de Tribologie et Dynamique des Systemes 2 , UMR-CNRS 5513, Ecole Centrale de Lyon, 36 avenue Guy de Collongue, F-69134 Ecully Cedex, FranceD. JuvéLaboratoire de Tribologie et Dynamique des Systemes 2 , UMR-CNRS 5513, Ecole Centrale de Lyon, 36 avenue Guy de Collongue, F-69134 Ecully Cedex, FranceD. TréheuxLaboratoire de Tribologie et Dynamique des Systemes 2 , UMR-CNRS 5513, Ecole Centrale de Lyon, 36 avenue Guy de Collongue, F-69134 Ecully Cedex, FranceMatthieu TouzinUniversité des Sciences et Technologies de Lille 3 Laboratoire de Structure et Propriétés de l’Etat Solide-UMR-CNRS 8008, , Bât. C6, F-59655 Villeneuve d’Ascq Cedex, FranceH.‐J. FittingUniversity of Rostock 4 Physics Department, , Universitätsplatz 3, D-18051 Rostock, Germany
2008en
ABI

Аннотация

The electron beam induced self-consistent charge transport in layered insulators (here, bulk alumina covered by a thin silica layer) is described by means of an electron-hole flight-drift model and an iterative computer simulation. Ballistic secondary electrons and holes, their attenuation and drift, as well as their recombination, trapping, and detrapping are included. Thermal and field-enhanced detrapping are described by the Poole–Frenkel effect. Furthermore, an additional surface layer with a modified electric surface conductivity is included which describes the surface leakage currents and will lead to particular charge incorporation at the interface between the surface layer and the bulk substrate. As a main result, the time-dependent secondary electron emission rate σ(t) and the spatial distributions of currents j(x,t), charges ρ(x,t), field F(x,t), and potential V(x,t) are obtained. For bulk full insulating samples, the time-dependent distributions approach the final stationary state with j(x,t)=const=0 and σ=1. In the case of a measurable surface leakage current, the steady stationary state is reached for σ<1. First measurements are extended to the sample current measurement including nonstationary components of charge incorporation and polarization as well as dc components of leakage currents.

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