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Untitled - IAP/TU Wien - Technische Universität Wien

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Nanostructure Characterisation by Electron Beam Techniques<br />

Surface excitations in electron spectroscopy<br />

F. Salvat-Pujol, 1,* W.S.M. Werner, 2 W. Smekal, 2 R. Khalid, 2 A. Bellissimo, 2<br />

M. Novák 3 , J. Zemek 4 , and P. Jiricek 4<br />

1 Insitut für Theoretische Physik, Goethe-<strong>Universität</strong> Frankfurt,<br />

Max-von-Laue-Straße 1, 60438 Frankfurt (Germany)<br />

2 Institut für Angewandte Physik, <strong>Technische</strong> <strong>Universität</strong> <strong>Wien</strong>,<br />

Wiedner Hauptstraße 8-10/134, 1040 <strong>Wien</strong> (Austria)<br />

3 Université Libre de Bruxelles, Service de Métrologie Nucléaire,<br />

CP 165/84, 50 Avenue F. D. Roosevelt, B-1050 Brussels, (Belgium)<br />

4 Institute of Physics, Academy of Sciences of the Czech Republic,<br />

Na Slovance 2, 182 21 Prague 8, (Czech Republic)<br />

*salvat-pujol@itp.uni-frankfurt.de<br />

A quantitative understanding of electron spectra relies on an adequate description of electron energy losses<br />

taking place both in the bulk of the solid and in the vicinity of the solid-vacuum interface (at either side of<br />

the surface). Several models for electron energy losses near planar interfaces have been published in the last<br />

three decades based on the semiclassic dielectric formalism (see references in [1]). However, these models<br />

often include several simplifying approximations: some are valid for selected trajectories, others employ a<br />

simplified dielectric response of the solid, etc.<br />

A detailed model for surface excitations in electron spectroscopy has been derived within the semiclassic<br />

dielectric formalism, encompassing other models in the literature and allowing one to investigate their<br />

relevant physical assumptions. The model has been implemented in a Monte Carlo simulation of reflectionelectron-energy-loss<br />

spectra (REELS). REELS have been simulated for 17 metals, obtaining a good<br />

agreement with published experimental spectra in absolute units (typically within $\sim10$ \%).<br />

The model has been further employed to interpret a series of recent electron energy-loss experiments. On the<br />

one hand, it has been instrumental in exposing the role played by surface excitations in secondary-electron<br />

emission in a recent measurement of a double-differential secondary-electron yield from polycrystalline<br />

samples (Al, Si, Ag) employing a time-coincidence technique. On the other hand, it has been used to<br />

interpret a series of angle-resolved REELS of a Au surface at grazing incidence [2]: it has been shown that<br />

energy losses at the vacuum side of the interface constitute an essential contribution to electron energy-loss<br />

spectra and must be accounted for in detail for a quantitative understanding of REELS.<br />

References<br />

[1] F. Salvat-Pujol and W.S.M. Werner, Surf. Interface Anal. 45 873-894 (2013).<br />

[2] W.S.M. Werner et al, Phys. Rev. Lett. 110 086110 (2013).<br />

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