% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{vanStraaten:844985,
author = {van Straaten, Gerben and Franke, Markus and Posseik,
Francois and Tautz, Frank Stefan and Kumpf, Christian},
title = {{N}on-dipolar effects in photoelectron-based normal
incidence {X}-ray standing wave experiments},
journal = {Journal of electron spectroscopy and related phenomena},
volume = {222},
issn = {0368-2048},
address = {New York, NY [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2018-02320},
pages = {106 - 116},
year = {2018},
abstract = {The normal incidence X-ray standing waves technique is one
of the most well-established methods for investigating the
geometric structure at interfaces and surfaces. It is able
to measure vertical positions and distances of individual
atomic species with very high precision (typically <0.02
Å). These data not only yield valuable structural
information, but also represent an excellent benchmark for
density functional theory and ab initio calculations.
Non-dipolar effects are well known to strongly affect the
result, in particular when light elements are involved. A
correction mechanism for these effects is established, but
in its commonly-used form it is based on one essential
restriction, namely the assumption of perfect normal
incidence of the X-rays with respect to the relevant lattice
planes of the crystal. Here, we show that small deviations
from normal incidence, as they are unavoidable in typical
experimental setups, lead to significant systematic errors
in the NIXSW results. The magnitude of this effect depends
on the specific conditions in a non-linear way and may reach
up to $5\%,$ corresponding to several tenths of an
Ångström in the adsorption height. We present a
straightforward way of accounting for this effect, and
demonstrate that recording the photoelectron yield in an
angular-resolved mode is indispensable, since the correction
parameters strongly depend on the electron take-off angle.},
cin = {PGI-3},
ddc = {620},
cid = {I:(DE-Juel1)PGI-3-20110106},
pnm = {143 - Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000423638100015},
doi = {10.1016/j.elspec.2017.07.007},
url = {https://juser.fz-juelich.de/record/844985},
}