% 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”.
@INPROCEEDINGS{Wulff:300271,
author = {Wulff, Harm and Quaas, M. and Deutsch, H. and Ahrens, Heiko
and Fröhlich, M. and Helm, Christiane A.},
title = {{F}ormation of palladium hydrides in low temperature
$\mathrm{{A}r/{H}_{2}}$-plasma},
journal = {Thin solid films},
volume = {596},
issn = {0040-6090},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {PUBDB-2016-02253},
pages = {185-189},
year = {2015},
abstract = {20 nm thick Pd coatings deposited on Si substrates with 800
nm SiO$_{2}$ and 1 nm Cr buffer layers were treated in a
2.45 GHz microwave plasma source at 700 W plasma power and
40 Pa working pressure without substrate heating. For
obtaining information on the effect of energy influx due to
ion energy on the palladium films the substrate potential
was varied from U$_{sub}$ = 0 V to − 150 V at constant gas
flow corresponding to mean ion energies E$_{i}$ from 0.22 eV
∙ cm$^{− 2}$ ∙ s$^{− 1}$ to 1.28 eV ∙ cm$^{− 2}$
∙ s$^{− 1}$.In contrast to high pressure reactions with
metallic Pd, under plasma exposure we do not observe solid
solutions over a wide range of hydrogen concentration. The
hydrogen incorporation in Pd films takes place
discontinuously. At 0 V substrate voltage palladium hydride
is formed in two steps to PdH$_{0.1}$4 and PdH$_{0.57}$. At
− 50 V substrate voltage Pd$_{H0.57}$ is formed directly.
However, substrate voltages of − 100 V and − 150 V cause
shrinking of the unit cell. We postulate the formation of
two fcc vacancy palladium hydride clusters PdH$_{Vac}$(I)
and PdH$_{Vac}$(II). Under longtime plasma exposure the fcc
PdHVac(II) phase forms cubic PdH$_{1.33}$.The fcc
PdH$_{0.57}$ phase decomposes at temperatures > 300 °C to
form metallic fcc Pd. The hydrogen removal causes a decrease
of lattice defects. In situ high temperature diffractometry
measurements also confirm the existence of PdHVac(II) as a
palladium hydride phase. Stoichiometric relationship between
cubic PdH$_{1.33}$ and fcc PdH$_{Vac}$(II) becomes evident
from XR measurements and structure considerations. We assume
both phases have the chemical composition Pd$_{3}$H$_{4}$.
Up to 700 °C we observe phase transformation between both
the fcc PdH$_{Vac}$(II) and cubic PdH$_{1.33}$ phases. These
phase transformations could be explained analog to a Bain
distortion by displacive solid state structural changes.},
month = {Apr},
date = {2015-04-20},
organization = {42nd International Conference on
Metallurgical Coatings and Thin Films,
San Diego (USA), 20 Apr 2015 - 24 Apr
2015},
cin = {DOOR},
ddc = {070},
cid = {I:(DE-H253)HAS-User-20120731},
pnm = {899 - ohne Topic (POF3-899)},
pid = {G:(DE-HGF)POF3-899},
experiment = {EXP:(DE-H253)D-D4-20150101},
typ = {PUB:(DE-HGF)16 / PUB:(DE-HGF)8},
UT = {WOS:000366204900031},
doi = {10.1016/j.tsf.2015.08.061},
url = {https://bib-pubdb1.desy.de/record/300271},
}