% 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{Loo:856521,
author = {Loo, Roger and Shimura, Yosuke and Ike, Shinichi and Vohra,
Anurag and Stoica, Toma and Stange, Daniela and Buca, Dan
Mihai and Kohen, David and Margetis, Joe and Tolle, John},
title = {{E}pitaxial {G}e{S}n: impact of process conditions on
material quality},
journal = {Semiconductor science and technology},
volume = {33},
number = {11},
issn = {0268-1242},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {FZJ-2018-05908},
pages = {114010},
year = {2018},
abstract = {The electrical and optical material properties of epitaxial
Ge1−xSnx and SiyGe1−x−ySnx are of high interest for
novel device applications. However, the limited Sn
solubility in Ge makes the epitaxial growth of Ge1−xSnx
and SiyGe1−x−ySnx challenging. Most of the literature
describing the epitaxial growth is for Ge2H6 and SnCl4 as Ge
and Sn precursors, respectively. A more recent publication
deals with the epitaxial growth of high-quality Ge1−xSnx
with the more conventional GeH4. In this manuscript, we
compare the structural and optical material quality of
Ge1−xSnx, epitaxially grown on Ge virtual substrates as a
function of growth pressure, growth temperature, the choice
of the carrier gas (H2 or N2) and the choice of the Ge
precursor (GeH4 versus Ge2H6). The best material quality in
terms of surface morphology and photoluminescence
characteristics is obtained if GeH4 is used as a Ge
precursor. For Ge1−xSnx grown with Ge2H6 and at
atmospheric pressure, pyramidical defects can be seen and
there is a risk for uncontrolled local Sn agglomeration. The
pyramidical defects are not observed on Ge1−xSnx layers
grown at reduced pressure, but the highest achievable
substitutional Sn concentration is lower. No pyramidical
defects are found for Ge1−xSnx layers grown with GeH4 and
the issue of uncontrolled local Sn agglomeration does not
appear.},
cin = {PGI-9 / JARA-FIT},
ddc = {620},
cid = {I:(DE-Juel1)PGI-9-20110106 / $I:(DE-82)080009_20140620$},
pnm = {521 - Controlling Electron Charge-Based Phenomena
(POF3-521)},
pid = {G:(DE-HGF)POF3-521},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000448113100002},
doi = {10.1088/1361-6641/aae2f9},
url = {https://juser.fz-juelich.de/record/856521},
}