Stress Evolution during Ge Nanoparticles Growth in a SiO
2
Matrix
Branko Pivac,* Pavo Dubč ek, Jasna Dasovic ́ , Jasminka Popovic ́ , and Nikola Radic ́
Materials Physics, R. Bos ̌ ković Institute, Bijenič ka 54, Zagreb 10000, Croatia
Sigrid Bernstorff
Elettra-Sincrotrone Trieste, SS 14, Km 163.5, in AREA Science Park, Basovizza 34149, Trieste, Italy
Janez Zavas ̌ nik
Jož ef Stefan Institute, Jamova Cesta 39, Ljubljana 1000, Slovenia
Max-Planck-Institut fü r Eisenforschung GmbH, Max-Planck-Straße 1, Dü sseldorf 40237, Germany
Branislav Vlahovic
North Carolina Central University, Durham, North Carolina 27707, United States
* S Supporting Information
ABSTRACT: Superstructures are explored that were ob-
tained by multilayer magnetron deposition at room temper-
ature of 20 SiO
2
and SiO
2
:Ge bilayers, each 2 × 4 nm thick,
and subsequently annealed in inert N
2
atmosphere at different
temperatures in the range of 500−750 °C. The structural and
optical changes induced by annealing and the formation and
growth of Ge nanoparticles (nps) from early clusters to their
full growth and final dissolution were studied by the
simultaneous grazing-incidence small- and wide-angle X-ray
scattering, transmission electron microscopy, and (time-
resolved) photoluminescence (PL). It is shown that in as-
deposited multilayers aggregation of small clusters already
occurred, and the clusters were reasonably well intercorrelated in the lateral plane. During annealing at T
a
= 550 °C or higher
temperatures, Ge nps start to form and remain partly amorphous at lower T
a
but crystallize completely at about 600 °C. At even
higher temperatures, the Ge nps dissolve and Ge diffuses out almost completely, leaving voids in the SiO
2
matrix. Visible PL
from the samples was detected and attributed to defects in the nps/matrix interface layers rather than to the nps itself because
PL persisted even after Ge nps dissolution.
1. INTRODUCTION
During the last decades, interest in semiconductor nanocrystals
embedded in dielectrics has been continuously growing
because of the fact that space confinement drastically affects
the properties of matter and thus, e.g., efficient visible
photoluminescence (PL) from Si nanocrystals was observed.
1
The properties of such nanoparticles (nps) are critically
dependent on their size because of quantum confinement
effects, which allow their application in the fields of
optoelectonics,
2
semiconductor memories,
3
and photovol-
taics.
4
Therefore, such nps are often named quantum dots
(QDs). The tunability of QDs affects the efficiency of
interaction with light, which is important in the field of
photovoltaics. One of the very promising candidates for QDs
realization is Si nps confined to a SiO
2
matrix because this
approach is compatible with standard Si microelectronic
integration technology.
5
Moreover, it was proposed as a
good candidate for “all-Si” tandem solar cells.
6
Compared to the intensively studied Si QDs, Ge nanocryst-
als have a more prominent quantum confinement effect
because of their larger excitonic Bohr radii,
7
i.e., because of the
smaller effective masses of electrons and holes. Further,
theoretical analysis indicates that indirect-to-direct-band-gap
transitions in the Ge energy-band structure occur with size
reduction, and the oscillator strengths are expected to be larger
in Ge QDs than in Si QDs.
8
This effect is attributed to
stronger overlaps of the electron-wave functions in Ge atoms,
9
which enhances light absorption in Ge QDs.
Received: September 27, 2018
Article
pubs.acs.org/IC
Cite This: Inorg. Chem. XXXX, XXX, XXX-XXX
© XXXX American Chemical Society A DOI: 10.1021/acs.inorgchem.8b02760
Inorg. Chem. XXXX, XXX, XXX−XXX
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