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@ARTICLE{Schindler:255689,
author = {Schindler, T. and Schmiele, M. and Schmutzler, T. and
Kassar, T. and Segets, D. and Peukert, W. and Radulescu, A.
and Kriele, A. and Gilles, R. and Unruh, T.},
title = {{A} {C}ombined {SAXS}/{SANS} {S}tudy for the in {S}itu
{C}haracterization of {L}igand {S}hells on {S}mall
{N}anoparticles: {T}he {C}ase of {Z}n{O}},
journal = {Langmuir},
volume = {31},
number = {37},
issn = {1520-5827},
address = {Washington, DC},
publisher = {ACS Publ.},
reportid = {FZJ-2015-05822},
pages = {10130 - 10136},
year = {2015},
abstract = {ZnO nanoparticles (NPs) have great potential for their use
in, e.g., thin film solar cells due to their electro-optical
properties adjustable on the nanoscale. Therefore, the
production of well-defined NPs is of major interest. For a
targeted production process, the knowledge of the
stabilization layer of the NPs during and after their
formation is of particular importance. For the study of the
stabilizer layer of ZnO NPs prepared in a wet chemical
synthesis from zinc acetate, only ex situ studies have been
performed so far. An acetate layer bound to the surface of
the dried NPs was found; however, an in situ study which
addresses the stabilizing layer surrounding the NPs in a
native dispersion was missing. By the combination of small
angle scattering with neutrons and X-rays (SANS and SAXS)
for the same sample, we are now able to observe the acetate
shell in situ for the first time. In addition, the changes
of this shell could be followed during the ripening process
for different temperatures. With increasing size of the ZnO
core (dcore) the surrounding shell (dshell) becomes larger,
and the acetate concentration within the shell is reduced.
For all samples, the shell thickness was found to be larger
than the maximum extension of an acetate molecule with
acetate concentrations within the shell below 50 vol $\%.$
Thus, there is not a monolayer of acetate molecules that
covers the NPs but rather a swollen shell of acetate ions.
This shell is assumed to hinder the growth of the NPs to
larger macrostructures. In addition, we found that the
partition coefficient μ between acetate in the shell
surrounding the NPs and the total amount of acetate in the
solution is about $10\%$ which is in good agreement with ex
situ data determined by thermogravimetric analysis.},
cin = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
(München) ; JCNS-FRM-II / Neutronenstreuung ; JCNS-1},
ddc = {670},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-1-20110106},
pnm = {6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich Centre for
Neutron Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)KWS2-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000361935500004},
doi = {10.1021/acs.langmuir.5b02198},
url = {https://juser.fz-juelich.de/record/255689},
}