% 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”.
@PHDTHESIS{Wang:847883,
author = {Wang, Liming},
title = {{M}anipulation of magnetism in iron oxide nanoparticle /
{B}a{T}i{O}$_{3}$ composites and low-dimensional iron oxide
nanoparticle arrays},
volume = {180},
school = {RWTH Aachen},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2018-03209},
isbn = {978-3-95806-351-8},
series = {Schriften des Forschungszentrums Jülich. Reihe
Schlüsseltechnologien / Key Technologies},
pages = {VI, 151 S.},
year = {2018},
note = {RWTH Aachen, Diss., 2018},
abstract = {Ferrimagnetic (FiM) iron oxide nanoparticles (NPs) on top
of ferroelectric BaTiO$_{3}$(BTO) substrates were prepared
and a magnetoelectric coupling (MEC) effect was observed in
the heterostructures. Iron oxide NPs first were
self-assembled as amonolayer on top of BTO substrates.
Grazing incidence small angle x-ray scattering(GISAXS) and
scanning electron microscopy (SEM) confirm a close-packed
hexagonal order of the NP monolayers. By inserting a Ti
layer and further capping with an Au layer, an enhanced MEC
effect was observed. Scanning transmission electron
microscopy (STEM) provides information about the layer
structure of the sample. The magnetization shows sharp
magnetization jumps at the phase transition temperatures of
the BTO substrate. Electric field manipulation of magnetism
was performed using a superconducting quantum interference
device (SQUID) setup with an electric field implemented. A
butterfly shaped curve of the magnetic moment vs. DC
electric field was obtained which is coincident with the
piezoelectric response of BTO single crystals which confirms
a strain mediated MEC. The magnetoelectric ac susceptibility
(MEACS) signal as function of temperature under an AC
electric field shows abrupt jumps at the BTO phase
transition temperatures. The magnetic depth profiles of NP
monolayers at various applied DC electric fields were
deduced from polarized neutron reflectivity (PNR) results.
Fitting of the data shows that the observed differences in
reflectivity curves are caused by the changed structural
properties of the substrate and layers as a major factor and
the altered magnetism of NP monolayers as a minor factor.
Also iron oxide NPs self-assembled on BTO films on Nb doped
SrTiO$_{3}$ (Nb doped STO) substrates were prepared. The DC
electric field vs. magnetization and MEACS results indicate
that there is a MEC between NPs and the BTO film. Interface
charge and strain transfer are responsible for the MEC
effects. Moreover, NPs self assembled into trench-patterned
silicon (Si) substrates were prepared to investigate the
magnetic anisotropy and collective magnetic behavior. The
magnetization vs. magnetic field shows a large shape-induced
magnetic anisotropy effect. After the application of a
magnetic saturation field along the trenches, electron
holography results show that an overall magnetic ordered
state exists in the nanoparticle assemblies. In the
direction of the trenches, the NPs exhibit a ferromagnetic
(FM) -like ordered state and a small memory effect was
observed. Whereas large memory effect was observed
perpendicular to the trenches. We conclude that the FM
ordered state suppresses a superspin glass state of the
dipolarly coupled NP moments. This work opens up viable
possibilities for energy-efficient electronic devices
fabricated by simple self-assembly techniques.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-FRM-II},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ /
I:(DE-Juel1)JCNS-FRM-II-20110218},
pnm = {144 - Controlling Collective States (POF3-144) / 524 -
Controlling Collective States (POF3-524) / 6212 - Quantum
Condensed Matter: Magnetism, Superconductivity (POF3-621) /
6213 - Materials and Processes for Energy and Transport
Technologies (POF3-621) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-524 /
G:(DE-HGF)POF3-6212 / G:(DE-HGF)POF3-6213 /
G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)MARIA-20140101 / EXP:(DE-MLZ)SPODI-20140101},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/847883},
}