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@PHDTHESIS{Schffmann:892131,
author = {Schöffmann, Patrick},
title = {{S}toichiometric control and magnetoelectric coupling in
artificial multiferroic heterostructures},
volume = {247},
school = {RWTH Aachen},
type = {Dissertation},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2021-01966},
isbn = {978-3-95806-575-8},
series = {Schriften des Forschungszentrums Jülich. Reihe
Schlüsseltechnologien / Key Technologies},
pages = {vii, 176 S.},
year = {2021},
note = {Dissertation, RWTH Aachen, 2021},
abstract = {The demand for smaller and faster information storage
media, new types of sensors and multifunctional devices has
lead to a rush in research on transition metal oxides
(TMO's). Strong electronic correlations in TMO's lead to a
wealth of new and interesting effects. Particularly the use
of artificial multiferroic heterostructures using advanced
thin film growth techniques, has attracted a lot of
interest, as they enable the tailoring of the physical
properties of individual materials and hold the promise of
new combined functionality. The subject of this thesis is
control of the magnetisation in thin TMO films using the
ferroelectric substrate
[Pb(Mg$_{1/3}$Nb${_{2/3}}$)O$_{3}$]$_{0.7}$-[PbTiO$_{3}$]$_{0.3}$
(PMN-PT). The first part of this thesis is about the
fabrication and investigation of SrCoO$_{3-{\delta}}$, which
has different magnetic and conductive properties depending
on the oxygen content. Importantly, the antiferromagnetic,
insulating SrCoO$_{2.5}$ can be transformed reversibly in
the ferromagnetic, metallic SrCoO$_{3}$. To grow epitaxial
and stoichiometric Sr$_{1}$Co$_{1}$O$_{2.5}$ films by
molecular beam epitaxy (MBE), the deposition parameter have
to be precisely controlled. To determine the Co-to-Sr ratio
$\textit{in-situ}$ and optimise it, Reflection High Energy
Electron Diffraction (RHEED) can be used. The RHEED
scattering pattern changes depending on the Co/Sr ratio and
can be used to determine Co excess or deficiency and to grow
stoichiometric Sr$_{1}$Co$_{1}$O$_{2.5}$ samples. High
quality SrCoO$_{2.5}$ can be transformed to SrCoO$_{3}$ by
heating in oxygen flow and the resulting films remain stable
in vacuum. SrCoO$_{3-{\delta}}$ films (with $\delta$< 0.25)
form three distinct magnetic phases and show an exchange
bias effect. The magnetic phases are distributed uniformly
throughout the film, as can be determined by Polarised
Neutron Reflectometry (PNR). Due to a mismatch of lattice
constants, SrCoO$_{2.5}$ films can't be grown directly on
PMN-PT. However, using an La$_{0.67}$Sr$_{0.33}$MnO$_{3}$
buffer layer, crystalline
SrCoO$_{2.5}$/La$_{0.67}$Sr$_{0.33}$MnO$_{3}$/PMN-PT
heterostructures can be grown. The second part of the
dissertation is about the magnetoelectric coupling in
Fe$_{3}$O$_{4}$/PMN-PT(001) and Fe$_{3}$O$_{4}$/PMN-PT(011)
heterostructures grown by pulsed laser deposition. The
strain and polarisation of the substrate with applied
electric field mediate the coupling to the magnetisation in
the ferrimagnetic layer. Using a qualitative model, the
strength of the different contributions can be estimated.
The substrate cut and orientation of the sample in the
magnetic field has a strong influence on the magnetoelectric
behaviour of the layer.},
cin = {JCNS-2 / PGI-4 / JARA-FIT},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (FZJ) (POF4-6G4)},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G4},
experiment = {EXP:(DE-MLZ)MARIA-20140101},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/892131},
}