% 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”.
@BOOK{Schumacher:133358,
author = {Schumacher, Daniel},
title = {{I}nterplay between magnetic and dielectric phenomena at
transition metal oxide interfaces},
volume = {56},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2013-01835},
isbn = {978-3-89336-855-6},
series = {Schriften des Forschungszentrums Jülich.
Schlüsseltechnologien / Key Technologies},
pages = {IV, 127 S.},
year = {2013},
abstract = {The present work is concerned with the preparation,
characterzation and analysis of thin film heterostructures
of perovskite oxide materials. Two different systems have
been analyzed in detail:
La$_{0.66}$Sr$_{0.33}$MnO$_{3}$/SrTiO$_{3}$ (LSMO/STO)
heterostructures have been investigated in order to
understand the unusual occurrence of an exchange bias effect
in multilayers of these two oxides [1]. Monocrystalline LSMO
single and LSMO/STO bilayers have been grown on STO by both
High Osygen Pressure Sputter Deposition (HSD) and Pulsed
Laser Deposition. It was possible to reproduce the Exchange
Bias effect in the samples grown by HSD by reducing the
oxygen pressure during the layer growth. In fact, the size
of the effect can be increased by further reduction of the
oxygen pressure. The macroscopic sample analysis by X-ray
Diffraction and Vibrating Sample Magnetometry suggests that
the occurence of the Exchange Bias effect is linked to
oxygen deficiencies in the LSMO layer. By combining X-ray
Reflectometry, Polarized Neutron Reflectometry and X-ray
Resonant magnetic Scattering (XRMS), the magnetic depth
profile of the samples has been determined. By this, a
region in LSMO at the interface to STO has been detected,
where the magnetic moment is strongly suppressed. By putting
together the results of the macroscopic sample analysis and
the scattering experiments, an explanation for the occurence
of the effect can be given: It is roposed, that a
combination of strain and oxygen deficiencies shifts the
LSMO at the interface in the antiferromagnetic phase of the
LSMO strain vs. doping phase diagram. This interface region
thus couples to the ferromagnetic part of the LSMO causing
the Exchange BIAS effect. The second heterostructure system
under investigation in this work are bilayers of
La$_{0.5}$Sr$_{0.5}$MnO$_{3}$ (LSMO) and BaTiO$_{3}$ (BTO).
possible dependence of the interface near magnetic structure
[...]},
cin = {PGI-4 / JCNS-2 / JARA-FIT},
cid = {I:(DE-Juel1)PGI-4-20110106 / I:(DE-Juel1)JCNS-2-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {422 - Spin-based and quantum information (POF2-422) / 424 -
Exploratory materials and phenomena (POF2-424) / 542 -
Neutrons (POF2-542) / 544 - In-house Research with PNI
(POF2-544) / 54G - JCNS (POF2-54G24)},
pid = {G:(DE-HGF)POF2-422 / G:(DE-HGF)POF2-424 /
G:(DE-HGF)POF2-542 / G:(DE-HGF)POF2-544 /
G:(DE-HGF)POF2-54G24},
typ = {PUB:(DE-HGF)3},
url = {https://juser.fz-juelich.de/record/133358},
}