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@ARTICLE{Waschk:872955,
author = {Waschk, M. and Sarkar, A. and Barthel, J. and Voigt, J. and
Schröder, S. and Zakalek, P. and Schmitz, Markus and Kirby,
B. J. and Pütter, S. and Schubert, J. and Brückel, T.},
title = {{I}mpact of growth kinetics on the interface morphology and
magnetization in {L}a 1/3 {S}r 2/3 {F}e{O} 3 /{L}a 2/3 {S}r
1/3 {M}n{O} 3 heterostructures},
journal = {Journal of physics / Condensed matter Condensed matter},
volume = {32},
number = {16},
issn = {1361-648X},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {FZJ-2020-00415},
pages = {165801 -},
year = {2020},
abstract = {The ability to create atomically perfect, epitaxial
heterostructures of correlated complex perovskite oxides
using state-of-art thin film deposition techniques has
generated new physical phenomena at engineered interfaces.
Here we report on the impact of growth kinetics on the
magnetic structure and exchange coupling at the interface in
heterostructures combining layers of antiferromagnetic
La1/3Sr2/3FeO3 (LSFO) and ferromagnetic La2/3Sr1/3MnO3
(LSMO) on (0 0 1)-oriented SrTiO3 (STO) substrates. Two
growth orders are investigated, (a) LSMO/LSFO/STO(0 0 1)
and (b) LSFO/LSMO/STO(0 0 1), where the LSFO layer is
grown by molecular beam epitaxy and the LSMO layer by high
oxygen pressure sputtering. The interface has been
investigated using electron microscopy and polarized neutron
reflectometry. Interdiffusion over seven monolayers is
observed in LSMO/LSFO (a) with an almost $50\%$ reduction in
magnetization at the interface and showing no exchange
coupling. However, the exchange bias effect ( mT at 10 K)
could be realized when the interface is atomically sharp, as
in LSFO/LSMO (b). Our study therefore reveals that, even for
well ordered and lattice-matched structures, the kinetics
involved in the growth processes drastically influences the
interface quality with a strong correlation to the magnetic
properties.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-HBS / JCNS-FRM-II / PGI-9
/ ER-C-2 / VS-II},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-HBS-20180709 /
I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)PGI-9-20110106 / I:(DE-Juel1)ER-C-2-20170209 /
I:(DE-Juel1)VS-II-20090406},
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)External-20140101},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:31899900},
UT = {WOS:000520153200001},
doi = {10.1088/1361-648X/ab678c},
url = {https://juser.fz-juelich.de/record/872955},
}