% 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”.
@ARTICLE{Yang:897408,
author = {Yang, Lin and Jin, Lei and Wysocki, Lena and Schöpf, Jörg
and Jansen, Daniel and Das, Brajagopal and Kornblum, Lior
and van Loosdrecht, Paul H. M. and Lindfors-Vrejoiu, Ionela},
title = {{E}nhancing the ferromagnetic interlayer coupling between
epitaxial {S}r{R}u{O} 3 layers},
journal = {Physical review / B},
volume = {104},
number = {6},
issn = {2469-9969},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2021-03774},
pages = {064444},
year = {2021},
abstract = {Magnetic interlayer coupling is a key ingredient in
designing magnetic multilayers with functionalities that
reach out to the realm of applications. In epitaxial
ferromagnetic (FM) oxide multilayers, the magnetic
interlayer coupling is, however, less studied and its
prediction is often a challenging task. Ultrathin FM SrRuO3
epitaxial films with perpendicular magnetic anisotropy,
interfaced with suitable oxides, may be susceptible of
forming skyrmions. Hence, a strong FM interlayer coupling
would be beneficial to achieve uniform switching behavior of
a SrRuO3-based multilayer. Previous studies reported that
the coupling of two SrRuO3 layers separated by a non-FM
oxide spacer is at best weakly FM and the two FM layers
switch at markedly different fields. Here we study the
magnetic interlayer coupling between two FM SrRuO3 layers
separated by ultrathin LaNiO3 in epitaxial heterostructures
grown on SrTiO3(100) single crystals. We found that FM
SrRuO3 layers separated by 2 monolayers (MLs) thick LaNiO3
show weak FM interlayer coupling of about 106μJ/m2 at 10 K.
The coupling becomes strongly FM for four MLs thick (about
1.6 nm) LaNiO3 spacers and the two SrRuO3 layers reverse
their magnetization at a common value of the perpendicular
magnetic field. This is likely due to a transition of the
LaNiO3 spacer from insulating to metallic, as its thickness
increases.},
cin = {ER-C-1},
ddc = {530},
cid = {I:(DE-Juel1)ER-C-1-20170209},
pnm = {5351 - Platform for Correlative, In Situ and Operando
Characterization (POF4-535)},
pid = {G:(DE-HGF)POF4-5351},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000691685400002},
doi = {10.1103/PhysRevB.104.064444},
url = {https://juser.fz-juelich.de/record/897408},
}