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@ARTICLE{KAUSHIK:639292,
author = {KAUSHIK, SONIA and Raj, Rakhul and Gupta, Pooja and
Chumakov, Andrei and Schwartzkopf, Matthias and Reddy, V.
Raghavendra and Kumar, Dileep},
title = {{G}rowth-induced magnetic anisotropy in {C}o/{C}$_{60}$
bilayers: {I}nsights from a two-grain {S}toner-{W}ohlfarth
model},
journal = {Physical review / B},
volume = {111},
number = {18},
issn = {2469-9950},
address = {Woodbury, NY},
reportid = {PUBDB-2025-04393},
pages = {184426},
year = {2025},
abstract = {Organic spintronics has gained significant interest within
the scientific community due to its potential applications
in spin-valve devices. However, the realization of an
efficient room-temperature organic spin-valve device remains
elusive, primarily due to the complex spin transport at
metal-organic interfaces. Hence, the study of these
metal-organic bilayer interfaces is essential for the
conception of such devices. This study investigates the
Co-C$_{60}$ interface and its impact on the magnetic
properties of the Co layer. We examine the structural and
magnetic properties of ultrathin cobalt (Co) films deposited
on a fullerene (C$_{60}$) layer to understand the origin of
magnetic anisotropy in metal-organic bilayer structures. The
penetration of ferromagnetic Co atoms into the C$_{60}$ film
is confirmed through x-ray reflectivity and
secondary-ion-mass spectroscopy. Additionally, grazing
incidence small-angle x-ray scattering and atomic force
microscopy provide ample insights into the morphological
properties of the Co/C$_{60}$ bilayers. Grazing incidence
x-ray diffraction and grazing incidence wide-angle x-ray
scattering confirm the texturing of Co in the bilayer at
higher cobalt thicknesses. Angular-dependent magneto-optic
Kerr effect hysteresis measurements, with varying Co layer
thicknesses, reveal information about growth-induced
uniaxial magnetic anisotropy. Unlike inorganic silicon
substrates, where Co texturing and magnetic anisotropy are
absent, magnetic anisotropy in Co films begins to develop at
a thickness of 25 Å on the C$_{60}$ layer and increases
with further cobalt deposition. This texturing induces a
dispersion in magnetic anisotropy, leading to an anomalous
increase in coercivity and remanence along the hard axis.
The anomalous behavior in coercivity and remanence variation
along the nominal hard axis is explained by the two-grain
Stoner-Wohlfarth model and is further corroborated by the
nonuniform spatial distribution of magnetic domains observed
through Kerr microscopy. Our simulations show that these
magnetic anomalies arise due to the formation of local
energy minima in the energy landscape near the nominal hard
axis.},
cin = {FS-PETRA-D / DOOR ; HAS-User},
ddc = {530},
cid = {I:(DE-H253)FS-PETRA-D-20210408 /
I:(DE-H253)HAS-User-20120731},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G3 - PETRA III (DESY) (POF4-6G3) /
INDIA-DESY - INDIA-DESY Collaboration
$(2020_Join2-INDIA-DESY)$},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G3 /
$G:(DE-HGF)2020_Join2-INDIA-DESY$},
experiment = {EXP:(DE-H253)P-P03-20150101},
typ = {PUB:(DE-HGF)16},
doi = {10.1103/PhysRevB.111.184426},
url = {https://bib-pubdb1.desy.de/record/639292},
}