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@PHDTHESIS{Bhatnagar:893740,
author = {Bhatnagar, Tanvi},
title = {{R}esolving interface effects in voltage controlled
magnetic heterostructures using advanced neutron scattering
and electron microscopy methods},
volume = {251},
school = {RWTH Aachen University},
type = {Dissertation},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2021-02795},
isbn = {978-3-95806-604-5},
series = {Schriften des Forschungszentrums Jülich Reihe
Schlüsseltechnologien / Key Technologies},
pages = {ix, 171},
year = {2021},
note = {Dissertation, RWTH Aachen University, 2021},
abstract = {Voltage control of magnetism (VCM) shows a strong potential
to impact the fieldof magnetic data storage and spintronic
devices with low power consumption. Withthis as an aim,
La0.7Sr0.3MnO3/Pb(Mg1/3Nb2/3)O3 - PbTiO3 (LSMO/PMN-PT
(001))heterostructure is deposited using oxide molecular
beam epitaxy. LSMO is ferromagneticat room temperature.
Grown on a piezoelectric /ferroelectric
substratePMN-PT(001), it forms an artificial multiferroic
heterostructure. This system wasstructurally characterized
using different techniques revealing growth of epitaxialLSMO
layers. The main part of this thesis focuses on the
investigation of magnetoelectriccoupling in
LSMO/PMN-PT(001). The measurements show change inthe nature
of ME coupling, by varying different parameters like
temperature anddirection of magnetization. In all
experiments the voltage is applied along [001] direction.The
magnetoelectric coupling in LSMO/PMN-PT(001) arises due to
strainand charge coupling. Since the substrate PMN-PT is
piezoelectric and ferroelectric,both strain effect and
switching of ferroelectric polarizations contribute to the
MEcoupling. Impact of both mechanism is visible in the
measurements. Strain couplingis dominant along hard axis
[100] of LSMO whereas charge coupling shows dominancealong
easy axis [110] of LSMO. Using polarized neutron
reflectometry (PNR),the magnetic depth profile as a function
of applied voltage reveals the presence ofan interlayer with
reduced nuclear scattering length density and magnetic
scatteringlength density. Examining this interlayer with
scanning transmission electronmicroscopy (STEM) and energy
dispersive X-ray spectroscopy (EDS) shows Ladeficiencyand
excess of Mn near the interface with the dark regions to be
particleswith a triangular cross-section. The stoichiometry
of these particles is confirmedwith field cooled-cooling
(FCC) curve which shows a jump in magnetization near
theCurie temperature TC = 43K of Mn3O4. The formation of
these particles is favoredwhen the LSMO films are strongly
strained which leads to defects near the interface.STEM
images shows the presence of defects near the interface.
Real-space magneticfield mapping as a function of
temperature is performed using off-axis electron
holographyon LSMO/PMN-PT(001) which demonstrates uniform
magnetic field in theLSMO films. The magnetic phase gradient
reduces with increasing temperature depictingreduction in
the magnetic field in LSMO layer with temperature. Based
onsimilar approach, a second heterostructure,
La0.7Sr0.3MnO3/ BaTiO3/ Nb:SrTiO3(LSMO/BTO/Nb:STO (001)) is
deposited using high oxygen pressure sputteringsystem and
oxide molecular beam epitaxy. Here, LSMO is a ferromagnetic
component,BTO layer is ferroelectric and Nb:STO is used a
conductive substrate. Thegrowth of this structure is a
two-step process. The BTO layer is grown in thehigh oxygen
pressure sputtering system using growth parameters optimized
duringa growth study.},
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 / EXP:(DE-MLZ)TREFF-20140101},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/893740},
}