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@ARTICLE{Prajapat:861839,
author = {Prajapat, C. L. and Singh, Surendra and Bhattacharya, D.
and Ravikumar, G. and Basu, S. and Mattauch, S. and Zheng,
Jian-Guo and Aoki, T. and Paul, Amitesh},
title = {{P}roximity effects across oxide-interfaces of
superconductor-insulator-ferromagnet hybrid heterostructure},
journal = {Scientific reports},
volume = {8},
number = {1},
issn = {2045-2322},
address = {[London]},
publisher = {Macmillan Publishers Limited, part of Springer Nature},
reportid = {FZJ-2019-02266},
pages = {3732},
year = {2018},
abstract = {A case study of electron tunneling or
charge-transfer-driven orbital ordering in superconductor
(SC)-ferromagnet (FM) interfaces has been conducted in
heteroepitaxial YBa2Cu3O7(YBCO)/La0.67Sr0.33MnO3(LSMO)
multilayers interleaved with and without an insulating
SrTiO3(STO) layer between YBCO and LSMO. X-ray magnetic
circular dichroism experiments revealed anti-parallel
alignment of Mn magnetic moments and induced Cu magnetic
moments in a YBCO/LSMO multilayer. As compared to an
isolated LSMO layer, the YBCO/LSMO multilayer displayed a
$(50\%)$ weaker Mn magnetic signal, which is related to the
usual proximity effect. It was a surprise that a similar
proximity effect was also observed in a YBCO/STO/LSMO
multilayer, however, the Mn signal was reduced by $20\%.$
This reduced magnetic moment of Mn was further verified by
depth sensitive polarized neutron reflectivity. Electron
energy loss spectroscopy experiment showed the evidence of
Ti magnetic polarization at the interfaces of the
YBCO/STO/LSMO multilayer. This crossover magnetization is
due to a transfer of interface electrons that migrate from
Ti(4+)−δ to Mn at the STO/LSMO interface and to Cu2+ at
the STO/YBCO interface, with hybridization via O 2p
orbitals. So charge-transfer driven orbital ordering is the
mechanism responsible for the observed proximity effect and
Mn-Cu anti-parallel coupling in YBCO/STO/LSMO. This work
provides an effective pathway in understanding the aspect of
long range proximity effect and consequent orbital
degeneracy parameter in magnetic coupling.},
cin = {JCNS-FRM-II / JCNS-2},
ddc = {600},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106},
pnm = {6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich Centre for
Neutron Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)MARIA-20140101},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:29487317},
UT = {WOS:000426151800065},
doi = {10.1038/s41598-018-22036-y},
url = {https://juser.fz-juelich.de/record/861839},
}