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@ARTICLE{Rodrigo:877690,
author = {Rodrigo, Rebecca and Faley, M. I. and Dunin-Borkowski,
Rafal},
title = {{N}ano{SQUID}s based on {N}b nanobridges},
journal = {Journal of physics / Conference Series},
volume = {1559},
number = {1},
issn = {1742-6588},
address = {Bristol},
publisher = {IOP Publ.87703},
reportid = {FZJ-2020-02400},
pages = {012011},
year = {2020},
abstract = {Atomic-scale imaging of interfacial polarizationin
cuprate-titanate heterostructuresCite as: Appl. Phys. Lett.
116, 251603 (2020); doi: 10.1063/5.0011081Submitted: 17
April 2020 . Accepted: 7 June 2020 .Published Online: 23
June 2020Shao-Bo Mi,1,a) Tian Yao,1 Shao-Dong Cheng,1,2
Micheal I. Faley,3 Ulrich Poppe,3 Lu Lu,1,2 Dawei
Wang,1,2and Chun-Lin Jia1,2,3AFFILIATIONS1State Key
Laboratory for Mechanical Behavior of Materials, Xi’an
Jiaotong University, Xi’an 710049, China2School of
Microelectronics, Xi’an Jiaotong University, Xi’an
710049, China3Ernst Ruska Centre for Microscopy and
Spectroscopy with Electrons and Peter Gr€unberg
Institute,ForschungszentrumJ€ulich, D-52425 J€ulich,
Germanya)Author to whom correspondence should be addressed:
shaobo.mi@xjtu.edu.cnABSTRACTThe interfaces in oxide
heterostructures that bring novel physical phenomena and
functionalities have attracted great attention infundamental
research and device applications. For uncovering
structure–property relationships of oxide
heterostructures, direct evidence ofthe atomic-scale
structure of heterointerfaces is highly desired. Here, we
report on studying the structure of interfaces between
YBa2Cu3O7-dthin films and SrTiO3 substrates by means of
aberration-corrected ultrahigh-resolution electron
microscopy. Employing advanced imagingand spectroscopic
techniques, shifts of atoms at the interface away from the
regular lattice sites are measured, leading to the
interfacial polarity.The local polarization induced by the
atomic shifts directs toward the cuprate films and is
estimated to be about 36.1 lC/cm2. Theobserved interfacial
polar layer is understood by the special atomic
configuration across the interface, which could modulate the
electricalproperties in superconducting devices that are
based on the ferroelectric/superconductor
heterosystems.Published under license by AIP Publishing.
https://doi.org/10.1063/5.0011081Heterostructures of
perovskite-based oxide materials haveattracted extensive
attention from both fundamental research andtechnological
applications because of their variety of fascinating
physicalproperties.1,2 It has been demonstrated that
interfaces in thedesigned heterostructures have striking
properties, which do not existin either of the constituent
bulk materials, e.g., 2D electron gas at theLaAlO3/SrTiO3
(LAO/STO) interface.3,4 In addition, the functionalitiesof
the perovskite-based oxide epitaxial layers can be modulated
bythe field effect arising from the adjacent layers or/and
the interfacecoupling in heterostructures (e.g., proximity
effects in superconductor–ferromagnet
heterostructures).5–7 Among the
perovskite-basedheterostructures, strongly
electron-correlated materials are of essentialimportance due
to their applications in superconducting
field-effectdevices, e.g., high-temperature superconducting
(HTS) ultrathin filmsgrown on insulating STO
substrates.8–10 In these heterostructures, thecritical
temperature (Tc) and phase transitions of the HTS
cupratefilms can be tuned by an external electric field
without involvingchemical and crystalline modulation of the
materials. Also, it wasreported that the Tc of the ultrathin
HTS films can be shifted by thecharge carriers, which are
injected by the dielectric gate polarizationunder an applied
electric field and thus leading to a suppression
ofsuperconductivity in the ultrathin HTS films.11–14The
Thomas–Fermi screening length (kTF) of YBa2Cu3O7-d(YBCO)
is on the order of 1nm.15 Therefore, the interface
couplingbetween the dielectric gate and the YBCO films has
importanteffect on shifting Tc of the ultrathin YBCO films.
In particular, theinterfacial polarity of the
heterostructures has been expected tochange the doping level
and thus to affect the superconductivity ofthe
unit-cell-thick HTS cuprate films.16 Although the
experimentaland theoretical investigations have been
performed on studyingHTS heterostructures,9,10,17–19 the
interfacial atomic arrangementof superconducting/insulating
heterostructures, including reconstructions,relaxations,
interatomic mixing, and distortions, is necessaryto be
clarified for a deep insight into the mechanismsbehind the
experimentally measured interface-related properties.In this
work, we provide the atomic-scale interface structure
ofYBCO/STO(001) obtained by using high-resolution imaging
andspectroscopic techniques of aberration-corrected
transmissionelectron microscopy (TEM) and scanning
transmission electronmicroscopy (STEM).Appl. Phys. Lett.
116, 251603 (2020); doi: 10.1063/5.0011081 116,
251603-1Published under license by AIP PublishingApplied
Physics Letters ARTICLE scitation.org/journal/apl},
cin = {ER-C-1 / PGI-5},
ddc = {530},
cid = {I:(DE-Juel1)ER-C-1-20170209 / I:(DE-Juel1)PGI-5-20110106},
pnm = {144 - Controlling Collective States (POF3-144) / 143 -
Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000558737600011},
doi = {10.1088/1742-6596/1559/1/012011},
url = {https://juser.fz-juelich.de/record/877690},
}