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@ARTICLE{Lin:859718,
author = {Lin, S.-C. and Kuo, C.-T. and Comes, R. B. and Rault, J. E.
and Rueff, J.-P. and Nemsak, Slavomir and Taleb, A. and
Kortright, J. B. and Meyer-Ilse, J. and Gullikson, E. and
Sushko, P. V. and Spurgeon, S. R. and Gehlmann, M. and
Bowden, M. E. and Plucinski, L. and Chambers, S. A. and
Fadley, C. S.},
title = {{I}nterface properties and built-in potential profile of a
{L}a{C}r {O} 3 / {S}r{T}i {O} 3 superlattice determined by
standing-wave excited photoemission spectroscopy},
journal = {Physical review / B},
volume = {98},
number = {16},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2019-00555},
pages = {165124},
year = {2018},
abstract = {LaCrO3(LCO)/SrTiO3(STO) heterojunctions are intriguing due
to a polar discontinuity along [001], exhibiting two
distinct and controllable charged interface structures
[(LaO)+/(TiO2)0 and (SrO)0/(CrO2)−] with induced
polarization, and a resulting depth-dependent potential. In
this study, we have used soft- and hard-x-ray standing-wave
excited photoemission spectroscopy (SW-XPS) to
quantitatively determine the elemental depth profile,
interface properties, and depth distribution of the
polarization-induced built-in potentials. We observe an
alternating charged interface configuration: a positively
charged (LaO)+/(TiO2)0 intermediate layer at the
LCOtop/STObottom interface and a negatively charged
(SrO)0/(CrO2)− intermediate layer at the STOtop/LCObottom
interface. Using core-level SW data, we have determined the
depth distribution of species, including through the
interfaces, and these results are in excellent agreement
with scanning transmission electron microscopy and electron
energy-loss spectroscopy mapping of local structure and
composition. SW-XPS also enabled deconvolution of the LCO
and STO contributions to the valence-band (VB) spectra.
Using a two-step analytical approach involving first
SW-induced core-level binding-energy shifts and then VB
modeling, the variation in potential across the complete
superlattice is determined in detail. This potential is in
excellent agreement with density functional theory models,
confirming this method as a generally useful tool for
interface studies.},
cin = {PGI-6},
ddc = {530},
cid = {I:(DE-Juel1)PGI-6-20110106},
pnm = {522 - Controlling Spin-Based Phenomena (POF3-522)},
pid = {G:(DE-HGF)POF3-522},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000447302700007},
doi = {10.1103/PhysRevB.98.165124},
url = {https://juser.fz-juelich.de/record/859718},
}