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@ARTICLE{Mlynczak:889937,
author = {Mlynczak, Ewa and Aguilera, Irene and Gospodaric, Pika and
Heider, T. and Jugovac, M. and Zamborlini, G. and Tusche, C.
and Suga, Shigemasa and Feyer, V. and Blügel, S. and
Plucinski, L. and Schneider, C. M.},
title = {{S}pin-polarized quantized electronic structure of
{F}e(001) with symmetry breaking due to the magnetization
direction},
journal = {Physical review / B},
volume = {103},
number = {3},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2021-00543},
pages = {035134},
year = {2021},
abstract = {Quantum well states formed by d electrons in metallic thin
films are responsible for many fundamental phenomena that
oscillate with layer thickness, such as magnetic anisotropy
or magnetoresistance. Using momentum microscopy and
angle-resolved photoemission, we mapped in unprecedented
detail the quantized electronic states of Fe(001) in a broad
photon energy range starting from soft x-ray (160 eV) down
to vacuum ultraviolet (8.4 eV). We show that it is possible
to simulate the experimentally observed photoemission
spectra with high accuracy by using the ab initio electronic
bulk band structure as the initial state, taking into
account that free electron final electronic states are
intrinsically broadened along the wave vector direction
perpendicular to the sample surface. To simulate the
thin-film case, we take into account a subset of the initial
electronic states, which results in the reproduction of the
quantized electronic structure observed in the experiment.
In addition, we present results of the spin-sensitive
measurements, which are confronted with the photoemission
simulation that takes into account the spin degree of
freedom. We demonstrate electronic states that can be
responsible for the oscillations of the magnetic anisotropy
in Fe(001) thin films with periods of about 5 and 9
monolayers. We show that these quantum well states change
position in reciprocal space depending on the magnetization
direction. Our photoemission simulation reproduces this
effect, which highlights its origin in the relativistic bulk
electronic band structure of bcc Fe. We also observed
magnetization-dependent spin-orbit gaps with the symmetry
lower than the bulk symmetry. We believe that the same
method of simulating photoemission spectra might facilitate
interpretation of the photoemission intensities measured for
other three-dimensional materials, especially when the
spin-polarized quantized electronic states are considered.},
cin = {IAS-1 / PGI-1 / JARA-FIT / JARA-HPC / PGI-6 / IEK-5},
ddc = {530},
cid = {I:(DE-Juel1)IAS-1-20090406 / I:(DE-Juel1)PGI-1-20110106 /
$I:(DE-82)080009_20140620$ / $I:(DE-82)080012_20140620$ /
I:(DE-Juel1)PGI-6-20110106 / I:(DE-Juel1)IEK-5-20101013},
pnm = {5211 - Topological Matter (POF4-521)},
pid = {G:(DE-HGF)POF4-5211},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000609013000002},
doi = {10.1103/PhysRevB.103.035134},
url = {https://juser.fz-juelich.de/record/889937},
}