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@ARTICLE{Bode:56495,
author = {Bode, M. and Heide, M. and von Bergmann, K. and Ferriani,
P. and Heinze, S. and Bihlmayer, G. and Kubetzka, A. and
Pietzsch, O. and Blügel, S. and Wiesendanger, R.},
title = {{C}hiral magnetic order at surfaces driven by inversion
asymmetry},
journal = {Nature},
volume = {447},
issn = {0028-0836},
address = {London [u.a.]},
publisher = {Nature Publising Group},
reportid = {PreJuSER-56495},
pages = {190 - 193},
year = {2007},
note = {Record converted from VDB: 12.11.2012},
abstract = {Chirality is a fascinating phenomenon that can manifest
itself in subtle ways, for example in biochemistry (in the
observed single-handedness of biomolecules) and in particle
physics (in the charge-parity violation of electroweak
interactions). In condensed matter, magnetic materials can
also display single-handed, or homochiral, spin structures.
This may be caused by the Dzyaloshinskii-Moriya interaction,
which arises from spin-orbit scattering of electrons in an
inversion-asymmetric crystal field. This effect is typically
irrelevant in bulk metals as their crystals are inversion
symmetric. However, low-dimensional systems lack structural
inversion symmetry, so that homochiral spin structures may
occur. Here we report the observation of magnetic order of a
specific chirality in a single atomic layer of manganese on
a tungsten (110) substrate. Spin-polarized scanning
tunnelling microscopy reveals that adjacent spins are not
perfectly antiferromagnetic but slightly canted, resulting
in a spin spiral structure with a period of about 12 nm. We
show by quantitative theory that this chiral order is caused
by the Dzyaloshinskii-Moriya interaction and leads to a
left-rotating spin cycloid. Our findings confirm the
significance of this interaction for magnets in reduced
dimensions. Chirality in nanoscale magnets may play a
crucial role in spintronic devices, where the spin rather
than the charge of an electron is used for data transmission
and manipulation. For instance, a spin-polarized current
flowing through chiral magnetic structures will exert a
spin-torque on the magnetic structure, causing a variety of
excitations or manipulations of the magnetization and giving
rise to microwave emission, magnetization switching, or
magnetic motors.},
keywords = {J (WoSType)},
cin = {IFF-1 / JARA-FIT / JARA-SIM},
ddc = {070},
cid = {I:(DE-Juel1)VDB781 / $I:(DE-82)080009_20140620$ /
I:(DE-Juel1)VDB1045},
pnm = {Kondensierte Materie},
pid = {G:(DE-Juel1)FUEK414},
shelfmark = {Multidisciplinary Sciences},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:17495922},
UT = {WOS:000246338700039},
doi = {10.1038/nature05802},
url = {https://juser.fz-juelich.de/record/56495},
}