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@ARTICLE{Mokrousov:46232,
author = {Mokrousov, Y. and Bihlmayer, G. and Blügel, S.},
title = {{F}ull-potential linearized augmented plane-wave method for
one-dimensional systems: {G}old nanowire and iron monowires
in a gold tube},
journal = {Physical review / B},
volume = {72},
number = {4},
issn = {1098-0121},
address = {College Park, Md.},
publisher = {APS},
reportid = {PreJuSER-46232},
pages = {045402},
year = {2005},
note = {Record converted from VDB: 12.11.2012},
abstract = {We present an implementation of the full-potential
linearized augmented plane-wave (FLAPW) method for carrying
out ab initio calculations of the ground state electronic
properties of (magnetic) metallic nanowires and nanotubes
based on the density-functional theory (DFT). The method is
truly one-dimensional, uses explicitly a wire geometry and
is realized as an extension of the FLEUR code. It includes a
wide variety of chiral symmetries known for tubular and
other one-dimensional systems. A comparative study shows
that in this geometry computations are considerably faster
than the widely used supercell approach. The method was
applied to some typical model structures explored in the
field of nanospintronics: the gold nanowire Au(6,0), the
free-standing Fe monowire, and the hybrid structure
Fe@Au(6,0). Their atomic structures are determined by total
energy minimization and force calculations. We calculated
the magnetic properties including the magnetocrystalline
anisotropy energies, the band structures, and densities of
states in these systems using the local density
approximation (LDA) and the generalized gradient
approximation (GGA) to the DFT. The results agree nicely
with the data available in the literature. We found that Fe
wires are ferromagnetic and are prone to a Peierls
dimerization. The Fe filled gold nanotube shows a large
negative spin polarization at the Fermi level, which makes
this structure a possible candidate for spin-dependent
transport applications in the field of spintronics. The Au
tube encasing the Fe wire changes the magnetization
direction of the Fe wire and increases the
magnetocrystalline anisotropy energy by an order of
magnitude.},
keywords = {J (WoSType)},
cin = {IFF-TH-I / CNI},
ddc = {530},
cid = {I:(DE-Juel1)VDB30 / I:(DE-Juel1)VDB381},
pnm = {Kondensierte Materie},
pid = {G:(DE-Juel1)FUEK242},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000230890300141},
doi = {10.1103/PhysRevB.72.045402},
url = {https://juser.fz-juelich.de/record/46232},
}