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@ARTICLE{Lounis:884767,
author = {Lounis, Samir},
title = {{M}ultiple-scattering approach for multi-spin chiral
magnetic interactions: application to the one- and
two-dimensional {R}ashba electron gas},
journal = {New journal of physics},
volume = {22},
number = {10},
issn = {1367-2630},
address = {[London]},
publisher = {IOP},
reportid = {FZJ-2020-03243},
pages = {103003},
year = {2020},
abstract = {Various multi-spin magnetic exchange interactions (MEI) of
chiral nature have been recently unveiled. Owing to their
potential impact on the realisation of twisted
spin-textures, their future implication in spintronics or
quantum computing is very promising. Here, I address the
long-range behavior of multi-spin MEI on the basis of a
multiple-scattering formalism implementable in Green
functions based methods such as the
Korringa–Kohn–Rostoker (KKR) Green function framework. I
consider the impact of spin–orbit coupling (SOC) as
described in the one- (1D) and two-dimensional (2D) Rashba
model, from which the analytical forms of the four- and
six-spin interactions are extracted and compared to the well
known bilinear isotropic, anisotropic and
Dzyaloshinskii–Moriya interactions (DMI). Similarly to the
DMI between two sites i and j, there is a four-spin chiral
vector perpendicular to the bond connecting the two sites.
The oscillatory behavior of the MEI and their decay as
function of interatomic distances are analysed and
quantified for the Rashba surfaces states characterizing Au
surfaces. The interplay of beating effects and strength of
SOC gives rise to a wide parameter space where chiral MEI
are more prominent than the isotropic ones. The multi-spin
interactions for a plaquette of N magnetic moments decay
like
${\left\{{q}_{\mathrm{F}}^{N-d}{P}^{\frac{1}{2}\left(d-1\right)}L\right\}}^{-1}$
simplifying to
${\left\{{q}_{\mathrm{F}}^{N-d}{R}^{\left[1+\frac{N}{2}\left(d-1\right)\right]}N\right\}}^{-1}$
for equidistant atoms, where d is the dimension of the
mediating electrons, q F the Fermi wave vector, L the
perimeter of the plaquette while P is the product of
interatomic distances. This recovers the behavior of the
bilinear MEI,
${\left\{{q}_{\mathrm{F}}^{2-d}{R}^{d}\right\}}^{-1}$, and
shows that increasing the perimeter of the plaquette weakens
the MEI. More important, the power-law pertaining to the
distance-dependent 1D MEI is insensitive to the number of
atoms in the plaquette in contrast to the linear dependence
associated with the 2D MEI. Furthermore, the N-dependence of
q F offers the possibility of tuning the interactions
amplitude by engineering the electronic occupation.},
cin = {IAS-1 / PGI-1 / JARA-FIT / JARA-HPC},
ddc = {530},
cid = {I:(DE-Juel1)IAS-1-20090406 / I:(DE-Juel1)PGI-1-20110106 /
$I:(DE-82)080009_20140620$ / $I:(DE-82)080012_20140620$},
pnm = {142 - Controlling Spin-Based Phenomena (POF3-142)},
pid = {G:(DE-HGF)POF3-142},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000576907700001},
doi = {10.1088/1367-2630/abb514},
url = {https://juser.fz-juelich.de/record/884767},
}