% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@INPROCEEDINGS{Rssmann:189302,
author = {Rüssmann, Philipp and Mavropoulos, Phivos and Long, Nguyen
Hoang and Bauer, David and Blügel, Stefan},
title = {{A}b initio description of quasiparicle spin interference
and time-reversal scattering processes off magnetic
impurties},
reportid = {FZJ-2015-02480},
year = {2014},
abstract = {In structure inversion-asymmetric environments such as
surfaces and interfaces the spin of quasiparticles can have
a profound effect on their interference. Quasiparticle
interference patterns measured typically by scanning
tunneling microscopy are not related in a trivial way to the
dispersion of the electronic states. In fact, for Bi(110)
[1] we could show that the observed interference patterns
can be interpreted only by taking spin-conserving scattering
events into account. In this contribution we go one step
further and include explicitly in the analysis the
scattering of single non-magnetic and magnetic impurities
with and without spin-orbit interaction. We present
density-functional calculations of the quasiparticle
interference at surfaces due to scattering off magnetic
adatoms. We consider two substrates Au(111) and a thin film
of Bi2Te3, a three-dimensional topological insulator
(3D-TI). Our focus is on 3d impurities on Au(111) where the
spin-orbit coupling (SOC) causes a Rashba-type splitting of
the surface. The spin polarization of the quasiparticle
waves shows a non-collinear behavior because of SOC. We
compare to previous model-based results [2] and discuss the
relation to the scattering properties of the impurity. As a
matter of principle, magnetic impurities at surfaces break
the topological protection in 3D-TI and we study this loss
of protection by taking into account time-reversed
transitions caused by the magnetic moment. In our
calculations we employ the KKR-Green function method for the
electronic structure and scattering properties at defects
[3, 4]. We acknowledge financial support from the DFG
(SPP-1666) and from the VITI project (DBB01126) of the
Helmholtz Association and computational support from the
JARA-HPC Supercomputing Centre at the RWTH Aachen
University. [1] J.I. Pascual, G. Bihlmayer, Yu. M. Koroteev,
H.-P. Rust, G. Ceballos, M. Hansmann, K. Horn, E. V.
Chulkov, S. Blügel, P. M. Echenique, and Ph. Hofmann Phys.
Rev. Lett. 93, 196802 (2004)[2] S. Lounis, A. Bringer, and
S. Blügel, Phys. Rev. Lett. 108, 207202 (2012).[3] S.
Heers, PhD Thesis, RWTH Aachen (2011); D.S.G. Bauer, PhD
Thesis, RWTH Aachen (2013), B. Zimmerman, PhD Thesis, RWTH
Aachen (2014)[4] N. H. Long, P. Mavropoulos, B. Zimmermann,
D. S. G. Bauer, S. Blügel, and Y. Mokrousov, Phys. Rev. B
90, 064406 (2014)},
month = {Nov},
date = {2014-11-12},
organization = {Topological and Dirac matter: from
modeling to imaging, Bordeaux (France),
12 Nov 2014 - 14 Nov 2014},
subtyp = {Other},
cin = {PGI-1 / IAS-1 / JARA-FIT},
cid = {I:(DE-Juel1)PGI-1-20110106 / I:(DE-Juel1)IAS-1-20090406 /
$I:(DE-82)080009_20140620$},
pnm = {422 - Spin-based and quantum information (POF2-422)},
pid = {G:(DE-HGF)POF2-422},
typ = {PUB:(DE-HGF)24},
url = {https://juser.fz-juelich.de/record/189302},
}