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@PHDTHESIS{Hanke:856628,
author = {Hanke, Jan-Philipp},
title = {{T}opological properties of complex magnets from an
advanced $\textit{ab-initio}$ {W}annier description},
volume = {183},
school = {RWTH Aachen},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2018-05994},
isbn = {978-3-95806-357-0},
series = {Schriften des Forschungszentrums Jülich. Reihe
Schlüsseltechnologien / Key Technologies},
pages = {XI, 173 S.},
year = {2018},
note = {RWTH Aachen, Diss., 2018},
abstract = {Berry phases impart an elegant interpretation of
fundamental condensed-matter phenomena as a direct
consequence of the electrons' adiabatic evolution under the
variation of control parameters. This thesis develops
advanced $\textit{ab initio}$ methods based ondensity
functional theory and applies them to investigate Berry
phase effects in complex magnets, rooting in the global
properties of two distinct types of phase spaces. The
non-trivial geometry of momentum space manifests in
intrinsic contributions to the anomalous Hall effect as well
as orbital magnetism in solids. While the former has been
subject to intensive research in the past decades, our
understanding of orbital magnetism in periodic systems is
still at a rather premature stage. Even its
quantum-mechanical description was elusive until the recent
advent of a rigorous but involved Berry phase theory, the
overall importance of which is unclear. To resolve this open
question, we implement the modern theory of orbital
magnetization within the full-potential linearized
augmented-plane-wave method that is known for its high
precision. By comparing to a commonly applied but simple
local approximation, we uncover in this thesis that the
Berry phase theory is crucial to predict reliably orbital
magnetism in systems studied extensively in spintronics,
including thin magnetic heterostructures and topological
magnets. Remarkably, we demonstrate that the emergent
magnetic field due to the chiral spin structure of
non-coplanar antiferromagnets constitutes an effcient
mechanism to lift the orbital degeneracy even in the absence
of spin-orbit coupling. In a new class of materials to which
we refer as topological orbital ferromagnets, the
macroscopic magnetization originates solely from pronounced
orbital magnetism due to non-local charge currents. We
identify promising candidates of film and bulk systems that
realize the predicted topological orbital magnetization,
without any reference to correlation or spin-orbit effects.
Paving the road towards innovative device architectures, the
burgeoning research field of spin-orbitronics exploits
relativistic phenomena to control electrically magnetism by
means of spin-orbit torques. Only recently, these torques
and the related Dzyaloshinskii-Moriya interaction were
recognized as innately geometrical effects that originate
from the global properties of a $\textit{mixed}$ phase space
entangling the crystal momentum with the magnetization
direction. However, the effcient treatment of such complex
higher-dimensional phase spaces sets a central challenge for
$\textit{ab initio}$ theory, calling for advanced
computational methods. This demand is met by a generalized
Wannier interpolation that we develop here in order to
describe Berry phase effects in generic parameter spaces
precisely. Using the scheme for spin torques and chiral
interactions in magnetic heterostructures, we correlate
their microscopic origin with the electronic structure, and
elucidate the role of chemical composition and disorder. In
addition, the developed formalism enables us to evaluate
effciently the dependence of these phenomena on the
magnetization direction, revealing large anisotropies in the
studied systems. Considering the interplay of magnetism and
topology, we uncover that magnetically induced band
crossings manifest in prominent magneto-electric responses
in magnetic insulators. We introduce the concept of mixed
Weyl semimetals to establish novel guiding principles for
engineering large spin-orbit torques in topologically
complex ferromagnets. Moreover, we show that topological
phase transitions in these materials are accompanied by
drastic changes of the local orbital chemistry.},
cin = {PGI-1 / IAS-1 / JARA-FIT / JARA-HPC},
cid = {I:(DE-Juel1)PGI-1-20110106 / I:(DE-Juel1)IAS-1-20090406 /
$I:(DE-82)080009_20140620$ / $I:(DE-82)080012_20140620$},
pnm = {142 - Controlling Spin-Based Phenomena (POF3-142)},
pid = {G:(DE-HGF)POF3-142},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/856628},
}