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@ARTICLE{Ishida:860515,
author = {Ishida, H. and Liebsch, A. and Wortmann, D.},
title = {{T}opological invariants of band insulators derived from
the local-orbital based embedding potential},
journal = {Physical review / B},
volume = {96},
number = {12},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2019-01251},
pages = {125413},
year = {2017},
abstract = {We demonstrate that topological invariants of band
insulators can be derived efficiently from the eigenvalues
of the local-orbital (LO) based embedding potential, called
also the contact (lead) self-energy. The LO based embedding
potential is a bulk quantity. Given the tight-binding
Hamiltonian describing the bulk valence and conduction
bands, it is constructed straightforwardly from the bulk
wave functions satisfying the generalized Bloch condition.
When the one-electron energy ɛ is located within a
projected bulk band gap at a given planar wave vector k, the
embedding potential becomes Hermitian. Its real eigenvalues
exhibit distinctly different behavior depending on the
topological properties of the valence bands, thus enabling
unambiguous identification of bulk topological invariants.
We consider the Bernevig-Hughes-Zhang model as an example of
a time-reversal invariant topological insulator and tin
telluride (SnTe) crystallized in a rock-salt structure as an
example of a topological crystalline insulator},
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 = {143 - Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000410178600009},
doi = {10.1103/PhysRevB.96.125413},
url = {https://juser.fz-juelich.de/record/860515},
}