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@ARTICLE{Tsukamoto:858694,
author = {Tsukamoto, Shigeru and Ono, Tomoya and Blügel, Stefan},
title = {{I}mprovement of accuracy in the wave-function-matching
method for transport calculations},
journal = {Physical review / B},
volume = {97},
number = {11},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2018-07539},
pages = {115450},
year = {2018},
abstract = {The wave-function-matching (WFM) technique for
first-principles transport-property calculations was
bettered by Sørensen et al. so as to exclude rapidly
decreasing evanescent waves [Sørensen et al., Phys. Rev. B
77, 155301 (2008)]. In their method, the translational
invariance of the transmission probability is not preserved
when moving the matching planes between electrode and
transition regions, and the sum of transmission and
reflection probabilities does not agree with the number of
transport channels in the transition region. The lack of the
translational invariance is caused by the overlap of the
layers between the electrode and transition regions. We
reformulate the WFM method by removing the layer overlap,
and the translational invariance of the transmission
probability becomes preserved. On the other hand, the error
in the sum of transmission and reflection probabilities is
attributed to using pseudoinverses that is accompanied by
the exclusion of rapidly decreasing evanescent waves. We
introduce a formulation to calculate the
transmission/reflection probability without the
pseudoinverses, resulting in that the sum of the
transmission and reflection probabilities exactly agrees
with the number of channels, and the accuracy is largely
improved. In addition, we prove that the accuracy in the
transmission probability obtained by our WFM technique is
comparable to that obtained by a nonequilibrium Green's
function method. Furthermore, we carry out electron
transport calculations on two-dimensional graphene sheets
embedded with B-N line defects sandwiched between a pair of
semi-infinite graphene electrodes and find the dependence of
the electron transmission on the transverse momentum
perpendicular to the transport direction.},
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) / 143 -
Controlling Configuration-Based Phenomena (POF3-143) /
Hybrid 2D-based interfaces from first principles
$(jias1e_20180501)$},
pid = {G:(DE-HGF)POF3-142 / G:(DE-HGF)POF3-143 /
$G:(DE-Juel1)jias1e_20180501$},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000428501200006},
doi = {10.1103/PhysRevB.97.115450},
url = {https://juser.fz-juelich.de/record/858694},
}