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@article{marzari-prb97,
Author = {Marzari, N. and Vanderbilt, D.},
Title = {Maximally localized generalized Wannier functions for
composite energy bands},
Journal = {Phys. Rev. B},
Volume = {56},
Pages = {12847},
Abstract = {We discuss a method for determining the optimally
localized set of generalized Wannier functions
associated with a set of Bloch bands in a
crystalline solid. By ''generalized Wannier
functions'' we mean a set of localized orthonormal
orbitals spanning the same space as the specified
set of Bloch bands. Although we minimize a
functional that represents the total spread
Sigma(n)(r(2))(n) - (r)(n)(2) of the Wannier
functions in real space, our method proceeds
directly from the Bloch functions as represented on
a mesh of k points, and carries out the minimization
in a space of unitary matrices U-mn((k)) describing
the rotation among the Bloch bands at each k
point. The method is thus suitable for use in
connection with conventional electronic-structure
codes. The procedure also returns the total electric
polarization as well as the location of each Wannier
center. Sample results for Si, GaAs, molecular C2H4,
and LiCl will be presented.},
Year = {1997},
}
@article{souza-prb01,
Author = {Souza, I. and Marzari, N. and Vanderbilt, D.},
Title = {Maximally localized Wannier functions for entangled energy bands},
Journal = {Phys. Rev. B},
Volume = {65},
Pages = {035109},
Abstract = {We present a method for obtaining well-localized
Wannier-like functions (WF's) for energy bands that
are attached to or mixed with other bands. The
present scheme removes the limitation of the usual
maximally localized WF's method [N. Marzari and
D. Vanderbilt, Phys. Rev. B 56, 12 847 (1997)] that
the bands of interest should form an isolated group,
separated by gaps from higher and lower bands
everywhere in the Brillouin zone. An energy window
encompassing N bands of interest is specified by the
user, and the algorithm then proceeds to disentangle
these from the remaining bands inside the window by
filtering out an optimally connected N-dimensional
subspace. This is achieved by minimizing a
functional that measures the subspace dispersion
across the Brillouin zone. The maximally localized
WF's for the optimal subspace are then obtained via
the algorithm of Marzari and Vanderbilt. The method,
which functions as a postprocessing step using the
output of conventional electronic-structure codes,
is applied to the s and d bands of copper, and to
the valence and low-lying conduction bands of
silicon. For the low-lying nearly-free-electron
bands of copper we find WF's which are centered at
the tetrahedral-interstitial sites, suggesting an
alternative tight-binding parametrization.},
Year = {2001}
}
@article{mostofi-cpc08,
Author = {Mostofi, A. A. and Yates, J. R. and Lee, Y.-S. and Souza,
I. and Vanderbilt, D. and Marzari, N.},
Title = {wannier90: A tool for obtaining maximally-localised Wannier
functions},
Journal = {Comput. Phys. Commun.},
Volume = {178},
Pages = {685},
Abstract = {We present wannier90, a program for calculating
maximally-localised Wannier functions (MLWF) from a
set of Bloch energy bands that may or may not be
attached to or mixed with other bands. The formalism
works by minimising the total spread of the MLWF in
real space. This is done in the space of unitary
matrices that describe rotations of the Bloch bands
at each k-point. As a result, wannier90 is
independent of the basis set used in the underlying
calculation to obtain the Bloch states. Therefore,
it may be interfaced straightforwardly to any
electronic structure code. The locality of MLWF can
be exploited to compute band-structure, density of
states and Fermi surfaces at modest computational
cost. Furthermore, wannier90 is able to output MLWF
for visualisation and other post-processing
purposes. Wannier functions are already used in a
wide variety of applications. These include analysis
of chemical bonding in real space; calculation of
dielectric properties via the modem theory of
polarisation; and as an accurate and minimal basis
set in the construction of model Hamiltonians for
large-scale systems, in linear-scaling quantum Monte
Carlo calculations, and for efficient computation of
material properties, such as the anomalous Hall
coefficient. wannier90 is freely available under the
GNU General Public License from
http://www.wannier.org/. Program summary Program
title: wannier90 Catalogue identifier: AEAK_v1_0
Program summary URL:
http://cpc.cs.qub.ac.uk/summaries/AEAK_v1_0.html
Program obtainable from: CPC Program Library,
Queen's University, Belfast, N. Ireland Licensing
provisions: Standard CPC licence,
http://cpc.cs.qub.ac.uk/licence/licence.html No. of
lines in distributed program, including test data,
etc.: 556 495 No. of bytes in distributed program,
including test data, etc.: 5 709 419 Distribution
format: tar.gz Programming language: Fortran 90,
perl Computer: any architecture with a Fortran 90
compiler Operating system: Linux, Windows, Solaris,
AIX, Tru64 Unix, OSX RAM: 10 MB Word size: 32 or 64
Classification: 7.3 External routines: BLAS
(http://www/netlib.oi-g/blas). LAPACK
(http://www.netlib.org/lapack). Both available under
open-source licenses. Nature of problem: Obtaining
maximally-localised Wannier functions from a set of
Bloch energy bands that may or may not be
entangled. Solution method: In the case of entangled
bands, the optimally-connected subspace of interest
is determined by minimising a functional which
measures the subspace dispersion across the
Brillouin zone. The maximally-localised Wannier
functions within this subspace are obtained by
subsequent minimisation of a functional that
represents the total spread of the Wannier functions
in real space. For the case of isolated energy bands
only the second step of the procedure is
required. Unusual features: Simple and user-friendly
input system. Wannier functions and interpolated
band structure output in a variety of file formats
for visualisation. Running time: Test cases take 1
minute. References: [1] N. Marzari, D. Vanderbilt,
Maximally localized generalized Wannier functions
for composite energy bands, Phys. Rev. B 56 (1997)
12847. [2] I. Souza, N. Marzari, D. Vanderbilt,
Maximally localized Wannier functions for entangled
energy bands, Phys. Rev. B 65 (2001) 035109. (C)
2007 Elsevier B.V. All rights reserved.},
Year = {2008}
}
@article{wang-prb06,
Author = {Wang, X. and Yates, J. R. and Souza, I. and Vanderbilt, D.},
Title = {Ab initio calculation of the anomalous Hall conductivity by
Wannier interpolation},
Journal = {Phys. Rev. B},
Volume = {74},
Pages = {195118},
Abstract = {The intrinsic anomalous Hall conductivity in ferromagnets
depends on subtle spin-orbit-induced effects in the
electronic structure, and recent ab initio studies
found that it was necessary to sample the Brillouin
zone at millions of k-points to converge the
calculation. We present an efficient
first-principles approach for computing this
quantity. We start out by performing a conventional
electronic-structure calculation including
spin-orbit coupling on a uniform and relatively
coarse k-point mesh. From the resulting Bloch
states, maximally localized Wannier functions are
constructed which reproduce the ab initio states up
to the Fermi level. The Hamiltonian and
position-operator matrix elements, needed to
represent the energy bands and Berry curvatures, are
then set up between the Wannier orbitals. This
completes the first stage of the calculation,
whereby the low-energy ab initio problem is
transformed into an effective tight-binding
form. The second stage only involves Fourier
transforms and unitary transformations of the small
matrices setup in the first stage. With these
inexpensive operations, the quantities of interest
are interpolated onto a dense k-point mesh and used
to evaluate the anomalous Hall conductivity as a
Brillouin zone integral. The present scheme, which
also avoids the cumbersome summation over all
unoccupied states in the Kubo formula, is applied to
bcc Fe, giving excellent agreement with
conventional, less efficient first-principles
calculations. Remarkably, we find that about 99\% of
the effect can be recovered by keeping a set of
terms depending only on the Hamiltonian matrix
elements, not on matrix elements of the position
operator.},
Year = {2006}
}
@Article{yao-prl04,
author = {Y. Yao and L. Kleinman and A. H. MacDonald and J. Sinova and
T. Jungwirth and D.-S. Wang and E. Wang and Q. Niu},
title = {},
journal = {Phys. Rev. Lett.},
volume = {92},
pages = {037204},
year = {2004},
}
@article{lopez-prb12,
Author = {M.~G. Lopez and D. Vanderbilt and T. Thonhauser and I. Souza},
Title = {},
Journal = {Phys. Rev. B},
Volume = {85},
Pages = {014435},
Year = {2012}
}
@article{yates-prb07,
Author = {Yates, J. R. and Wang, X. and Vanderbilt, D. and Souza, I.},
Title = {Spectral and Fermi surface properties from Wannier interpolation},
Journal = {Phys. Rev. B},
Volume = {75},
Pages = {195121},
Abstract = {We present an efficient first-principles approach for
calculating Fermi surface averages and spectral
properties of solids, and use it to compute the
low-field Hall coefficient of several cubic metals
and the magnetic circular dichroism of iron. The
first step is to perform a conventional
first-principles calculation and store the low-lying
Bloch functions evaluated on a uniform grid of k
points in the Brillouin zone. We then map those
states onto a set of maximally localized Wannier
functions, and evaluate the matrix elements of the
Hamiltonian and the other needed operators between
the Wannier orbitals, thus setting up an "exact
tight-binding model." In this compact representation
the k-space quantities are evaluated inexpensively
using a generalized Slater-Koster
interpolation. Owing to the strong localization of
the Wannier orbitals in real space, the smoothness
and accuracy of the k-space interpolation increases
rapidly with the number of grid points originally
used to construct the Wannier functions. This allows
k-space integrals to be performed with ab initio
accuracy at low cost. In the Wannier representation,
band gradients, effective masses, and other k
derivatives needed for transport and optical
coefficients can be evaluated analytically,
producing numerically stable results even at band
crossings and near weak avoided crossings.},
Year = {2007}
}
@article{marzari-rmp12,
Author = {N. Marzari and A. A. Mostofi and J. R. Yates and I. Souza
and D. Vanderbilt},
Title = {},
Journal = {Rev. Mod. Phys.},
Volume = {84},
Pages = {1419},
Year = {2012}
}
@article{marzari-arxiv98,
Author = {N. Marzari and D. Vanderbilt},
Title = {},
Journal = {arXiv:9802210},
Volume = {},
Pages = {},
Year = {1998}
}
@article{vanderbilt-prb90,
Author = {D. Vanderbilt},
Title = {},
Journal = {Phys. Rev. B},
Volume = {41},
Pages = {7892},
Year = {1990}
}
@article{yao-prb07,
Author = {Y. Yao and Y. Liang and D. Xiao and Q. Niu and S.-Q. Shen
and X. Dai and Z. Fang},
Title = {},
Journal = {Phys. Rev. B},
Volume = {75},
Pages = {020401},
Year = {2007}
}
@article{lee-prl05,
Author = {Lee, Y.-S. and Nardelli, M. B. and Marzari, N.},
Title = {Band structure and quantum conductance of nanostructures from
maximally localized wannier functions: The case of
functionalized carbon nanotubes},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Pages = {076804},
Abstract = {We have combined large-scale, Gamma-point
electronic-structure calculations with the maximally
localized Wannier functions approach to calculate
efficiently the band structure and the quantum
conductance of complex systems containing thousands
of atoms while maintaining full first-principles
accuracy. We have applied this approach to study
covalent functionalizations in metallic
single-walled carbon nanotubes. We find that the
band structure around the Fermi energy is much less
dependent on the chemical nature of the ligands than
on the sp(3) functionalization pattern disrupting
the conjugation network. Common aryl
functionalizations are more stable when paired with
saturating hydrogens; even when paired, they still
act as strong scattering centers that degrade the
ballistic conductance of the nanotubes already at
low degrees of coverage.},
Year = {2005}
}
@misc{UserGuide,
author = {A.~A.~Mostofi and G.~Pizzi and I.~Souza and J.~R.~Yates},
year = {},
howpublished = " User Guide to {\tt wannier90}, available at
\url{http://www.wannier.org/user\_guide.html}"
}
@Article{xiao-rmp10,
title = {Berry phase effects on electronic properties},
author = {Xiao, Di and Chang, Ming-Che and Niu, Qian },
journal = {Rev. Mod. Phys.},
volume = {82},
pages = {1959--2007},
numpages = {48},
year = {2010},
month = {Jul},
doi = {10.1103/RevModPhys.82.1959},
publisher = {American Physical Society}
}
@article{ceresoli-prb06,
Author = {Ceresoli, D. and Thonhauser, T. and Vanderbilt, D. and
Resta, R.},
Title = {Orbital magnetization in crystalline solids: Multi-band
insulators, Chern insulators, and metals},
Journal = {Phys. Rev. B},
Volume = {74},
Pages = {024408},
Abstract = {We derive a multi-band formulation of the orbital
magnetization in a normal periodic insulator (i.e.,
one in which the Chern invariant, or in two
dimensions (2D) the Chern number,
vanishes). Following the approach used recently to
develop the single-band formalism [Thonhauser,
Ceresoli, Vanderbilt, and Resta,
Phys. Rev. Lett. 95, 137205 (2005)], we work in the
Wannier representation and find that the
magnetization is comprised of two contributions, an
obvious one associated with the internal circulation
of bulklike Wannier functions in the interior and an
unexpected one arising from net currents carried by
Wannier functions near the surface. Unlike the
single-band case, where each of these contributions
is separately gauge invariant, in the multi-band
formulation only the sum of both terms is gauge
invariant. Our final expression for the orbital
magnetization can be rewritten as a bulk property in
terms of Bloch functions, making it simple to
implement in modern code packages. The
reciprocal-space expression is evaluated for 2D
model systems and the results are verified by
comparing to the magnetization computed for finite
samples cut from the bulk. Finally, while our formal
proof is limited to normal insulators, we also
present a heuristic extension to Chern insulators
(having nonzero Chern invariant) and to metals. The
validity of this extension is again tested by
comparing to the magnetization of finite samples cut
from the bulk for 2D model systems. We find
excellent agreement, thus providing strong empirical
evidence in favor of the validity of the heuristic
formula.},
Year = {2006}
}
@article{nardelli-prb99,
title = {Electronic transport in extended systems: Application
to carbon nanotubes},
volume = {60},
journal = {Phys. Rev. B},
author = {Marco Buongiorno Nardelli},
year = {1999},
pages = {7828}
}
@article{gygi-cpc03,
Author = {Gygi, F. and Fattebert, J. L. and Schwegler, E.},
Title = {Computation of Maximally Localized Wannier Functions using a
simultaneous diagonalization algorithm},
Journal = {Comput. Phys. Commun.},
Volume = {155},
Pages = {1-6},
Abstract = {We show that a simultaneous diagonalization algorithm used
in signal processing applications can be used in the
context of electronic structure calculations to
efficiently compute Maximally Localized Wannier
Functions (MLWFs). Applications to calculations of
MLWFs in molecular and solid systems demonstrate the
efficiency of the approach. We also present and
discuss a parallel version of the algorithm. An
extension of the concept of MLWF to generalized
minimum spread wavefunctions is proposed. (C) 2003
Elsevier B.V. All rights reserved.},
Year = {2003}
}
@article{posternak-prb02,
Author = {Posternak, M. and Baldereschi, A. and Massidda, S. and
Marzari, N.},
Title = {Maximally localized Wannier functions in antiferromagnetic
MnO within the FLAPW formalism},
Journal = {Phys. Rev. B},
Volume = {65},
Pages = {184422},
Abstract = {We have calculated the maximally localized Wannier
functions of MnO in its antiferromagnetic (AFM)
rhombohedral unit cell, which contains two formula
units. Electron Bloch functions are obtained with
the linearized-augmented-plane-wave method within
both the local-spin density (LSD) and the LSD+U
schemes. The thirteen uppermost occupied spin-up
bands correspond in a pure ionic scheme to the five
Mn 3d orbitals at the Mn-1 (spin-up) site and the
four O 2s/2p orbitals at each of the O-1 and O-2
sites. Maximal localization identifies uniquely four
Wannier functions for each O, which are trigonally
distorted sp(3)-like orbitals. They display a weak
covalent bonding between O 2s/2p states and
minority-spin d states of Mn-2, which is absent in a
fully ionic picture. This bonding is the fingerprint
of the interaction responsible for the AFM ordering,
and its strength depends on the one-electron scheme
being used. The five Mn Wannier functions are
centered on the Mn-1 site, and are atomic orbitals
modified by the crystal field. They are not uniquely
defined by the criterion of maximal localization and
we choose them as the linear combinations that
diagonalize the r(2) operator, so that they display
the D-3d symmetry of the Mn-1 site.},
Year = {2002}
}
@book{grosso-book00,
author = "G. Grosso and G. P. Parravicini",
title = "Solid State Physics",
publisher = "Academic Press",
address = "",
year = 2000}
@book{ziman-book72,
author = "J. Ziman",
title = "Principles of the Theory of Solids",
edition = "2nd ed.",
publisher = "Cambridge University Press",
address = "",
year = 1972}
@Article{blount-ssp62,
author= {E. I. Blount},
journal = {Solid State Physics},
title = { },
volume = {13},
pages = {305},
year= {1962},
}
@Article{pizzi-cpc14,
author= {G. Pizzi and D. Volja and B. Kozinsky and M. Fornari and N. Marzari},
journal = {Comput. Phys. Commun.},
title = {BoltzWann: A code for the evaluation of thermoelectric and electronic transport properties with a maximally-localized Wannier functions basis},
volume = {185},
pages = {422},
year= {2014},
doi= {doi:10.1016/j.cpc.2013.09.015}
}
@InCollection{mahan-itc06,
author= {G. D. Mahan},
booktitle = {Intern. Tables for Crystallography},
title = {Transport properties},
volume = {D},
chapter = {1.8},
pages = {7828},
year= {2006},
}
@article{sakuma-prb13,
title = {Symmetry-adapted Wannier functions in the maximal localization procedure},
author = {Sakuma, R.},
journal = {Phys. Rev. B},
volume = {87},
pages = {235109},
year = {2013}
}
@ARTICLE{tsirkin-arxiv17,
author = {{Tsirkin}, S.~S. and {Aguado Puente}, P. and {Souza}, I.},
title = "{Gyrotropic effects in trigonal tellurium studied from first principles}",
journal = {ArXiv e-prints},
archivePrefix = "arXiv",
eprint = {1710.03204},
primaryClass = "cond-mat.mtrl-sci",
keywords = {Condensed Matter - Materials Science},
year = 2017,
month = oct,
adsurl = {http://adsabs.harvard.edu/abs/2017arXiv171003204T},
adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}
@Article{yoda-sr15,
author = {T. Yoda and T. Yokoyama and S. Murakami},
title = {Current-induced Orbital and Spin Magnetizations in Crystals with Helical Structure},
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