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    Kubo–Greenwood electrical conductivity formulation and implementation for projector augmented wave datasets

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    KGECpaper.v6b.pdf
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    Final Accepted Manuscript
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    Author
    Calderín, L.
    Karasiev, V.V.
    Trickey, S.B.
    Affiliation
    Department of Materials Science and Engineering, University of Arizona, Tucson
    Issue Date
    2017-12
    Keywords
    Electron transport
    Kubo-Greenwood
    Electrical conductivity
    Kohn-Sham density functional theory
    Plane wave
    Projector augmented wave
    
    Metadata
    Show full item record
    Publisher
    ELSEVIER SCIENCE BV
    Citation
    Kubo–Greenwood electrical conductivity formulation and implementation for projector augmented wave datasets 2017, 221:118 Computer Physics Communications
    Journal
    Computer Physics Communications
    Rights
    © 2017 Elsevier B.V. All rights reserved.
    Collection Information
    This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.
    Abstract
    As the foundation for a new computational implementation, we survey the calculation of the complex electrical conductivity tensor based on the Kubo-Greenwood (KG) formalism (Kubo, 1957; Greenwood, 1958), with emphasis on derivations and technical aspects pertinent to use of projector augmented wave datasets with plane wave basis sets (BIlichl, 1994). New analytical results and a full implementation of the KG approach in an open-source Fortran 90 post-processing code for use with Quantum Espresso (Giannozzi et al., 2009) are presented. Named KGEC ([K]ubo [G]reenwood [E]lectronic [C]onductivity), the code calculates the full complex conductivity tensor (not just the average trace). It supports use of either the original KG formula or the popular one approximated in terms of a Dirac delta function. It provides both Gaussian and Lorentzian representations of the Dirac delta function (though the Lorentzian is preferable on basic grounds). KGEC provides decomposition of the conductivity into intra- and inter band contributions as well as degenerate state contributions. It calculates the dc conductivity tensor directly. It is MPI parallelized over k-points, bands, and plane waves, with an option to recover the plane wave processes for their use in band parallelization as well. It is designed to provide rapid convergence with respect to k-point density. Examples of its use are given.
    Note
    Pre-print submitted, no embargo.
    ISSN
    00104655
    DOI
    10.1016/j.cpc.2017.08.008
    Version
    Final accepted manuscript
    Sponsors
    U.S. Dept. of Energy [DE-SC0002139]
    Additional Links
    http://linkinghub.elsevier.com/retrieve/pii/S0010465517302539
    ae974a485f413a2113503eed53cd6c53
    10.1016/j.cpc.2017.08.008
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