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dc.contributor.authorCalderín, L.
dc.contributor.authorKarasiev, V.V.
dc.contributor.authorTrickey, S.B.
dc.date.accessioned2017-11-23T01:57:41Z
dc.date.available2017-11-23T01:57:41Z
dc.date.issued2017-12
dc.identifier.citationKubo–Greenwood electrical conductivity formulation and implementation for projector augmented wave datasets 2017, 221:118 Computer Physics Communicationsen
dc.identifier.issn00104655
dc.identifier.doi10.1016/j.cpc.2017.08.008
dc.identifier.urihttp://hdl.handle.net/10150/626127
dc.description.abstractAs 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.
dc.description.sponsorshipU.S. Dept. of Energy [DE-SC0002139]en
dc.language.isoenen
dc.publisherELSEVIER SCIENCE BVen
dc.relation.urlhttp://linkinghub.elsevier.com/retrieve/pii/S0010465517302539en
dc.rights© 2017 Elsevier B.V. All rights reserved.en
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/
dc.subjectElectron transporten
dc.subjectKubo-Greenwooden
dc.subjectElectrical conductivityen
dc.subjectKohn-Sham density functional theoryen
dc.subjectPlane waveen
dc.subjectProjector augmented waveen
dc.titleKubo–Greenwood electrical conductivity formulation and implementation for projector augmented wave datasetsen
dc.typeArticleen
dc.contributor.departmentDepartment of Materials Science and Engineering, University of Arizona, Tucsonen
dc.identifier.journalComputer Physics Communicationsen
dc.description.notePre-print submitted, no embargo.en
dc.description.collectioninformationThis 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.en
dc.eprint.versionFinal accepted manuscripten
refterms.dateFOA2018-05-18T10:00:28Z
html.description.abstractAs 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.


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