The Basics of Electronic Structure Theory for Periodic Systems

When density functional theory is used to describe the electronic structure of periodic systems, the application of Bloch's theorem to the Kohn-Sham wavefunctions greatly facilitates the calculations. In this paper of the series, the concepts needed to model infinite systems are introduced. The...

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Main Authors: Peter Kratzer, Jörg Neugebauer
Format: Article
Language:English
Published: Frontiers Media S.A. 2019-03-01
Series:Frontiers in Chemistry
Subjects:
Online Access:https://www.frontiersin.org/article/10.3389/fchem.2019.00106/full
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spelling doaj-7ce246e99eac4c529540ee08845728da2020-11-24T21:16:17ZengFrontiers Media S.A.Frontiers in Chemistry2296-26462019-03-01710.3389/fchem.2019.00106436184The Basics of Electronic Structure Theory for Periodic SystemsPeter Kratzer0Jörg Neugebauer1Faculty of Physics, University of Duisburg-Essen, Duisburg, GermanyMax-Planck-Institut für Eisenforschung, Düsseldorf, GermanyWhen density functional theory is used to describe the electronic structure of periodic systems, the application of Bloch's theorem to the Kohn-Sham wavefunctions greatly facilitates the calculations. In this paper of the series, the concepts needed to model infinite systems are introduced. These comprise the unit cell in real space, as well as its counterpart in reciprocal space, the Brillouin zone. Grids for sampling the Brillouin zone and finite k-point sets are discussed. For metallic systems, these tools need to be complemented by methods to determine the Fermi energy and the Fermi surface. Various schemes for broadening the distribution function around the Fermi energy are presented and the approximations involved are discussed. In order to obtain an interpretation of electronic structure calculations in terms of physics, the concepts of bandstructures and atom-projected and/or orbital-projected density of states are useful. Aspects of convergence with the number of basis functions and the number of k-points need to be addressed specifically for each physical property. The importance of this issue will be exemplified for force constant calculations and simulations of finite-temperature properties of materials. The methods developed for periodic systems carry over, with some reservations, to less symmetric situations by working with a supercell. The chapter closes with an outlook to the use of supercell calculations for surfaces and interfaces of crystals.https://www.frontiersin.org/article/10.3389/fchem.2019.00106/fulldensity functional theoryhigh-throughput calculationsBrillouin zone samplingsupercell approachconvergence testssolid-state chemistry techniques
collection DOAJ
language English
format Article
sources DOAJ
author Peter Kratzer
Jörg Neugebauer
spellingShingle Peter Kratzer
Jörg Neugebauer
The Basics of Electronic Structure Theory for Periodic Systems
Frontiers in Chemistry
density functional theory
high-throughput calculations
Brillouin zone sampling
supercell approach
convergence tests
solid-state chemistry techniques
author_facet Peter Kratzer
Jörg Neugebauer
author_sort Peter Kratzer
title The Basics of Electronic Structure Theory for Periodic Systems
title_short The Basics of Electronic Structure Theory for Periodic Systems
title_full The Basics of Electronic Structure Theory for Periodic Systems
title_fullStr The Basics of Electronic Structure Theory for Periodic Systems
title_full_unstemmed The Basics of Electronic Structure Theory for Periodic Systems
title_sort basics of electronic structure theory for periodic systems
publisher Frontiers Media S.A.
series Frontiers in Chemistry
issn 2296-2646
publishDate 2019-03-01
description When density functional theory is used to describe the electronic structure of periodic systems, the application of Bloch's theorem to the Kohn-Sham wavefunctions greatly facilitates the calculations. In this paper of the series, the concepts needed to model infinite systems are introduced. These comprise the unit cell in real space, as well as its counterpart in reciprocal space, the Brillouin zone. Grids for sampling the Brillouin zone and finite k-point sets are discussed. For metallic systems, these tools need to be complemented by methods to determine the Fermi energy and the Fermi surface. Various schemes for broadening the distribution function around the Fermi energy are presented and the approximations involved are discussed. In order to obtain an interpretation of electronic structure calculations in terms of physics, the concepts of bandstructures and atom-projected and/or orbital-projected density of states are useful. Aspects of convergence with the number of basis functions and the number of k-points need to be addressed specifically for each physical property. The importance of this issue will be exemplified for force constant calculations and simulations of finite-temperature properties of materials. The methods developed for periodic systems carry over, with some reservations, to less symmetric situations by working with a supercell. The chapter closes with an outlook to the use of supercell calculations for surfaces and interfaces of crystals.
topic density functional theory
high-throughput calculations
Brillouin zone sampling
supercell approach
convergence tests
solid-state chemistry techniques
url https://www.frontiersin.org/article/10.3389/fchem.2019.00106/full
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