First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity

Density-functional perturbation theory (DFPT) is nowadays the method of choice for the accurate computation of linear and nonlinear-response properties of materials from first principles. A notable advantage of DFPT over alternative approaches is the possibility of treating incommensurate lattice di...

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Main Authors: Miquel Royo, Massimiliano Stengel
Format: Article
Language:English
Published: American Physical Society 2019-06-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.9.021050
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spelling doaj-9417b7f2672d4672bed0aaacd667bc0f2020-11-25T01:46:26ZengAmerican Physical SocietyPhysical Review X2160-33082019-06-019202105010.1103/PhysRevX.9.021050First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and FlexoelectricityMiquel RoyoMassimiliano StengelDensity-functional perturbation theory (DFPT) is nowadays the method of choice for the accurate computation of linear and nonlinear-response properties of materials from first principles. A notable advantage of DFPT over alternative approaches is the possibility of treating incommensurate lattice distortions with an arbitrary wave vector q at essentially the same computational cost as the lattice-periodic case. Here we show that q can be formally treated as a perturbation parameter and used in conjunction with the established results of perturbation theory (e.g., the “2n+1” theorem) to perform a long-wave expansion of an arbitrary response function in powers of the wave-vector components. This procedure provides a powerful general framework to access a wide range of spatial dispersion effects that were formerly difficult to calculate by means of first-principles electronic structure methods. In particular, the physical response to the spatial gradient of any external field can now be calculated at negligible cost by using the response functions to uniform perturbations (electric, magnetic, or strain fields) as the only input. We demonstrate our method by calculating the flexoelectric and dynamical quadrupole tensors of selected crystalline insulators and model systems.http://doi.org/10.1103/PhysRevX.9.021050
collection DOAJ
language English
format Article
sources DOAJ
author Miquel Royo
Massimiliano Stengel
spellingShingle Miquel Royo
Massimiliano Stengel
First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
Physical Review X
author_facet Miquel Royo
Massimiliano Stengel
author_sort Miquel Royo
title First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
title_short First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
title_full First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
title_fullStr First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
title_full_unstemmed First-Principles Theory of Spatial Dispersion: Dynamical Quadrupoles and Flexoelectricity
title_sort first-principles theory of spatial dispersion: dynamical quadrupoles and flexoelectricity
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2019-06-01
description Density-functional perturbation theory (DFPT) is nowadays the method of choice for the accurate computation of linear and nonlinear-response properties of materials from first principles. A notable advantage of DFPT over alternative approaches is the possibility of treating incommensurate lattice distortions with an arbitrary wave vector q at essentially the same computational cost as the lattice-periodic case. Here we show that q can be formally treated as a perturbation parameter and used in conjunction with the established results of perturbation theory (e.g., the “2n+1” theorem) to perform a long-wave expansion of an arbitrary response function in powers of the wave-vector components. This procedure provides a powerful general framework to access a wide range of spatial dispersion effects that were formerly difficult to calculate by means of first-principles electronic structure methods. In particular, the physical response to the spatial gradient of any external field can now be calculated at negligible cost by using the response functions to uniform perturbations (electric, magnetic, or strain fields) as the only input. We demonstrate our method by calculating the flexoelectric and dynamical quadrupole tensors of selected crystalline insulators and model systems.
url http://doi.org/10.1103/PhysRevX.9.021050
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