Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps

Accurate computational predictions of band gaps are of practical importance to the modeling and development of semiconductor technologies, such as (opto)electronic devices and photoelectrochemical cells. Among available electronic-structure methods, density-functional theory (DFT) with the Hubbard &...

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Main Authors: Nicole E. Kirchner-Hall, Wayne Zhao, Yihuang Xiong, Iurii Timrov, Ismaila Dabo
Format: Article
Language:English
Published: MDPI AG 2021-03-01
Series:Applied Sciences
Subjects:
Online Access:https://www.mdpi.com/2076-3417/11/5/2395
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author Nicole E. Kirchner-Hall
Wayne Zhao
Yihuang Xiong
Iurii Timrov
Ismaila Dabo
author_facet Nicole E. Kirchner-Hall
Wayne Zhao
Yihuang Xiong
Iurii Timrov
Ismaila Dabo
author_sort Nicole E. Kirchner-Hall
collection DOAJ
description Accurate computational predictions of band gaps are of practical importance to the modeling and development of semiconductor technologies, such as (opto)electronic devices and photoelectrochemical cells. Among available electronic-structure methods, density-functional theory (DFT) with the Hubbard <i>U</i> correction (DFT+<i>U</i>) applied to band edge states is a computationally tractable approach to improve the accuracy of band gap predictions beyond that of DFT calculations based on (semi)local functionals. At variance with DFT approximations, which are not intended to describe optical band gaps and other excited-state properties, DFT+<i>U</i> can be interpreted as an approximate spectral-potential method when <i>U</i> is determined by imposing the piecewise linearity of the total energy with respect to electronic occupations in the Hubbard manifold (thus removing self-interaction errors in this subspace), thereby providing a (heuristic) justification for using DFT+<i>U</i> to predict band gaps. However, it is still frequent in the literature to determine the Hubbard <i>U</i> parameters semiempirically by tuning their values to reproduce experimental band gaps, which ultimately alters the description of other total-energy characteristics. Here, we present an extensive assessment of DFT+<i>U</i> band gaps computed using self-consistent <i>ab initio U</i> parameters obtained from density-functional perturbation theory to impose the aforementioned piecewise linearity of the total energy. The study is carried out on 20 compounds containing transition-metal or <i>p</i>-block (group III-IV) elements, including oxides, nitrides, sulfides, oxynitrides, and oxysulfides. By comparing DFT+<i>U</i> results obtained using nonorthogonalized and orthogonalized atomic orbitals as Hubbard projectors, we find that the predicted band gaps are extremely sensitive to the type of projector functions and that the orthogonalized projectors give the most accurate band gaps, in satisfactory agreement with experimental data. This work demonstrates that DFT+<i>U</i> may serve as a useful method for high-throughput workflows that require reliable band gap predictions at moderate computational cost.
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spelling doaj.art-40e90d3db253458fa1edb25e458decc72023-12-03T13:01:03ZengMDPI AGApplied Sciences2076-34172021-03-01115239510.3390/app11052395Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band GapsNicole E. Kirchner-Hall0Wayne Zhao1Yihuang Xiong2Iurii Timrov3Ismaila Dabo4Department of Materials Science and Engineering and the Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USADepartment of Materials Science and Engineering and the Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USADepartment of Materials Science and Engineering and the Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USATheory and Simulation of Materials (THEOS) and National Centre for Computational Design and Discovery of Novel Materials (MARVEL), École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, SwitzerlandDepartment of Materials Science and Engineering and the Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USAAccurate computational predictions of band gaps are of practical importance to the modeling and development of semiconductor technologies, such as (opto)electronic devices and photoelectrochemical cells. Among available electronic-structure methods, density-functional theory (DFT) with the Hubbard <i>U</i> correction (DFT+<i>U</i>) applied to band edge states is a computationally tractable approach to improve the accuracy of band gap predictions beyond that of DFT calculations based on (semi)local functionals. At variance with DFT approximations, which are not intended to describe optical band gaps and other excited-state properties, DFT+<i>U</i> can be interpreted as an approximate spectral-potential method when <i>U</i> is determined by imposing the piecewise linearity of the total energy with respect to electronic occupations in the Hubbard manifold (thus removing self-interaction errors in this subspace), thereby providing a (heuristic) justification for using DFT+<i>U</i> to predict band gaps. However, it is still frequent in the literature to determine the Hubbard <i>U</i> parameters semiempirically by tuning their values to reproduce experimental band gaps, which ultimately alters the description of other total-energy characteristics. Here, we present an extensive assessment of DFT+<i>U</i> band gaps computed using self-consistent <i>ab initio U</i> parameters obtained from density-functional perturbation theory to impose the aforementioned piecewise linearity of the total energy. The study is carried out on 20 compounds containing transition-metal or <i>p</i>-block (group III-IV) elements, including oxides, nitrides, sulfides, oxynitrides, and oxysulfides. By comparing DFT+<i>U</i> results obtained using nonorthogonalized and orthogonalized atomic orbitals as Hubbard projectors, we find that the predicted band gaps are extremely sensitive to the type of projector functions and that the orthogonalized projectors give the most accurate band gaps, in satisfactory agreement with experimental data. This work demonstrates that DFT+<i>U</i> may serve as a useful method for high-throughput workflows that require reliable band gap predictions at moderate computational cost.https://www.mdpi.com/2076-3417/11/5/2395DFT+<i>U</i>Hubbard correctionLöwdin orthogonalizationband gapself-interaction
spellingShingle Nicole E. Kirchner-Hall
Wayne Zhao
Yihuang Xiong
Iurii Timrov
Ismaila Dabo
Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
Applied Sciences
DFT+<i>U</i>
Hubbard correction
Löwdin orthogonalization
band gap
self-interaction
title Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
title_full Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
title_fullStr Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
title_full_unstemmed Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
title_short Extensive Benchmarking of DFT+<i>U</i> Calculations for Predicting Band Gaps
title_sort extensive benchmarking of dft i u i calculations for predicting band gaps
topic DFT+<i>U</i>
Hubbard correction
Löwdin orthogonalization
band gap
self-interaction
url https://www.mdpi.com/2076-3417/11/5/2395
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