Hubbard U through polaronic defect states
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{
"revision": 5,
"id": "1587",
"created": "2022-12-15T20:58:48.755030+00:00",
"metadata": {
"doi": "10.24435/materialscloud:g7-0z",
"status": "published",
"title": "Hubbard U through polaronic defect states",
"mcid": "2023.4",
"license_addendum": null,
"_files": [
{
"description": "Atomic structures of the materials considered in this work",
"key": "structures.zip",
"size": 32706,
"checksum": "md5:e1e309ddf0677ecdd72016bc8202f810"
},
{
"description": "README file",
"key": "README.txt",
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"owner": 143,
"_oai": {
"id": "oai:materialscloud.org:1587"
},
"keywords": [
"Polarons",
"density-functional theory",
"DFT+U",
"hybrid functionals",
"self-interaction"
],
"conceptrecid": "1586",
"is_last": true,
"references": [
{
"type": "Journal reference",
"doi": "10.1038/s41524-022-00958-6",
"url": "https://doi.org/10.1038/s41524-022-00958-6",
"comment": "Paper in which the method is described",
"citation": "Falletta, S., Pasquarello, A. Hubbard U through polaronic defect states, npj Computational Materials 8, 263 (2022)"
}
],
"publication_date": "Jan 06, 2023, 11:10:29",
"license": "Creative Commons Attribution 4.0 International",
"id": "1587",
"description": "Since the preliminary work of Anisimov and co-workers, the Hubbard corrected DFT+U functional has been used for predicting properties of correlated materials by applying on-site effective Coulomb interactions to specific orbitals. However, the determination of the Hubbard U parameter has remained under intense discussion despite the multitude of approaches proposed. Here, we define a selection criterion based on the use of polaronic defect states for the enforcement of the piecewise linearity of the total energy upon electron occupation. A good agreement with results from piecewise-linear hybrid functionals is found for the electronic and structural properties of polarons, including the formation energies. The values of U determined in this way are found to give a robust description of the polaron energetics upon variation of the considered state. In particular, we also address a polaron hopping pathway, finding that the determined value of U leads to accurate energetics without requiring a configurational-dependent U. It is emphasized that the selection of U should be based on physical properties directly associated with the orbitals to which U is applied, rather than on more global properties such as band gaps and band widths. For comparison, we also determine U through a well-established linear-response scheme finding noticeably different values of U and consequently different formation energies. Possible origins of these discrepancies are discussed. As case studies, we consider the self-trapped electron in BiVO\u2084, the self-trapped hole in MgO, the Li-trapped hole in MgO, and the Al-trapped hole in \ud835\udefc-SiO\u2082.",
"version": 1,
"contributors": [
{
"email": "stefano.falletta@epfl.ch",
"affiliations": [
"Chaire de Simulation \u00e0 l'Echelle Atomique (CSEA), Ecole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland"
],
"familyname": "Falletta",
"givennames": "Stefano"
},
{
"email": "alfredo.pasquarello@epfl.ch",
"affiliations": [
"Chaire de Simulation \u00e0 l'Echelle Atomique (CSEA), Ecole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland"
],
"familyname": "Pasquarello",
"givennames": "Alfredo"
}
],
"edited_by": 576
},
"updated": "2023-01-06T10:10:30.007198+00:00"
}