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First-principle simulations of electronic structure in semicrystalline polyethylene

In order to increase our fundamental knowledge about high-voltage cable insulation materials, realistic polyethylene (PE) structures, generated with a novel molecular modeling strategy, have been analyzed using first principle electronic structure simulations. The PE structures were constructed by f...

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Autores principales: Moyassari, A., Unge, M., Hedenqvist, M. S., Gedde, U. W., Nilsson, F.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: AIP Publishing LLC 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5440234/
https://www.ncbi.nlm.nih.gov/pubmed/28571365
http://dx.doi.org/10.1063/1.4983650
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author Moyassari, A.
Unge, M.
Hedenqvist, M. S.
Gedde, U. W.
Nilsson, F.
author_facet Moyassari, A.
Unge, M.
Hedenqvist, M. S.
Gedde, U. W.
Nilsson, F.
author_sort Moyassari, A.
collection PubMed
description In order to increase our fundamental knowledge about high-voltage cable insulation materials, realistic polyethylene (PE) structures, generated with a novel molecular modeling strategy, have been analyzed using first principle electronic structure simulations. The PE structures were constructed by first generating atomistic PE configurations with an off-lattice Monte Carlo method and then equilibrating the structures at the desired temperature and pressure using molecular dynamics simulations. Semicrystalline, fully crystalline and fully amorphous PE, in some cases including crosslinks and short-chain branches, were analyzed. The modeled PE had a structure in agreement with established experimental data. Linear-scaling density functional theory (LS-DFT) was used to examine the electronic structure (e.g., spatial distribution of molecular orbitals, bandgaps and mobility edges) on all the materials, whereas conventional DFT was used to validate the LS-DFT results on small systems. When hybrid functionals were used, the simulated bandgaps were close to the experimental values. The localization of valence and conduction band states was demonstrated. The localized states in the conduction band were primarily found in the free volume (result of gauche conformations) present in the amorphous regions. For branched and crosslinked structures, the localized electronic states closest to the valence band edge were positioned at branches and crosslinks, respectively. At 0 K, the activation energy for transport was lower for holes than for electrons. However, at room temperature, the effective activation energy was very low (∼0.1 eV) for both holes and electrons, which indicates that the mobility will be relatively high even below the mobility edges and suggests that charge carriers can be hot carriers above the mobility edges in the presence of a high electrical field.
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spelling pubmed-54402342017-06-13 First-principle simulations of electronic structure in semicrystalline polyethylene Moyassari, A. Unge, M. Hedenqvist, M. S. Gedde, U. W. Nilsson, F. J Chem Phys ARTICLES In order to increase our fundamental knowledge about high-voltage cable insulation materials, realistic polyethylene (PE) structures, generated with a novel molecular modeling strategy, have been analyzed using first principle electronic structure simulations. The PE structures were constructed by first generating atomistic PE configurations with an off-lattice Monte Carlo method and then equilibrating the structures at the desired temperature and pressure using molecular dynamics simulations. Semicrystalline, fully crystalline and fully amorphous PE, in some cases including crosslinks and short-chain branches, were analyzed. The modeled PE had a structure in agreement with established experimental data. Linear-scaling density functional theory (LS-DFT) was used to examine the electronic structure (e.g., spatial distribution of molecular orbitals, bandgaps and mobility edges) on all the materials, whereas conventional DFT was used to validate the LS-DFT results on small systems. When hybrid functionals were used, the simulated bandgaps were close to the experimental values. The localization of valence and conduction band states was demonstrated. The localized states in the conduction band were primarily found in the free volume (result of gauche conformations) present in the amorphous regions. For branched and crosslinked structures, the localized electronic states closest to the valence band edge were positioned at branches and crosslinks, respectively. At 0 K, the activation energy for transport was lower for holes than for electrons. However, at room temperature, the effective activation energy was very low (∼0.1 eV) for both holes and electrons, which indicates that the mobility will be relatively high even below the mobility edges and suggests that charge carriers can be hot carriers above the mobility edges in the presence of a high electrical field. AIP Publishing LLC 2017-05-28 2017-05-22 /pmc/articles/PMC5440234/ /pubmed/28571365 http://dx.doi.org/10.1063/1.4983650 Text en © 2017 Author(s). 0021-9606/2017/146(20)/204901/11/$0.00 All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle ARTICLES
Moyassari, A.
Unge, M.
Hedenqvist, M. S.
Gedde, U. W.
Nilsson, F.
First-principle simulations of electronic structure in semicrystalline polyethylene
title First-principle simulations of electronic structure in semicrystalline polyethylene
title_full First-principle simulations of electronic structure in semicrystalline polyethylene
title_fullStr First-principle simulations of electronic structure in semicrystalline polyethylene
title_full_unstemmed First-principle simulations of electronic structure in semicrystalline polyethylene
title_short First-principle simulations of electronic structure in semicrystalline polyethylene
title_sort first-principle simulations of electronic structure in semicrystalline polyethylene
topic ARTICLES
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5440234/
https://www.ncbi.nlm.nih.gov/pubmed/28571365
http://dx.doi.org/10.1063/1.4983650
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