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Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material

[Image: see text] Ferroelectricity ( J. ValasekPhys. Rev.1921, 17, 475), a spontaneous formation of electric polarization, is a solid state phenomenon, usually, associated with ionic compounds or complex materials. Here we show that, atypically for elemental solids, few-layer graphenes can host an e...

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Autores principales: Garcia-Ruiz, Aitor, Enaldiev, Vladimir, McEllistrim, Andrew, Fal’ko, Vladimir I.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10214444/
https://www.ncbi.nlm.nih.gov/pubmed/37158207
http://dx.doi.org/10.1021/acs.nanolett.2c04723
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author Garcia-Ruiz, Aitor
Enaldiev, Vladimir
McEllistrim, Andrew
Fal’ko, Vladimir I.
author_facet Garcia-Ruiz, Aitor
Enaldiev, Vladimir
McEllistrim, Andrew
Fal’ko, Vladimir I.
author_sort Garcia-Ruiz, Aitor
collection PubMed
description [Image: see text] Ferroelectricity ( J. ValasekPhys. Rev.1921, 17, 475), a spontaneous formation of electric polarization, is a solid state phenomenon, usually, associated with ionic compounds or complex materials. Here we show that, atypically for elemental solids, few-layer graphenes can host an equilibrium out-of-plane electric polarization, switchable by sliding the constituent graphene sheets. The systems hosting such effect include mixed-stacking tetralayers and thicker (5–9 layers) rhombohedral graphitic films with a twin boundary in the middle of a flake. The predicted electric polarization would also appear in marginally (small-angle) twisted few-layer flakes, where lattice reconstruction would give rise to networks of mesoscale domains with alternating value and sign of out-of-plane polarization.
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spelling pubmed-102144442023-05-27 Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material Garcia-Ruiz, Aitor Enaldiev, Vladimir McEllistrim, Andrew Fal’ko, Vladimir I. Nano Lett [Image: see text] Ferroelectricity ( J. ValasekPhys. Rev.1921, 17, 475), a spontaneous formation of electric polarization, is a solid state phenomenon, usually, associated with ionic compounds or complex materials. Here we show that, atypically for elemental solids, few-layer graphenes can host an equilibrium out-of-plane electric polarization, switchable by sliding the constituent graphene sheets. The systems hosting such effect include mixed-stacking tetralayers and thicker (5–9 layers) rhombohedral graphitic films with a twin boundary in the middle of a flake. The predicted electric polarization would also appear in marginally (small-angle) twisted few-layer flakes, where lattice reconstruction would give rise to networks of mesoscale domains with alternating value and sign of out-of-plane polarization. American Chemical Society 2023-05-09 /pmc/articles/PMC10214444/ /pubmed/37158207 http://dx.doi.org/10.1021/acs.nanolett.2c04723 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Garcia-Ruiz, Aitor
Enaldiev, Vladimir
McEllistrim, Andrew
Fal’ko, Vladimir I.
Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title_full Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title_fullStr Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title_full_unstemmed Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title_short Mixed-Stacking Few-Layer Graphene as an Elemental Weak Ferroelectric Material
title_sort mixed-stacking few-layer graphene as an elemental weak ferroelectric material
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10214444/
https://www.ncbi.nlm.nih.gov/pubmed/37158207
http://dx.doi.org/10.1021/acs.nanolett.2c04723
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