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Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin

The excitation spectrum in the region of the intraband (Dirac plasmon) and interband ([Formula: see text] plasmon) plasmons in graphene/Pt-skin terminated Pt [Formula: see text] Ni(111) is reproduced by using an ab-initio method and an empirical model. The results of both methods are compared with e...

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Autores principales: Despoja, Vito, Radović, Ivan, Politano, Antonio, Mišković, Zoran L.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7221714/
https://www.ncbi.nlm.nih.gov/pubmed/32276378
http://dx.doi.org/10.3390/nano10040703
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author Despoja, Vito
Radović, Ivan
Politano, Antonio
Mišković, Zoran L.
author_facet Despoja, Vito
Radović, Ivan
Politano, Antonio
Mišković, Zoran L.
author_sort Despoja, Vito
collection PubMed
description The excitation spectrum in the region of the intraband (Dirac plasmon) and interband ([Formula: see text] plasmon) plasmons in graphene/Pt-skin terminated Pt [Formula: see text] Ni(111) is reproduced by using an ab-initio method and an empirical model. The results of both methods are compared with experimental data. We discover that metallic screening by the Pt layer converts the square-root dispersion of the Dirac plasmon into a linear acoustic-like plasmon dispersion. In the long-wavelength limit, the Pt d electron excitations completely quench the [Formula: see text] plasmon in graphene at about [Formula: see text] eV, that is replaced by a broad peak at about 6 eV. Owing to a rather large graphene/Pt-skin separation (≈3.3 Å), the graphene/Pt-skin hybridization becomes weak at larger wave vectors, so that the [Formula: see text] plasmon is recovered with a dispersion as in a free-standing graphene.
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spelling pubmed-72217142020-05-21 Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin Despoja, Vito Radović, Ivan Politano, Antonio Mišković, Zoran L. Nanomaterials (Basel) Article The excitation spectrum in the region of the intraband (Dirac plasmon) and interband ([Formula: see text] plasmon) plasmons in graphene/Pt-skin terminated Pt [Formula: see text] Ni(111) is reproduced by using an ab-initio method and an empirical model. The results of both methods are compared with experimental data. We discover that metallic screening by the Pt layer converts the square-root dispersion of the Dirac plasmon into a linear acoustic-like plasmon dispersion. In the long-wavelength limit, the Pt d electron excitations completely quench the [Formula: see text] plasmon in graphene at about [Formula: see text] eV, that is replaced by a broad peak at about 6 eV. Owing to a rather large graphene/Pt-skin separation (≈3.3 Å), the graphene/Pt-skin hybridization becomes weak at larger wave vectors, so that the [Formula: see text] plasmon is recovered with a dispersion as in a free-standing graphene. MDPI 2020-04-08 /pmc/articles/PMC7221714/ /pubmed/32276378 http://dx.doi.org/10.3390/nano10040703 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Despoja, Vito
Radović, Ivan
Politano, Antonio
Mišković, Zoran L.
Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title_full Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title_fullStr Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title_full_unstemmed Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title_short Insights on the Excitation Spectrum of Graphene Contacted with a Pt Skin
title_sort insights on the excitation spectrum of graphene contacted with a pt skin
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7221714/
https://www.ncbi.nlm.nih.gov/pubmed/32276378
http://dx.doi.org/10.3390/nano10040703
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