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Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate

[Image: see text] Scanning electron microscopy (SEM) is widely used to observe graphene on metal substrates. However, the origin of the SEM image contrast of graphene is not well understood. In this work, we performed in situ SEM imaging of layer-number-controlled graphene on a Ni substrate using a...

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Autores principales: Shihommatsu, Kota, Takahashi, Junro, Momiuchi, Yuta, Hoshi, Yudai, Kato, Hiroki, Homma, Yoshikazu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2017
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6645151/
https://www.ncbi.nlm.nih.gov/pubmed/31457340
http://dx.doi.org/10.1021/acsomega.7b01550
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author Shihommatsu, Kota
Takahashi, Junro
Momiuchi, Yuta
Hoshi, Yudai
Kato, Hiroki
Homma, Yoshikazu
author_facet Shihommatsu, Kota
Takahashi, Junro
Momiuchi, Yuta
Hoshi, Yudai
Kato, Hiroki
Homma, Yoshikazu
author_sort Shihommatsu, Kota
collection PubMed
description [Image: see text] Scanning electron microscopy (SEM) is widely used to observe graphene on metal substrates. However, the origin of the SEM image contrast of graphene is not well understood. In this work, we performed in situ SEM imaging of layer-number-controlled graphene on a Ni substrate using a high-pass energy filter for secondary electrons. We found that the graphene layer contrast was maximized at 15–20 eV, corresponding to the π–σ* interband transition in graphene. Our results indicate that the SEM image of graphene is produced by attenuation of the electrons emitted from the metal substrate by the monoatomic layers of graphene.
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spelling pubmed-66451512019-08-27 Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate Shihommatsu, Kota Takahashi, Junro Momiuchi, Yuta Hoshi, Yudai Kato, Hiroki Homma, Yoshikazu ACS Omega [Image: see text] Scanning electron microscopy (SEM) is widely used to observe graphene on metal substrates. However, the origin of the SEM image contrast of graphene is not well understood. In this work, we performed in situ SEM imaging of layer-number-controlled graphene on a Ni substrate using a high-pass energy filter for secondary electrons. We found that the graphene layer contrast was maximized at 15–20 eV, corresponding to the π–σ* interband transition in graphene. Our results indicate that the SEM image of graphene is produced by attenuation of the electrons emitted from the metal substrate by the monoatomic layers of graphene. American Chemical Society 2017-11-13 /pmc/articles/PMC6645151/ /pubmed/31457340 http://dx.doi.org/10.1021/acsomega.7b01550 Text en Copyright © 2017 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes.
spellingShingle Shihommatsu, Kota
Takahashi, Junro
Momiuchi, Yuta
Hoshi, Yudai
Kato, Hiroki
Homma, Yoshikazu
Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title_full Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title_fullStr Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title_full_unstemmed Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title_short Formation Mechanism of Secondary Electron Contrast of Graphene Layers on a Metal Substrate
title_sort formation mechanism of secondary electron contrast of graphene layers on a metal substrate
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6645151/
https://www.ncbi.nlm.nih.gov/pubmed/31457340
http://dx.doi.org/10.1021/acsomega.7b01550
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