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Electric-Field Emission Mechanism in Q-Carbon Field Emitters

[Image: see text] In this paper, we report the excellent field emission properties of Q-carbon and analyze its field emission characteristics through structural, morphological, and electronic property correlations, supported by density functional theory (DFT) simulation studies. The Q-carbon field e...

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Autores principales: Haque, Ariful, Karmakar, Subrata, Trivedi, Ravi Kumar, Chakraborty, Brahmananda, Droopad, Ravi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10018518/
https://www.ncbi.nlm.nih.gov/pubmed/36936320
http://dx.doi.org/10.1021/acsomega.2c07576
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author Haque, Ariful
Karmakar, Subrata
Trivedi, Ravi Kumar
Chakraborty, Brahmananda
Droopad, Ravi
author_facet Haque, Ariful
Karmakar, Subrata
Trivedi, Ravi Kumar
Chakraborty, Brahmananda
Droopad, Ravi
author_sort Haque, Ariful
collection PubMed
description [Image: see text] In this paper, we report the excellent field emission properties of Q-carbon and analyze its field emission characteristics through structural, morphological, and electronic property correlations, supported by density functional theory (DFT) simulation studies. The Q-carbon field emitters show impressive and stable field emission properties, such as a low turn-on electric field of ∼2.38 V/μm, a high emission current density of ∼33 μA/cm(2), and a critical field of ∼2.44 V/μm for the transition from a linear region to the saturation region in the F–N plot. The outstanding field emission properties of Q-carbon are attributed to (i) a unique sp(2)/sp(3) mixture in Q-carbon, (ii) sp(2)-bonded highly conductive amorphous carbon-rich channels inside the Q-carbon cluster, (iii) a large local field enhancement due to the local geometry and microstructure of Q-carbon, and (iv) the presence of sp(2)-bonded amorphous carbon regions in the composite film. The temperature-dependent field emission properties, such as extreme sensitivity and an enhancement in the emission current density with temperature, can be explained by the local density of states near the Fermi level and the excellent thermal stability of the Q-carbon field emitters. From DFT simulation studies, the computed work function and the field-enhancement factor were determined to be 3.62 eV and ∼2300, respectively, which explains the excellent field emission characteristics of Q-carbon. The obtained field emission properties, in most cases, were superior to those from other carbon/diamond-based field emitters, which will open new frontiers in field emission-based electronic applications.
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spelling pubmed-100185182023-03-17 Electric-Field Emission Mechanism in Q-Carbon Field Emitters Haque, Ariful Karmakar, Subrata Trivedi, Ravi Kumar Chakraborty, Brahmananda Droopad, Ravi ACS Omega [Image: see text] In this paper, we report the excellent field emission properties of Q-carbon and analyze its field emission characteristics through structural, morphological, and electronic property correlations, supported by density functional theory (DFT) simulation studies. The Q-carbon field emitters show impressive and stable field emission properties, such as a low turn-on electric field of ∼2.38 V/μm, a high emission current density of ∼33 μA/cm(2), and a critical field of ∼2.44 V/μm for the transition from a linear region to the saturation region in the F–N plot. The outstanding field emission properties of Q-carbon are attributed to (i) a unique sp(2)/sp(3) mixture in Q-carbon, (ii) sp(2)-bonded highly conductive amorphous carbon-rich channels inside the Q-carbon cluster, (iii) a large local field enhancement due to the local geometry and microstructure of Q-carbon, and (iv) the presence of sp(2)-bonded amorphous carbon regions in the composite film. The temperature-dependent field emission properties, such as extreme sensitivity and an enhancement in the emission current density with temperature, can be explained by the local density of states near the Fermi level and the excellent thermal stability of the Q-carbon field emitters. From DFT simulation studies, the computed work function and the field-enhancement factor were determined to be 3.62 eV and ∼2300, respectively, which explains the excellent field emission characteristics of Q-carbon. The obtained field emission properties, in most cases, were superior to those from other carbon/diamond-based field emitters, which will open new frontiers in field emission-based electronic applications. American Chemical Society 2023-02-27 /pmc/articles/PMC10018518/ /pubmed/36936320 http://dx.doi.org/10.1021/acsomega.2c07576 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Haque, Ariful
Karmakar, Subrata
Trivedi, Ravi Kumar
Chakraborty, Brahmananda
Droopad, Ravi
Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title_full Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title_fullStr Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title_full_unstemmed Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title_short Electric-Field Emission Mechanism in Q-Carbon Field Emitters
title_sort electric-field emission mechanism in q-carbon field emitters
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10018518/
https://www.ncbi.nlm.nih.gov/pubmed/36936320
http://dx.doi.org/10.1021/acsomega.2c07576
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