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Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te)
The successful synthesis of the single to few layer transition metal dichalcogenides has opened a new era in the nanoelectronics. For their efficient implementations in the electronic devices while taking care of their overheating issues, the characterization of their thermal transport properties is...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6418116/ https://www.ncbi.nlm.nih.gov/pubmed/30872639 http://dx.doi.org/10.1038/s41598-019-40882-2 |
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author | Zulfiqar, Muhammad Zhao, Yinchang Li, Geng Li, ZhengCao Ni, Jun |
author_facet | Zulfiqar, Muhammad Zhao, Yinchang Li, Geng Li, ZhengCao Ni, Jun |
author_sort | Zulfiqar, Muhammad |
collection | PubMed |
description | The successful synthesis of the single to few layer transition metal dichalcogenides has opened a new era in the nanoelectronics. For their efficient implementations in the electronic devices while taking care of their overheating issues, the characterization of their thermal transport properties is extremely vital. So, we have systematically investigated the thermal transport properties of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) by combining the first-principles calculations with Boltzmann transport equation. We find that monolayer WTe(2) possesses the lowest lattice thermal conductivity κ(L) (33:66 Wm(−1)K(−1) at 300 K) among these six semiconducting materials, in contrast to the highest κ(L) (113:97 Wm(−1)K(−1) at 300 K) of WS(2) among them. Further analyses reveal that the higher (lower) anharmonic and isotopic scatterings together with the lower (higher) phonon group velocities lead to the lowest (highest) value of κ(L) in WTe(2) (WS(2)) monolayer. In addition, we have also calculated the cumulative thermal conductivity κ(C) as a function of mean free path, which indicates that the nanostructures with the length of about 400 nm would reduce κ(L) drastically. These results offer important understanding from thermal conductivity point of view to design the 2D transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) electronics. |
format | Online Article Text |
id | pubmed-6418116 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-64181162019-03-18 Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) Zulfiqar, Muhammad Zhao, Yinchang Li, Geng Li, ZhengCao Ni, Jun Sci Rep Article The successful synthesis of the single to few layer transition metal dichalcogenides has opened a new era in the nanoelectronics. For their efficient implementations in the electronic devices while taking care of their overheating issues, the characterization of their thermal transport properties is extremely vital. So, we have systematically investigated the thermal transport properties of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) by combining the first-principles calculations with Boltzmann transport equation. We find that monolayer WTe(2) possesses the lowest lattice thermal conductivity κ(L) (33:66 Wm(−1)K(−1) at 300 K) among these six semiconducting materials, in contrast to the highest κ(L) (113:97 Wm(−1)K(−1) at 300 K) of WS(2) among them. Further analyses reveal that the higher (lower) anharmonic and isotopic scatterings together with the lower (higher) phonon group velocities lead to the lowest (highest) value of κ(L) in WTe(2) (WS(2)) monolayer. In addition, we have also calculated the cumulative thermal conductivity κ(C) as a function of mean free path, which indicates that the nanostructures with the length of about 400 nm would reduce κ(L) drastically. These results offer important understanding from thermal conductivity point of view to design the 2D transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) electronics. Nature Publishing Group UK 2019-03-14 /pmc/articles/PMC6418116/ /pubmed/30872639 http://dx.doi.org/10.1038/s41598-019-40882-2 Text en © The Author(s) 2019 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/. |
spellingShingle | Article Zulfiqar, Muhammad Zhao, Yinchang Li, Geng Li, ZhengCao Ni, Jun Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title | Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title_full | Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title_fullStr | Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title_full_unstemmed | Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title_short | Intrinsic Thermal conductivities of monolayer transition metal dichalcogenides MX(2) (M = Mo, W; X = S, Se, Te) |
title_sort | intrinsic thermal conductivities of monolayer transition metal dichalcogenides mx(2) (m = mo, w; x = s, se, te) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6418116/ https://www.ncbi.nlm.nih.gov/pubmed/30872639 http://dx.doi.org/10.1038/s41598-019-40882-2 |
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