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Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering

[Image: see text] Strain engineering can effectively improve the energy band degeneracy of two-dimensional transition metal dichalcogenides so that they exhibit good thermoelectric properties under strain. In this work, we have studied the phonon, electronic, thermal, and thermoelectric properties o...

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Autores principales: Wang, Hao, Lan, Yang-Shun, Dai, Bo, Zhang, Xiao-Wei, Wang, Zhi-Guo, Ge, Ni-Na
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2021
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8582045/
https://www.ncbi.nlm.nih.gov/pubmed/34778655
http://dx.doi.org/10.1021/acsomega.1c04286
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author Wang, Hao
Lan, Yang-Shun
Dai, Bo
Zhang, Xiao-Wei
Wang, Zhi-Guo
Ge, Ni-Na
author_facet Wang, Hao
Lan, Yang-Shun
Dai, Bo
Zhang, Xiao-Wei
Wang, Zhi-Guo
Ge, Ni-Na
author_sort Wang, Hao
collection PubMed
description [Image: see text] Strain engineering can effectively improve the energy band degeneracy of two-dimensional transition metal dichalcogenides so that they exhibit good thermoelectric properties under strain. In this work, we have studied the phonon, electronic, thermal, and thermoelectric properties of 1T-phase monolayer HfS(2) with biaxial strain based on first-principles calculations combined with Boltzmann equations. At 0% strain, the results show that the lattice thermal conductivity of monolayer HfS(2) is 5.01 W m(–1) K(–1) and the electronic thermal conductivities of n-type and p-type doped monolayer HfS(2) are 2.94 and 0.39 W m(–1) K(–1), respectively, when the doping concentration is around 5 × 10(12) cm(–2). The power factors of the n-type and p-type doped monolayer HfS(2) are different, 29.4 and 1.6 mW mK(–2), respectively. Finally, the maximum ZT value of the n-type monolayer HfS(2) is 1.09, which is higher than 0.09 of the p-type monolayer HfS(2). Under biaxial strain, for n-type HfS(2), the lattice thermal conductivity, the electronic thermal conductivity, and the power factor are 1.55 W m(–1) K(–1), 1.44 W m(–1) K(–1), and 22.9 mW mK(–2) at 6% strain, respectively. Based on the above factor, the ZT value reaches its maximum of 2.29 at 6% strain. For p-type HfS(2), the lattice thermal conductivity and the electronic thermal conductivity are 1.12 and 1.53 W m(–1) K(–1) at 7% strain, respectively. Moreover, the power factor is greatly improved to 29.5 mW mK(–2). Finally, the maximum ZT value of the p-type monolayer HfS(2) is 3.35 at 7% strain. It is obvious that strain can greatly improve the thermoelectric performance of monolayer HfS(2), especially for p-type HfS(2). We hope that the research results can provide data references for future experimental exploration.
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spelling pubmed-85820452021-11-12 Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering Wang, Hao Lan, Yang-Shun Dai, Bo Zhang, Xiao-Wei Wang, Zhi-Guo Ge, Ni-Na ACS Omega [Image: see text] Strain engineering can effectively improve the energy band degeneracy of two-dimensional transition metal dichalcogenides so that they exhibit good thermoelectric properties under strain. In this work, we have studied the phonon, electronic, thermal, and thermoelectric properties of 1T-phase monolayer HfS(2) with biaxial strain based on first-principles calculations combined with Boltzmann equations. At 0% strain, the results show that the lattice thermal conductivity of monolayer HfS(2) is 5.01 W m(–1) K(–1) and the electronic thermal conductivities of n-type and p-type doped monolayer HfS(2) are 2.94 and 0.39 W m(–1) K(–1), respectively, when the doping concentration is around 5 × 10(12) cm(–2). The power factors of the n-type and p-type doped monolayer HfS(2) are different, 29.4 and 1.6 mW mK(–2), respectively. Finally, the maximum ZT value of the n-type monolayer HfS(2) is 1.09, which is higher than 0.09 of the p-type monolayer HfS(2). Under biaxial strain, for n-type HfS(2), the lattice thermal conductivity, the electronic thermal conductivity, and the power factor are 1.55 W m(–1) K(–1), 1.44 W m(–1) K(–1), and 22.9 mW mK(–2) at 6% strain, respectively. Based on the above factor, the ZT value reaches its maximum of 2.29 at 6% strain. For p-type HfS(2), the lattice thermal conductivity and the electronic thermal conductivity are 1.12 and 1.53 W m(–1) K(–1) at 7% strain, respectively. Moreover, the power factor is greatly improved to 29.5 mW mK(–2). Finally, the maximum ZT value of the p-type monolayer HfS(2) is 3.35 at 7% strain. It is obvious that strain can greatly improve the thermoelectric performance of monolayer HfS(2), especially for p-type HfS(2). We hope that the research results can provide data references for future experimental exploration. American Chemical Society 2021-10-26 /pmc/articles/PMC8582045/ /pubmed/34778655 http://dx.doi.org/10.1021/acsomega.1c04286 Text en © 2021 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 Wang, Hao
Lan, Yang-Shun
Dai, Bo
Zhang, Xiao-Wei
Wang, Zhi-Guo
Ge, Ni-Na
Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title_full Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title_fullStr Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title_full_unstemmed Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title_short Improved Thermoelectric Performance of Monolayer HfS(2) by Strain Engineering
title_sort improved thermoelectric performance of monolayer hfs(2) by strain engineering
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8582045/
https://www.ncbi.nlm.nih.gov/pubmed/34778655
http://dx.doi.org/10.1021/acsomega.1c04286
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