Cargando…

Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate

WTe(2), a low-symmetry transition metal dichalcogenide, has broad prospects in functional device applications due to its excellent physical properties. When WTe(2) flake is integrated into practical device structures, its anisotropic thermal transport could be affected greatly by the substrate, whic...

Descripción completa

Detalles Bibliográficos
Autores principales: Fang, Mengke, Liu, Xiao, Liu, Jinxin, Chen, Yangbo, Su, Yue, Wei, Yuehua, Zhou, Yuquan, Peng, Gang, Cai, Weiwei, Deng, Chuyun, Zhang, Xue-Ao
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10302967/
https://www.ncbi.nlm.nih.gov/pubmed/37368247
http://dx.doi.org/10.3390/nano13121817
_version_ 1785065167730507776
author Fang, Mengke
Liu, Xiao
Liu, Jinxin
Chen, Yangbo
Su, Yue
Wei, Yuehua
Zhou, Yuquan
Peng, Gang
Cai, Weiwei
Deng, Chuyun
Zhang, Xue-Ao
author_facet Fang, Mengke
Liu, Xiao
Liu, Jinxin
Chen, Yangbo
Su, Yue
Wei, Yuehua
Zhou, Yuquan
Peng, Gang
Cai, Weiwei
Deng, Chuyun
Zhang, Xue-Ao
author_sort Fang, Mengke
collection PubMed
description WTe(2), a low-symmetry transition metal dichalcogenide, has broad prospects in functional device applications due to its excellent physical properties. When WTe(2) flake is integrated into practical device structures, its anisotropic thermal transport could be affected greatly by the substrate, which matters a lot to the energy efficiency and functional performance of the device. To investigate the effect of SiO(2)/Si substrate, we carried out a comparative Raman thermometry study on a 50 nm-thick supported WTe(2) flake (with κ(zigzag) = 62.17 W·m(−1)·K(−1) and κ(armchair) = 32.93 W·m(−1)·K(−1)), and a suspended WTe(2) flake of similar thickness (with κ(zigzag) = 4.45 W·m(−1)·K(−1), κ(armchair) = 4.10 W·m(−1)·K(−1)). The results show that the thermal anisotropy ratio of supported WTe(2) flake (κ(zigzag)/κ(armchair) ≈ 1.89) is about 1.7 times that of suspended WTe(2) flake (κ(zigzag)/κ(armchair) ≈ 1.09). Based on the low symmetry nature of the WTe(2) structure, it is speculated that the factors contributing to thermal conductivity (mechanical properties and anisotropic low-frequency phonons) may have affected the thermal conductivity of WTe(2) flake in an uneven manner when supported on a substrate. Our findings could contribute to the 2D anisotropy physics and thermal transport study of functional devices based on WTe(2) and other low-symmetry materials, which helps solve the heat dissipation problem and optimize thermal/thermoelectric performance for practical electronic devices.
format Online
Article
Text
id pubmed-10302967
institution National Center for Biotechnology Information
language English
publishDate 2023
publisher MDPI
record_format MEDLINE/PubMed
spelling pubmed-103029672023-06-29 Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate Fang, Mengke Liu, Xiao Liu, Jinxin Chen, Yangbo Su, Yue Wei, Yuehua Zhou, Yuquan Peng, Gang Cai, Weiwei Deng, Chuyun Zhang, Xue-Ao Nanomaterials (Basel) Article WTe(2), a low-symmetry transition metal dichalcogenide, has broad prospects in functional device applications due to its excellent physical properties. When WTe(2) flake is integrated into practical device structures, its anisotropic thermal transport could be affected greatly by the substrate, which matters a lot to the energy efficiency and functional performance of the device. To investigate the effect of SiO(2)/Si substrate, we carried out a comparative Raman thermometry study on a 50 nm-thick supported WTe(2) flake (with κ(zigzag) = 62.17 W·m(−1)·K(−1) and κ(armchair) = 32.93 W·m(−1)·K(−1)), and a suspended WTe(2) flake of similar thickness (with κ(zigzag) = 4.45 W·m(−1)·K(−1), κ(armchair) = 4.10 W·m(−1)·K(−1)). The results show that the thermal anisotropy ratio of supported WTe(2) flake (κ(zigzag)/κ(armchair) ≈ 1.89) is about 1.7 times that of suspended WTe(2) flake (κ(zigzag)/κ(armchair) ≈ 1.09). Based on the low symmetry nature of the WTe(2) structure, it is speculated that the factors contributing to thermal conductivity (mechanical properties and anisotropic low-frequency phonons) may have affected the thermal conductivity of WTe(2) flake in an uneven manner when supported on a substrate. Our findings could contribute to the 2D anisotropy physics and thermal transport study of functional devices based on WTe(2) and other low-symmetry materials, which helps solve the heat dissipation problem and optimize thermal/thermoelectric performance for practical electronic devices. MDPI 2023-06-07 /pmc/articles/PMC10302967/ /pubmed/37368247 http://dx.doi.org/10.3390/nano13121817 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/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 (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Fang, Mengke
Liu, Xiao
Liu, Jinxin
Chen, Yangbo
Su, Yue
Wei, Yuehua
Zhou, Yuquan
Peng, Gang
Cai, Weiwei
Deng, Chuyun
Zhang, Xue-Ao
Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title_full Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title_fullStr Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title_full_unstemmed Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title_short Improved Thermal Anisotropy of Multi-Layer Tungsten Telluride on Silicon Substrate
title_sort improved thermal anisotropy of multi-layer tungsten telluride on silicon substrate
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10302967/
https://www.ncbi.nlm.nih.gov/pubmed/37368247
http://dx.doi.org/10.3390/nano13121817
work_keys_str_mv AT fangmengke improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT liuxiao improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT liujinxin improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT chenyangbo improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT suyue improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT weiyuehua improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT zhouyuquan improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT penggang improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT caiweiwei improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT dengchuyun improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate
AT zhangxueao improvedthermalanisotropyofmultilayertungstentellurideonsiliconsubstrate