Cargando…
Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces
Two-dimensional (2D) materials and their corresponding van der Waals heterostructures have drawn tremendous interest due to their extraordinary electrical and optoelectronic properties. Insulating 2D hexagonal boron nitride (h-BN) with an atomically smooth surface has been widely used as a passivati...
Autores principales: | , , , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2017
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5338337/ https://www.ncbi.nlm.nih.gov/pubmed/28262778 http://dx.doi.org/10.1038/srep43886 |
_version_ | 1782512534239051776 |
---|---|
author | Liu, Yi Ong, Zhun-Yong Wu, Jing Zhao, Yunshan Watanabe, Kenji Taniguchi, Takashi Chi, Dongzhi Zhang, Gang Thong, John T. L. Qiu, Cheng-Wei Hippalgaonkar, Kedar |
author_facet | Liu, Yi Ong, Zhun-Yong Wu, Jing Zhao, Yunshan Watanabe, Kenji Taniguchi, Takashi Chi, Dongzhi Zhang, Gang Thong, John T. L. Qiu, Cheng-Wei Hippalgaonkar, Kedar |
author_sort | Liu, Yi |
collection | PubMed |
description | Two-dimensional (2D) materials and their corresponding van der Waals heterostructures have drawn tremendous interest due to their extraordinary electrical and optoelectronic properties. Insulating 2D hexagonal boron nitride (h-BN) with an atomically smooth surface has been widely used as a passivation layer to improve carrier transport for other 2D materials, especially for Transition Metal Dichalcogenides (TMDCs). However, heat flow at the interface between TMDCs and h-BN, which will play an important role in thermal management of various electronic and optoelectronic devices, is not yet understood. In this paper, for the first time, the interface thermal conductance (G) at the MoS(2)/h-BN interface is measured by Raman spectroscopy, and the room-temperature value is (17.0 ± 0.4) MW · m(−2)K(−1). For comparison, G between graphene and h-BN is also measured, with a value of (52.2 ± 2.1) MW · m(−2)K(−1). Non-equilibrium Green’s function (NEGF) calculations, from which the phonon transmission spectrum can be obtained, show that the lower G at the MoS(2)/h-BN interface is due to the weaker cross-plane transmission of phonon modes compared to graphene/h-BN. This study demonstrates that the MoS(2)/h-BN interface limits cross-plane heat dissipation, and thereby could impact the design and applications of 2D devices while considering critical thermal management. |
format | Online Article Text |
id | pubmed-5338337 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-53383372017-03-08 Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces Liu, Yi Ong, Zhun-Yong Wu, Jing Zhao, Yunshan Watanabe, Kenji Taniguchi, Takashi Chi, Dongzhi Zhang, Gang Thong, John T. L. Qiu, Cheng-Wei Hippalgaonkar, Kedar Sci Rep Article Two-dimensional (2D) materials and their corresponding van der Waals heterostructures have drawn tremendous interest due to their extraordinary electrical and optoelectronic properties. Insulating 2D hexagonal boron nitride (h-BN) with an atomically smooth surface has been widely used as a passivation layer to improve carrier transport for other 2D materials, especially for Transition Metal Dichalcogenides (TMDCs). However, heat flow at the interface between TMDCs and h-BN, which will play an important role in thermal management of various electronic and optoelectronic devices, is not yet understood. In this paper, for the first time, the interface thermal conductance (G) at the MoS(2)/h-BN interface is measured by Raman spectroscopy, and the room-temperature value is (17.0 ± 0.4) MW · m(−2)K(−1). For comparison, G between graphene and h-BN is also measured, with a value of (52.2 ± 2.1) MW · m(−2)K(−1). Non-equilibrium Green’s function (NEGF) calculations, from which the phonon transmission spectrum can be obtained, show that the lower G at the MoS(2)/h-BN interface is due to the weaker cross-plane transmission of phonon modes compared to graphene/h-BN. This study demonstrates that the MoS(2)/h-BN interface limits cross-plane heat dissipation, and thereby could impact the design and applications of 2D devices while considering critical thermal management. Nature Publishing Group 2017-03-06 /pmc/articles/PMC5338337/ /pubmed/28262778 http://dx.doi.org/10.1038/srep43886 Text en Copyright © 2017, The Author(s) http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Liu, Yi Ong, Zhun-Yong Wu, Jing Zhao, Yunshan Watanabe, Kenji Taniguchi, Takashi Chi, Dongzhi Zhang, Gang Thong, John T. L. Qiu, Cheng-Wei Hippalgaonkar, Kedar Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title | Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title_full | Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title_fullStr | Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title_full_unstemmed | Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title_short | Thermal Conductance of the 2D MoS(2)/h-BN and graphene/h-BN Interfaces |
title_sort | thermal conductance of the 2d mos(2)/h-bn and graphene/h-bn interfaces |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5338337/ https://www.ncbi.nlm.nih.gov/pubmed/28262778 http://dx.doi.org/10.1038/srep43886 |
work_keys_str_mv | AT liuyi thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT ongzhunyong thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT wujing thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT zhaoyunshan thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT watanabekenji thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT taniguchitakashi thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT chidongzhi thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT zhanggang thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT thongjohntl thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT qiuchengwei thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces AT hippalgaonkarkedar thermalconductanceofthe2dmos2hbnandgraphenehbninterfaces |