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Interface Energy Coupling between β-tungsten Nanofilm and Few-layered Graphene
We report the thermal conductance induced by few-layered graphene (G) sandwiched between β-phase tungsten (β-W) films of 15, 30 and 40 nm thickness. Our differential characterization is able to distinguish the thermal conductance of β-W film and β-W/G interface. The cross-plane thermal conductivity...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5610176/ https://www.ncbi.nlm.nih.gov/pubmed/28939834 http://dx.doi.org/10.1038/s41598-017-12389-1 |
Sumario: | We report the thermal conductance induced by few-layered graphene (G) sandwiched between β-phase tungsten (β-W) films of 15, 30 and 40 nm thickness. Our differential characterization is able to distinguish the thermal conductance of β-W film and β-W/G interface. The cross-plane thermal conductivity (k) of β-W films is determined at 1.69~2.41 Wm(−1)K(−1) which is much smaller than that of α-phase tungsten (174 Wm(−1)K(−1)). This small value is consistent with the large electrical resistivity reported for β-W in literatures and in this work. The β-W/β-W and β-W/G interface thermal conductance (G (W/W) and G (W/G)) are characterized and compared using multilayered β-W films with and without sandwiched graphene layers. The average G (W/W) is found to be at 280 MW m(−2)K(−1). G (W/G) features strong variation from sample to sample, and has a lower-limit of 84 MW m(−2)K(−1), taking into consideration of the uncertainties. This is attributed to possible graphene structure damage and variation during graphene transfer and W sputtering. The difference between G (2W/G) and G (W/W) uncovers the finite thermal resistance induced by the graphene layer. Compared with up-to-date reported graphene interface thermal conductance, the β-W/G interface is at the high end in terms of local energy coupling. |
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