Electrical and Thermal Transport in Coplanar Polycrystalline Graphene–hBN Heterostructures
We present a theoretical study of electronic and thermal transport in polycrystalline heterostructures combining graphene (G) and hexagonal boron nitride (hBN) grains of varying size and distribution. By increasing the hBN grain density from a few percent to 100%, the system evolves from a good cond...
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Veröffentlicht in: | Nano letters 2017-03, Vol.17 (3), p.1660-1664 |
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creator | Barrios-Vargas, José Eduardo Mortazavi, Bohayra Cummings, Aron W Martinez-Gordillo, Rafael Pruneda, Miguel Colombo, Luciano Rabczuk, Timon Roche, Stephan |
description | We present a theoretical study of electronic and thermal transport in polycrystalline heterostructures combining graphene (G) and hexagonal boron nitride (hBN) grains of varying size and distribution. By increasing the hBN grain density from a few percent to 100%, the system evolves from a good conductor to an insulator, with the mobility dropping by orders of magnitude and the sheet resistance reaching the MΩ regime. The Seebeck coefficient is suppressed above 40% mixing, while the thermal conductivity of polycrystalline hBN is found to be on the order of 30–120 Wm–1 K–1. These results, agreeing with available experimental data, provide guidelines for tuning G-hBN properties in the context of two-dimensional materials engineering. In particular, while we proved that both electrical and thermal properties are largely affected by morphological features (e.g., by the grain size and composition), we find in all cases that nanometer-sized polycrystalline G-hBN heterostructures are not good thermoelectric materials. |
doi_str_mv | 10.1021/acs.nanolett.6b04936 |
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By increasing the hBN grain density from a few percent to 100%, the system evolves from a good conductor to an insulator, with the mobility dropping by orders of magnitude and the sheet resistance reaching the MΩ regime. The Seebeck coefficient is suppressed above 40% mixing, while the thermal conductivity of polycrystalline hBN is found to be on the order of 30–120 Wm–1 K–1. These results, agreeing with available experimental data, provide guidelines for tuning G-hBN properties in the context of two-dimensional materials engineering. 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By increasing the hBN grain density from a few percent to 100%, the system evolves from a good conductor to an insulator, with the mobility dropping by orders of magnitude and the sheet resistance reaching the MΩ regime. The Seebeck coefficient is suppressed above 40% mixing, while the thermal conductivity of polycrystalline hBN is found to be on the order of 30–120 Wm–1 K–1. These results, agreeing with available experimental data, provide guidelines for tuning G-hBN properties in the context of two-dimensional materials engineering. 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By increasing the hBN grain density from a few percent to 100%, the system evolves from a good conductor to an insulator, with the mobility dropping by orders of magnitude and the sheet resistance reaching the MΩ regime. The Seebeck coefficient is suppressed above 40% mixing, while the thermal conductivity of polycrystalline hBN is found to be on the order of 30–120 Wm–1 K–1. These results, agreeing with available experimental data, provide guidelines for tuning G-hBN properties in the context of two-dimensional materials engineering. In particular, while we proved that both electrical and thermal properties are largely affected by morphological features (e.g., by the grain size and composition), we find in all cases that nanometer-sized polycrystalline G-hBN heterostructures are not good thermoelectric materials.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>28195494</pmid><doi>10.1021/acs.nanolett.6b04936</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-5335-4652</orcidid><orcidid>https://orcid.org/0000-0003-3031-5057</orcidid><orcidid>https://orcid.org/0000-0003-0323-4665</orcidid></addata></record> |
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subjects | Boron nitride Electronics Grains Graphene Heterostructures Nanostructure Physics Thermal properties Transport |
title | Electrical and Thermal Transport in Coplanar Polycrystalline Graphene–hBN Heterostructures |
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