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High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas
Thermoelectric conversion is an energy harvesting technology that directly converts waste heat from various sources into electricity by the Seebeck effect of thermoelectric materials with a large thermopower (S), high electrical conductivity (σ), and low thermal conductivity (κ). State‐of‐the‐art na...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5770668/ https://www.ncbi.nlm.nih.gov/pubmed/29375980 http://dx.doi.org/10.1002/advs.201700696 |
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author | Ohta, Hiromichi Kim, Sung Wng Kaneki, Shota Yamamoto, Atsushi Hashizume, Tamotsu |
author_facet | Ohta, Hiromichi Kim, Sung Wng Kaneki, Shota Yamamoto, Atsushi Hashizume, Tamotsu |
author_sort | Ohta, Hiromichi |
collection | PubMed |
description | Thermoelectric conversion is an energy harvesting technology that directly converts waste heat from various sources into electricity by the Seebeck effect of thermoelectric materials with a large thermopower (S), high electrical conductivity (σ), and low thermal conductivity (κ). State‐of‐the‐art nanostructuring techniques that significantly reduce κ have realized high‐performance thermoelectric materials with a figure of merit (ZT = S (2)∙σ∙T∙κ(−1)) between 1.5 and 2. Although the power factor (PF = S (2)∙σ) must also be enhanced to further improve ZT, the maximum PF remains near 1.5–4 mW m(−1) K(−2) due to the well‐known trade‐off relationship between S and σ. At a maximized PF, σ is much lower than the ideal value since impurity doping suppresses the carrier mobility. A metal‐oxide‐semiconductor high electron mobility transistor (MOS‐HEMT) structure on an AlGaN/GaN heterostructure is prepared. Applying a gate electric field to the MOS‐HEMT simultaneously modulates S and σ of the high‐mobility electron gas from −490 µV K(−1) and ≈10(−1) S cm(−1) to −90 µV K(−1) and ≈10(4) S cm(−1), while maintaining a high carrier mobility (≈1500 cm(2) V(−1) s(−1)). The maximized PF of the high‐mobility electron gas is ≈9 mW m(−1) K(−2), which is a two‐ to sixfold increase compared to state‐of‐the‐art practical thermoelectric materials. |
format | Online Article Text |
id | pubmed-5770668 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-57706682018-01-26 High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas Ohta, Hiromichi Kim, Sung Wng Kaneki, Shota Yamamoto, Atsushi Hashizume, Tamotsu Adv Sci (Weinh) Communications Thermoelectric conversion is an energy harvesting technology that directly converts waste heat from various sources into electricity by the Seebeck effect of thermoelectric materials with a large thermopower (S), high electrical conductivity (σ), and low thermal conductivity (κ). State‐of‐the‐art nanostructuring techniques that significantly reduce κ have realized high‐performance thermoelectric materials with a figure of merit (ZT = S (2)∙σ∙T∙κ(−1)) between 1.5 and 2. Although the power factor (PF = S (2)∙σ) must also be enhanced to further improve ZT, the maximum PF remains near 1.5–4 mW m(−1) K(−2) due to the well‐known trade‐off relationship between S and σ. At a maximized PF, σ is much lower than the ideal value since impurity doping suppresses the carrier mobility. A metal‐oxide‐semiconductor high electron mobility transistor (MOS‐HEMT) structure on an AlGaN/GaN heterostructure is prepared. Applying a gate electric field to the MOS‐HEMT simultaneously modulates S and σ of the high‐mobility electron gas from −490 µV K(−1) and ≈10(−1) S cm(−1) to −90 µV K(−1) and ≈10(4) S cm(−1), while maintaining a high carrier mobility (≈1500 cm(2) V(−1) s(−1)). The maximized PF of the high‐mobility electron gas is ≈9 mW m(−1) K(−2), which is a two‐ to sixfold increase compared to state‐of‐the‐art practical thermoelectric materials. John Wiley and Sons Inc. 2017-11-24 /pmc/articles/PMC5770668/ /pubmed/29375980 http://dx.doi.org/10.1002/advs.201700696 Text en © 2017 The Authors. Published by WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim This is an open access article under the terms of the Creative Commons Attribution (http://creativecommons.org/licenses/by/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited. |
spellingShingle | Communications Ohta, Hiromichi Kim, Sung Wng Kaneki, Shota Yamamoto, Atsushi Hashizume, Tamotsu High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title | High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title_full | High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title_fullStr | High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title_full_unstemmed | High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title_short | High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas |
title_sort | high thermoelectric power factor of high‐mobility 2d electron gas |
topic | Communications |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5770668/ https://www.ncbi.nlm.nih.gov/pubmed/29375980 http://dx.doi.org/10.1002/advs.201700696 |
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