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High Thermoelectric Power Factor of High-Mobility 2D Electron Gas.


ABSTRACT: 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 (?), and low thermal conductivity (?). State-of-the-art nanostructuring techniques that significantly reduce ? have realized high-performance thermoelectric materials with a figure of merit (ZT = S2???T??-1) between 1.5 and 2. Although the power factor (PF = S2??) 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 ?. At a maximized PF, ? 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 ? of the high-mobility electron gas from -490 µV K-1 and ?10-1 S cm-1 to -90 µV K-1 and ?104 S cm-1, while maintaining a high carrier mobility (?1500 cm2 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.

SUBMITTER: Ohta H 

PROVIDER: S-EPMC5770668 | biostudies-literature | 2018 Jan

REPOSITORIES: biostudies-literature

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High Thermoelectric Power Factor of High-Mobility 2D Electron Gas.

Ohta Hiromichi H   Kim Sung Wng SW   Kaneki Shota S   Yamamoto Atsushi A   Hashizume Tamotsu T  

Advanced science (Weinheim, Baden-Wurttemberg, Germany) 20171124 1


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 (<i>S</i>), 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 (<i>ZT</i> = <i>S</i><sup>2</sup>∙σ∙<i>T</i>∙κ<sup>-1</sup>)  ...[more]

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