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.
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Ohta et al. (2017) studied this question.
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