Abstract

Bi2Te3 thermoelectric materials are utilized for refrigeration for decades, while their application of energy harvesting requires stable thermoelectric and mechanical performances at elevated temperatures. This work reveals that a steady zT of ≈0.85 at 200 to 300 °C can be achieved by doping small amounts of copper iodide (CuI) in Bi2Te2.2Se0.8–silicon carbide (SiC) composites, where SiC nanodispersion enhances the flexural strength. It is found that CuI plays two important roles with atomic Cu/I dopants and CuI precipitates. The Cu/I dopants show a self‐tuning behavior due to increasing solubility with increasing temperatures. The increased doping concentration increases electrical conductivity at high temperatures and effectively suppresses the intrinsic excitation. In addition, a large reduction of lattice thermal conductivity is achieved due to the “in situ” CuI nanoprecipitates acting as phonon‐scattering centers. Over 60% reduction of bipolar thermal conductivity is achieved, raising the maximum useful temperature of Bi2Te3 for substantially higher efficiency. For module applications, the reported materials are suitable for segmentation with a conventional ingot. This leads to high device ZT values of ≈0.9–1.0 and high efficiency up to 9.2% from 300 to 573 K, which can be of great significance for power generation from waste heat.

Highlights

  • Introduction tions ofBi2Te3-based thermoelectric materials in waste-heat recovery in the low-mid temperature range are receiving more and more attention.[14]

  • Thermoelectric materials that enable direct exchange between of the primary energy is lost as waste heat,[3] there is a high only for scientific interest and for industrial importance.[1,2,3,4] demand for stable thermoelectric performance in low-temper

  • This work has shifted the thermoelectric performance of n-type Bi2Te2.2Se0.8 to elevated temperatures up to 300 °C

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Summary

SiC Dispersion

SiC nanodispersion has been widely demonstrated to be effective in enhancing the mechanical strength along with the thermoelectric performance of Bi2Te3-based alloys.[22,23,24,25] SiC nanoparticles were employed to improve the mechanical stability of Bi2Te2.2Se0.8. We can understand why the CuI-2 mol% sample still shows an obvious self-tuning behavior in the second measurement, while the CuI-1.5 mol% sample presents a weaker increasing trend of carrier concentration (Figure 4a). As I1− and Te2− have almost identical ionic radii (206 and 207 pm, respectively),[41] a change in the lattice parameter due to iodine loss is not expected for this system The increased carrier concentration with temperature is the reason in this work, as analysis of the diffuse reflectance data assuming direct gap transition[47] does not indicate any major shift in optical gap by Cu/I doping (Figure S10, Supporting Information). By extending the use of the segmented leg to higher temperatures, the overall efficiency is increased to 9.2% (inset in Figure 7b), which rivals that of mid temperature materials (hot side temperature ≈675–900 K[49]), making Bi2Te3 competitive for wasteheat power generation applications

Conclusions
Experimental Section
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