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Lanthanide Contraction as a Design Factor for High‐Performance Half‐Heusler Thermoelectric Materials

Forming solid solutions, as an effective strategy to improve thermoelectric performance, has a dilemma that alloy scattering will reduce both the thermal conductivity and carrier mobility. Here, an intuitive way is proposed to decouple the opposite effects, that is, using lanthanide contraction as a...

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Bibliographic Details
Published in:Advanced materials (Weinheim) 2018-08, Vol.30 (32), p.e1800881-n/a
Main Authors: Liu, Yintu, Fu, Chenguang, Xia, Kaiyang, Yu, Junjie, Zhao, Xinbing, Pan, Hongge, Felser, Claudia, Zhu, Tiejun
Format: Article
Language:English
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Summary:Forming solid solutions, as an effective strategy to improve thermoelectric performance, has a dilemma that alloy scattering will reduce both the thermal conductivity and carrier mobility. Here, an intuitive way is proposed to decouple the opposite effects, that is, using lanthanide contraction as a design factor to select alloying atoms with large mass fluctuation but small radius difference from the host atoms. Typical half‐Heusler alloys, n‐type (Zr,Hf)NiSn and p‐type (Nb,Ta)FeSb solid solutions, are taken as paradigms to attest the validity of this design strategy, which exhibit greatly suppressed lattice thermal conductivity and maintained carrier mobility. Furthermore, by considering lanthanide contraction, n‐type (Zr,Hf)CoSb‐based alloys with high zT of ≈1.0 are developed. These results highlight the significance of lanthanide contraction as a design factor in enhancing the thermoelectric performance and reveal the practical potential of (Zr,Hf)CoSb‐based half‐Heusler compounds due to the matched n‐type and p‐type thermoelectric performance. Lanthanide contraction is suggested as an intuitive consideration for selecting alloying atoms that have large mass fluctuation but small radius difference with the host atoms. In this vein, high‐performance n‐type Hf alloyed ZrCoSb‐based solid solutions are designed and verified, resulting in a high zT of ≈1.0, due to the largely suppressed lattice thermal conductivity and nondegraded carrier mobility.
ISSN:0935-9648
1521-4095
DOI:10.1002/adma.201800881