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Ultrahigh Power Factor in Thermoelectric System Nb(0.95)M(0.05)FeSb (M = Hf, Zr, and Ti)

Conversion efficiency and output power are crucial parameters for thermoelectric power generation that highly rely on figure of merit ZT and power factor (PF), respectively. Therefore, the synergistic optimization of electrical and thermal properties is imperative instead of optimizing just ZT by th...

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Detalles Bibliográficos
Autores principales: Ren, Wuyang, Zhu, Hangtian, Zhu, Qing, Saparamadu, Udara, He, Ran, Liu, Zihang, Mao, Jun, Wang, Chao, Nielsch, Kornelius, Wang, Zhiming, Ren, Zhifeng
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6051200/
https://www.ncbi.nlm.nih.gov/pubmed/30027058
http://dx.doi.org/10.1002/advs.201800278
Descripción
Sumario:Conversion efficiency and output power are crucial parameters for thermoelectric power generation that highly rely on figure of merit ZT and power factor (PF), respectively. Therefore, the synergistic optimization of electrical and thermal properties is imperative instead of optimizing just ZT by thermal conductivity reduction or just PF by electron transport enhancement. Here, it is demonstrated that Nb(0.95)Hf(0.05)FeSb has not only ultrahigh PF over ≈100 µW cm(−1) K(−2) at room temperature but also the highest ZT in a material system Nb(0.95)M(0.05)FeSb (M = Hf, Zr, Ti). It is found that Hf dopant is capable to simultaneously supply carriers for mobility optimization and introduce atomic disorder for reducing lattice thermal conductivity. As a result, Nb(0.95)Hf(0.05)FeSb distinguishes itself from other outstanding NbFeSb‐based materials in both the PF and ZT. Additionally, a large output power density of ≈21.6 W cm(−2) is achieved based on a single‐leg device under a temperature difference of ≈560 K, showing the realistic prospect of the ultrahigh PF for power generation.