Cargando…

Hf/Sb co-doping induced a high thermoelectric performance of ZrNiSn: First-principles calculation

Previous experiments showed that Hf/Sb co-doping in ZrNiSn impressively improved the electrical conductivity (σ). To explore the physical reasons for this improvement, the electronic structures of Hf(x)Zr(1−x)NiSn(1−y)Sb(y) (x = 0, 0.25, 0.5; y = 0, 0.02) have been systematically investigated by usi...

Descripción completa

Detalles Bibliográficos
Autores principales: Zhang, Ju, Zhang, Xiwen, Wang, Yuanxu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5674061/
https://www.ncbi.nlm.nih.gov/pubmed/29109433
http://dx.doi.org/10.1038/s41598-017-15205-y
Descripción
Sumario:Previous experiments showed that Hf/Sb co-doping in ZrNiSn impressively improved the electrical conductivity (σ). To explore the physical reasons for this improvement, the electronic structures of Hf(x)Zr(1−x)NiSn(1−y)Sb(y) (x = 0, 0.25, 0.5; y = 0, 0.02) have been systematically investigated by using the first-principles method and semiclassical Boltzmann transport theory. 50% Hf doping at Zr site in ZrNiSn simultaneously increases the degeneracy and dispersion of energy bands near the conduction band edge, which are helpful to optimizing Seebeck coefficient and slightly improving σ. Furthermore, 2% Sb co-doping at Sn site in Hf(0.5)Zr(0.5)NiSn not only increases total density of states near the Fermi energy but also retains high mobility, and N (v) reaches eleven at the conduction band minimum, thereby inducing a large improvement in σ. Additionally, the Bader charge analysis shows the reason why Sb co-doping supplies more electrons. It is most likely derived from that Sb loses more electrons and Sb-Ni has a stronger hybridization than Sn-Ni. Moreover, we predict that the ZT of Hf(0.5)Zr(0.5)NiSn(0.98)Sb(0.02) at 1000 K can reach 1.37 with the carrier concentration of 7.56 × 10(18) cm(−3), indicating that Hf/Sb co-doping may be an effective approach in optimizing thermoelectric properties of ZrNiSn alloy compounds.