| Autor: |
Perez, Christopher J., Cerretti, Giacomo, Wille, Elizabeth L. K., Devlin, Kasey P., Grewal, Navtej S., Justl, Andrew P., Wood, Maxwell, Bux, Sabah K., Kauzlarich, Susan M. |
| Zdroj: |
Chemistry of Materials; October 2021, Vol. 33 Issue: 20 p8059-8069, 11p |
| Abstrakt: |
The band structure of Yb14MgSb11is tuned by substituting the more earth-abundant cations, Ca and Ba, on the four crystallographically distinct Yb sites (Yb13–xCaxBaMgSb11(x= 1, 2, 3, 4, 5, 6)). Single crystals of composition Yb9.7(2)Ca3.85(5)Ba0.29(4)Mg1.13(3)Sb11.0(1)were grown from Sn flux revealing the cation site preferences. Magnetic measurements on this crystal show paramagnetic behavior consistent with the presence of ∼0.85 Yb3+. High-purity samples (>98%) with compositions close to nominal of Yb13–xCaxBaMgSb11(x= 1–6) were prepared by ball milling and spark plasma sintering. The carrier concentration can be rationalized with the presence of Yb3+for all samples and decreases as a function of xin a systematic fashion at room temperature and increases above ∼600 K for x= 3–6. The temperature dependence of the carrier concentration can be understood considering the electronic structure with a light and heavy band valence band contributing to the properties and suggests the involvement of a localized flat band or impurity state that is active with increasing amounts of Ca. The effect of temperature leads to sustained high Seebeck coefficients with low electrical resistivity arising from the transitioning of the light to heavy band with localization of carriers in the flat band or impurity state for Ca-rich compositions. Speed of sound measurements show that the lattice stiffens with increasing x. Despite the stiffening lattice, the thermal conductivity decreases until x= 3, 4 at which point it increases slightly. The x= 4 sample reaches a peak figure of merit (zT) of 1.32 at 1273 K while being 16% lighter by the molar mass compared to Yb14MnSb11thereby providing a more power dense material. |
| Databáze: |
Supplemental Index |
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