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Solid Solution Yb<sub>2–<i>x</i></sub>Ca<i><sub><i>x</i></sub></i>CdSb<sub>2</sub>: Structure, Thermoelectric Properties, and Quality Factor
14
Citations
37
References
2021
Year
Solid solutions of Yb<sub>2-<i>x</i></sub>A<i><sub><i>x</i></sub></i>CdSb<sub>2</sub> (A = Ca, Sr, Eu; <i>x</i> ≤ 1) are of interest for their promising thermoelectric (TE) properties. Of these solid solutions, Yb<sub>2-<i>x</i></sub>Ca<i><sub><i>x</i></sub></i>CdSb<sub>2</sub> has end members with different crystal structures. Yb<sub>2</sub>CdSb<sub>2</sub> crystallizes in the polar space group <i>Cmc</i>2<sub>1</sub>, whereas Ca<sub>2</sub>CdSb<sub>2</sub> crystallizes in the centrosymmetric space group <i>Pnma</i>. Other solid solutions, Yb<sub>2-<i>x</i></sub>A<i><sub><i>x</i></sub></i>CdSb<sub>2</sub> (A = Sr, Eu), crystallize in the polar space group for <i>x</i> ≤ 1, and compositions with <i>x</i> ≥ 1 have not been reported. Both structure types are composed of corner-sharing CdSb<sub>4</sub> tetrahedra condensed into sheets that differ by the stacking of the layers. Single crystals of the solid solution Yb<sub>2-<i>x</i></sub>Ca<i><sub><i>x</i></sub></i>CdSb<sub>2</sub> (<i>x</i> = 0-1) were studied to elucidate the structural transition between the Yb<sub>2</sub>CdSb<sub>2</sub> and Ca<sub>2</sub>CdSb<sub>2</sub> structure types. For <i>x</i> ≤ 1, the structures remain in the polar space group <i>Cmc</i>2<sub>1</sub>. As the Ca content is increased, a positional disorder arises in the intralayer cation sites (Yb2/Ca2) and the Cd site, resulting in inversion of the CdSb<sub>4</sub> tetrahedral chain. This phenomenon could be indicative of an intergrowth of the opposing space group. The TE properties of polycrystalline samples of Yb<sub>2-<i>x</i></sub>Ca<i><sub><i>x</i></sub></i>CdSb<sub>2</sub> (<i>x</i> ≤ 1) were measured from 300 to 525 K. The lattice thermal conductivity is extremely low (0.3-0.4 W/m·K) and the Seebeck coefficients are high (100-180 μV/K) across the temperature range. First-principles calculations show a minimum in the thermal conductivity for the <i>x</i> = 0.3 composition, in good agreement with experimental data. The low thermal conductivity stems from the acoustic branches being confined to low frequencies and a large number of phonon scattering channels provided by the localized optical branches. The TE quality factor of the Yb<sub>1.7</sub>A<sub>0.3</sub>CdSb<sub>2</sub> (A = Ca, Sr, Eu) series has been calculated and predicts that the A = Ca and Sr solid solutions may not improve with carrier concentration optimization but that the Eu series is worthy of additional modifications. Overall, the <i>x</i> = 0.3 compositions provide the highest <i>zT</i> because they provide the best electronic properties with the lowest thermal conductivity.
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