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Materials Data on Ca14AlSb11 by Materials Project

Ca14AlSb11 crystallizes in the tetragonal I4_1/acd space group. The structure is three-dimensional. there are four inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a 6-coordinate geometry to six Sb+2.82- atoms. There are a spread of Ca–Sb bond distances ranging from 3.18–3.76 Å. In the second Ca2+ site, Ca2+ is bonded in a 6-coordinate geometry to six Sb+2.82- atoms. There are a spread of Ca–Sb bond distances ranging from 3.19–3.75 Å. In the third Ca2+ site, Ca2+ is bonded to six Sb+2.82- atoms to form CaSb6 octahedra that share corners with eight CaSb6 octahedra, corners with two equivalent AlSb4 tetrahedra, and faces with two equivalent CaSb6 octahedra. The corner-sharing octahedra tilt angles range from 39–55°. There are a spread of Ca–Sb bond distances ranging from 3.14–3.41 Å. In the fourth Ca2+ site, Ca2+ is bonded to six Sb+2.82- atoms to form CaSb6 octahedra that share corners with four CaSb6 octahedra, corners with two equivalent AlSb4 tetrahedra, edges with two equivalent CaSb6 octahedra, and faces with two CaSb6 octahedra. The corner-sharing octahedra tilt angles range from 37–55°. There are a spread of Ca–Sb bond distances ranging from 3.21–3.27 Å. Al3+ is bonded to four equivalent Sb+2.82- atoms to form AlSb4 tetrahedra that share corners with twelve CaSb6 octahedra. The corner-sharing octahedra tilt angles range from 44–47°. All Al–Sb bond lengths are 2.74 Å. There are four inequivalent Sb+2.82- sites. In the first Sb+2.82- site, Sb+2.82- is bonded in a 10-coordinate geometry to eight Ca2+ atoms. In the second Sb+2.82- site, Sb+2.82- is bonded in a 7-coordinate geometry to seven Ca2+ and one Al3+ atom. In the third Sb+2.82- site, Sb+2.82- is bonded in a 7-coordinate geometry to eight Ca2+ atoms. In the fourth Sb+2.82- site, Sb+2.82- is bonded in a 8-coordinate geometry to eight Ca2+ atoms.

36 MATERIALS SCIENCE↗

The Zintl pnictides Yb10CdSb9 and Yb14CdSb11: New candidate thermoelectric materials

The synthesis of new materials is the lifeline of solid-state science, and it continues to offer us unique opportunities for testing various theoretical formulations and models on a practical material. Such an avenue, therefore, provides a breeding ground for technological innovations and advancements that can completely revolutionize our world. Here, we report the results of our exploratory syntheses in the Yb–Cd–Sb compositional space that lead to the identification of two new Zintl antimonides, namely, Yb10CdSb9 and Yb14CdSb11. Their crystal structures were established via single-crystal X-ray diffraction methods; the basic electronic and transport properties of the new materials were also characterized. Yb10CdSb9 crystallizes in a disordered variant of the tetragonal Ca10LiMgSb9 structure type with unit cell parameters a = 11.8473(8) Å and c = 17.1302(12) Å (space group P42/mnm). Yb14CdSb11 crystallizes in the tetragonal Ca14AlSb11 structure type with unit cell parameters: a = 16.605(3) Å and c = 12.144(7) Å (space group I41/acd). Although the structures of both compounds can be rationalized within the framework of the Zintl formalism, based on the partitioning of the valence electrons in the much disordered Yb10CdSb9 phase, the charge is indicative of a slightly electron-rich composition. Electronic structure calculations in both cases support the notion of intrinsic semiconductor behavior, as expected for a Zintl phase. The temperature dependence of the electrical resistivity of a single crystal of Yb10CdSb9 is in line with that, and the evolution of the Seebeck coefficient indicates an electron-dominated transport mechanism, and a respectable power factor of 0.71 μW/cm K2 at 460 K can be calculated for Yb10CdSb9. The electrical resistivity of Yb14CdSb11, however, evolves in a semimetallic manner, which could suggest an overdoped sample or degenerate semiconducting behavior.

Ogunbunmi, Michael O. (ORCID:0000000253409198)↗