Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “Sb 2 Te 3”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

92 records · Page 6

Synthesis and Transport Properties of the Family of Zintl Phases Ca 3 RESb 3 (RE = La–Nd, Sm, Gd–Tm, Lu): Exploring the Roles of Crystallographic Disorder and Core 4f Electrons for Enhancing Thermoelectric Performance

Zintl phases with complex crystal structures have been studied as promising candidate-materials for thermoelectric (TE) applications. Here, we report the syntheses of the family of rare-earth metal Zintl phases with the general formula Ca 4–x RE x Sb 3 (x ≈ 1; RE = La–Nd, Sm, Gd–Tm, Lu). The structural elucidation is based on refinements of single-crystal X-ray diffraction data for 12 unique chemical compositions. The cubic structure is confirmed as belonging to the anti-Th 3 P 4 structure type (space group I4¯3d, no. 220, Z = 4), where the Ca and RE atoms share the same atomic site with ca. 75% and 25% occupancies, respectively. Such crystallographic disordering of divalent Ca and trivalent RE atoms in the structure provides a pathway to intricate bonding. The latter, together with the presence of heavy elements such as Sb and the lanthanides, are expected to enhance the scattering probability of phonons, thereby leading to as low thermal conductivity κ as that of the ordered RE 4 Sb 3 . The drive of the hypothetical parent compound Ca 4 Sb 3 to be stabilized by alloying with rare-earth metals can be understood following the Zintl-Klemm concept, as the resultant formula may be rationalized as (Ca 2+ ) 3 RE 3+ (Sb 3– ) 3 , indicating the realization of closed-shell electronic configurations for all elements. This notion is confirmed by electronic structure calculations, which reveal narrow bandgaps E g = 0.77 and 0.53 eV for Ca 3 LaSb 3 and Ca 3 LuSb 3 , respectively. Additionally, the incorporation of RE atoms into the structure drives the phase into a state of a degenerate semiconductor with dominant hole charge carriers.

36 MATERIALS SCIENCE↗

Materials Data on LiGe3SbTe5 by Materials Project

LiGe3SbTe5 is Caswellsilverite-derived structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Li1+ is bonded to six Te2- atoms to form LiTe6 octahedra that share corners with three equivalent GeTe6 octahedra, corners with three equivalent SbTe6 octahedra, edges with three equivalent GeTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent LiTe6 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. There are three shorter (2.97 Å) and three longer (3.09 Å) Li–Te bond lengths. There are three inequivalent Ge4+ sites. In the first Ge4+ site, Ge4+ is bonded to six Te2- atoms to form GeTe6 octahedra that share corners with three equivalent GeTe6 octahedra, corners with three equivalent SbTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with nine GeTe6 octahedra. The corner-sharing octahedra tilt angles range from 0–7°. There are three shorter (2.91 Å) and three longer (3.09 Å) Ge–Te bond lengths. In the second Ge4+ site, Ge4+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing GeTe6 octahedra. The corner-sharing octahedra tilt angles range from 7–8°. There are three shorter (2.91 Å) and three longer (3.17 Å) Ge–Te bond lengths. In the third Ge4+ site, Ge4+ is bonded to six Te2- atoms to form GeTe6 octahedra that share corners with three equivalent LiTe6 octahedra, corners with three equivalent GeTe6 octahedra, edges with three equivalent LiTe6 octahedra, and edges with nine GeTe6 octahedra. The corner-sharing octahedra tilt angles range from 2–8°. There are three shorter (2.91 Å) and three longer (3.21 Å) Ge–Te bond lengths. Sb3- is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with three equivalent LiTe6 octahedra, corners with three equivalent GeTe6 octahedra, edges with three equivalent LiTe6 octahedra, edges with three equivalent GeTe6 octahedra, and edges with six equivalent SbTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Te bond lengths are 3.09 Å. There are five inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to three equivalent Ge4+ and three equivalent Sb3- atoms to form a mixture of edge and corner-sharing TeGe3Sb3 octahedra. The corner-sharing octahedra tilt angles range from 0–5°. In the second Te2- site, Te2- is bonded to six Ge4+ atoms to form a mixture of edge and corner-sharing TeGe6 octahedra. The corner-sharing octahedra tilt angles range from 5–7°. In the third Te2- site, Te2- is bonded to six Ge4+ atoms to form a mixture of edge and corner-sharing TeGe6 octahedra. The corner-sharing octahedra tilt angles range from 7–8°. In the fourth Te2- site, Te2- is bonded to three equivalent Li1+ and three equivalent Ge4+ atoms to form a mixture of edge and corner-sharing TeLi3Ge3 octahedra. The corner-sharing octahedra tilt angles range from 3–8°. In the fifth Te2- site, Te2- is bonded to three equivalent Li1+ and three equivalent Sb3- atoms to form a mixture of distorted edge and corner-sharing TeLi3Sb3 octahedra. The corner-sharing octahedra tilt angles range from 0–3°.

36 MATERIALS SCIENCE↗