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Materials Data on Li(ZrS2)2 by Materials Project

LiZr2S4 crystallizes in the monoclinic P2/m space group. The structure is three-dimensional. Li1+ is bonded to six S2- atoms to form LiS6 octahedra that share corners with six equivalent ZrS6 octahedra, edges with two equivalent LiS6 octahedra, and edges with six ZrS6 octahedra. The corner-sharing octahedra tilt angles range from 1–2°. All Li–S bond lengths are 2.64 Å. There are two inequivalent Zr+3.50+ sites. In the first Zr+3.50+ site, Zr+3.50+ is bonded to six S2- atoms to form ZrS6 octahedra that share corners with six equivalent LiS6 octahedra, edges with two equivalent LiS6 octahedra, and edges with six ZrS6 octahedra. The corner-sharing octahedra tilt angles range from 1–2°. There are two shorter (2.58 Å) and four longer (2.61 Å) Zr–S bond lengths. In the second Zr+3.50+ site, Zr+3.50+ is bonded to six S2- atoms to form ZrS6 octahedra that share edges with four equivalent LiS6 octahedra and edges with six ZrS6 octahedra. There are four shorter (2.59 Å) and two longer (2.60 Å) Zr–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to two equivalent Li1+ and three Zr+3.50+ atoms to form a mixture of edge and corner-sharing SLi2Zr3 square pyramids. In the second S2- site, S2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Zr+3.50+ atoms.

36 MATERIALS SCIENCE↗

Electronic Structure Progression across the ACu 2 Q 2 (MQ 2 ) n Semiconductor Series

Moving beyond the engineering of known materials and elemental substitution within common structure types is critical for designing unique properties. Here, we present a new homologous series, ACu 2 Q 2 (MQ 2 ) n (A = Sr, Ba, 2Na; MQ 2 = ZrS2, HfSe 2 ), establishing 11 new members. In β-BaCu 2 Q 2 and Na 2 Cu 2 Se 2 (n = 0), the [Cu 2 Q 2 ] 2– motifs extend in two dimensions, whereas those in α-BaCu 2 Q 2 extend in three dimensions. Hence, there are two structural evolutions within the ACu 2 Q 2 (MQ 2 )n family driven by the polymorphism of the host structures. MQ 2 (n → ∞) displays 2D layers of edge-sharing [MQ 6 ] 8– octahedra that are 1-octahedron-thick and connected via van der Waals bonding. Each insertion of MQ 2 into ACu 2 Q 2 incorporates [MQ 6 ] 8– octahedra extending infinitely in one direction, confined to being 1-octahedron-thick in the second direction, with n controlling the number of [MQ 6 ] 8– octahedra in the third direction. Therefore, increasing n predictively expands the [Cu 2 MnQ 2n+2 ] 2– network in the direction controlled by n and relative to the A + /A 2+ ions. We demonstrate that for a given set of elements, one can enforce a “Host(Insertion)n” formula to systematically evolve both crystal and electronic structures from the host (n = 0) to the insertion (n → ∞) materials through intermediate values of n. Specifically, the energetic misalignment of the electronic band extrema of the parents predictively determines the band extrema and the resulting band gaps of all intermediate n members.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗