skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Structure, bonding, and properties of CaZn[sub 1[minus]x]Cd[sub x]Sn and CaSn[sub 0. 5]Ge[sub 1. 5]

Journal Article · · Journal of Solid State Chemistry; (United States)
;  [1]
  1. Iowa State Univ., Ames, IA (United States)

CaZnSn, the end member of the CaZn[sub 1-x]Cd[sub x]Sn series, crystallizes in the LiGaGe structure type, an ordered ternary version of CaIn[sub 2] (space group P6[sub 3]mc, Z = 2, a = 4.621(2) [angstrom], c = 7.643(2) [angstrom]). Alternating Zn and Sn form puckered hexagonal layers that are interconnected by 0.40 [angstrom] longer Zn-Sn bonds (around intercalated Ca) to form a distorted wurtzite-like framework. This structure is retained through x = 0.75. The other member, CaCdSn, has the Fe[sub 2]P structure type (space group P62m, Z = 4, a = 7.6319(5), c = 4.6996(4) [angstrom]) and consists of two kinds of augmented trigonal prisms of Ca and Cd centered by different Sn atoms. CaSn[sub 0.52(2)]Ge[sub 1.48(2)] crystallizes in the P6[sub 3]mc space group (a = 4.117(1), c = 10.300 (3) [angstrom]) and has the KSnAs structure, with puckered ordered layers of Sn and Ge separated by calcium. The composition is the tin-rich limit of stability. The CaZn[sub 1[minus]x]Cd[sub x]Sn phases for x = 0, 0.25, 0.50 are weak Pauli paramagnets and metals ([approximately]50 [mu][Omega][center dot]cm at 290 K). Distortions of the hexagonal wurtzite-based matrix by the inserted Ca are thought to be responsible for this unexpected result. CaCdSn and CaSn[sub 0.5]Ge[sub 1.5] are diamagnetic although the former shows a nearly temperature-independent resistivity of [approximately]35 [mu][Omega][center dot] cm.

OSTI ID:
7198996
Journal Information:
Journal of Solid State Chemistry; (United States), Vol. 107:2; ISSN 0022-4596
Country of Publication:
United States
Language:
English