Fq. Huang et al., New layered materials: Syntheses, structures, and optical and magnetic properties of CsGdZnSe3, CsZrCuSe3, CsUCuSe3, and BaGdCuSe3, INORG CHEM, 40(20), 2001, pp. 5123-5126
Four new quaternary selenides CsGdZnSe3, CsZrCuSe3, CsUCuSe3, and BaGdCuSe3
have been synthesized with the use of traditional high-temperature solid-s
tate experimental methods. These compounds are isostructural with KZrCuS3,
crystallizing with four formula units in the orthorhombic space group Cmcm.
Cell constants (Angstrom) at 153 K are CsGdZnSe3 4.1684(7), 15.765(3), 11.
0089(18); CsZrCuSe3 3.903(2), 15.841(10), 10.215(6); CsUCuSe3 4.1443(7), 15
.786(3), 10.7188(18); and BaGdCuSe3 4.1839(6), 13.8935(19), 10.6692(15). Th
e structure of these ALnMSe(3) compounds (A = Cs, Ba; Ln = Zr, Gd, U; M = C
u, Zn) is composed of (2)(infinity)[LnMSe(3)(n-)] (n = 1, 2) layers separat
ed by A atoms. The Ln atom is octahedrally coordinated to six Se atoms, the
M atom is tetrahedrally coordinated to four Se atoms, and the A atom is co
ordinated to a bicapped trigonal prism of eight Se atoms. Because there are
no Se-Se bonds in the structure, the oxidation state of A is 1+ (Cs) or 2 (Ba), that of Ln is 3+ (Gd) or 4+ (Zr, U), and that of M is 1+ (Cu) or 2(Zn). CsGdZnSe3 and BaGdCuSe3, which are paramagnetic, obey the Curie-Weiss
law and have effective magnetic moments of 7.87(6) and 7.85(5) mu (B) for
Gd3+, in good agreement with the theoretical value of 7.94 mu (B). Optical
transitions at 1.88 and 2.92 eV for CsGdZnSe3 and 1.96 eV for BaGdCuSe3 wer
e deduced from diffuse reflectance spectra.