TY - JOUR
T1 - New layered materials
T2 - Syntheses, structures, and optical and magnetic properties of CsGdZnSe3, CsZrCuSe3, CsUCuSe3, and BaGdCuSe3
AU - Fu Qiang Huang, Qiang Huang
AU - Mitchell, K.
AU - Ibers, James A
PY - 2001/9/24
Y1 - 2001/9/24
N2 - Four new quaternary selenides CsGdZnSe3, CsZrCuSe3, CsUCuSe3, and BaGdCuSe3 have been synthesized with the use of traditional high-temperature solid-state experimental methods. These compounds are isostructural with KZrCuS3, crystallizing with four formula units in the orthorhombic space group Cmcm. Cell constants (Å) 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). The structure of these ALnMSe3 compounds (A = Cs, Ba, Ln = Zr, Gd, U; M = Cu, Zn) is composed of ∞
2[LnMSe3
n-] (n = 1, 2) layers separated 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 coordinated 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) μB for Gd3+, in good agreement with the theoretical value of 7.94 μB. Optical transitions at 1.88 and 2.92 eV for CsGdZnSe3 and 1.96 eV for BaGdCuSe3 were deduced from diffuse reflectance spectra.
AB - Four new quaternary selenides CsGdZnSe3, CsZrCuSe3, CsUCuSe3, and BaGdCuSe3 have been synthesized with the use of traditional high-temperature solid-state experimental methods. These compounds are isostructural with KZrCuS3, crystallizing with four formula units in the orthorhombic space group Cmcm. Cell constants (Å) 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). The structure of these ALnMSe3 compounds (A = Cs, Ba, Ln = Zr, Gd, U; M = Cu, Zn) is composed of ∞
2[LnMSe3
n-] (n = 1, 2) layers separated 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 coordinated 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) μB for Gd3+, in good agreement with the theoretical value of 7.94 μB. Optical transitions at 1.88 and 2.92 eV for CsGdZnSe3 and 1.96 eV for BaGdCuSe3 were deduced from diffuse reflectance spectra.
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U2 - 10.1021/ic0104353
DO - 10.1021/ic0104353
M3 - Article
C2 - 11559069
AN - SCOPUS:0035944080
SN - 0020-1669
VL - 40
SP - 5123
EP - 5126
JO - Inorganic Chemistry
JF - Inorganic Chemistry
IS - 20
ER -