TY - JOUR
T1 - Synthesis and characterization of three new rare-earth titanium oxyselenides
T2 - Ln3.67Ti2O3Se6 (Ln = Ce, Nd, Sm)
AU - Tougait, O.
AU - Ibers, J. A.
PY - 2000
Y1 - 2000
N2 - Three new compounds, Ln3.67Ti2O3Se6 (Ln = Ce, Nd, Sm), have been prepared from the reaction in stoichiometric ratios of Ln, TiO2, Ti, and Se in sealed fused-silica tubes at 950 °C. A KBr flux was used to promote the crystal growth. Single-crystal X-ray diffraction measurements show that these compounds are isostructural. They crystallize with four formula units in the monoclinic space group C2/m in a new structure type that contains four crystallographically independent Ln atoms with three different coordination geometries and three nonequivalent Ti atoms in octahedral geometry. The structure comprises infinite condensed slabs of composition (∞)/2[Ln4Ti2O4Se4Se(5/2)] alternating along the a axis with extended slabs of composition (∞)/2[Ln3.33Ti2O2Se3Se(5/2)]. To achieve charge balance, Ti3+ and Ti4+ cations must be present in equal numbers; these are randomly distributed over the Ti sites. Crystal data at -120 °C follow: Ce3.67Ti2O3Se6, a = 28.315(6) Å, b = 3.8719(8) Å, c = 11.271(2) Å, β = 90.45(3)°, R(F) = 0.0286; Nd3.67Ti2O3Se6, a = 28.121(6) Å, b = 3.8232(8) Å, c = 11.179(2) Å, β = 90.15(3)°, R(F) = 0.0322; Sm3.67Ti2O3Se6, a = 27.961(6) Å, b = 3.7827(8) Å, c = 11.128(2) Å, β = 90.26(3)°, R(F) = 0.0294. The magnetic susceptibilities of the Ln3.67Ti2O3Se6 (Ln = Ce, Nd, Sm) compounds are dominated by the trivalent rare-earth cations and display paramagnetic behavior down to 5 K.
AB - Three new compounds, Ln3.67Ti2O3Se6 (Ln = Ce, Nd, Sm), have been prepared from the reaction in stoichiometric ratios of Ln, TiO2, Ti, and Se in sealed fused-silica tubes at 950 °C. A KBr flux was used to promote the crystal growth. Single-crystal X-ray diffraction measurements show that these compounds are isostructural. They crystallize with four formula units in the monoclinic space group C2/m in a new structure type that contains four crystallographically independent Ln atoms with three different coordination geometries and three nonequivalent Ti atoms in octahedral geometry. The structure comprises infinite condensed slabs of composition (∞)/2[Ln4Ti2O4Se4Se(5/2)] alternating along the a axis with extended slabs of composition (∞)/2[Ln3.33Ti2O2Se3Se(5/2)]. To achieve charge balance, Ti3+ and Ti4+ cations must be present in equal numbers; these are randomly distributed over the Ti sites. Crystal data at -120 °C follow: Ce3.67Ti2O3Se6, a = 28.315(6) Å, b = 3.8719(8) Å, c = 11.271(2) Å, β = 90.45(3)°, R(F) = 0.0286; Nd3.67Ti2O3Se6, a = 28.121(6) Å, b = 3.8232(8) Å, c = 11.179(2) Å, β = 90.15(3)°, R(F) = 0.0322; Sm3.67Ti2O3Se6, a = 27.961(6) Å, b = 3.7827(8) Å, c = 11.128(2) Å, β = 90.26(3)°, R(F) = 0.0294. The magnetic susceptibilities of the Ln3.67Ti2O3Se6 (Ln = Ce, Nd, Sm) compounds are dominated by the trivalent rare-earth cations and display paramagnetic behavior down to 5 K.
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U2 - 10.1021/cm000203m
DO - 10.1021/cm000203m
M3 - Article
AN - SCOPUS:0033810266
SN - 0897-4756
VL - 12
SP - 2653
EP - 2658
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 9
ER -