The new compounds CsTaQ 3 (Q ) S, Se, and Te) have been synthesized through stoichiometric reactions of the elements with Cs 2 Q n reactive fluxes at 923 K. Their crystal structures have been determined by single-crystal X-ray methods. CsTaQ 3 crystallize in the hexagonal space group D 6h 4 -P6 3 /mmc with two formula units per cell. Crystal data: CsTaS 3 , a ) 7.266(2) Å, c ) 5.961(2) Å, V ) 272.55(10) Å 3 (T038. The compounds adopt the BaVS 3 structure type and feature ∞ 1 [TaQ 3 -] chains of face-sharing octahedra. The Ta 5+ centers are displaced from the centers of the Q 6 octahedra along the direction of the chains in a centrosymmetric fashion. Geometrical considerations and band structure calculations at the extended Hu ¨ckel and density functional (DFT) levels of theory suggest that the most likely distortion pattern is the one with all Ta 5+ centers displaced in the same direction within a given chain. A second-order Jahn-Teller effect is responsible for this distortion. Very weak interchain communication would result in a centrosymmetric structure. The chains are separated by 12-coordinate Cs + cations. CsTaSe 3 is an insulator. CsTaTe 3 shows semiconducting behavior and is diamagnetic or weakly paramagnetic. Differential scanning calorimetry (DSC) and high-temperature powder diffraction data indicate that CsTaTe 3 undergoes a phase transition at ≈493 K.
Experimental and Theoretical SectionSyntheses. CsTaQ3 (Q ) S, Se, and Te) were synthesized by the reactive-flux method. 20 Elemental S (Johnson Matthey, 99.999%), Se (Aldrich, 99.5%), and Te (Aldrich, 99.8%) were stoichiometrically added to Cs (Aldrich, 99.5%) dissolved in liquid NH 3 at 194 K to form Cs 2S5, Cs2Se3, and Cs2Te3, respectively. Cs2Qn was then ground together with powders of Ta (Aldrich, 99.9%) and Q in a 1:2:1 ratio for Q ) S and a 1:2:3 ratio for Q ) Se and Te and sealed under high vacuum in fused-silica tubes. The charged tubes were heated at 923 K for 6 d, then cooled to room temperature at 4 K/h. Black