Abstract

The bimetallic complex CpMo(SMe)4MoCp, 1, oxidizes reversibly at 0.20 and 0.64 V vs. SCE. Reaction with TCNQ and TCNQF4 leads to three crystalline phases of different stoichiometry, 1:2 in 1·(TCNQ)2 , 2:1 in 12 ·TCNQ and 1:1 in 1·TCNQF4 , whose crystal structures have been determined by single-crystal X-ray diffraction. Tetramerized TCNQ chains are present in 1·(TCNQ)2 , separated from each other by 1AHâ– +radical cations. This 2:1 salt exhibits semiconducting behavior (σRT=0.018 S cm–1). A transition is observed at 160 K in the spin susceptibility and in the EPR linewidth temperature dependence. Below this temperature only the Curie susceptibility of the non-interacting 1AHâ– +cations remains. In the 2:112 ·TCNQ salt, both neutral 1 and oxidized 1AHâ– +coexist in the solid state, giving rise to alternating … (1AHâ– +)(TCNQAHâ– –)(1AHâ– +)(TCNQAHâ– –) … chains while the empty spaces between the columns are filled with neutral donor molecules. Noticeable differences in the bond distances and angles between neutral1 and oxidized 1AHâ– +are identified and rationalized. No intermolecular interactions can be found in this compound, whose magnetism is best described by a Curie law for two independentS=1/2 spins. In the 1:1 TCNQF4 salt, uniform TCNQF4 stacks are isolated from each other by a honeycomb net of 1AHâ– +cations. Owing to the large interplanar TCNQF4–TCNQF4 distance [3.43(4) A], the material behaves as a Mott insulator.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call