Structures and physical properties of magnetic organic conductors based on bent donor molecule EDT-EDSe-TTFVS

[Display omitted] ► New magnetic organic conductors based on bent donor molecule EDT-EDSe-TTFVS. ► Quasi one-dimensional conduction pathway. ► Semiconducting behavior with good conductivity at room temperature. ► Antiferromagnetic interaction caused by relatively strong π–d interaction. The preparat...

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Published inSynthetic Metals Vol. 162; no. 21-22; pp. 1809 - 1814
Main Authors Sun, Jibin, Shao, Jiafeng, Jiang, Guiyang, Lu, Xiaofeng, Zhang, Shangxi, Li, Xuexiang, Wang, Baolin, Sugimoto, Toyonari, Shao, Xiangfeng
Format Journal Article
LanguageEnglish
Published Amsterdam Elsevier B.V 01.12.2012
Elsevier BV
Elsevier
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Summary:[Display omitted] ► New magnetic organic conductors based on bent donor molecule EDT-EDSe-TTFVS. ► Quasi one-dimensional conduction pathway. ► Semiconducting behavior with good conductivity at room temperature. ► Antiferromagnetic interaction caused by relatively strong π–d interaction. The preparation, crystal structures, and physical properties of magnetic organic conductors based on a new bent donor molecule ethylenedithio-ethylenediseleno-tetrathiafulvalene-thioquinone-1,3-dithiolemethide (EDT-EDSe-TTFVS 3) are reported. The single crystals of 32FeCl4(EtOH) and 32FeBr4 are obtained by the electrochemical oxidation of 3 in the presence of (n-Bu4N)FeX4 (X=Cl, Br) at 45°C. Semiconducting behavior is observed with moderate conductivities of 4.0 and 0.6Scm−1 for 32FeCl4(EtOH) and 32FeBr4, respectively. In the crystal structures of both salts, the donor molecules and magnetic FeX4− ions form segregated layers. Within the organic layer, the donor molecules form columnar stacks, and the intra-columnar intermolecular overlap integrals are larger than the inter-columnar ones, resulting in the quasi one-dimensional electronic structures. There are atomic close contacts between the donor and FeX4 ion layers, which gives rise to the antiferromagnetic interaction of Fe(III) d-spins in both salts. Moreover, the Fe(III) d-spins in 32FeBr4 are subject to the antiferromagnetic ordering at 5K due to the strong π–d and d–d interactions.
ISSN:0379-6779
1879-3290
DOI:10.1016/j.synthmet.2012.07.027