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Decoupling anion-ordering and spin-Peierls transitions in a strongly one-dimensional organic conductor with a chessboard structure, (o-Me(2)TTF)(2)NO(3)

A mixed-valence conducting cation radical salt of the unsymmetrically substituted o-Me(2)TTF donor molecule (TTF is tetrathiafulvalene) was obtained upon electrocrystallization in the presence of the non-centrosymmetric NO(3) (−) anion. It crystallizes at room temperature in the monoclinic P2(1)/c s...

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Detalles Bibliográficos
Autores principales: Jeannin, Olivier, Reinheimer, Eric W., Foury-Leylekian, Pascale, Pouget, Jean-Paul, Auban-Senzier, Pascale, Trzop, Elzbieta, Collet, Eric, Fourmigué, Marc
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5929382/
https://www.ncbi.nlm.nih.gov/pubmed/29755752
http://dx.doi.org/10.1107/S2052252518004967
Descripción
Sumario:A mixed-valence conducting cation radical salt of the unsymmetrically substituted o-Me(2)TTF donor molecule (TTF is tetrathiafulvalene) was obtained upon electrocrystallization in the presence of the non-centrosymmetric NO(3) (−) anion. It crystallizes at room temperature in the monoclinic P2(1)/c space group, with the anion disordered on an inversion centre. The donor molecules are stacked along the a axis. A 90° rotation of the longest molecular axis of o-Me(2)TTF generates a chessboard-like structure, preventing lateral S⋯S contacts between stacks and providing a strongly one-dimensional electronic system, as confirmed by overlap interaction energies and band structure calculations. A strong dimerization within the stacks explains the semi­conducting behaviour of the salt, with σ(room temp) = 3–5 S cm(−1) and E (activated) = 0.12–0.14 eV. An X-ray diffuse scattering survey of reciprocal space, combined with full structure resolutions at low temperatures (250, 85 and 20 K), evidenced the succession of two structural transitions: a ferroelastic one with an anion-ordering (AO) process and the establishment of a (0, ½, ½) superstructure below 124 (±3) K, also visible via resistivity thermal dependence, followed by a stack tetramerization with the establishment of a (½, ½, ½) superstructure below 90 (±5) K. The latter ground state is driven by a spin-Peierls (SP) instability, as demonstrated by the temperature dependence of the magnetic susceptibility. Surprisingly, these two kinds of instability appear to be fully decoupled here, at variance with other tetra­methyl­tetra­thia­fulvalene (TMTTF) or tetramethyl­tetra­selena­fulvalene (TMTSF) salts with such non-centrosymmetric counter-ions.