The previously mentioned (SMeEt2)[Pd(dmit)2]2
(1) and the new (SMeEt2)0.5[Pd(dmit)2]
(2) phases are obtained by electrocrystallisation of (SMeEt2)2[Pd(dmit)2] in acetonitrile. The crystal structures of 1 and 2 are determined by X-ray diffraction methods, both at room and low temperatures. Though not previously detected, a cation disorder is evidenced in both phases at room temperature which is removed in 1 at low temperatures. Conductivity measurements show a rather smooth metal to insulator transition in the 150–200 K range for 1
whereas 2 behaves as a semiconductor in the whole range of temperature. Under pressure, the transition of 1 is shifted down to lower temperatures and becomes more abrupt. Electronic band structure calculations (by means of the extended Hückel tight-binding model) show that the cation disorder evidenced in 1 is responsible for two different electron transfers occurring from the (SMeEt2)+ cation layers to the two crystallographically independent anion layers, resulting thus in the observed room temperature metal-like behaviour of 1. The ambient pressure phase transition of 1 is shown to be the consequence of a more homogeneous electron transfer, possibly leading to a Mott–Hubbard localised state at low temperatures, as is also
the case for 2. Under pressure, the more abrupt phase transition observed in 1 is believed to originate from a different metallic regime.
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