MOLECULAR METALS: STRUCTURE AND PROPERTIES. O.A. Dyachenko, V.V. Gritsenko, S.V. Konovalikhin, R.N. Lyubovskaya, E.B. Yagubskii, R.B. Lyubovskii, Institute of Chemical Physics, RAS, Chernogolovka MD 142432 Russia, and E.Canadell, ICMAB, Campus de la UAB, 08193 Bellaterra, Spain
The structure-conductivity relationships were derived from crystalline
diffraction experiments for the salts based on
bis(ethylenedithio)tetrathiafulvalene (ET) and
5,6-dihydro-1,4-dithiin-2,3-dithiol (DDDT), which are potential electronic
materials. As a subject for crystallochemical analysis were chosen the family
of molecular conductors
(ET)8[Hg4X12(PhY)2] (X=Y=Cl, metal
down to 1.3 K; X=Cl, Y=Br, TMI=10 K; X=Br, Y=Cl, TMI=90
K; X=Y=Br, TMI= 125 K), the first stable down to 1.3 K molecular
metals, [Ni(DDDT)2]3(AuBr2)2 and
[Pd(DDDT)2]Ag1.54Br3.50, in the
M(DDDT)2 family of conducting complexes, as well as such relative
compounds as molecular semiconductors
(ET)8[Hg4Br12(MeC6H4Cl)
Anion and anionic layer structure
Conducting layer structure (packing and overlapping types, shortened
intermolecular contacts)
Conductivity. On the basis of this analysis it has been established, that: i)
the packing type of a conducting layer determines the conductivity type
(superconductor, metal, semiconductor), and ii) there is an inverse dependence
between the temperatures of metal-insulator transitions (TMI) and
the densities of conducting layers. Tight-binding band structure calculations
have been carried out for comparison of the electronic structures of relative
molecular metals.