In the search for new functional molecular materials whose physical properties can be easily tuned by simple changes on the molecular structures of their building units, we have designed and synthesized a family of paramagnetic/luminescent metal complexes of general formula [MIII(X2An)3]3- (MIII = Cr, Fe; X = Cl, Br, I, H, CN; An = 2,5-dihydroxy-1,4-benzoquinone).1,2 These metal complexes are valuable building blocks for the preparation of functional materials, such as molecule-based ferrimagnets and magnetic molecular conductors, where the nature of the X substituent at the 3,6 positions of the anilate ring can play a key role in determining their physical properties.3-5 Here we report the synthesis and the full characterization of these metal complexes as well as the synthesis and characterization of a novel family of molecular ferrimagnets formulated as A[MnIICrIII(X2An)3] (A = (n-Bu)4N+, [(phen)3(H3O)]+, X = Cl, Br, I). In this family, a simple change of the substituent atom (X) on the bridging ligand allows for a fine tuning of the magnetic properties: the ordering temperature increases from 5.5 to 6.3, 8.2 and 11.0 K for X = Cl, Br, I, H, respectively.3 Furthermore, by combining the paramagnetic metal complex [Fe(Cl2An)3]3- with the organic donor BEDT-TTF (bis-ethylenedithio-tetrathiafulvalene) and its chiral derivatives (S,S,S,S)- and (R,R,R,R)-TM-BEDT-TTF via electrocrystallization, two novel families of paramagnetic molecular conductors have been obtained. The crystal structures and the physical properties of these magnetic/conducting hybrid systems will be also reported in this communication along with the synthesis and full characterization of the [Al(ClCNAn)3]3- complex, a novel red luminophore under convenient visible light irradiation.4,5
Figure: (left) AC susceptibility measurements for the compounds of the [MnIICrIII(X2An)3]– (X = Cl, Br, I, H) series and a partial view of the crystal structure; (right) Conductivity measurements for the a”’-[BEDT-TTF]18 [Fe(Cl2An)3]3·3CH2Cl2·6H2O system and a partia view of the crystal structure.
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