Polymétallorotaxanes conjugués contenant des unités pentacoordinantes

Conjugated polymetallorotaxanes containing pentacoordinating units. The present paper reports the synthesis and cyclic voltammetry study of new conjugated polyrotaxanes containing penta-coordinating units around copper or zinc centres. The gathering and threading effect of these metal centres has been used to prepare the desired prerotaxanes, whose macrocyclic and linear components incorporate a tridentate chelate of the terpy type (terpy = 2,2′,6′,2″-terpyridine) and a phen (phen = 1,10-phenantroline) derivative, respectively. Electrochemical oxidative coupling of the end groups (thiophene or pyrrole) leads to the corresponding polymers. Ion-exchange processes, induced by demetalation/remetalation, have been investigated as well as the conductivity of the polymer films prepared.     

Low-spin states in <Superscript>182</Superscript>Os and K<Superscript>π</Superscript> = 0<Superscript>+</Superscript>, 2<Superscript>+</Superscript> excited bands

Excited states in ¹⁸²Os were populated by the β⁺/EC decay of ¹⁸²Ir following mass separation. Gamma-ray and conversion electron spectroscopy techniques were employed. Monopole (E0) contributions were determined in transitions populating the ground-state band. A systematic study of the low-spin structures in the Os isotopes is presented and a detailed analysis in the framework of a microscopic configuration mixing approach is performed.     

A Ru(terpy)(phen)-incorporating ring and its light-induced geometrical changes

A Ru(terpy)(phen) motif has been inscribed in a 39-membered ring by functionalizing the ligands and subsequently performing a cyclization reaction on the complex; by visible light irradiation, a dramatic geometrical changeover of the cyclic complex takes place which can be reversed thermally.     

Light-driven expulsion of the sterically hindering ligand L in tris-diimine ruthenium(II) complexes of the Ru(phen)2(L)2+ family: a pronounced ring effect

Three new ruthenium(II) complexes have been prepared which contain two 1,10-phenanthroline units and a third sterically hindering chelate. In one case, the hindering ligand is a disubstituted 2,2'-bipyridine (bpy) attached to two very bulky manisyl groups. The two other systems are similar in terms of size of the hindering groups (anisyl substituents) located close to the central metal. The complexes investigated in the Present Report are aimed at providing building blocks of future light-driven molecular machines. The photochemical expulsion of the sterically hindering chelate has thus been studied by UV-vis spectroscopy and 1H NMR. Surprisingly, the manisyl-containing complex turned out to be photochemically inert, indicating that a too bulky group acts as a protecting function versus decomplexation rather than as a destabilizing group. For the two other systems, a pronounced ring effect was observed: whereas the acyclic systems undergo fast photochemical expulsion of the bipy-based ligand, in the cyclic complex, the bipy-incorporating ring is decoordinated about 5 times less efficiently than the acyclic ligand of the previous case. These observations on the strong dependence of the photochemical behavior of the ruthenium(II) complexes on their structural properties are corroborated by X-ray diffraction studies on the three compounds investigated.     

Pi-conjugated ligand polymers entwined around copper centres

We describe conjugated polymers entwined around Cu1 with alternating alpha-quaterthienyl (poly[Cu(T2)2]) or 3',4',3',4'-tetrahexyl-alpha-sexythienyl (poly[Cu(T3)2]) moieties and 1,10-phenanthroline complexing sites. Our strategy is to synthesise the 2,9-bis(oligothienyl)-1,10-phenanthroline precursors, then to assemble these ligands by means of Cu1 templating followed by electropolymerisation. Poly[Cu(T2)2] shows separate electroactivities for Cu redox centres and conjugated backbones, whereas the electroactivities overlap in the case of poly[Cu(T3)2]. An X-ray absorption study on these polymers in their reduced state at the Cu-K edge identifies, in both cases, four nitrogen atoms as the closest copper(I) neighbours. For poly[Cu(T2)2], the Cu1 environment is a distorted tetrahedron similar to a monomer model compound, but with a slightly higher number of steric constraints. The Cu1 environment for poly[Cu(T3)2] is a less distorted tetrahedron with an unusually short Cu1-N average bond length. Cu1 removal in poly[Cu(T2)2] induces an irreversible collapse of the structure, whereas the reversibility of Cu1 binding is almost perfect for poly[Cu(T3)2], as the hexyl chains prevent irreversible gliding of the wires after copper removal. Combined electrochemical and resistance measurements reveal that the Cu centres in poly[Cu(T2)2] play the role of mechanical support for the structure with no significant electronic interactions with the conjugated backbone, whereas in the case of poly[Cu(T3)2] copper centres contribute to the conductivity of the structure.