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JP Sauvage

Publications and source records attributed to JP Sauvage.

7 recordsLinked to original sources

A linear multiporphyrinic

A linear multiporphyrinic [2]-rotaxane has been synthesized using the transition metal-templating method for threading a gold(III)-incorporating macrocycle onto a rodlike, phenanthroline-derived chelate bearing carboxylate end groups. Stoppering has been performed by reacting the resulting prerotaxane with the amino derivative of a zinc tetraarylporphyrin under EDC-HOBt activation. A 34% yield has been realized for this one-pot, double amide bond formation.

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Synthesis of Copper(I) catenanes incorporating a disulfide bridge and their deposition on a gold surface

The synthesis of two coordinating catenates with the ability to undergo surface-confined chemistry is described. For each catenate, one of the rings includes a 2,9-diphenyl-1,10-phenanthroline unit as a coordinating moiety and a disulfide bridge, which allows adsorption of the catenate onto a gold surface, thus going from a molecular catenate to a [gold-adsorbed] species in which gold atoms are elements of one of the rings.

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Chiroptical properties of an optically pure dicopper(I) trefoil knot and its enantioselectivity in luminescence quenching reactions

Chiroptical spectroscopy is used to investigate the properties of an optically pure dinuclear copper(I) trefoil knot. For the metal-to-ligand charge tranfer (MLCT) transition in the visible region (520 nm), the electric and magnetic transition dipole moments are determined from absorption and circular dichroism spectra: 2.8 Debye and 0.5 Bohr magneton (muB). Circular polarization in the luminescence (CPL) of the knot is determined and this allows the electric and magnetic transition dipole moments in emission to be calculated: 0.02 Debye and 0.003 muB. The large difference between the moments in absorption and emission shows that the emission observed does not originate directly from the 1MLCT state. Given the low probability for radiative decay we assign the long-lived emitting excited state to a 3MLCT state. The copper(I) trefoil knot is found to quench the emission from TbIII and EuIII(dpa)3(3)-(dpa = pyridine-2,6-dicarboxylate) with a bimolecular rate constant of 3.2 and 3.3 x 10(7)M(-1)S(-1), respectively, at room temperature in water-acetonitrile (1:1 by volume). Experimental results indicate that the (lambda)-knot preferentially quenches the lambda enantiomer of the lanthanide complex with an enantioselectivity (ratio of quenching rate constants for lambda and lambda: kqlambda/kqdelta) of 1.012+/-0.002 for EuIII and 1.0180+/-0.003 for TbIII.

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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.

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