Research - Electron transfer



 
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           Chemical topology

            Molecular machines

        Electron transfer





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In natural photosynthesis in photosynthetic bacteria, a very effective charge separation occurs with a lifetime of several seconds over a long distance, (about 100 Angström). Our studies of artificial photosynthesis focus on catenanes and rotaxanes in which the constituent elements, ring and wire, each have a different pendent porphyrin. Such arrays are particularly well adapted to the study of electron transfer in chromophores between which there is absolutely no connection.
 

 

Several series of arrays have been prepared and studied: in the above example the thread is terminated by two zinc porphyrin stoppers (electron donors in the singlet excited state) which act as the blocking groups, and the ring incorporates a gold porphyrin. This system involves perforce very little friction between the ring and the axle. A rotational movement of 180 degree is observed as a result of decomplexation of Cu(I) from the central site. There is a notable difference between the rate of electron transfer for the situation 'close' and 'distant'. In the free rotaxane the transfer occurs over several tens of
picoseconds, while in the extended form several hundred picoseconds are required. Charge recombination appears to be relatively slow (tens of nanometres).

The study of artifical photosynthesis concerns research into systems in which vectorial electron transfer leads to species with a long-lived charge separated state. In the molecular triad below, Ir(III) bis-terpy is the central electroactive species which
acts as an electron relay between the primary electron donor, the free-base porphyrin, and the secondary electron acceptor, a gold porphyrin. The use of Ir(III) as the central metal circumvents difficulties encountered with analogous Ru(II) complexes in which energy rather than electron transfer was the dominant process.

 

Using time-resolved emission measurements and transient absorption spectroscopy, it is possible to establish the lifetimes of the various electron transfer processes. The fully charge-separated state has a lifetime of 3.5 ns in dichloromethane and is formed with a 50% efficiency by two successive electron transfers. Its deactivation proceeds quantitatively through the triplet state.