C O M M U N I C A T I O N S
polyads with donor-acceptor geometries that could not be otherwise
accessed by covalent chemistry.
Acknowledgment. This work was carried out with partial
support from the University of Trieste, INSTM, MIUR (PRIN 2006,
prot. 200634372 and Firb, prot. RBNE033KMA), the EU (RTN
networks “WONDERFULL” and “EMMMA”), the Deutsche For-
schungsgemeinshaft (SFB 583), FCI, and the Office of Basic Energy
Science of the U.S. Department of Energy. This paper is dedicated
to Prof. Dan Meyerstein on the occasion of his 70th birthday.
Supporting Information Available: Characterization of 2 and 3.
Differential absorption spectra and time absorption profile of 4.
Spectroelectrochemistry of methyl 5-ferroceneacetoxyisophthalate and
Ru(CO)TPP. This material is available free of charge via the Internet
Figure 1. Differential absorption spectra (visible and near-infrared) obtained
upon femtosecond flash photolysis (420 nm-150 nJ) of 3 in CH2Cl2 with
several time delays between 0 and 167 ps at room temperature. Arrow
illustrates the time evolution. (Insert) Time-absorption profile at 480 nm
(black) and 532 nm (gray), reflecting the charge separation and charge shift
dynamics.
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•-
kinetically. As a matter of fact, the lifetime of the C60
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•-
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In conclusion, we have prepared a triad by a combination of
hydrogen bonding and metal coordination that were employed to
organize the different units along a supramolecular redox gradient.
The excitation of the central Ru(CO)TPP unit results in the transfer
of an electron from Ru(CO)TPP to C60, followed by a charge shift
to yield C60•--Fc•+, as demonstrated by a systematic study based
on time-resolved absorption measurements. This work illustrates
that the redox gradient approach can also be applied to the
construction of supramolecular donor-acceptor systems, opening
the door to the preparation and investigation of supramolecular
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(22) The absorption coefficient of the one-electron oxidized ferrocene at 630
nm is very weak (Figure S5).
(23) It should be noted that in this spectral range (i.e., 400-900 nm) even the
relative intensities are a good match between the photolytically and
spectroelectrochemically generated species.
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