Sazanovich et al.
quently, emission from Dyad-5 occurs primarily from Zni*
(Figure 4A). The integrated amplitude of this emission using
Soret excitation of the aryl-substituted porphyrin (Zna) is
about 20% lower than that obtained using Soret excitation
of Zni (after correction for absorbance at λex and residual
emission from Zna). On the basis of these results, we estimate
that Zna*Zni f ZnaZni* energy transfer has a yield of g80%
for Dyad-5 in toluene (Figure 1 and Table 2).
Fluorescence Lifetimes. The excited-state lifetimes for
the free base porphyrin moiety of Dyads-1-4 in both toluene
and benzonitrile are given in Table 2 along with the lifetimes
for the reference compounds. The yields of ZnFb* f Zn+Fb-
hole transfer in Dyads-1-4 were calculated from these
lifetimes using the formula ΦHT ) 1 - (τFdyba*d/τrFebf*) and are
given in the last column of Table 2. The Fb* lifetimes for
Dyads-1-3 in toluene (12-13 ns) are comparable to the
reference values (slightly over 13 ns), consistent with the
similar emission yields, indicating minimal Fb* quenching
by hole transfer. The yield increases to ΦHT ∼ 0.2 for Dyads-
1-3 in benzonitrile on the basis of a small reduction in Fb*
lifetime compared to that in 8 (paralleling the reduction in
fluorescence yield). For Dyad-4, the Fb* lifetime is slightly
quenched in toluene (∼11 ns versus ∼13 ns; ΦHT ∼0.2) and
more so in benzonitrile (4.2 ns versus 13.5 ns; ΦHT ∼0.6).
Figure 5. Representative time-resolved absorption spectra (A) and kinetic
profile (B) for Dyad-3 in toluene at room temperature using predominant
excitation of the zinc porphyrin component with a 551 nm 130 fs flash.
The fit to the kinetic data at 515 nm in part B gives a dominant component
with a time constant of 69 ps and a minor ∼1 ps phase. The average value
for the dominant component reflecting the Zn* lifetime from measurements
at several detection wavelengths is given in Table 2.
A similar analysis for Dyad-5 gives the yield of ZnaZni*
f Zna+Zni- hole transfer (Figure 1B). The Zn* lifetime for
this dyad in toluene of 1.9 ns presumably derives mainly
from Zni* (the lower-energy unit). This lifetime is only
slightly shorter than that of 2.1 ns for imine-substituted
reference porphyrin Zn-16 and gives ΦHT ∼ 0.1; similar
results are found in benzonitrile (Table 2). The lower hole-
transfer yields for Dyad-5 compared to Dyad-4 no doubt
derive from Zna+Zni- in the former being at higher energy
than Zn+Fb- in the latter.
little change to 3 ns (‚ ‚ ‚), consistent with the Fb* (fluores-
cence) lifetime of ∼13 ns (Table 2) and the minor spectral
changes that accompany Fb* decay, which primarily involves
formation of the excited triplet state FbT (70-80% yield in
the isolated pigment45).
Figure 5B shows a kinetic profile for the decay of the Zn*
excited-state absorption and the formation of the Fb*
bleaching at 515 nm (•) for Dyad-3 in toluene. Also shown
is a fit to a dual-exponential function (convolved with an
instrument response) plus a constant (for Fb* and FbT)
affording a dominant (>90%) kinetic component having time
constant of 69 ( 4 ps and a minor 1.1 ( 0.3 ps component
that may represent some vibrational relaxation of Zn*.
Analysis of kinetic traces at a number of wavelengths gives
a time constant for the main component of 68 ( 4 ps, which
is assigned as the Zn* lifetime for Dyad-3 in toluene (Table
2). Virtually the same Zn* lifetime (65 ( 10 ps) is found
for Dyad-2, which is consistent with the similar linkers
employed in the two arrays. A 5-fold shorter Zn* lifetime
(13 ( 2 ps) is found for Dyad-1, reflecting more rapid energy
Transient Absorption Spectra and Kinetics. All the
dyads were examined by time-resolved absorption difference
spectroscopy to obtain the rate constant and yield for Zn*Fb
f ZnFb* or Zn*Zn f ZnZn* energy transfer and to assess
the contribution of competing electron transfer (Figure 1).
The data were analyzed in the same fashion as we have
previously described for other porphyrin-based arrays.43,44
Representative data for Dyad-3 and Dyad-4 in toluene are
briefly described (Figures 5 and 6) and differences for the
other dyads and solvents highlighted. The measured Zn*
lifetimes and calculated rate constants are listed in Table 2.
Dyads-1-3 in Toluene. The absorption difference spec-
trum observed at 0.5 ps after excitation of Dyad-3 in toluene
(Figure 5A, s) is ascribed principally to Zn*, with a minor
contribution of Fb* (due to direct excitation of the latter).
By 270 ps (- -), the free base bleaching at 515 nm has
increased substantially, resulting from the Zn*Fb f ZnFb*
energy-transfer process. Subsequently, the spectrum shows
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(45) (a) Gradyushko, A. T.; Sevchenko, A. N.; Solovyov, K. N.; Tsvirko,
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(47) (a) Yang, S. I.; Seth, J.; Strachan, J.-P.; Gentemann, S.; Kim, D.;
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6626 Inorganic Chemistry, Vol. 42, No. 21, 2003