Ground state and time resolved excited state optical absorption
spectra and luminescence spectra are reported
for La2(OEP)3,
Eu2(OEP)3, and
Ce2(OEP)3 (OEP =
2,3,7,8,12,13,17,18-octaethylporphyrinate).
The porphyrin
macrocycles in these molecules are strongly coupled due to their mean
separation of ≤3.5 Å. The triple
deckers show many optical properties analogous to those found for
double decker porphyrin sandwich
complexes, including features not exhibited by porphyrin monomers.
Following excitation, the lowest
1(π,π*)
state of La2(OEP)3 decays in ∼10 ps
predominantly to the phosphorescent 3(π,π*) state,
which lives for ∼10
μs. The lowest 1(π,π*) state of
Eu2(OEP)3 also decays rapidly and with
high yield to the lowest 3(π,π*)
state, which has a rather short lifetime of 630 ps. The lack of
luminescence from Eu2(OEP)3 is ascribed
to
deactivation of the 3(π,π*) state through one or
more low-energy ligand-field states of the metal ion.
Ce2(OEP)3
is also nonluminescent. Unlike
La2(OEP)3 and
Eu2(OEP)3, the
1(π,π*) lifetime of 7 ps for
Ce2(OEP)3 largely
reflects deactivation within the singlet manifold. The decay of
1(π,π*) to the ground state likely
involves
low-lying (f,f) states, although a charge transfer state may play a
role. The small (∼20%) population of
3(π,π*) that forms from
1(π,π*) also decays rapidly (τ ∼ 300 ps),
again via ligand-field states of the metal
ions. These combined results further demonstrate the importance of
(i) π−π interactions in defining the
electronic properties of chromophores brought within van der Waals
distance and (ii) metal-centered excited
states in determining the relaxation rates and pathways following
photoexcitation of tetrapyrrole complexes.