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two absorption regions, one in the UV region at about 300–400 nm
(B-band) and the other in the visible region at 600–700 nm (Q-
band). Aggregation behavior of Pc is a result of coplanar association
of rings progressing from monomer to dimer and higher order
complexes and it is dependent on concentration, nature of solvent
and substituents, metal ions and temperature [29]. Aggregation in
MPcs is observed as a broadened or split Q-band, with the high en-
ergy band being due to the aggregate and the low energy band due
to the monomer. Complexes 6 and 7 show Q-band absorptions at
698 nm, 697 nm whereas complexes 8 and 9 show Q-bands
absorption at 682 nm, 680 nm in DMSO, Table 1. In CHCl3, com-
plexes 6 and 7 show Q-band absorption at 700 and 699 nm,
whereas complexes 8 and 9 show Q-band absorption at 685 and
682 nm, respectively, Table 1 and Fig. 1. This red shift in complexes
6 and 7 is due to substitution at non-peripheral position. It is well
Fig. 3. Triplet state decay curve of complex 7 in DMSO.
monomeric phthalocyanines, showing the interaction between
the two rings is minimal.
known that
a substitution results in red shifting of the spectra
[30,31]. Complexes 6–9 show B-bands from 320 to 337 nm. How-
ever, complexes 6 and 7 in CHCl3 has an extra band near 742 and
743 nm, which could be associated with a loss of symmetry often
observed in chlorinated solvents [32]. The observation of the extra
band in chloroform is due to protonation since this solvent may
contain small amounts of acid as observed before [33]. This extra
band is not observed in DMSO. The broad shoulder observed at
632, 630, 619, 613 nm for 6–9, respectively, in chloroform has been
reported to indicate aggregation of complexes of ball-type struc-
ture [17–19].
3.3. Triplet quantum yields and lifetimes
The triplet quantum yields (UT) and lifetimes of the complexes
are listed in Table 1 and Fig. 3 shows the triplet decay curve for the
complex 7 (in DMSO) which obeyed second order kinetics. Triplet
quantum yields represent the fraction of absorbing molecules that
undergo intersystem crossing to the metastable triplet excited
state.
A well defined band near 620 nm in ball-type phthalocyanines
is due to exciton coupling between the two Pc rings [17]. The spec-
tra of complexes 6 to 9 in DMSO shows bands in this region, which
may be attributed to intermolecular interactions between the rings
in agreement with literature. However, there is more broadening
for 8 and 9 which are peripherally substituted, due to aggregation.
Non-peripheral substitution prevents aggregation to a larger ex-
tent compared to peripheral substitution. Thus it is clear that there
is more aggregation for complexes 8 and 9 which are peripherally
substituted compared to non-peripherally substituted 6 and 7, as is
typical of phthalocyanines [31].
High UT values and correspondingly low UF values are observed
for ZnPc derivatives compared to MgPc counterparts substituted at
same positions, due to a more efficient intersystem crossing (ISC),
for the former complexes. The UT values for 6–9 are 0.84, 0.88, 0.62
and 0.74, respectively. The UT values are higher for the non-periph-
erally substituted derivatives 6 and 7 compared to their peripher-
ally substituted derivatives 8 and 9, due to reduced aggregation in
the former.
Complexes 6–9 have low UIC values, which may be explained by
strong intramolecular interactions between the Pc rings, probably
due to the cofacial structure. All complexes showed reasonably
long triplet lifetimes with sT ranging from 310 to 910
ls. MgPc
derivatives 6 and 8 show longer T when compared to ZnPc deriv-
s
3.2. Fluorescence spectra and quantum yields
atives 7 and 9, due to the heavy atom effect of Zn. Non-peripheral
substitution in 7 shows slightly shorter sT values compared to
peripheral substitution in 9 for ZnPc derivatives, hence showing
a small effect of position of the substituent on the triplet lifetime
values. However, comparing MgPc complexes 8 with 6 shows a
large effect of peripheral substitution on triplet lifetimes. The sT
values are much longer for peripheral (8) compared to non-periph-
eral (6) substitution in MgPc derivatives.
The absorption, fluorescence excitation and emission spectra of
complex 6–9 in DMSO are shown in Fig. 2. The excitation, absorp-
tion and emission spectral data are listed in Table 1. The absorption
and excitation spectra show the same Q-band maxima, however,
the absorption spectra are broadened in the 600–650 nm region
for 8 and 9 compared to the emission and excitation spectra, due
to aggregation. The proximity of the wavelength of each compo-
nent of the Q-band absorption to the Q-band maxima of the exci-
tation spectra for all complexes suggests that the nuclear
configurations of the ground and excited states are similar and
not affected by excitation. The emission spectra are mirror images
of the excitation spectra. Stokes shifts were 10 or 11 nm, typical of
ZnPc complexes [32]. The effect of point of substitution is not clear
from the nature of excitation and emission spectra.
The fluorescence quantum yield (UF) values are typical of MPc
complexes for MgPc and ZnPc derivatives (6–9). The UF values ran-
ged from 0.11 to 0.22 in DMSO. The UF values were lower for ZnPc
derivatives than for MgPc derivatives. This is attributed to the cen-
tral Zn metal which is heavier than Mg and hence encourages
intersystem crossing to the triplet state as will be confirmed below.
Face-to-face interaction of the two monomers in dimers is
expected to decrease the energy gap between the singlet state
and the triplet state and enhance the formation of triplet state
(i.e. intersystem crossing increases) decreasing fluorescence [34].
However, in this work the UF values are similar to those of
4. Conclusions
The syntheses of the ball-type Mg(II)Pc and Zn(II)Pc complexes
6–8 and photophysical properties of complexes 6–9 are presented.
MgPc derivatives 6 and 8 show longer sT when compared to corre-
sponding ZnPc derivatives 7 and 9. The largest triplet yields were
observed for the non-peripherally substituted complexes 6 and 7,
showing that non-peripheral substitution favors increased popula-
tion of the triplet state. All complexes show reasonably high triplet
state quantum yields and long triplet life which are required for
efficient photosensitization.
Acknowledgments
This work was supported by the Department of Science and
Technology (DST) and National Research Foundation (NRF), South
Africa through DST/NRF South African Research Chairs Initiative