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267
structure using the BLYP functionals with the long-range correction
(LC) [20] and a 6-31G(d,p) basis set. All calculations are performed
using the GAMESS package [21].
The S0 → S1 transition in the SQ dye is viewed as HOMO → LUMO
transition, and as seen in Fig. 5a and b, it involves a charge-transfer
from the oxygen atoms at the both sides of the squaric ring to the
carbon atoms in the ring. The excitation energy obtained by TD-DFT
calculation was calculated to be 2.46 eV (504 nm), which is about
0.3 eV more than the experimental value. This discrepancy is mainly
due to the neglect of solvent molecules.
Considering the final photoproduct of indolenine framework
and the observation that the electronic excitation energy is local-
ized around the squaric ring, we speculate that a solvent molecule
attack on the left side of the squaric ring. Thus, the following adduct,
where CH3O– add on the left carbon atom in the squaric ring (Fig. 5c
and d), was examined in the calculation. After the geometry opti-
mization, the electronic excitation energy was calculated to be
2.61 eV (475 nm), which is about 30 nm blue-shifted from the orig-
inal SQ molecule. This excitation is also HOMO → LUMO transition
and it involves a charge transfer from the central squaric ring to the
left indolenine framework. The oscillation strength for this transi-
tion was given as 0.2, which is relatively small due to the nature of
long-range charge-transfer transition. The observed blue-shift is in
agreement with the experimental findings and it is partly due to the
breaking of the electronic conjugation between the two moieties
attached to the squaric ring. It is assumed that the addition of sol-
vent molecules weaken the bond strength between the indolenine
and squaric ring part, leading to the dissociation. Furthermore, it
was predicted from the NMR spectrum of the intermediate species
that the double bond peak corresponding to the indolenine and
squaric ring bond was weakend.
Finally, it is commented that the above reaction is not a ther-
mally induced reaction. It was checked by the change in the
absorption spectrum of SQ solutions at 323 K, but no change was
observed for hours. Since the temperature rise due to light irra-
diation is only a few degrees in our experiment, the degradation
observed is due to light irradiation.
4. Conclusion
The photodegradation process of a squarilium dye was inves-
tigated by several analytical methods. It was clarified that the
processes depended on the solvent and the solvent molecules were
involved in the reaction mechanism. Since there have been only a
few reports on the molecular mechanism of the photodegradation
of squarilium dyes, the mechanism would be informative for those
who design the molecular structure or utilize squarilium dyes as
photosensitizer, recording media, etc.
Fig. 5. Highest occupied molecular orbitals (HOMO) and lowest unoccupied molec-
ular orbitals (LUMO) for the squarylium dye (a, b) and its adduct (c, d) with a
methanol molecule at the equilibrium structure in the electronic ground state.
Acknowledgements
by GC–MS due to high evaporation temperature. The indolenine
framework was found only for the samples after light irradia-
tion, and the molecular structure is shown in Fig. 1. This result
strongly suggests that the single bond connecting the indoleneine
framework and the squarine ring was dissociated in the pho-
todegradation process.
This research was financially supported by a Grant-in-Aid for
Scientific Research from the Japan Society for the Promotion of Sci-
ence (No. 18686063). The sample was provided by Kyowa Hakko
Chemical Co., Ltd.
References
In order to obtain the detailed understanding of the reaction
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correlation functionals and a 6-31G(d,p) basis set. Subsequently,
the time-dependent (TD) DFT calculations [18,19] are performed
for calculating the vertical excitation energy at the equilibrium
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