Table 1. Electro-Optical Properties of the Pyrenoimidazole Based Dyes
λ
abs, nm (ε, ꢁ 103 Mꢀ1 cmꢀ1
)
dye
thf
dmf
TiO2
λ
em, nm Eox, Va Eox*, eVb HOMO/LUMO, eVc
5a
5b
405 (31.7), 354 (31.3), 289 (48.8)
389 (35.7), 364 (37.3), 290 (29.9)
485
544
597
626
0.80
0.63
ꢀ0.97
ꢀ0.83
5.60/3.06
5.43/3.20
452 (32.4), 384 (18.7), 354 (23.5), 423 (35.5), 380 (24.6), 289 (25.9)
287 (30.5)
5c
464 (44.9), 358 (24.2), 290 (31.7)
442 (45.1), 357 (20.5), 290 (27.9)
580
624
0.54
ꢀ0.87
5.34/3.16
a Oxidation potentials with reference to the ferrocene which was used as an internal standard. b Computed from the formula Eox* = Eox ꢀ E0ꢀ0 where
the band gap was derived from the optical edge c From HOMO = 4.8 þ Eox and LUMO = HOMO ꢀ E0ꢀ0 where E0ꢀ0 was estimated from optical edge.
observed for most the organic dyes generally originating
from the dye-TiO2 interaction leading to a partial depro-
tonation of the carboxylic acid unit.15 However, in more
basic solvents such as dimethyl formamide and in the
presence of triethylamine they showed a slight blue-shift
for the charge transfer transition (Figures S1ꢀS4, SI)
typical of the presence of deprotonated species.
Figure 1. Absorption and emission spectra of the dyes 5aꢀc
recorded in tetrahydrofuran.
spectra of the dyes recorded in THF solutions. All the dyes
possess three absorption peaks at around 280, 350 and
>400 nm. The two bands in the ultraviolet region are
present in all the dyes and are probably originating from
the electronic transitions localized within the pyrenoimi-
dazole segment. The third absorption occurring in the
visible region is sensitive to the nature of the conjugation
pathway and red-shifts on progressive addition of thio-
phene units.12 The dye 5c bearing terthiophene as linker
Figure 2. Computed orbital energies (observed solution data
shown in parentheses) and electronic distribution in the dyes.
To get further insight into the molecular structure and
electron distribution of dyes, the geometries of the dyes
were optimized by density functional theory (DFT) calcu-
lations at the B3LYP/6-31G (d, p) level. Figure 2 shows the
relative energies and electron distributions of the HOMO
and LUMO of the dyes 5aꢀc. The HOMO is delocalized
over the pyrenoimidazole π system with the highest elec-
tron density located at the two nitrogen atoms of the
imidazole moiety, while the LUMO is located in the
anchoring group through the π bridge constituted by the
benzene and/or thiophene moieties. Thus, the HOMOꢀ
LUMO excitation induced by light irradiation could move
the electron distribution from the pyrenoimidazole seg-
ment to the anchoring unit through the conjugation
pathway.
shows a significant red-shift and enhancement in extinc-
tion coefficient in the longer-wavelength band when com-
pared with that of the dyes 5a and 5b. Also, the peak
position of the charge transfer transition for 5a is much
shorter when compared with the other two dyes, probably
due to the electron-deficiency of the benzene linker relative
to the thiophene unit.13 All the dyes when adsorbed on
TiO2 exhibits red-shifted absorption profile (Figure S5, SI)
in comparison to that measured in solution. The red-
shifted absorption may be attributed to the intermolecular
interactions at the TiO2 surface which is likely to happen
due to the planar pyrenoimidazole π-system or to the
thicker TiO2 layer.14 This is contrary to the blue-shift
(12) Zhang, F.; Luo, Y.-H.; Song, J.-S.; Guo, X.-Z.; Liu, W.-L.; Ma,
C.-P.; Huang, Y.; Ge, M.-F.; Bo, Z.; Meng, Q.-B. Dyes Pigm. 2009, 81,
224.
(13) Qin, P.; Yang, X.; Chen, R.; Sun, L.; Marinado, T.; Edvinsson,
T.; Boschloo, G.; Hagfeldt, A. J. Phys. Chem. C 2007, 111, 1853.
(14) Cheng, H.-M.; Hsieh, W.-F. Energy Environ Sci. 2010, 3, 442.
(15) (a) Hagberg, D. P.; Edvinsson, T.; Marinado, T.; Boschloo, G.;
Hagfeldt, A.; Sun, L. Chem. Commun. 2006, 2245. (b) Yen, Y.-S.; Hsu,
Y.-C.; Lin, J. T.; Chang, C.-W.; Hsu, C.-P.; Yin, D. J. J. Phys. Chem. C
2008, 112, 12557.
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Org. Lett., Vol. 13, No. 10, 2011