M. El-Sedik et al. / Dyes and Pigments 92 (2012) 1126e1131
1131
Table 2
Similar to N-triazinyl-1-aminopyrenes [6], our unpublished
semi-empirical computations revealed strongly polar excited states
connected with electron transition from anthracenyl moiety to
triazinyl ring. Their energy decreases dramatically with the number
of chlorine atoms on triazinyl ring and with increasing the solvent
polarity. As a result, these CT states could influence the deactivation
mechanism of the emitting excited state and consequently the
fluorescence quantum yield of studied compounds.
Fluorescence lifetimes of the compounds in dioxan and ethyl acetate.
NO
Dioxan
Ethyl acetate
3
4
5
12.2 ns
10.3 ns
13.3 ns
8.2 ns
6.6 ns
9.0 ns
symmetry. Consequently, two absorption bands with practically the
same middle intensity appear: the broad band in the region
360e440 nm (lmax ¼ 400 nm), the second band with clear-cut
vibronic structure in the region 320e350 nm e.g. [9].
In the same way as the fluorescence quantum yields, the fluo-
rescence lifetimes (Table 2) decrease with increasing electron-
withdrawing nature of triazinyl ring and with increasing of the
solvent polarity.
The substitution of hydrogen atom on amino group of
2-aminoanthracene by electron-withdrawing triazinyl group cau-
ses a decrease in conjugation of the amino 2pp electrons with the
To confirm a common validity of the theoretical results pre-
sented for N-triazinyl-1-aminopyrenes [6], i.e. the dominant role of
CT states for fluorescence quenching, the detailed theoretical study
of N-triazinyl derivatives of a series of polynuclear aromatic amines
is now in progress in our laboratory.
anthracene
p-system; consequently, a hypsochromic shift of the
first absorption band was observed. Simultaneously, a well defined
vibronic structure of the spectra of N-triazinyl derivatives was
recorded. Neither solvent polarity nor a substituent on triazinyl
ring influenced the position of the absorption maxima of N-tri-
azinyl derivatives (Table 1, Figs. 1e5).
4. Conclusion
Five new N-triazinyl derivatives of 2-aminoanthracene were
prepared; their structure was confirmed by elemental analysis, MS
and NMR spectra. The UV/Vis absorption and fluorescence spectra,
fluorescence quantum yields and lifetimes were measured in four
solvents. It was found that a character of a substituent on triazinyl
ring and the solvent polarity do not influence the shape and the
position of the absorption and fluorescence spectra. On the other
hand, the character of appended N-substituent and the solvent
polarity affect the qF of studied compounds significantly. In the
same way as for N-triazinyl 1-aminopyrene and 3-aminoperylene,
the dichloro derivative of N-triazinyl 2-aminoanthracene does not
fluoresce at all. The gradual substitution of chlorine atoms by
electron-donating groups causes a strong increasing of qF. We
suppose that a dramatic fluorescence quenching of dichloro
derivative is caused by a participation of CT states in deactivation
cascade, as has been recently theoretically explained for N-triazinyl
derivatives of 1-aminopyrene.
From the shape of the absorption spectra and from the character
of fluorescence anisotropy for 3 and 5 in 2-methyltetrahydrofuran
(2-MTHF) at 140 K in the spectral range 320e410 nm (Fig. 6), two
well separated bands exhibiting a very similar clear-cut vibronic
structure are evident. According to our CNDO/S calculations (Win-
MOPAC 2.0 Package, unpublished results) of presented compounds,
both bands correspond to electronic transitions to the excited states
mixed from Lb and La states localized on aminoantracenyl moiety;
the second shorter wavelength transition shows somewhat higher
character of La state (a higher CI coefficient of HOMO-LUMO
configuration). The oscillator strength of the first transitions are
0.08 (3) and 0.122 (5), of the second ones are 0.190 (3) and 0.205 (5).
A similar vibronic structure of both bands proves a significant
participation of anthracene La state in both transitions. According to
our theoretical results, the difference of transition moment direc-
tions between the first and the second transition is large (45ꢀ for 3
and 65ꢀ for 5) and is small between the second transition and the
transition corresponding to Bb, lmax ¼ 300e310 nm (15ꢀ for 3 and 4ꢀ
for 5). These results arein agreement with the decrease of anisotropy
degree in the range 320e410 nm.
Acknowledgements
The financial support provided by the Czech Ministry of
Education Youth and Sports (grant VZ MSMT No 0021627501).
The fluorescence spectra of studied compounds show a vibronic
structure and approximate mirror symmetry with the first
absorption band. With decreasing electronegativity of triazinyl ring
and with increasing the solvent polarity, the fluorescence maxima
are shifted slightly bathochromically. The Stokes shifts are small
(1e2 ꢂ 103 cmꢁ1). The excitation fluorescence and absorption
spectra are almost identical.
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