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I. Hanyz et al. / Journal of Molecular Structure 887 (2008) 165–171
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Table 3
Absorption and fluorescence parameters of ST1, ST2, ST3 and ST4
Sample
Absorption kA
(nm)
A275/350
Fluorescence kF
(nm)
max
FWHM350 (F) (cmꢀ1
)
UF
max
ST1
ST2
ST3
ST4
277
–
274
272
347
347
346
347
1.44
–
0.96
1.31
432
428
431
429
3340
3449
3347
3737
0.10
0.15
0.16
0.19
kA
– Wavelength of absorption maximum, A275/350 – absorption band intensity ratio,
max
kFmax – Wavelength of fluorescence maximum, FWHM350 (F) – the fluorescence band half-width for the main band with a maximum at about 430 nm for kex = 350 nm (data
evaluated on the basis of gaussian analysis), UF – fluorescence quantum yield.
the differences in ST2 behaviour when compared to that of the
remaining dyes. The dyes ST1, ST3 and ST4 exist in two isomeric
forms – the cis and trans forms are characterized by the bands with
the maxima at nearly 275 and 350 nm, respectively [1–3,7,8,22].
The lack of the band in the maximum range of 250–300 nm in
ST2 indicates that the cis form does not exist in this dye. The vari-
ations in the dye’s absorption features are attributed to the differ-
ences in the molecular structure of the substituents attached to the
main molecular skeleton; the alkoxy group in ST2 causes that the
molecule is more resistant to isomerization and the cis form in
ST2 does not occur.
by the excitation spectra presented in Fig. 2D; two emission bands
are observed (at 275 and 350 nm) when the trans-dye is registered
(at 425 nm).
The fluorescence quantum yields of the dyes is rather low (they
range from 0.10 to 0.19) and they are a little bit lower than the
quantum yields of other stilbentriazine dyes [3,22]. The UF values
slightly depend on the dye molecular structure (Table 3). The loss
of fluorescence in the cis-dyes is explained as due to processes in
which excitation energy is needed for photoisomerization
[2,11,23,24] and ET as well as non-radiative processes.
Figs. 2A–D evidently confirm occurrence of energy transfer from
the cis form (donor) to the trans form (acceptor). Excitation of the
cis does not lead to its own fluorescence, however emission of the
trans form, when excitation is in the range of cis absorbance, takes
place as seen in Fig. 2C. It is seen that cis–trans energy transfer
gives emission of trans fluorescence. The efficiency of energy trans-
fer, UET can be roughly calculated from direct and sensitized accep-
tor fluorescence on the basis of the absorption spectra (Fig. 2A) and
excitation spectra (Fig. 2D). The data show that about 50% of cis
excitation is transferred to the trans form.
Moreover the weak trans-dye fluorescence properties (UF
< 0.20) indicate that a part of excitation could also be deactivated
in some nonradiative processes like for example: heat liberation,
steric effects and/or activation of other photochemical processes.
The isomerisation process is a subject of the following chapter.
In Figs. 2B and C, the fluorescence spectra are shown when mea-
sured at two excitation wavelengths: 350 and 275 nm. Fig. 2B con-
firms the intensive fluorescence of the trans form of the dyes
(absorbing at about 350 nm) characterized by the spectra with a
hump at about 415 and maximum at 430 nm which differ slightly
from the emission spectra observed in [3,15]. The source of ob-
served difference and an asymmetry of the fluorescence spectra to-
gether with the existence of splitted bands are rather unknown. It
could be existence of an another mesomer form in the samples;
however this explanation needs further experiments with tri-
azine–stilbene dyes substituted with various peripheral groups.
Similar emission features were also observed for other substituted
triazine–stilbene dyes (data not published). Moreover, the results
in Fig. 2C (excitation at 275 nm) evidently show that although in
this experiment the cis form is excited, the fluorescence signal is
emitted in the same spectral range as that in Fig. 2B. The results
in Figs. 2B and C could be explained in two aspects: (i) only one
spectral form of the dyes exists characterised with the absorption
bands at nearly 275 and 350 nm regions, (ii) two forms (cis and
trans) are present in the samples. The (i) is excluded for at least
two reasons: first, the fluorescence signals of the samples when ex-
cited at 275 nm are nearly twice lower than those observed for
350 nm excitation although the absorbance of the samples in the
range of 270–275 nm is twice intensive than that at 340–350 nm
region; second, in the emission excitation spectra (Fig. 2D) the
intensity ratios (at 350 nm bands with respect to the bands at
275 nm) are reversed in intensity when compared to those in the
absorption spectra. Thus, we have every reason to believe that
there are two spectral dye structures in our samples: the cis form
and the trans form (ii) characterized by absorption at 270–275
and 340–350 nm, respectively [12,13]. As seen the shapes of fluo-
rescence are very similar and independent of excitation wave-
length for all investigated dyes; the band positions and half
widths are gathered in Table 3. On the basis of Figs. 2B and C we
can draw at least three conclusions: (i) trans dye form is responsi-
ble for fluorescence; fluorescence spectra shapes are not depen-
dent on the excitation wavelength, (ii) energy transfer (ET) from
the cis to the trans form takes place; excitation at 275 nm gives
fluorescence of the trans-dyes (it concerns to ST1, ST3 and ST4),
(iii) the cis dyes do not fluoresce; whatever excitation is used
(275 or 350 nm), only fluorescence of the trans form is observed.
These conclusions are consistent with the results of other papers
which deal with cis and trans forms [3,13–16,23] and are confirmed
3.2. Influence of pH, temperature and light exposure on cis–trans
isomerisation
In this chapter, we present the results obtained for the dyes ST2
and ST3. The dye ST2 seems to be the most interesting molecules
because it is the only investigated dye among others which does
not have a cis form. The dyes ST1, ST3 and ST4 have very similar
properties and therefore we present the results of the dyes ST3
and ST2 as examples of two dye groups. Fig. 3A presents an influ-
ence of pH on the absorption features of the ST2 dissolved in water
(pH 5.6) and in the buffered solutions (pH 6, 7 and 9). The results
evidently indicate that pH of the media in the range from 5.6 to 9
does not alter the structure of the investigated dyes and their
absorption properties (or only slightly). A similar conclusion we
can draw from the temperature experiment; in the range from 6
to 30 °C no changes are observed in the dye spectral properties
(Fig. 3B). These results evidently indicate that the reaction of media
and heat treatment do not alter the structure of the investigated
dyes and no trans–cis transition takes place.
In the next stage of our investigation, we have examined the
alternation in absorption and fluorescence caused by light expo-
sure. The experiments were done for the samples illuminated with
the light intensity of the order of mW/cm2 to avoid secondary ef-
fects (like for example two-photon processes). In Figs. 4A–D, we
have shown the results obtained for the sample ST2 when dis-
solved in the buffered solution of pH 7 (in pH 5.6, 7 and 9 the
changes are very similar and results are not shown). Fig. 4A shows
variations in absorption behaviour in ST2 upon light in the time