D.N. Tomilin et al.
Dyes and Pigments 176 (2020) 108228
Fig. 3. The electron density difference plot between
the Si (i ¼ 1, 2) and S0 state of the benzo[b]-fused
derivative 1b (plotted for the isosurface value of
0.001 a.u.). Red and blue correspond to positive (
ρ
>
0) and negative (
ρ < 0) regions, respectively, and
thus represent increase and decrease in electron
density due to the excitation. μ(S1) and μ(S2) - dipole
moment S1 and S2 states, respectively. (For inter-
pretation of the references to color in this figure
legend, the reader is referred to the Web version of
this article.)
As far as many known meso-CF3-BODIPY dyes [21–24,49,50,55–58], as
well as some here synthesized CF3-BODIPY exhibit excellent fluorescent
properties, it seems that the lack of fluorescence in derivatives 1a and 1b
should be caused by other reasons than in the case of meso-Ph-BODIPY
[51,52], probably by the presence of fused indole substituent.
Aggregation-caused emission quenching effect for BODIPYs 1a,b could
be excluded because of their high solubility in n-hexane/MeCN and low
concentration of solutions used.
may be due to the competition of the radiative transition from the 1LE
fluorescent state and the additional nonradiative transition from the 1LE
state to the 1CT non-fluorescent state, as shown schematically in Fig. S7.
3. Conclusions
In conclusion, an expedient strategy for the synthesis of highly effi-
cient BODIPY fluorophores of novel family of meso-CF3-cycloheptane-
and cycloheptene[b]-fused BODIPY dyes fluorescing in a 588–634 nm
region with good quantum yields (Φf ¼ 0.54–0.68) has been developed.
The key step of this strategy is the P2O5-promoted condensation of
readily accessible trifluoro-1-(2,3-cycloalkanopyrrol-2-yl)ethanols with
diverse pyrroles. The strategy proved to be a general easy route to
previously inaccessible asymmetric BODIPY fluorophores.
In order to better understand the quenching mechanism, we
compared the photophysical properties of benzo[b]-fused (indole-
derived) derivatives 1b (and 1a) with those of cycloheptene[b]-fused
derivative 1e, which intensively fluoresces unlike benzo[b]-fused de-
rivatives. Other substituents (in the positions 3 and 8) were the same for
pair 1b and 1e. The maxima of the absorption bands of these derivatives
almost coincide (Table 3), that is very convenient for the comparison.
Fig. 2 displays the absorption spectra of compounds 1b and 1e. It is
seen that the main absorption band of the benzo[b]-fused dye 1b is much
wider and extends up to 700 nm, while the absorption of dye 1e ends at
� 650 nm.
Declaration of competing interests
The authors declare that they have no known competing financial
interests or personal relationships that could have appeared to influence
the work reported in this paper.
Taking into account these differences, we assume that in the case of
benzo[b]-fused dyes, another one weak transition is located on the red
side of the main transition. Due to the strong overlap of bands, the
maximum of this second band cannot be determined accurately.
Therefore, only the red tail of this absorption band is observed.
To test this hypothesis, TD-CAM-B3LYP/SVP calculations (Gaussian
09, Revision B.01 [59]) for the first five electronic transitions of dyes 1a,
1b and 1e have been performed and their results are presented in
Table S1 (ESI). The molecular orbitals involved into these transitions are
shown in Fig. S6. Results for the first three transitions for 1b and 1e are
shown in Table 4.
CRediT authorship contribution statement
Denis N. Tomilin: Investigation. Elena F. Sagitova: Investigation.
Konstantin B. Petrushenko: Software, Validation. Lyubov N. Sobe-
nina: Project administration, Writing - original draft. Igor A. Ushakov:
Visualization, Validation, Software. Guoqiang Yang: Investigation,
Validation. Rui Hu: Investigation, Validation. Boris A. Trofimov:
Conceptualization, Methodology.
TD-DFT calculations reveal that the longest absorption bands in 1e is
the envelope of a single and intense (f ¼ 0.74) S0 → S1 transition, which
is due to the one electron excitation from the HOMO to the LUMO (98%)
(Table 4). The weaker S0 → S2 and S0 → S3 transitions, which are far
enough from the transition S0 → S1 located in the high-energy spectral
region form the second absorption band in the spectrum of 1e.
A completely different picture is observed for benzo[b]-fused de-
rivatives 1a and 1b. Here, the long-wavelength part of the spectra is
formed by two closely spaced transitions, the main contribution to
which are done by HOMO-LUMO and HOMO-1-LUMO single-electron
excitations (Table 4 for 1b as example and Table S1). The first of them,
the S0 → S1 transition, is relatively low-intense and has a moderate
charge transfer (CT) character, and the second, intense S0 → S2 transi-
tion, is a local excited type (LE) transition. This is obvious from the
electron density difference plot (Fig. 3) and the picture of the molecular
orbitals of derivatives 1a and 1b involved in these transitions (Fig. S6).
As a result, the absence of fluorescence of the derivatives 1a and 1b
Acknowledgements
This work was supported by the Russian Foundation for Basic
Research (project no. 19-53-53008 NSFC_a). The main results were ob-
tained using the equipment of the Baikal Analytical Center for Collective
Use, Siberian Branch of the Russian Academy of Sciences.
Appendix A. Supplementary data
Supplementary data to this article can be found online at https://doi.
References
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