3.1. Synthesis and Characterization
Scheme 1 and Scheme 2 demonstrate the synthesis pathway of BODIPY (3) and, complexes (4 and 5), respectively. The literature-known iridium (1) [29], and ruthenium (2) [30] compounds, were treated with BODIPY dye (3) in ethylene glycol, 15 h, reflux to give novel compounds (4 and 5). The purity of compounds (3-5) was confirmed by FT-IR, matrix-assisted MALDI-MS, 1H, and 19F NMR spectrometry. The spectral data of compounds are given in the SI part (Fig. S1-S6). In addition, the crystal structure of compound 3 was determined by single crystal X-ray diffraction (Fig. 2). FT-IR spectrum of 3 shows the characteristic BODIPY peaks at 1365 (B-F str) and 1307 (B-N str). In FT-IR spectra of 4 and 5, the peaks at 841 cm−1 belong to the PF6− counter ions of the complexes (Fig. S1). Molecular ion peak and the lack of one fluorine peak were related to the calculated values of compound 3 (Fig. S2a). Molecular ion peak and the lack of one PF6- were related to the calculated values of compound 4 (Fig. S2b), while molecular ion peak and the lack of two PF6- were related to the calculated values of compound 5 (Fig. S2c). The 1H NMR spectra of compounds (3-5) were given in (Figs. S3-S5), respectively. The 1H NMR spectra of compound 3 exhibited singlet signals for methyl protons at 1.30 and 2.51 ppm. The proton peaks of pyrrole exhibited at 5.93 ppm. The aromatic protons of the compound exhibited at 7.20-8.70 ppm interval. The 1H NMR spectra of compound 4 exhibited singlet for signals for methyl protons at 2.17 ppm. The proton peaks of pyrrole exhibited at 5.30 ppm. The other proton peaks of the compound exhibited at 7.19-9.00 ppm interval. The 1H NMR spectra of compound 5 exhibited singlet for signals for methyl protons at 2.04 ppm. The proton peaks of pyrrole exhibited at 5.30 ppm. All the aromatic proton peaks of the compound exhibited at 7.11-9.00 ppm interval. The 19F NMR spectra of compounds (3-5) were given in SI (Fig. S6).
3.2. X-ray crystallography
The crystal structure of compound 3 was determined by single-crystal X-ray crystallography, the selected data collection and refinement details were presented in Table 1.
Table 1. X-ray crystallographic data and refinement parameters for compound 3.
Compound
|
3
|
Empirical formula
|
C23H21B1F2N4
|
Formula weight
|
402.25
|
Temperature (K)
|
150 (2)
|
Crystal system
|
Monoclinic
|
Space group
|
P21/n
|
a (Å)
|
16.5067(7)
|
b (Å)
|
6.9833(3)
|
c (Å)
|
17.3670(7)
|
b (°)
|
103.8983(16)
|
Volume (Å3)
|
1943.31(14)
|
Z
|
4
|
Density (calc, Mg/m3)
|
1.375
|
Absorption coeff. (mm-1)
|
0.096
|
F(000)
|
840
|
qmax (°)
|
25.24
|
Reflections collected
|
3963
|
Independent reflections
|
3102
|
Rint (merging R value)
|
0.0996
|
Parameters
|
275
|
R (F2>2sF2)
|
0.0864
|
wR (all data)
|
0.1646
|
Goodness-of-fit on F2
|
1.285
|
The compound 3 is a BODIPY derivative which is meso- substituted with dipyridyl- moiety as shown in Figure 2. All bond and conformational parameters are found in normal range for previous BODIPY and dipyridyl derivatives [41,42]. The 16-membered main BODIPY core of the structure having two five-membered and one six-membered rings is nearly planar, and two fluorine atoms bonded to boron in a tetrahedral geometry located in two sides of those plane. Two pyridine rings of the dipyridyl moiety are also planar even single C18-C19 bond could have been let their rotation, the nitrogen atoms of two pyridine rings are found in trans positions respect to each other. The angle between planes of BODIPY core and dipyridyl- moiety is 67.74° (Fig. S7).
3.3. Photophysical and photochemical properties
Photophysical properties of novel compounds (3-5) in THF solutions were examined via UV-vis absorption and emission spectroscopy. Normalized absorption spectra of compounds (3-5) were shown in Figure 3a. Maximum absorption band of 3 was observed at 504 nm (ε = 108000 M−1 cm−1). Maximum absorption band of 4 and 5 were observed at 533 nm (ε = 79000 M−1 cm−1) and 558 nm (ε = 39000 M−1 cm−1), respectively. These bands can be assigned to the S0-S1 transitions. The molar absorption coefficient (ε) of 4 was seen to be higher than that of 5 (Table 2). Stokes shifts of the compounds 4 and 5 were about 61 and 62 nm respectively (Table 2). Absorption spectra of compounds (3-5) in THF solutions were investigated at different concentrations (10-6-10-5 M for 3 and 10-5-10-4 M for 4 and 5) and any change at absorption wavelength was observed (Fig. S8a, S9a, S10a). This result demonstrates that the relationship between the maximum absorption wavelength and concentration of the compounds are convenient with Lambert-Beer law, and this means that compounds have no aggregation between given concentration intervals. Emission spectra of compounds (3-5) in THF solutions were investigated at different concentrations (10-6-10-7 M for 3 and 10-4-10-5 M for 4 and 5). Normalized emission spectra of compounds (3-5) were shown in Figure 3b. The maximum emission band of 3 was observed at 518 nm when excited at 450 nm. The maximum emission band of 4 and 5 were at 594 nm and 620 nm when excited at 450 nm, respectively (Fig. 3b). Fluorescence lifetimes (τF) of the compounds were directly measured (Fig. S11) and τF values were determined by monoexponentially calculations as 1.3±0.004 ns, 0.9±0.02 ns and 0.02±0.014 for 3, 4, and 5, respectively (Table 2). It was observed that maximum emission wavelengths of BODIPY linked iridium (4) and ruthenium (5) complexes shifted red region (~76 nm for 4 and ~102nm for 5) with a concomitant decrease of ε values. As a result of this bathochromic shift, Stoke’s shifts of these derivatives increased. On the other hand, the direct technique was used to determine 1O2 generation. For compounds 4, 5 and Rose Bengal (RB) as a standard, the 1O2 phosphorescence peaks at 1270 nm were measured in THF solutions. Compounds (4, 5, and RB) were each given the same absorbance values (0.210), after which they were stimulated by a xenon arc light source at the corresponding absorption maxima and determined by a near-IR detector (Fig. S12). Since same absorbance values of the compounds were examined, the area below the phosphorescence peaks can be straight correlated. Compounds 4 and 5 were produced 1O2. Using Eq. (2), the 1O2 quantum yields were calculated to be 0.36 for compound 4 and 0.41 for compound 5. The outcomes demonstrated that compound 5 produced 1O2 more effectively than compound 4. The increase in φΔ can be explained by the accounts for the rise in spin-orbital coupling (SOC) and the yield of intersystem crossing (ISC) [43]. These two new compounds have remarkable photosensitizing activity like as many BODIPY derivatives in literature and more effective than some other PSs based on BODIPY based Ir and Ru complexes [26, 27, 44-46].
Table 2. Photophysical properties of compoundsa
Compound
|
λabs (nm)
|
λems (nm)
|
εb, M-1cm-1
|
Δstokes (nm)
|
ƬFc (ns)c
|
ɸFd
|
φΔe
|
3
|
504
|
518
|
108000
|
14
|
1.3±0.004
|
0.14
|
N.D.f
|
4
|
533
|
594
|
79000
|
61
|
0.9±0.2
|
0.06
|
0.36
|
5
|
558
|
620
|
39000
|
62
|
0.02±0.014
|
0.05
|
0.41
|
[a] THF.
[b] Molar extinction coefficients.
[c] Lifetime.
[d] Fluorescence quantum yield.
[e] Singlet oxygen quantum yield.
[f] No phosphorescence for this compound.