Agnieszka Skotnicka1, Przemysław Czeleń2. 1. Faculty of Chemical Technology and Engineering, UTP University of Science and Technology, Seminaryjna 3, 85-326 Bydgoszcz, Poland. 2. Department of Physical Chemistry, Collegium Medicum, N. Copernicus University, Kurpińskiego 5, 85-950 Bydgoszcz, Poland.
Abstract
Novel fluorescent dyes such as benzoxazole-boron complexes, bearing β-ketoiminate ligands, have been synthesized and characterized with a focus on the influence of a substituent on the basic photophysical properties. 1H, 11B, 13C, 15N, and 19F nuclear magnetic resonance (NMR) spectra of substituted 2-phenacylbenzoxazole difluoroboranes have been recorded and discussed. It is worth mentioning that a high correlation coefficient was found between 15N-NMR parameters and substituent constants. The photophysical properties of these new dyes have been investigated by fluorescence and ultraviolet-visible (UV-Vis) absorption spectroscopy. The geometry optimization, vibrational spectra, and the HOMO and LUMO energies were calculated based on density functional theory with the use of the B3LYP functional and 6-311++G(d,p) basis set.
Novel fluorescent dyes such as benzoxazole-boron complexes, bearing β-ketoiminate ligands, have been synthesized and characterized with a focus on the influence of a substituent on the basic photophysical properties. 1H, 11B, 13C, 15N, and 19F nuclear magnetic resonance (NMR) spectra of substituted 2-phenacylbenzoxazole difluoroboranes have been recorded and discussed. It is worth mentioning that a high correlation coefficient was found between 15N-NMR parameters and substituent constants. The photophysical properties of these new dyes have been investigated by fluorescence and ultraviolet-visible (UV-Vis) absorption spectroscopy. The geometry optimization, vibrational spectra, and the HOMO and LUMO energies were calculated based on density functional theory with the use of the B3LYP functional and 6-311++G(d,p) basis set.
Boron dipyrromethene (BODIPY) dyes display excellent photophysical and optoelectronic properties, such as high photostability, a large absorption coefficient in the visible and near-infrared (IR) ranges, excellent chemical stability, high fluorescence quantum yields, relatively long excited-state lifetime, good solubility in organic solvents, relative insensitivity to environmental conditions, and good biocompatibility [1,2,3]. Moreover, the BODIPY chromophore is a versatile platform for the construction of fluorescent probes for bioimaging and biosensing applications [4,5,6]. In addition, novel photoinitiators based on the BODIPY are widely used for efficient cationic polymerization of epoxy, epoxy-silicone, and vinyl ether monomers [7,8].There are mainly three types of these fluorine-boron complexes, classified as N,N bidentate, O,O bidentate, and N,O bidentate compounds. The typical BODIPY core contains two pyrrole units and its structure is usually symmetric. The compounds studied now contain NBF2O moiety. They carry an unsymmetrically chelated BF2 moiety. It was found that some difluoroboron β-ketoiminate boron complexes bearing benzoxazole gave strong emissions in solid states on account of aggregation-induced emission (AIE). The reversible mechanofluorochromism was due to the transformation between crystalline and amorphous states [9,10].In our previous published work, we have investigated the influence of heteroatom (X = O, S, and NMe) substitution in a five-membered heterocyclic ring on the photophysical properties of novel BF2 complexes containing or not a dimethylamino group (R = NMe2) [11]. It was shown that the fluorescence yields of the dimethylamino derivatives were much larger (up to one order of magnitude) than those of the corresponding unsubstituted compounds. Therefore, using the electron-donating or electron-accepting substituents, the electronic properties of the compounds may be tuned [12,13]. This study provides a report on the basic photophysical properties of a recently synthesized series of substituted 2-phenacylbenzoxazole difluoroboranes (Scheme 1) with a view towards the effect of substitution on their properties.
Scheme 1
Structure and atom numbering in 1–8.
2. Results and Discussion
2.1. Synthesis and NMR Data
Treatment of 2-methylbenzoxazole with benzoyl chloride and triethylamine causes that the 2-methyl group undergoes double benzoylation, i.e., it is transformed to –CH=C(Ph)–COOPh. Non purified intermediate products 1a–8a were always used in the subsequent synthetic step. By refluxing their morpholine solutions, 1a–8a can be easily transformed into 2-phenacylbenzoxazoles 1b–8b [14]. In solution, compounds 1b–8b exist in two tautomeric forms, ketimine form (K) and enolimine form (O), through keto-enol tautomerization. The ketimine tautomer structure was confirmed by the methylene signals observed at the range of 4.54–4.67 ppm (s, 2H) in their 1H-NMR spectra. Enolimine tautomers were also confirmed by the 1H-NMR signals at 6.05–6.43 ppm (s, 1H, C=CH) and 12.4–12.8 ppm (s, 1H, OH) [15]. The tautomeric mixture 1b–8b was then allowed to react with the boron trifluoride ethyl etherate in the presence of N-ethyldiisopropylamine in dichloromethane to give the corresponding BF2 complex 1–8 (Scheme 2).
Scheme 2
The schematic representation of the synthesis of 2-phencylbenzoxazole difluoroboranes where R = 4-NMe2 (1), 4-OMe (2), 4-Me (3), 3-Me (4), H (5), 3-OMe (6), 4-Cl (7), 3-Cl (8).
The 1H, n class="Chemical">11B, 13C, 15N, and 19F-NMR spectra that confirm the structures of 1–8 are maintained in solution. NMR chemical shifts of characteristic nuclei are collected in Table 1.
Table 1
Selected 1H, 11B, 13C, 15N and 19F-NMR chemical shifts of 2-phenacylbenzoxazole difluoroboranes 1–8 for 0.1–0.2 M solution in CDCl3 at 30 °C.
No.
Substituent
C10
C11
H10
B13
F13
N13
1
4-NMe2
77.74
172.13
6.81
1.79
−134.64
-
2
4-OMe
78.85
172.23
6.37
1.80
−135.59
−215.72
3
4-Me
79.74
172.63
6.44
1.84
−135.34
−215.01
4
3-Me
80.33
172.70
6.47
1.85
−135.14
−214.18
5
H
82.11
170.79
6.49
1.85
−135.07
−213.54
6
3-OMe
80.56
172.28
6.47
1.84
−134.98
−213.97
7
4-Cl
80.63
171.01
6.45
1.81
−134.98
−213.00
8
3-Cl
81.17
170.64
6.48
1.81
−134.78
−212.43
The 1H-NMR signal of H10 of 2-phenacylbenzoxazole difluoroboranes 1–8 can be seen at δ = 6.37–6.81 ppm in CDCl3, which is a singlet. The presence of a boron atom is confirmed by signals at δ = 1.79–1.85 ppm (triplet). The resonance of F13 at δ = −134.14 to −135.59 ppm shows as a quartet (two fluorine atoms). Analogously Kubota et al. [16] observed signals at −134.6 ppm (q, 2F) for boron complex of 2-methylbenzothiazole. N3 in the 15N-NMR spectra of 2-phenacylbenzoxazole difluoroboranes 1–8 resonates in the ranges of δ = −212.43 to −215.72 ppm. These signals were correlated to the Hammett substituent constant σ [17]. It was observed that with increasing electron-withdrawing ability of substituent, the 15N-NMR signal experienced a continuous upfield shift, which was indicated by a linear dependence of the chemical shift against σ (δ(15N) = 4.79 σ–214.12, R2 = 0.909), Figure 1. 1H NMR and 13C NMR spectra of 1–8 are available in Supplementary Materials.
Figure 1
A plot of N3 chemical shift [ppm] vs. Hammett constant for 1–8.
2.2. Spectroscopic Properties
The measured absorption spectra of all eight compounds obtained in chloroform are given in Figure 2, and the associated data are presented in Table 2. Chloroform is a known solvent to prevent boron-ligand dissociation, exciplex formation, or the photochemical reactions possible in solvents containing Lewis bases, aromatic rings, or double bonds [18].
Figure 2
Normalized absorption spectra of 1–8 in chloroform (values were converted to have the maximum normalized at 1).
Table 2
Photophysical properties of examined compounds measured in chloroform.
No.
Substituent
λabs(nm)
λfl(nm)
ε(M−1·cm−1)
Stokes Shift (cm−1)
ϕfl(× 10−2)
1
4-NMe2
410
458
42,500
2449
98.18
2
4-OMe
362
433
32,900
4530
1.82
3
4-Me
354
428
31,219
4884
0.66
4
3-Me
352
423
22,961
4769
0.48
5
H
350
424
27,000
4905
0.54
6
3-OMe
354
429
26,727
4938
0.57
7
4-Cl
355
428
29,615
4805
0.58
8
3-Cl
353
430
29,648
5073
0.50
As shown in Figure 2, 2-phenacylbenzoxazole difluoroboranes 1–8 have an intense, wide absorption band in the 300–410 nm region, which is attributed to the π → π* transition but also associated with n → π* photochemically forbidden transition. The position of the absorption band depends on the dye structure. Absorption at λmax was found to progressively shift to longer wavelength upon substituting unsubstituted complex 5 by weaker electron-withdrawing (Cl) and then electron-releasing (4-Me, 4-OMe, and 4-NMe2) substituents. It must be highlighted that the electron pulling effect from the boron atom created a strong electronic current in the six-membered ring such as B-O-C-C-C-N, which is responsible for the higher % of bathochromic in compound 2 in chloroform. A considerable red-shift of the absorption band was observed for compound 1 (4-NMe2). The 4-NMe2 substituent causes a 58 nm red shift in absorption relative to the parent compound 5. The molar absorption coefficient (ε) of 1 (42,500) was significantly higher than for other complexes (Table 2). These red-shifts of the absorption maxima position along with the high molar absorption coefficients indicate that the transitions of the R = NMe2 derivative have a π → π* nature associated with a significant charge transfer (CT) [11].The changes in Stokes shifts (Figure 3) and the molar absorption coefficients related to the nature of the substituent in 2-phenacyl moiety are also reflected in changes in the fluorescence quantum yields. As can be seen in Table 2, the measurements of the fluorescence quantum yields of the investigated dyes remain very small. Only derivatives with electron-releasing groups exhibit fluorescence quantum yields significantly higher (up to one order of magnitude for 1).
Figure 3
The normalized UV-Vis absorption (a) fluorescence and (b) spectra of 1 and 5 in CHCl3.
From the data presented in Table 3 and Figure 4, it is seen that the polar protic solvents such as methanol, dimethylformamide, acetonitryle, and dimethyl sulfoxide cause a bathochromic shift of the absorption band. The largest shift of the absorption bands towards longer wavelengths is observed for the most protic solvent, which is dimethyl sulfoxide. It is clear from Table 3 that the Stokes shift increases with varying solvent polarity. With an increase in solvent polarity, the magnitude of the Stokes shift varies from 2449 cm−1 to 3043 cm−1 for compound 1 (4-NMe2), and from 4530 cm−1 to 6464 cm−1 for other derivatives.
Table 3
Spectroscopic properties of 2-phenacylbenzoxazole difluoroboranes 1–8 in solvents of different polarity.
No.
Toluene
CHCl3
THF
AcOEt
Acetone
MeOH
DMF
MeCN
DMSO
1
λabs (nm)
407
410
408
407
420
419
426
415
431
λflu (nm)
453
458
465
462
427
473
479
475
486
Stokes (cm−1)
2495
2449
3004
2925
2623
2725
2597
3043
2626
2
λabs (nm)
362
362
361
359
360
358
363
359
375
λflu (nm)
450
433
432
435
432
431
435
463
438
Stokes (cm−1)
5402
4530
4553
4867
4630
4731
4560
6257
3836
3
λabs (nm)
355
354
354
352
352
351
355
351
356
λflu (nm)
434
428
429
432
426
471
431
455
431
Stokes (cm−1)
5127
4884
4938
5261
4935
7259
4967
6512
4888
4
λabs (nm)
354
352
353
351
351
349
353
350
355
λflu (nm)
435
423
427
433
430
424
429
448
430
Stokes (cm−1)
5261
4769
4909
5395
5234
5068
5019
6250
4913
5
λabs (nm)
354
350
351
349
349
349
352
349
354
λflu (nm)
433
424
425
447
433
425
427
447
456
Stokes (cm−1)
5154
4905
5071
6282
5559
5124
4990
6282
4993
6
λabs (nm)
356
354
354
352
352
351
355
351
357
λflu (nm)
436
429
428
431
432
426
432
434
455
Stokes (cm−1)
5154
4938
4884
5207
5261
5016
5021
5448
4916
7
λabs (nm)
357
355
355
352
353
352
355
352
358
λflu (nm)
458
428
456
448
456
463
459
455
460
Stokes (cm−1)
6431
4805
6239
6088
5601
6545
6382
6447
6462
8
λabs (nm)
354
353
352
351
351
350
353
350
354
λflu (nm)
456
430
454
454
454
454
456
452
459
Stokes (cm−1)
6319
5037
6383
6464
6464
6545
6399
6447
6462
Figure 4
(a) Normalized absorption (a) and fluorescence (b) spectra of 2-(4-dimethylamino)benzoylbenzoxazole difluoroborane (1) in solvents of different polarity.
2.3. Solvatochromism
To verify the effect of solvent polarity, Stokes shifts (Δν) of 1–8 in a variety of solvents were plotted against the solvent polarity parameter Δf (ε, n) with the general form of the Lippert-Mataga equation given below [19,20]
in which Δν = ν − ν stands for Stokes shift, ν and ν are absorption and emission frequency (cm−1), ħ is the Planck’s constant, c is the velocity of light in vacuum, a is the Onsager radius, and b is a constant. Δf is the orientation polarizability, ε is the refractive index, n is the dielectric constant, μ and μ are the dipole moments of the emissive and ground states, respectively, and ε0 is the permittivity of the vacuum. (μ − μ)2 is proportional to the slope of the Lippert-Mataga plot.Lippert-Mataga plots showed higher Stokes shifts for all compounds in acetonitrile as a solvent, nonlinear nature of the plot was observed in acetonitrile for 1–6 shown in Figure 5, while such behavior for 7 and 8 was observed in chloroform. Compound 7 exhibited similar nature to that of 8.
Figure 5
Lippert–Mataga plot of compounds 1–8.
2.4. Computational Details
An important factor in assessing the practical use of the compounds under consideration is their reactivity. The use of computational chemistry methods allows us to describe this property of the tested molecules in the context of a set of descriptors based on the energy values of the frontal orbitals [21]. In Table 4, there are presented values characterizing all considered substituted 2-phenacylbenzoxazole difluoroboranes, including energy values of HOMO and LUMO orbitals, energy gaps, and hardness (η). Obtained data show that among all considered molecules, the highest reactivity is exhibited by the derivative containing 4-dimethylamino substituent. Such a molecule is characterized by the lowest values of hardness and energy gap. The distribution of HOMO and LUMO orbitals obtained for this molecule is presented in Figure 6. The rest of the considered derivatives exhibit quite similar values of both reactivity descriptors, however, there is observed a trend indicating that substitution in the fourth position to aromatic ring is more favorable than in the third. Taking into account all considered substituents, a decrease in reactivity is observed in the following order 4-NMe2 > 4-OMe > 4-Cl > 4-Me > 3-Cl > H > 3-Me > 3-OMe.
Table 4
The values of hardness (η), energy gap, and energies of HOMO and LUMO orbitals were estimated for considered molecules.
No.
Substituent
HOMO (eV)
LUMO (eV)
Energy gap (eV)
η (eV)
1
4-NMe2
−5.664
−2.090
3.574
1.787
2
4-OMe
−6.168
−2.323
3.846
1.923
3
4-Me
−6.328
−2.423
3.906
1.953
4
3-Me
−6.389
−2.454
3.935
1.967
5
H
−9.438
−2.504
3.934
1.967
6
3-OMe
−6.390
−2.425
3.964
1.982
7
4-Cl
−6.523
−2.663
3.860
1.930
8
3-Cl
−6.595
−2.684
3.910
1.955
Figure 6
Distribution of HOMO (a) and LUMO (b) orbitals for 2-(4-dimethylamino)benzoyl-benzoxazole difluoroborane (1).
2.5. Vibrational Analysis
Vibrational spectroscopy is used extensively for the study of molecular conformations, identification of functional groups and reaction kinetics, etc. Spectroscopy FT-IR and quantum chemical calculations using the B3LYP functional and 6-311++G(d,p) basis set have been employed to study the structure of the title compounds. Substituted 2-phenacylbenzoxazoles 1b–8b (starting compounds that were converted to BF2 complexes) exist in two tautomeric forms, the ketimine form (K) and enolimine form (O), through keto-enol tautomerization. A strong band observed in the FT-IR spectrum at around 1660 cm−1 was assigned to the C=O stretching vibration of ketimine tautomer. The free hydroxyl group absorbs strongly in the region 3700–3584 cm−1, whereas the existence of intramolecular hydrogen bond formation can lower the O–H stretching frequency in the range 3500–3200 cm−1 with an increase in intensity and breadth [22]. In the present study, a strong band observed at about 3380 cm−1 in FT-IR spectrum was assigned to O–H stretching vibration. The observed FT-IR spectrum of 2-(4-dimethylamino)benzoylbenzoxazole (1b), where the intensity was plotted against the vibrational wavenumber, is shown in Figure 7.
Figure 7
The observed IR absorption spectra of 2-(4-dimethylamino)benzoylbenzoxazole (1b) in the region 500–2000 cm−1 and 2800–3200 cm−1.
For the substituted 2-phenacylbenzoxazole difluoroboranes 1–8, no O–H and C=O vibrations could be observed in the FT-IR spectra. The theoretical spectrogram for the FT-IR spectrum of 2-(4-dimethylamino)benzoylbenzoxazole difluoroborane (1) was also constructed and compared with the experimental spectrum. The computed vibrational frequencies of this molecule were found in good agreement with experimental results. To improve the numerical agreement, the linear scaling method as given by Yoshida et al. [23] has been used. In this, the calculated harmonic vibrational wavenumbers have been scaled by the formula (νobs/νcal = (1.0087–0.000016 × νcal) cm−1) to facilitate a better agreement with the observed values. The value of the correlation coefficient was found to be R2 = 0.9997, which shows good agreement of the simulated wavenumbers with the observed one for the molecule of 2-(4-dimethylamino)benzoylbenzoxazole difluoroborane (1). The comparison of the experimental and simulated IR spectrum is presented in Figure 8.
Figure 8
Comparison of the observed with simulated (scaled) IR absorption spectra of 2-(4-dimethylamino)benzoylbenzoxazole difluoroborane (1) in the region 500–2000 cm−1 and 2800–3200 cm−1.
3. Experimental
3.1. Materials
All reagents and solvents were purchased from Sigma-Aldrich (Poznań, Poland) and used without further purification. The highest (≥99%) purity of all used chemicals was required for spectroscopic studies.
3.2. Synthesis
The compounds were obtained from 2-phenacylbenzoxazoles 1b–8b (Scheme 2) as described earlier [15]. The typical procedure was as follows: BF3 etherate (three equivalents) was added to the magnetically stirred solution (nitrogen atmosphere) of substituted 2-phenacylbenzoxazole (1 g) in dry chloroform (15–20 mL) and N-ethyldiisopropylamine (three equivalents). Then the solution was stirred overnight at room temperature, and concentrated Na2CO3 water solution (20 mL) was added slowly to the mixture. The organic fraction was separated, the water layer extracted with chloroform (two times using ca. 20–30 mL), dried (Na2SO4) and evaporated under reduced pressure. Residual solids were purified by flash chromatography (SiO2) using DCM as an eluent.
The 1H-NMR spectra were recorded using an Ascend III spectrometer operating at 400 MHz, Bruker (Bydgoszcz, Poland). Chloroform was used as a solvent and tetramethylsilane (TMS) as the internal standard. Chemical shifts (δ) were reported in ppm relative to TMS and coupling constants (J) in Hz.The elemental analysis was made with a Vario MACRO 11.45–0000, Elemental Analyser System GmbH, operating with the VARIOEL software (version 5.14.4.22).The melting point was measured on the Melting Point M-565 Apparatus (Buchi) with the measuring speed 5 °C/min.The absorption and emission spectra were measured at room temperature in a quartz cuvette (1 cm) using an Agilent Technology UV-Vis Cary 60 Spectrophotometer and a Hitachi F-7000 Spectrofluorometer, respectively.The fluorescence quantum yields for the compounds in chloroform were determined as follows, the fluorescence spectrum of diluted (A ≈ 0.1) boranes solution was recorded by excitation at the absorption band maximum of the reference. Diluted 9,10-diphenylanthracene in cyclohexane (ϕ = 0.93) [24] was used as reference. The fluorescence spectrum of 9,10-diphenylanthracene was obtained by excitation at its absorption peak at 355 nm. The quantum yield of the tested compounds (ϕ) was calculated using the following equation [25]:
where ϕ is the fluorescence quantum yield of the reference sample (9,10-diphenylanthracene) in cyclohexane, A and A are the absorbance of the dye and reference samples at the excitation wavelengths (355 nm), I and I are the integrated emission intensity for the dyes and references sample, n and n are the refractive indices of the solvents used for the dyes and reference, respectively. Coumarine 153 in cyclohexane (ϕ = 0.90 [26]; λ = 393 nm) was used as reference standard for compound carrying −NMe2 group.Infrared spectra have been recorded in the region 360–7000 cm−1 on a Bruker Alpha FT-IR spectrometer with a spectral resolution of 2 cm−1 using the ATR (attenuated total reflectance) method.The geometry optimization, vibrational spectra, and the HOMO and LUMO energies were calculated based on density functional theory with the use of B3LYP [27,28,29] functional and 6-311++G(d,p) basis set [30,31]. All calculations were carried out using Gaussian 09 software [32]. The analysis of the frontier orbitals and IR spectra including extraction of frequencies and a visual presentation of the vibrational modes and orbitals was realized with the use of Avogadro 1.2.0 application [33].
4. Conclusions
The indicated aims were achieved through a synthesis of a series of 2-phenacylbenzoxazole difluoroboranes substituted by a weaker electron-withdrawing (Cl) and electron-releasing (4-Me, 4-OMe, and 4-NMe) substituents. Complexes have been identified based on a magnetic atomic nucleus 1H, 11B, 13C, 15N, and 19F isotope resonance spectra. 15N-NMR shifts correlate with the substituent character of the phenyl ring with R2 = 0.91. The spectral data show that the absorption and fluorescence properties of 2-phenacylbenzoxazole difluoroboranes 1–8 depend on the character of the substituent. The experimental results indicate the positive solvatochromism of studied compounds with increasing solvent polarity. Among all derivatives, only 2-(4-dimethylamino)-benzoylbenzoxazole difluoroborane 1 (the NMe2 group was the strongest electron donor in the series) presented strong and relatively red-shifted fluorescence in the chloroform. Other complexes hardly demonstrated any fluorescence, indicating that probably only benzoxazole-boron complexes with strongly electron-releasing groups like amino groups could be attractive for their use as new fluorescent molecules for future applications in bio-labeling, medicine, or fluorescence microscopy, and they might be alternative or supplementary to popular BODIPY dyes. Furthermore, the study using these compounds as photosensitizers in the photopolymerization process is still in progress.
Authors: Borys Ośmiałowski; Anna Zakrzewska; Beata Jędrzejewska; Anna Grabarz; Robert Zaleśny; Wojciech Bartkowiak; Erkki Kolehmainen Journal: J Org Chem Date: 2015-02-09 Impact factor: 4.354