Tsutomu Ishi-i*a,
Kei Ikedab,
Michiaki Ogawaa and
Yutarou Kusakakib
aDepartment of Biochemistry and Applied Chemistry, National Institute of Technology, Kurume College, 1-1-1 Komorino, Kurume 830-8555, Japan. E-mail: ishi-i@Kurume-nct.ac.jp
bMaterial Engineering Advanced Course, Advanced Engineering School, National Institute of Technology, Kurume College, 1-1-1, Komorino, Kurume, Fukuoka 830-8555, Japan
First published on 14th October 2015
In this paper, we report a systematic study on the light-emitting behavior of a series of triphenylamine-based donor–acceptor-type dyes in the solution and solid states as well as in the aggregated state in polar aqueous media. The emission band shifted bathochromically along with the decrease in the fluorescence quantum yield as the solvent polarity was increased from nonpolar cyclohexane to polar DMF. In a THF/water medium, the emission was quenched in a low water volume, whereas the emission was recovered and increased in a high water volume. In a low water volume, the dye molecules exist in a monomeric form, and the fluorescence quenching increases with increasing water fraction, similar to that observed in the solvent-polarity-dependence study. In contrast, the dye molecules aggregated in a high water volume. This is probably because the inside of aggregates is less polar than the outside, thus preventing nonradiative deactivation and recovering the emission. This unusual emission was achieved by triphenylamine-based dyes containing a relatively strong acceptor moiety such as quinoxaline, benzothiadiazole, and thiadiazolopyridine, providing longer-wavelength red and near-IR emission. In the benzothiadiazole-based dyes, when the phenyl groups in the donor moieties were replaced with methyl groups, the fluorescence quantum yield decreased, indicating that the triphenylamine donor moiety is suitable for emission in the aggregated state. The nonplanar structure of triphenylamine disrupts an ordered packing and produces a less-ordered spherical aggregate, leading to an efficient light emission even in polar aqueous media.
Alternatively, push–pull-type conjugated systems comprising electron-donating and electron-accepting moieties are the simplest systems for generating longer-wavelength emissions.8 With the increase in the strength of donor–acceptor conjugates, the emission band shifts bathochromically, producing red and near-infrared (near-IR) light emissions.9,10 The red and near-IR light emissions produced by such systems are very important for biological applications, because they lie in the biological optical window.11 However, the efficiency of longer-wavelength emission decreases in polar aqueous media, because a highly polarized excited state arising from the donor–acceptor characteristic increases the formation of a nonradiative deactivation channel.12,13
In a previous communication, we reported that red-light emission can be attributed to the aggregation of donor–acceptor dyes comprising benzothiadiazole acceptor and triphenylamine donor moieties even in a polar aqueous medium.14 The prevention of the highly polarized excited state due to aggregation also contributes to red-light emission,15 in addition to the prevention of intramolecular rotation as widely known in aggregation-induced emission.16–20 Recently, some donor–acceptor systems were developed for aggregation-induced emission, where, in fact, red and near-IR light emissions were achieved in an aqueous medium containing an organic solvent.21–28 An amino donor moiety was combined with an acceptor moiety such as cyano-substituted oligo(phenylene vinylenes),21,22 triazines,23 fluorenones,24 boron dipyrromethenes,25 fumaronitriles,26 acrylonitriles,27 and quinoline-malononitriles.28 Important information about aggregation-induced emission can be obtained, if such interesting light-emitting systems are systematically studied by screening the donor and acceptor moieties. Thus, more efforts should be devoted to systematic studies on elucidating the structure–property relationship of this interesting emission behavior. In this study, a series of novel donor–acceptor-type dyes were synthesized, and a library of donor–acceptor light-emitting systems was developed as follows: first, various benzothiadiazole–triphenylamine-based donor–acceptor–donor and donor–acceptor dyes were studied to generalize the light emission behavior in the aggregated state. To further expand the generality, additional π-electron spacers such as ethylene, acetylene, and benzene moieties were introduced between the triphenylamine donor and benzothiadiazole acceptor moieties. Second, the benzothiadiazole acceptor moiety was replaced with weak acceptor moieties such as benzene, naphthalene, and thiazolothiazole, as well as with strong acceptor moieties such as quinoxaline, fluorobenzothiadiazole, and thiadiazolopyridine. In this donor–acceptor library, the characteristics of donor–acceptor conjugate were determined based on the combined electrochemical and photochemical results. The emission behavior in the aggregated state was systematically studied based on the donor–acceptor strength. Finally, the donor moiety was screened. In the triphenylamine moiety, the phenyl group was replaced with a methyl group to evaluate the steric and electronic effects of the donor moiety. In this paper, we report a systematic study on the light-emitting behavior of various donor–acceptor-type dyes and propose a convenient strategy for generating longer-wavelength emission based on the aggregation of donor–acceptor-type dyes.
| Comp. | Ered1/2b (V, vs. Fc/Fc+) | Eox1/2b (V, vs. Fc/Fc+) | ELUMOc (eV) | EHOMOc (eV) | ΔEc (eV) |
|---|---|---|---|---|---|
| a Measured in dichloromethane (5.0 × 10−4 M) in the presence of tetrabutylammonium hexafluoroborate (0.1 M) at a scan rate of 100 mV s−1.b Ered1/2 is the half-wave reduction potential, and Eox1/2 is the half-wave oxidation potential.c HOMO and LUMO level were calculated using the HOMO level of ferrocene (−4.80 eV). ELUMO = −(4.80 + Eredonset). EHOMO = −(4.80 + Eoxoffset). ΔE = ELUMO − EHOMO.d The quasireversible oxidation potentials could not be observed. | |||||
| 1a | −1.90 | 0.47 | −2.85 | −5.33 | 2.48 |
| 1b | −1.77 | 0.28, 0.50d | −2.98 | — | — |
| 1c | −1.65 | 0.56 | −3.10 | −5.44 | 2.34 |
| 1d | −1.86 | 0.48 | −2.90 | −5.34 | 2.44 |
| 2 | −1.93 | 0.49 | −2.83 | −5.34 | 2.51 |
| 3 | −1.89 | 0.51 | −2.86 | −5.36 | 2.50 |
| 4 | −1.90 | — | −2.85 | — | — |
| 5 | −1.94 | 0.37 | −2.81 | −5.22 | 2.41 |
| 6 | −2.03 | 0.25 | −2.72 | −5.13 | 2.05 |
| 7 | — | 0.45 | — | −5.34 | — |
| 8 | — | 0.49 | — | −5.34 | — |
| 9 | −2.52 | 0.50 | −2.21 | −5.40 | 3.19 |
| 10 | −2.14 | 0.50 | −2.61 | −5.38 | 2.77 |
| 11 | −1.86 | 0.51 | −2.90 | −5.40 | 2.50 |
| 12 | −1.64 | 0.52 | −3.11 | −5.41 | 2.30 |
In addition to the oxidation potential, a quasireversible reduction potential was observed between −1.64 and −2.52 V (vs. Fc/Fc+) for dyes 1a–d, 2, 3, 5, 6, and 9–12 bearing a relatively strong acceptor moiety, indicating the donor–acceptor characteristic. In contrast, the reduction potential was not observed in dyes 7 and 8 bearing a benzene moiety and a naphthalene moiety, respectively. In the triphenylamine-based donor–acceptor–donor dyes, the order of electron–accepting property increased as follows: dye 12 (−1.64 V, vs. Fc/Fc+) bearing a thiadiazolopyridine moiety > dye 11 (−1.86 V) bearing a fluorobenzothiadiazole moiety ≥ dye 1a (−1.90 V) bearing a benzothiadiazole moiety > dye 10 (−2.14 V) bearing a quinoxaline moiety > dye 9 (−2.52 V) bearing a thiazolothiazole moiety > dye 7/8 bearing a benzene/naphthalene moiety.
The HOMO and LUMO energy levels and band gaps were estimated from the reduction and oxidation potentials (Table 1). Quinoxaline-, benzothiadiazole-, and thiadiazolopyridine-based dyes 1a, 10, 11, and 12 exhibited smaller band gaps (2.30 to 2.77 eV) than benzene-, naphthalene-, and thiazolothiazole-based dyes 7, 8, and 9 (>3.19 eV). Thus, the dyes can be divided into two groups: a strong donor–acceptor system (dyes 1a and 10–12) and a weak donor–acceptor system (dyes 7–9). Moreover, the band gap decreased from dye 1a (2.48 eV) to dyes 5 (2.41 eV) and 6 (2.05 eV) by replacing the phenyl group of the donor moieties with a methyl group.
On the other hand, the fluorescence spectra showed a strong dependence on solvent polarity. The emission band (λem) shifted bathochromically along with the decrease in the fluorescence quantum yield (ΦF) as the solvent polarity was increased (Fig. 1, S2 and S3, and Table S1, ESI†).25–27 When the benzothiadiazole–triphenylamine dye 1a was dissolved in nonpolar solvents such as cyclohexane and toluene, a yellow light was emitted at 557–592 nm with a high ΦF value of 0.80–0.85 (Fig. 1 and Table S1, ESI†). The emission band shifted to the longer-wavelength orange-red-light region at 614, 639, and 657 nm in THF, DCM, and DMF, respectively. Along with the bathochromic shift, the ΦF value decreased from 0.85 in cyclohexane to 0.36 and 0.22 in DCM and DMF, respectively (Table S1, ESI†). This decrease in fluorescence correlated with the increase in polarity, which facilitates the excited-state polarization of the molecule through a charge-transfer process.21 The polarized excited-state is stabilized by solvation owing to the polar solvent molecules.15
A similar trend of bathochromic shift along with the decrease in fluorescence was observed also in asymmetric donor–acceptor dyes 2 and 3 bearing one triphenylamine moiety and in donor–acceptor–donor dyes 1b–d bearing an additional π-electron spacer between the donor and acceptor moieties. In contrast, such a strong dependence on solvent polarity was not observed in dye 4 lacking triphenylamine donor moieties. The emission band shifted slightly in the 477–507 nm range (Fig. 1). The lacking donor moieties prevents the polarization of excited-state, leading to the slight solvent dependence. Significant polarity dependence was observed in dye 1d bearing an additional benzene π-spacer. The emission band shifted bathochromically from 527 nm in cyclohexane to 680 nm in DMF. The ΦF value was less than 0.01 in DMF. Compared to dye 1a, the bathochromic shift along with decrease in the emission of dye 1d increased significantly in polar media. The increased fluorescence can be attributed to twisted intramolecular charge transfer (TICT),25,31 as observed in the benzothiadiazole–triphenylamine dye bearing a benzene spacer.32 The difference in solvent-polarity dependence can be obtained from the Mataka–Lippert plot; the solvent effect can be evaluated using this plot from the dependence of the Stokes shift on the solvent polarity parameter.33 In the plot, the slope (13
700) of dye 1d is larger than that (8000) of dye 1a (Fig. S4, ESI†).
In a polar DMF solution, the emission band shifted bathochromically from 434–522 nm in dyes 7–9 to 615–659 nm in dyes 1a, 10, and 11 in the triphenylamine-based donor–acceptor–donor dyes (Fig. 1, S2 and Table S1, ESI†). Along with the bathochromic shift, the ΦF value decreased from 0.55–0.60 in dyes 7–9 to 0.11–0.34 in dyes 1a, 10, and 11. In particular, a significant fluorescence quenching was observed in dye 12 bearing a strong acceptor thiadiazolopyridine moiety; the emission intensity was too weak to be detected. Thus, the solvent-polarity dependence increased as follows: dyes 12 > 11 ≥ 1a > 10 > 9 > 7/8. This trend is consistent with the electron-accepting property of the dyes as determined by cyclic voltammetry.
In the benzothiadiazole-based donor–acceptor–donor dyes 1a, 5, and 6, the solvent-polarity dependence increased by replacing the phenyl group of the donor moieties with a methyl group (Fig. 1, S2 and Table S1, ESI†). In DMF, the emission band shifted bathochromically from 657 nm in dye 1a to 666 and 679 nm in dyes 5 and 6, respectively, as predicted from the cyclic voltammetry data. A large fluorescence quenching (ΦFL = 0.05) was observed in dye 6 bearing strong electron-donating dimethylamino groups.
The emission observed in the solution state was observed also in the solid state with moderate ΦF values (Table S1, ESI†). This indicates that emission will occur even in aqueous systems upon the formation of aggregates.
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Fig. 2 (a and b) UV/vis absorption and (c and d) fluorescence spectra of 1a in THF/water (10 : 0, 9 : 1, 8 : 2, 7 : 3, 6 : 4, 5 : 5, 4 : 6, 3 : 7, 2 : 8, and 1 : 9, (v/v)) at 1.0 × 10−5 M excited at 460 nm. | ||
The formation of aggregates in the emission recovery region was confirmed by the shifts in the absorption and emission bands. In dye 1a, the absorption band slightly changed to approximately 460–463 nm in the fluorescence quenching region (10–60% water fraction), indicating that the molecules of dye 1a existed as monomers (Fig. 3a). In the monomer region, the emission band shifted bathochromically from 614 nm to 639 nm due to the increase in polarity as observed in polar solvents such as DCM and DMF (Fig. 3b). On the other hand, in the emission recovery region (70–90% water fraction), the absorption band shifted bathochromically from 460 nm (60% water) to 496 nm (90% water) (Fig. 3a). The observed bathochromic shift (Δλabs) of 39 nm is most likely due to the formation of π-stacked aggregates with the J-type stacking mode, as predicted by the molecular exciton model.34 Moreover, a significant hypsochromic shift (Δλem) of the emission band was observed, from 639 nm (60% water) to 610 nm (90% water), despite an increase in the polarity (Fig. 3b). This Δλem value of 29 nm is most likely due to the local hydrophobic environment inside the aggregate structure. Thus, the fluorescence quenching was prevented by the aggregation, leading to the emission recovery and enhancement. The observed transition from the bathochromic to hypsochromic shift in the emission band is consistent with the change in the fluorescence quantum yields.
At 90% water fraction, the aggregate formation of dye 1a was confirmed and detected from the position of λFL at ∼610 nm. In the concentration range from 1 × 10−5 M to 1 × 10−10 M, the emission band hardly shifted. The fluorescence intensity at 610 nm correlated linearly with the concentration (Fig. S17 and S18, ESI†). The results indicate that the aggregates were maintained and did not dissociate into monomers even at a dilute concentration of 1 × 10−10 M.
A similar fluorescence emission behavior of aggregates was observed also in other triphenylamine–benzothiadiazole dyes 1b, 1c, and 1d bearing various π-spacers and also in asymmetric dyes 2 and 3 (Fig. 3 and S5–S9, ESI†). In these systems, the emission was quenched in a low water volume, whereas the emission was recovered and increased in a high water volume (Fig. 3c). In the emission recovery region, the bathochromic shift of the absorption band and the hypochromic shift of the emission band were observed also. Interestingly, dye 1d bearing a benzene pacer showed a large hypochromic shift of +29 nm at 90% water fraction, which is larger than those (−10 to +7 nm) of dyes 1a–c, 2, and 3. The hypochromic shift in dye 1d can be attributed to the TICT characteristic as indicated by the change in emission depending on solvent polarity. At the initial state of 0% water fraction, the emission band shifted to a longer-wavelength region because of the TICT effect, leading to a large hypochromic shift at 90% water fraction. Because of the bathochromic shift, the reddish-orange-light emission (at 627 nm) at 0% water fraction changed to an orange-light emission (at 588 nm) at 90% water fraction. The results indicate that the emission intensity as well as the emission color can be controlled by the combined effect of aggregation and TICT.
At 90% water fraction, dyes 1a, 1b, 1c, 1d, 2, and 3 showed red/orange-light emissions at 610 nm, 647 nm, 622 nm, 588 nm, 601 nm, and 604 nm (Fig. 8), with ΦF values of 0.80, 0.15, 0.28, 0.44, 0.54, and 0.47, respectively. The benzothiadiazole acceptor and triphenylamine donor moieties may play an important role in the emission of aggregates. Therefore, dye 4, without the triphenylamine donor moieties, as well as dyes 5 and 6 lacking the phenyl groups in the donor moieties were investigated (Fig. 4, 5, S10 and S11, ESI†).
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Fig. 4 (a and b) UV/vis absorption and (c and d) fluorescence spectra of 4 in THF/water (10 : 0, 9 : 1, 8 : 2, 7 : 3, 6 : 4, 5 : 5, 4 : 6, 3 : 7, 2 : 8, and 1 : 9, (v/v)) at 1.0 × 10−5 M excited at 390 nm. | ||
In dye 4, the fluorescence emission system was divided into two regions of low and high water volumes, as observed in dyes 1a–d, 2, and 3. However, dye 4 showed a different light-emitting behavior. In a low water volume, the ΦF value remained unchanged at ∼0.8, whereas the ΦF value decreased significantly to 0.08 in a high water volume (Fig. 5c). Compared to dyes 1a–d, 2, and 3, the donor–acceptor effect in dye 4 was weakened due to the lack of triphenylamine donor moieties. The weak donor–acceptor effect also resulted in the light-emitting color of the 90% water fraction, a greenish-blue light emission with a λem of 499 nm (Fig. 8). The significant fluorescence quenching in a high water volume can be attributed to different aggregate morphologies as described below.
Next, the effect of a donor moiety on the aggregation and emission behaviors was evaluated. In dye 5 bearing methylphenylamino groups and dye 6 bearing dimethylamino groups, the transition from the initial to the final emission state via the fluorescence quenching state was observed, similar to that observed for the corresponding dye 1a bearing diphenylamino groups. At 90% water fraction, the emission band shifted bathochromically from 610 nm in 1a to 625 nm in 5 and to 663 in 6, by replacing the phenyl group of the donor moieties with a methyl group. The trend is consistent with the order of electron-donating characteristic as determined by cyclic voltammetry. Although an emission recovery was observed in a high water volume, the degree of emission recovery was different. Dye 5 showed a moderate recovery of ΦF from 0.59 (0% water fraction) to 0.49 (90%), whereas dye 6 showed only a weak recovery from 0.46 (0%) to 0.14 (90%) (Fig. 5c). The degree of emission recovery in dye 5 was similar to that (from 0.79 (0%) to 0.80 (90%)) of dye 1a. In addition to dye 1a, both dyes 4 and 5 formed aggregates in the emission recovery region, as shown by the bathochromic shift of the absorption band and the hypochromic shift of the emission band (Fig. 5a and b). However, a difference was observed in the hypochromic shift. As the water fraction was changed from 60% to 90%, large hypsochromic shifts of 29 and 30 nm in dyes 1a and 5 were achieved, respectively, whereas a small shift of 11 nm was observed in dye 6 (Fig. 5b). The aggregates in dye 6 bearing dimethylamino groups may have different morphologies and insufficient hydrophobic space inside the aggregate structure, leading to a low emission recovery. The results indicate that the diphenylamino (the triphenylamine moiety) and methylphenylamino groups contribute more to the emission recovery than the dimethylamino moiety. The superiority can be attributed to the nonplanarity of the donor moieties (the diphenylamino and methylphenylamino groups) as described below.
To generally develop this light-emission system, triphenylamine-based donor–acceptor–donor dyes 7–12 bearing various acceptor moieties were investigated in THF/water aqueous media (Fig. 6 and S12–16, ESI†). In the strong acceptor systems 10–12, emission recovery was also observed in a high water volume along with the bathochromic shifts of the absorption band and the hypsochromic shifts of the emission band, as observed in the benzothiadiazole acceptor system 1a (Fig. 6 and 7). In 90% water fraction, the emission band shifted bathochromically with the increase in the electron-accepting property as follows: 1a (610 nm) ≥ 11 (603 nm) > 10 (558 nm). In dye 12 bearing a thiadiazolopyridine acceptor moiety, the emission band was observed in the longest wavelength of 658 nm at 90% water fraction, thus extending the emission tail to the near-IR region. However, a relatively small ΦF value of 0.12 was obtained (Fig. 7c). The small value can be explained by the energy-gap law: the nonradiative deactivation rate increases exponentially with decreasing emission energy.35 Thus, it can be concluded that a turn-on-type change in emission was achieved by a triphenylamine-based dye system containing a strong acceptor moiety: the fluorescence-quenching OFF-state changed to the light-emitting ON-state upon the formation of aggregates.
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Fig. 6 (a and b) UV/vis absorption and (c and d) fluorescence spectra of 7 in THF/water (10 : 0, 9 : 1, 8 : 2, 7 : 3, 6 : 4, 5 : 5, 4 : 6, 3 : 7, 2 : 8, and 1 : 9, (v/v)) at 1.0 × 10−5 M excited at 350 nm. | ||
On the other hand, weak acceptor systems 7–9 showed different emission behaviors (Fig. 7). In a low water volume, the emission intensity remained unchanged, because the highly polarized excited state could not be achieved by the weak donor–acceptor characteristic. The weak donor–acceptor effect was reflected also in the emitting colors: a blue-light emission with a λem of approximately 420–430 nm in dye 7, a blue-light emission of approximately 440–460 nm in dye 8, and a greenish-blue-light emission of approximately 480–500 nm in dye 9 were observed (Fig. 8). In a high water volume, the emission intensity decreased moderately (Fig. 7c). A similar behavior of unchanged emission and subsequent decrease in ΦF were also observed in dye 4 lacking triphenylamine donor moieties as described above. The difference between dyes 4 and 7–9 is the degree of decrease in ΦF. Compared to the large decrease in ΦF (ΦF = 0.08, 90% water fraction) in dye 4, a slight decrease in ΦF was observed in dyes 7–9. Thus, dyes 7–9 showed a moderate ΦF value even in a high water volume as follows: 0.25 in dye 7, 0.44 in dye 8, and 0.23 in dye 9 in 90% water fraction (Fig. 7c). These values are comparable to those of dyes 1a and 10–12 bearing strong acceptor moieties. However, a turn-on-type emission could not be achieved by the weak acceptor system because of the unchanged emission intensity in a low water volume. In the triphenylamine-based dyes, the strong donor–acceptor characteristic is very important for generating a turn-on-type emission in an aqueous environment.
As described above, the dyes have inherent emission behavior in the solid state (Table S1, ESI†). In the triphenylamine-based dyes, the ΦF values indicate a good relationship between the aggregated state (90% water fraction) and solid state (Fig. 9). For example, dyes 1a, 1d, 2, 3, 5, 8, and 11 with relatively large ΦF values in the solid state indicate relatively large ΦF values in 90% water fraction. It can be concluded that the inherent emission behavior in the solid state is preserved also in the aggregated state. In contrast, no relationship for ΦF value was observed in dye 4 lacking donor moieties. A small ΦF value of 0.08 was obtained in 90% water fraction; however, an excellent inherent emission behavior was observed in the solid state (ΦF = 0.92). On the other hand, dye 6 bearing dimethylamino groups showed a relatively good relationship for ΦF value, even though the inferior emission recovery in 90% water fraction indicated different aggregate morphologies.
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| Fig. 9 Plots of fluorescence quantum yields between the aggregated state (90% water fraction) and solid state in 1a–d, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, and 12. | ||
The morphology of aggregates was observed by atomic force microscopy (AFM). In triphenylamine-based dyes 1a–d, 2, 3, and 7–12, a spherical aggregate morphology of several hundred nm size was observed (Fig. 10). The size of spherical aggregates is in good agreement with the DLS measurement (Fig. S19 and S20, ESI†). The spherical morphology can be attributed to a less-ordered aggregation owing to the nonplanar triphenylamine moieties, preventing an ordered packing of the molecules and thus producing an increased number of conformations of the molecules.36 The less-ordered aggregation was transformed to an ordered aggregation by replacing the phenyl group in the donor moieties with a methyl group. In dye 6 bearing dimethylamino groups, a crystalline-like corn-tassel-type aggregate was observed, probably composed of small aggregates. Thus, the aggregates lacking diphenylamino groups (triphenylamine moieties) have a different morphology and insufficient hydrophobic space inside the aggregate structure, leading to a low emission recovery. Furthermore, the crystallinity increased significantly in dye 4 lacking triphenylamine donor moieties, indicating a different plate form of aggregate (Fig. 10). The aggregation probably proceeded in an ordered manner due to the lack of triphenylamine moieties. Thus, it can be concluded that the triphenylamine moiety plays an important role in emission recovery.
To investigate different aggregate morphologies, selected dyes (1a, 4, 6, and 12) were reprecipitated from concentrated THF/water solutions at 90% water fraction.37 In dye 4 lacking triphenylamine moieties, the X-ray diffraction (XRD) analysis showed a sharp reflection pattern, indicating the formation of crystalline aggregates (Fig. 11). The crystallinity was prevented by introducing a triphenylamine moiety in dyes 1a and 12, exhibiting a broad XRD pattern, indicating less-ordered aggregation (Fig. 11). Dye 6 bearing a dimethylamino group showed weak-intensity reflections, unlike the sharp XRD pattern observed in dye 4 and the broad XRD pattern observed in dyes 1a and 12. Therefore, the less-ordered aggregation arising from the nonplanar triphenylamine moieties is probably required for light emission in polar aqueous media.
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Fig. 11 X-ray diffraction patterns of 1a, 4, 6, and 12. The samples were prepared by reprecipitation from THF/water (1 : 9, v/v) at 2.0 × 10−3 M. | ||
The triphenylamine moiety plays an important role in the aggregation and emission behaviors. When the phenyl group in the donor moieties was replaced with a methyl group, the emission efficiency decreased. When a triphenylamine moiety was used as the donor moiety, the fluorescence-quenching problem arising from an ordered aggregation could be prevented. This is because the nonplanar structure of triphenylamine disrupts an ordered packing and produces a less-ordered spherical aggregate.
The emitted color can be controlled by tuning the acceptor moiety. With the increase in electron-accepting property, the emission band shifted to a longer wavelength, from the blue-light region to the red-light region. This red-light emission in aqueous media has great potential for biological applications, as the wavelength of the emission lies in the biological optical window. Moreover, this red-light emission can be generated by a two-photon excitation using a near-IR light source.29,30 The two-photon excitation is very useful for developing a biological system because of the increased penetration depth in tissues with less photodamage and pinpoint excitation by a focused light.38
We believe that this study provides a versatile strategy for achieving efficient light emission in an aqueous environment. The strategy is based on a simple combination of an electron-accepting moiety and an electron-donating amino moiety. Currently, new light-emitting systems are developed in our laboratory to improve the present strategy.
N-Methyldiphenylamine (13), bis(pinacolato)diboron, 1,4-diodobenzene (17), 4-diphenylaminophenylboronic acid (18), 1,4-dibromoanthracene (19), dithiooxamide (20), 4-(diphenylamino)benzaldehyde (21), and 4,7-dibromo-[1,2,5]thiadiazolo[3,4-c]pyridine (24) are commercially available and were used without purification. The benzothiadiazole dyes 1a–d,29 2,30 3,15 4,29 6,29 4,7-dibromo-2,1,3-benzothiadiazole (16),39 5,8-dibromoquinoxaline (22),40 and 4,7-dibromo-5-fluoro-2,1,3-benzothiadiazole (23)41 were prepared according to the same methods reported previously.
:
1, v/v) to give 15 in 34% yield (209 mg, 068 mmol) as a white solid: mp 83–85 °C; IR (KBr, cm−1) 3087, 3035, 2975, 2927, 2874, 2816, 1610, 1591, 1495, 1371, 1363 (νBO), 1349, 1323, 1315, 1268, 1195, 1144, 1132, 1095, 861, 822, 701, 656; 1H NMR (400 MHz, CDCl3) δ 1.33 (s, 12H, CH3), 3.34 (s, 3H, CH3), 6.88 (d, J = 8.6 Hz, 2H, ArH), 7.09 (t, J = 7.5 Hz, 1H, ArH), 7.15 (d, J = 7.5 Hz, 2H, ArH), 7.33 (t, J = 7.5 Hz, 2H, ArH), 7.67 (d, J = 8.6 Hz, 2H, ArH). 13C NMR (100 MHz, CDCl3) δ 24.84, 40.11, 83.36, 116.13, 123.49, 123.81, 129.42, 135.92, 148.31, 151.38; FAB-MS (positive, NBA) m/z 309 (M+). Anal. calcd for C19H24BNO2 (309.21): C, 73.80; H, 7.82; N, 3.50. Found: C, 73.68; H, 7.76; N, 3.55.
:
1, v/v) and to give 5 in 69% yield (103 mg, 0.21 mmol). An analytical sample was obtained by recrystallization from hexane/dichloromethane as red powder: mp 190–191 °C; IR (KBr, cm−1) 3057, 3035, 2924, 2820, 1604, 1592, 1517, 1495, 1480, 1348, 1253, 1195, 1137, 1112, 888, 816, 753, 697; 1H NMR (400 MHz, CDCl3) δ 3.40 (s, 6H, CH3), 7.06 (t, J = 7.5 Hz, 2H, ArH), 7.10 (d, J = 8.6 Hz, 4H, ArH), 7.18 (d, J = 7.5 Hz, 4H, ArH), 7.34 (t, J = 7.5 Hz, 4H, ArH), 7.71 (s, 2H, ArH), 7.88 (d, J = 8.6 Hz, 4H, ArH); 13C NMR (100 MHz, CDCl3) δ 40.22, 118.15, 122.71, 122.77, 127.09, 129.03, 129.38, 129.87, 132.13, 148.48, 148.97, 154.25; FAB-MS (positive, NBA) 498 m/z (M+). Anal. calcd for C36H26N4S (498.64): C, 77.08; H, 5.26; N, 11.24. Found: C, 77.03; H, 5.25; N, 11.21.
:
1, v/v) and by recrystallization from hexane/chloroform to give 7 in 60% yield (340 mg, 0.602 mmol) as pale yellow powder: mp 243–244 °C; IR (KBr, cm−1) 3060, 3030, 1589, 1488, 1327, 1276, 818, 749, 695; 1H NMR (400 MHz, CDCl3) δ 7.04 (t, J = 7.3 Hz, 4H, ArH), 7.14 (d, J = 7.3 Hz, 8H, ArH), 7.15 (d, J = 8.8 Hz, 4H, ArH), 7.27 (t, J = 7.3 Hz, 8H, ArH), 7.52 (d, J = 8.8 Hz, 4H, ArH), 7.63 (s, 4H, ArH); 13C NMR (100 MHz, CDCl3) δ 122.93, 123.89, 124.43, 126.91, 127.57, 129.28, 134.56, 139.00, 147.16, 147.65; FAB-MS (positive, NBA) m/z 564 (M+). Anal. calcd for C42H32N2 (564.72): C, 89.33; H, 5.71; N, 4.96. Found: C, 89.43; H, 5.70; N, 4.95.
:
1, v/v) and by GPC eluting with chloroform to give 8 in 44% yield (272 mg, 0.44 mmol). An analytical sample was obtained by recrystallization from hexane/chloroform as white powder: mp 252–254 °C; IR (KBr, cm−1) 3062, 3032, 1590, 1508, 1492, 1387, 1314, 1272, 751, 697; 1H NMR (400 MHz, CDCl3) δ 7.06 (t, J = 7.3 Hz, 4H, ArH), 7.20 (d, J = 7.3 Hz, 8H, ArH), 7.20 (d, J = 7.8 Hz, 4H, ArH), 7.31 (t, J = 7.3 Hz, 8H, ArH), 7.41 (d, J = 7.8 Hz, 4H, ArH), 7.46–7.48 (m, 2H, ArH), 7.48 (s, 2H, ArH), 8.06–8.10 (m, 2H, ArH); 13C NMR (100 MHz, CDCl3) δ 122.96, 123.26, 124.54, 125.72, 126.46, 129.31 (×2), 130.89, 132.04, 134.74, 139.24, 147.02, 147.78; FAB-MS (positive, NBA) m/z 614 (M+). Anal. calcd for C46H34N2 (614.78): C, 89.87; H, 5.57; N, 4.56. Found C, 89.84; H, 5.61; N, 4.53.
:
1, v/v) and by GPC eluting with chloroform to give 9 in 48% yield (151 mg, 0.24 mmol). An analytical sample was obtained by recrystallization from hexane/dichloromethane orange powder: mp 289–290 °C; IR (KBr, cm−1) 3066, 3034, 3018, 1590, 1492, 1443, 1277, 749, 692; 1H NMR (400 MHz, CDCl3) δ 7.08 (d, J = 8.8 Hz, 4H, ArH), 7.10 (t, J = 7.3 Hz 4H, ArH), 7.16 (d, J = 7.3 Hz, 8H, ArH), 7.31 (t, J = 7.3 Hz, 8H, ArH), 7.81 (d, J = 8.8 Hz, 4H, ArH), 13C NMR (100 MHz, CDCl3) δ 121.93, 123.98, 125.32, 127.13, 127.24, 129.49, 146.89, 149.96, 150.15, 168.36; FAB-MS (positive, NBA) m/z 628 (M+). Anal. calcd for C40H28N4S2·(628.81): C, 76.40; H, 4.49; N, 8.91. Found: C, 76.45; H, 4.49; N, 8.90.
:
2, v/v) and by GPC eluting with chloroform to give 10 in 61% yield (373 mg, 0.605 mmol). An analytical sample was obtained by recrystallization from hexane/dichloromethane as pale yellow powder: mp 242–244 °C; IR (KBr, cm−1) 3063, 3031, 1588, 1511, 1488, 1466, 1333, 1317, 1276, 753, 697; 1H NMR (400 MHz, CDCl3) δ 7.06 (t, J = 7.3 Hz, 4H, ArH), 7.16–7.24 (m, 12H, ArH), 7.29 (t, J = 7.3 Hz, 8H, ArH), 7.62 (d, J = 8.8 Hz, 4H, ArH), 7.87 (s, 2H, ArH), 8.90 (s, 2H, ArH); 13C NMR (100 MHz, CDCl3) δ 122.55, 123.13, 124.86, 129.30, 129.97, 131.41, 131.91, 139.38, 141.22, 143.92, 147.39, 147.61; FAB-MS (positive, NBA) m/z 616 (M+). Anal. calcd for C44H32N4 (616.75): C, 85.69; H, 5.23; N, 9.08. Found: C, 85.78; H, 5.22; N, 9.06.
:
1, v/v) and by GPC eluting with chloroform to give 11 in 80% yield (309 mg, 0.648 mmol). An analytical sample was obtained by recrystallization from hexane/dichloromethane as an orange solid: mp 253–257 °C; IR (KBr, cm−1) 3060, 3034, 3006, 1589, 1557, 1515, 1487, 1326, 1317, 1277, 1195, 1180, 1043, 885, 830, 754, 697, 527, 514; 1H NMR (400 MHz, CDCl3) δ 7.07 (t, J = 8.8 Hz, 4H, ArH), 7.09 (t, J = 8.8 Hz, 4H, ArH), 7.18–7.23 (m, 12H, ArH), 7.30 (t, J = 8.8, Hz, 4H, ArH), 7.32 (t, J = 8.8, Hz, 4H, ArH), 7.61 (d, J = 11.7 Hz, 1H, ArH), 7.72 (d, J = 8.8 Hz, 2H, ArH), 7.88 (d, J = 8.8 Hz, 2H, ArH); 13C NMR (100 MHz, CDCl3) δ 116.5 (d, J = 16.5 Hz), 118.7 (d, J = 32.1 Hz), 122.18, 122.46, 123.38, 123.56, 125.06, 125.10, 129.35, 129.41, 129.91 (×2), 131.30, 131.34, 132.9 (d, J = 10.7 Hz), 147.27, 147.40, 147.90, 148.59, 151.16, 155.27 (d, J = 10.7 Hz), 159.56 (d, J = 249.5 Hz); FAB-MS (positive, NBA) 640 m/z (M+). Anal. calcd for C42H29FN4S (640.77): C, 78.73; H, 4.56; N, 8.74. Found: C, 78.40; H, 4.51; N, 8.44.
:
1, v/v) and by GPC eluting with chloroform to give 12 in 65% yield (203 mg, 0.325 mmol). An analytical sample was obtained by recrystallization from hexane/dichloromethane as a red powder: mp 185–187 °C; IR (KBr, cm−1) 3060, 3033, 1589, 1487, 1454, 1334, 1316, 1275, 754, 697; 1H NMR (400 MHz, CDCl3) δ 7.08 (t, J = 7.3 Hz, 2H, ArH), 7.10 (t, J = 7.3 Hz, 2H, ArH), 7.17–7.25 (m, 12H, ArH), 7.27–7.34 (m, 8H, ArH), 7.90 (d, J = 8.8 Hz, 2H, ArH), 8.53 (d, J = 8.8 Hz, 2H, ArH), 8.76 (s, 1H, ArH); 13C NMR (100 MHz, CDCl3) δ 121.78, 122.83, 123.49, 123.85, 125.03, 125.41, 125.65, 128.00, 129.39, 129.43, 129.75, 130.07, 130.77, 142.17, 147.08, 147.35, 148.39, 149.75, 149.90, 151.09, 156.75; FAB-MS (positive, NBA) m/z 623 (M+). Anal. calcd for C41H29N5S (623.77): C, 78.95; H, 4.69; N, 11.23. Found: C, 78.81; H, 4.63; N, 11.21.Footnote |
| † Electronic supplementary information (ESI) available: The cyclic voltammograms, the fluorescence spectra in various solvents, the fluorescence images in various solvents, the plots of the Stokes shift against the solvent polarity parameter, the UV/vis and fluorescence spectra in THF/water, and the DLS charts in THF/water. See DOI: 10.1039/c5ra18231j |
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