Open Access Article
Yohei
Hattori
*a,
Ryota
Kitajima
a,
Atsumi
Baba
a,
Kohei
Yamamoto
a,
Ryota
Matsuoka
bcd,
Tetsuro
Kusamoto
bcde and
Kingo
Uchida
a
aMaterials Chemistry Course, Faculty of Advanced Science and Technology, Ryukoku University, Seta, Otsu, Shiga 520-2194, Japan. E-mail: hattori@rins.ryukoku.ac.jp
bDepartment of Life and Coordination-Complex Molecular Science, Institute for Molecular Science, 5-1, Higashiyama, Myodaiji, Okazaki, Aichi 444-8787, Japan
cSOKENDAI (The Graduate University for Advanced Studies), Shonan Village, Hayama, Kanagawa 240-0193, Japan
dGraduate School of Engineering Science, Osaka University, 1-3, Machikaneyama, Toyonaka, Osaka 560-8531, Japan
eJST-PRESTO, 4-1-8, Honcho, Kawaguchi, Saitama 332-0012, Japan
First published on 26th September 2023
Eight new stable luminescent radicals are reported. We previously reported that the photoluminescence quantum yields (PLQYs) of diphenylpyridylmethyl radicals is dramatically increased by the addition of mesityl (2,4,6-trimethylphenyl) groups. By changing the mesityl groups to other hydrocarbon-substituted phenyl groups, the issue of the fluoresence efficiency and photostability of these radicals could be clarified. Contrary to our expectations, changing 2,4,6-trimethyl to 2,4,6-triisopropyl did not produce a positive effect, other than some improvement in purification. Nevertheless, a PLQY of more than 60% was a significant value. The addition of methyl substituents at the meta-positions drastically quenched the fluorescence in dichloromethane, while maintaining bright fluorescence in chloroform. Removing one of the ortho-methyl groups somewhat decreased the fluorescence efficiency but greatly improved the photostability. By using a phenyl substituent instead of a methyl group, more stabilization under photoirradiation could be achieved.
Leaving aside the new types of luminescent radicals that are on the rise,4 polyhalogenated triarylmethyl radicals have established a high degree of stability and a variety of derivative types.5 The most basic stable luminescent triarylmethyl radicals are triphenylmethyl radicals such as tris(2,4,6-trichlorophenyl)methyl radical (TTM, Scheme 1)6 and perchlorotriphenylmethyl radical (PTM),7 and the second group that is similarly easy to obtain and handle is diphenylpyridylmethyl radicals such as (3,5-dichloro-4-pyridyl)bis(2,4,6-trichlorophenyl)methyl radical (PyBTM)8 and (3,5-difluoro-4-pyridyl)bis(2,4,6-trichlorophenyl)methyl radical (F2PyBTM).9 PyBTM and F2PyBTM are superior to TTM in terms of their stability under light irradition8,9 and unique in their ability to form metal complexes.10 However, diphenylpyridyl radicals had been less explored than triphenylmethyl radicals for making highly fluorescent derivatives in organic solvent11 until new reporting, in 2022, on an F2PyBTM NHC-Gold(I) complex12 with 36% photoluminescence quantum yield (PLQY) in dichloromethane and para-mesitylated F2PyBTM (Mes2F2PyBTM)13 with 69% chloroform.
In addition to the idea of substituting the para-positions to the radical centre of the PyBTM by two phenyl groups (PyPBTM),14ortho-methyl groups on the phenyl groups play an important role in enhancing fluorescence.13 One mesityl group works as an electron-donor in mesitylated PyBTM derivatives and composes a donor–acceptor system with a relatively easily reducible radical centre. The ortho-methyl groups obstruct π-conjugation between the mesityl and diphenylpyridylmethyl in the D0 ground state, and suppress the structural relaxation in the D1 excited state.
Here, we prepared several new Mes2F2PyBTM and Mes2PyBTM analogues with modified hydrocarbon substituents on the terminal phenyl groups. Detailed effects of these substituents on PLQY and photostability were elucidated.
Absorption and emission spectra in dichloromethane of 1, 2, and 4 were very similar to their corresponding mesityl radicals (Fig. 1).13 The lowest energy absorption changes little from PyBTM and F2PyBTM because the triisopropylphenyl groups are poorly conjugated with the radical moieties at the ground state. In order to estimate structures using DFT, we adopted the UB3LYP level of theory with 6-31G(d, p) basis sets, since they closely reproduced the experimental absorption and emission spectra from previous studies. The solvent effect of dichloromethane was considered by using a polarizable continuum model (PCM).15 In the DFT optimized structure of 1, 2, and 4, the triisopropylphenyl groups are nearly perpendicular to the bonded dichorophenyl group, similarly to Mes2F2PyBTM (Table 1, Table S1 (ESI†), Scheme 3, ϕ4 and ϕ5).
| 1 | 2 | 3 | 4 | |
|---|---|---|---|---|
| φ 1: Torsion angle of pyridyl ring. φ2 and φ3: torsion angles of dichlorophenyl rings. ϕ4 and ϕ5: dihedral angles between dichlorophenyl groups and 2,4,6-triisopropylphenyl groups. | ||||
| φ 1 | 48° [36°] | 48° [37°] | 32° [23°] | 32° [23°] |
| φ 2 | 49° [52°] | 49° [52°] | 52° [54°] | 52° [53°] |
| φ 3 | 49° [47°] | 49° [48°] | 52° [48°] | 52° [49°] |
| ϕ 4 | 90° [55°] | 88° [55°] | 89° [54°] | 89° [54°] |
| ϕ 5 | 88° [87°] | 89° [89°] | ||
On the other hand, the emission maxima of radicals were to some extent redshifted from PyBTM and F2PyBTM because one of the triisopropylphenyl groups is conjugated by a certain amount with the bonded dichorophenyl group. The TD-DFT optimized dihedral angles between the triisopropylphenyl ring and dichlorophenyl ring (ϕ4) were ca. 54–55°, whereas the dihedral angles between the mesityl ring and dichlorophenyl ring were ca. 49–54°. These changes can be explained by the electronic structures, similarly to the cases of mesityl groups. The lowest excitation of these radicals can generally be regarded as the β-spin electron transition from the β-HOMO to the β-LUMO by TD-DFT calculations, where the spin of an unpaired electron of the radical is defined as α-spin. Since the β-HOMOs of 1, 2, 3, and 4 are mainly distributed on one of the triisopropylphenyl groups (Fig. 2), these triisopropylphenyl groups become cationic at the lowest excited state (D1) by intramolecular electron transfer. The cationic triisopropylphenyl ring seeks conjugation between the bonded dichlorophenyl ring and stabilizes its energy by delocalizing the plus charge.
![]() | ||
| Fig. 2 TD-DFT calculated frontier orbitals of 1, 2, 3, and 4 at the D1 optimized structure calculated using UB3LYP/6-31G(d,p). | ||
The PLQYs (Φf) of 1, 2, and 4 were inferior to those of the corresponding mesityl radicals in both dichloromethane and chloroform (Table 2 and Table S2, ESI†), while 4 in particular was still highly emissive. The PLQYs of the radicals are simply determined by the competition of the rate of fluorescence (kf) and the rate of the non-radiative decay from the D1 to D0. These parameters can be calculated from measured PLQYs and fluorescence lifetimes. The kf values of TippPyBTM (1), Tipp2PyBTM (2), and Tipp2F2PyBTM (4) were lower than those of MesPyBTM, Mes2PyBTM, and Mes2F2PyBTM, respectively. This effect can be explained by the lower conjugation between the triisopropylphenyl and dichlorophenyl groups, which probably delayed the transition from D1 to D0. Actually, the TD-DFT calculated oscillator strengths of the D0-D1 transitions at the D1 optimized structures of 1, 2, and 4 were slightly smaller than those of the corresponding mesityl radicals. The knr values show that the isopropyl groups also do not contribute to decreasing the internal conversion caused by vibronic coupling, and they were rather counterproductive in 1 and 2.
| λ em (nm) | Φ f (%) | τ/ns | k f/107 s−1 | k nr/107 s−1 | |
|---|---|---|---|---|---|
| Photophysical parameters of MesPyBTM, Mes2PyBTM, and Mes2F2PyBTM are cited from ref. 13. All Φf values were obtained by absolute PLQY measurement. | |||||
| MesPyBTM | 645 | 30 | 26 | 1.2 | 2.7 |
| 1 | 637 | 22 | 22 | 1.0 | 3.5 |
| Mes2PyBTM | 628 | 47 | 38 | 1.2 | 1.4 |
| 2 | 618 | 39 | 37 | 1.1 | 1.6 |
| 3 | 632 | 46 | 32 | 1.4 | 1.7 |
| Mes2F2PyBTM | 623 | 66 | 44 | 1.5 | 0.8 |
| 4 | 617 | 62 | 47 | 1.3 | 0.8 |
Previously, it was reported that aryl substitution of PyBTM further improved the photostability of the radicals.14 However, the photostabilities of MesPyBTM, Mes2PyBTM, and Mes2F2PyBTM were very near to that of PyBTM. Perpendicular mesityl groups do not help to improve photostability. Similarly, 1, 2, 3 and 4 were not more photostable than PyBTM (Fig. S2a and Table S3, ESI†), although they are still much more photostable than TTM.8 Perpendicular triisopropylphenyl groups also do not help to improve photostability.
In order to clarify the role of m-positions on the phenyl groups, we next prepared F2PyBTM derivatives with 2,3,4,5,6-pentamethylphenyl groups. Ph*F2PyBTM (5) and Ph*2F2PyBTM (6) were synthesized using 2,3,4,5,6-pentamethylphenylboronic acid (Scheme 4). The steric effect of the ortho-methyl groups was not expected to change, but the inductive effect of m-methyl groups became a matter of interest.
Absorption spectra of these radicals were very similar to that of Mes2F2PyBTM (Fig. 3). The pentamethylphenyl group was not conjugated with the radical, similarly to the mesityl and triisopropylphenyl groups. The DFT optimized dihedral angles between the pentamethyl group and the dichlorophenyl group were nearly 90° (Table 3 and Scheme 5). Surprisingly, the fluorescence of 5 and 6 was quite weak (<2%) in dichloromethane. The TD-DFT calculation shows that their first excited state D1 is almost completely composed of the excitation of the β-spin electron, which is similar to other PyBTM derivatives. The main transition, the β-HOMO–LUMO transition, can be regarded as intramolecular electron transfer from β-HOMO on the added phenyl group to the β-LUMO on the radical moiety. The β-HOMOs were to some extent delocalized on the dichlorophenyl group in the mesityl and triisopropylphenyl radicals; however, the β-HOMOs of pentamethylphenyl radicals are almost localized on the pentamethyl phenyl groups (Fig. 4), and the dihedral angles between the pentaphenyl and dichlorophenyl groups are still nearly 90° at the D1 state (Table 3). This means that plus and minus charges at the D1 state of 5 and 6 are more separated. The luminescence of such radicals tends to be quenched in polar solvents.11,16
| 5 | 6 | 7 | 8 | |
|---|---|---|---|---|
| φ 1: Torsion angle of pyridyl ring. φ2 and φ3: torsion angles of dichlorophenyl rings. ϕ4 and ϕ5: dihedral angles between dichlorophenyl groups and (alkyl)phenyl groups. ϕ6 and ϕ7: dihedral angles between o-phenylene groups and phenyl groups. | ||||
| φ 1 | 32° [25°] | 32° [24°] | 32° [27°] | 32° [25°] |
| φ 2 | 52° [50°] | 52° [52°] | 52° [52°] | 52° [50°] |
| φ 3 | 53° [51°] | 52° [49°] | 52° [46°] | 52° [48°] |
| ϕ 4 | 88° [89°] | 88° [88°] | 48° [34°] | 48° [39°] |
| ϕ 5 | 88° [89°] | 51° [50°] | 50° [49°] | |
| ϕ 6 | 52° [39°] | |||
| ϕ 7 | 52° [51°] | |||
![]() | ||
| Fig. 4 TD-DFT calculated frontier orbitals of 5 and 6 at the D1 optimized structure calculated using UB3LYP/6-31G(d,p). | ||
The table of photophysical parameters of Ph*F2PyBTM (5) and Ph*2F2PyBTM (6) show that they have quite large non-radiative decay rates in dichloromethane in addition to small rates of fluorescence. Luminescence quenching in polar organic solvents have been reported in the donor–acceptor system using TTM as an acceptor. Even chloroform (relative permittivity εr = 4.8) can largely decrease the PLQY of the carbazole-TTM system.11ab In the cases of Ph*F2PyBTM (5) and Ph*2F2PyBTM (6), dichloromethane (εr = 9.1) quenches the fluorescence, while chloroform maintains high-efficiency fluorescence (30% and 47%, respectively, Table S2, ESI†). We propose that the minimum polarity of a solvent that can quench the fluorescence is a measure of the degree of polarization at the intramolecular charge transfer excited state in the D–A radical systems.
So far, we have considered PyPBTM derivatives with alkyl groups at double ortho-positions. What about the effect of an alkyl group at a single ortho-position, and what about the effect of an aryl group at a single ortho-position? Using 2,4,-dimethylphenylboronic acid and 2-biphenylboronic acid, we prepared Xyl2F2PyBTM (7) and Biph2F2PyBTM (8), respectively (Scheme 6).
Absorption spectra of 7 and 8 show that the lowest energy absorptions of these radicals are slightly redshifted (Fig. 3). This means that the xylyl and biphenyl groups can be conjugated to the radical moieties due to less steric groups at the ortho-positions. The DFT-optimized dihedral angles between the dichlorophenyl ring and xylyl or biphenyl were 48–51° at the ground state (Table 3 and Scheme 5). The emission peaks of these radicals were more greatly bathochromically shifted, since the conjugation between dichlorophenyl and xylyl or biphenyl was strengthened. The TD-DFT-optimized dihedral angles were 34° in 7 and 39° in 8 on one side Fig. 5.
![]() | ||
| Fig. 5 TD-DFT calculated frontier orbitals of 7 and 8 at the D1 optimized structure calculated using UB3LYP/6-31G(d,p). | ||
Xyl2F2PyBTM (7) showed bright fluorescence in solutions, and its PLQY was 40% in dichloromethane. The rate of fluorescence (kf) of 7 was similar to that of Mes2F2PyBTM (Tables 2 and 4). The difference in PLQYs between 7 and Mes2F2PyBTM derives from the difference in the rate of non-radiative decay (knr), which is seen in the shorter fluorescence lifetime (26 ns) of 7 compared to the fluorescence lifetime (44 ns) of Mes2F2PyBTM. It was shown that even a single ortho-methyl group has a considerable effect in suppressing the non-radiative decay, although it did not reach that of double ortho-methyl groups. The PLQY of 15% for 8 was a bit larger than that of PyPBTM, although it showed similar redshifted emission (Table 4). The fluorescence lifetime of 8 was slightly longer than those of F2PyBTM and PyPBTM, and the rate of fluorescence of 8 was faster than that of PyPBTM.
| λ em (nm) | Φ f (%) | τ/ns | k f/107 s−1 | k nr/107 s−1 | |
|---|---|---|---|---|---|
| a Cited from ref. 8. b Cited from ref. 9. c Cited from ref. 13. All Φf values were obtained by absolute PLQY measurement. | |||||
| PyBTMa | 585 | 2 | 6.4 | 0.3 | 14 |
| F2PyBTMb | 566 | 4 | 12.5 | 0.3 | 7.7 |
| PyPBTMc | 654 | 9.5 | 12 | 0.8 | 7.5 |
| 5 | 725 | 0.5 | 0.7 | 0.7 | 142 |
| 6 | 670 | 1.3 | 2.4 | 0.5 | 41 |
| 7 | 642 | 40 | 26 | 1.5 | 2.3 |
| 8 | 653 | 15 | 15 | 1.0 | 5.7 |
The photostabilities of Ph*F2PyBTM (5) and Ph*2F2PyBTM (6) in chloroform were clearly improved over that of PyBTM (Fig. S2b and Table S4, ESI†). We speculate that photostability almost entirely depends on the stability of the intramolecular charge transfer excited state. The two additional methyl groups of the pentamethylphenyl group compared to the mesityl group are thought to stabilize the positive charge on the terminal phenyl groups through electronic or steric effects.
Xyl2F2PyBTM (7) had larger photostability than F2PyBTM and Mes2F2PyBTM in dichloromethane (Fig. 6). The lack of one ortho-methyl group can be interpreted as having less protection by methyl groups, but the conjugation between the dichlorophenyl and xylyl groups had a larger stabilization effect. Photostabilization by conjugation between benzene rings is more pronounced in 8. Conjugation of the phenylene ring with both dichlorophenyl and terminal ortho-phenyl rings (Fig. 5) resulted in stabilization of about 100 times that of PyBTM under 370 nm UV irradiation (Table S3, ESI†). These effects are consistent with the previous reports of photostabilization of TTM using carbazole donors and phenyl rings.17
![]() | ||
| Fig. 6 Plots showing the emission decay of 7 and 8 in dichloromethane under continuous excitation with light at λex = 370 nm ± 10 nm. | ||
:
toluene (9
:
1 v/v) emulsion (3.5 mL) was added, and the mixture was heated at 70 °C. Degassed triethylamine (1.2 mL, 8.6 mmol) was finally added, and the reaction mixture was stirred at 70 °C overnight. The reaction mixture was cooled down to room temperature, added chloroform, and filtered on a pad of silica and sodium sulfate. The solvent was evaporated and purified by silica gel column chromatography (CHCl3
:
hexane = 1
:
1). The yellow oil (806 mg) was separated by GPC (CHCl3) to obtain pure 1H (240 mg, 0.348 mmol, 35%) and 2H (113 mg, 0.132 mmol, 13%).
:
1 mixture of two conformers).
1H NMR (400 MHz, CDCl3, ppm): δ 8.52 (s, 0.5H), 8.50 (s, 0.5H), 8.39 (s, 0.5H), 8.38 (s, 0.5H), 7.44 (d, J = 2.1 Hz, 0.5H), 7.40 (d, J = 2.2 Hz, 0.5H), 7.31 (d, J = 2.2 Hz, 0.5H), 7.26 (br, 0.5H), 7.22 (d, J = 1.5 Hz, 0.5H), 7.21 (d, J = 1.6 Hz, 0.5H), 7.10 (d, J = 1.5 Hz, 0.5H), 7.07 (d, J = 1.6 Hz, 0.5H), 7.05 (s, 2H), 6.83 (s, 0.5H), 6.83 (s, 0.5H), 2.93 (sep, J = 6.9 Hz, 1H), 2.66–2.54 (m, 2H), 1.29 (d, J = 6.9, Hz, 6H), 1.15–1.04 (m, 12H).
13C NMR (100 MHz, CDCl3, ppm): δ 149.7, 149.5, 149.1, 147.9, 147.8, 146.3, 146.2, 144.2, 144.1, 142.9, 142.8, 138.1, 138.0, 137.4, 137.4, 137.0, 137.0, 136.4, 134.6, 134.5, 134.2, 134.1, 133.9, 133.7, 133.7, 133.6, 133.3, 132.1, 131.9, 131.8, 131.6, 130.5, 130.1, 130.0, 129.9, 128.8, 128.5, 120.9, 120.8, 50.0, 34.5, 30.6, 30.5, 24.3, 24.3, 24.2, 24.0.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C33H31Cl7N+ 686.02707; found 686.02764.
13C NMR (100 MHz, CDCl3, ppm): δ 149.6, 149.1, 147.9, 146.5, 146.3, 146.3, 144.9, 142.6, 137.1, 137.0, 136.7, 136.3, 134.7, 134.1, 134.0, 133.9, 132.8, 132.2, 132.0, 131.7, 130.0, 130.0, 120.9, 50.3, 30.6, 30.6, 30.5, 30.4, 24.5, 24.3, 24.3, 24.3, 24.3, 24.1, 24.1.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C48H54Cl6N+ 854.23819; found 854.23855.
:
toluene (9
:
1 v/v) emulsion (3.5 mL) was added, and the mixture was heated at 80 °C. Degassed triethylamine (0.85 mL, 6.1 mmol) was finally added, and the reaction mixture was stirred at 80 °C overnight. The reaction mixture was cooled down to room temperature, added dichloromethane, and filtered on a Celite pad. The solvent was evaporated and purified by silica gel column chromatography (CHCl3
:
hexane = 1
:
1). The mixture was separated by GPC (CHCl3) to obtain crude 3H (291 mg, 44%) and pure 4H (128 mg, 0.195 mmol, 20%). Recrystallization of crude 3H from dichloromethane-methanol twice gave pure 3H (69.8 mg, 0.106 mmol, 11%).
13C NMR (100 MHz, CDCl3, ppm): δ 149.1, 146.3, 142.8, 137.2, 136.1, 135.4, 134.2, 133.8, 133.0, 131.4, 131.0, 129.6, 120.8, 42.0, 34.5, 30.5, 24.3, 24.2, 24.1.
HRMS(MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C33H31Cl5NF2+ 654.08617; found 654.08662.
13C NMR (100 MHz, CDCl3, ppm): δ 149.1, 146.4, 142.5, 136.1, 135.3, 135.1, 134.0, 133.8, 133.6, 132.1, 131.0, 125.5, 125.4, 125.2, 120.9, 42.4, 42.3, 34.5, 30.5, 24.4, 24.3, 24.2.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C48H54Cl4NF2+ 822.29729; found 822.29764.
:
toluene (9
:
1 v/v) emulsion (2.4 mL) was added, and the mixture was heated at 70 °C. Degassed triethylamine (0.56 mL, 4.0 mmol) was finally added, and the reaction mixture was stirred at 70 °C overnight. The reaction mixture was cooled down to room temperature, added chloroform, and filtered on a Celite pad. The solvent was evaporated and purified by silica gel column chromatography (CHCl3
:
hexane = 1
:
1). The mixture (538 mg) was separated by GPC (CHCl3) to obtain crude 5H (224 mg, 55%) and 6H (91 mg, 19%). Recrystallization from dichloromethane-methanol gave 5H (142 mg, 24%) and 6H (35 mg, 0.049 mmol, 7.3%).
13C NMR (100 MHz, CDCl3, ppm): δ 145.0, 137.2, 136.6, 136.5, 135.4, 135.1, 134.1, 133.6, 132.8, 131.3, 131.3, 130.8, 129.5, 124.8, 124.7, 124.6, 42.1, 42.0, 18.5, 17.0, 16.7.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C29H23Cl5NF2+ 598.02357; found 598.02323.
13C NMR (100 MHz, CDCl3, ppm): δ 144.7, 136.7, 136.5, 135.4, 135.3, 135.1, 133.7, 133.5, 132.8, 132.0, 131.4, 131.0, 130.7, 125.2, 42.3, 18.6, 17.0, 16.7.
HRMS(MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C40H38Cl4NF2+ 710.17209; found 710.17249.
:
toluene (9
:
1 v/v) emulsion (1.8 mL) was added, and the mixture was heated at 70 °C. Degassed triethylamine (0.45 mL, 3.2 mmol) was finally added, and the reaction mixture was stirred at 70 °C overnight. The reaction mixture was cooled down to room temperature, added chloroform, and filtered on a Celite pad. The solvent was evaporated and purified by silica gel column chromatography (CHCl3
:
hexane = 1
:
1). The mixture was separated by GPC (CHCl3) to obtain crude 7H and monoadduct. (58 mg, ca. 20%). Recrystallization from dichloromethane-methanol gave 7H (25.0 mg, 0.040 mmol, 8.0%).
1H NMR (400 MHz, CDCl3, ppm): δ 8.36 (s, 1H), 8.24 (s, 1H), 7.27 (s, 4H), 7.12 (d, 2H. J = 7.8 Hz), 7.09 (s, 2H), 7.06 (d, 2H. J = 7.8 Hz), 6.84 (s, 1H), 2.36 (s, 6H), 2.26 (s, 6H).
13C NMR (100 MHz, CDCl3, ppm): δ 143.4, 138.2, 136.2, 135.8, 135.1, 132.1, 131.5, 130.3, 129.5, 126.9, 42.2, 21.2, 20.4.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C34H26Cl4NF2+ 626.07819; found 626.07819.
:
toluene (9
:
1 v/v) emulsion (1.8 mL) was added, and the mixture was heated at 70 °C. Degassed triethylamine (0.42 mL, 3.0 mmol) was finally added, and the reaction mixture was stirred at 70 °C overnight. The reaction mixture was cooled down to room temperature, added chloroform, and filtered on a Celite pad. The solvent was evaporated and purified by silica gel column chromatography (CHCl3
:
hexane = 1
:
1). The mixture was separated by GPC (CHCl3) to obtain crude 8H (195 mg, ca. 54%). Recrystallization from dichloromethane-methanol three times gave pure 8H (177 mg, 0.245 mmol, 49%).
1H NMR (400 MHz, CDCl3, ppm): δ 8.30 (s, 1H), 8.19 (s, 1H), 7.46–7.43 (m, 8H), 7.25–7.23 (m, 6H), 7.12–7.10 (m, 4H), 7.04 (s, 4H), 6.63 (s, 1H).
13C NMR (100 MHz, CDCl3, ppm): δ 142.9, 140.9, 140.4, 137.4, 136.0, 135.2, 134.9, 133.6, 133.4, 131.8, 130.8, 130.7, 130.0, 128.7, 128.2, 127.8, 127.2, 125.0, 42.0.
HRMS (MALDI-TOF MS positive mode) m/z: [MH]+ calcd for C42H26Cl4NF2+ 722.07819; found 722.07761.
:
hexane = 1
:
1) and dried in vacuo to afford 1 (96.6 mg, 0.140 mmol, 89%) as a red solid.
Elemental analysis calcd for C33H29Cl7N: C 57.63, H 4.25, N 2.04, found: C 57.98, H 4.18, N 2.11.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C33H29Cl7N− 684.01142; found 684.01141.
:
hexane = 1
:
1) and dried in vacuo to afford 2 (53.7 mg, 0.0628 mmol, 90%) as a red solid.
Elemental analysis calcd for C48H52Cl6N: C 67.38, H 6.13, N 1.64, found: C 67.61, H 6.12, N 1.51.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C48H52Cl6N− 852.22364; found 852.22402.
:
hexane = 1
:
1) and dried in vacuo to afford 3 (44 mg, 0.067 mmol, quant.) as a red solid.
Elemental analysis calcd for C33H29Cl5F2N: C 60.53, H 4.46, N 2.14, found: C 60.64, H 4.36, N 2.00.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C33H29Cl5NF2− 652.07162; found 652.07115.
:
hexane = 1
:
2) and dried in vacuo to afford 4 (46.0 mg, 0.0559 mmol, 93%) as a red solid.
Elemental analysis calcd for C48H52Cl4F2N: C 70.07, H 6.37, N 1.70, found: C 70.30, H 6.55, N 1.64.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C48H52Cl4NF2− 820.28274; found 820.28223.
:
hexane = 1
:
1) and dried in vacuo to afford 5 (38.8 mg, 0.0648 mmol, 84%) as a red solid.
Elemental analysis calcd for C29H21Cl5F2N: C 58.18, H 3.54, N 2.34, found: C 58.03, H 3.25, N 2.30.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C29H21Cl5NF2− 596.00902; found 596.00916.
:
hexane = 1
:
1) and dried in vacuo to afford 4 (20.5 mg, 0.0289 mmol, 84%) as a red solid.
Elemental analysis calcd for C40H36Cl4F2N: C 67.62, H 5.11, N 1.97, found: C 67.25, H 5.25, N 2.00.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C40H36Cl4NF2− 708.15754; found 708.15708.
:
hexane = 1
:
1) and dried in vacuo to afford 5 (20 mg, 0.032 mmol, 96%) as a red solid.
Elemental analysis calcd for C34H24Cl4F2N + 0.2CHCl3: C 63.17, H 3.75, N 2.15, found: C 63.03, H 3.86, N 2.13.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C34H24Cl4NF2− 624.06364; found 624.06312.
:
hexane = 1
:
1) and dried in vacuo to afford 6 (69.6 mg, 0.0963 mmol, 96%) as a red solid.
Elemental analysis calcd for C42H24Cl4F2N: C 69.83, H 3.35, N 1.94, found: C 69.71, H 3.30, N 1.81.
HRMS (MALDI-TOF MS negative mode) m/z: [M]− calcd for C42H24Cl4NF2− 720.06364; found 720.06349.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ma00469d |
| This journal is © The Royal Society of Chemistry 2023 |