Open Access Article
Peifeng Mei,
Akinobu Matsumoto,
Hironobu Hayashi
,
Mitsuharu Suzuki
,
Naoki Aratani
* and
Hiroko Yamada
*
Graduate School of Science and Technology, Nara Institute of Science and Technology (NAIST), Takayama-cho, Ikoma, Nara 630-0192, Japan. E-mail: aratani@ms.naist.jp; hyamada@ms.naist.jp
First published on 7th June 2018
A large 1,3-phenylene-bridged hexameric naphthalene wheel N6 and a heptameric wheel N7 were synthesized simply by Suzuki–Miyaura coupling via one-pot reaction from monomers. We could control the distribution of N6 and N7 via the reaction conditions. The hexameric wheel structure was revealed by X-ray diffraction analysis. The wheel N6 exhibited C60 encapsulation ability in the solid state, which was also confirmed by single crystal X-ray analysis.
High-resolution matrix assisted laser desorption/ionization time-of-flight (HR-MALDI-TOF) mass spectrum of N6 displays the parent ion peaks at m/z 1212.4686 (calcd for C96H60 = 1212.4690 [M]+). Although the 1H NMR spectrum of N6 in CDCl3 at room temperature was very broad, that in C2D2Cl4 at 60 °C became sharper and simple, exhibiting only a single set of signals that consists of two singlet peaks at 7.67 and 7.56 ppm due to the Hc and Hd, respectively, and signals due to Ha and Hb in the range of 7.66 ppm and He and Hf at 8.10 and 7.47 ppm, respectively. These data indicate that the wheel N6 takes a C6 symmetric structure in solution at 60 °C.
Definitive structural assignment of N6 was accomplished through a single crystal X-ray diffraction analysis, which unveiled a distinct hexagonal conformation (Fig. 1a).‡ The phenylene-bridges are on the co-plane, suggesting less structural strain. The dihedral angles between the naphthalene mean-planes and phenylene groups are in the range of 58–64°. Interestingly, the hexagons are interconnected through phenylene C–H and naphthalene π-plane interactions in the crystal, forming an infinite one-dimensional tubular packing structure along the c-axis (Fig. 1b).
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| Fig. 1 (a) Single crystal X-ray structure of N6 and (b) packing structure of N6. Thermal ellipsoids are scaled at 50% probability. Solvent molecules are omitted for clarity. | ||
Fig. 2 shows the UV-vis absorption and fluorescence spectra of N6 in CH2Cl2. Cyclic hexamer N6 shows a single absorption band at 306 nm and a blue emission at 383 nm. This broad single band can be qualitatively understood in terms of the weak π-conjugation and the exciton coupling,9 as similarly to previously reported 1,3-phenylene naphthalene dimer.10 Given the rigid hexagonal conformation for the wheel, J-type exciton coupling of transition dipoles is effective. The interacting components lead to red-shifted absorption band compared with naphthalene monomer (275 nm in CH2Cl2). The steady-state fluorescence spectrum in toluene is also displayed in Fig. 2.
To further understand the electronic features of N6, the density functional theory (DFT) and the time-dependent (TD)-DFT calculations both at the B3LYP/6-31G(d) level using the Gaussian 09 software package were carried out (Fig. 3).11 It is revealed that the frontier orbitals are degenerated. The coefficients of HOMO and LUMO of N6 localize on the six naphthalene units. The main absorption band of N6 at 306 nm predominantly comprises the S2 and S3 transitions (oscillator strength, f = 1.03 and f = 1.02), whereas the long wavelength S1 absorption is forbidden (f = 0.00). The transition energies and oscillator strengths simulated by TD-DFT calculations showed a good agreement with the observed absorption spectrum of N6.
In the next step, the encapsulation of C60 into N6 was examined, since the diameter of the interior cavity of N6 is ca. 15 Å, being possibly fit to the diameter of C60.12 Unfortunately, however, the addition of C60 into a toluene solution of N6 did not change the absorption spectrum probably because of weak interactions between two components. The encapsulation was also not confirmed by NMR spectroscopy. Thus we attempted to make co-crystals of N6 with C60. The host–guest binding structure was unambiguously confirmed by the single-crystal X-ray diffraction analysis (Fig. 4).‡ Higher concentration on the crystallization process could give the encapsulation complex. In the solid-state, the naphthalene units of C60@N6 take a similar structure to those of N6 with respects to dihedral angles of phenylene toward naphthalene (51–72°), and an inside space (15 Å diameter). The positions of C60 are disordered at two parts (66:34). As shown in Fig. 4, a C60 molecule is nicely captured within the cavity. Closer inspection of the crystal structure reveals that the naphthalene planes are protruding their planar face toward the interior space, which interacts with C60. Interestingly, the C60 molecules in the crystal are aligned with the aid of N6 agent to form a 1D structure along the a-axis (Fig. 4b).
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| Fig. 4 (a) Single crystal X-ray structure of C60@N6 and (b) packing structure of C60@N6. Thermal ellipsoids are scaled at 50% probability. Solvent molecules are omitted for clarity. | ||
During this research, Yokozawa and co-workers reported an efficient cyclization reaction of o- and m-alternate polyphenylenes.13 In order to check the effect of the reaction conditions, we applied Yokozawa's conditions on our cyclic naphthalene synthesis. Interestingly, the distribution of the wheel size was shifted to the larger size, and we successfully isolated N6 and N7 in 4% and 13% yields, respectively (Scheme 1). HR-MALDI-TOF mass spectrum of N7 displayed the parent ion peaks at m/z 1414.5469 (calcd for C112H70 = 1414.5472 [M]+). To observe a relatively clear 1H NMR spectrum in C2D2Cl4, it was needed to measure the spectrum at higher temperature than that for N6. The 1H NMR spectrum of N7 in C2D2Cl4 at 120 °C was simple, exhibiting only a single set of signals that consists of two singlet peaks at 7.66 and 7.59 ppm due to the Hd and Hc, respectively, at 7.75 ppm due to Ha and signals due to Hb in the range of 7.61–7.66 ppm and He and Hf at 8.13 and 7.40 ppm, respectively.
UV-vis absorption and fluorescence spectra of N7 in CH2Cl2 are also shown in Fig. 2. Cyclic heptamer N7 exhibits a slightly red-shifted absorption band at 308 nm and a blue-shifted emission at 382 nm. These are presumably because the conformational deformation from N6 to N7 makes the forbidden S1 transition to be just a little allowed.
UV/Vis absorption spectra were measured with a JASCO UV/Vis/NIR spectrophotometer V-570.
TLC and gravity column chromatography were performed on Art. 5554 (Merck KGaA) plates and silica gel 60N (Kanto Chemical), respectively. All other solvents and chemicals were reagent-grade quality, obtained commercially, and used without further purification. For spectral measurements, spectral-grade solvents were purchased from Nacalai Tesque.
All DFT calculations were performed with a Gaussian 09 program package. The geometries were fully optimized at the Becke's three-parameter hybrid functional combined with the Lee–Yang–Parr correlation functional abbreviated as the B3LYP level of density functional theory. The 6-31G(d) bases set implemented was used for structure optimizations and frequency analyses.
:
CH2Cl2 = 3
:
1). After being purified by a preparative GPC, 4.0 mg of N6 was gained in 6% yield as a white solid. 1H NMR (C2D2Cl4, 600 MHz, ppm, 60 °C) δ 7.47 (q, J = 9.6 Hz, 12H), 7.56 (s, 12H), 7.66–7.67 (m, 24H) and 8.10 (q, J = 9.6 Hz, 12H). 13C NMR (C2D2Cl4, 151 MHz, ppm, 60 °C) δ 126.14, 126.60, 126.71, 128.31, 129.09, 132.05, 132.22, 139.83 and 141.01. UV-vis (CH2Cl2): λmax (ε [M−1 cm−1]) = 306(8.7 × 104) nm. Fluorescence (CH2Cl2, λex = 306 nm): λmax = 383 nm.
:
CH2Cl2 = 3
:
1). After being purified by GPC, 7.0 mg of N7 was gained in 13% yield and 2.0 mg of N6 in 4% yield. 1H NMR (C2D2Cl4, 400 MHz, ppm, 120 °C) δ 7.49 (m, 14H), 7.59 (s, 7H), 7.61 (d, 7H), 7.66 (d, 21H), 7.75 (d, 7H) and 8.13 (m, 14H). 13C NMR (C2D2Cl4, 151 MHz, ppm, 120 °C) δ 120.46, 125.92, 125.93, 126.50, 126.66, 128.24, 129.28, 131.60, 132.30, 139.85 and 141.08. UV-vis (CH2Cl2): λmax (ε [M−1 cm−1]) = 308(1.1 × 105) nm. Fluorescence (CH2Cl2, λex = 308 nm): λmax = 382 nm.The structure was solved by using direct methods (SHELXT program).14 Structure refinements were carried out by using SHELXL-2014/7 program.15
Footnotes |
| † Electronic supplementary information (ESI) available: X-ray crystal analysis and NMR and mass spectra. CCDC 1838834 (N6) and 1838835 (C60@N6). For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c8ra03601b |
‡ Crystallographic data for N6: C96H60·O, Mw = 1229.44, monoclinic, space group P21/c (#14), a = 11.962(6), b = 32.625(16), c = 15.124(8) Å, β = 93.619(8)°, V = 5890(5) Å3, T = 90(2) K, Z = 2, reflections measured 29 202, 9464 unique. The final R1 was 0.1193 (>2σ(I)), and the final wR on F2 was 0.3390 (all data), GOF = 1.109. Crystallographic data for C60@N6: C96H60·C60·4(C6H5Cl), Mw = 2384.24, triclinic, space group P (#2), a = 11.110(5), b = 14.775(6), c = 17.361(7) Å, α = 94.214(7)°, β = 94.286(7)°, γ = 101.721(7)°, V = 2771(2) Å3, T = 90(2) K, Z = 1, reflections measured 15 703, 10 790 unique. The final R1 was 0.0691 (>2σ(I)), and the final wR on F2 was 0.2025 (all data), GOF = 1.036. The contributions to the scattering arising from the presence of disordered solvents in the crystals of N6 were removed by use of the utility SQUEEZE in the PLATON software package.16 |
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