

基于二甲基苯并联咪唑的钌(Ⅱ)多吡啶配合物的合成、光谱和电化学性质
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关键词:
- 钌多吡啶配合物
- / 苯并联咪唑
- / 电化学
- / 质子耦合电子传递(PCET)
- / 晶体结构
English
Synthesis, Spectroscopic and Electrochemical Properties of Ruthenium(Ⅱ) Polypyridyl Complexes with Dimethyl-bibenzimidazolate Ligands
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Ruthenium(Ⅱ) polypyridyl complexes have been deeply researched because of their excellent redox and photophysical properties, particularly, high stability and absorption and emission spectra in visible range, promising applications as solar energy conversion, molecular electronics, and so on[1-4]. Among them, ruthenium polypyridyl complexes based on biimidazole (H2biim) [5-10] or bibenzimidazole (H2bbim) [9-13] or their derivatives moieties[14-19] have received much attention. The presence of the acidic imidazole proton allows deprotonation of the complexes and this results in a rich chemistry where changes in pH can be used to affect the electrochemical and photophysical properties of the complexes[20]. The ability of complexes contain-ing the biimidazole or bibenzimidazole ligands to engage in hydrogen bonding via the externally-directed pair of N - H groups has been exploited extensively in crystal engineering and supramolecular chemistry.
As is well known, hydrogen bonding is one of the most popular tools in supramolecular chemistry because hydrogen bonds have relatively high strength and predictable directional nature compared to other non-covalent interactions[21-23]. There is a growing awareness of the important role that hydrogen-bonded complexes can play in complex electron-transfer mech-anisms[24]. The proton-coupled electron transfer (PCET) reactions can occur within hydrogen-bonded intermedi-ates. With incorporation of reversible redox couples and proper designs, electron transfer can provide a con-venient means both to detect the hydrogen-bonded complexes and control their assembly.
In this paper, we reported a family of ruthenium complexes, namely [(bpy)2Ru(DMBbimHx)]y+ (DMB-bimH2=7, 7'-dimethyl-2, 2'-bibenzimidazole, 1-A: x=2, y=2; 1-B:x=1, y=1; 1-C:x=0, y=0). The un-deprotonated 1-A, mono-deprotonated 1-B and bi-deprotonated 1-C were synthesized, and their spectroscopic and electro-chemical properties were studied. Interestingly, differ-ent electrochemical behaviors of the mono -deprotonated 1-B were observed in dichloromethane and the more polar acetonitrile. In dichloromethane, it undergoes a two-step oxidation, which indicates the existence of PCET between the [Ru(bpy)2(DMBbimH)]+ cations.
The single crystals of [Ru(bpy)2(DMBbimH)]PF6· 2CH2Cl2 (2), hydrogen-bonded dimer of [Ru(bpy)2 (DMBbimH)] +, were obtained from the solution of 1-B in dichloromethane. The [Ru(bpy)2 (DMBbimH)]+ cations exist as hydrogen-bonded dimers in dichloromethane, which is consistent with the result of electrochemical measurements of complex 1-B.
1. Experimental
1.1 Materials and methods
The reagents and solvents employed were commer-cially available and were used as received. 1H NMR spectra were recorded on a Varian Mercury-Plus 300 NMR spectrometer with chemical shifts relative to tet-ramethylsilane (TMS). The C, H and N microanalyses were carried out with a Vario EL elemental analyzer. Electron spray ionization (ESI) mass spectra were obtained on an LCQ DECA XP quadrupole ion trap mass spectrometer with methanol as the carrier solvent. UV-Vis spectra were performed on a Shimadzu UV - 315 UV-Vis spectrophotometer at room temperature, and the solvents used for spectral experiments were dis-tilled from CaH2 and kept over molecular sieves (type 4A).
The cyclic voltammetry (CV) and square wave voltammetry (SWV) measurements were made with a CHI-660 Electrochemical Workstation. The experi-ments were performed with a standard three-electrode arrangement: working electrode, glassy carbon elec-trode; quasi reference electrode, Ag-AgCl electrode; counter electrode, Pt wire electrode. Background correction was accomplished by subtracting the current curves of the blank electrolyte (containing the same concentration of supporting electrolyte) from the experi-mental curve. The experiments were performed with 0.001 mol·L-1 solutions of the complexes in dried acetonitrile or dried dichloromethane with 0.1 mol·L-1 ammonium hexafluorophosphate as supporting electro-lyte.
1.2 Syntheses
DMBbimH2[25] and cis-Ru(bpy)2Cl2·2H2O[26] were synthesized as reported in the literature procedures.
1.2.1 Synthesis of [Ru(bpy)2(DMBbimH2)](PF6)2 (1-A)[5]
[Ru(bpy)2Cl2]·2H2O (1 mmol), DMBbimH 2 (1.4 mmol) and ethylene glycol (14 mL) were added into a 50 mL three neck flask. The mixture was stirred and refluxed for 3 h under nitrogen protection, then cooled to room temperature and filtered. 100 mL water was added to the filtrate, followed by the addition of 2 mL hydrochloric acid and 0.8 g KPF6. The mixture was stirred for a while then filtered, and the precipitate was rinsed with water several times then dried at 70 ℃. Yield: 85% on the basis of [Ru(bpy)2Cl2]·2H2O. Anal. Calcd. for C36H 30F12N8P2Ru(%): C, 44.78; H, 3.13; N, 11.60. Found(%): C, 45.04; H, 3.32; N, 11.78. ESI-MS (positive, CH3OH): m/z 675.3 ([Ru(bpy)2(DMBbimH)]+); 338.3 ([Ru(bpy)2(DMBbimH2)]2+). 1H NMR (300 MHz, DMSO - d6): δ 13.84 (s, 2H, N - H), 8.83 (d, J=8.2 Hz, 2H, bpy-H), 8.73 (d, J=8.1 Hz, 2H, bpy-H), 8.21 (td, J= 7.8, 1.5 Hz, 2H, bpy - H), 8.04 (td, J=7.9, 1.5 Hz, 2H, bpy-H), 7.98 (dd, J=5.7, 1.3 Hz, 2H, bpy-H), 7.88 (d, J =5.5 Hz, 2H, bpy - H), 7.57 (ddd, J=7.2, 5.6, 1.3 Hz, 2H, bpy-H), 7.46 (ddd, J=7.0, 5.6, 1.3 Hz, 2H, bpy-H), 7.19 (dd, J=7.7, 4.4 Hz, 2H, DMBbimH2-H6), 6.97 (t, J =7.7 Hz, 2H, DMBbimH2 -H5), 5.45 (d, J=8.3 Hz, 2H, DMBbimH2-H4), 2.60 (s, 6H, Me-H).
1.2.2 Synthesis of [Ru(bpy) 2(DMBbimH)]PF 6 (1-B)
The complex 1-A was dissolved in the minimum volume of dichloromethane and subjected to column chromatography on neutral alumina (1 cm×10 cm). A red-violet band was eluted with dichloromethane-acetonitrile (3:1, V/V). The solvent was evaporated to dryness under vacuum, then the complex 1-B was obtained with a yield of 75%. Anal. Calcd. for C36H29F6N8PRu(%): C, 52.75; H, 3.57; N, 13.67. Found (%): C, 52.53; H, 3.63; N, 13.42. ESI-MS (positive, CH3OH): m/z 675.3 ([Ru(bpy)2(DMBbimH)]+); 338.3 ([Ru(bpy)2(DMBbimH2)]2+). 1H NMR (300 MHz, DMSO-d6): δ 8.77 (d, J=8.2 Hz, 2H, bpy-H), 8.68 (d, J=8.1 Hz, 2H, bpy-H), 8.14 (td, J=7.9, 1.4 Hz, 2H, bpy-H), 8.06~ 7.88 (m, 4H, bpy - H), 7.76 (d, J=5.6 Hz, 2H, bpy - H), 7.52 (ddd, J=7.2, 5.6, 1.2 Hz, 2H, bpy-H), 7.44 (ddd, J =7.1, 5.5, 1.3 Hz, 2H, bpy-H), 6.85 (d, J=7.2 Hz, 2H, DMBbimH-H6), 6.66 (t, J=7.7 Hz, 2H, DMBbimH-H5), 5.31 (d, J=8.1 Hz, 2H, DMBbimH - H4), 2.55 (s, 6H, Me-H).
1.2.3 Synthesis of Ru(bpy)2(DMBbim) (1-C)
The complex 1-A was dissolved in a small amount of methanol, and an excessive amount of ammonia gas was introduced[27], and the precipitate was filtered to obtain the complex 1 - C. Yield: 50%. Anal. Calcd. for C36H28N8Ru(%): C, 64.18; H, 4.19; N, 16.63. Found (%): C, 62.37; H, 4.02; N, 16.36. ESI - MS (positive, CH3OH): m/z 675.3 ([Ru(bpy)2(DMBbimH)] +); 338.3 ([Ru(bpy)2(DMBbimH2)]2+). 1H NMR (300 MHz, DMSO-d6): δ 8.69 (d, J=8.2 Hz, 2H, bpy-H), 8.60 (d, J=8.1 Hz, 2H, bpy-H), 8.04 (t, J=7.8 Hz, 2H, bpy-H), 7.89 (d, J= 5.5 Hz, 2H, bpy-H), 7.83 (t, J=7.8 Hz, 2H, bpy-H), 7.73 (d, J=5.5 Hz, 2H, bpy-H), 7.45 (t, J=6.6 Hz, 2H, bpy-H), 7.36 (t, J=6.6 Hz, 2H, bpy-H), 6.52 (d, J=7.0 Hz, 2H, DMBbim-H6), 6.32 (t, J=7.5 Hz, 2H, DMBbim - H5), 5.16 (d, J=7.9 Hz, 2H, DMBbim-H4), 2.49 (s, 6H, Me-H).
1.2.4 Synthesis of [Ru(bpy)2(DMBbimH)]PF6·2CH2Cl2 (2)
Single crystals of 2 were grown at room tempera-ture by slow evaporation of the solution of 1-B in dichloromethane. Dark red single crystals were obtained about one week later. Anal. Calcd. for C38H33Cl4F6N8PRu(%): C, 46.12; H, 3.36; N, 11.32. Found(%): C, 46.05; H, 3.43; N, 11.27.
1.3 Structure determination
The intensity data for compound 2 were collected on a Bruker Smart Apex CCD area detector, using graphite-monochromated Mo Kα radiation (λ=0.071 073 nm). The structure was solved by direct method and refined by full matrix least squares techniques against F2 (SHELXTL-2016 program package[28-29]). The hydro-gen atoms of the"amine group"were located by Fourier difference synthesis and refined isotropically. All other hydrogen atoms were included at calculated positions with fixed thermal parameters. All non -hydrogen atoms were refined anisotropically. The solvents were squeezed by SQUEEZE/PLATON program. Crystal data, data collection parameters and refinement statis-tics are listed in Table 1. Selected bond lengths and angles are presented in Table 2.
CCDC: 2005043, 2.
Table 1
Empirical formula C38H33Cl4F6N8PRu Formula weight 989.56 Crystal system Monoclinic Space group C2/c a / nm 3.182 7(2) b / nm 1.638 4(1) c / nm 1.885 3(1) β/(°) 111.255(2) V / nm3 9.162(1) Z 8 Dc / (g·cm-3) 1.435 Absorption coefficient / mm-1 0.671 F(000) 3 984 Crystal size / mm 0.230×0.200×0.160 θ range for data collection / (°) 3.094~25.999 Limiting indices -39 ≤ h ≤39, -20 ≤ k ≤20, -21 ≤ l ≤ 23 Reflection collected, unique 36 729, 8 972 (Rint=0.108 5) Reflection observed 6 835 Completeness to θ=25.242 / % 99.7 Data, restraint, parameter 8 972, 0, 469 Goodness-of-fit on F2 1.032 Final R indices [I > 2σ(I)] R1a=0.067 8, wR2b=0.175 6 R indices (all data) R1a=0.086 6, wR2b=0.189 1 a R1=Σ||Fo|-|Fc||/Σ|Fo|; bwR2=[Σw(Fo2-Fc2)2/Σw(Fo2)2]1/2. Table 2
Ru1-N1 0.204 3(4) Ru1-N2 0.204 7(4) Ru1-N3 0.205 4(4) Ru1-N4 0.205 2(4) Ru1-N5 0.208 9(4) Ru1-N7 0.210 8(4) C21-N5 0.138 9(6) C28-N5 0.133 6(6) C26-N6 0.138 8(6) C28-N6 0.135 4(6) C29-N7 0.134 7(6) C30-N7 0.138 9(6) C29-N8 0.134 8(6) C35-N8 0.139 9(6) C28-C29 0.144 4(6) N2-Ru1-N1 78.6(2) N4-Ru1-N3 78.8(2) N5-Ru1-N7 78.3(1) N2-Ru1-N3 89.0(2) N4-Ru1-N5 85.1(1) N1-Ru1-N7 85.8(1) N3-Ru1-N5 95.6(1) N2-Ru1-N7 97.6(2) N1-Ru1-N5 95.4(1) N4-Ru1-N7 94.9(2) N3-Ru1-N1 100.5(2) N2-Ru1-N4 100.9(2) N4-Ru1-N1 179.2(1) N2-Ru1-N5 173.0(1) N3-Ru1-N7 171.7(1) C31-C30-C35 120.3(4) C22-C21-C26 121.0(4) C24-C25-C26 115.4(4) N7-C30-C35 108.3(4) C23-C22-C21 116.5(4) C24-C25-C27 124.0(5) C30-C31-C32 117.1(4) C22-C23-C24 122.0(5) C26-C25-C27 120.6(4) N5-C21-C22 131.3(4) C25-C24-C23 122.9(5) N6-C26-C25 129.5(4) N5-C21-C26 107.7(4) C1-N1-C5 117.5(4) N6-C26-C21 108.2(4) C25-C26-C21 122.2(4) C10-N2-C6 118.0(4) N7-C29-C28 116.1(4) N5-C28-N6 115.3(4) C11-N3-C15 118.9(4) N8-C29-C28 129.1(4) N5-C28-C29 117.3(4) C20-N4-C16 118.5(4) C31-C30-N7 131.4(4) N6-C28-C29 127.4(4) N7-C29-N8 114.9(4) C31-C32-C33 122.2(5) C28-N5-C21 104.7(4) C29-N8-C35 104.8(4) C34-C33-C32 122.3(5) C28-N6-C26 104.0(4) C33-C34-C35 115.7(4) C33-C34-C36 122.3(4) C29-N7-C30 104.7(4) C35-C34-C36 122.0(4) C34-C35-N8 130.2(4) C34-C35-C30 122.4(4) N8-C35-C30 107.4(4) 2. Results and discussion
2.1 Synthesis
Reaction between cis-Ru(bpy)2Cl2·2H2O and DMBbimH2 in refluxing ethylene glycol resulted in the formation of Ru(bpy)2 (DMBbimH 2)] (PF 6)2, 1-A, which can be converted into mono-deprotonated 1-B and bi-deprotonated 1 - C under suitable condition. The reac-tions in Fig. 1 are reversible and each of the three species involved can be converted into any one of the other two simply by the adjustment of pH. We have been able to isolate all of the three species in their pure states.
Figure 1
The mass spectra of these complexes were nearly identical, where peaks at 675.3 and 338.3 can be assigned to [Ru(bpy)2(DMBbimH)]+ and [Ru(bpy)2 (DMBbimH2)]2+. This helps us to confirm the structures of the complexes to some extent. However, the 1H NMR (section 2.2), UV-Vis spectra (section 2.3), and electro-chemical properties (section 2.4) of the complexes 1-A, 1-B, and 1-C showed obvious differences. Single crys-tals were grown from the dichloromethane solution of 1-B. The molecular structure of compound [Ru(bpy)2 (DMBbimH)]PF6·2CH2Cl2 (2) has been confirmed by X-ray crystallography (section 2.5).
2.2 1H NMR
NMR spectroscopy has proved to be a useful tool in the structural characterization of ruthenium polypyri-dyl complexes[30]. We confirm the structures of complex-es 1 - A, 1 - B and 1 - C through their 1H NMR spectra (Fig. 2) which were recorded in DMSO-d6 at room temperature.
Figure 2
In the spectrum of 1-A, the four doublets and four triplets between δ 8.83 and δ 7.46 belong to the aromatic protons of bpy groups. The relative intensities of these resonances were, as expected, 1:1:1:1:1:1:1:1. The doublet at δ 7.19, triplet at δ 6.97, doublet at δ 5.45 can be respectively assigned to the aromatic protons H6, H5 and H4 of DMBbimH2, and a singlet at δ 2.60 can be assigned to the methyl group of DMBbimH2. In the spectrum of 1-A, there was a broad signal at δ 13.80. The broadness and extreme low-field shift suggest that it corresponds to the N-H protons of DMBbimH2.
In the spectrum of 1 - B, two of resonances of the bpy group were overlapped at δ 8.06~7.88. With the removal of the first proton, the signal of N - H proton disappeared, signals of H4, H5 and H6 of complex 1-B shifted towards the up - field region by 0.14, 0.31 and 0.34, respectively. The chemical shift of the methyl group protons is at δ 2.55.
For 1-C, the varieties of chemical shifts of bpy group and methyl group (δ 2.49) protons were smaller, while the aromatic protons of DMBbim ligand exhibited a larger shift. With the removal of the second proton, signals of H4, H5 and H6 of complex 1 - C further shifted towards the up - field region by 0.15, 0.34 and 0.33, respectively. This is because that as the bi-benzimidazole ligand is gradually deprotonated, the overall electron cloud density of the ligand increases. H4, H5 and H6 are getting closer and closer to the de-hydrogenated N atoms, so they are gradually affected by dehydrogenation.
2.3 Absorption spectral studies.
Absorption spectral profiles of the complexes in acetonitrile are presented in Fig. 3, and the related data are summarized in Table 3. In order to compare the rel-ative intensity of the absorption bands, iso-molar solu-tions (60 μmol·L-1) of the complexes were used.
Figure 3
Table 3
Complex λmax / nm 1-A 244(sharp), 292(sharp), 335(sharp), 354(sharp), 476(broad) 1-B 246(sharp), 295(sharp), 341(moderate), 515(broad) 1-C 212(sharp), 247(sharp), 296(sharp), 338(moderate), 552(broad) The highly intense absorption bands observed in UV region arise mainly due to the π - π* transitions within the bpy and DMBbimH x units[15, 31]. The strong absorption band at 290~300 nm can be attributed to π-π* transition of bpy ligand. The 335 nm absorption band of 1 - A, 341 nm band of 1 - B, 338 nm band of 1-C, are assigned to π-π* transition of the DMBbimHx ligands, respectively. The moderately intense broad bands in visible region can be attributed to M(dπ) → bpy(π*) and M(dπ)→DMBbimHx(π*) MLCT transi-tions.
In the absorption spectral profiles, it was observed that the MLCT bands in the complexes underwent grad-ual red-shifts. With the removal of protons, the absorp-tion peak was red -shifted from 476 nm (1-A) to 515 nm (1-B) and finally to 552 nm (1-C). This is because the interaction (mono-deprotonation or bi-deprotonation in DMBbimHx ligand) greatly increases the electron densi-ty at the Ru(Ⅱ) center and leads to a less-positive oxida-tion potential (section 2.4), resulting in the decrease of MLCT band energy.
2.4 Electrochemistry
Electrochemical behaviors of the complexes in dichloromethane and acetonitrile were studied through CV and SWV methods using Ag/AgCl reference elec-trode and ammonium hexafluorophosphate as support-ing electrolyte. E1/2 values were obtained from SWV using glassy carbon electrode.
As shown in Fig. 4, in dichloromethane, the mono-nuclear complex 1 - A underwent oxidation irreversibly at 1.35 V. CV and SWV measurements of 1-B in dichloromethane revealed characteristic phenomena for cooperative proton electron transfer. Two successive electrode oxidation couples (E1/2, 1=0.97 V and E1/2, 2= 1.33 V (vs Ag/AgCl)) were observed, revealing that the complex undergoes two successive one-electron revers-ible oxidation processes due to Ru(Ⅱ) - Ru(Ⅱ)/Ru(Ⅲ)- Ru(Ⅱ)and Ru(Ⅲ)-Ru(Ⅱ)/Ru(Ⅲ)-Ru(Ⅲ) processes, respec-tively. This is due to the presence of hydrogen -bonded dimers in 1-B. In 1-B, there is only one N-H bond on the DMBbimH ligand. Two [Ru(bpy)2(DMBbimH)]+ cat-ions are easily bonded by hydrogen bonds to form a dimer structure, which can not only exist in solid state, but also exist stably in weak polar solvents. The redox of two Ru centers in the dimer is not completely sym-metrical and simultaneous. One of the metal centers Ru(Ⅱ) is oxidized to Ru(Ⅲ) first (Fig. 5), and then the oth-er metal center is oxidized. The extent of electronic in-teraction between two metal centers in homo-bimetallic complexes can be estimated from the differences between two oxidation potentials (△E1/2=|E1/2, 2-E1/2, 1|)[15]. E1/2 value obtained in this way was 0.36 V.
Figure 4
Figure 5
The doubly deprotonated complex 1-C underwent oxidation irreversibly at 0.71 V in dichloromethane. As expected, deprotonation of the bi-benzimidazole ligand leads to shifts towards more negative potentials for the oxidation of the ruthenium center. This indicates an enhanced electron density at the metal center induced by deprotonation[11].
As we know, the polarity of solvent has a great effect on the formation of hydrogen-bonded species and the electrochemical properties of complexes. Therefore, the electrochemical behaviors of the complexes in ace-tonitrile, whose polarity is much stronger than dichloro-methane, were explored. The CV and SWV of the complexes are shown in Fig. 6. In the curves we can easily find that each complex exhibited a reversible wave corresponding to Ru(Ⅱ)/Ru(Ⅲ) oxidation process in acetonitrile. Ru(Ⅱ)/Ru(Ⅲ) oxidation potential gradually shifted towards lower potential as the complex was changed from 1-A (E1/2=1.22 V) to 1-B (E1/2=0.88) and finally to 1 - C (E1/2 =0.57 V) and this is line with the observed absorption spectral trends.
Figure 6
Comparing Fig. 4 and Fig. 6, we can easily find out that the electrochemical properties of complex 1 - B in dichloromethane and acetonitrile differ greatly, which is due to the different polarities of solvents. In dichloro - methane, mononuclear complex 1 - B undergoes a two - step oxidation, which indicates the existence of PCET between [Ru(bpy)2(DMBbimH)]+ cations. The [Ru(bpy)2 (DMBbimH)]+ cations exist as hydrogen-bonded dimers in dichloromethane, and the existence of hydrogen-bonded dimers is proved by single crystal structure (section 2.5). However, the dimers cannot exist stably in more polar acetonitrile, and the cations exist as monomers, therefore, only one peak can be observed on CV and SWV curves.
In conclusion, for 1- B, dimers are formed prefer-entially over the corresponding monomers in weakly polar solvents, such as dichloromethane. CV measure-ments show that 1-B reversibly generates stable mixed-valence states RuⅡRuⅢ upon oxidation. As a result, it is reasonable that the mixed - valence states are stabi-lized by proton transfer of complementary hydrogen bonds[27].
2.5 Single-crystal structure of 2
Dark red single crystals of complex [Ru(bpy)2 (DMBbimH)]PF6·2CH 2Cl2 (2) were obtained from dichloromethane solution of 1-B. The single crystal structure of 1-B indicates that it belongs to C 2/c space group of monoclinic system. Each asymmetric unit con-tains a [Ru(bpy)2(DMBbimH)]+ cation, a PF6- anion and two dichloromethane molecules. The components are supported by elemental analysis data. The solvents were squeezed by SQUEEZE/PLATON program because the dichloromethane molecules were disor-dered.
As shown in Fig. 7a, each Ru(Ⅱ)ion is coordinated with six N atoms from two bpy ligands and one DMB-bimH- ligand to form an octahedral coordination geom-etry. The Ru-N bond length between Ru(Ⅱ)ion and bpy is between 0.204 3(4) and 0.205 4(4) nm, and the Ru-N bond length with DMBbimH- ligand is slightly longer (0.208 9(4)~0.210 8(4) nm), but agrees with literature values[5-19]. The N-Ru-N bite angles vary from 78.3° to 78.8°, while the trans angles lie in a range of 171.7(2)° ~179.2(2)°. The DMBbimH- ligand coordinates in a bidentated manner with N5 and N7, remaining the other two N atoms (N6 and N8) uncoordinated. The hydrogen atoms on N6 and N8 are disordered, and H6A and H8A are both half-occupied due to the sym-metry. Each [Ru(bpy)2(DMBbimH)] + cation pairs up with a symmetry-equivalent cation to generate a dimer-ic unit [Ru(bpy)2(DMBbimH]22+ containing a self-com-plementary double hydrogen-bonded bridge (Fig. 7a). The N6…N6A separation is 0.271 5 nm and the N6 - H6A -N6A angle is 166.5°, and the N8…N8A separa-tion is 0.278 5 nm and the N8 - H8A - N8A angle is 172.9°. Only half of hydrogen atoms (H6A and H8A) are presented in Fig. 7a. The Ru…Ru distance defined by this supramolecular arrangement is 1.011 9 nm.
Figure 7
The dihedral angle between the planes of two benzimidazole in a DMBbimH- ligand is 6.2°, indicat-ing an almost planar structure of the DMBbimH-moiety in 2. It is worth mentioning that the angle between two DMBbimH- ligands in a dimer is twisted to about 57.2° (Fig. 7b), which should be attributed to the side- by-side steric repulsion between the methyl groups at the 7 and 7' positions.
There are abundant weak intermolecular forces in the structure, as shown in Fig. 8[32]. The cations and anions are connected by C-H…F weak hydrogen bonds (Table 4) to form two-dimensional layers, which are linked into three-dimensional network by N- H…N hydrogen bonds between cations. The solvent mole-cules fill in one- dimensional channels along the c-axis direction formed by the cations and anions.
Figure 8
Table 4
D-H…A d(D-H) / nm d(H…A) / nm d(D…A) / nm ∠DHA / (°) C11-H11…F5 0.093 0.254 0.342 0(8) 157.7 C12-H12…F1 0.093 0.258 0.325 0(9) 128.9 C14-H14…F2A 0.093 0.242 0.328 8(7) 155.6 C19-H19…F3B 0.093 0.262 0.354 8(9) 172.0 C19-H19…F5B 0.093 0.252 0.326 2(7) 136.8 N6-H6…N6C 0.088 0.186 0.272 1(8) 166.6 N8-H8…N8C 0.089 0.191 0.280 0(7) 172.9 Symmetry codes: A: -x+1/2, -y+3/2, -z+1; B: x, -y+1, z+1/2; C: -x+1, y, -z+3/2. 3. Conclusions
In summary, three ruthenium(Ⅱ) polypyridyl com-plexes containing 7, 7'-dimethyl-2, 2'- bibenzimidazole ligand (DMBbimH x) were synthesized and determined by 1H NMR, UV - Vis absorption and electrochemical measurements. From 1 - A to 1-B and then to 1-C, N-H in DMBbimHx ligands gradually deprotonated, result-ing in evident differences of the spectroscopic and electrochemical properties of complexes. Interestingly, for mono-deprotonated 1-B, the electrochemical proper-ties behaved very differently in dichloromethane and acetonitrile, which is due to different polarities of solvents. In acetonitrile, there was only one redox peak in CV curve, while in dichloromethane, it underwent a two - step oxidation, which indicates the existence of PCET in hydrogen-bonded dimers formed by [Ru(bpy)2 (DMBbimH)]+ cations. The single crystal structure of 2 indicates that [Ru(bpy)2(DMBbimH)]+ cations exist as hydrogen-bonded dimers in weakly polar solvent dichloromethane. This is consistent with the result of electrochemical measurements of complex 1-B in dichloromethane.
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Table 1. Crystal data and structure parameters for complex 2
Empirical formula C38H33Cl4F6N8PRu Formula weight 989.56 Crystal system Monoclinic Space group C2/c a / nm 3.182 7(2) b / nm 1.638 4(1) c / nm 1.885 3(1) β/(°) 111.255(2) V / nm3 9.162(1) Z 8 Dc / (g·cm-3) 1.435 Absorption coefficient / mm-1 0.671 F(000) 3 984 Crystal size / mm 0.230×0.200×0.160 θ range for data collection / (°) 3.094~25.999 Limiting indices -39 ≤ h ≤39, -20 ≤ k ≤20, -21 ≤ l ≤ 23 Reflection collected, unique 36 729, 8 972 (Rint=0.108 5) Reflection observed 6 835 Completeness to θ=25.242 / % 99.7 Data, restraint, parameter 8 972, 0, 469 Goodness-of-fit on F2 1.032 Final R indices [I > 2σ(I)] R1a=0.067 8, wR2b=0.175 6 R indices (all data) R1a=0.086 6, wR2b=0.189 1 a R1=Σ||Fo|-|Fc||/Σ|Fo|; bwR2=[Σw(Fo2-Fc2)2/Σw(Fo2)2]1/2. Table 2. Selected bond lengths (nm) and angles (°) for complex 2
Ru1-N1 0.204 3(4) Ru1-N2 0.204 7(4) Ru1-N3 0.205 4(4) Ru1-N4 0.205 2(4) Ru1-N5 0.208 9(4) Ru1-N7 0.210 8(4) C21-N5 0.138 9(6) C28-N5 0.133 6(6) C26-N6 0.138 8(6) C28-N6 0.135 4(6) C29-N7 0.134 7(6) C30-N7 0.138 9(6) C29-N8 0.134 8(6) C35-N8 0.139 9(6) C28-C29 0.144 4(6) N2-Ru1-N1 78.6(2) N4-Ru1-N3 78.8(2) N5-Ru1-N7 78.3(1) N2-Ru1-N3 89.0(2) N4-Ru1-N5 85.1(1) N1-Ru1-N7 85.8(1) N3-Ru1-N5 95.6(1) N2-Ru1-N7 97.6(2) N1-Ru1-N5 95.4(1) N4-Ru1-N7 94.9(2) N3-Ru1-N1 100.5(2) N2-Ru1-N4 100.9(2) N4-Ru1-N1 179.2(1) N2-Ru1-N5 173.0(1) N3-Ru1-N7 171.7(1) C31-C30-C35 120.3(4) C22-C21-C26 121.0(4) C24-C25-C26 115.4(4) N7-C30-C35 108.3(4) C23-C22-C21 116.5(4) C24-C25-C27 124.0(5) C30-C31-C32 117.1(4) C22-C23-C24 122.0(5) C26-C25-C27 120.6(4) N5-C21-C22 131.3(4) C25-C24-C23 122.9(5) N6-C26-C25 129.5(4) N5-C21-C26 107.7(4) C1-N1-C5 117.5(4) N6-C26-C21 108.2(4) C25-C26-C21 122.2(4) C10-N2-C6 118.0(4) N7-C29-C28 116.1(4) N5-C28-N6 115.3(4) C11-N3-C15 118.9(4) N8-C29-C28 129.1(4) N5-C28-C29 117.3(4) C20-N4-C16 118.5(4) C31-C30-N7 131.4(4) N6-C28-C29 127.4(4) N7-C29-N8 114.9(4) C31-C32-C33 122.2(5) C28-N5-C21 104.7(4) C29-N8-C35 104.8(4) C34-C33-C32 122.3(5) C28-N6-C26 104.0(4) C33-C34-C35 115.7(4) C33-C34-C36 122.3(4) C29-N7-C30 104.7(4) C35-C34-C36 122.0(4) C34-C35-N8 130.2(4) C34-C35-C30 122.4(4) N8-C35-C30 107.4(4) Table 3. Absorption spectroscopic data for complexes in acetonitrile
Complex λmax / nm 1-A 244(sharp), 292(sharp), 335(sharp), 354(sharp), 476(broad) 1-B 246(sharp), 295(sharp), 341(moderate), 515(broad) 1-C 212(sharp), 247(sharp), 296(sharp), 338(moderate), 552(broad) Table 4. Selected hydrogen bond parameters in 2
D-H…A d(D-H) / nm d(H…A) / nm d(D…A) / nm ∠DHA / (°) C11-H11…F5 0.093 0.254 0.342 0(8) 157.7 C12-H12…F1 0.093 0.258 0.325 0(9) 128.9 C14-H14…F2A 0.093 0.242 0.328 8(7) 155.6 C19-H19…F3B 0.093 0.262 0.354 8(9) 172.0 C19-H19…F5B 0.093 0.252 0.326 2(7) 136.8 N6-H6…N6C 0.088 0.186 0.272 1(8) 166.6 N8-H8…N8C 0.089 0.191 0.280 0(7) 172.9 Symmetry codes: A: -x+1/2, -y+3/2, -z+1; B: x, -y+1, z+1/2; C: -x+1, y, -z+3/2. -

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