Huiming Zhang,
Xiaogang Yan,
Jiang Zhao,
Xiaolong Yang,
Zuan Huang,
Guijiang Zhou* and
Yong Wu*
MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, State Key Laboratory for Mechanical Behavior of Materials, Institute of Chemistry for New Energy Material, Department of Chemistry, Faculty of Science, Xi'an Jiaotong University, Xi'an 710049, P. R. China. E-mail: zhougj@mail.xjtu.edu.cn; specwy@mail.xjtu.edu.cn
First published on 30th September 2015
Under controlled conditions, platinum(II) polymetallaynes with different 2,2′-biimidazole-based organic spacers have been synthesized readily. Their photophysical properties and fluorescent response behaviors to Cu2+ ions have been investigated in detail. By adjusting both the configuration of the 2,2′-biimidazole-based spacers and the steric effect, the fluorescent response behaviors of the polymetallaynes to Cu2+ ions can be tuned dramatically. The fluorescent signal from the polymetallayne with an optimized structure can be quenched rapidly by Cu2+ ions with a high Stern–Volmer constant KSV of ca. 6.8 × 104 M−1 and a low detecting limit (DL) of ca. 0.99 ppm. These results not only highlight the great potential of these polymetallaynes as novel Cu2+ sensors, but also provide new strategies for optimizing the sensing abilities of the 2,2′-biimidazole-based ion sensors.
Polymetallaynes obtained by the incorporation of transition metal ions into a polymeric skeleton have been identified as an exciting and extensively investigated area in the field of conjugated polymers.18 The novel skeletons of polymetallaynes provide good scope for coupling the chemical, electronic and optical properties of metal complexes to those of the organic component, thus accessing novel polymers with new functional properties such as optical power limiting,19 electroluminescence,20 and photovoltaic behavior.21 It has been shown that the chemical and electronic features of the organic components can have a great influence on the optoelectronic properties of polymetallaynes.18 Therefore, employing the 2,2′-biimidazole unit should be a feasible way to develop novel polymetallaynes, which has never been reported to the best of our knowledge. Bearing this in mind, polymetallaynes with the 2,2′-biimidazole unit have been developed. In addition, their fluorescent response behaviors to Cu2+ ions have been successfully tuned by optimizing the configuration of the 2,2′-biimidazole units and the steric effect. The results obtained will not only provide important structure–property relationship information of these polymetallaynes, but also indicate their potential in the field of ion sensors. Importantly, this contribution should provide a new strategy for optimizing the properties of the 2,2′-biimidazole-based sensors.
BIA1 (VDCM/VMeOH = 20:
1, yield 95%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.10 (d, J = 0.8 Hz, 2H), 6.95 (d, J = 0.4 Hz, 2H), 4.03 (s, 6H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.64, 127.81, 122.59, 35.32; FAB-MS (m/z): 162 [M]+; anal. calcd for C8H10N4: C, 59.24; H, 6.21; N, 34.54; found: C, 59.19; H, 6.28; N, 34.47.
BIA2 (VDCM/VMeOH = 20:
1, yield 89%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.09 (d, J = 1.2 Hz, 2H), 6.98 (d, J = 1.2 Hz, 2H), 4.41 (t, J = 7.2 Hz, 4H), 1.70 (t, J = 6.8 Hz 4H), 1.26 (m, 12H), 0.83 (t, J = 6.8 Hz, 6H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.04, 127.88, 120.95, 47.31, 31.24, 30.99, 26.13, 22.44, 13.93; FAB-MS (m/z): 302 [M]+; anal. calcd for C18H30N4: C, 71.48; H, 10.00; N, 18.52; found: C, 71.36; H, 10.11; N, 18.43.
BIA3 (VDCM/VMeOH = 10:
1, yield 83%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.18 (s, 2H), 6.95 (s, 2H), 4.36 (s, 4H); 13C NMR (100 MHz, CDCl3): δ (ppm) 137.99, 130.21, 118.71, 43.12; FAB-MS (m/z): 160 [M]+; anal. calcd for C8H8N4: C, 59.99; H, 5.03; N, 34.98; found: C, 59.89; H, 5.15; N, 34.88.
BIBr1 (VDCM/VMeOH = 20:
1, yield 63%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.19 (s, 2H), 3.96 (s, 6H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.89, 128.51, 106.72, 33.87; FAB-MS (m/z): 320 [M]+; anal. calcd for C8H8Br2N4: C, 30.03; H, 2.52; N, 17.51; found: C, 29.91; H, 2.57; N, 17.46.
BIBr2 (VDCM/VMeOH = 20:
1, yield 66%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.08 (s, 2H), 4.44 (t, J = 7.6 Hz, 4H), 1.66 (t, J = 6.8 Hz, 4H), 1.25 (m, 12H), 0.86 (t, J = 6.4 Hz, 6H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.41, 128.70, 105.53, 46.09, 31.15, 30.22, 26.05, 22.48, 13.94; FAB-MS (m/z): 460 [M]+; anal. calcd for C18H28Br2N4: C, 46.97; H, 6.13; N, 12.17; found: C, 46.89; H, 6.21; N, 12.09.
BIBr3 (VDCM/VMeOH = 10:
1, yield 60%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.19 (s, 2H), 4.32 (s, 4H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.25, 130.72, 102.89, 41.64; FAB-MS (m/z): 318 [M]+; anal. calcd for C8H6Br2N4: C, 30.22; H, 1.90; N, 17.62; found: C, 30.17; H, 2.05; N, 17.49.
BISi1 (VDCM/VMeOH = 50:
1, yield 75%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.36 (s, 2H), 4.00 (s, 6H), 0.27 (s, 18H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.40, 133.75, 118.34, 103.64, 92.57, 33.59, −0.17; FAB-MS (m/z): 354 [M]+; anal. calcd for C18H26N4Si2: C, 60.97; H, 7.39; N, 15.80; found: C, 60.89; H, 7.32; N, 15.73.
BISi2 (VDCM/VMeOH = 50:
1, yield 73%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.33 (s, 2H), 4.49 (t, J = 7.6 Hz, 4H), 1.70 (t, J = 6.8 Hz, 4H), 1.25 (m, 12H), 0.87–0.84 (m, 6H), 0.26 (s, 18H); 13C NMR (100 MHz, CDCl3): δ (ppm) 137.77, 133.94, 117.43, 103.00, 93.04, 46.05, 31.26, 30.38, 26.20, 22.50, 13.96, −0.21; FAB-MS (m/z): 494 [M]+; anal. calcd for C28H46N4Si2: C, 67.96; H, 9.37; N, 11.32; found: C, 67.91; H, 9.42; N, 11.27.
BISi3 (VDCM/VMeOH = 30:
1, yield 85%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.41 (s, 2H), 4.36 (s, 4H), 0.27 (s, 18H); 13C NMR (100 MHz, CDCl3): δ (ppm) 135.96, 132.02, 128.48, 104.21, 91.49, 41.14, −0.22; FAB-MS (m/z): 352 [M]+; anal. calcd for C18H24N4Si2: C, 61.32; H, 6.86; N, 15.89; found: C, 61.23; H, 6.93; N, 15.79.
L1 (VDCM/VMeOH = 20:
1, yield 97%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.40 (s, 2H), 4.04 (s, 6H), 3.56 (s, 2H); 13C NMR (100 MHz, CDCl3): δ (ppm) 138.50, 134.10, 117.33, 85.69, 72.15, 33.67; FAB-MS (m/z): 210 [M]+; anal. calcd for C12H10N4: C, 68.56; H, 4.79; N, 26.65; found: C, 68.47; H, 4.84; N, 26.55.
L2 (VDCM/VMeOH = 20:
1, yield 90%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.37 (s, 2H), 4.54 (t, J = 7.2 Hz, 4H), 3.53 (s, 2H), 1.70 (t, J = 7.2 Hz, 4H), 1.24 (m, 12H), 0.85 (t, J = 6.4 Hz, 6H); 13C NMR (100 MHz, CDCl3): δ (ppm) 137.88, 134.44, 116.41, 85.16, 72.45, 46.06, 31.17, 30.43, 26.06, 22.45, 13.93; FAB-MS (m/z): 350 [M]+; anal. calcd for C22H30N4: C, 75.39; H, 8.63; N, 15.98; found: C, 75.29; H, 8.60; N, 15.93.
L3 (VDCM/VMeOH = 10:
1, yield 97%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.46 (s, 2H), 4.04 (s, 4H), 3.59 (s, 2H); 13C NMR (100 MHz, CDCl3): δ (ppm) 136.35, 132.04, 128.43, 86.17, 71.24, 41.23; FAB-MS (m/z): 208 [M]+; anal. calcd for C12H8N4: C, 69.22; H, 3.87; N, 26.91; found: C, 69.15; H, 3.92; N, 26.85.
P1 (yield 87%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.05 (s), 3.99 (s), 2.12 (br), 1.58 (br), 1.46–1.41 (m), 0.92 (m); 31P NMR (161.9 MHz, CDCl3): δ (ppm) 3.42; gel permeation chromatography (GPC): number-average molecular weight (Mn) = 8.8 × 104 g mol−1, polydispersity index (PDI) = 1.40 (against polystyrene standards).
P2 (yield 85%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.02 (s), 4.53 (s), 2.11 (br), 1.62–1.49 (br), 1.47–1.41 (m), 1.20 (br), 0.93–0.90 (m), 0.85–0.81 (m); 31P NMR (161.9 MHz, CDCl3): δ (ppm) 3.64; gel permeation chromatography (GPC): number-average molecular weight (Mn) = 8.0 × 104 g mol−1, polydispersity index (PDI) = 1.48 (against polystyrene standards).
P3 (yield 86%) 1H NMR (400 MHz, CDCl3): δ (ppm) 7.10 (s), 4.26 (s), 2.09 (br), 1.58–1.57 (br), 1.47–1.41 (m), 0.95–0.91 (m); 31P NMR (161.9 MHz, CDCl3): δ (ppm) 3.47; gel permeation chromatography (GPC): number-average molecular weight (Mn) = 8.8 × 104 g mol−1, polydispersity index (PDI) = 1.47 (against polystyrene standards).
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Fig. 1 The UV-vis and photoluminescence (PL) spectra for the 2,2′-biimidazole-based polymetallaynes in THF at 293 K. |
Polymers | Absorption λabsa (nm) 293 K | Emission λema (nm) 293 K/77 K | τc S1/T1 | ΦFd | Ege (eV) | ΔT5% (°C) |
---|---|---|---|---|---|---|
a Measured in THF at a concentration of 10−5 M for the repeating unit.b Shoulder.c The lifetime (τ) for the first singlet states (S1) was referred to the emission band at ca. 410 nm and that for the first triplet states (T1) was referred to the emission band around 510 nm. The τ for T1 was measured at 77 K. The excitation wavelength for the measure was set to 330 nm.d The fluorescent quantum yields (ΦF) were measured in THF with quinine sulfate in 1.0 M H2SO4 (ΦF ca. 0.56) as the standard. The excitation wavelength for the measure was set to 334 nm.e Calculated from the absorption onset. | ||||||
P1 | 380 | 405, 420b, 505/502, 540 | 1.75 ns/121.5 μs | 0.10 | 3.08 | 300 |
P2 | 377 | 406, 420b, 505/504, 540 | 1.75 ns/141.3 μs | 0.12 | 3.09 | 305 |
P3 | 383 | 413, 427b/518, 554 | 2.59 ns/131.1 μs | 0.10 | 3.00 | 303 |
To obtain the proper photoluminescence (PL) spectra of these polymetallaynes, their excitation spectra were measured in THF. From the excitation spectra (Fig. S1†), the most suitable excitation wavelength should be in the range from 330 nm to 350 nm. Therefore, the excitation wavelength was set to 340 nm for PL measurements of these biimidazole-based polymetallaynes. In THF solution, all the polymetallaynes exhibited an emission band at ca. 410 nm (Fig. 1 and Table 1) in their PL spectra under excitation with 340 nm light. From the absorption onset, P3 should possess the smallest band gap (Eg) (Table 1 and Fig. 1) due to the better conjugation extending ability of the biimidazole unit in P3. Therefore, it shows the longest emission wavelength (ca. 413 nm). Possessing a similar Eg, P1 and P2 display a similar emission maximum (Table 1 and Fig. 1). It seems that there is another emission band at a longer wavelength, ca. 500 nm, for P1 and P2, especially for P1. At 77 K, all the polymetallaynes showed a dominant emission band around 510 nm with a long lifetime in the order of microseconds (Table 1 and Fig. S2†), indicating its phosphorescent character. The major emission band at low temperatures can show good overlap with the weak emission band in P1 and P2 at room temperature (Fig. S2†). Therefore, this weak emission with long wavelength should be the phosphorescent signal induced by the platinum(II) centers. The phosphorescent signal at room temperature has also been observed in the fluorine-based analog. With quinine sulfate as a standard, the fluorescent quantum yields (ΦF) for P1, P2 and P3 are 0.10, 0.12 and 0.10, respectively.
The thermal stability of the polymetallaynes was investigated by thermogravimetric analysis (TGA) under a nitrogen atmosphere. The TGA results indicate their thermal stability with the 5% weight-reduction temperature (ΔT5%) at ca. 300 °C (Table 1). The good thermal properties will benefit their applications.
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Fig. 2 Fluorescence spectra of the biimidazole-based polymetallaynes upon the titration of Cu2+ in THF at 293 K. |
From the fluorescence titration spectra for these polymetallaynes (Fig. 2), it can be seen clearly that the fluorescent signal for P1 and P3 has been efficiently quenched by Cu2+ ions. As shown in Fig. 2a and c, upon the addition of Cu2+ ions, the emission peaks at 405 nm for P1 and 413 nm for P2 decrease gradually with increasing Cu2+ concentration in the solution samples. After adding 1.2 equivalents of Cu2+, 73% and 84% of the fluorescence intensity has been quenched for P1 and P2, respectively. However, it seems that the fluorescent signal for P2 is quite insensitive to the added Cu2+ ions, because only 15% of the fluorescence intensity can be quenched at 1.2 equivalents of Cu2+ ions. The fluorescence quenching efficiency can be described by the Stern–Volmer equation, I0/I = KSV[A] + 1,29 relating to the fluorescence intensity, I, at different concentrations of the analyte quencher, [A]. In this equation, I0 is the intensity at [A] = 0 and KSV is the Stern–Volmer constant. Based on the fluorescence titration results of these polymetallaynes in THF solution with Cu2+, KSVs of these systems were determined to be 3.5 × 104 M−1 for P1, 7.9 × 103 M−1 for P2 and 6.8 × 104 M−1 for P3 (Fig. S3†). Accordingly, the detecting limits (DL) obtained by the literature method30 were 2.0 × 10−6 M, 3.4 × 10−6 M and 9.9 × 10−7 M for P1, P2 and P3, respectively. The data indicates quantitatively a much higher sensitivity of the fluorescent signal of P1 and P3 to the external Cu2+ ions than that of P2. It is well known that the Cu2+ ions can coordinate easily with bipyridine (N,N′)-type bidentate ligands.29 Therefore, the fluorescence quenching in these polymetallaynes should be ascribed to the electron-transfer interactions between the polyyne backbone and Cu2+ ions induced by the coordination of the 2,2′-biimidazole units with the Cu2+ ions. Based on the KSV and DL data, it is clear that the coordinating ability of the 2,2′-biimidazole units in different polymetallaynes is in the order of P3 > P1 ≫ P2, indicating the critical role played by the structural features of the 2,2′-biimidazole unit in determining the fluorescence response behaviors of these polymetallaynes.
The titration plots of the emission intensity of these biimidazole-based polymetallaynes against [Cu2+]/[biimidazole unit] were obtained to interpret their fluorescence quenching behaviors. From the titration plots (Fig. S4†), the 1:
1 stoichiometry for [Cu2+]/[biimidazole unit] can be clearly observed.31 Furthermore, the mass spectra also revealed that the organic ligands can form one-to-one adducts with Cu2+ ions as well (Fig. S5†). Based on the stoichiometry of the fluorescence quenching process, the chelating pattern of Cu2+ ions with the N,N′-type ligands5,11 and the mass spectrum results, the possible mechanism involved in the fluorescence quenching of these biimidazole-based polymetallaynes is proposed in Fig. 3. According to the chelating pattern of Cu2+ ions with the N,N′-type bidentate ligands,5,11 the coordinating of the 2,2′-biimidazole units with Cu2+ ions in P1 and P2 will involve the rotation of the imidazole rings to induce the configuration conversion of the 2,2′-biimidazole units from the low-energy optimized configuration with two alkyl groups in the trans pattern to the coplanar configuration with two alkyl groups in cis form (Fig. 3). Despite the energy difference between the two types of configurations of the 2,2′-biimidazole units in P1 and P2 being nearly identical (Fig. 4), P1 and P2 still exhibit markedly different fluorescent titration spectra (Fig. 2). Therefore, it can be concluded that energy associated with the configuration transfer of the 2,2′-biimidazole units might not be the decisive factor in the coordination process between the 2,2′-biimidazole units and Cu2+ ions in P1 and P2. To clarify this issue, the optimized configuration of the segment of P2 was obtained (Fig. 5). From the optimized configuration of the segment of P2, it can be seen clearly that there should be severe steric effect between the hexyl groups and the bulky tributylphosphine units chelated with the platinum(II) centers in the configuration transfer of the 2,2′-biimidazole units (Fig. 5). Obviously, the severe steric effect will greatly restrain the rotation of the imidazole rings and impede the formation of the desired configuration favorable for the coordination of the 2,2′-biimidazole units with Cu2+ ions (Fig. 3). Therefore, P2 shows much lower KSV (7.9 × 103 M−1), almost an order magnitude lower, than P1 and P3 together with the highest DL of 3.4 × 10−6 M. However, there would be almost no space hindrance effect if the alkyl units attached to the 2,2′-biimidazole units are much smaller methyl groups. Therefore, the imidazole rings can easily rotate to facilitate the formation of the cis coplanar configuration of the 2,2′-biimidazole units in P1 and the coordination with the external Cu2+ ions to effectively quench the fluorescent signal of P1 (Fig. 3). Owing to the great tendency for the coordination of the Cu2+ ions with N,N′-type bidentate ligands,27 the coordination between Cu2+ ions and the 2,2′-biimidazole units in P1 should release much more energy than that required for the configuration conversion of the 2,2′-biimidazole units. This means that the coordination between the cis 2,2′-biimidazole units and Cu2+ ions should be an energy-favored processed. Therefore, it will guarantee the coordination of the Cu2+ ions with the 2,2′-biimidazole units in P1 and effective fluorescence quenching in P1 by the added Cu2+ ions, as indicated by Fig. 2. Therefore, P1 exhibits a much higher KSV of 3.5 × 104 M−1 as well as a lower DL of 2.0 × 10−6 M than P2.
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Fig. 3 Proposed mechanism for the different fluorescence quenching behaviors in P1 (a), P2 (b) and P3 (c). |
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Fig. 4 Energy difference between the low-energy optimized trans configuration and the coplanar cis configuration of the different 2,2′-biimidazole units in P1 (a), P2 (b) and P3 (c). |
Obviously, the configuration of the 2,2′-biimidazole units in the backbone of P3 should be in great favor of their coordination with Cu2+ ions. The imidazole ring would need nearly no rotation to form the favored cis configuration of the 2,2′-biimidazole units in P3 (Fig. 3) because the dihedral angle between the two imidazole rings is only ca. 12° in the optimized configuration of the 2,2′-biimidazole units in P3 (Fig. 4 and S6†). Furthermore, the energy difference between the low-energy optimized configuration and the coplanar cis configuration of the 2,2′-biimidazole units in P3 is very small (Fig. 4), which will greatly facilitate the formation of the coplanar configuration. All these factors will effectively promote the coordination of Cu2+ ions with the 2,2′-biimidazole units in P3. Therefore, the fluorescent signal of P3 can be quenched most effectively by the added Cu2+ ions, which is indicated by its fluorescent titration spectra (Fig. 2) and the highest KSV of 6.8 × 104 M−1 and the lowest DL of 9.9 × 10−7 M for P3 among the three polymetallaynes.
Interestingly, the quenched fluorescent signals of these polymetallaynes can be restored easily by adding S2− ions (Fig. S7†). Clearly, the recovered fluorescence should be due to the very strong bonding between Cu2+ cations and S2− anions indicated by the extremely low Ksp (ca. 1.3 × 10−36 at 298 K) of CuS. This result also shows that the interaction between Cu2+ cations and 2,2′-biimidazole units should form one-to-one adducts, which leaves the one side of the Cu2+ cations exposed to the S2− anions to facilitate their bonding process. Therefore, the result should also indicate the validity of the proposed mechanism in Fig. 3. In addition, these results should mean that the polymetallaynes might be recycled for Cu2+ sensing by adding S2− anions.
From the aforementioned results, it can be concluded that optimizing both the configuration of the 2,2′-biimidazole units and the steric effect can play a very critical role in tuning the fluorescent response behaviors of the polymetallaynes to Cu2+ ions. Clearly, these results will definitely provide valuable information for optimizing the sensing properties of the 2,2′-biimidazole derivatives as Cu2+ sensors.
The response behavior of the fluorescent signal of these polymetallaynes to other cations with different charge has also been investigated. As shown in Fig. 6 and S8,† the experimental results clearly show that only the Cu2+ ions can show the most efficient quenching effect to the fluorescent signal of these polymetallaynes, especially P1 and P3 (Fig. 6). In addition, after absorption calibration, the precious metal ions, such as Ru3+, Ir3+ and Rh3+, will not interfere with the Cu2+ sensing process of P1 and P3 as well. This result shows that P1 and P3 can exhibit good selectivity, if they would be employed as Cu2+ sensors.
Footnote |
† Electronic supplementary information (ESI) available: Synthetic detail of 2,2′-biimidazole, PL spectra at different temperature and theoretical fitting results. See DOI: 10.1039/c5ra17853c |
This journal is © The Royal Society of Chemistry 2015 |