一种水中稳定的锌(Ⅱ)金属有机骨架用于检测四环素
English
A stable Zinc(Ⅱ)metal-organic framework in water for the detection of tetracycline
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Key words:
- metal-organic framework
- / crystal structure
- / tetracycline
- / fluorescent sensor
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In recent years, the emergence of antibiotics as a new class of organic pollutants in the natural water environment has attracted extensive attention from domestic scholars. Tetracycline (TET) antibiotics are one of the most widely used antibiotics in China due to their low cost and low toxicity. They have a high half - life in water. They often accumulate in trace form in water, and enter mammals through drinking water and the food chain, causing liver damage, increasing drug resistance, and threatening environmental safety[1]. Therefore, it is of great significance to study the detection of TET.
Metal-organic frameworks (MOFs) are porous materials that have recently attracted a great deal of attention due to their high potential for use in molecule design[2-3]. These materials are constructed from inorganic clusters and organic molecules to form 1D, 2D, or 3D structures. Due to its many advantages, MOFs have been successfully applied in fields such as heterogeneous catalysis[4-7], gas storage and separation[8-10], drug delivery[11], sensing[12-13], energy storage[14], and conductivity[15]. A large number of MOFs with luminescent sensing properties were synthesized and used for the detection of specific metal ions, small organic molecules, antibiotics, and nitroaromatic compounds (NACs) [16-18]. Especially, the MOFs of transition metal ions with d10 electronic structure have better luminescence properties, because the metal ions may shift and enhance the emission of organic ligands[19-21].
Herein, we report a new MOF, which was constructed with 1, 1′-ethylbiphenyl-3, 3′, 5, 5′-tetracarboxylic acid (H4L), 4, 4′ - bipyridine (4, 4′ - bpy) as well as Zn ion, namely [Zn(H2L)(4, 4′-bpy)]n (1). It has good stability and fluorescence properties in water and can be used as a highly sensitive and selective fluores- cence probe to detect TET with a detection limit of 0.17 µmol·L-1. In addition, the fluorescence quench- ing mechanism of 1 is also discussed in detail.
1. Experimental
1.1 Reagents and instruments
All reagents and solvents were commercially avail- able and used directly without further purification. The C, H, and N elemental analyses were conducted with a PerkinElmer PE - 2400 elemental analyzer. The crystal data were collected on a Bruker SMART APEX -Ⅱ sin- gle-crystal X-ray diffractometer. Powder X- ray diffrac- tion (PXRD) patterns were recorded with a Bruker D8 ADVANCE diffractometer operating at 40 kV and 40 mA using Cu Kα radiation (λ=0.154 18 nm) at a scan- ning rate of 2 (°)·min-1 from 5° to 50°. Thermal gravi- metric analysis (TGA) was performed with a NETZSCH STA 449F3 thermal gravimetric analyzer in flowing nitrogen at a heating rate of 10℃·min-1. The UV -Vis spectra were measured using a UV - 2700 spectropho- tometer. Fluorescence experiments were carried out on a Hitachi F-7100 Fluorescence Spectrophotometer.
1.2 Synthesis of MOF 1
A mixture of Zn(NO3)2·6H2O (0.1 mmol, 0.029 7 g), H4L (0.05 mmol, 0.017 9 g), and 4, 4′ - bpy (0.05 mmol, 0.007 8 g) were dissolved in a mixed solvent of DMF (3 mL), H2O (3 mL), and HNO3 (0.1 mL, 6 mol· L-1). And then the mixed solution was placed in a 10 mL glass bottle and reacted at 95 ℃ for 3 d. Finally, colorless bulk transparent crystals were obtained. Yield: 47% (based on Zn). Anal. Calcd. for C28H20N2O8Zn(%): C, 58.15; H, 3.46; N, 4.85. Found (%): C, 58.21; H, 3.45; N, 4.64.
1.3 Crystal structure determination
The crystal with regular shape and moderate size was selected, and the single crystal data of 1 were col- lected on the Bruker SMART APEX -Ⅱ diffractometer (Mo Kα radiation and λ=0.071 073 nm). The diffrac- tion data were corrected by semi - empirical absorption using the SADABS program. The crystal structure was solved using direct methods and then refined by the full-matrix least-squares techniques on F 2 using SHELXL. All non -hydrogen atoms were refined aniso- tropically. The crystallographic data of MOF 1 is shown in Table 1. Selected bond lengths and bond angles are listed in Table 2.
Table 1
Parameter 1 Parameter 1 Formula C28H20N2O8Zn V / nm3 2.398 1(6) Formula weight 577.81 Z 4 Crystal system Monoclinic Dc / (g·cm-3) 1.595 Space group C2/c F(000) 1 176 a / nm 2.029 1(3) Goodness-of-fit (on F2) 1.021 b / nm 1.0105 5(14) R1, wR2 [I > 2σ(I)] 0.038 5, 0.092 5 c / nm 1.419 233(19) R1, wR2 (all data) 0.049 1, 0.098 4 β / (°) 124.508(2) Table 2
Zn1—O1 0.197 93(16) Zn1—O1A 0.197 93(16) Zn1—N1 0.207 03(18) Zn1—N1A 0.207 04(18) O1—Zn1—O1A 13.803(11) O—Zn1—N1 10.786(7) O1A—Zn1—N1 9.937(7) O—Zn1—N1A 9.937(7) O1A—Zn1—N1A 10.786(7) N1—Zn1—N1A 9.807(10) Symmetry code: A: 1-x, y, 0.5-z. CCDC: 2212375, 1.
2. Results and discussion
2.1 Crystal structure
MOF 1 crystallizes in the monoclinic crystal sys- tem with the C2/c space group. The asymmetric unit of 1 consists of one Zn(Ⅱ) ion, one H2L2- ligand, and one 4, 4′-bpy ligand. As shown in Fig. 1a, each Zn(Ⅱ) is fourcoordinated by two O atoms (O1, O1A) from two different H2L2- ligands, two nitrogen atoms (N1, N1A) from 4, 4′ - bpy ligands. All the Zn—O (0.197 93 (16) nm) and Zn —N (0.207 03(18) - 0.207 04(18) nm) bond lengths fall into the normal ranges (Table 2). As shown in Fig. 1b, the single crystal structure analysis shows that H2L2- ligands adopt monodentate coordination mode, connecting with Zn(Ⅱ) to form 1D chains. Finally, the 1D chains are connected by 4, 4′-bpy to form a 2D wavelike network.
Figure 1
Figure 1. (a) Ellipsoid diagram of the molecular structure of MOF 1; (b) 2D wavelike network of 150% ellipsoid probability; Symmetry codes: A: 1-x, y, 0.5-z; B: 0.5-x, 0.5-y, 1-z; C: 0.5-x, 0.5-y, -z; D: 0.5-x, 0.5-y, -1-z; E: x, y, -1-z; F: x, y, 1+z; G: 1.5-x, 0.5-y, 2-z; H: 1.5-x, 0.5-y, 1-z; I: 1.5-x, 0.5-y, -z; J: 1+x, y, z; K: 1+x, y, 1+z; L: 1+x, y, 2+z
2.2 Thermal stability
To identify the thermal stability of MOF 1, the TGA was performed. As shown in Fig. 2, the weight loss of 1 was 12.1% before 110 ℃, which corresponds to the release of the free water. The 2D networks started to decompose upon further heating up to about 400 ℃.
Figure 2
2.3 Purity and skeleton stability
To confirm the purity of MOF 1, the PXRD pattern of 1 was measured. The position of the diffraction peak in the PXRD experiment was consistent with those of single crystal structure simulation, implying the pure phase of 1 (Fig. 3). The skeleton is basically unchanged when 1 was immersed in acidic and basic aqueous solutions for 24 h, indicating that 1 has good acid and alkali resistance (Fig. 4).
Figure 3
Figure 4
2.4 Photoluminescence property
Due to the excellent luminescence properties of d10 metal MOFs, the luminescence of 1 and the H4L ligand were investigated. As shown in Fig. 5, H4L had an emission peak at 444 nm (λex=362 nm). Compared to the fluorescence spectrum of the ligand, the fluores- cence intensity of 1 was stronger than that of the ligand, which may be due to coordination interactions[22]. The emission spectrum of 1 had a partial redshift, which may be caused by the charge transfer between H4L and Zn(Ⅱ)[23].
Figure 5
2.5 Antibiotics sensing
The wanton use of antibiotics has caused great pollution to the water system and environment. Therefore, it is very urgent for us to find a simple and efficient method to detect antibiotics[24]. Therefore, the luminescence sensing of 1 for different antibiotics was investigated, including lincomycin hydrochloride (LIN), metronidazole (MDZ), ornidazole (ODZ), TET, roxithromycin (ROX), chloramphenicol (CAP), gentamicin sulfate (GEN), azithromycin (AZM), cefixime (CEF) and penicillin sodium (PEN). As shown in Fig. 6a, when TET was added, the fluorescence of 1 showed the maximum quenching. In the presence of other antibiotics, anti - interference experiments were carried out for TET. The experimental results showed that the fluorescence of 1 was also quenched to a large extent when TET was added in the presence of other antibiotics (Fig. 6b). Subsequently, the quantitative experiment of TET was carried out. When the concentration of TET increased, the fluorescence intensity of 1 gradually decreased. When the concentration of TET reached 250 µmol·L-1, the quenching efficiency of TET was as high as 97.97% (Fig. 6c). And I0/I value was also linearly correlated with a low TET concentration (Fig. 6d). The detection limit was calculated using 3σ/k (σ: standard deviation, k: slope), and the detection limit for 1 towards TET was 0.17 µmol·L-1. In addition, after four cycles, we found that the fluorescence intensity could still be restored to the original intensity. 1 may be a recyclable fluorescent sensor (Fig. 6e). It was found that when TET of 250 µmol·L-1 was added, the luminescence intensities decreased rapidly and the fluorescence hardly changed after 20 s (Fig. 6f).
Figure 6
Figure 6. (a) Luminescent intensity of 1 in different antibiotics; (b) Luminescence intensity of 1 in mixed antibiotics; (c) Emission spectra of 1 with different concentrations of TET; (d) Stern-Volmer plot for MOF 1 detecting TET in low concentration; (e) Cycle stability of 1 for the detection of TET (red square: 1, blue square: 1 + TET); (f) Effect of response time on the fluorescent intensities upon the addition of TET2.6 Possible sensing mechanism
The reasons for fluorescence quenching that have been reported are as follows: (Ⅰ)the collapse and disintegration of the crystal framework, the mechanism of energy competition and absorption, the exchange of central metal ions, the mechanism of energy transfer, the mechanism of photoinduced electron transfer (PET)[25-31]. First of all, as shown in Fig. 7, PXRD patterns of 1 were consistent with as-synthesized samples immersed in TET solution for 24 h, indicating that the crystal structure was intact. Therefore, framework collapse is not the reason for fluorescence quenching. Secondly, because 1 detects antibiotics, it indicates that there is no metal ion exchange during fluorescence quenching. Another possible mechanism is energy allocation and transfer. We can see that there is a partial overlap between the emission spectrum of 1 and the UV absorption (300-400 nm) spectrum of TET (Fig. 8). The reason for the fluorescence quenching of 1 may be due to energy absorption and energy transfer. Finally, the LUMO level of TET (-2.72 eV) is lower than 1 (Fig. 9). The reason for fluorescence quenching may be that the electron transfers from the LUMO level of 1 to TET. At the same time, I0/I value was also linearly correlated with low TET concentration (Fig. 6d), indicating that the mechanism for fluorescence quenching should be more than one. When the concentration is low, it is linear, indicating that the competitive absorption is weak. With the increase in concentration, it is nonlinear, and the absorption also increases[32-34].
Figure 7
Figure 8
Figure 9
2.7 Practical application in Yanhe River water
To prove the practicability of this method, TET was tested in Yanhe River water through the spiked recovery experiment. As shown in Table 3, the spiked recoveries at different concentrations were obtained, ranging from 94% to 103%. The relative standard deviation (RSD) values were 1.7% - 2.4%, indicating the reliability and practicability of 1 to detect TET in real samples.
Table 3
Spiked /(µmol·L-1) Detected /(µmol·L-1) RSD* / % Recovery / % 0 Not detected — — 5 4.7 1.7 94 15 15.1 1.9 101 30 30.8 2.4 103 *n=3 3. Conclusions
In summary, a Zn-MOF (1) is successfully synthe- sized under solvothermal conditions. Structural analysis shows that 1 is a 2D wavelike network. It has high selectivity and sensitivity for the detection of TET by fluorescence quenching. Through the spiked recovery experiment, TET in the actual water samples along the river can also be detected. Finally, the sensing mechanism is discussed in detail. The cause of TET quenching might be energy resonance transfer or electron transfer.
Conflicts of interest: The authors declare no competing financial interest.
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[1]
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Figure 1 (a) Ellipsoid diagram of the molecular structure of MOF 1; (b) 2D wavelike network of 1
50% ellipsoid probability; Symmetry codes: A: 1-x, y, 0.5-z; B: 0.5-x, 0.5-y, 1-z; C: 0.5-x, 0.5-y, -z; D: 0.5-x, 0.5-y, -1-z; E: x, y, -1-z; F: x, y, 1+z; G: 1.5-x, 0.5-y, 2-z; H: 1.5-x, 0.5-y, 1-z; I: 1.5-x, 0.5-y, -z; J: 1+x, y, z; K: 1+x, y, 1+z; L: 1+x, y, 2+z
Figure 6 (a) Luminescent intensity of 1 in different antibiotics; (b) Luminescence intensity of 1 in mixed antibiotics; (c) Emission spectra of 1 with different concentrations of TET; (d) Stern-Volmer plot for MOF 1 detecting TET in low concentration; (e) Cycle stability of 1 for the detection of TET (red square: 1, blue square: 1 + TET); (f) Effect of response time on the fluorescent intensities upon the addition of TET
Table 1. Crystal data and structure refinement parameters for 1
Parameter 1 Parameter 1 Formula C28H20N2O8Zn V / nm3 2.398 1(6) Formula weight 577.81 Z 4 Crystal system Monoclinic Dc / (g·cm-3) 1.595 Space group C2/c F(000) 1 176 a / nm 2.029 1(3) Goodness-of-fit (on F2) 1.021 b / nm 1.0105 5(14) R1, wR2 [I > 2σ(I)] 0.038 5, 0.092 5 c / nm 1.419 233(19) R1, wR2 (all data) 0.049 1, 0.098 4 β / (°) 124.508(2) Table 2. Selected bond lengths (nm) and angles (°) for 1
Zn1—O1 0.197 93(16) Zn1—O1A 0.197 93(16) Zn1—N1 0.207 03(18) Zn1—N1A 0.207 04(18) O1—Zn1—O1A 13.803(11) O—Zn1—N1 10.786(7) O1A—Zn1—N1 9.937(7) O—Zn1—N1A 9.937(7) O1A—Zn1—N1A 10.786(7) N1—Zn1—N1A 9.807(10) Symmetry code: A: 1-x, y, 0.5-z. Table 3. Recovery test of TET spiked in Yanhe River water samples
Spiked /(µmol·L-1) Detected /(µmol·L-1) RSD* / % Recovery / % 0 Not detected — — 5 4.7 1.7 94 15 15.1 1.9 101 30 30.8 2.4 103 *n=3 -
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