Citation: Ling-Bin ZHU, Fei LI, Ming-Ling SUN, Ye-Yan QIN, Yuan-Gen YAO. Three New Isostructural Metal-organic Coordination Polymers from Triangular Pyridinedicarboxylate Ligand: Syntheses, Structures and Properties[J]. Chinese Journal of Structural Chemistry, ;2021, 40(8): 1031-1038. doi: 10.14102/j.cnki.0254–5861.2011–3078 shu

Three New Isostructural Metal-organic Coordination Polymers from Triangular Pyridinedicarboxylate Ligand: Syntheses, Structures and Properties

  • Corresponding author: Yuan-Gen YAO, yyg@fjirsm.ac.cn
  • Received Date: 25 December 2020
    Accepted Date: 5 February 2021

    Fund Project: the National Natural Science Foundation of China 21703247the Science Foundation of Fujian Province 2018J05029the Science Foundation of Fujian Province 2019J05156the Science Foundation of Fujian Province 2019H0053

Figures(6)

  • Three new isostructural coordination polymers, namely, [Mg(cpna)(H2O)2]n (1), [Mn(cpna)(H2O)2]n (2) and [Co(cpna)(H2O)2]n (3) (H2cpna = 5-(3-carboxylphenyl)nicotic acid) are reported. They were synthesized by hydrothermal reactions of transition metal or alkaline earth metal chloride with 5-(3-carboxylphenyl)nicotic acid, respectively. Complexes 1~3 exhibit 2D layers with a 3, 3-connected topology with Schläfli symbol {4.82}. Such layers including hexagonal rings and a quadrangular ring are further extended into an ordered 3D framework by hydrogen bonds between the cpna2- ligands and water molecules. The rare complex 1 has excellent luminescence and can be used as luminescent materials, while 2 and 3 possess prominent magnetism with potential applications in magnetic materials.
  • Functional coordination chemistry is based on molecular basis, and molecular design and assembly are used to construct functional coordination complexes. The potentials for use in photoelectricity[1], catalysis[2], adsorption[3-5], nonlinear optics[6] and magnetism[7] are also discussed. In recent years, with the improvement of synthesis and measurement technology, the theory of crystallography has become more and more mature. The simple nitrogencontaining ligands and their derivatives such as imidazole and triazole have not been able to meet the needs of developing new complexes. It is noted that much attention has been paid to the coordination polymers that are assembled by polycarboxylic acids and N-heterocyclic ligands. The spacer of these aromatic multi-carboxylate ligands sometimes plays an important role in forming the final structure of the molecule due to their varied coordination capability[8]. For example, Liang et al. synthesized a heterometal complex {[Gd2Cu3(pydc)6(H2O)]·4H2O}n by reacting 2, 5-pyridinedicarboxylic acid with copper and rare earth metal ions under hydrothermal conditions[9], and Lahoud et al. used 1H-pyrazole-3, 5-dicarboxylicacid and various rare earth metal ions to synthesize rare earth complexes[10]. However, studies engaged in 5-(3-carboxylphenyl)nicotic acid are less[11-14]. We delved into the construction and properties of the complexes derived from pyridyl carboxylic ligands. Due to the coordination of metals and ligands, the emission wavelength of organic ligand will be significantly affected. Therefore, the luminescent properties can be controlled by changing metal ions, organic ligands, synthetic methods and conditions, etc., so that a specific luminescent material can be obtained[15]. By means of crystal engineering, one can obtain a coordination polymer with improved magnetic properties or other useful properties by controlling the position and connection of the spin-bearing left magnetic properties or other useful properties by controlling the position and connection of the spin-bearing left[13].

    In this work, we have been continuing our efforts in the self-assembly and characterization of new metal assemblies based on 5-(3-carboxylphenyl)nicotic acid ligand. H2cpna contains both nitrogen and carboxylate groups and can be used in a variety of coordination modes. Since the polycarboxylic groups can be deprotonated in whole or in part, they can serve as a donor or acceptor of a hydrogen bond, contributing to the formation of a supramolecular structure. In recent years, compared with transition metals and rare earth metals, MOFs based on alkaline earth metal construction have also been reported, but there are still few, so not only the transition metal salt (Co2+ and Mn2+) but also the alkaline earth metal salt (Mg2+) were used to synthesize complexes with the ligand H2cpna.

    Herein, we report the successful self-assembly of three new isostructural complexes: Mg(cpna)(H2O)2 (1), Mn(cpna)(H2O)2 (2), and Co(cpna)(H2O)2 (3), which exhibit 2-fold structures with a short symbol of {4.82} and then extend into 3D frameworks by hydrogen bonds. Since these three complexes are isostructural, we only list the molecular structural formula of complex 1 as a representative (Scheme 1). All complexes were characterized by single-crystal X-ray diffraction, topological analyses, infrared spectra, elemental analyses and thermogravimetric analyses. In addition, the photo-luminescence of complex 1 was discussed in detail, while magnetic properties of complexes 2 and 3 were also studied.

    Scheme1

    Scheme1.  Cordination mode of cpna2- in complex 1

    All raw materials were purchased through commercial channels and not purified. Elemental analyses (C, H, N) were measured on an EA1110 CHNS-0 CE elemental analyzer. Infrared spectroscopy was performed on a Nicolet Magna 750 FT-IR spectrometer with KBr pellets at 400~4000 cm-1. Powder X-ray diffraction data (PXRD) were collected on a Rigaku MiniFlex Ⅱ diffractometer with Cu radiation (λ = 1.54056 Å). Thermal gravimetric analyses (TGA) were determined on a NETSCHZ STA-449C thermal analyzer from room temperature to 800 ℃ under nitrogen atmosphere at a heating rate of 10 ℃·min. The luminescence spectra were measured on a FLS920 luminescence spectrophotometer at room temperature by powdered solid samples. The magnetic measurements were made with a commercial quantum design physical property measurement system (PPMS).

    2.1.1   Synthesis of [Mg(cpna)(H2O)2]n (1)

    MgCl2·2.5H2O (0.046 g, 0.2 mmol) and H2cpna (0.049 g, 0.2 mmol) were dissolved in 8 mL of deionized water, then 10 uL of acetonitrile was added, stirred for 30 minutes, placed in a 25 mL stainless-steel autoclave lined with polytetrafluoroethylene tubes, and crystallized at 140 ℃ for 90 h. Then, it was cooled to room temperature, and the crystals were filtered and washed with distilled water. It was cooled to obtain a pure phase of colorless rod crystals of 2 in a yield of 58% (by Mg). Anal. Calcd. for C13H11MgNO6: C, 51.78; H, 3.68; N, 4.65%. Found: C, 51.31; H, 3.82; N, 4.33%. IR (KBr pellet, cm-1): 3374(m), 3294(m), 3080(m), 2900(s), 1615(s), 1544(s), 1425(s), 1377(s), 917(m), 863(m), 768(s), 712(s), 419(m).

    2.1.2   Synthesis of [Mn(cpna)(H2O)2]n (2)

    The synthesis method of complex 2 is the same as that of 1, except that MgCl2·2.5H2O is replaced by MnCl2·4H2O. It was cooled to obtain a pure phase of white rod crystals of 2 in a yield of 49% (by Mn). Anal. Calcd. for C13H11MnNO6: C, 47.01; H, 3.34; N, 4.22%. Found: C, 47.05; H, 3.30; N, 4.18%. IR (KBr pellet, cm-1): 3349(m), 3238(m), 3088(m), 1615(s), 1615(s), 1409(s), 1369(s), 871(m), 775(m), 704(s), 585(m), 427(m).

    2.1.3   Synthesis of [Co(cpna)(H2O)2]n (3)

    The synthesis method of complex 3 is the same as that of complex 1, except that MgCl2·2.5H2O is replaced by CoCl2·4H2O. It was cooled to obtain a pure phase of red rod crystals of 3 in 52% yield (by Co). Anal. Calcd. for C13H11CoNO6: C, 46.45; H, 3.30; N, 4.17%. Found: C, 46.66; H, 3.35; N, 4.12%. IR (KBr pellet, cm-1): 3373(m), 3254(m), 3104(m), 1615(s), 1552(s), 1432(s), 1377(s), 847(m), 767(s), 712(s), 569(s), 427(s).

    Crystal data, data collection and structure refinement details are summarized in Table 1. The data were collected using a computer-controlled Oxford Xcalibur E diffractometer with graphite-monochromatic Mo radiation (λMo = 0.71073 Å) at 298(2) K. The final unit cell parameters were derived by global refinements of reflections obtained from integration of all the frame data. Empirical absorption corrections were applied using the SADABS program. The structure was solved by direct methods using the SHELXS program and refined by full-matrix least-squares techniques SHELXL on F2[16]. Hydrogen atoms were located using the geometric method. Non-hydrogen atoms were refined with anisotropic thermal parameters. The SQUEEZE option of PLATON could eliminate disordered guest molecules[17].

    Table 1

    Table 1.  Summary of Crystal Data and Structure Refinements for 1~3
    DownLoad: CSV
    1 2 3
    Chemical formula C13H11MgNO6 C13H11MnNO6 C13H11CoNO6
    Mr 301.54 332.17 336.16
    Crystal system, space group Monoclinic, P21/c Monoclinic, P21/c Monoclinic, P21/c
    a, b, c (Å) 13.4566(4), 11.8575(4), 7.7031(3) 13.5539(4), 11.9453(3)7.8035(2) 13.3887(5), 11.8184(5)7.7360(3)
    β (°) 98.186(3) 98.510(3) 98.246(4)
    Z 4 4 4
    Radiation type Mo Mo Mo
    V3) 1216.60(7) 1249.52(6) 1211.44(8)
    µ (mm-1) 0.18 1.09 1.45
    Crystal size (mm) 0.25 × 0.12 × 0.07 0.19 × 0.10 × 0.07 0.25 × 0.10 × 0.08
    Tmin, Tmax 0.975, 0.988 0.878, 0.927 0.841, 0.891
    No. of measured, independentand observed 5011, 2383, 1813 4847, 2544, 2270 5037, 2511, 2229
    Rint 0.027 0.026 0.025
    (sinθ/λ)max-1) 0.645 1.356 0.680
    R (F2 > 2σ(F 2))a, wR(F2)b, S 0.042, 0.101, 1.071 0.048, 0.146, 1.065 0.047, 0.151, 1.030
    No. of reflections 2383 2480 2509
    No. of parameters 196 192 199
    No. of restraints 0 0 0
    H-atom treatment H atoms treated by a mixture of independent and constrained refinement H-atom parameters constrained H atoms treated by a mixture of independent and constrained refinement
    Δρmax, Δρmin (e·Å−3) 0.32, –0.34 0.46, –0.61 1.22, –0.43
    aR = Σ||Fo| – |Fc||/Σ|Fo|, bwR = [Σ[w(Fo2Fc2)2]/Σw(Fo2)2]1/2

    Single-crystal X-ray diffraction reveals that complexes 1~3 are all isostructural. They crystallize in monoclinic space group P21/c. For the sake of simplicity, herein, we only describe the structure of complex 1 in detail, and other structures of complexes are shown in Fig. S1. As shown in Fig. 1, unit of 1 includes an independent Mg2+ left, a fully deprotonated H2cpna ligand, and two water molecules. All Mg(Ⅱ) ions in 1 are equivalent, and the coordination environment around the central Mg(Ⅱ) ion is shown in Fig. 2. The central Mg(Ⅱ) ion is in a slightly distorted octahedral coordination sphere, coordinating with one nitrogen atom (N(1)) and three oxygen atoms (O(1), O(2), O(3)) from three different cpna molecules (Mg−N(1) 2.239(2) Å, Mg(1)−O(1)2.208(2) Å, Mg(1)−O(2) 2.161(2) Å and Mg(1)−O(3) 2.024(3) Å) and with two oxygen atoms (O(1W), O(2W)) from two H2O molecules (Mg(1)−O(1W) 2.086(4) Å and Mg(1)−O(2W) 2.043(8) Å). All bonds are consistent with the literature reports[18]. The L−Mg(1)−L (L = O, N) bond angles range from 88.36(7)° to 174.47(8)°, which are listed in Table 2 in detail. The H2cpna ligand removes hydrogen from the two carboxyl groups during coordination process and bridge two Mg(Ⅱ) ions and displays two coordination modes (μ2-η1: η1 and μ1-η1: η0). Owing to the coordination of cpna2- ligands with Mg2+ metal, both the pyridyl and phenyl rings in the cpna2- ligands are distorted and the dihedral angle between two aromatic rings of the cpna2- is 25.62° (Fig. 2a). In the asymmetric unit 1, the two cpna2- ligands adopt a µ3-η1: η1: η1 bridging mode to connect two neighboring Mg(Ⅱ) ions, fabricating a coplanar quadrangular ring, and four Mg(Ⅱ) are linked by four cpna2- ligands to form a non-planar octagonal boat-like ring. Both quadrangular rings and octagonal rings are spaced apart to result in a unique 2D network layer (Fig. 2b).

    Table 2

    Table 2.  Selected Bond Lengths (Å) and Bond Angles (°) for Complex 1
    DownLoad: CSV
    Bond Dist. Bond Dist. Bond Dist.
    Mg(1)−O(3) 2.0243(16) Mg(1)−O(2W) 2.0438(19) Mg(1)−O(1W) 2.0864(18)
    Mg(1)−O(2) 2.1611(17) Mg(1)−O(1) 2.2082(15) Mg(1)−N(1) 2.239(2)
    Angle (°) Angle (°) Angle (°)
    O(3)−Mg(1)−O(2W) 91.80(8) O(3)−Mg(1)−O(1W) 90.16(7) O(2W)−Mg(1)−O(1W) 174.47(8)
    O(3)−Mg(1)−O(2) 88.36(7) O(2W)−Mg(1)−O(2) 92.25(7) O(1W)−Mg(1)−O(2) 92.97(7)
    O(3)−Mg(1)−O(1) 148.21(7) O(2W)−Mg(1)−O(1) 92.27(7) O(1W)−Mg(1)−O(1) 88.77(7)
    O(2)−Mg(1)−O(1) 59.99(6) O(3)−Mg(1)−N(1) 122.54(7) O(2W)−Mg(1)−N(1) 85.12(8)
    O(1W)−Mg(1)−N(1) 89.46(7) O(2)−Mg(1)−N(1) 149.01(6) O(1)−Mg(1)−N(1) 89.22(6)
    Symmetry codes: (ⅰ) x+1, –y+1/2, z+1/2; (ⅱ) –x, –y+1, –z

    Figure 1

    Figure 1.  Perspective view of the coordination environment of the Mg(Ⅱ) atom in 1 with 50% thermal ellipsoids.Symmetry codes: (ⅰ) x+1, –y+1/2, z+1/2; (ⅱ) –x, –y+1, –z; (ⅲ) x–1, –y+1/2, z–1/2

    Figure 2

    Figure 2.  (a) Dihedral angle between two aromatic rings of the cpna2- is 25.62°. (b) A polyhedral view of the 2D layer structure. (c) View of topological (4.82) net of the 2D layer. (d) 3D supramolecular framework constructed by hydrogen bonds

    In order to more directly understand the framework of complex 1, we apply the method of topology analysis to reduce the multidimensional structure to simple nodes and linkers. Each cpna2- is connected to three Mg(Ⅱ) ions and each Mg2+ is surrounded by three cpna2- liands, so both cpna2- and Mg2+ can be simplified as 3-connected nodes. The overall structure of 1 can be rationalized as a 3, 3-connected topology with Schläfli symbol {4.82} (Fig. 2c).

    Interestingly, the 2D layers are extended into an ordered 3D framework by hydrogen bonds between the cpna2-ligands (C(11)–H(11)⋯O(4): 3.284(3) Å, 145°), in which C atoms are from the pyridyl rings and O atoms are from the uncoordinated carboxylate groups of cpna2– ligands, as well as a hydrogen bond (O(1W)–H(1WB)⋯O(2): 2.841(2) Å, 153°; O(2W)–H(2WB)⋯O(2): 2.740(2) Å, 169°; O(1W)– H(1WA)⋯O(4): 2.833(2) Å, 141°; O(2W)–H(2WA)⋯O(4): 2.736(2) Å, 151°) between the coordinating water molecules and ligands, in which O atoms are from coordination water molecules and carboxylate groups of cpna2- ligands, respectively (Fig. 2d). The detailed hydrogen bonds are listed in Table 3.

    Table 3

    Table 3.  Hydrogen Bonds for Complex 1 (Å and °)
    DownLoad: CSV
    D–H···A D–H H···A D···A D–H···A
    O(1W)–H(1WA)···O(4) 0.86 2.11 2.833(2) 141
    O(1W)–H(1WB)···O(2) 0.86 2.04 2.841(2) 153
    O(2W)–H(2WA)···O(4) 0.85 1.96 2.736(2) 151
    O(2W)–H(2WB)···O(2) 0.81 1.95 2.740(2) 169
    C(7)–H(7)···O(1) 0.93 2.41 3.034(3) 124
    C(11)–H(11)···O(4) 0.93 2.48 3.284(3) 145
    Symmetry codes: (ⅱ) –x+1, –y, –z; (ⅳ) –x+1, y–1/2, –z–1/2; (ⅴ) x, 1/2–y, –1/2+z; (ⅵ) 1–x, –1/2+y, 1/2–z; (ⅶ) x, 1/2–y, 1/2+z; (ⅷ) –x, –1/2+y, –1/2–z

    The infrared spectra of complexes 1~3 show that the characteristic peaks of water molecule O–H are in the range of 3500~3300 cm-1: 3374 cm-1 (1), 3349 cm-1 (2) and 3373 cm-1 (3). The absorption of phenyl ring hydrocarbon (At–H) is in the range of 3200~3000 cm-1: 3080 cm-1 (1), 3088 cm-1 (2) and 3104 cm-1 (3). When the carboxyl group is coordinated with metal, the proton is removed, and the characteristic peak of the group disappears in the range of 1725~1700 cm-1, as well as the characteristic absorption peaks of COO- in the 1650~1440 cm-1 region: 1615 cm-1, 1544 cm-1 (1), 1615 cm-1, 1522 cm-1 (2), 1615 cm-1, 1552 cm-1 (3) (Fig. S2). The above analyses are consistent with the X-ray diffraction results.

    In order to better study the various properties of the complexes, their purity need to be characterized firstly. We performed powder X-ray diffraction (XRD) analyses on the three complexes synthesized, and found the XRD patterns of complexes 1~3 obtained by experiment are basically consistent with the simulated ones (Fig. S3-Fig. S5). The purity of these three complexes is high, and the related properties of them can be studied.

    Complexes 1~3 are stable in air and maintain stable crystalline states at room temperature. To investigate the thermal stabilities of complexes 1~3, we performed thermogravimetric analysis (TG). The thermal decomposition plots of compounds 1~3 are shown in Fig. S6. Complex 1 was thermal stable up to 102 ℃, then lost 12.1% between 102 and 237 oC, corresponding to the decomposition of two H2O molecules (calculated 11.9%). After that the H2cpna ligands begin to decompose. The weight loss curves of complexes 2 and 3 are similar to 1. In 2, the departure of the coordinated water molecules of complex 2 occurs from 121 to 200 oC (observed 10.8%, calculated 11.1%). Complex 3 loses two coordinated water molecules in 125~210 ℃ with the weight loss of 10.5% (calculated 10.7%).

    Fluorescent coordination polymers (L-CPs) have attracted much attention due to their wide application prospects in lighting, sensing, and biological imaging[19, 20]. The researches on transition metal-based L-CPs based on rare earth ions and d10 electronic configuration is the most[21]. The special closed-shell electronic configuration of Mg(Ⅱ) is coordinated with organic ligands without the loss of light energy caused by d-d transitions. It is very suitable for the construction of L-CPs based on the luminescence mechanism of organic ligands.

    Luminescent properties of complex 1 at room temperature have been studied. It can be seen from Fig. 3, when excited at 275 nm, the free ligand H2cpna and complex 1 have the largest emission peaks at 392 and 338 nm, respectively. According to literature reports, the luminescence of H2cpna ligands can be attributed to the transition of n→π*/ππ* within ligands[21]. It can also be seen from Fig. 3 that when the ligands form complex 1 with Mg ions, the emission intensity of 1 relative to the ligand is enhanced due to the increased rigidity of the ligand after coordinating with Mg2+, which reduces the loss of non-radiative energy[22, 23]. At the same excitation wavelength (ex = 275 nm), the largest fluorescence emission peak of complex 1 is 338 nm. Compared to the free H2cpna, the luminescence of complex 1 has certain blue shifts, resulting from the ligand lefted charge transfer. It can also be concluded that the energy transfer process and phonon dynamics within the scintillators take place mainly in the same luminescence centre species, so the emission spectra of 1 remained similar when excited either by ionizing radiation or by nonionizing irradiation[24, 25].

    Figure 3

    Figure 3.  Emission spectra of H2cpna and complex 1

    The magnetic susceptibility measurements for compounds 2 and 3 were performed with polycrystalline samples from 300 to 2 K under an applied field of 1000 Oe. For 2, the χmT value is 4.36 cm3·mol–1· K at room temperature, which is very close to the value of 4.375 cm3·mol–1 K for an isolated Mn(Ⅱ) ion with g = 2.0. Upon cooling, the χmT remains constant to about 30 K, after which it decreases abruptly to a minimum value of 3.42 cm3·mol–1·K at 2 K, indicating the paramagnetic behavior. The paramagnetic behavior in 2 is also suggested by the very small Weiss constant θ = −0.25 K, obtained from the data of χm-1 νs. T in the temperature range of 20~300 K by Curie-Weiss law (Fig. 4). For 3, the experimental χmT value at 300 K is 3.39 cm3·mol–1·K, which is larger than that expected for non-interacting high-spin Co(Ⅱ) ions (1.88 cm3·mol–1·K with g = 2.0). This divergence suggests that the orbital contribution of octahedral Co(Ⅱ) ions is involved. After further cooling, the χmT decreases continuously and reaches a minimum value of 1.80 cm3·mol–1·K at 2 K. From 2 to 300 K, the χm follows the Curie-Weiss law giving θ = –4.87 K and C = 3.45 cm3·mol–1·K (Fig. 5). Considering the structure of 3, the negative Weiss constant may be caused by the spin-orbital coupling together with the zero-field splitting.

    Figure 4

    Figure 4.  χmT and χm-1 νs. T curves measured under an applied field 1000 Oe for 2

    Figure 5

    Figure 5.  χmT and χm-1 νs. T curves measured under an applied field of 1000 Oe for 3

    In summary, we synthesized three novel isostructural complexes, namely, Mg(cpna)(H2O)2 (1), Mn(cpna)(H2O)2 (2) and Co(cpna)(H2O)2 (3), based on 5-(3-carboxylphenyl) nicotic acid (H2dcpa) under hydrothermal conditions. Although the metal lefts are different in three complexes, they exhibit the same structures because they are carried out under the same reaction conditions. Interestingly, all of them exhibit 2D layered structures with a short symbol of {4.82} topology and ultimately stretch into 3D frameworks by hydrogen bonds. In addition, we have characterized the properties of these complexes. The rare complex 1 has excellent luminescence and it can be used as a potential luminescent material, while complexes 2 and 3 have pronounced magnetism and may be utilized as magnetic materials.


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