Structure and magnetic properties of Mn(Ⅱ) coordination polymers regulated by N-auxiliary ligands

Xiaxia LIU Xiaofang MA Luxia GUO Xianda HAN Sisi FENG

Citation:  Xiaxia LIU, Xiaofang MA, Luxia GUO, Xianda HAN, Sisi FENG. Structure and magnetic properties of Mn(Ⅱ) coordination polymers regulated by N-auxiliary ligands[J]. Chinese Journal of Inorganic Chemistry, 2025, 41(3): 587-596. doi: 10.11862/CJIC.20240269 shu

通过含氮辅助配体调节的锰(Ⅱ)配位聚合物的结构和磁性质

  • 基金项目:

    国家自然科学基金 21671124

摘要: 以Mn(Ⅱ)离子和6-(3′, 4′-二羧基苯氧基)-1, 2, 4-苯三羧酸(H5L)为原料, 在1, 10-菲咯啉(phen)和1, 4-双(1H-咪唑-1-基)苯(1, 4-bib)含氮辅助配体存在下通过水热法制备了2个新型锰配位聚合物{[Mn2(HL)(phen)3(H2O)2]·7.5H2O}n (1)和[Mn4(HL)2(1, 4-bib)3(H2O)2]n (2)。利用红外光谱、单晶X射线衍射、热重分析和粉末X射线衍射等手段对配位聚合物12的结构进行表征。单晶X射线衍射结果表明, 1具有基于双核锰结构单元的一维链状结构, 2具有基于四核锰结构单元的(3, 8)-连接三维网络结构。磁性研究表明, 12的锰离子之间均表现为反铁磁相互作用。由于2的四核锰结构单元中Mn…Mn间距较短, 所以反铁磁相互作用较强。

English

  • In recent years, coordination polymers (CPs) designed and synthesized by metal ions and organic ligands have attracted extensive attention, because they are not only structurally diverse, but also display potential applications as functional materials in adsorption separation[1], magnetism[2], proton conduction[3], catalysis[4], and chemical sensing[5]. At present, there have been many studies on the structures and related properties of CPs. The results show that the preparation of CPs can be affected by many factors, including the coordination properties of metal ions[6], the structure of ligands[7], solvents[8], pH[9], temperature[10], and so on. Among them, the reasonable selection of the ligand is very important for the construction of target CPs. Especially in the design and synthesis of magnetic CPs, the selection of suitable bridging ligands can deliver magnetic interactions more efficiently. Semi-rigid polycarboxylate ligands combine the advantages of rigid and flexible ligands and have various coordination modes such as syn-syn, syn-anti, anti-anti, and μ-oxo, which can exhibit various ways of transferring magnetic interactions[11]. Besides, Mn(Ⅱ) ion with five unpaired electrons is often used to construct novel magnetic CPs. Several carboxylate-bridged Mn(Ⅱ) complexes with interesting magnetic properties have been reported[12-14].

    To synthesize new magnetic materials formed by manganese metal ions and semi-rigid polycarboxylic acid ligands, a semi-rigid polycarboxylic acid ligand, 6-(3′, 4′-dicarboxylphenoxy)-1, 2, 4-benzenetricarboxylic acid (H5L), was chosen for the following reasons: (1) two benzene rings can rotate freely by —O— group, which exhibit conformational flexibility; (2) five carboxyl groups of the ligand can be partially or completely deprotonated to form diverse coordination modes; (3) benzene rings can function as a mediator for transmitting exchange interaction between paramagnetic metal centers[15]. Furthermore, the mixed-ligands strategy is an effective method for assembling different types of CPs[16-17]. N-donor ligands are electroneutral and have simple coordination modes, which can satisfy the coordination geometry requirements of the metal ions in the assembly process by cooperative coordination with carboxylic acid groups[18-19].

    Hence, in this work, we employed H5L as polycarboxylate ligand, terminal ligand 1, 10-phenanthroline (phen) and bridging ligand 1, 4-bis(1H-imidazol-1-yl)benzene (1, 4-bib) as the auxiliary ligands to assemble two new Mn(Ⅱ) CPs, namely {[Mn2(HL)(phen)3(H2O)2]·7.5H2O}n (1) and [Mn4(HL)2(1, 4-bib)3(H2O)2]n (2) (Scheme 1). Complexes 1 and 2 exhibit different molecular structures and dimensionalities. The synthesis, structures, and magnetic properties of 1 and 2 are discussed in detail.

    Scheme 1

    Scheme 1.  Synthesis strategy for complexes 1 and 2

    H5L was obtained from Jinan Henghua Sci. & Tec. Co., Ltd. of China and used as received. All other solvents and materials used in the experiments were purchased commercially without any further purification. The FTIR spectra with KBr pellets were recorded in a range of 4 000-400 cm-1 on a Bruker TENSOR27 spectrometer. Elemental analyses (C, H, and N) were performed on an Elementar UNICUBE organic elemental analyzer. The powder X-ray diffraction (PXRD) patterns were measured on a Bruker D8 Advance instrument equipped with Cu radiation (λ=0.154 18 nm) at room temperature and collected from 5° to 50° with a scanning speed of 5 (°)·min-1. The operating voltage and current were 40 kV and 100 mA, respectively. Thermal stability analyses were performed on an SDT 650 thermal gravimetric analyzer from room temperature to 800 ℃ with a heating rate of 10 ℃·min-1 under N2 atmosphere. Magnetic susceptibility measurement data were obtained with a SQUID magnetometer (Quantum MPMS) in a temperature range of 2-300 K by using an applied field of 1 000 Oe.

    A mixture of Mn(CH3COO)2·4H2O (24.51 mg, 0.10 mmol), H5L (39.00 mg, 0.10 mmol), phen (18.02 mg, 0.10 mmol), and H2O (10 mL) was placed in a 15 mL Teflon-lined stainless steel vessel, and the pH of the reaction suspension was adjusted to 4 with HNO3 (1 mol·L-1). The mixture was heated to 120 ℃ and kept constant for 72 h. After cooling to room temperature, yellow bulk crystals of 1 were obtained, then washed with distilled water and dried in air. Yield: 35% (based on H5L). Elemental analysis Calcd. for C53H49Mn2 N6O20.50(%): C, 52.70; N, 6.96; H, 4.10; Found(%): C, 52.01; N, 6.75; H, 4.38. FTIR (KBr, cm-1): 3 418(s), 2 920(w), 1 599(s), 1 517(w), 1 425(w), 1 381(m), 1 261(w), 1 219(w), 1 102(w), 846(m), 782(w), 728(m) (Fig.S1, Supporting information).

    The preparation of complex 2 was similar to the preparation of 1, except that phen (18.02 mg, 0.10 mmol) was replaced by 1, 4-bib (21.00 mg, 0.10 mmol). Finally, colorless block crystals of 2 were collected by filtration and washed with distilled water. The yield of the product was 45% (based on H5L). Elemental analysis Calcd. for C35H23Mn2N6O12(%): C, 50.68; N, 10.13; H, 2.80; Found(%): C, 50.47; N, 9.93; H, 2.89. FT-IR (KBr, cm-1): 3 415(s), 2 921(w), 1 617(s), 1 563(w), 1 382(m), 1 312(w), 1 260(w), 1 225(w), 1 112(w), 780(w), 710(w), 622(w), 483(w) (Fig.S1).

    Single crystal X-ray data of complexes 1 and 2 were collected on a D8-Quest diffractometer equipped with Mo radiation (λ=0.071 073 nm), and the absorption correction of crystal diffraction data was carried out by using the SADABS program. The crystal skeletons of 1 and 2 were analyzed by the direct method using the Olex2 and SHELXL-2014. All non-hydrogen atoms and anisotropic parameters were refined by full-matrix least-squares on F 2. The H atoms were refined as follows: the H atoms attached to C atoms were positioned geometrically, while the hydrogen atoms of lattice water molecules were located in the difference Fourier maps, and the distances of the O—H bond were limited to 0.082 nm. For complex 1, some guest solvent molecules were found to be highly disordered, so they were removed by using the SQUEEZE option of PLATON. The detailed crystallographic data and structure refinement parameters of 1 and 2 are collected in Table 1, and selected bond lengths and angles of the complexes are given in Tables S1 and S2.

    Table 1

    Table 1.  Crystal data and structure refinement parameters for complexes 1 and 2
    下载: 导出CSV
    Parameter 1 2
    Empirical formula C53H38Mn2N6O15·5.5H2O C35H23Mn2N6O12
    Formula weight 1207.86 829.47
    T / K 294 295
    Crystal system Monoclinic Triclinic
    Space group C2/c P1
    a / nm 2.735 98(9) 1.117 3(3)
    b / nm 1.448 58(2) 1.120 2(3)
    c / nm 2.743 88(9) 1.448 7(4)
    α / (°) 91.511(9)
    β / (°) 97.155(2) 93.75(1)
    γ / (°) 117.544(9)
    V / nm3 10.790 1(3) 1.600 9(8)
    Z 8 2
    F(000) 4 984 842
    Dc / (g·cm-3) 1.487 1.721
    μ / mm-1 0.55 0.87
    θ range / (°) 2.8-25.5 2.8-25.0
    Goodness-of-fit on F 2 1.01 1.04
    Reflection collected 46 843 13 908
    Independent reflection 10 019 (Rint=0.044) 5 553 (Rint=0.040)
    Reflection observed [I > 2σ(I)] 7 348 4 076
    R1 [I > 2σ(I)] 0.041 0.042
    wR2 [I > 2σ(I)] 0.102 0.103

    The single-crystal diffraction analysis shows that complex 1 crystallizes in monoclinic P1 space group, and its asymmetric unit consists of two Mn(Ⅱ) ions, one HL4- ligand, three phen ligands, two coordination water molecules, and solvent molecules. As shown in Fig.1a, the Mn1 and Mn2 ions both adopt six-coordination to form the twisted octahedron configuration, and the metal ion is located in the center of the octahedron. Mn1 is coordinated with two carboxyl oxygen atoms (O2 and O3) from two HL4- ligands and four nitrogen atoms (N1, N2, N3, and N4) from two phen ligands. Mn2 is surrounded by two carboxyl oxygen atoms (O4 and O7) from two different HL4- ligands, two nitrogen atoms (N5 and N6) from phen ligand, and two coordination water molecules (O12 and O13). The Mn—O and Mn—N bond distances vary from 0.210 2(2) to 0.223 7(2) nm, and 0.225 1(2) to 0.233 4(2) nm, respectively.

    Figure 1

    Figure 1.  (a) Coordination environment of Mn(Ⅱ) ion in complex 1 with the thermal ellipsoids at 30% probability level; (b) 1D chain structure formed by HL4- ligands linking to Mn(Ⅱ) ions; (c) 2D layered structure formed by ππ stacking interactions between the benzene rings of phen

    Symmetry codes: -x+1/2, -y+1/2, -z; -x+1, -y, -z.

    In the assembly of complex 1, the H5L ligands are partially deprotonated and adopt the coordination mode of μ4-(κ1-κ1)-(κ0-κ1)-(κ0-κ1)-(κ0-κ0)-(κ0-κ0). To accommodate the formation of coordination bonds, the two benzene rings of the ligand are twisted with a dihedral angle of 84.80(1)°. Mn1 and Mn1 are bridged by two carboxyl groups from two different HL4- ligands to form an eight-membered ring, and the Mn…Mn distance is 0.471 6(2) nm. Mn2 and Mn2 are connected by two different HL4- ligands to form a sixteen-membered ring with Mn…Mn distance of 0.913 4(2) nm. Eight- membered and sixteen-membered rings appear alternately along the a-axis direction, forming a 1D chain structure (Fig.1b). Moreover, the phen ligands are located at two apices of each 1D chain. 1D chains are further build into a 2D layer lying in the ab plane organized by weak ππ interactions between the pyridine rings of phen. The distance between the centroids is 0.362 9(2) nm (Fig 1c).

    Complex 2 crystallizes in monoclinic crystal system, space group C2/c, and its asymmetric unit includes two Mn(Ⅱ) ions, one HL4- ligand, one half 1, 4-bib ligands, and one coordinated water molecule. As shown in Fig.2a, the Mn1 ion adopts the six-coordination with five carboxylated oxygen atoms (O1, O3, O4, O6, and O11) from the four HL4- ligands and one nitrogen atom (N3) from the 1, 4-bib ligand to form an octahedral configuration in which Mn1 is located at the center of the octahedron, while O1, O3, O11 and N3 are located on the equatorial plane, and O4 and O6 are located on the axis perpendicular to the equatorial plane. The Mn2 ion adopts five-coordination to form a deformed triangular bipyramid configuration, and the five vertices of the triangular bipyramid are occupied by three carboxyl oxygen atoms (O1, O3, and O10), a nitrogen atom (N1) from the 1, 4-bib ligand and a coordination water molecule (O12). The corresponding Mn—O bond lengths around Mn1 and Mn2 range from 0.211 0(2) to 0.228 2(2) nm, and Mn—N bond lengths are 0.216 6(3) and 0.219 3(3) nm.

    Figure 2

    Figure 2.  (a) Displacement ellipsoid plot (30% probability) of the coordination environments of Mn(Ⅱ) ions in complex 2; (b) Mn(Ⅱ) tetranuclear unit in 2; (c) 3D polyhedral structure of 2 (the polyhedron of Mn1 and Mn2 are represented with green and orange colors, respectively); (d) 3D topology net of 2

    Symmetry codes: -x, -y, -z; x, y+1, z; -x+1, -y+1, -z.

    Different from that in complex 1, HL4- connects Mn(Ⅱ) ions in the coordination mode of μ7-(κ1-κ2)-(κ0-κ2)-(κ1-κ0)-(κ1-κ1)-(κ0-κ0), with the dihedral angle being 89.79(8)°. Four Mn(Ⅱ) ions are connected via carboxylic groups to form a tetranuclear manganese unit, in which four coplanar Mn(Ⅱ) ions are connected by two equivalent μ3-η1η2 carboxylic acid bridges, forming an Mn4 parallelogram (Fig.2b). There are two different bridging motifs between non-equivalent Mn(Ⅱ) ions, which define the edges of Mn4 parallelogram. The one is a μ2-η1η1 carboxylic bridge with a distance between Mn and Mn of 0.354 6(2) nm. The other is μ2-η2 carboxylic bridge with a longer Mn…Mn distance of 0.385 9(2) nm. Tetranuclear units are connected by HL4- establishing a 2D layered structure parallel to the ab plane. Adjacent 2D layers are further connected by 1, 4-bib to form a 3D framework (Fig.2c).

    From the topological point of view, the HL4- ligand could be viewed as a 3-connected node, and the tetranuclear manganese unit could be regarded as an 8-connected linker, so the overall structure of 2 can be viewed as a (3, 8)-connected 3D network structure with the topological symbol of {43}2{46.618.84} (Fig.2d).

    Generally, the structures of CPs are influenced by many factors, including synthesis conditions (solvent, pH, temperature, molar ratio of reactants), anion types, metal ions, ligands, etc. Herein, complexes 1 and 2 were both obtained by the reaction of polycarboxylic acid ligand H5L, N-auxiliary ligand, and manganese salt under hydrothermal conditions. The conditions for the synthesis of 1 and 2 are similar, with the difference being the N-auxiliary ligand. Due to the large steric hindrance and single coordination mode of auxiliary ligand phen, it is easy to chelate with metal ions, which ultimately leads to the formation of the 1D chain structure of 1. In 2, due to the addition of auxiliary ligand 1, 4-bib, the partial coordination sites of metal ions are occupied by nitrogen atoms in 1, 4-bib which plays the role of bridging ligand, and finally, 2 forms a 3D framework structure.

    Analyzing and comparing the synthesis and structure of complexes 1 and 2, it is found that the structural differences between complexes 1 and 2 are due to the different coordination modes of the ligand HL4-. Fig.3 shows the coordination pattern of HL4- in the manganese complexes, μ4-(κ1-κ1)-(κ0-κ1)-(κ0-κ1)-(κ0-κ0)-(κ0-κ0) for 1 in the presence of phen coligand and μ7-(κ1-κ2)-(κ0-κ2)-(κ1-κ0)-(κ1-κ1)-(κ0-κ0) for 2 in the presence of 1, 4-bib coligand, indicating that the N-donor coligands have a significant effect on the coordination mode of the ligand HL4-, resulting in the structures differences between 1 and 2.

    Figure 3

    Figure 3.  Various coordination modes of HL4- observed in complexes 1 (left) and 2 (right)

    The phase purity of complexes 1 and 2 were characterized by PXRD. The experimental and simulated PXRD patterns are shown in Fig.S2. The positions of the experimental diffraction peaks were consistent with those of the simulated diffraction peaks based on the result of the single-crystal diffraction experiments, indicating the high phase purity of 1 and 2. The difference of peak intensities may be attributed to the different crystallographic orientations of the crystals.

    To evaluate the stability of complexes 1 and 2, thermogravimetric analysis (TGA) was performed (Fig.S3). In the TGA curve of 1, there was a weight loss of 14.29% from 30 to 140 ℃, corresponding to the liberation of free and coordinated water molecules (Calcd. 14.16%), and further weight loss was observed at about 250 ℃, owing to the collapse of the framework of 1. For 2, a weight loss of 2.35% was observed in a temperature range of 85-120 ℃, which corresponds to the release of the coordinated water molecule (Calcd. 2.17%). A continuous weight loss starting at 315 ℃ was accompanied by the subsequent decomposition of the framework.

    To gain insight into magnetic changes of complexes 1 and 2, the variable-temperature magnetization of finely ground single-crystal samples was measured in a temperature range of 2-300 K with an applied magnetic field of 1 000 Oe.

    The magnetic susceptibility of 1 is shown as χM-1 and χMT vs T plots in Fig.4a. At 300 K, the experimental χMT value of 1 was 8.68 cm3·mol-1·K, which is slightly lower than the expected value (8.75 cm3·mol-1·K) of two uncorrelated spins of Mn(Ⅱ) ions (g=2.0, S= 5/2). With the decrease in temperature, the χMT value decreased first slowly and then rapidly, reaching the minimum value of 4.83 cm3·mol-1·K at 2.0 K, suggesting the existence of antiferromagnetic behavior. The χM value increased monotonously with the decrease in temperature indicating antiferromagnetic ordering. In the 2-300 K range, the magnetic susceptibility could be well fitted to the Curie-Weiss law, χ=C/(T-θ), yielding a Curie constant C=8.80 cm3·mol-1·K and a negative Weiss constant θ of -1.62 K (Fig.4b). The negative θ value further confirms a dominant antiferromagnetic interaction between the Mn(Ⅱ) ions.

    Figure 4

    Figure 4.  (a) χM and χMT vs T plots and (b) χM-1 vs T plots for complex 1

    The solid line represents the best fit.

    To quantitatively evaluate the magnetic interactions in complex 1, it is necessary to determine the main magnetic interaction pathways in CPs. As mentioned above, the structure of 1 is considered to be a 1D chain formed by two different Mn(Ⅱ) dimers alternately connected along the a-axis. The Mn…Mn distance of binuclear Mn(Ⅱ) linked by a pair of carboxyl groups is 0.471 6(2) nm, while the Mn…Mn distance of binuclear Mn(Ⅱ) connected by ligands is 0.913 4(2) nm. Therefore, the magnetic interaction between the binuclear manganese linked by ligands can be ignored. We speculated that the main magnetic interaction of 1 may be limited to the Mn2(μ-COO)2 dimer. Taking into account the dinuclear Mn(Ⅱ) model, the magnetic susceptibility data were analyzed using the Bleaney- Bowers expression based on a Heisenberg Hamiltonian Ĥ=-1Ŝ2[20]. Here, J is the exchange coupling parameter between Mn(Ⅱ) ions for 1. The corresponding equation is given as follows:

    $ {\chi }_{\mathrm{d}\mathrm{i}\mathrm{m}\mathrm{e}\mathrm{r}}=\frac{{N}_{\mathrm{A}}{g}^{2}{\beta }^{2}}{kT}·\frac{A}{B} $

    (1)

    where A=exp(2x)+5exp(6x)+14exp(12x)+30exp(20x)+55exp(30x), B=1+3exp(2x)+5exp(6x)+exp(21x)+9exp(2x)+11exp(30x), x=J/(kT), and NA, g, β, and k have their usual meanings.

    Further, the inter-dimer interaction (zj′) through intermolecular interaction is treated by the molecular field approximation. Thus, the total magnetic susceptibility is:

    $ {\chi }_{\mathrm{M}}=\frac{{\chi }_{\mathrm{d}\mathrm{i}\mathrm{m}\mathrm{e}\mathrm{r}}}{1-\left(\frac{2zj\text{'}}{{N}_{\mathrm{A}}{g}^{2}{\beta }^{2}}\right){\chi }_{\mathrm{d}\mathrm{i}\mathrm{m}\mathrm{e}\mathrm{r}}} $

    (2)

    Based on Eq.2, the optimization gave the following parameters: J=-0.60 cm-1, zj′=-0.40 cm-1, and g=1.92 with the agreement factor R=4.66×10-3. The g value was in accord with the expectation for a dinuclear Mn(Ⅱ) complex[21]. The small negative J value further suggests weak antiferromagnetic interaction within the Mn2(μ-COO)2 dimer in 1.

    For 2, the observed χMT value at 300 K was about 8.76 cm3·mol-1·K, being close to the spin-only value of 8.75 cm3·mol-1·K expected for two high-spin Mn(Ⅱ) ions (g=2.0 and S=5/2) (Fig.5a). As the temperature was lowered, the χMT value continued to decrease slowly until about 60 K. Below this temperature, the value of the χMT decreased sharply, reaching a minimum value of 4.47 cm3·mol-1·K at 2.0 K, indicating the antiferromagnetic behavior. The χM value of 2 increased with temperature decreasing, and a round peak appeared near 13 K. The increase of the χM value below 8 K is due to the presence of paramagnetic impurities. Above 13 K, a typical paramagnetic Curie-Weiss behavior was observed, with a negative Weiss constant θ= -26.05 K and Curie constant C=9.70 cm3·mol-1·K (Fig.5b). The negative θ value is indicative of antiferromagnetic interactions in 2.

    Figure 5

    Figure 5.  (a) χM and χMT vs T plots and (b) χM-1 vs T plot for 2

    The solid line represents the best fit.

    Based on the structure analysis of complex 2, the main magnetic interactions may be considered to occur within the discrete tetranuclear manganese units linked by carboxylate groups, whereas the exchange interactions between Mn(Ⅱ) ions from adjacent tetranuclear units can be ignored because these units are well separated. The Mn…Mn interactions within tetranuclear unit are 0.354 6(2) and 0.385 9(2) nm, and the exchange angles are 78.402(9)° and 101.598(9)°, respectively. Considering the 3D characteristics of 2, the system can be magnetically treated as a square Mn4 unit model. The magnetic susceptibility for such a system can be expressed as[22]:

    $ {\chi }_{\mathrm{t}\mathrm{e}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{m}\mathrm{e}\mathrm{r}}=\frac{{N}_{\mathrm{A}}{g}^{2}{\beta }^{2}}{3kT}·\frac{A}{B} $

    (3)

    $ {\chi }_{\mathrm{M}}=\frac{{\chi }_{\mathrm{t}\mathrm{e}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{m}\mathrm{e}\mathrm{r}}(1-\rho )}{1-\left(\frac{zj\text{'}}{{N}_{\mathrm{A}}{g}^{2}{\beta }^{2}}\right){\chi }_{\mathrm{t}\mathrm{e}\mathrm{t}\mathrm{r}\mathrm{a}\mathrm{m}\mathrm{e}\mathrm{r}}}+\frac{4NA{g}^{2}{\beta }^{2}\rho }{3kT} $

    (4)

    where A=90exp(2x)+630exp(6x)+2 016exp(12x)+4 320 exp(20x) + 6 390exp(30x) + 8 190exp(42x) + 8 400exp(56x)+7 344exp(72x)+5 310exp(90x)+2 310exp(110x), B=6 + 45exp(2x) + 105exp(6x) + 168exp(12x) + 216exp(20x)+231exp(30x)+195exp(42x)+150exp(56x)+102exp(72x)+57exp(90x)+21exp(110x), and x=J/(kT). Molecular field approximation (zJ′) and paramagnetic impurities (ρ) are added in Eq.4 to explain the actual magnetic property of 2.

    Here χtetramer is the susceptibility of the square Mn4 unit, deduced from the exchange Hamiltonian Ĥ=-2J(Ŝ1Ŝ2+Ŝ1Ŝ2′+Ŝ1′Ŝ2+Ŝ1′Ŝ2′+Ŝ2Ŝ2′). The best-fit parameters were found as J=-3.16 cm-1, g=1.97, zj′=4.90 cm-1, ρ=0.48, and R=7.91×10-4. The negative value of J further corroborates the presence of antiferromagnetic interactions between Mn(Ⅱ) ions through the carboxylic bridging. Moreover, compared to 1, the stronger antiferromagnetic exchange coupling may be attributed to complete coplanar Mn4 subunits in which the shorter Mn…Mn distances facilitate electron interactions.

    In summary, we have successfully constructed two Mn(Ⅱ) coordination polymers (1 and 2) through a similar synthesis process. Structure and properties modulation has been achieved by using N-auxiliary ligands with different linkages. Structural analyses reveal that two kinds of binuclear manganese units are alternately connected and extended along the a-axis to form a 1D chain in complex 1, and the Mn(Ⅱ)-carboxylate tetranuclear are cooperatively extended by HL4- and 1, 4-bib coligand to generate a (3, 8)-connected 3D network with a new topological symbol {43}2{46.618.84} in complex 2. Magnetic studies indicate the presence of antiferromagnetic exchanges in 1 and 2. 1 presents an Mn2 dinuclear model with a coupling value of J=-0.60 cm-1, and 2 represents a square Mn4 tetranuclear model with a coupling value of J=-3.16 cm-1. Subsequent works will be focused on the construction of novel coordination polymers based on other polynuclear metal units by using similar organic ligands.

    Supporting information is available at http://www.wjhxxb.cn


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  • Scheme 1  Synthesis strategy for complexes 1 and 2

    Figure 1  (a) Coordination environment of Mn(Ⅱ) ion in complex 1 with the thermal ellipsoids at 30% probability level; (b) 1D chain structure formed by HL4- ligands linking to Mn(Ⅱ) ions; (c) 2D layered structure formed by ππ stacking interactions between the benzene rings of phen

    Symmetry codes: -x+1/2, -y+1/2, -z; -x+1, -y, -z.

    Figure 2  (a) Displacement ellipsoid plot (30% probability) of the coordination environments of Mn(Ⅱ) ions in complex 2; (b) Mn(Ⅱ) tetranuclear unit in 2; (c) 3D polyhedral structure of 2 (the polyhedron of Mn1 and Mn2 are represented with green and orange colors, respectively); (d) 3D topology net of 2

    Symmetry codes: -x, -y, -z; x, y+1, z; -x+1, -y+1, -z.

    Figure 3  Various coordination modes of HL4- observed in complexes 1 (left) and 2 (right)

    Figure 4  (a) χM and χMT vs T plots and (b) χM-1 vs T plots for complex 1

    The solid line represents the best fit.

    Figure 5  (a) χM and χMT vs T plots and (b) χM-1 vs T plot for 2

    The solid line represents the best fit.

    Table 1.  Crystal data and structure refinement parameters for complexes 1 and 2

    Parameter 1 2
    Empirical formula C53H38Mn2N6O15·5.5H2O C35H23Mn2N6O12
    Formula weight 1207.86 829.47
    T / K 294 295
    Crystal system Monoclinic Triclinic
    Space group C2/c P1
    a / nm 2.735 98(9) 1.117 3(3)
    b / nm 1.448 58(2) 1.120 2(3)
    c / nm 2.743 88(9) 1.448 7(4)
    α / (°) 91.511(9)
    β / (°) 97.155(2) 93.75(1)
    γ / (°) 117.544(9)
    V / nm3 10.790 1(3) 1.600 9(8)
    Z 8 2
    F(000) 4 984 842
    Dc / (g·cm-3) 1.487 1.721
    μ / mm-1 0.55 0.87
    θ range / (°) 2.8-25.5 2.8-25.0
    Goodness-of-fit on F 2 1.01 1.04
    Reflection collected 46 843 13 908
    Independent reflection 10 019 (Rint=0.044) 5 553 (Rint=0.040)
    Reflection observed [I > 2σ(I)] 7 348 4 076
    R1 [I > 2σ(I)] 0.041 0.042
    wR2 [I > 2σ(I)] 0.102 0.103
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  • 发布日期:  2025-03-10
  • 收稿日期:  2024-07-16
  • 修回日期:  2024-11-11
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