DOI:
10.1039/C4RA13501F
(Paper)
RSC Adv., 2015,
5, 14897-14905
Syntheses, structures, topologies, and luminescence properties of four coordination polymers based on bifunctional 6-(4-pyridyl)-terephthalic acid and bis(imidazole) bridging linkers†
Received
30th October 2014
, Accepted 23rd January 2015
First published on 23rd January 2015
Abstract
Four mixed-ligand coordination networks, namely, {[Cu(pta)(1,4-bimb)0.5(H2O)0.5]·H2O}n (1), {[Co(pta) (4,4′-bimbp) (H2O)]·H2O}n (2),{[Cd(pta)(1,4-bidb)0.5]·2H2O}n (3), and {[Zn(pta)(1,3-bimb)0.5]·1.5H2O}n (4), were obtained under the solvothermal reactions in the presence of bis(imidazole) linkers (H2pta = 6-(4-pyridyl)-terephthalic acid, 1,4-bidb = 1,4-bis(imidazol-1-yl)-2,5-dimethyl benzene, 1,3-bimb = 1,3-bis(imidazol-1-ylmethyl)benzene, 1,4-bimb = 1,4-bis(imidazol-1-ylmethyl)benzene, and 4,4′-bimbp = 4,4′-bis(imidazol-1-ylmethyl)biphenyl). Their structures were determined by single-crystal X-ray diffraction analyses and further characterized by elemental analyses, IR spectra, powder X-ray diffraction (PXRD), and thermogravimetric (TG) analyses. Complex 1 displays a novel (3,4,4)-connected topology with the Schläfli symbol of (4.82)2(42.82.102)(8.104.12). Complex 2 features a 2D (3,5)-connected (42.67.8)(42.6)-3,5L2 sheet. Complexes 3 and 4 both exhibit a 3-fold 3D → 3D parallel entangled (3,4)-connected net with the Schläfli symbols of (4.6.8)(4.62.63)-fsc-3,4-C2/c and (4.6.8)(4.62.83)-3,4T1 for 3 and 4, respectively. Moreover, the solid state luminescence and the luminescent lifetime of 3 and 4 have been investigated.
Introduction
The coordination polymers (CPs), an emerging class of functional crystalline materials, have attracted much attention for their fascinating structures and interesting topologies, as well as their potential applications in gas storage and separation, magnetism, fluorescence, sensing, drug delivery, catalysis, and electronic devices.1–3 Although many CPs have been constructed from the assembly of metal centres and organic linkers, the prediction of such materials is still a huge challenge due to the complicated influence factors, two primary categories of which are the nature of organic linkers and the reaction conditions.4–6
As is known to all, the polycarboxylate ligands as well as the pyridine derivatives are two kinds of most widely used organic ligands due to their strong coordination abilities and diverse coordination modes.7,8 Up to now, many CPs with versatile structures have been constructed from the above-mentioned two kinds of organic ligands. However, the bifunctional organic ligands, which contains carboxyl groups and pyridine ring together, are comparatively rare.9 Generally speaking, the ligands consisting of carboxylate groups and the pyridine ring have more coordination modes to the metal ions or metal clusters and will result in considerable structural complexity and diversity of CPs.10 Besides, the advantages of the mixed-ligand synthetic strategy inspired us to introduce the bis(imidazole) bridging linkers into the reaction systerm.11 As well as polycarboxylate linkers, (bis)imidazole bridging linkers are frequently used in the assembly process of coordination polymers acting in bridging pillars, guest molecules, or charge balance roles.12 Moreover, the (bis)imidazole bridging linkers also play an important role in altering the coordination modes of polycarboxylate ligands.13 The particular behaviors allow them to be promising candidates for designing frameworks with diverse topologies.
To the best of our knowledge, 6-(4-pyridyl)-terephthalic acid based CPs have never been documented up to now, although the H2pta ligand possessing several interesting characters: (i) it has two carboxyl groups that may be completely or partially deprotonated, inducing rich coordination modes and allowing interesting structures with higher dimensionalities, (ii) it can act as a hydrogen-bond acceptor as well as donor, depending upon the degree of deprotonation, (iii) the two planars o the phenyl and pyridine ring can form different dihedral angles through the rotation of C–C single bonds, thus it may ligate metal centers in different orientations. These characters may lead to cavities, interpenetration, helical structures, and other novel motifs with unique topologies. Thus, these considerations inspired us to explore new coordination frameworks with designed 6-(4-pyridyl)-terephthalic acid (H2pta) and different N-donor ancillary ligands under solvothermal conditions. In this paper, we reported the syntheses and characterizations of four novel coordination polymers: {[Cu(pta)(1,4-bimb)0.5(H2O)0.5]·H2O}n (1), {[Co(pta)(4,4′-bimbp) (H2O)]·H2O}n (2),{[Cd(pta)(1,4-bidb)0.5]·2H2O}n (3), and {[Zn(pta)(1,3-bimb)0.5]·1.5H2O}n (4), which exhibiting a systematic variation of architectures from (3,4,4)-connected (4.82)2(42.82.102)(8.104.12) architecture (1), 2D (3,5)-connected 3,5L2 sheet (2).3-fold (3,4)-connected fsc-3,4-C2/c net (3), to 3-fold (3,4)-connected 3,4T1 net (4) (Scheme 1). These results reveal that the bifunctional 6-(4-pyridyl)-terephthalic acid is a good candidate to construct interesting CPs. Moreover, the ancillary ligand backbones have great influence on the topology of coordination architectures and may be used as a tool to tune the degree of interpenetrations.
 |
| Scheme 1 Mixed-ligand strategy in the construction of complexes 1–4. | |
Experimental section
Materials and physical measurements
All chemical reagents were purchased from Jinan Henghua Sci. & Tec. Co. Ltd. without further purification. IR spectra were measured on a Nicolet 740 FTIR Spectrometer at the range of 600–4000 cm−1. Elemental analyses were carried out on a CE instruments EA 1110 elemental analyzer. TGA was measured from 25 to 800 °C on a SDT Q600 instrument at a heating rate 5 °C min−1 under the N2 atmosphere (100 mL min−1). X-ray powder diffractions were measured on a Panalytical X-Pert pro diffractometer with Cu-Kα radiation. Fluorescence spectra were performed on a Hitachi F-4500 fluorescence spectrophotometer at room temperature. Luminescence lifetime for crystal solid samples were recorded at room temperature on an Edinburgh FLS920 phosphorimeter.
Synthesis of {[Cu(pta)(1,4-bimb)0.5(H2O)0.5]·H2O}n (1)
A mixture of H2pta (0.20 mmol, 0.046 g), 1,4-bimb (0.20 mmol, 0.048 g), CuCl (0.20 mmol, 0.019 g), NaOH (0.40 mmol, 0.016 g), and 14 mL H2O was placed in a Teflon-lined stainless steel vessel, heated to 170 °C for 3 days, followed by slow cooling (a descent rate of 10 °C h−1) to room temperature. Blue block crystals of 1 were obtained. Yield of 45% (based on Cu). Anal. (%) calcd for C40H34Cu2N6O11: C, 53.27; H, 3.80; N, 9.32. Found: C, 52.86; H, 3.91; N, 9.23. IR (KBr pellet, cm−1): 3549 (w), 3396 (m), 1619 (vs), 1580 (vs), 1538 (s), 1401 (s), 1361 (vs), 1269 (m), 846 (m), 755 (w).
Synthesis of {[Co(pta)(4,4′-bimbp)(H2O)]·H2O}n (2)
A mixture of H2pta (0.20 mmol, 0.046 g), 4,4′-bimbp (0.30 mmol, 0.094 g), Co(NO3)2·6H2O (0.20 mmol, 0.058 g), NaOH (0.40 mmol, 0.016 g), and 12 mL H2O was placed in a Teflon-lined stainless steel vessel, heated to 170 °C for 3 days, followed by slow cooling (a descent rate of 10 °C h−1) to room temperature. Pink block crystals of 2 were obtained. Yield of 41% (based on Co). Anal. (%) calcd for C33H28CoN5O6: C, 61.02; H, 4.35; N, 10.78. Found: C, 60.37; H, 4.63; N, 10.33. IR (KBr pellet, cm−1): 3380 (m), 3125 (m), 1604 (s), 1559 (m), 1520 (s), 1368 (s), 1068 (s), 853 (m), 785 (w).
Synthesis of {[Cd(pta)(1,4-bidb)0.5]·2H2O}n (3)
A mixture of H2pta (0.20 mmol, 0.046 g), 1,4-bidb (0.20 mmol, 0.048 g), CdSO4·8/3H2O (0.20 mmol, 0.051 g), NaOH (0.30 mmol, 0.012 g), and 14 mL H2O was placed in a Teflon-lined stainless steel vessel, heated to 170 °C for 3 days, followed by slow cooling (a descent rate of 10 °C h−1) to room temperature. Colorless block crystals of 3 were obtained. Yield of 59% (based on Cd). Anal. (%) calcd for C20H18CdN3O6: C, 47.21; H, 3.57; N, 8.26. Found: C, 46.91; H, 3.47; N, 8.11. IR (KBr pellet, cm−1): 3361 (m), 3111 (m), 1612 (s), 1581 (s), 1520 (vs), 1494 (vs), 1411 (s), 1373 (s), 1329 (m), 1271 (m), 849 (m), 775 (w).
Synthesis of {[Zn(pta)(1,3-bimb)0.5]·1.5H2O}n (4)
A mixture of H2pta (0.20 mmol, 0.046 g), 1,3-bimb (0.20 mmol, 0.048 g), ZnSO4·7H2O (0.20 mmol, 0.057 g), NaOH (0.40 mmol, 0.016 g), and 12 mL H2O was placed in a Teflon-lined stainless steel vessel, heated to 170 °C for 3 days, followed by slow cooling (a descent rate of 10 °C h−1) to room temperature. Colorless block crystals of 4 were obtained. Yield of 63% (based on Zn). Anal. (%) calcd for C40H34N6O11Zn2: C, 53.05; H, 3.78; N, 9.28. Found: C, 53.18; H, 3.74; N, 9.23. IR (KBr pellet, cm−1): 3441 (s), 3114 (m), 1617 (vs), 1581 (vs), 1535 (s), 1518 (vs), 1483 (m),1401 (m), 1364 (vs), 1230 (m), 847 (m), 773 (m).
X-ray crystallography
Intensity data collection was carried out on a Siemens SMART diffractometer equipped with a CCD detector using Mo-Kα monochromatized radiation (λ = 0.71073 Å) at 296(2) K. The absorption correction was based on multiple and symmetry-equivalent reflections in the data set using the SADABS program based on the method of Blessing. The structures were solved by direct methods and refined by full-matrix least-squares using the SHELXTL package.14 Anisotropic thermal factors were assigned to all the non-hydrogen atoms. Hydrogen atoms were included in calculated positions and refined with isotropic thermal parameters riding on the parent atoms. And the hydrogen atoms attached to oxygen were refined with O–H = 0.85 Å and Uiso(H) = 1.2Ueq(O). In complex 2, the occupancy ratio of O1w is 50. Crystallographic data for complexes 1–4 are given in Table 1. Selected bond lengths and angles for 1–4 are listed in Table S1.†
Table 1 Crystal data for 1–4a
Complex |
1 |
2 |
3 |
4 |
R1 = Σ‖Fo| − |Fc‖/Σ|Fo|, wR2 = [Σw(Fo2 − Fc2)2]/Σw(Fo2)2]1/2. |
Empirical formula |
C40H34Cu2N6O11 |
C66H56Co2N10O11 |
C20H18CdN3O6 |
C40H34N6O11Zn2 |
Formula weight |
901.81 |
1283.07 |
508.77 |
905.47 |
Crystal system |
Monoclinic |
Monoclinic |
Monoclinic |
Monoclinic |
Space group |
C2/c |
C2/c |
C2/c |
C2/c |
a (Å) |
24.350(7) |
15.0742(11) |
11.979(2) |
14.092(2) |
b (Å) |
13.403(4) |
19.7770(14) |
18.789(4) |
18.273(3) |
c (Å) |
14.137(4) |
21.3225(15) |
18.662(5) |
16.325(3) |
β (°) |
123.397(4) |
105.1130(10) |
96.494(2) |
92.766(3) |
V (Å3) |
3851.9(19) |
6136.9(8) |
4173.4(15) |
4198.9(11) |
Z |
4 |
4 |
8 |
4 |
Dcalcd (Mg m−3) |
1.555 |
1.389 |
1.619 |
1.432 |
μ (mm−1) |
1.175 |
0.611 |
1.088 |
1.208 |
θ Range (°) |
1.82–25.00 |
1.74–27.10 |
2.03–25.00 |
1.83–25.00 |
Reflections collected |
9700 |
15786 |
10389 |
10648 |
Data/restraints/parameters |
3380/4/278 |
6681/589/485 |
3680/6/288 |
3706/4/277 |
F(000) |
1848 |
2656 |
2040 |
1856 |
T (K) |
296(2) |
296(2) |
296(2) |
296(2) |
Rint |
0.0358 |
0.0386 |
0.0166 |
0.0451 |
R1 (wR2) (all data) |
0.0543 (0.1070) |
0.0783 (0.1780) |
0.0330 (0.1156) |
0.0824 (0.2218) |
Gof |
0.999 |
1.004 |
1.000 |
0.999 |
Result and discussion
Syntheses and characterization
Complexes 1–4 were obtained by employing bifunctional 6-(4-pyridyl)-terephthalic acid (H2pta) and four different bis(imidazole) bridging linkers. The solid states of 1–4 are stable upon extended exposure to air. Powder X-ray diffraction (PXRD) has been used to check the phase purity of the bulk samples in the solid state. For complexes 1–4, the measured PXRD patterns closely match the simulated patterns generated from the results of single crystal diffraction data, indicative of pure products (Fig. S1, see ESI†). The absorption bands of IR spectrum in the range of 3300–3500 cm−1 for 1-4 can be attributed to the characteristic peaks of water O–H vibrations. The absence of the expected characteristic bands around 1700 cm−1 is attributable to the complete deprotonation of the H2pta ligand in the reactions. The strong antisymmetric (νas) and symmetric (νs) carboxyl vibrations are observed at about 1600 and 1400 cm−1, respectively. And the Δνas–s values of 177 cm−1, 132 cm−1 for 1, 206 cm−1, 189 cm−1 for 2, 118 cm−1, 170 cm−1 for 3, and 180 cm−1, 171 cm−1 for 4, respectively (Fig. S2†).15
Structural description of {[Cu(pta)(1,4-bimb)0.5(H2O)0.5]·H2O}n (1)
Structural analysis reveals that complex 1 crystallizes in the monoclinic system, space group C2/c and the asymmetric unit contains two halves of CuII ions, one pta2− ligand, half of 1,4-bimb ligand, half of coordinated water molecule, and one lattice water molecule (Fig. 1a). Cu(1) and Cu(2) show different coordination environments. Cu(1) is penta-coordinated by two N atoms from two independent pta2− ligands, two carboxylate O atoms from two pta2− ligands, and one coordinated water molecule. The Cu(2) ion has a distorted {CuO2N4} octahedral geometry, completed by four O atoms from two carboxyl groups of two pta2− ligands and two N atoms from two 1,4-bimb ligands. The bond lengths of Cu–N/O are in the range of 1.961(3)–2.546(4) Å.
 |
| Fig. 1 (a) Coordination environment of CuII ions in 1 (symmetry codes: (A) 1/2 − x, 1/2 − y, −z; (B) 2 − x, y, 3/2 − z; (C) 2 − x, −y, 1 − z; (D): x, −y, 1/2 + z; (E) 1 − x, −y, −z.). (b) The 3,4-connected [Cu(pta)]n sheet of 1. (c) Schematic view of the 3D structure frameworks of 1 along c axis. (d) The novel (3,4,4)-connected (4.82)2(42.82.102)(8.104.12) architecture of 1. | |
The pta2− ligand acts as one μ3 node to coordinate with three CuII ions via the deprotonated carboxylate oxygen atom and the N atom (Mode I, Scheme 2). The dihedral angle between the phenyl ring and pyridine ring in pta2− is 44.53(1)°. In complex 1, Cu(1) ions are coordinated by pta2− ligands to form a 1D loop chain along c axis with the Cu⋯Cu distance being 8.052 Å. And the 1D loop chains are further expanded to a 2D (3,4)-connected [Cu(pta)]n layer by linking the Cu(2) atoms (Fig. 1b). Finally, the bridging 1,4-bimb ligands hinged the neighbouring layers together to result in a 3D [Cu(pta)(1,4-bimb)]n framework (Fig. 1c) with the 1,4-bimb separated Cu⋯Cu distance being 13.897 Å. On analysis of the topology, the whole structure of complex 1 can be regarded as (3,4,4)-connected architecture with the Point Schläfli symbol of (4.82)2(42.82.102)(8.104.12) from the viewpoint of topology (Fig. 1d).16
 |
| Scheme 2 The coordination modes of H2pta in complexes 1-4. | |
Structural description of {[Co(pta)(4,4′-bimbp)(H2O)]·H2O}n (2)
Structural reveals that complex 2 crystallizes in the monoclinic system, space group C2/c. The asymmetric unit contains two CoII ions, one pta2− ligand, and one 4,4′-bimbp ligand. As shown in Fig. 2a, the CoII ion displays a distorted {CoO3N3} octahedral geometry, completed by three N atoms from two 4,4′-bimbp ligands [Co(1)–N(2) = 2.16(17), Co(1)–N(5B) = 2.14(16) Å] and one pta2− ligand [Co(1)–N(1C) = 2.20(14) Å], and three O atoms from another two pta2− ligands [Co(1)–O(1A) = 2.08(12), Co(1)–O(4) = 2.11(12) Å] and one coordinated water molecule [Co(1)–O(5) = 2.16(12) Å].
 |
| Fig. 2 (a) Coordination environment of CoII ion in 2 (symmetry codes: (A) −1/2 + x, 1/2 − y, −1/2 + z; (B) −1/2 + x, 1/2 − y, −1/2 + z; (C)−x, y, 3/2 − z.). (b) The 1D [Co(pta)]n ladder chain and the 1D [Co(4,4′-bimbp)]n snake chain in 2. (c) The 2D (3,5)-connected (42.67.8)(42.6)-3,5L2 sheet of 2. (d) The 3D packing architecture of 2. | |
Although pta2− ligand also acts as one μ3 node to coordinate with three metal ions via the deprotonated carboxylate oxygen atom and the N atom, it shows one different coordination mode (Mode II, Scheme 2). The dihedral angle between the phenyl ring and pyridine ring is larger than the one in 2, 50.84(8)° in 2 and 44.53(1)° in 1. Co ions are coordinated by pta2− ligands to form a 1D wave ladder [Co(pta)]n chain, in which the adjacent three kinds of Co⋯Co distances being 8.756 Å, 10.230 Å, and 11.422 Å, respectively (Fig. 2b). The 4,4′-bimbp ligand adopted cis-coordination mode to link the CoII centers together, exhibiting a 1D snake chain with the Co⋯Co distance being 14.637 Å. Two kinds of chains joined together by sharing the CoII centers, giving a 2D layer. To illustrate the unique structure of 3, the topological analysis approach is employed, the network of complex 2 can be rationalized to a (3,5)-connected 3,5L2 topology with the point Schläfli symbol of (42.67.8)(42.6) by donoting the CoII ions as five-connected nodes and pta2− ligands as three-connected nodes, respectively (Fig. 2c). Furthermore, neighboring layers stack in a parallel fashion along the b axis to form a 3D supramolecular framework with inter-layer C–H⋯π interactions [C(25)–H(25)⋯π = 3.690(1) Å, ∠C–H⋯π = 137.3(7)°] between the 4,4′-bimbp ligand and the phenyl ring of the pta2− ligand (Fig. 2d).
Structural description of {[Cd(pta)(1,4-bidb)0.5]·2H2O}n (3)
The single-crystal X-ray diffraction analysis reveals that complex 3 crystallizes in the monoclinic system, space group C2/c space group. As shown in Fig. 3a, there is one CdII ions, one pta2− ligand, one 1,4-bidb ligand, and two lattice water molecules in the asymmetric unit. CdII is hexa-coordinated, completed by four O atoms from three pta2− ligands and two N atoms from one pta2− ligand and one 1,4-bidb ligand, resulting in a distorted octahedral geometry. The bond lengths of Cd–O are in the range of 2.244(3)–2.488(3) Å, and the Cd–N bond lengths are 2.243(3) and 2.288(3) Å, respectively. The pta2− ligand acts as one μ3 node to coordinate with three CdII ions by the (κ1–κ1)-μ1 chelating carboxyl groups and pyridyl group (Mode III, Scheme 2). The dihedral angle between phenyl ring and pyridyl ring being 49.52(0)°. CdII ions are connected by μ3-pta2− ligand to generate a 3,3-connected [Cd(pta)]n sheet (Fig. 3b). The networks are further linked by 1,4-bidb ligands to result in a 3D framework consisting of quadrilateral cavities with effective sizes of 11.63 × 13.78 Å2 (Fig. 3c). Besides, the C–H⋯π interactions [C(20)–H(20C)⋯π = 2.905(9) Å, ∠C–H⋯π = 131.7(7)°] between the Hmethyl and the phenyl ring of pta2− in two different frameworks play important roles in maintaining the stable of final 3D interpenetrating structure.
 |
| Fig. 3 Coordination environment of CdII ion in 3 (symmetry codes: (B) 3/2 − x, 1/2 − y, −z; (C) −1/2 + x, 1/2 y, –1/2 + z; (D) 1/2 − x, 1/2 + y, 1/2 − z.). (b) View of the 3,3-connected [Cd(pta)]n sheet along a axis. (c) Schematic view of the 3D structure frameworks of 3 along b axis. (d) The 3-fold 3D → 3D parallel entangled (3,4)-connected (4.6.8)(4.62.63)-fsc-3,4-C2/c net. | |
From the topology view, complex 3 can be regard as a 3-fold 3D → 3D parallel entangled (3,4)-connected fsc-3,4-C2/c net with Point symbol of (4.6.8)(4.62.63) by denoting the CdII ions and pta2− as four- and three-connected nodes, respectively (Fig. 3d).
Structure descriptions of {[Zn(pta)(1,3-bimb)0.5]·1.5H2O}n (4)
Similar to complex 3, complex 4 also owns a 3-fold 3D → 3D parallel entangled (3,4)-connected networks. X-ray single-crystal diffraction analysis reveals that complex 4 crystallizes in the monoclinic system, C2/c space group. There are one ZnII ion, one pta2− ligand, half of 1,3-bimb ligand, and one and half lattice water molecules in the asymmetric unit. As shown in Fig. 4a, ZnII is coordinated by two O atoms from two pta2− ligands and two N atoms from two 1,3-bimb ligands, exhibiting a distorted tetrahedron geometry. The bond lengths of Zn–O are 1.972(4) and 1.980(4) Å, and the Zn–N bond lengths are 1.988(5) and 2.070(4) Å, respectively.
 |
| Fig. 4 (a) Coordination environment of ZnII ion in 4 (symmetry codes: (A) 2 − x, y, −1/2 − z; (D) 3/2 − x, −1/2 + y, 1/2 − z; (E) −1/2 + x, 1/2 − y, −1/2 + z.). (b) The 3,3-connected [Zn(pta)]n sheet along a axis. (c) Schematic view of the 3D structure frameworks of 4 along b axis. (d) The 3-fold 3D → 3D parallel entangled (3,4)-connected (4.6.8)(4.62.83)-3,4T1 net. | |
In complex 4, pta2− ligand exhibits the coordination mode of Mode II. The pta2− ligand linked three ZnII ions into a 2D 3,3-connected [Zn(pta)]n layer (Fig. 4b), which are further expanded to a 3D porous framework with 1,3-bimb linkers as pillars (Fig. 4c). Moreover, three independent frameworks are interpenetrated to form a more stable 3D networks. Different from the C–H⋯π interactions in complex 2, the π-π interactions in complex 3, containing the π-π interactions [Cg⋯Cg = 3.775 Å] between the phenyl ring of pta2− and pyridyl ring of another pta2−, and the π–π interactions [Cg⋯Cg = 3.672 Å] between two adjacent imidazole ring make the 3D interpenetrating structure more stable. The topology analysis shows that the overall framework of complex 4 can be rationalized to a 3-fold binodal (3,4)-connected 3,4T1 net with the Point Schläfli symbol of (4.6.8)(4.62.83) by denoting pta2− as 3-connected nodes and ZnII ions as 4-connected nodes, respectively (Fig. 4d).
Structural comparison and discussion
As shown in the Scheme 2 and Table 2, the H2pta ligands are completely deprotonated and exhibit three different coordination modes. All pta2− ligands coordinated with three transition metal ions by using the pyrindyl N atom and monodentate/chelating carboxyl groups. Besides, all the pta2− ligands holding the dihedral angle between phenyl ring and pyridyl ring, indicating the conformation of pta2− ligands have adjustments when coordinating with the metal ions. For complex 1, the pta2− ligands linked CuII ions into a 3,4-connected [Cu(pta)]n sheet. And then the 1D [Cu(1,4-bimb)]n chains tandemed the neighboring [Cu(pta)]n sheets, leaving a (3,4,4)-connected (4.82)2(42.82.102)(8.104.12) architecture. As for complex 2, a 1D [Co(pta)]n ladder chain was obtained through the interactions between the pta2− ligands and CoII ions. By sharing the CoII ions with a 1D snaked [Co(4,4′-bibmp)]n2n+, a 2D (3,5)-connected 3,5L2 sheet was constructed. Different from the 1D metal-bis(imidazole) linker chains in complex 1 and 2, the bis(imidazole) linkers in complex 3 and 4 are just bridging the adjacent 2D [M(pta)]n layers, constructing 3D frameworks with 1D channels. And then the 3D nets interpenetrated with each other, giving 3-fold 3,4-connected (4.6.8)(4.62.63)-fsc-3,4-C2/c net for 3, and (4.6.8)(4.62.83)-3,4T1 net for 4. The minor difference between complex 3 and 4 can mainly attributed to the divergence of angles among organic linkers around metal ions.
Table 2 The comparisons of complexes 1–4
Complex |
Coord. mode |
Ancillary ligands/roles/separated M⋯M distance (Å) |
Dihedral angle (°) of H2pta |
Structure and topology |
1 |
Mode I |
1,4-Bimb/bridging/13.897(5) |
44.53(1) |
3D (3,4,4)-connected (4.82)2(42.82.102)(8.104.12) net |
2 |
Mode II |
4,4′-Bimbp/bridging/14.637(4) |
50.84(8) |
2D (3,5)-connected (42.67.8)(42.6)-3,5L2 sheet |
3 |
Mode III |
1,4-Bidb/bridging/13.784(2) |
49.52(0) |
3-Fold 3D (3,4)-connected (4.6.8)(4.62.63)-fsc-3,4-C2/c net |
4 |
Mode II |
1,3-Bimb/bridging/13.119(8) |
47.70(3) |
3-Fold 3D (3,4)-connected (4.6.8)(4.62.83)-3,4T1 net |
In summary, the bis(imidazole) bridging linkers can modulate their conformations to fine-tune themselves to satisfy the coordination preference of metal centers, which often leads to structural changes and affords unprecedented architectures. The mixed-ligands synthetic strategy has advantages for their synergistic effects of two linkers.
Thermal analyses
The experiments of thermogravimetric analysis (TGA) were performed under N2 atmosphere with a heating rate of 10 °C min−1, shown in Fig. S3.† For complex 1, the first weight loss in the temperature range of 85–135 °C is consistent with the removal of the coordinated and lattice water molecules (obsd 6.5%, calcd 6.0%). And then the packing structure starts to collapse with the temperature increasing. For complex 2, the framework is stable until 385 °C after released the coordinated and lattice water molecules (obsd 5.1%, calcd: 4.2%), and then it starts to lose its organic ligands as a result of thermal decomposition with the final remaining weight is ca. 13.6% (calcd for Co2O3 12.7%). For complex 3, an initial weight loss of 7.5% corresponds to the loss of lattice water molecules (calcd: 7.1%). Above 350 °C, the second weight loss corresponds to the loss of the organic ligands. The TGA curve of complex 4 displays the first loss of 6.3% in the temperature range of 90–140 °C corresponding to the loss of lattice water molecules (calcd: 5.9%). And then the framework collapses with thermal stability residues.
Photoluminescence properties
The fluorescence spectrum of H2pta and complex 3, and 4 have been investigated in the solid state at room temperature, shown in Fig. 5. The photoluminescent spectra of H2pta show the main peaks at 423 nm under 353 nm wavelength excitation, which could be attributed to the π* → n or π* → π transitions.17 The emission spectra exhibit emission peaks of 408 nm (λex = 330 nm) for 3, and 487 nm (λex = 412 nm) for 4, respectively, which can be assigned to the intraligand (π* → n or π* → π) emission because these emissions are neither metal-to-ligand charge transfer (MLCT) nor ligand-to-metal transfer (LMCT) in nature since the CdII and ZnII ions are difficult to oxidize or reduce due to its d10 configuration.18 The difference of the emission behaviours for complexes 3 and 4 probably derives from the different conformations of organic ligands and the differences in the rigidity of solid state crystal packing structures. The luminescence lifetime for complexes 3 and 4 were recorded at room temperature on an Edinburgh FLS920 phosphorimeter with a 450 W xenon lamp as excitation source. And the luminescence lifetimes of complexes 3 and 4 are 2.29 ns (for 3) and 2.46 ns (for 4), respectively.
 |
| Fig. 5 Emission spectra of H2pta and complexes 3 and 4 in the solid state at room temperature. | |
Conclusions
In summary, four CPs were synthesized by employing bifunctional 6-(4-pyridyl)-terephthalic acid (H2pta) and four different bis(imidazole) bridging linkers, which exhibiting a systematic variation of architectures from (3,4,4)-connected (4.82)2(42.82.102)(8.104.12) architecture, 2D (3,5)-connected 3,5L2 sheet, 3-fold (3,4)-connected fsc-3,4-C2/c net, to 3-fold (3,4)-connected 3,4T1 net. These results reveal that the bifunctional 6-(4-pyridyl)-terephthalic acid is a good candidate and the mixed-ligands synthetic strategy has advantages for their synergistic effects of two linkers. Moreover, the luminescence properties of complexes 3 and 4 in solid state show strong purple and green fluorescence in the solid state at room temperature, indicate that these compounds may be potential fluorescence materials.
Conflict of interest
The authors declare no competing financial interest.
Acknowledgements
The work was supported by financial support from the Natural Science Foundation of China (Grant nos 21101097, 21451001), Natural Science Foundation of Shandong Province (ZR2010BQ023), key discipline and innovation team of Qilu Normal University.
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Footnote |
† Electronic supplementary information (ESI) available: IR spectrum, Powder XRD patterns, TG curves and X-ray crystallographic data, for 1–4. CCDC 1031083–1031086. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c4ra13501f |
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