Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S205322961600437X/fp3027sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S205322961600437X/fp3027Isup2.hkl | |
Portable Document Format (PDF) file https://doi.org/10.1107/S205322961600437X/fp3027sup3.pdf |
CCDC reference: 1468086
Metal–organic frameworks (MOFs), as a relatively new type of inorganic–organic hybrid materials, have received widespread attention over the past decade due to their structural diversity, fascinating topologies, chemical tailorability and tenability, as well as their excellent properties with promising applications, such as gas storage and separation (Li et al., 2015; Waller et al., 2015; Alezi et al., 2015), nonlinear optics (He et al., 2015), catalysis (Chen et al., 2016; Kitagawa et al., 2004), magnetism (Aulakh et al., 2015), luminescence (Lin et al., 2015), drug delivery (Ma, Li, Xiao et al., 2015), sensing (Weiss et al., 2016) and detection (Xie et al., 2015). During the attainment of MOFs, many factors can influence the construction progress, e.g. metal ions, organic ligands, solvents, pH values, reaction temperatures, and so on (Rao et al., 2009; Liu et al., 2010). Among many on-going efforts to develop high-performance MOF materials, the selection and utilization of different organic ligands are considered to be the most significant factors that affect the structures and properties of the final products (Wan et al., 2015; Liu et al., 2011).
Moreover, a number of reports have shown that many carboxylate-based MOFs involving transition metal ions (e.g. Zn2+, Cd2+ and Co2+) with or without nitrogen-containing auxiliary ligands are unstable and lose their structural integrity rapidly when exposed to air due to the relatively weak metal–oxygen bonds within the frameworks are easy to be attacked by water molecules (Ma et al., 2011; Canivet et al., 2014; Zhang et al., 2014). This drawback has been recognized as an imperative issue for their practical applications. Four main strategies are used to prepare the hydrostable carboxylate-based MOFs: (i) using high oxidation state metals (e.g. Zr4+, Cr3+ etc.) (Kandiah et al., 2010); (ii) introducing hydrophobic groups (e.g. methyl and ethyl) to the organic ligands (Ma et al., 2011); (iii) doping hybrid composites (e.g. carbon nanotubes or hetero-metals) into the frameworks to prepare the complex (Li et al., 2012); (iv) using interpenetration or catenation of the frameworks to narrow the pore size (Jasuja & Walton, 2013).
3,3'-Dimethyl-4,4'-bipyridine (dmbpy) may act in bidentate bridging mode (Ma, Li, Wu et al., 2015), whereas the 4,4'-oxydibenzoate (oda) ligand has versatile binding and coordination modes, and can also be used to construct multinuclear structures (Yang et al., 2012). To our knowledge, very few examples of MOFs based on carboxylate and dmbpy ligands have been reported. On the basis of these considerations, we chose to react Zn(NO3)2·6H2O with 4,4'-oxydi(benzoic acid) (H2oba) and dmbpy, and obtained the title compound, {[Zn2(oba)2(dmbpy)]·4H2O)}n, (I).
Reagent-grade 4,4'-oxydi(benzoic acid) (H2oba) and Zn(NO3)2·6H2O metal salts were obtained from Aladdin and used as received. 3,3'-Dimethyl-4,4'-bipyridine (dmbpy) was isolated based on the procedure of Ma et al. (2011). Elemental analyses for C, H, and N were carried out using a Vario EL III Elemental Analyzer. IR spectra were recorded (4000–400 cm-1) as KBr disks on a Shimadzu IR-440 spectrometer. Thermogravimetric analyses (TGA) were performed on an automatic simultaneous thermal analyzer (DTG-60, Shimadzu) under a flow of N2 at a heating rate of 10 K min-1 between ambient temperature and 1073 K. Powder XRD investigations were carried out on a Bruker AXS D8-Advanced diffractometer at 40 kV and 40 mA with Cu Kα (λ = 1.5406 Å) radiation. Luminescence spectra for crystalline samples were recorded at room temperature on an Edinburgh FLS920 phosphorimeter.
A mixture of Zn(NO3)2·6H2O (0.089 g, 0.3 mmol), H2oba (0.077 g, 0.3 mmol) and dmbpy (0.028 g, 0.15 mmol) was dissolved in N,N-dimethylacetamide (DMA; 10 ml) and stirred for 30 min. Tthe solution was then heated to 403 K for 3 d in a 23 ml Teflon-lined stainless steel autoclave, followed by cooling to room temperature to yield colourless single crystals (yield 40%, based on H2oba). Analysis calculated for C20H18NO7Zn: C 53.37, H 4.00, N 3.11%; found: C 53.59, H 4.16, N 3.02%. IR (KBr, cm-1): 3444 (vs), 2977 (w), 2927 (w), 1609 (vs), 1373 (s), 1228 (s), 1155 (s), 1083 (m), 866 (m), 775 (s), 662 (s), 593 (w), 507 (w), 440 (w).
Crystal data, data collection and structure refinement details are summarized in Table 1. All H atoms were positioned geometrically and constrained using the riding-model approximation, with C—H = 0.93 (aromatic) or 0.96 Å (methyl) and Uiso (H) = 1.2 Ueq (C). The routine SQUEEZE routine (Spek, 2015) in PLATON (Spek, 2009) was applied to remove diffuse electron density caused by badly disordered water molecules. The formula unit was arrived at through combination of elemental analyses, IR spectra and thermogravimetric characterization. The dmbpy ligand was disordered strongly. We have used the PART instruction to deal with this problem; however, in the PART 2 section, the –CH3 group still vibrated in two positions, namely C29B and C29C. This complicated disorder led to difficulty in adding the 0.25 H atoms at C21B and C19B, so the final formula is lacking 0.5 H atoms.
The FT–IR spectrum of (I) was recorded as KBr pellets (Fig. S1 in the Supporting information). In the IR spectrum, strong broad bands at 3444 cm-1 can be assigned to the ν(O—H) stretching vibrations of the water molecules. Features at 2977 and 2927 cm-1 are associated with the methyl groups of dmbpy ligands. The features at 1609 and 1373 cm-1 are associated with the asymmetric (C—O—C) and symmetric (C—O—C) stretching vibrations.
The asymmetric unit of (I) includes one Zn2+ ion, one oba2- dianionic ligand, half a dmbpy ligand and two lattice water molecules. Each ZnII centre is five-coordinated by four carboxylate O atoms from four different oba2- ligands and one N atom from a dmbpy ligand (Fig. 1), adopting a distorted square-pyramidal geometry (i.e. ZnO4N), with Zn—O bond lengths and O—Zn—O angles in the ranges 2.023 (3)–2.047 (3) Å and 88.63 (17)–160.50 (11)°, respectively, all of which are within the reasonable range of those reported for other five-coordinated ZnII complexes with O- and N-donating ligands (Ma et al., 2011). In the polymeric structure of (I), the oba2- ligands adopt a µ4-bridging mode connecting four ZnII ions, whereas the dmbpy ligand is coordinated in a trans-bidentate bridging mode linking two ZnII ions from dinuclear zinc cores separated by 13.913 (2) Å. The four oba2- ligands link two ZnII ions to construct a dinuclear zinc building block, [Zn2(COO)4], which can be regarded as a supramolecular secondary building unit (SBU) or cluster node. The connectivity of the oba2- ligand to Zn2+ ions leads to the formation of a two-dimensional net, where the dinuclear zinc cores are separated by 14.165 (3) Å (Fig. 2). The rigid µ2-dmbpy struts connect the layer to other ones alternately up and down, resulting in a three-dimensional structure (Fig. 3). The free volume of voids created by the formal removal of the lattice waters is 872.0 Å3, which is about 20.5% of the unit-cell volume. The single net leaves voids that are filled by mutual interpenetration of an independent equivalent framework in a twofold interpenetrating architecture (Fig. 4).
A better insight into this framework can be achieved by topology analysis (Blatov et al., 2014). In this structure, each SBU can act as a 6-connected node, with oba2- and dmbpy ligands as linkers, and the title compound can be represented as a rob net with a point symbol of (48.66.8) (Fig. 5).
Besides (I), there are only five three-dimensional frameworks with rob topology involving the oba2- and ZnII/MgII ions with or without N-containing auxiliary ligands, viz. [Zn2(oba)2(bpy)]·DMA (DMA is N,N-dimethylacetamide and bpy is -4,4'-bypyridine; Pramanik et al., 2011), (II), and [Zn2(oba)2(bpy)]·DMF (DMF is dimethylformamide; Tan et al., 2012), (III), [Zn2(oba)2(bpe)]·2DMF (bpe is ???; Kondo et al., 2007), [Zn2(oba)2(3-BPT)]·2.5DMF (3-BPT is ???; Xie & Wu, 2014) and [Mg3(oba)3(H2O)(DMA)2]·2DMA (Li et al., 2011). From these, (II) and (III) show the same twofold interpenetrating framework with different inclusions (Pramanik et al., 2011; Tan et al., 2012). Indeed, the participation of angular ligands (like oba2-) with ZnII is an essential condition in the design of new interpenetrating networks with rob topology. Thus, similar to compounds (II) and (III), which are built from oba2- and 4,4'-bipyridine ligands, the title compound was constructed from oba2- and methyl-functionalized bipyridine (dmbpy). However, this functionalization does not affect the interpenetration, since structures (I)–(III) demonstrate the same twofold interpenetration pattern, which differs from the interpenetration mode of the other three compounds. Moreover, in comparison to (I)–(III), the two twofold interpenetrating three-dimensional zinc-based MOFs involving dmbpy ligands and linear benzene-1,4-dicarboxylate or naphthalene-1,4-dicarboxylate ligands (Ma et al., 2011; Ma, Li, Xiao et al., 2015) exhibit pcu topology.
To characterize the thermal stability of (I), we performed the thermogravimetric analysis (TGA). The relevant experiments for the crystalline sample of (I) were performed under an N2 atmosphere wherein the sample was heated to 1073 K at a rate of 10 K min-1. The TG–DTA curves are shown in Fig. 6 and the results reveal that (I) demonstrate a good thermal stability. The weight loss in the temperature range 373–573 K corresponds to the removal of two lattice water molecules (calculated 8.01%, observed 8.22%). Upon further heating, the framework was stable up to 643 K and then a sharp weight loss was observed above 643 K due to the degradation of the framework.
The pH-dependent stabilities of (I) in aqueous solutions were investigated by XRPD (Fig. 7). For these tests, 50 mg of as-synthesized crystals were soaked in aqueous solutions with different pH values and stirred for 3 d at room temperature. According to these results, the title compound is stable at pH range from 5 to 9. Stirring under more basic (pH = 13–14) or acidic (pH = 2–3) conditions, show complete decomposition of their framework. The stabilities of title compound are similar to several aluminum-isophthalate-based MOFs (CAU-10-X, where X = H, CH3, OCH3, NO2, NH2 or OH) (Reinsch et al., 2013), but lower than the series of carboxylate-based MOFs involving zirconium ions (Schaate et al., 2011). However, the results is very remarkable, especially when compared with other MOFs constructed from aromatic carboxylate N-containing auxiliary ligands and zinc/cadmium ions (Tan et al., 2015; Chen et al., 2006).
Luminescence properties of coordination polymers with d10 metal centres have attracted intense interest because of their potential applications as sensing luminescent materials (An et al., 2011; Gole et al., 2011). Herein, we examined the luminescence properties of (I) in the solid state at room temperature. The photoluminescence spectrum of H2oba shows an emission maximum at 432 nm (Hu et al., 2012). The emission band of the free ligand is probably attributable to the π*–π transition. Upon complexation of the ligand with ZnII ions, the emission peak occur at 426 nm (λex = 310 nm) (Fig. 8). The small blue-shift indicates that the luminescence of (I) probably origins from the oba2- ligands and the role of the ZnII centre is believed to stabilize the ligands and increase the conformational rigidity of the ligands by coordination.
The assembly of a zinc(II) salt with H2oba and methyl-functionalized dmbpy ligands under solvothermal conditions results in the formation of the title twofold interpenetrating three-dimensional MOF, (I), with rob underlying topology. It have been shown that (I) is stable in aqueous solutions in the pH range 5–9, and it emits a bright blue fluorescence (λem = 426 nm). The compound represents a new example of a twofold interpenetrating three-dimensional framework in an isoreticular series of structures with rob topology based on an angular ligand (oba2-) in combination with a linear N-containing auxiliary ligand (dmbpy).
Metal–organic frameworks (MOFs), as a relatively new type of inorganic–organic hybrid materials, have received widespread attention over the past decade due to their structural diversity, fascinating topologies, chemical tailorability and tenability, as well as their excellent properties with promising applications, such as gas storage and separation (Li et al., 2015; Waller et al., 2015; Alezi et al., 2015), nonlinear optics (He et al., 2015), catalysis (Chen et al., 2016; Kitagawa et al., 2004), magnetism (Aulakh et al., 2015), luminescence (Lin et al., 2015), drug delivery (Ma, Li, Xiao et al., 2015), sensing (Weiss et al., 2016) and detection (Xie et al., 2015). During the attainment of MOFs, many factors can influence the construction progress, e.g. metal ions, organic ligands, solvents, pH values, reaction temperatures, and so on (Rao et al., 2009; Liu et al., 2010). Among many on-going efforts to develop high-performance MOF materials, the selection and utilization of different organic ligands are considered to be the most significant factors that affect the structures and properties of the final products (Wan et al., 2015; Liu et al., 2011).
Moreover, a number of reports have shown that many carboxylate-based MOFs involving transition metal ions (e.g. Zn2+, Cd2+ and Co2+) with or without nitrogen-containing auxiliary ligands are unstable and lose their structural integrity rapidly when exposed to air due to the relatively weak metal–oxygen bonds within the frameworks are easy to be attacked by water molecules (Ma et al., 2011; Canivet et al., 2014; Zhang et al., 2014). This drawback has been recognized as an imperative issue for their practical applications. Four main strategies are used to prepare the hydrostable carboxylate-based MOFs: (i) using high oxidation state metals (e.g. Zr4+, Cr3+ etc.) (Kandiah et al., 2010); (ii) introducing hydrophobic groups (e.g. methyl and ethyl) to the organic ligands (Ma et al., 2011); (iii) doping hybrid composites (e.g. carbon nanotubes or hetero-metals) into the frameworks to prepare the complex (Li et al., 2012); (iv) using interpenetration or catenation of the frameworks to narrow the pore size (Jasuja & Walton, 2013).
3,3'-Dimethyl-4,4'-bipyridine (dmbpy) may act in bidentate bridging mode (Ma, Li, Wu et al., 2015), whereas the 4,4'-oxydibenzoate (oda) ligand has versatile binding and coordination modes, and can also be used to construct multinuclear structures (Yang et al., 2012). To our knowledge, very few examples of MOFs based on carboxylate and dmbpy ligands have been reported. On the basis of these considerations, we chose to react Zn(NO3)2·6H2O with 4,4'-oxydi(benzoic acid) (H2oba) and dmbpy, and obtained the title compound, {[Zn2(oba)2(dmbpy)]·4H2O)}n, (I).
Reagent-grade 4,4'-oxydi(benzoic acid) (H2oba) and Zn(NO3)2·6H2O metal salts were obtained from Aladdin and used as received. 3,3'-Dimethyl-4,4'-bipyridine (dmbpy) was isolated based on the procedure of Ma et al. (2011). Elemental analyses for C, H, and N were carried out using a Vario EL III Elemental Analyzer. IR spectra were recorded (4000–400 cm-1) as KBr disks on a Shimadzu IR-440 spectrometer. Thermogravimetric analyses (TGA) were performed on an automatic simultaneous thermal analyzer (DTG-60, Shimadzu) under a flow of N2 at a heating rate of 10 K min-1 between ambient temperature and 1073 K. Powder XRD investigations were carried out on a Bruker AXS D8-Advanced diffractometer at 40 kV and 40 mA with Cu Kα (λ = 1.5406 Å) radiation. Luminescence spectra for crystalline samples were recorded at room temperature on an Edinburgh FLS920 phosphorimeter.
The FT–IR spectrum of (I) was recorded as KBr pellets (Fig. S1 in the Supporting information). In the IR spectrum, strong broad bands at 3444 cm-1 can be assigned to the ν(O—H) stretching vibrations of the water molecules. Features at 2977 and 2927 cm-1 are associated with the methyl groups of dmbpy ligands. The features at 1609 and 1373 cm-1 are associated with the asymmetric (C—O—C) and symmetric (C—O—C) stretching vibrations.
The asymmetric unit of (I) includes one Zn2+ ion, one oba2- dianionic ligand, half a dmbpy ligand and two lattice water molecules. Each ZnII centre is five-coordinated by four carboxylate O atoms from four different oba2- ligands and one N atom from a dmbpy ligand (Fig. 1), adopting a distorted square-pyramidal geometry (i.e. ZnO4N), with Zn—O bond lengths and O—Zn—O angles in the ranges 2.023 (3)–2.047 (3) Å and 88.63 (17)–160.50 (11)°, respectively, all of which are within the reasonable range of those reported for other five-coordinated ZnII complexes with O- and N-donating ligands (Ma et al., 2011). In the polymeric structure of (I), the oba2- ligands adopt a µ4-bridging mode connecting four ZnII ions, whereas the dmbpy ligand is coordinated in a trans-bidentate bridging mode linking two ZnII ions from dinuclear zinc cores separated by 13.913 (2) Å. The four oba2- ligands link two ZnII ions to construct a dinuclear zinc building block, [Zn2(COO)4], which can be regarded as a supramolecular secondary building unit (SBU) or cluster node. The connectivity of the oba2- ligand to Zn2+ ions leads to the formation of a two-dimensional net, where the dinuclear zinc cores are separated by 14.165 (3) Å (Fig. 2). The rigid µ2-dmbpy struts connect the layer to other ones alternately up and down, resulting in a three-dimensional structure (Fig. 3). The free volume of voids created by the formal removal of the lattice waters is 872.0 Å3, which is about 20.5% of the unit-cell volume. The single net leaves voids that are filled by mutual interpenetration of an independent equivalent framework in a twofold interpenetrating architecture (Fig. 4).
A better insight into this framework can be achieved by topology analysis (Blatov et al., 2014). In this structure, each SBU can act as a 6-connected node, with oba2- and dmbpy ligands as linkers, and the title compound can be represented as a rob net with a point symbol of (48.66.8) (Fig. 5).
Besides (I), there are only five three-dimensional frameworks with rob topology involving the oba2- and ZnII/MgII ions with or without N-containing auxiliary ligands, viz. [Zn2(oba)2(bpy)]·DMA (DMA is N,N-dimethylacetamide and bpy is -4,4'-bypyridine; Pramanik et al., 2011), (II), and [Zn2(oba)2(bpy)]·DMF (DMF is dimethylformamide; Tan et al., 2012), (III), [Zn2(oba)2(bpe)]·2DMF (bpe is ???; Kondo et al., 2007), [Zn2(oba)2(3-BPT)]·2.5DMF (3-BPT is ???; Xie & Wu, 2014) and [Mg3(oba)3(H2O)(DMA)2]·2DMA (Li et al., 2011). From these, (II) and (III) show the same twofold interpenetrating framework with different inclusions (Pramanik et al., 2011; Tan et al., 2012). Indeed, the participation of angular ligands (like oba2-) with ZnII is an essential condition in the design of new interpenetrating networks with rob topology. Thus, similar to compounds (II) and (III), which are built from oba2- and 4,4'-bipyridine ligands, the title compound was constructed from oba2- and methyl-functionalized bipyridine (dmbpy). However, this functionalization does not affect the interpenetration, since structures (I)–(III) demonstrate the same twofold interpenetration pattern, which differs from the interpenetration mode of the other three compounds. Moreover, in comparison to (I)–(III), the two twofold interpenetrating three-dimensional zinc-based MOFs involving dmbpy ligands and linear benzene-1,4-dicarboxylate or naphthalene-1,4-dicarboxylate ligands (Ma et al., 2011; Ma, Li, Xiao et al., 2015) exhibit pcu topology.
To characterize the thermal stability of (I), we performed the thermogravimetric analysis (TGA). The relevant experiments for the crystalline sample of (I) were performed under an N2 atmosphere wherein the sample was heated to 1073 K at a rate of 10 K min-1. The TG–DTA curves are shown in Fig. 6 and the results reveal that (I) demonstrate a good thermal stability. The weight loss in the temperature range 373–573 K corresponds to the removal of two lattice water molecules (calculated 8.01%, observed 8.22%). Upon further heating, the framework was stable up to 643 K and then a sharp weight loss was observed above 643 K due to the degradation of the framework.
The pH-dependent stabilities of (I) in aqueous solutions were investigated by XRPD (Fig. 7). For these tests, 50 mg of as-synthesized crystals were soaked in aqueous solutions with different pH values and stirred for 3 d at room temperature. According to these results, the title compound is stable at pH range from 5 to 9. Stirring under more basic (pH = 13–14) or acidic (pH = 2–3) conditions, show complete decomposition of their framework. The stabilities of title compound are similar to several aluminum-isophthalate-based MOFs (CAU-10-X, where X = H, CH3, OCH3, NO2, NH2 or OH) (Reinsch et al., 2013), but lower than the series of carboxylate-based MOFs involving zirconium ions (Schaate et al., 2011). However, the results is very remarkable, especially when compared with other MOFs constructed from aromatic carboxylate N-containing auxiliary ligands and zinc/cadmium ions (Tan et al., 2015; Chen et al., 2006).
Luminescence properties of coordination polymers with d10 metal centres have attracted intense interest because of their potential applications as sensing luminescent materials (An et al., 2011; Gole et al., 2011). Herein, we examined the luminescence properties of (I) in the solid state at room temperature. The photoluminescence spectrum of H2oba shows an emission maximum at 432 nm (Hu et al., 2012). The emission band of the free ligand is probably attributable to the π*–π transition. Upon complexation of the ligand with ZnII ions, the emission peak occur at 426 nm (λex = 310 nm) (Fig. 8). The small blue-shift indicates that the luminescence of (I) probably origins from the oba2- ligands and the role of the ZnII centre is believed to stabilize the ligands and increase the conformational rigidity of the ligands by coordination.
The assembly of a zinc(II) salt with H2oba and methyl-functionalized dmbpy ligands under solvothermal conditions results in the formation of the title twofold interpenetrating three-dimensional MOF, (I), with rob underlying topology. It have been shown that (I) is stable in aqueous solutions in the pH range 5–9, and it emits a bright blue fluorescence (λem = 426 nm). The compound represents a new example of a twofold interpenetrating three-dimensional framework in an isoreticular series of structures with rob topology based on an angular ligand (oba2-) in combination with a linear N-containing auxiliary ligand (dmbpy).
A mixture of Zn(NO3)2·6H2O (0.089 g, 0.3 mmol), H2oba (0.077 g, 0.3 mmol) and dmbpy (0.028 g, 0.15 mmol) was dissolved in N,N-dimethylacetamide (DMA; 10 ml) and stirred for 30 min. Tthe solution was then heated to 403 K for 3 d in a 23 ml Teflon-lined stainless steel autoclave, followed by cooling to room temperature to yield colourless single crystals (yield 40%, based on H2oba). Analysis calculated for C20H18NO7Zn: C 53.37, H 4.00, N 3.11%; found: C 53.59, H 4.16, N 3.02%. IR (KBr, cm-1): 3444 (vs), 2977 (w), 2927 (w), 1609 (vs), 1373 (s), 1228 (s), 1155 (s), 1083 (m), 866 (m), 775 (s), 662 (s), 593 (w), 507 (w), 440 (w).
Crystal data, data collection and structure refinement details are summarized in Table 1. All H atoms were positioned geometrically and constrained using the riding-model approximation, with C—H = 0.93 (aromatic) or 0.96 Å (methyl) and Uiso (H) = 1.2 Ueq (C). The routine SQUEEZE routine (Spek, 2015) in PLATON (Spek, 2009) was applied to remove diffuse electron density caused by badly disordered water molecules. The formula unit was arrived at through combination of elemental analyses, IR spectra and thermogravimetric characterization. The dmbpy ligand was disordered strongly. We have used the PART instruction to deal with this problem; however, in the PART 2 section, the –CH3 group still vibrated in two positions, namely C29B and C29C. This complicated disorder led to difficulty in adding the 0.25 H atoms at C21B and C19B, so the final formula is lacking 0.5 H atoms.
Data collection: SMART (Bruker, 2008); cell refinement: SMART (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: DIAMOND (Brandenburg, 2005; software used to prepare material for publication: SHELXTL (Bruker, 2008).
[Zn2(C14H8O5)2(C12H12N2)]·4H2O | F(000) = 1848 |
Mr = 899.5 | Dx = 1.41 Mg m−3 |
Orthorhombic, Pcca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P2a2ac | Cell parameters from 8103 reflections |
a = 16.864 (4) Å | θ = 2.6–25.2° |
b = 11.067 (2) Å | µ = 1.20 mm−1 |
c = 22.764 (4) Å | T = 296 K |
V = 4248.6 (14) Å3 | Block, colorless |
Z = 4 | 0.22 × 0.20 × 0.18 mm |
Bruker SMART APEX DUO CCD diffractometer | 3849 independent reflections |
Radiation source: fine-focus sealed tube | 3314 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.025 |
phi and ω scans | θmax = 25.3°, θmin = 1.8° |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | h = −20→15 |
Tmin = 0.781, Tmax = 0.815 | k = −13→13 |
26264 measured reflections | l = −26→27 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.128 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0634P)2 + 4.8367P] where P = (Fo2 + 2Fc2)/3 |
3849 reflections | (Δ/σ)max = 0.016 |
266 parameters | Δρmax = 0.53 e Å−3 |
246 restraints | Δρmin = −0.50 e Å−3 |
[Zn2(C14H8O5)2(C12H12N2)]·4H2O | V = 4248.6 (14) Å3 |
Mr = 899.5 | Z = 4 |
Orthorhombic, Pcca | Mo Kα radiation |
a = 16.864 (4) Å | µ = 1.20 mm−1 |
b = 11.067 (2) Å | T = 296 K |
c = 22.764 (4) Å | 0.22 × 0.20 × 0.18 mm |
Bruker SMART APEX DUO CCD diffractometer | 3849 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2008) | 3314 reflections with I > 2σ(I) |
Tmin = 0.781, Tmax = 0.815 | Rint = 0.025 |
26264 measured reflections |
R[F2 > 2σ(F2)] = 0.045 | 246 restraints |
wR(F2) = 0.128 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.53 e Å−3 |
3849 reflections | Δρmin = −0.50 e Å−3 |
266 parameters |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
C1 | 0.0546 (2) | 0.3973 (3) | 0.40649 (16) | 0.0589 (9) | |
C2 | 0.0883 (2) | 0.3310 (4) | 0.35506 (15) | 0.0614 (9) | |
C3 | 0.0575 (2) | 0.2214 (4) | 0.33640 (18) | 0.0680 (11) | |
H3 | 0.0147 | 0.1879 | 0.3563 | 0.082* | |
C4 | 0.0892 (2) | 0.1613 (4) | 0.28896 (18) | 0.0734 (11) | |
H4 | 0.0681 | 0.0874 | 0.2773 | 0.088* | |
C5 | 0.1520 (2) | 0.2106 (4) | 0.25892 (18) | 0.0697 (10) | |
C6 | 0.1844 (3) | 0.3200 (4) | 0.27632 (19) | 0.0781 (12) | |
H6 | 0.2269 | 0.3534 | 0.2560 | 0.094* | |
C7 | 0.1525 (3) | 0.3787 (4) | 0.32435 (18) | 0.0730 (11) | |
H7 | 0.1744 | 0.4517 | 0.3365 | 0.088* | |
C8 | 0.23239 (13) | 0.1993 (2) | 0.17420 (11) | 0.0698 (11) | |
C9 | 0.31206 (15) | 0.1671 (2) | 0.17514 (11) | 0.0838 (14) | |
H9 | 0.3297 | 0.1076 | 0.2008 | 0.101* | |
C10 | 0.36539 (11) | 0.2240 (3) | 0.13770 (11) | 0.0773 (12) | |
H10 | 0.4187 | 0.2025 | 0.1383 | 0.093* | |
C11 | 0.33907 (12) | 0.3131 (2) | 0.09932 (9) | 0.0522 (8) | |
C12 | 0.25940 (13) | 0.3453 (2) | 0.09838 (11) | 0.0658 (10) | |
H12 | 0.2418 | 0.4049 | 0.0727 | 0.079* | |
C13 | 0.20606 (10) | 0.2884 (2) | 0.13582 (13) | 0.0773 (12) | |
H13 | 0.1528 | 0.3099 | 0.1352 | 0.093* | |
C14 | 0.3975 (2) | 0.3798 (3) | 0.06168 (14) | 0.0539 (8) | |
N1A | 0.13457 (17) | 0.7306 (2) | 0.47790 (12) | 0.0619 (9) | 0.564 (6) |
C18A | 0.2118 (2) | 0.7201 (3) | 0.4572 (2) | 0.0697 (18) | 0.564 (6) |
H18A | 0.2312 | 0.6451 | 0.4456 | 0.084* | 0.564 (6) |
C19A | 0.2600 (2) | 0.8217 (4) | 0.4537 (2) | 0.0743 (18) | 0.564 (6) |
H19A | 0.3117 | 0.8147 | 0.4398 | 0.089* | 0.564 (6) |
C20A | 0.2310 (2) | 0.9338 (3) | 0.47094 (15) | 0.0701 (12) | 0.564 (6) |
C21A | 0.15383 (19) | 0.9443 (2) | 0.4917 (2) | 0.0785 (18) | 0.564 (6) |
C22A | 0.10559 (13) | 0.8427 (3) | 0.4952 (2) | 0.0719 (17) | 0.564 (6) |
H22A | 0.0539 | 0.8497 | 0.5090 | 0.086* | 0.564 (6) |
N1B | 0.12462 (15) | 0.7505 (2) | 0.48373 (12) | 0.0619 (9) | 0.436 (6) |
C18B | 0.1182 (2) | 0.8396 (3) | 0.52649 (17) | 0.074 (2) | 0.436 (6) |
H18B | 0.0844 | 0.8286 | 0.5583 | 0.088* | 0.436 (6) |
C19B | 0.1625 (2) | 0.9451 (3) | 0.52171 (19) | 0.076 (2) | 0.436 (6) |
C20B | 0.2130 (2) | 0.9616 (2) | 0.47418 (16) | 0.0701 (12) | 0.436 (6) |
C21B | 0.2194 (3) | 0.8724 (4) | 0.43142 (12) | 0.079 (2) | 0.436 (6) |
C22B | 0.1752 (3) | 0.7669 (3) | 0.43620 (11) | 0.073 (2) | 0.436 (6) |
H22B | 0.1795 | 0.7072 | 0.4076 | 0.088* | 0.436 (6) |
C23A | 0.1193 (7) | 1.0573 (8) | 0.5101 (4) | 0.120 (4) | 0.50 |
H23A | 0.1591 | 1.1061 | 0.5287 | 0.179* | 0.50 |
H23B | 0.0771 | 1.0418 | 0.5375 | 0.179* | 0.50 |
H23C | 0.0986 | 1.0992 | 0.4765 | 0.179* | 0.50 |
C23B | 0.2713 (7) | 0.8897 (13) | 0.3822 (5) | 0.111 (6) | 0.25 |
H23D | 0.2562 | 0.9616 | 0.3614 | 0.166* | 0.25 |
H23E | 0.2676 | 0.8214 | 0.3564 | 0.166* | 0.25 |
H23F | 0.3249 | 0.8978 | 0.3959 | 0.166* | 0.25 |
C23C | 0.1536 (11) | 1.0333 (15) | 0.5664 (7) | 0.116 (6) | 0.25 |
H23G | 0.1191 | 1.0964 | 0.5527 | 0.174* | 0.25 |
H23H | 0.2045 | 1.0668 | 0.5759 | 0.174* | 0.25 |
H23I | 0.1311 | 0.9964 | 0.6007 | 0.174* | 0.25 |
O1 | −0.00252 (16) | 0.3506 (2) | 0.43328 (11) | 0.0686 (7) | |
O2 | 0.08591 (19) | 0.4959 (3) | 0.41976 (11) | 0.0804 (9) | |
O3 | 0.1801 (2) | 0.1448 (3) | 0.21242 (14) | 0.0899 (10) | |
Zn1 | 0.05787 (2) | 0.59574 (4) | 0.490891 (16) | 0.05170 (17) | |
O4 | 0.37543 (16) | 0.4771 (2) | 0.03891 (11) | 0.0665 (7) | |
O5 | 0.46489 (17) | 0.3341 (3) | 0.05522 (13) | 0.0755 (8) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.063 (2) | 0.072 (2) | 0.0422 (18) | −0.0232 (18) | 0.0015 (15) | −0.0008 (16) |
C2 | 0.059 (2) | 0.077 (2) | 0.0478 (19) | −0.0234 (19) | 0.0049 (16) | −0.0076 (17) |
C3 | 0.060 (2) | 0.080 (3) | 0.064 (2) | −0.029 (2) | 0.0082 (17) | −0.013 (2) |
C4 | 0.066 (2) | 0.081 (3) | 0.073 (3) | −0.021 (2) | 0.005 (2) | −0.023 (2) |
C5 | 0.064 (2) | 0.082 (3) | 0.064 (2) | −0.012 (2) | 0.0092 (18) | −0.017 (2) |
C6 | 0.071 (3) | 0.092 (3) | 0.071 (3) | −0.025 (2) | 0.021 (2) | −0.012 (2) |
C7 | 0.076 (3) | 0.082 (3) | 0.062 (2) | −0.032 (2) | 0.013 (2) | −0.015 (2) |
C8 | 0.070 (3) | 0.078 (3) | 0.061 (2) | 0.000 (2) | 0.0121 (19) | −0.017 (2) |
C9 | 0.071 (3) | 0.119 (4) | 0.062 (2) | 0.017 (3) | −0.002 (2) | 0.027 (3) |
C10 | 0.054 (2) | 0.111 (3) | 0.067 (2) | 0.026 (2) | 0.0013 (18) | 0.027 (2) |
C11 | 0.0530 (19) | 0.062 (2) | 0.0419 (16) | 0.0199 (16) | −0.0027 (14) | −0.0049 (15) |
C12 | 0.057 (2) | 0.058 (2) | 0.082 (3) | 0.0184 (18) | −0.0099 (19) | 0.000 (2) |
C13 | 0.052 (2) | 0.066 (2) | 0.114 (4) | 0.0128 (19) | 0.004 (2) | −0.010 (2) |
C14 | 0.060 (2) | 0.059 (2) | 0.0428 (17) | 0.0258 (17) | 0.0010 (15) | −0.0055 (15) |
N1A | 0.0648 (18) | 0.0636 (18) | 0.0571 (17) | −0.0475 (16) | 0.0012 (14) | −0.0045 (14) |
C18A | 0.070 (3) | 0.064 (3) | 0.075 (4) | −0.040 (3) | 0.014 (3) | −0.009 (3) |
C19A | 0.066 (4) | 0.067 (3) | 0.090 (4) | −0.039 (3) | 0.018 (3) | −0.015 (3) |
C20A | 0.073 (3) | 0.064 (2) | 0.074 (2) | −0.049 (2) | 0.011 (2) | −0.0075 (19) |
C21A | 0.084 (3) | 0.061 (3) | 0.090 (4) | −0.039 (3) | 0.022 (3) | −0.014 (3) |
C22A | 0.069 (3) | 0.069 (3) | 0.077 (4) | −0.046 (3) | 0.016 (3) | 0.000 (3) |
N1B | 0.0648 (18) | 0.0636 (18) | 0.0571 (17) | −0.0475 (16) | 0.0012 (14) | −0.0045 (14) |
C18B | 0.082 (4) | 0.068 (3) | 0.071 (4) | −0.043 (3) | 0.002 (4) | 0.004 (3) |
C19B | 0.086 (4) | 0.068 (3) | 0.075 (4) | −0.046 (3) | 0.015 (4) | −0.003 (3) |
C20B | 0.073 (3) | 0.064 (2) | 0.074 (2) | −0.049 (2) | 0.011 (2) | −0.0075 (19) |
C21B | 0.087 (4) | 0.074 (4) | 0.074 (4) | −0.054 (4) | 0.018 (4) | −0.008 (3) |
C22B | 0.082 (4) | 0.068 (4) | 0.070 (4) | −0.053 (3) | 0.006 (3) | −0.007 (3) |
C23A | 0.102 (7) | 0.077 (5) | 0.180 (9) | −0.030 (5) | 0.049 (7) | −0.034 (7) |
C23B | 0.142 (13) | 0.077 (10) | 0.113 (12) | −0.066 (10) | 0.083 (10) | −0.048 (9) |
C23C | 0.120 (12) | 0.084 (10) | 0.143 (12) | −0.020 (10) | 0.031 (11) | −0.029 (9) |
O1 | 0.0738 (17) | 0.0752 (17) | 0.0568 (15) | −0.0265 (14) | 0.0152 (13) | −0.0091 (13) |
O2 | 0.100 (2) | 0.0868 (19) | 0.0540 (15) | −0.0488 (17) | 0.0197 (14) | −0.0175 (14) |
O3 | 0.096 (2) | 0.087 (2) | 0.087 (2) | −0.0156 (18) | 0.0344 (18) | −0.0249 (17) |
Zn1 | 0.0558 (3) | 0.0568 (3) | 0.0425 (2) | −0.03991 (19) | 0.00089 (16) | 0.00041 (16) |
O4 | 0.0709 (16) | 0.0594 (15) | 0.0693 (16) | 0.0290 (13) | 0.0059 (13) | 0.0073 (13) |
O5 | 0.0667 (16) | 0.0844 (19) | 0.0753 (17) | 0.0388 (15) | 0.0175 (14) | 0.0181 (15) |
C1—O1 | 1.251 (4) | C20A—C21A | 1.3900 |
C1—O2 | 1.249 (4) | C20A—C20Ai | 1.599 (4) |
C1—C2 | 1.494 (5) | C21A—C22A | 1.3900 |
C2—C3 | 1.387 (5) | C21A—C23A | 1.443 (8) |
C2—C7 | 1.392 (5) | C22A—H22A | 0.9300 |
C3—C4 | 1.376 (6) | N1B—C22B | 1.3900 |
C3—H3 | 0.9300 | N1B—C18B | 1.3900 |
C4—C5 | 1.374 (5) | N1B—Zn1 | 2.0557 (17) |
C4—H4 | 0.9300 | C18B—C19B | 1.3899 |
C5—O3 | 1.369 (5) | C18B—H18B | 0.9300 |
C5—C6 | 1.386 (6) | C19B—C20B | 1.3900 |
C6—C7 | 1.381 (6) | C19B—C23C | 1.416 (9) |
C6—H6 | 0.9300 | C20B—C21B | 1.3899 |
C7—H7 | 0.9300 | C20B—C20Bi | 1.509 (4) |
C8—O3 | 1.378 (3) | C21B—C22B | 1.3901 |
C8—C9 | 1.3900 | C21B—C23B | 1.435 (9) |
C8—C13 | 1.3900 | C22B—H22B | 0.9300 |
C9—C10 | 1.3900 | C23A—H23A | 0.9600 |
C9—H9 | 0.9300 | C23A—H23B | 0.9600 |
C10—C11 | 1.3900 | C23A—H23C | 0.9600 |
C10—H10 | 0.9300 | C23B—H23D | 0.9600 |
C11—C12 | 1.3900 | C23B—H23E | 0.9600 |
C11—C14 | 1.500 (4) | C23B—H23F | 0.9600 |
C12—C13 | 1.3900 | C23C—H23G | 0.9600 |
C12—H12 | 0.9300 | C23C—H23H | 0.9600 |
C13—H13 | 0.9300 | C23C—H23I | 0.9600 |
C14—O4 | 1.251 (4) | O1—Zn1ii | 2.050 (3) |
C14—O5 | 1.253 (4) | Zn1—O2 | 2.017 (3) |
N1A—C18A | 1.3900 | Zn1—O5iii | 2.040 (3) |
N1A—C22A | 1.3900 | Zn1—O4iv | 2.046 (3) |
Zn1—N1A | 1.9971 (17) | Zn1—O1ii | 2.050 (3) |
C18A—C19A | 1.3900 | Zn1—Zn1ii | 2.9107 (7) |
C18A—H18A | 0.9300 | O4—Zn1v | 2.046 (3) |
C19A—C20A | 1.3900 | O5—Zn1vi | 2.040 (3) |
C19A—H19A | 0.9300 | ||
O1—C1—O2 | 124.6 (4) | C21A—C22A—H22A | 120.0 |
O1—C1—C2 | 118.2 (3) | N1A—C22A—H22A | 120.0 |
O2—C1—C2 | 117.2 (3) | C22B—N1B—C18B | 120.0 |
C3—C2—C7 | 118.0 (3) | C22B—N1B—Zn1 | 120.44 (15) |
C3—C2—C1 | 121.8 (3) | C18B—N1B—Zn1 | 119.56 (15) |
C7—C2—C1 | 120.3 (3) | C19B—C18B—N1B | 120.0 |
C4—C3—C2 | 121.2 (4) | C19B—C18B—H18B | 120.0 |
C4—C3—H3 | 119.4 | N1B—C18B—H18B | 120.0 |
C2—C3—H3 | 119.4 | C18B—C19B—C20B | 120.0 |
C3—C4—C5 | 119.8 (4) | C18B—C19B—C23C | 117.8 (10) |
C3—C4—H4 | 120.1 | C20B—C19B—C23C | 122.2 (10) |
C5—C4—H4 | 120.1 | C21B—C20B—C19B | 120.0 |
O3—C5—C4 | 116.1 (4) | C21B—C20B—C20Bi | 109.6 (3) |
O3—C5—C6 | 123.3 (4) | C19B—C20B—C20Bi | 125.49 (13) |
C4—C5—C6 | 120.6 (4) | C20B—C21B—C22B | 120.0 |
C7—C6—C5 | 118.9 (4) | C20B—C21B—C23B | 120.0 (7) |
C7—C6—H6 | 120.5 | C22B—C21B—C23B | 120.0 (6) |
C5—C6—H6 | 120.5 | N1B—C22B—C21B | 120.0 |
C6—C7—C2 | 121.5 (4) | N1B—C22B—H22B | 120.0 |
C6—C7—H7 | 119.3 | C21B—C22B—H22B | 120.0 |
C2—C7—H7 | 119.3 | C21B—C23B—H23D | 109.5 |
O3—C8—C9 | 119.8 (2) | C21B—C23B—H23E | 109.5 |
O3—C8—C13 | 120.2 (2) | H23D—C23B—H23E | 109.5 |
C9—C8—C13 | 120.0 | C21B—C23B—H23F | 109.5 |
C10—C9—C8 | 120.0 | H23D—C23B—H23F | 109.5 |
C10—C9—H9 | 120.0 | H23E—C23B—H23F | 109.5 |
C8—C9—H9 | 120.0 | C19B—C23C—H23G | 109.5 |
C9—C10—C11 | 120.0 | C19B—C23C—H23H | 109.5 |
C9—C10—H10 | 120.0 | H23G—C23C—H23H | 109.5 |
C11—C10—H10 | 120.0 | C19B—C23C—H23I | 109.5 |
C10—C11—C12 | 120.0 | H23G—C23C—H23I | 109.5 |
C10—C11—C14 | 119.90 (19) | H23H—C23C—H23I | 109.5 |
C12—C11—C14 | 119.99 (19) | C1—O1—Zn1ii | 129.9 (2) |
C13—C12—C11 | 120.0 | C1—O2—Zn1 | 125.0 (2) |
C13—C12—H12 | 120.0 | C5—O3—C8 | 118.5 (3) |
C11—C12—H12 | 120.0 | N1A—Zn1—O2 | 97.99 (11) |
C12—C13—C8 | 120.0 | N1A—Zn1—O5iii | 97.88 (12) |
C12—C13—H13 | 120.0 | O2—Zn1—O5iii | 88.61 (14) |
C8—C13—H13 | 120.0 | N1A—Zn1—O4iv | 101.70 (12) |
O4—C14—O5 | 124.6 (4) | O2—Zn1—O4iv | 87.04 (13) |
O4—C14—C11 | 117.7 (3) | O5iii—Zn1—O4iv | 160.35 (10) |
O5—C14—C11 | 117.7 (3) | N1A—Zn1—O1ii | 101.71 (11) |
C18A—N1A—C22A | 120.0 | O2—Zn1—O1ii | 160.30 (10) |
C18A—N1A—Zn1 | 126.48 (16) | O5iii—Zn1—O1ii | 88.45 (12) |
C22A—N1A—Zn1 | 113.42 (16) | O4iv—Zn1—O1ii | 89.22 (11) |
C19A—C18A—N1A | 120.0 | N1A—Zn1—N1B | 8.5 |
C19A—C18A—H18A | 120.0 | O2—Zn1—N1B | 105.34 (11) |
N1A—C18A—H18A | 120.0 | O5iii—Zn1—N1B | 93.62 (11) |
C20A—C19A—C18A | 120.0 | O4iv—Zn1—N1B | 106.02 (11) |
C20A—C19A—H19A | 120.0 | O1ii—Zn1—N1B | 94.28 (11) |
C18A—C19A—H19A | 120.0 | N1A—Zn1—Zn1ii | 178.25 (11) |
C19A—C20A—C21A | 120.0 | O2—Zn1—Zn1ii | 82.68 (7) |
C19A—C20A—C20Ai | 132.6 (4) | O5iii—Zn1—Zn1ii | 80.51 (7) |
C21A—C20A—C20Ai | 107.3 (4) | O4iv—Zn1—Zn1ii | 79.93 (7) |
C20A—C21A—C22A | 120.0 | O1ii—Zn1—Zn1ii | 77.63 (7) |
C20A—C21A—C23A | 123.4 (5) | N1B—Zn1—Zn1ii | 170.04 (10) |
C22A—C21A—C23A | 116.6 (5) | C14—O4—Zn1v | 127.6 (2) |
C21A—C22A—N1A | 120.0 | C14—O5—Zn1vi | 127.2 (2) |
Symmetry codes: (i) −x+1/2, −y+2, z; (ii) −x, −y+1, −z+1; (iii) x−1/2, −y+1, −z+1/2; (iv) −x+1/2, y, z+1/2; (v) −x+1/2, y, z−1/2; (vi) x+1/2, −y+1, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [Zn2(C14H8O5)2(C12H12N2)]·4H2O |
Mr | 899.5 |
Crystal system, space group | Orthorhombic, Pcca |
Temperature (K) | 296 |
a, b, c (Å) | 16.864 (4), 11.067 (2), 22.764 (4) |
V (Å3) | 4248.6 (14) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 1.20 |
Crystal size (mm) | 0.22 × 0.20 × 0.18 |
Data collection | |
Diffractometer | Bruker SMART APEX DUO CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2008) |
Tmin, Tmax | 0.781, 0.815 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 26264, 3849, 3314 |
Rint | 0.025 |
(sin θ/λ)max (Å−1) | 0.600 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.128, 1.06 |
No. of reflections | 3849 |
No. of parameters | 266 |
No. of restraints | 246 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.53, −0.50 |
Computer programs: SMART (Bruker, 2008), SAINT (Bruker, 2008), SHELXS97 (Sheldrick, 2008), SHELXL2014 (Sheldrick, 2015), DIAMOND (Brandenburg, 2005, SHELXTL (Bruker, 2008).
Zn1—N1A | 1.9971 (17) | Zn1—O4ii | 2.046 (3) |
Zn1—O2 | 2.017 (3) | Zn1—O1iii | 2.050 (3) |
Zn1—O5i | 2.040 (3) | ||
N1A—Zn1—O2 | 97.99 (11) | O5i—Zn1—O4ii | 160.35 (10) |
N1A—Zn1—O5i | 97.88 (12) | N1A—Zn1—O1iii | 101.71 (11) |
O2—Zn1—O5i | 88.61 (14) | O2—Zn1—O1iii | 160.30 (10) |
N1A—Zn1—O4ii | 101.70 (12) | O5i—Zn1—O1iii | 88.45 (12) |
O2—Zn1—O4ii | 87.04 (13) | O4ii—Zn1—O1iii | 89.22 (11) |
Symmetry codes: (i) x−1/2, −y+1, −z+1/2; (ii) −x+1/2, y, z+1/2; (iii) −x, −y+1, −z+1. |