Yuquan
Feng
*,
Linxia
Lv
,
Dongqin
Bi
,
Zhiguo
Zhong
,
Jing
Li
,
Zilong
Yue
,
Zhaoge
Zeng
,
Shuhan
Zhang
and
Zhaohui
Meng
College of Chemistry and Pharmacy Engineering, Nanyang Normal University, Nanyang 473061, China. E-mail: yqfeng2008@126.com; Fax: +86 377 6351 3583; Tel: +86 377 6351 3583
First published on 15th December 2021
A novel open-framework borate-rich cadmium borophosphate has been obtained by the boric acid reflux method. The compound exhibits a complicated network which is composed of CdO6 octahedra and an interesting 1D wheel-shaped anion, ∞{[BO2(OH)]3B6P6O27}12n−, built from trigonal-planar BO2(OH), tetrahedral BO4 and PO4 units. This work not only features the first open-framework borate-rich (B/P > 1) cadmium borophosphate, but also exhibits its excellent ion-exchange capacities with Na+ cations and efficient photocatalytic activities for the degradation of reactive brilliant red (X3B).
X-ray structural analysis indicated that 1 crystallizes in the centrosymmetric hexagonal crystal system with the space group P63/m (no. 176), and its whole structure can be regarded as a 3D open-framework built by alternating linkage of CdO6 octahedra, BO4, {BO2(OH)} and PO4 group units via shared corners. The asymmetric structural unit of 1 consists of one independent Cd site, two B sites, one P site, six O sites, one –OH group and two water molecules, as well as one K site and two Na sites acting as counteracting cations. Fig. 1 shows the coordination environment of the Cd(1), B(1), B(2) and P(1) sites. The Cd2+ cation is six-coordinated by six O atoms to generate a slightly distorted octahedron with Cd–O bond distances ranging from 2.222(10) to 2.370(9) Å.1b,7 The B(1) and B(2) atoms exhibit two different coordination modes: the B(1) atom is tetrahedrally coordinated by four oxygen atoms [O(1), O(2), O(3) and O(6)], while the B(2) atom is triangularly coordinated by two oxygen atoms [O(6) and O(6)i; i = x, y, 1/2 − z] and one –O(7)H group resulting in a trigonal-planar {BO2(OH)} unit. The P(1) atom adopts four O atoms [O(2), O(3), O(4) and O(5)] leading to a tetrahedral geometric configuration. The B–O bond lengths range from 1.346(14) to 1.507(17) Å, and the P–O bond distances lie between 1.503(9) and 1.552(9) Å.3 The abovementioned Cd–O, B–O and P–O bond lengths are all in their expected ranges and comparable with those observed in known borophosphates.4 The results of bond valence calculations9 revealed that the oxidation states of cadmium, boron and phosphorus sites are in their normal valence +II, +III and +V, respectively. The O(7) sites are protonated hydroxyl groups (–OH groups), while the other O atoms are in their normal oxidation state −II.
Two BO4 units and one {BO2(OH)} unit are connected by sharing oxygen atoms to yield a {B3O7(OH)} trimer, and the {B3O7(OH)} trimer is linked with the surrounding two PO4 groups, resulting in a cluster {B3P2O11(OH)} which can be regarded as the FBU of the borophosphate anion (Fig. S1†). These adjacent FBUs are further extended via O atoms from the PO4 groups into a 1D wheel-shaped borophosphate anion, ∞{[BO2(OH)]3B6P6O27}12n− (Fig. 2). The 1D wheel-shaped borophosphate anion contains {B6P6} 12-MRs which are constructed by the alternating linkage of six BO4 groups and six PO4 groups. The size of {B6P6} 12-MR is 7.9160(16) Å × 8.9966(13) Å. Within the borophosphate anion ∞{[BO2(OH)]3B6P6O27}12n−, {B6P4} 10-MR (9.6307(17) Å × 5.7595(9) Å) that is constructed from six BO4 groups from four different {B3O7(OH)} trimers and four PO4 groups can be observed along the a-axis (Fig. 3). In other words, each PO4 group is connected to two neighboring {B3O7(OH)} trimers, while each {B3O7(OH)} trimer is surrounded by four adjacent PO4 groups. Then the borophosphate anion ∞{[BO2(OH)]3B6P6O27}12n− is further connected with the Cd2+ cations by bridging O atoms, forming a 3D open-framework structure (Fig. 4). In the open-framework, each Cd2+ cation is bonded to two adjacent borophosphate anions, and each borophosphate anion is linked to six Cd2+ cations. In order to better study the connection modes of the open-framework structure, a topological approach10 was applied to simplify such a 3D architecture. If each {B3O7(OH)} trimer was viewed as a single node, the 3D structure could be simplified as a 6-, 6- and 4-connected topological network. The topological structure for the open-framework along the c-axis is shown in Fig. 5.
Fig. 2 View of the wheel-shaped borophosphate anion ∞{[BO2(OH)]3B6P6O27}12n− containing {B6P6} 12-MR along the c-axis. Colour codes: B(1) and B(2): green; P(1): rose; O atoms: red. |
Fig. 3 View of the 1D borophosphate anionic chain exhibiting {B6P4} 10-MR along the a-axis. Colour codes: BO2(OH) and BO4: green; PO4: rose; 10-MR: yellow. |
The EDS experimental analysis shows that 1 consists of the Cd, K, Na, P, B and O elements (Fig. S2†). The result is in good agreement with that of X-ray structural analysis. In order to confirm the purity of the as-synthesized products, the powder XRD pattern of 1 was obtained. The results revealed that the experimental powder XRD pattern is in agreement with the simulated pattern of the single-crystal structure (Fig. S3†). In addition, the IR spectrum of 1 was studied between 400 and 4000 cm−1 (KBr pellet) (Fig. S4†). The peaks at 3455 and 1641 cm−1 can be assigned to the stretching and bending vibrations of the –OH units (water molecules and BO2(OH) groups). The peaks at 1403 and 1267 cm−1 can be ascribed to the stretching and bending vibrations of the BO3 groups. The peaks at 1013, 852 and 614 cm−1 are attributed to the symmetric stretching and bending vibrations of the BO4 groups, respectively. The peaks at 1115 and 928 cm−1 and 810, 674, 560 and 555 cm−1 are attributed to the asymmetric stretching and bending vibrations of the P–O bonds, respectively.8a,e Furthermore, the peaks at 470 and 419 cm−1 can be assigned to the K–O and Na–O bonds.
The UV-vis diffuse-reflectance spectrum of 1 was obtained on a UH4150 spectrophotometer. According to the absorbance data between 200–800 nm, an (ahv)2versus optical energy (hv) curve was generated by means of the Tauc plot method and is shown in Fig. 6. The optical band gap of 3.79 eV of 1 (UV absorption cutoff edge: 327 nm) is comparable to that of the borophosphate compound Na3Cd3B(PO4)4 (3.44 eV and 360 nm).1b Moreover, the luminescence properties of 1 in the solid-state were also studied at RT (Fig. S5†). Upon excitation at 225 nm, strong emission occurs with the maximum at 342 nm. The emission may be ascribed to the {BO2(OH)}, BO4 and PO4 groups in the borophosphate anion ∞{[BO2(OH)]3B6P6O27}12n−. The results of the luminescence test are also in agreement with those of UV-vis diffuse-reflectance. The CIE chromaticity coordinate (x, y) is calculated according to the emission peak. Fig. S6† shows the CIE (1931) chromaticity diagram of 1. The x and y values are 0.234 and 0.226, respectively, which are located in the blue region. In addition, the lifetime of 1 (Fig. 7) has also been studied (λex = 225 nm and λem = 342 nm). The plot of counts versus time could be well fitted according to the double-exponential equation [I = A1exp(−t/τ1) + A2exp(−t/τ2)] with a calculated τ value of 1.74 ns.
The ion-exchange capacities of 1 with Na+ cations have been studied. The crystalline sample of 1 (0.014 g) and 0.1 mmol Na+ ions (0.179 g Na2HPO4·12H2O/5.84 mg NaCl/8.50 mg NaNO3/13.6 mg CH3COONa·3H2O) were placed in a Teflon-lined stainless-steel autoclave (50 mL) at 220 °C for 12 hours.11 The ion-exchanged crystals were repeatedly washed with deionized water and detected by EDS (Fig. S7†), ICP-MS and PXRD (Fig. S3†), and the experimental result reveals that the K+ cations in 1 can be completely exchanged with the Na+ cations and the structure can remain stable after the ion-exchange experiment.
The thermal stability of 1 was studied in the range of 30–900 °C with a heating rate of 10 °C min−1 in a dynamic N2 atmosphere (gas flow: 0.1 L min−1). The experimental results indicate a total mass loss of 4.55% between 81 and 769 °C in two steps (Δmcalcd/m = 4.52%) (Fig. S8†). In the first step, between 81 and 437 °C, the weight is reduced by 1.24%, which corresponds to the release of one water molecule (Δmcalcd/m = 1.27%). In the second step, between 437 and 769 °C, the weight decreases by 3.31%, which is attributed to the loss of one water molecule and three –OH groups (2.5 water molecules, Δmcalcd/m = 3.25%).8e The loss of three –OH groups was observed in the second step, indicating that the decomposition of the open-framework should occur in this stage. In order to better confirm the composition of the final product after thermal analysis, EDS experimental analysis was performed. The results reveal that the final product may be metallic oxide containing Na, K, Cd, P, B and O elements.
Considering the fact that colourless borophosphate probably exhibits photocatalytic activities, we are interested in investigating its photocatalytic properties for the degradation of organic complexes. The catalyst photoactivity was evaluated by using X3B (the reactive brilliant red) degradation in water as a model reaction. The UV light source was a high-pressure mercury lamp (375 W) equipped with Pyrex glass. The experiment was carried out in a thermostated reactor under fixed conditions (1.00 g L−1 catalyst, 40 ppm X3B, and 10 mM H2O2). At the given intervals of light irradiation, small aliquots were taken and filtered through a membrane (0.22 μm). The X3B concentration in solution was analyzed by measuring its maximal absorbance at 511 nm using a V2200 spectrometer.
Due to the fact that reactive brilliant red (X3B) is hardly adsorbed on catalyst 1, all the suspensions containing the necessary components were first sonicated for 5 min and shaken in the dark for 30 min to achieve equilibrium before light irradiation. Fig. 8 shows the curve for the degradation of X3B under different conditions in aqueous solution. The results reveal that X3B itself degrades slightly under UV light (curve b), which is due to the fact that the dye itself can absorb light and undergo photolysis. In aqueous solution, the photodegradation of organic complexes is very slow due to the inability to reduce O2 by the conduction electrons on the irradiated catalyst (curve c). The organic complexes degrade more rapidly when H2O2 is present (curve d), which is in good agreement with the fact that H2O2 is a better electron acceptor than O2. It can capture the conduction electrons of the catalyst and produce an active species, ˙OH, which can mineralize most organic pollutants.12 The control experiments show that the organics were not degraded or degraded very slowly in the absence of light or in the absence of a catalyst (curves a and d), respectively. This indicates that the Fenton-like reaction between H2O2 and the catalyst is not efficient, and it is very difficult to photolyze H2O2 directly under the present conditions. In the presence of both the catalyst and H2O2, the degradation of organics under light is very obvious (curve e).
Fig. 8 Time profiles of X3B degradation under different conditions: (a) 1 + H2O2 + dark; (b) O2 + UV; (c) 1 + O2 + UV; (d) H2O2 + UV; (e) 1 + H2O2 + UV. |
For practical use in water treatments, the catalyst stability is also an important factor to be considered. For this concern, recycling experiments were performed for X3B degradation under UV light irradiation under the same conditions as described above. After each run was completed, 6.0 mL of stock solution with X3B (40 ppm) and H2O2 (10 mM) was supplied to restore the initial concentration, and then the same steps were repeated. The catalyst activity was still excellent even after six runs (Fig. 9), and the reaction rate just slightly decreased from one run to another. Such a decrease in the reaction rate may be attributed to the gradually decreased catalyst concentration and the effection of intermediates. The result shows that the catalyst has a high stability during the recycling experiments, and 1 can act as an efficient catalyst for the degradation of reactive brilliant red (X3B).
Fig. 9 Recycling experiment for X3B degradation under UV light in the presence of H2O2 over 1 in aqueous solution. |
In summary, a novel 3D open-framework borate-rich cadmium borophosphates with B/P > 1 was prepared through the boric acid flux method. The UV-vis diffuse-reflectance spectrum reveals an optical band gap of 3.79 eV and a UV absorption cutoff edge at 327 nm. 1 shows a strong emission peak at 342 nm with a lifetime of 1.74 ns upon excitation at 225 nm. The ion-exchange experiment reveals that the K+ cations in 1 can be completely exchanged with the Na+ cations in a Teflon-lined stainless-steel autoclave (50 mL) at 220 °C for 12 hours. Moreover, 1 exhibits efficient photocatalytic activities for the degradation of reactive brilliant red (X3B). This is the first example of the use of metal borophosphate as the catalyst for photocatalytic degradation in the series of borophosphates. This work indicates that 1 can act as a new potential photocatalytic material. The successful synthesis of 1 predicts that more open-framework cadmium borophosphates with attractive structural features and applications would be prepared in the near future.
Footnote |
† Electronic supplementary information (ESI) available: Supporting figures: the FBU of the borophosphate anion, EDS, PXRD for 1, IR, luminescence curve, CIE (1931) chromaticity diagram, TG curve, BVS and the selected bond lengths and angles (CCDC: 2112879). For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1ce01449h |
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