CoTiO3 for highly efficient peroxymonosulfate activation: The critical role of Co–O–Ti bond for rapid redox cycles of Co2+/Co3+

Aiping Liang Chaolin Li Chen Ling Hengpan Duan Wenhui Wang

Citation:  Aiping Liang, Chaolin Li, Chen Ling, Hengpan Duan, Wenhui Wang. CoTiO3 for highly efficient peroxymonosulfate activation: The critical role of Co–O–Ti bond for rapid redox cycles of Co2+/Co3+[J]. Chinese Chemical Letters, 2025, 36(10): 110788. doi: 10.1016/j.cclet.2024.110788 shu

CoTiO3 for highly efficient peroxymonosulfate activation: The critical role of Co–O–Ti bond for rapid redox cycles of Co2+/Co3+

English

  • Advanced oxidation processes (AOPs) are widely applied in wastewater treatment especially for the efficient removal of refractory organic pollutants [1-3]. Amongst peroxymonosulfate (PMS) based homogeneous AOPs has been considered as a promising technique for wastewater remediation due to its strong ability to oxidize contaminants and produce long half-life periods of SO4•− [4-6]. However, the homogeneous system generally suffers from harsh pH environment requirement, large consumption of oxidant, extensive use of ionic catalysts at concentration dozens or even hundreds of times higher than their emission standard, and the excess slug production [7,8]. Thus, considerable efforts have been devoted to developing heterogeneous catalysts for PMS activation. Along this line, advanced heterogeneous catalysts such as Co-based catalysts [7,9], Fe-based catalysts [2,10-12] and metal–N–C [13-15] have been reported. Amongst, Co-based heterogeneous catalysts show excellent performance of activating PMS, but most of them are limited by insufficient utilization and regeneration rate of Co2+ (the active sites), as well as the leaching of the Co [16].

    In previous studies, two effective approaches have been proposed to solve the above issues. The first one is to disperse the Co-based catalysts on a host with large surface area and strong interaction with the catalysts, thus inhibiting the aggregation of catalysts and diminishing the possible Co leaching [17]. Another promising approach is to design Co-based composite metal oxide (e.g., perovskite catalysts [1], spinel catalysts [18] and double hydroxide catalysts [19]), which obviously improve the structural stability of catalysts from metal leaching. LaCoO3, a typical example of perovskite catalysts, was widely used due to its reasonable high stability and catalytic activity, however, intrinsic high state of Co (i.e., Co3+) in the farmwork hinders its continuous activation of PMS. As a matter of fact, perovskite AxByOz with low-state A-site metals as the active site would be more prone to donate electrons for catalytic activation. In addition, B-site metals are essential for the regeneration of the A-site active site and the structural stability of the catalyst [20,21].

    Based on above design principles, we herein proposed perovskite cobalt titanate (CoTiO3) as a promising PMS activator and suspected that the presence of Co–O–Ti bond would cause a strong interaction between Co and Ti, thus promoting the rapid transfer of electrons in the catalytic process. To verify the above hypothesis, CoTiO3 nanocatalyst was synthesized by a simple one-step hydrothermal method and employed as PMS activator. As a result, CoTiO3/PMS system removes 98.2% of hydroxychloroquine (HCQ, drugs for effective treatment of COVID-19) within 20 min at low dose of PMS (0.5 mmol/L), shows high tolerance to the environmental pH range (3.5–10.6) and significant versatility for various refractory organics. Combined with the material characterization and DFT calculations, the mechanism for the excellent catalytic performance of heterogeneous CoTiO3 was revealed. Furthermore, the possible degradation pathway of HCQ and toxicity studies of intermediate products in CoTiO3/PMS systems were proposed based on GCMS– and T.E.S.T. analysis. In addition, CoTiO3–CNT–PVDF membrane was designed to further demonstrate the practical application of the catalysts using continuous flow-through mode approach.

    X-ray diffraction (XRD) pattern of the obtained catalysts can be assigned to perovskite CoTiO3 (JCPDS No.15–0866) as shown in Fig. 1a, confirming its successful synthesis using a simple one-step hydrothermal method. X-Ray photoelectron spectroscopy (XPS) were collected to analyze the chemical states of elements in CoTiO3. As shown in Fig. 1b, both peaks with binding energies of 786.8 eV and 780.6 eV originated from Co2+ [18,22,23], which was usually reported as a highly active center for PMS activation. Two major peaks are observed at 458.6 eV and 463.9 eV for Ti 2p spectrum (Fig. 1c) [24], which can be assigned to Ti3+ and Ti4+ with percentage of 51.5% and 48.5%, respectively. In addition, the splitting energy of 5.7 eV between two Ti 2p peaks is well in agreement with the TiO6 octahedra [25,26]. The O 1s spectra of CoTiO3 consists of three peaks at 529.9, 531.4 and 532.7 eV (Fig. 1d), which can be assigned to the Co–O–Ti bond, oxygen vacancies and surface-bonded hydroxyl groups [27,28]. The Fourier transform infrared spectroscopy (FTIR) (Fig. 1e) reveal the vibration of Ti-O-Ti (800–500 cm−1) and Co–O–Ti (1091 cm−1) [29-32]. The structure was further investigated by Raman spectroscopy (Fig. 1f), where the vibration peaks at 521 cm−1 and 689 cm−1 can be assigned to symmetric bending motion of TiO6 and CoO6 octahedra, respectively [33,34]. It is worth noting that the formation of Co–O–Ti linkage and oxygen vacancy are beneficial to the electron transfer in the catalytic activation process, improving the redox cycle efficiency of Co/Ti, whose mechanism will be discussed in following parts. The scanning electron microscope (SEM) images in Fig. 1g demonstrates the nano-block morphology of CoTiO3 with lateral length less than 500 nm. The characteristic d-spacing of 0.2537 nm shown by HRTEM (Fig. 1h) can be assigned to (110) plane of CoTiO3. Moreover, the uniform elemental distribution with composition of CoTi0.99O3.03 was confirmed by energy dispersive X-ray spectroscopy (EDS) analysis, which is consistent with CoTiO3 (Fig. S1 in Supporting information).

    Figure 1

    Figure 1.  Material characterizations of CoTiO3. (a) XRD pattern (inset shows the crystal structure of CoTiO3). High-resolution XPS spectra of (b) Co 2p, (c) Ti 2p and (d) O 1s. (e) FTIR spectra. (f) Raman spectra. (g) SEM images. (h) HRTEM image (insets show TEM image and SAED pattern).

    The catalytic performance was evaluated by degradation of HCQ in CoTiO3/PMS system. As exhibited in Fig. 2a and Fig. S2 (Supporting information), CoTiO3/PMS system with low CoTiO3 and PMS dosages (i.e., 0.5 g/L and 0.5 mmol/L, respectively) can efficiently remove 98.2% of HCQ (10 mg/L) within 20 min, which is much faster than that of PMS (11.2%) or CoTiO3 (19.1%) alone. Besides, the degradation rate only reaches 62.3% in Co3O4/PMS systems under identical conditions, reflecting that monometallic cobalt oxide catalyst showed a significantly lower activity than CoTiO3. To further demonstrate the excellent degradation performance of CoTiO3/PMS system, it was compared with the well-known efficient homogeneous systems with same molar of ionic catalysts (i.e., Fe2+/PMS, Cu2+/PMS and Co2+-Ti4+/PMS). It is found that the degradation of HCQ followed the first-order reaction model (Fig. S3 in Supporting information). As shown in Fig. 2b and Fig. S4 (Supporting information), the degradation rate constant for CoTiO3/PMS system (0.5683 min−1) was higher than that of any reported homogeneous systems herein, including its homogenous counterpart with the same molar concentration of metal ions (i.e., Co2+-Ti4+/PMS system). The above results demonstrate that there is no synergistic effect between Co2+ and Ti4+ in the homogeneous system, while in the heterogeneous CoTiO3, the presence of Co–O–Ti accelerates the electron transfer within the system, which is more conducive to the catalytic process. Besides, we also found that the pH of CoTiO3/PMS system is maintained in the neutral environment (pH mainly lies between 6 and 7), while the Co2+-Ti4+/PMS system lies in a strong acidic environment with pH range between 3 and 3.5 as shown in Fig. S5 (Supporting information). As is well-known, strong acid environment would inhibit the oxidation ability of the generated OH [35], so the Co2+-Ti4+/PMS system exhibits lower degradation efficiency. Moreover, the mineralization efficiency of HCQ within 20 min is as high as 71.6% (Fig. 2c), demonstrating the strong oxidation capacity of CoTiO3/PMS system. More importantly, the CoTiO3/PMS system can degrade more than 90% of HCQ within 20 min after 5 cycling experiments and the leaching amount of Co ions is always less than 0.25 mg/L, which is lower than environmental standard stipulated by European Union (1 mg/L) [36], clearly demonstrating its good reusability and stability (Fig. 2d and Fig. S6 in Supporting information). As is well-known, the practical application of homogenous PMS system is significantly hindered by the harsh requirement on environmental pH and massive production of heavy metal-containing sludge [37]. In stark contrast, the CoTiO3/PMS system possesses high tolerance to the environmental pH and the removal efficiency of 10 mg/L HCQ at 20 min is higher than 80% in the pH range of 3.5–10.6 (Fig. 2e and Fig. S7 in Supporting information). Furthermore, the versatility of CoTiO3/PMS system is also confirmed by the efficient degradation of several typical organic pollutants like endocrine disruptor (i.e., BPA), pharmaceutical (i.e., CBZ), antibiotic (i.e., SMX), and dye (i.e., MB) as shown in Fig. 2f and Fig. S8 (Supporting information). The degradation rate of above pollutants by CoTiO3/PMS system can achieve higher than 85% in a short period of time (< 20 min). In addition, it is worth mentioning that the CoTiO3/PMS system can maintain the high catalytic performance in the presence of common ionic and organic species (i.e., CO32− (0–10 mmol/L), Ca2+ (0–5 mmol/L) and humic acid (HA, 0–20 mg/L)) (Fig. S9 in Supporting information). All these results clearly demonstrate that the CoTiO3/PMS system holds great potential regarding to the practical application in organic wastewater treatment.

    Figure 2

    Figure 2.  (a) Degradation efficiencies of HCQ and (b) the first order kinetic reaction rate constant in first 5 min in different systems. (c) Total organic carbon (TOC) removal of HCQ in CoTiO3/PMS system. (d) Cycle experiments of CoTiO3/PMS conducted with recycled CoTiO3. (e) The influence of initial pH on HCQ degradation in CoTiO3/PMS system. (f) Degradation of different pollutants in CoTiO3/PMS system.

    The linear sweep voltammetry (LSV) result shows distinctly increased current after adding PMS in pure CoTiO3 suspension, indicating efficient electron transfer between CoTiO3 and PMS for generating reactive species (Fig. 3a). EPR measurement was carried out with DMPO trapping agent to verify the existing radicals in CoTiO3/PMS system. As shown in Figs. 3b and c, the characteristic signals of DMPO–SO4•–, DMPO–OH and DMPO–O2•− can be clearly seen during the reaction process in CoTiO3/PMS system, confirming the presence of SO4•−, OH and O2•−. Meanwhile, the typical three-line spectra (1:1:1) of stable TEMP-1O2 was not observed in EPR test, indicating little 1O2 is produced in the system (Fig. S10 in Supporting information). To further reveal the major reactive species in HCQ degradation over CoTiO3/PMS system, a series of quenching experiments were conducted. As shown in Figs. 3d and e, with the addition of MeOH (OH and SO4•− quencher, 100 mmol/L) [38] and TBA (OH quencher, 100 mmol/L) [39], the degradation efficiency of HCQ in CoTiO3/PMS system was decreased by 76.2% and 33.1%, respectively. Moreover, upon the addition of BQ (O2•− quencher, 4 mmol/L) [40] in CoTiO3/PMS system, the HCQ degradation efficiency is decreased by 23.3%. With the addition of FFA (1O2 quencher, 100 mmol/L), the degradation efficiency of HCQ was just decreased by 2%, suggesting a negligible degradation contribution from non-free radical pathways enabled by 1O2. The above results clearly indicate SO4•− and OH are the major reactive species for HCQ degradation in CoTiO3/PMS system, while O2•− showed slight contribution. The overall contribution is as follows: SO4contribution•− > OHcontribution > O2contribution•−. Furthermore, the concentration evolution of major reactive oxidation species (i.e., SO4•− and OH) in CoTiO3/PMS and Co2+-Ti4+/PMS during the activation process were monitored by EPR. As shown in Fig. S11 (Supporting information), the amount of DMPO-SO4•− and DMPO-OH in the homogeneous system decreased significantly in 10 min. In contrast, the free radicals in CoTiO3/PMS system were found to increase gradually over the same time period as shown in Fig. 3f and Fig. S10, verifying the continuous catalysis of CoTiO3 due to the fast regeneration of its active site.

    Figure 3

    Figure 3.  (a) LSV curves of CoTiO3 with/without PMS and HCQ. EPR spectra of (b) SO4•−, OH and (c) O2•− in CoTiO3/PMS system using DMPO trapping agent at different time intervals. (d) Removal efficiency and (e) inhibition ratio of HCQ degradation in the presence of different quenchers and (f) the corresponding quantitative concentration of SO4•− and OH in CoTiO3/PMS system using DMPO trapping agent at different time intervals.

    To uncover the mechanism of the excellent catalytic performance of CoTiO3 in activating PMS, the adsorption/activation of PMS on CoTiO3 were explored by performing density functional theory (DFT) calculations. Computational details can be found in Supporting information. As shown in Fig. 4a, dynamic catalytic process for PMS activation via CoTiO3 with high exposure of (104) facets was revealed. The HSO5 was randomly placed on the CoTiO3 at the beginning, but it adsorbed on Co sites and Ti sites, thus forming a cyclic electron chain by HSO5- and Co–O–Ti together. Afterwards, the HSO5- was activated to form SO4•− and OH via breaking the O–O bond. We also have found that the energy of product was much lower than that of the reactant (Fig. 4b), revealing that the PMS activation is favorable in thermodynamics, which is consistent with the superior catalytic performance of CoTiO3. Furthermore, the Bader charge results indicate that the valence electrons of Co sites decreased significantly after PMS activation, while only a slight number of valence electrons were transferred at Ti site. Due to the higher density of electron clouds around Co, it is more inclined to act as an electron "supplier" to PMS, while Ti acts as a "feeder" and transmits its electrons through Co–O–Ti bond (Fig. 4c and Fig. S12 in Supporting information). Besides, the valence electrons on HSO5- before and after activation is −0.524 and −1.755, respectively. Based on the above theoretical calculations, it is clear that the PMS is efficiently activated to generate SO4•− and OH by accepting the electrons from CoTiO3 (~1.231 eV).

    Figure 4

    Figure 4.  (a) Adsorption and activation of HSO5. (b) Gibbs free energy (△G) of different states of HSO5 on CoTiO3 crystal. (c) Analyse of Bader charge before and after activation.

    To confirm the understanding based on DFT calculations, the high resolution XPS spectra before and after activation PMS were explored. As can be seen in Fig. 5a, the percentage of Co2+ in the catalyst after use for 5 degradation cycles decreased from 100% to 53.1%, respectively, as they donate electrons to activate PMS (Eq. 1). This analysis is supported by the fact that the oxidation potential of CoTiO3 (~0.28 V, Fig. 5d) is even much lower than that oxidation potential of the common efficient ionic catalysts (e.g., Co2+, Fe2+ and Cu2+), confirming its stronger electron-donating capacity [41-43]. On the other hand, Co2+ still maintained a high proportion (i.e., 53.1%) after 5 degradation cycles, indicating its efficient regeneration, which is also supported by the continuous decomposition of PMS in the CoTiO3/PMS system (Fig. S13 in Supporting information) and excellent cycle stability for HCQ degradation. Meanwhile, Figs. 5b and c showed the slight decrease of Ti3+ (from 52.7% to 43.9%) and surface oxygen (from 24.2% to 18.7%) on the used CoTiO3, which is mainly due to the regeneration of Co2+ through the bridge of Co–O–Ti bond (Fig. S14 in Supporting information).

    Figure 5

    Figure 5.  XPS spectra of the fresh CoTiO3 and used CoTiO3 after 5 degradation cycles: (a) Co 2p, (b) Ti 2p and (c) O 1s. (d) The CV curve of CoTiO3. (e) Schematic illustration of PMS activation for HCQ removal.

    Combined with the material characterization and DFT calculations, CoTiO3 catalyst is expected to work as follows during the PMS activation. First and foremost, the formation of Co–O–Ti bond (as verified by FTIR, Raman and XPS analysis) induces the higher electron density of Co site, leading to the formation of Co2+, which in return serves as active sites to contribute electrons for PMS activation [41]. During this process, SO4•− and OH could be generated for HCQ removal (Eqs. 1 and 2). Then, according to the standard reduction potentials in Langes' Chemistry Handbook (Eqs. 3-5), the reduction potential of Co3+ is 1.82 V, while Ti3+ is involved, the E0 decreases to 1.63 V. Therefore, the reduction of Co3+ by Ti3+ is more thermodynamically feasible, verifying catalysts containing Co–O–Ti bond could provide fast regeneration of Co2+ [34,44]. Finally, Ti4+ further efficiently reacts with HSO5 to achieve recovery (Eq. 6) [45]. In addition, the regeneration of Co2+ can be also achieved through the reduction by PMS and electron-rich intermediates (i.e., Os, Eq. 7) [7,46], which reduces the amount of surface oxygen on the used CoTiO3. Based on the above investigations, it can be concluded that the formation of Co–O–Ti linkage facilitates the rapid recycling of Co2+/Co3+ on CoTiO3, enabling continuously efficient activation of PMS. Schematic illustration of CoTiO3 activated PMS for HCQ removal is shown in Fig. 5e. In addition, fast regeneration of Co2+ ensures the high concentration of SO4•− and OH produce, thus making HCQ more inclined to be converted into low or non-toxic products as confirmed by the degradation pathway and toxicity analysis (Figs. S15 and S16 in Supporting information).

    $ \mathrm{Co}^{2+}+\mathrm{HSO}_5^{-} \rightarrow \mathrm{Co}^{3+}+\mathrm{SO}_4^{\bullet-}+\mathrm{OH}^{-} $

    (1)

    $ \mathrm{SO}_4^{\bullet-}+\mathrm{OH}^{-} \rightarrow \mathrm{SO}_4^{2-}+\;^{\bullet}\mathrm{OH} $

    (2)

    $ \mathrm{Co}^{3+}+\mathrm{e}^{-} \rightarrow \mathrm{Co}^{2+}, E^0=1.82 \mathrm{~V} $

    (3)

    $ \mathrm{Ti}^{4+}+\mathrm{e}^{-} \rightarrow \mathrm{Ti}^{3+}, E^0=0.19 \mathrm{~V} $

    (4)

    $ \mathrm{Co}^{3+}+\mathrm{Ti}^{3+} \rightarrow \mathrm{Co}^{2+}+\mathrm{Ti}^{4+}, E^0=1.63 \mathrm{~V} $

    (5)

    $ \mathrm{Ti}^{4+}+\mathrm{HSO}_5^{-}+\mathrm{H}^{+}+\mathrm{V}_{\mathrm{O}}^{\bullet \bullet} \rightarrow \mathrm{Ti}^{3+}+\mathrm{SO}_5^{\bullet-}+\mathrm{H}^{+}+\mathrm{O}_{\mathrm{O}}^{\times} $

    (6)

    $ \mathrm{Co}^{3+}+\mathrm{HSO}_5^{-}+\mathrm{H}^{+}+\mathrm{V}_{\mathrm{O}}^{\bullet \bullet} \rightarrow \mathrm{Co}^{2+}+\mathrm{SO}_5^{\bullet-}+\mathrm{H}^{+}+\mathrm{O}_{\mathrm{O}}^{\times} $

    (7)

    where $\mathrm{V}_0^{\bullet \bullet}$ is the double-charged oxygen vacancy, and $\mathrm{O}_{\mathrm{O}}^{\times}$ is the oxygen ion in CoTiO3.

    The separation and recovery of powder catalysts are key challenges limiting the practical applications of heterogenous AOPs. To this end, CoTiO3–CNT–PVDF catalytic membrane reactor was designed to demonstrate its ability to remove microcontaminants in wastewater via continuous flow-through mode (Fig. 6a). As shown in Fig. 6b and Fig. S17 (Supporting information), the HCQ could be efficiently degraded (> 90%) through continuous flow within 540 min via CoTiO3–CNT–PVDF membrane with little cobalt ion leaching. The excellent catalytic performance is consistent with the catalyst agglomeration-free property of the membrane, which enables the efficient use of the catalyst (Fig. S18 in Supporting information). Furthermore, compared with previously developed membrane-based AOPs (Fig. 6c and Table S3 in Supporting information), the CoTiO3–CNT–PVDF membrane/PMS system delivers a highest removal efficiency and longest operation duration for degrading various organic pollutants. To understand the excellent stability, the XRD patterns and SEM images of the composite membrane were collected before and after the reaction. As shown in Fig. 6d, the crystal structure of the membrane is well maintained after long time operation, although the peak intensity slightly decreases. Fig. 6e shows the membrane morphology and skeleton are well maintained after the reaction, which is consistent with the superior stability of the membrane reactor. It can be concluded that when the catalysts, PMS and pollutant are confined together in the channel of membrane, the generated active species would quickly interact with the pollutant in situ, so as to accurately and effectively remove the pollutant.

    Figure 6

    Figure 6.  (a) Schematic diagram of the preparation of CoTiO3–CNT–PVDF membrane. (b) HCQ degradation efficiency of CoTiO3–CNT–PVDF membrane. (c) Comparison of CoTiO3–PVDF–CNT membrane/PMS system with previously developed catalytic membranes in Table S2 (Supporting information). (d) XRD patterns and (e) SEM images of CoTiO3–CNT–PVDF membrane before and after reaction.

    To sum up, in CoTiO3/PMS system, Co is more inclined to act as an electron "supplier" to PMS due to its higher electron density, while Ti acts as a "feeder" and transmits its electrons through Co–O–Ti bond to ensure cobalt regeneration, then facilitating the redox cycle of Co2+/Co3+ during PMS activation and thus accelerating the superior degradation of various pollutants. In practical application demonstration, a designed CoTiO3–CNT–PVDF membrane reactor can effectively remove HCQ pollutant via practically feasible filter-through mode, whose performance is superior to previously developed membrane-based AOPs. This work reports a catalytic model of CoTiO3–PVDF membrane/PMS, which provides new strategies for the continuous, rapid, economical and stable removal of stubborn contaminants from wastewater.

    The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

    Aiping Liang: Writing – review & editing, Writing – original draft, Resources, Methodology, Investigation. Chaolin Li: Writing – review & editing, Supervision. Chen Ling: Methodology, Investigation. Hengpan Duan: Methodology, Investigation. Wenhui Wang: Conceptualization, Writing – review & editing, Supervision, Funding acquisition.

    This work was supported by the National Natural Science Foundation of China (Nos. 52100084 and 52170155) and Shenzhen Natural Science Fund (the stable support plan program, No. GXWD20231129152058003).

    Supplementary material associated with this article can be found, in the online version, at doi:10.1016/j.cclet.2024.110788.


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  • Figure 1  Material characterizations of CoTiO3. (a) XRD pattern (inset shows the crystal structure of CoTiO3). High-resolution XPS spectra of (b) Co 2p, (c) Ti 2p and (d) O 1s. (e) FTIR spectra. (f) Raman spectra. (g) SEM images. (h) HRTEM image (insets show TEM image and SAED pattern).

    Figure 2  (a) Degradation efficiencies of HCQ and (b) the first order kinetic reaction rate constant in first 5 min in different systems. (c) Total organic carbon (TOC) removal of HCQ in CoTiO3/PMS system. (d) Cycle experiments of CoTiO3/PMS conducted with recycled CoTiO3. (e) The influence of initial pH on HCQ degradation in CoTiO3/PMS system. (f) Degradation of different pollutants in CoTiO3/PMS system.

    Figure 3  (a) LSV curves of CoTiO3 with/without PMS and HCQ. EPR spectra of (b) SO4•−, OH and (c) O2•− in CoTiO3/PMS system using DMPO trapping agent at different time intervals. (d) Removal efficiency and (e) inhibition ratio of HCQ degradation in the presence of different quenchers and (f) the corresponding quantitative concentration of SO4•− and OH in CoTiO3/PMS system using DMPO trapping agent at different time intervals.

    Figure 4  (a) Adsorption and activation of HSO5. (b) Gibbs free energy (△G) of different states of HSO5 on CoTiO3 crystal. (c) Analyse of Bader charge before and after activation.

    Figure 5  XPS spectra of the fresh CoTiO3 and used CoTiO3 after 5 degradation cycles: (a) Co 2p, (b) Ti 2p and (c) O 1s. (d) The CV curve of CoTiO3. (e) Schematic illustration of PMS activation for HCQ removal.

    Figure 6  (a) Schematic diagram of the preparation of CoTiO3–CNT–PVDF membrane. (b) HCQ degradation efficiency of CoTiO3–CNT–PVDF membrane. (c) Comparison of CoTiO3–PVDF–CNT membrane/PMS system with previously developed catalytic membranes in Table S2 (Supporting information). (d) XRD patterns and (e) SEM images of CoTiO3–CNT–PVDF membrane before and after reaction.

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  • 发布日期:  2025-10-15
  • 收稿日期:  2024-06-18
  • 接受日期:  2024-12-19
  • 修回日期:  2024-11-08
  • 网络出版日期:  2024-12-20
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