 Open Access Article
 Open Access Article
Shuyan Gong†
ab, 
Anqi Wang†ab, 
Jilai Zhanga, 
Jian Guana, 
Ning Han *abc and 
Yunfa Chen
*abc and 
Yunfa Chen *abc
*abc
aState Key Laboratory of Multiphase Complex Systems, Institute of Process Engineering, Chinese Academy of Sciences, Beijing 100190, PR China
bCenter of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, No. 19A Yuquan Road, Beijing 100049, PR China
cCenter for Excellence in Regional Atmospheric Environment, Institute of Urban Environment, Chinese Academy of Sciences, Xiamen 361021, PR China
First published on 31st January 2020
Nowadays, it is necessary and challenging to prepare Cu2O in a large scale for various applications such as catalysis due to its excellent properties. Here, gram-scale Cu2O with nm size is successfully prepared using a simple liquid-phase reduction method at 25 °C. The amount of NaOH is found to be the key factor to determine the particle size of Cu2O by modifying the complexation and reduction reactions. The obtained ultra-fine Cu2O exhibits high performance of >95% efficiency for removing high-concentration (3000 ppm) ozone at 25 °C and even at a high relative humidity (RH) of 90% for more than 8 h. Furthermore, the Cu2O nanoparticles are coated onto an aluminium honeycomb substrate to form a monolithic catalyst, which shows high ozone removal efficiency of >99% in dry air and >97% in 90% RH for >10 h at a space velocity of 8000 h−1. The high performance could be attributed to the enhanced release of the ozone decomposition intermediate by the small size of Cu2O, as verified by O2 temperature-programmed desorption and X-ray photoelectron spectroscopy. All these results show the industrial promise of the large scale synthesis of ultrafine Cu2O applicable for high-performance ozone removal.
Although ozone is thermodynamically unstable, it decomposes slowly below 523 K without a catalyst. Catalytic decomposition has realized the catalytic removal of ozone at 25 °C and has become the focus of current research because of its high decomposition efficiency, safety and economy. The active components of the catalyst mainly include noble metals13–15 and transition metal oxides.16–19 Imamura et al. reported that p-type semiconductors have higher decomposition efficiency for ozone than n-type semiconductors.20 Oyama measured the conductivity of the catalyst by the Hall effect and compared the correlation between oxide activity and conductivity, thereby further confirming that the p-type semiconductor oxide has higher activity for the catalytic decomposition of ozone.21 Cu2O is a typical p-type semiconductor oxide, and intensive efforts have been focused on the shape and size control of Cu2O.22–24 In general, Cu2O particles with various morphologies can be produced by different synthetic methods, including thermal decomposition,25 solvothermal synthesis,26 hydrothermal method,27 polyol synthesis,28 seed-mediated chemical deposition,29 and liquid-phase reduction.30 It has been found that Cu2O with a smaller particle size tends to exhibit higher performance for ozone degradation.31 However, there is still much work to do for the development of the Cu2O catalyst, particularly in terms of large-scale synthesis and size reduction. For example, for good morphology control, one of the difficulties is the small amount of precursor solutions used for Cu2O synthesis, which induces a low yield.32 Another one is the dilution of precursor solutions and the use of surfactants such as oleic acid, poly(vinylpyrrolidone), or sodium dodecyl sulfate, due to which the products need to be thoroughly washed with water and ethanol to remove the residual surfactants and byproducts. This process is not only energy-intensive, but also causes high wastewater emission as the output increases. Therefore, it is urgent and challenging to controllably synthesize Cu2O with large scale production and high catalytic performance.
In this method, the large-scale synthesis of fine Cu2O nanoparticles with a production of above 20 grams in an experimental batch is achieved using highly concentrated precursor solutions, which may meet the criteria for practical applications. Importantly, the obtained Cu2O displays complete removal of ozone to 1000 ppm at 25 °C both in dry flow and high relative humidity levels (ca. 90%). The ozone conversion could still be above 99% and 95% in dry flow and RH 90%, respectively, for high-concentration 3000 ppm ozone. Finally, the prepared Cu2O is processed on an Al honeycomb substrate and exhibits high elimination efficiency and stability for ozone decomposition, which shows great potential for practical applications.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2, 1
2, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 and 1
2.5 and 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5.
5.
Fabrication of Cu2O–Al honeycomb: 0.2 g Cu2O powder was slurried in 10 g Al2O3 sol. Al honeycomb (1 mm pore and 20 mm thickness) was precipitated in the slurry several times, and the final product was dried at 25 °C in a fume hood. The weight of the Al honeycomb was measured before and after coating, and the active material (defined as the weight of all additives: Al2O3 sol and Cu2O powder) weight was determined by calculating the difference.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 mL g−1 h−1 with a total gas flow of 200 mL min−1. The ozone conversion was calculated as 100% × (Cinlet − Coutlet)/Cinlet. The test of moisture-resistance properties was produced by bubbling water with the airflow, and the relative humidity (RH) was measured by a humidity and temperature sensor meter (center 310 RS-232, TES, Taiwan).
000 mL g−1 h−1 with a total gas flow of 200 mL min−1. The ozone conversion was calculated as 100% × (Cinlet − Coutlet)/Cinlet. The test of moisture-resistance properties was produced by bubbling water with the airflow, and the relative humidity (RH) was measured by a humidity and temperature sensor meter (center 310 RS-232, TES, Taiwan).
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 samples became broader compared with that of Cu2O-1
2.5 samples became broader compared with that of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 (Fig. 1b), which indicated a smaller particle size. Fig. 2 exhibits the SEM, TEM, and HRTEM images of the three samples, from which we can see that all the samples appear to contain the stacking of nanometric particles due to the small size. The particle size of Cu2O-1
5 (Fig. 1b), which indicated a smaller particle size. Fig. 2 exhibits the SEM, TEM, and HRTEM images of the three samples, from which we can see that all the samples appear to contain the stacking of nanometric particles due to the small size. The particle size of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 was about 100 nm, and the particle sizes of Cu2O-1
5 was about 100 nm, and the particle sizes of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 were below 50 nm. Moreover, it was noticed that the nanoparticles of Cu2O-1
2.5 were below 50 nm. Moreover, it was noticed that the nanoparticles of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 were composed of even smaller particles with a size of just several nanometers (Fig. 2e and inset), which was in good agreement with the broadened XRD pattern. The measured particle lattice fringe of about 0.212 nm (as shown in Fig. 2g–i) corresponds to the interplanar distance of the (200) facet in Cu2O.24 The grain sizes calculated by the Scherrer equation and the specific surface areas of the three samples are listed in Table 1. It shows that Cu2O-1
2.5 were composed of even smaller particles with a size of just several nanometers (Fig. 2e and inset), which was in good agreement with the broadened XRD pattern. The measured particle lattice fringe of about 0.212 nm (as shown in Fig. 2g–i) corresponds to the interplanar distance of the (200) facet in Cu2O.24 The grain sizes calculated by the Scherrer equation and the specific surface areas of the three samples are listed in Table 1. It shows that Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 presents the smallest grain size of about 5.1 nm and the corresponding largest specific surface area of 42.7 m2 g−1.
2.5 presents the smallest grain size of about 5.1 nm and the corresponding largest specific surface area of 42.7 m2 g−1.
|  | ||
| Fig. 1 (a) Powder XRD patterns and (b) high-resolution XRD of the main peak of prepared Cu2O samples. | ||
| Catalysts | Specific surface area (m2 g−1) | Grain size (nm) | 
|---|---|---|
| 1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 Cu2O | 37.2 | 10.9 | 
| 1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 Cu2O | 42.7 | 5.1 | 
| 1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 Cu2O | 18.9 | 21.1 | 
The ratio of OH−/Cu2+ is the key to control the size of Cu2O by modifying the complexation and reduction reactions. On one hand, OH− could act as a ligand to complex with Cu2+ cations, forming dependent precursors. The SEM images and XRD patterns of the precursors obtained at different molar ratios of CuSO4 and NaOH are shown in Fig. 3. The nanosheet-shaped CuSO4(OH)6 precursor was formed due to an insufficient amount of the OH− ligand when the ratio of CuSO4 and NaOH was 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2, as shown in Fig. 3a and d, while the Cu(OH)2 nanowire precursor was formed when the ratio of CuSO4 and NaOH increased to 1
2, as shown in Fig. 3a and d, while the Cu(OH)2 nanowire precursor was formed when the ratio of CuSO4 and NaOH increased to 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 and 1
2.5 and 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 (verified from Fig. 3b–d). The different precursors produced have different redox potentials, having an effect on the reaction thermodynamics. On the other hand, a highly alkaline solution can improve the reaction rate of the reducing agent AA.33,34 The reduction rate was slow in the condition of 1
5 (verified from Fig. 3b–d). The different precursors produced have different redox potentials, having an effect on the reaction thermodynamics. On the other hand, a highly alkaline solution can improve the reaction rate of the reducing agent AA.33,34 The reduction rate was slow in the condition of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 due to the consumption of OH− by complexation; thus, the Cu2O nuclei gradually grew to form a small-size Cu2O monomer. In contrast, some Cu(OH)42− precursor species may be produced under the ratio of 1
2 due to the consumption of OH− by complexation; thus, the Cu2O nuclei gradually grew to form a small-size Cu2O monomer. In contrast, some Cu(OH)42− precursor species may be produced under the ratio of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 (although Cu(OH)42− cannot be detected by XRD, it can be speculated by the color change of the reaction system from a blue Cu(OH)2 precipitate (1
5 (although Cu(OH)42− cannot be detected by XRD, it can be speculated by the color change of the reaction system from a blue Cu(OH)2 precipitate (1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5) to a deep blue Cu(OH)42− solution (1
2.5) to a deep blue Cu(OH)42− solution (1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5)), which will decrease the redox potential; thus, few nuclei are formed, leading to the formation of Cu2O with a large size. Theoretically, there should be a suitable amount of OH− to balance the complexation and reduction reactions. Combined with the experimental results, we infer that the Cu(OH)2 nanowire precursor is mainly formed when the ratio is 1
5)), which will decrease the redox potential; thus, few nuclei are formed, leading to the formation of Cu2O with a large size. Theoretically, there should be a suitable amount of OH− to balance the complexation and reduction reactions. Combined with the experimental results, we infer that the Cu(OH)2 nanowire precursor is mainly formed when the ratio is 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5; at the same time, the reduction reaction rate is relatively high due to a suitable alkaline environment. As a result, a large amount of the Cu2O nuclei are formed instantly and cluster to reduce the surface energy, forming aggregated ultrafine nanoparticles. A schematic of the Cu2O formation process under different amounts of NaOH is shown in Fig. 3e.
2.5; at the same time, the reduction reaction rate is relatively high due to a suitable alkaline environment. As a result, a large amount of the Cu2O nuclei are formed instantly and cluster to reduce the surface energy, forming aggregated ultrafine nanoparticles. A schematic of the Cu2O formation process under different amounts of NaOH is shown in Fig. 3e.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2, 1
2, 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 and 1
2.5 and 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5) were tested at 25 °C in dry and high humidity conditions. Fig. 4a shows that all the three samples exhibit high catalytic activities for 1000 ppm ozone in dry flow, with the ozone conversion efficiency in the sequence of Cu2O-1
5) were tested at 25 °C in dry and high humidity conditions. Fig. 4a shows that all the three samples exhibit high catalytic activities for 1000 ppm ozone in dry flow, with the ozone conversion efficiency in the sequence of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 (100%) > Cu2O-1
2.5 (100%) > Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 (97.5%) > Cu2O-1
2 (97.5%) > Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 (94.6%). Water vapor is known to have a negative impact on the ozone catalytic activity; the ozone conversions over Cu2O-1
5 (94.6%). Water vapor is known to have a negative impact on the ozone catalytic activity; the ozone conversions over Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 dropped to 77.9% and 68.6%, respectively, at 90% RH. However, the ozone conversion over Cu2O-1
5 dropped to 77.9% and 68.6%, respectively, at 90% RH. However, the ozone conversion over Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 was still nearly 100% after the 8 h test under the high RH of 90%. These results suggest that particle size has a great influence on ozone catalytic activity, and Cu2O-1
2.5 was still nearly 100% after the 8 h test under the high RH of 90%. These results suggest that particle size has a great influence on ozone catalytic activity, and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 shows complete conversion for 1000 ppm ozone both in dry and high humidity conditions at 25 °C. To explore more about the activity, the ozone concentration of 3000 ppm was introduced; the decomposition efficiency is shown in Fig. 4b. For the Cu2O-1
2.5 shows complete conversion for 1000 ppm ozone both in dry and high humidity conditions at 25 °C. To explore more about the activity, the ozone concentration of 3000 ppm was introduced; the decomposition efficiency is shown in Fig. 4b. For the Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 catalysts, the ozone conversion has different degrees of decline either under dry or high humidity conditions due to the high concentration. However, Cu2O-1
5 catalysts, the ozone conversion has different degrees of decline either under dry or high humidity conditions due to the high concentration. However, Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 still maintains the best catalytic efficiency for 3000 ppm ozone, and the ozone conversion is 99.2% in dry flow. Importantly, water vapor has little effect on the activity, and ozone conversion is above 95% under 90% RH, showing its promise for dealing with high-concentration and high-humidity ozone. The catalytic activity of Cu2O-1
2.5 still maintains the best catalytic efficiency for 3000 ppm ozone, and the ozone conversion is 99.2% in dry flow. Importantly, water vapor has little effect on the activity, and ozone conversion is above 95% under 90% RH, showing its promise for dealing with high-concentration and high-humidity ozone. The catalytic activity of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 is compared with those of some recently reported catalysts (Table 2).35–45 It is noted that the reaction rate (mol g−1 h−1) of Cu2O-1
2.5 is compared with those of some recently reported catalysts (Table 2).35–45 It is noted that the reaction rate (mol g−1 h−1) of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 is one of the highest in the list, especially under high humidity. In order to make a more reasonable comparison, the reaction rate is normalized to the catalyst specific area, i.e., the surface-specific catalytic rate (SA, the number of moles of decomposed ozone per square meter per hour, mol m−2 h−1). It is obvious that the SA of Cu2O-1
2.5 is one of the highest in the list, especially under high humidity. In order to make a more reasonable comparison, the reaction rate is normalized to the catalyst specific area, i.e., the surface-specific catalytic rate (SA, the number of moles of decomposed ozone per square meter per hour, mol m−2 h−1). It is obvious that the SA of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 is 1–2 orders of magnitude higher than those of the other published catalysts, suggesting its high intrinsic catalytic activity for ozone removal. It should be noted that there are no mesopores in ultrafine Cu2O and thus, water vapor can only be adsorbed/desorbed on the surface, which would account for the high humidity resistivity as compared with that of the large-surface-area porous oxide catalyst reported in the literature.
2.5 is 1–2 orders of magnitude higher than those of the other published catalysts, suggesting its high intrinsic catalytic activity for ozone removal. It should be noted that there are no mesopores in ultrafine Cu2O and thus, water vapor can only be adsorbed/desorbed on the surface, which would account for the high humidity resistivity as compared with that of the large-surface-area porous oxide catalyst reported in the literature.
| Catalyst | Conc.a (ppm) | RHb (%) | SVc (mL g−1 h−1) | SBETd (m2 g−1) | Conv.e (%) | Rate (mmol g−1 h−1) | SAf (mmol m−2 h−1) | 
|---|---|---|---|---|---|---|---|
| a Ozone initial concentration.b Relative humidity.c Space velocity.d Specific surface area determined by BET method.e Ozone conversion.f Surface specific catalytic activity. | |||||||
| MnO2 | 120 | 50 | 600 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 90 | 63 | 2.0 | 2.3 × 10−2 | 
| MIL-100(Fe) | 45 | 45 | 200 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 1726 | 100 | 0.4 | 2.3 × 10−3 | 
| Ce-OMS-2 | 40 | 90 | 600 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 200 | 90 | 0.96 | 4.8 × 10−3 | 
| α-MnO2 | 14 | ∼1 | 660 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 80.7 | 100 | 0.41 | 5.1 × 10−3 | 
| α-MnO2 | 50 | 22 | 540 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 52.4 | 99 | 1.2 | 2.3 × 10−2 | 
| 70 | 25 | 0.3 | 5.8 × 10−3 | ||||
| H-MnO2 | 120 | 50 | 600 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 228 | 60 | 1.9 | 8.5 × 10−3 | 
| H-δ-MnO2 | 3000 | Dry | 600 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 206 | 100 | 80 | 3.9 × 10−1 | 
| MnFe0.5Ox | 10 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 90 | 12 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 262 | 90 | 4.8 | 1.8 × 10−2 | 
| MnOx | 1000 | Dry | 120 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 116.2 | 98.5 | 5.3 | 4.5 × 10−2 | 
| CoOx | 1000 | Dry | 120 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 67.0 | 88.1 | 4.7 | 7.0 × 10−2 | 
| Ag-H-MCM | 4400 | Dry | 114 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 574 | 97.8 | 22 | 3.8 × 10−2 | 
| LaFe0.95Ni0.05O3 | 1000 | Dry | 240 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 18.7 | 97.7 | 10 | 5.3 × 10−1 | 
| RH | 93 | 9.9 | 5.3 × 10−1 | ||||
| Cu2O-1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 | 1000 | Dry | 240 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 26.5 | 100 | 10.7 | 4 × 10−1 | 
| 90 | 100 | 10.7 | 4 × 10−1 | ||||
| Cu2O-1 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 | 3000 | Dry | 240 ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 000 | 26.5 | 100 | 32 | 1.2 | 
| 90 | 95 | 31 | 1.17 | ||||
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 exhibited the main reduction peaks located at 260 °C and 275 °C, which could be assigned to the reduction of the Cu2O species.46 It was noted that the dominant reduction peaks of Cu2O-1
5 exhibited the main reduction peaks located at 260 °C and 275 °C, which could be assigned to the reduction of the Cu2O species.46 It was noted that the dominant reduction peaks of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 were observed at around 220 °C, and the second peak was located at about 260 °C. In particular, for Cu2O-1
2.5 were observed at around 220 °C, and the second peak was located at about 260 °C. In particular, for Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5, most of the reduction occurred at the lowest temperature of 220 °C. This result suggests that the position of the reduction peak is strongly related to the particle size and Cu2O-1
2.5, most of the reduction occurred at the lowest temperature of 220 °C. This result suggests that the position of the reduction peak is strongly related to the particle size and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 has the highest reducibility. The easier redox property of Cu2O-1
2.5 has the highest reducibility. The easier redox property of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 may be helpful for its catalytic properties for ozone decomposition.
2.5 may be helpful for its catalytic properties for ozone decomposition.
O2-TPD was conducted to explore the evolution of oxygen (Fig. 5b). The peak occurring below 100 °C is usually attributed to the desorption of physically adsorbed oxygen, and the peak at higher temperatures (<400 °C) can be ascribed to the release of chemically adsorbed oxygen.47,48 Evidently, the strongest oxygen desorption peak was observed in the O2-TPD profile of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 in the temperature range from 100 °C to 400 °C, indicating that it possessed the most active adsorbed oxygen. Compared with the observation for Cu2O-1
2.5 in the temperature range from 100 °C to 400 °C, indicating that it possessed the most active adsorbed oxygen. Compared with the observation for Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5, the first oxygen desorption peaks of Cu2O-1
5, the first oxygen desorption peaks of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 (185 °C) and Cu2O-1
2 (185 °C) and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 (128 °C) were observed at lower temperatures below 200 °C. Overall, the O2-TPD results indicate that the oxygen mobility and storage in Cu2O-1
2.5 (128 °C) were observed at lower temperatures below 200 °C. Overall, the O2-TPD results indicate that the oxygen mobility and storage in Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 are the highest among the three catalysts, which is beneficial to the release of intermediate adsorbed oxygen during the ozone decomposition process.
2.5 are the highest among the three catalysts, which is beneficial to the release of intermediate adsorbed oxygen during the ozone decomposition process.
Oyama investigated the ozone decomposition mechanism,49,50 and the process can be proposed as follows:
| O3 + * → O2 + O2− | (1) | 
| O3 + O2− → O2 + O22− | (2) | 
| O22− → O2 + * (slow) | (3) | 
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 shifted to a higher location at about 933.5 eV (shown in Fig. 6b). This suggests that the surface of Cu2O is partially oxidized to CuO, which can also be verified by the shake-up satellite in the range of 940–945 eV in the Cu 2p spectra of the used catalysts.52,53 To study the effect of CuO, the Cu2O-1
5 shifted to a higher location at about 933.5 eV (shown in Fig. 6b). This suggests that the surface of Cu2O is partially oxidized to CuO, which can also be verified by the shake-up satellite in the range of 940–945 eV in the Cu 2p spectra of the used catalysts.52,53 To study the effect of CuO, the Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 catalyst was calcined in an air atmosphere at 600 °C for 2 h to obtain CuO, which, however, exhibited a poor ozone conversion efficiency of less than 10% during the 8 h test. Therefore, the active sites of ozone catalytic degradation might be the surface Cu(I) sites or some other crystal defects such as Cu vacancies, which made Cu2O p-type. The first O 1s peak around 530.3 eV for the fresh samples can be assigned to the lattice oxygen of Cu2O (Fig. 6c).54 After testing for ozone decomposition, the peak of lattice oxygen slightly moved to a lower binding energy at around 529.7 eV (Fig. 6d), which could be attributed to the lattice oxygen of CuO.55 Importantly, it was noticed that there was a broad peak in the high binding energy region of 531–534 eV in the O 1s spectra of the used catalysts. This peak at high binding energy can be ascribed to the chemisorbed oxygen species produced during the ozone decomposition process.20 The ratio of surface adsorbed oxygen in the Cu2O-1
2.5 catalyst was calcined in an air atmosphere at 600 °C for 2 h to obtain CuO, which, however, exhibited a poor ozone conversion efficiency of less than 10% during the 8 h test. Therefore, the active sites of ozone catalytic degradation might be the surface Cu(I) sites or some other crystal defects such as Cu vacancies, which made Cu2O p-type. The first O 1s peak around 530.3 eV for the fresh samples can be assigned to the lattice oxygen of Cu2O (Fig. 6c).54 After testing for ozone decomposition, the peak of lattice oxygen slightly moved to a lower binding energy at around 529.7 eV (Fig. 6d), which could be attributed to the lattice oxygen of CuO.55 Importantly, it was noticed that there was a broad peak in the high binding energy region of 531–534 eV in the O 1s spectra of the used catalysts. This peak at high binding energy can be ascribed to the chemisorbed oxygen species produced during the ozone decomposition process.20 The ratio of surface adsorbed oxygen in the Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 catalyst was the lowest compared with that for Cu2O-1
2.5 catalyst was the lowest compared with that for Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2 and Cu2O-1
2 and Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 5 in the normalized O 1s spectra. The XPS results suggested that although some of the surface-active sites in Cu2O-1
5 in the normalized O 1s spectra. The XPS results suggested that although some of the surface-active sites in Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 were occupied by the intermediate adsorbed oxygen species, the remaining highly active sites could still exhibit efficient ozone degradation. According to our previous work, the covering of surface-active sites by intermediate adsorbed oxygen is the main cause of Cu2O catalyst deactivation, and the root reason for the highest ozone catalytic activity of the Cu2O-1
2.5 were occupied by the intermediate adsorbed oxygen species, the remaining highly active sites could still exhibit efficient ozone degradation. According to our previous work, the covering of surface-active sites by intermediate adsorbed oxygen is the main cause of Cu2O catalyst deactivation, and the root reason for the highest ozone catalytic activity of the Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 catalyst is its smallest particle size, which is beneficial to the release of adsorbed oxygen.31 This result is also consistent with that of O2-TPD analysis.
2.5 catalyst is its smallest particle size, which is beneficial to the release of adsorbed oxygen.31 This result is also consistent with that of O2-TPD analysis.
|  | ||
| Fig. 6 XPS spectra of (a) Cu 2p, (b) O 1s in fresh samples, (c) Cu 2p and (d) O 1s in catalysts used in dry stream for 8 h. | ||
As a proof-of-concept study for the application of the catalyst, Cu2O nanoparticles were coated onto an Al honeycomb substrate to form a monolithic catalyst. Fig. 7a shows the photograph of the Cu2O–Al honeycomb (diameter = 20 mm, thickness = 20 mm) coated by high-yield Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 (>20 g), where the active material on the Al honeycomb is about 0.2 g. The Cu2O–Al honeycomb can decompose 10 ppm ozone completely for at least 24 h both in dry and high humidity conditions, as shown in Fig. 7a. In contrast, the Al honeycomb substrate alone exhibits relatively low catalytic activity of about 20–40% irrespective of whether it is coated with the Al2O3 sol. To further assess the potential of the catalyst, high-concentration ozone (3000 ppm) and high velocity (800 mL min−1) were applied, and the conversion of 3000 ppm ozone over the Cu2O–Al honeycomb was still nearly 100% (99.4%) after the 12 h test in dry flow with a space velocity of 8000 h−1. Then, water vapor was added into the system; it was noticeable that although ozone conversion dropped slightly, it was still as high as 97.7% after the 24 h test, as shown in Fig. 7b. Overall, the high-output and highly active Cu2O nanoparticles exhibit high catalytic performance and stability for ozone removal and display great potential for practical applications.
2.5 (>20 g), where the active material on the Al honeycomb is about 0.2 g. The Cu2O–Al honeycomb can decompose 10 ppm ozone completely for at least 24 h both in dry and high humidity conditions, as shown in Fig. 7a. In contrast, the Al honeycomb substrate alone exhibits relatively low catalytic activity of about 20–40% irrespective of whether it is coated with the Al2O3 sol. To further assess the potential of the catalyst, high-concentration ozone (3000 ppm) and high velocity (800 mL min−1) were applied, and the conversion of 3000 ppm ozone over the Cu2O–Al honeycomb was still nearly 100% (99.4%) after the 12 h test in dry flow with a space velocity of 8000 h−1. Then, water vapor was added into the system; it was noticeable that although ozone conversion dropped slightly, it was still as high as 97.7% after the 24 h test, as shown in Fig. 7b. Overall, the high-output and highly active Cu2O nanoparticles exhibit high catalytic performance and stability for ozone removal and display great potential for practical applications.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) OH− was the key parameter, which was optimized at 2.5. The as-synthesized Cu2O showed complete removal for 1000 ppm ozone both under dry and high humidity conditions at 25 °C. For high-concentration 3000 ppm ozone, the conversion was 99.2% in dry flow and still above 95% in humid flow. The results of O2-TPD and XPS suggested that the accumulation of intermediate oxygen species on the catalyst surface was the main cause for limiting ozone decomposition efficiency, and the small particle size of Cu2O-1
OH− was the key parameter, which was optimized at 2.5. The as-synthesized Cu2O showed complete removal for 1000 ppm ozone both under dry and high humidity conditions at 25 °C. For high-concentration 3000 ppm ozone, the conversion was 99.2% in dry flow and still above 95% in humid flow. The results of O2-TPD and XPS suggested that the accumulation of intermediate oxygen species on the catalyst surface was the main cause for limiting ozone decomposition efficiency, and the small particle size of Cu2O-1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2.5 was beneficial to its release. Moreover, a Cu2O–Al honeycomb was fabricated and showed 99.4% and 97.7% ozone removal efficiency at dry and 90% RH conditions, respectively, at 3000 ppm and a space velocity of 8000 h−1. These results show the promise of the simple strategy for producing high-yield Cu2O for effective ozone elimination.
2.5 was beneficial to its release. Moreover, a Cu2O–Al honeycomb was fabricated and showed 99.4% and 97.7% ozone removal efficiency at dry and 90% RH conditions, respectively, at 3000 ppm and a space velocity of 8000 h−1. These results show the promise of the simple strategy for producing high-yield Cu2O for effective ozone elimination.
| Footnote | 
| † Shuyan Gong and Anqi Wang contributed equally. | 
| This journal is © The Royal Society of Chemistry 2020 |