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Figure 3. (a) Photocatalytic CO2RR product yields of Ni-CsPbCl3 with various Ni doping ratios under conditions without or with an external magnetic field. (b) UV‒visible absorption spectra of Ni-CsPbCl3 with different Ni doping ratios. (c) Relationships between the photocatalytic CO yield and magnetic field intensity for CsPbCl3 and Ni-CsPbCl3 with a nickel doping ratio of 8.0 at%. (d) Changes in the photocatalytic CO yield over time for CsPbCl3 and Ni-CsPbCl3 with a nickel doping ratio of 8.0 at%.
Figure 5. (a) Photogenerated currents for CsPbCl3 and Ni-CsPbCl3 with a Ni doping ratio of 8.0 at%. (b) EPR spectra of CsPbCl3 and Ni-CsPbCl3 with a Ni doping ratio of 8.0 at%. (c) XMCD spectra of Ni-CsPbCl3 with a Ni doping ratio of 8.0 at%. (d) Schematic diagram illustrating the mechanism of magnetic field-induced CO2RR performance enhancement.
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Goeppert A, Czaun M, Jones J P, et al. Recycling of carbon dioxide to methanol and derived products – closing the loop. Chemical Society Reviews, 2014, 43 (23): 7995–8048. doi: 10.1039/C4CS00122B
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[2] |
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[3] |
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[4] |
Mikkelsen M, Jørgensen M, Krebs F C. The teraton challenge. A review of fixation and transformation of carbon dioxide. Energy & Environmental Science, 2010, 3 (1): 43–81. doi: 10.1039/B912904A
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[5] |
Jiang Z, Sun H, Wang T, et al. Nature-based catalyst for visible-light-driven photocatalytic CO2 reduction. Energy & Environmental Science, 2018, 11 (9): 2382–2389. doi: 10.1039/C8EE01781F
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[6] |
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[9] |
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[10] |
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[13] |
Kim T H, Cho K, Lee S H, et al. Spin polarization in Fe-doped CsPbBr3 perovskite nanocrystals for enhancing photocatalytic CO2 reduction. Chemical Engineering Journal, 2024, 492: 152095. doi: 10.1016/j.cej.2024.152095
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[19] |
Jiang Y, Liao J F, Chen H Y, et al. All-solid-state Z-scheme α-Fe2O3/amine-RGO/CsPbBr3 hybrids for visible-light-driven photocatalytic CO2 reduction. Chem, 2020, 6 (3): 766–780. doi: 10.1016/j.chempr.2020.01.005
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[20] |
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