2021
DOI: 10.1002/solr.202100558
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Boosting Cascade Electron Transfer for Highly Efficient CO2 Photoreduction

Abstract: Artificial photosynthesis converting carbon dioxide into chemical fuels with a high added value is a promising solution to both fossil fuel shortage/pollution and global climate change; however, the development of highly efficient photocatalysts toward this goal is still largely bereft of fresh ideas. Herein, we propose a “cascade electron transfer” strategy through spurring both interfacial and inner electron transfer rates for a 0D/2D photocatalyst of CsPbBr3/CuTCPP metal organic framework (MOF). Upon photoe… Show more

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Cited by 14 publications
(19 citation statements)
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References 57 publications
(58 reference statements)
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“…In addition, τ2 and τ3 represented the relaxation process from the S1 to the S0 state and the intersystem crossing from the S1 to the excited triplet (T1) state, respectively. [49] Notably, the relaxation time of Cu2 was much longer than that of Cu1 in each channel owing to the increase in the coordination numbers leading to an increase in the charge transfer, which was consistent with the results obtained from the first-principles analysis. In addition, Figure 6a,b reveals that the normalized decay curves of Cu1 and Cu2 at different wavelengths maintain a plateau with different normalized intensities after ≈1000 ps owing to the extremely slow recombination of carriers from the T1 to S0 state.…”
Section: Ultrafast Carrier Dynamicssupporting
confidence: 89%
“…In addition, τ2 and τ3 represented the relaxation process from the S1 to the S0 state and the intersystem crossing from the S1 to the excited triplet (T1) state, respectively. [49] Notably, the relaxation time of Cu2 was much longer than that of Cu1 in each channel owing to the increase in the coordination numbers leading to an increase in the charge transfer, which was consistent with the results obtained from the first-principles analysis. In addition, Figure 6a,b reveals that the normalized decay curves of Cu1 and Cu2 at different wavelengths maintain a plateau with different normalized intensities after ≈1000 ps owing to the extremely slow recombination of carriers from the T1 to S0 state.…”
Section: Ultrafast Carrier Dynamicssupporting
confidence: 89%
“…Li and co‐workers built the “cascade electron transfer” by combining CsPbBr 3 QDs and 2D Cu‐based porphyrin MOF nanosheets (CsPbBr 3 /CuTCPP MOF) to spur both interfacial and inner electron transfer (Figure 9f). [ 83 ] The optimized CsPbBr 3 /CuTCPP MOF (0.1 wt% Cu) achieved the yield of 11.8 and 2.95 μmol g −1 h −1 for CO and CH 4 , respectively.…”
Section: Methods To Improve Photoelectrochemical Performancementioning
confidence: 99%
“…Combining with CsPbBr 3 nanomaterials, Ni-based and Cu-based 2D MOF materials also showed superior photocatalytic performance, and were reported by Xi et al and Li et al respectively. [82,83] In Xi's work, they compared the properties of CsPbBr 3 nanocubes, nanorods, and nanowires, and found that the charge carrier dynamics is depend on the aspect ratio of the PVK. [82] As shown in Figure 9e, the Ni-based MOF/ CsPbBr 3 nanowires (NMF/CPB-NWs) exhibited the highest CO production rate of 81.0 μmol g À1 h À1 .…”
Section: Type-ii Heterojunctionsmentioning
confidence: 99%
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“…Another key hurdle in the formation of the highly reactive charge-separated state is the ease of photoinduced electron transfer, also called charge transfer, from either the singlet or triplet states, in MOFs ,, and COFs . These processes generally occur in the picosecond (10 –12 s) time scale. …”
Section: Excited-state Properties Of Porphyrin-containing Mofs and Cofsmentioning
confidence: 99%