Unlocking solar-derived CO2 conversion to hydrocarbons over plasmonic Cu-Fe tandem catalysts under industrially relevant conditions: Difference between revisions
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{{DOI|doi=10.1038/s41467-026-75764-5}} | {{DOI|doi=10.1038/s41467-026-75764-5}} | ||
== Abstract Summary == | |||
This article describes a ''photo-thermal'' CO<sub>2</sub> hydrogenation system based on a potassium-promoted Cu–Fe tandem catalyst, not a molecular photocatalytic CO<sub>2</sub> reduction system. The reported chemistry converts CO<sub>2</sub> and H<sub>2</sub> into CO and hydrocarbons under continuous-flow illumination and external heating. The best-performing material, 2K Cu<sub>2</sub>Fe<sub>1</sub>, gave high selectivity toward C<sub>2+</sub> hydrocarbons under elevated pressure, with the article attributing the performance to tandem catalysis in which Cu promotes reverse water-gas shift chemistry and in situ formed χ-Fe<sub>5</sub>C<sub>2</sub> promotes Fischer–Tropsch-type carbon–carbon coupling. Mechanistic studies support a major role for light-induced non-thermal effects together with localized heating and accelerated iron carburization. | |||
== Advances and Special Progress == | |||
The article presents several advances within photo-thermal CO<sub>2</sub> hydrogenation chemistry. | |||
First, it reports strong hydrocarbon formation under conditions described as industrially relevant by the article itself: continuous flow, elevated pressure, and moderate external heating combined with illumination. Under 250 °C and 20 bar, the catalyst reached 77.4% selectivity to C<sub>2+</sub> hydrocarbons and a C<sub>2</sub>-C<sub>5</sub> hydrocarbon yield of 5.04 mmol g<sup>−1</sup> h<sup>−1</sup>. | |||
Second, the catalyst uses earth-abundant transition metals, Cu and Fe, rather than noble-metal-centered molecular photocatalytic designs. The article emphasizes a tandem architecture in which the two metals play distinct catalytic roles. | |||
Third, potassium promotion improved CO<sub>2</sub> adsorption, CO adsorption, and chain growth probability relative to the unpromoted material, giving an optimized 2 wt% K loading. | |||
Fourth, the study provides unusually detailed mechanistic evidence for a photo-thermal hydrocarbon-forming system. Direct versus indirect illumination experiments, in situ DRIFTS, in situ XRD, CO-TPR, CO<sub>2</sub>-TPSR, transient photocurrent, TRPL, and wavelength-dependent catalysis were used to distinguish thermal from non-thermal contributions and to connect Cu plasmon excitation with faster formation of χ-Fe<sub>5</sub>C<sub>2</sub>. | |||
Fifth, the catalyst showed stable performance during repeated light on/off cycling after activation, supporting structural robustness under the tested conditions. | |||
== Additional Remarks == | |||
This article is chemically important, but it does ''not'' describe a molecular photocatalytic CO<sub>2</sub> reduction system. Instead, it reports a heterogeneous plasmonic photo-thermal catalytic process that couples light absorption, heat generation, reverse water-gas shift reactivity, and Fischer–Tropsch-type hydrocarbon synthesis. | |||
That distinction matters for interpretation. In molecular photocatalysis, one usually analyzes discrete photosensitizers, sacrificial electron donors, quenching pathways, and molecular catalyst redox states in solution. None of that framework is the primary one here. The present system operates in the gas phase with H<sub>2</sub> as reductant, elevated pressure, external heating, and a solid catalyst bed under Xe-lamp irradiation. | |||
A strength of the work is that it addresses carbon–carbon bond formation rather than only C<sub>1</sub> products. Another strength is the mechanistic focus on active phase evolution, especially the conversion of Fe to χ-Fe<sub>5</sub>C<sub>2</sub>. A limitation for a reader specifically seeking molecular photocatalytic CO<sub>2</sub> reduction data is that common molecular-photocatalysis descriptors such as photosensitizer identity, sacrificial donor concentration, quenching constants, and product TON values are not part of the reported system. | |||
== Content of the Published Article in Detail == | |||
The article studies the direct conversion of CO<sub>2</sub> with H<sub>2</sub> to hydrocarbons using a solid Cu–Fe catalyst under combined illumination and heating. The catalyst family was prepared by co-precipitation, calcination, reduction, potassium impregnation, and passivation. Different Cu/Fe ratios and potassium loadings were screened, and 2K Cu<sub>2</sub>Fe<sub>1</sub> was identified as the best composition. | |||
The reaction setup was a continuous-flow reactor equipped with a quartz window and irradiated with a 300 W Xe lamp. The catalyst mass was 50 mg. A thermocouple was placed about 1 mm below the catalyst surface. The feed gas had H<sub>2</sub>/CO<sub>2</sub> = 4:1, with N<sub>2</sub> as an internal standard. Most key tests discussed in the main text used 250 °C external heating, 4 W cm<sup>−2</sup> light intensity, a gas hourly space velocity of 12000 mL g<sup>−1</sup> h<sup>−1</sup>, and pressures between 10 and 20 bar. Additional tests used lower space velocity, lower temperature, indirect illumination, or different light intensities. | |||
Catalytically, monometallic Fe showed some ability to form hydrocarbons, while monometallic Cu was nearly fully selective to CO. This comparison supports a tandem interpretation. According to the article, Cu mainly promotes the reverse water-gas shift reaction, producing CO from CO<sub>2</sub>. The Fe-containing phase then converts CO-derived intermediates into hydrocarbons through Fischer–Tropsch-type chemistry. After reaction, the active Fe phase was identified mainly as χ-Fe<sub>5</sub>C<sub>2</sub>, formed in situ from metallic Fe during catalyst activation and operation. | |||
The article presents several lines of evidence for this tandem picture. Before reaction, the reduced catalyst contained metallic Cu and metallic Fe, with a thin oxidized surface layer attributed to passivation. After reaction, diffraction, Mössbauer spectroscopy, TEM, XPS, and TGA-TPH supported conversion of the Fe component to χ-Fe<sub>5</sub>C<sub>2</sub>. No Fe<sub>3</sub>C was detected by the TPH analysis described in the article. | |||
Potassium promotion was examined by CO<sub>2</sub>-TPD and CO-TPD. These measurements showed stronger CO<sub>2</sub> and CO adsorption for the K-promoted catalyst. The article interprets this as beneficial for generating CO-derived intermediates and shifting selectivity toward longer hydrocarbons, partly by moderating hydrogenation behavior. | |||
Mechanistic interpretation was further developed with direct and indirect illumination experiments. For indirect illumination, a thin Ti<sub>2</sub>O<sub>3</sub> layer was placed above the catalyst bed to provide similar photo-thermal heating while blocking direct photochemical excitation of the catalyst. Under direct illumination, CO<sub>2</sub> conversion increased linearly with light intensity from 2.8 to 4.0 W cm<sup>−2</sup>, which the article interprets as characteristic of dominant non-thermal contributions with a minor thermal contribution. Indirect illumination gave substantially lower conversion, supporting the importance of direct light-induced effects. At higher intensity, the non-thermal contribution appeared to plateau. | |||
The article also tested lower temperature operation at 200 °C. With light, the catalyst still produced hydrocarbons and formed χ-Fe<sub>5</sub>C<sub>2</sub>. Without direct light, the product stream was mainly CO and metallic Fe remained dominant. This is an important observation because it links illumination to accelerated formation of the carbide phase needed for Fischer–Tropsch-type hydrocarbon synthesis. | |||
In situ DRIFTS was used to follow surface intermediates during reaction. Under dark conditions, the spectra showed bicarbonate and carbonate species at lower temperature, then formate species at higher temperature, followed by adsorbed CO, and finally hydrocarbon-related bands at 250 °C. The article therefore supports the sequence: | |||
CO<sub>2</sub> adsorption as bicarbonate/carbonate → hydrogenation to formate → decomposition to CO → further hydrogenation and C–C coupling to hydrocarbons. | |||
Comparable DRIFTS experiments on monometallic Cu and Fe clarified their different roles. On Cu, carbonate, formate, and adsorbed CO were seen, but no strong methane signal, consistent with Cu functioning mainly in reverse water-gas shift chemistry. On Fe, similar oxygenated intermediates were seen together with weaker hydrocarbon-related bands, consistent with Fe-containing phases supporting hydrocarbon formation. | |||
Under illumination, the same classes of intermediates were observed in DRIFTS, but they appeared at lower temperature and with higher intensity. The article interprets this as evidence that light does not change the basic reaction pathway, but accelerates the formation and evolution of key intermediates. The comparison of peak intensities for bicarbonate, adsorbed CO, and olefin-related species further supported faster intermediate buildup under light. | |||
In situ XRD directly tracked iron phase evolution. Under illumination, the metallic Fe diffraction peak diminished at lower temperature, and χ-Fe<sub>5</sub>C<sub>2</sub> appeared earlier than under dark conditions. CO-TPR also showed lower-temperature events under illumination, including earlier CO uptake and lower-temperature Fe-phase transformation associated with carbide formation. CO<sub>2</sub>-TPSR showed similarly lower temperatures for CO<sub>2</sub> consumption and product formation under light. | |||
To explain these effects, the article considers three possibilities and argues that the most plausible one is plasmonic Cu-mediated promotion of Fe carburization. UV–vis spectroscopy showed a metallic Cu plasmon band near 505 nm. Transient photocurrent and TRPL measurements indicated more efficient charge separation or transfer in the bimetallic Cu–Fe catalyst than in the monometallic materials. Additional wavelength-dependent catalysis showed the highest activity under 500 nm irradiation, consistent with the Cu plasmon response. Taken together, the data support the article’s proposal that plasmonic excitation of Cu accelerates reverse water-gas shift chemistry and promotes interfacial electronic interactions with Fe, lowering the apparent barrier to χ-Fe<sub>5</sub>C<sub>2</sub> formation. | |||
The main products were CO, CH<sub>4</sub>, C<sub>2</sub>-C<sub>5</sub> olefins, C<sub>2</sub>-C<sub>5</sub> paraffins, and C<sub>6+</sub> hydrocarbons. At higher pressure, CO selectivity decreased and hydrocarbon formation increased. Product distributions from C<sub>3</sub> to C<sub>5</sub> followed the Anderson–Schulz–Flory distribution according to the article. The olefin/paraffin ratio decreased at higher pressure and lower space velocity, which the authors interpret as increased hydrogenation and chain termination. | |||
Because this is not a molecular photocatalytic system, the article does not discuss a discrete photosensitizer, reductive or oxidative quenching cycle, a sacrificial electron donor, or solution-phase reduced catalyst intermediates. Instead, light acts through the solid catalyst itself, especially through Cu-associated plasmonic excitation and photo-thermal energy delivery. | |||
== Catalyst == | |||
The catalyst is a heterogeneous potassium-promoted bimetallic Cu–Fe material, with the optimized composition designated 2K Cu<sub>2</sub>Fe<sub>1</sub>. It is not molecular, not immobilized molecularly, and not a discrete coordination complex. | |||
Before reaction, the reduced catalyst contains metallic Cu and metallic Fe, with minor surface oxidation attributed to passivation. During reaction, the Fe phase is converted in situ mainly to χ-Fe<sub>5</sub>C<sub>2</sub>, which the article identifies as the active phase for Fischer–Tropsch-type hydrocarbon formation. Cu is assigned the main role in reverse water-gas shift chemistry, while Fe carbide is assigned the main role in C–C coupling and hydrocarbon production. | |||
Potassium acts as a promoter that enhances CO<sub>2</sub> adsorption, strengthens CO adsorption, and favors chain growth toward C<sub>2+</sub> hydrocarbons. A 2 wt% K loading gave the best performance among the tested values. The catalyst also showed stable composition and performance during the reported cycling experiment after activation. | |||
== Photosensitizer == | |||
No separate molecular or heterogeneous photosensitizer is reported. | |||
Instead, the light-harvesting function is attributed to the catalyst itself, especially the metallic Cu component, which shows a plasmon absorption band at about 505 nm. The article proposes that Cu acts as the photoactive plasmonic component, generating hot carriers and localized heating under illumination. These effects are linked to enhanced reverse water-gas shift activity and to promotion of Fe carburization at the Cu–Fe interface. | |||
Because there is no discrete photosensitizer, the article does not report excited-state quenching by a sacrificial donor, oxidative or reductive quenching cycles, or separate photosensitizer stability data. | |||
== Investigation == | |||
{{#experimentlist:|form=Photocatalytic_CO2_conversion_experiments|name=inv0}} | |||
[[Category:Topic]] | |||
Latest revision as of 16:48, 14 August 2026
Imported from: /opt/downloadPDF/chemwiki_pubstore/ee728a8dd9e24ae23adaa4566ee60d36/s41467-026-75764-5_reference_6a7f2a5845688.pdf
Abstract Summary[edit | edit source]
This article describes a photo-thermal CO2 hydrogenation system based on a potassium-promoted Cu–Fe tandem catalyst, not a molecular photocatalytic CO2 reduction system. The reported chemistry converts CO2 and H2 into CO and hydrocarbons under continuous-flow illumination and external heating. The best-performing material, 2K Cu2Fe1, gave high selectivity toward C2+ hydrocarbons under elevated pressure, with the article attributing the performance to tandem catalysis in which Cu promotes reverse water-gas shift chemistry and in situ formed χ-Fe5C2 promotes Fischer–Tropsch-type carbon–carbon coupling. Mechanistic studies support a major role for light-induced non-thermal effects together with localized heating and accelerated iron carburization.
Advances and Special Progress[edit | edit source]
The article presents several advances within photo-thermal CO2 hydrogenation chemistry.
First, it reports strong hydrocarbon formation under conditions described as industrially relevant by the article itself: continuous flow, elevated pressure, and moderate external heating combined with illumination. Under 250 °C and 20 bar, the catalyst reached 77.4% selectivity to C2+ hydrocarbons and a C2-C5 hydrocarbon yield of 5.04 mmol g−1 h−1.
Second, the catalyst uses earth-abundant transition metals, Cu and Fe, rather than noble-metal-centered molecular photocatalytic designs. The article emphasizes a tandem architecture in which the two metals play distinct catalytic roles.
Third, potassium promotion improved CO2 adsorption, CO adsorption, and chain growth probability relative to the unpromoted material, giving an optimized 2 wt% K loading.
Fourth, the study provides unusually detailed mechanistic evidence for a photo-thermal hydrocarbon-forming system. Direct versus indirect illumination experiments, in situ DRIFTS, in situ XRD, CO-TPR, CO2-TPSR, transient photocurrent, TRPL, and wavelength-dependent catalysis were used to distinguish thermal from non-thermal contributions and to connect Cu plasmon excitation with faster formation of χ-Fe5C2.
Fifth, the catalyst showed stable performance during repeated light on/off cycling after activation, supporting structural robustness under the tested conditions.
Additional Remarks[edit | edit source]
This article is chemically important, but it does not describe a molecular photocatalytic CO2 reduction system. Instead, it reports a heterogeneous plasmonic photo-thermal catalytic process that couples light absorption, heat generation, reverse water-gas shift reactivity, and Fischer–Tropsch-type hydrocarbon synthesis.
That distinction matters for interpretation. In molecular photocatalysis, one usually analyzes discrete photosensitizers, sacrificial electron donors, quenching pathways, and molecular catalyst redox states in solution. None of that framework is the primary one here. The present system operates in the gas phase with H2 as reductant, elevated pressure, external heating, and a solid catalyst bed under Xe-lamp irradiation.
A strength of the work is that it addresses carbon–carbon bond formation rather than only C1 products. Another strength is the mechanistic focus on active phase evolution, especially the conversion of Fe to χ-Fe5C2. A limitation for a reader specifically seeking molecular photocatalytic CO2 reduction data is that common molecular-photocatalysis descriptors such as photosensitizer identity, sacrificial donor concentration, quenching constants, and product TON values are not part of the reported system.
Content of the Published Article in Detail[edit | edit source]
The article studies the direct conversion of CO2 with H2 to hydrocarbons using a solid Cu–Fe catalyst under combined illumination and heating. The catalyst family was prepared by co-precipitation, calcination, reduction, potassium impregnation, and passivation. Different Cu/Fe ratios and potassium loadings were screened, and 2K Cu2Fe1 was identified as the best composition.
The reaction setup was a continuous-flow reactor equipped with a quartz window and irradiated with a 300 W Xe lamp. The catalyst mass was 50 mg. A thermocouple was placed about 1 mm below the catalyst surface. The feed gas had H2/CO2 = 4:1, with N2 as an internal standard. Most key tests discussed in the main text used 250 °C external heating, 4 W cm−2 light intensity, a gas hourly space velocity of 12000 mL g−1 h−1, and pressures between 10 and 20 bar. Additional tests used lower space velocity, lower temperature, indirect illumination, or different light intensities.
Catalytically, monometallic Fe showed some ability to form hydrocarbons, while monometallic Cu was nearly fully selective to CO. This comparison supports a tandem interpretation. According to the article, Cu mainly promotes the reverse water-gas shift reaction, producing CO from CO2. The Fe-containing phase then converts CO-derived intermediates into hydrocarbons through Fischer–Tropsch-type chemistry. After reaction, the active Fe phase was identified mainly as χ-Fe5C2, formed in situ from metallic Fe during catalyst activation and operation.
The article presents several lines of evidence for this tandem picture. Before reaction, the reduced catalyst contained metallic Cu and metallic Fe, with a thin oxidized surface layer attributed to passivation. After reaction, diffraction, Mössbauer spectroscopy, TEM, XPS, and TGA-TPH supported conversion of the Fe component to χ-Fe5C2. No Fe3C was detected by the TPH analysis described in the article.
Potassium promotion was examined by CO2-TPD and CO-TPD. These measurements showed stronger CO2 and CO adsorption for the K-promoted catalyst. The article interprets this as beneficial for generating CO-derived intermediates and shifting selectivity toward longer hydrocarbons, partly by moderating hydrogenation behavior.
Mechanistic interpretation was further developed with direct and indirect illumination experiments. For indirect illumination, a thin Ti2O3 layer was placed above the catalyst bed to provide similar photo-thermal heating while blocking direct photochemical excitation of the catalyst. Under direct illumination, CO2 conversion increased linearly with light intensity from 2.8 to 4.0 W cm−2, which the article interprets as characteristic of dominant non-thermal contributions with a minor thermal contribution. Indirect illumination gave substantially lower conversion, supporting the importance of direct light-induced effects. At higher intensity, the non-thermal contribution appeared to plateau.
The article also tested lower temperature operation at 200 °C. With light, the catalyst still produced hydrocarbons and formed χ-Fe5C2. Without direct light, the product stream was mainly CO and metallic Fe remained dominant. This is an important observation because it links illumination to accelerated formation of the carbide phase needed for Fischer–Tropsch-type hydrocarbon synthesis.
In situ DRIFTS was used to follow surface intermediates during reaction. Under dark conditions, the spectra showed bicarbonate and carbonate species at lower temperature, then formate species at higher temperature, followed by adsorbed CO, and finally hydrocarbon-related bands at 250 °C. The article therefore supports the sequence: CO2 adsorption as bicarbonate/carbonate → hydrogenation to formate → decomposition to CO → further hydrogenation and C–C coupling to hydrocarbons.
Comparable DRIFTS experiments on monometallic Cu and Fe clarified their different roles. On Cu, carbonate, formate, and adsorbed CO were seen, but no strong methane signal, consistent with Cu functioning mainly in reverse water-gas shift chemistry. On Fe, similar oxygenated intermediates were seen together with weaker hydrocarbon-related bands, consistent with Fe-containing phases supporting hydrocarbon formation.
Under illumination, the same classes of intermediates were observed in DRIFTS, but they appeared at lower temperature and with higher intensity. The article interprets this as evidence that light does not change the basic reaction pathway, but accelerates the formation and evolution of key intermediates. The comparison of peak intensities for bicarbonate, adsorbed CO, and olefin-related species further supported faster intermediate buildup under light.
In situ XRD directly tracked iron phase evolution. Under illumination, the metallic Fe diffraction peak diminished at lower temperature, and χ-Fe5C2 appeared earlier than under dark conditions. CO-TPR also showed lower-temperature events under illumination, including earlier CO uptake and lower-temperature Fe-phase transformation associated with carbide formation. CO2-TPSR showed similarly lower temperatures for CO2 consumption and product formation under light.
To explain these effects, the article considers three possibilities and argues that the most plausible one is plasmonic Cu-mediated promotion of Fe carburization. UV–vis spectroscopy showed a metallic Cu plasmon band near 505 nm. Transient photocurrent and TRPL measurements indicated more efficient charge separation or transfer in the bimetallic Cu–Fe catalyst than in the monometallic materials. Additional wavelength-dependent catalysis showed the highest activity under 500 nm irradiation, consistent with the Cu plasmon response. Taken together, the data support the article’s proposal that plasmonic excitation of Cu accelerates reverse water-gas shift chemistry and promotes interfacial electronic interactions with Fe, lowering the apparent barrier to χ-Fe5C2 formation.
The main products were CO, CH4, C2-C5 olefins, C2-C5 paraffins, and C6+ hydrocarbons. At higher pressure, CO selectivity decreased and hydrocarbon formation increased. Product distributions from C3 to C5 followed the Anderson–Schulz–Flory distribution according to the article. The olefin/paraffin ratio decreased at higher pressure and lower space velocity, which the authors interpret as increased hydrogenation and chain termination.
Because this is not a molecular photocatalytic system, the article does not discuss a discrete photosensitizer, reductive or oxidative quenching cycle, a sacrificial electron donor, or solution-phase reduced catalyst intermediates. Instead, light acts through the solid catalyst itself, especially through Cu-associated plasmonic excitation and photo-thermal energy delivery.
Catalyst[edit | edit source]
The catalyst is a heterogeneous potassium-promoted bimetallic Cu–Fe material, with the optimized composition designated 2K Cu2Fe1. It is not molecular, not immobilized molecularly, and not a discrete coordination complex.
Before reaction, the reduced catalyst contains metallic Cu and metallic Fe, with minor surface oxidation attributed to passivation. During reaction, the Fe phase is converted in situ mainly to χ-Fe5C2, which the article identifies as the active phase for Fischer–Tropsch-type hydrocarbon formation. Cu is assigned the main role in reverse water-gas shift chemistry, while Fe carbide is assigned the main role in C–C coupling and hydrocarbon production.
Potassium acts as a promoter that enhances CO2 adsorption, strengthens CO adsorption, and favors chain growth toward C2+ hydrocarbons. A 2 wt% K loading gave the best performance among the tested values. The catalyst also showed stable composition and performance during the reported cycling experiment after activation.
Photosensitizer[edit | edit source]
No separate molecular or heterogeneous photosensitizer is reported.
Instead, the light-harvesting function is attributed to the catalyst itself, especially the metallic Cu component, which shows a plasmon absorption band at about 505 nm. The article proposes that Cu acts as the photoactive plasmonic component, generating hot carriers and localized heating under illumination. These effects are linked to enhanced reverse water-gas shift activity and to promotion of Fe carburization at the Cu–Fe interface.
Because there is no discrete photosensitizer, the article does not report excited-state quenching by a sacrificial donor, oxidative or reductive quenching cycles, or separate photosensitizer stability data.
Investigation[edit | edit source]
| cat | cat conc [µM] | PS | PS conc [mM] | e-D | e-D conc [M] | . | . | solvent A | . | . | . | additives | . | . | . | . | λexc [nm] | . | TON CO | . | . | TON CH4 | TON H2 | . | TON HCOOH | . | . | ||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 1. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 2. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 3. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 4. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 5. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 6. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 7. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 8. | not reported | not reported | not reported | K/Ti2O3 | not reported | not reported | not reported | not reported | not reported |
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| 9. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 10. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 11. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 12. | not reported | not reported | not reported | Molecule:100493 | not reported | not reported | not reported | not reported | not reported |
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| 13. | not reported | not reported | not reported | K/Ti2O3 | not reported | not reported | not reported | not reported | not reported |
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| 14. | not reported | not reported | not reported | K/Ti2O3 | not reported | not reported | not reported | not reported | not reported |
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| 15. | not reported | not reported | not reported | K/Ti2O3 | not reported | not reported | not reported | not reported | not reported |
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| 16. | not reported | not reported | not reported | K/Ti2O3 | not reported | not reported | not reported | not reported | not reported |
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Investigations
- inv0 (Molecular process, Photocatalytic CO2 conversion experiments)

