in the present CO2/NaOH system.
In addition, Pastrana‐Martínez et al. prepared a graphene derivative–TiO2 composites for photocatalytic water reduction of CO2 into renewable fuels under UV–vis light irradiation [62]. Meanwhile, the findings present that the pH of solution has significant influence toward selective ethanol formation. The prepared GO/TiO2 composite exhibited superior photocatalytic activity for EtOH production (144.7 μmol gcat−1 h−1) at pH 11.0 and for MeOH production (47.0 μmol gcat−1 h−1) at pH 4.0. It is found that the yield of C2 hydrocarbons is much lower than that of C1 products due to the demand of more electrons and complicated reaction mechanism, which cannot be varied. Therefore, it is more feasible that the long‐chain hydrocarbons are formed as secondary products over photocatalysts that can realize efficient C1–C2 conversion in the future.
2.4.1.6 Other Hydrocarbons
Apart from these hydrocarbons produced in CO2 photoreduction with high frequency, some complicated hydrocarbons with more than two carbon numbers have been reported recently. Fusco et al. reported firstly the formation of C2 hydrocarbons, acetic acid, through CO2 photoreduction over TiO2@PEI‐grafted‐MWCNTs hybrids under UV–Vis light irradiation [63]. Besides, Park et al. decorated Cu nanoparticles and CdS quantum dots on the surface of TiO2 nanotubes, forming a ternary nanostructured photocatalyst that is capable of converting CO2 and H2O into C1–C3 hydrocarbons, including CH4, C2H6, C3H6, and C3H8 (Figure 2.12b–e) [64]. In this system, CdS quantum dots are responsible of harvesting solar light and forming hot electrons that will rapidly move to Cu nanoparticles through TiO2 nanotubes. At Cu nanoparticles, the concentrated electrons can react with CO2 molecular and produce CxHy under visible‐light excitation (above 420 nm), as shown in Figure 2.12a. In contrast, over five hours irradiation, free H2 molecular that is more easily formed than CO2 reduction products was not detected, which inferred that competitive H2 evolution reaction has been suppressed efficiently in this CdS/(Cu–TNTs) hybrid system. The photocatalytic reduction of CO2 over the CdS/(Cu–TNTs) hybrid is initiated likely through a one‐electron reduction to form ˙CO2−, reacting in turn with a H atom (H·) to produce hydrocarbons (Figure 2.12f). CO2 hydrogenation leading to hydrocarbon formation appears to be a less likely pathway because of the absence of H2 detected in the headspace of the photolysis reactor during five hours of irradiation with visible light. However, the yield and efficiency are sharply decreased owing to involvement of more electrons, formation of longer C–C chains, and production of more by‐products, which severely undermine the proportion of expected products, such as C3 or C4 hydrocarbons. Therefore, to increase the formation possibility and efficiency of major hydrocarbons, electrocatalytic CO2 reduction is paid attention through introducing more strong hot electrons to react with adsorbed CO2 molecular over a variety of electrocatalysts, leading to longer carbon chain hydrocarbons [65].
Figure 2.12 (a) Scheme of the photocatalytic CO2 reduction over CdS/(Cu–NaxH2−xTi3O7) irradiated by light. (b) Gas evolution rates of C1–C3 hydrocarbons on CdS/(Cu–NaxH2−xTi3O7) as well as the specific surface area, where the Na/Ti ratios were 0.093 (low), 0.143 (medium), and 0.507 (high). (c–e) Mass spectra of the formed hydrocarbons (methane, ethane, and propane) with the labeling of 13C. (f) Proposed elementary reaction mechanisms of photocatalytic CO2 conversion into hydrocarbons.
Source: Park et al. [64].
2.4.2 Carbon Monoxide (CO)
Apart from the hydrocarbons, other carbon‐containing fuels such as CO also are produced as main product in CO2‐involving photocatalysis [66]. From the view of redox potential, CO formation reaction (−0.48 eV vs. NHE) is inferior to the production of CH4 (−0.38 eV vs. NHE) and CH3OH (−0.24 eV vs. NHE), while the formation reactions of CH4 and CH3OH involve six‐ and eight‐electron reaction process, in which a series of elemental reaction are unclear and slow. In contrast, carbon monoxide is simpler than CH4, CH3OH, and other hydrocarbons, which means fewer needs of reductive electrons. Therefore, the CO reduction reaction is thermodynamically triggered, and CO is a preferred product in CO2 photoreduction. For instance, Miyauchi and coworkers reported CuO‐decorated Nb3O8 nanosheets for photocatalytic CO2 reduced into CO, and simultaneously the reaction pathway over this system had been deeply investigated through electron spin resonance (ESR) and isotope‐labeled experiments [67]. The results indicate that amorphous copper oxide nanoclusters can work as efficient electrocatalysts grafted onto the surface of niobate nanosheets for the reduction of carbon dioxide to carbon monoxide. Furthermore, the photocatalytic activity and reaction pathway of Cu(II)‐grafted Nb3O8 nanosheets were investigated using ESR analysis and isotope‐labeled molecules (H218O and 13CO2). The results of the labeling experiments demonstrated that under UV irradiation, electrons are extracted from water to produce oxygen (18O2) and then reduce CO2 to produce 13CO. ESR analysis confirmed that excited holes in the VB of Nb3O8 nanosheets react with water and that excited electrons in the CB of Nb3O8 nanosheets are injected into the Cu(II) nanoclusters through the interface and are involved in the reduction of CO2 into CO. The Cu(II) nanocluster‐grafted Nb3O8 nanosheets are composed of nontoxic and abundant elements and can be facilely synthesized by a wet chemical method. The nanocluster grafting technique described here can be applied for the surface activation of various semiconductor light harvesters, such as metal oxide and/or metal chalcogenides, and is expected to aid in the development of efficient CO2 photoreduction systems. Furthermore, Tahir et al. synthesized Ag nanoparticles/TiO2 nanowires core–shell heterojunction for efficient photoreduction of CO2 to CO in the presence of hydrogen [68]. Ag‐NPs coated over TiO2 NWs exhibited strong absorption of visible light due to localized surface plasmon resonance (LSPR) excitation, trapped electrons, and hindered charge recombination rate. The synergistic effect of Ag‐NPs coated over TiO2 NWs for CO2 conversion was evaluated in a gas‐phase system under UV and visible‐light irradiation. The plasmonic Ag‐NPs/TiO2 NWs demonstrated excellent photoactivity in the reduction of CO2 into CO, CH4, and CH3OH under visible‐light irradiation. The results show that 3 wt% Ag‐NPs‐loaded TiO2 NWs was found to be the most active, giving the highest CO evolution of 983 mmol g−1 h−1 at selectivity 98%. This amount of CO produced was 23 times more than the TiO2 NWs and 109 times larger than the yield of CO produced over the pure TiO2. More importantly, the quantum yield was substantially enhanced for CO evolution. The LSPR excitation and synergic effect of Ag‐NPs that can effectively accelerate the charge separation were proposed to be responsible for the enhancement of photocatalytic activity. The photostability of Ag‐NPs/TiO2 NWs evidenced in cyclic runs for selective CO production under visible light, yet photoactivity declined over the