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Review

CO2 Electroreduction over Metallic Oxide, Carbon-Based, and Molecular Catalysts: A Mini-Review of the Current Advances

1
Laboratoire de Chimie Appliquée des Matériaux, Faculty of Sciences, Mohammed V University in Rabat, Rabat 1014, Morocco
2
Mulhouse Materials Science Institute (IS2M), Université de Haute-Alsace, CNRS, UMR 7361, F-68100 Mulhouse, France
3
Département de Chimie, Université de Strasbourg, F-67000 Strasbourg, France
4
Department of Chemistry, College of Science, Princess Nourah Bint Abdulrahman University, P.O. Box 84428, Riyadh 11671, Saudi Arabia
5
Aix Marseille Univ, Univ Toulon, CNRS, IM2NP, CS 60584, CEDEX 9, F-83041 Toulon, France
*
Authors to whom correspondence should be addressed.
Catalysts 2022, 12(5), 450; https://doi.org/10.3390/catal12050450
Submission received: 11 March 2022 / Revised: 7 April 2022 / Accepted: 13 April 2022 / Published: 19 April 2022

Abstract

:
Electrochemical CO2 reduction reaction (CO2RR) is one of the most challenging targets of current energy research. Multi-electron reduction with proton-coupled reactions is more thermodynamically favorable, leading to diverse product distribution. This requires the design of stable electroactive materials having selective product generation and low overpotentials. In this review, we have explored different CO2RR electrocatalysts in the gas phase and H-cell configurations. Five groups of electrocatalysts ranging from metals and metal oxide, single atom, carbon-based, porphyrins, covalent, metal–organic frameworks, and phthalocyanines-based electrocatalysts have been reviewed. Finally, conclusions and prospects have been elaborated.

Graphical Abstract

1. Introduction

Carbon dioxide (CO2) is the most well-known greenhouse gas, which is produced both naturally and artificially. It is also required for the growth of all plants on the planet, as well as many industrial operations [1]. In an ideal world, CO2 generated on Earth would be balanced by CO2 consumed, ensuring that CO2 levels remain constant and environmental stability is maintained. Unfortunately, as human industrial activities have become more intense, this equilibrium has been broken, resulting in increased CO2 generation and making global warming an urgent concern. As a result, limiting CO2 production and turning CO2 into usable materials appears to be vital, if not critical, for environmental protection, and numerous governments throughout the world have shown their concern by boosting research funding to address the CO2 problem. Numerous research studies have focused on the development and implementation of renewable energy sources as a way to reduce reliance on fossil fuels [2,3], as well as CO2 capture and utilization technologies. CO2 usage would minimize greenhouse gas emissions in the atmosphere and seas, where they might cause harm, and CO2 could also be utilized to make valuable compounds [4,5,6].
As CO2 is the most thermodynamically stable carbon molecule, it needs a lot of energy to transform into value-added compounds. Various chemical reactions have been described that can convert CO2 into compounds such as CO, hydrocarbons, or oxygenated hydrocarbons. Gas-phase reactions, liquid-phase reactions, electrochemical reactions, and photocatalytic reactions have all been described. Gas-phase activities include dry reforming of methane (CH4 + CO2 → 2CO + 2H2) and hydrogenation of CO2 (CO2 + H2 → CO + H2O, commonly known as the water-gas shift reversal reaction; CO2 + 4H2 → CH4 + 2H2O). The liquid phase technique uses CO2 dissolved in an aqueous phase (CO2 (aq) + H2 (aq) → COOH) to make formic acid. Several review studies on CO2 hydrogenation have been published [5,6,7,8]. The hydrogenation of CO2 or the synthesis of formic acid, on either side, necessitates H2, which is most typically generated from methane by steam reforming, which also generates a significant quantity of CO2.
Although electrochemical CO2 reduction has garnered a lot of interest recently, the poor solubility of CO2 in aqueous solutions has been a major impediment. The use of a gas diffusion electrode has made it possible to employ gaseous CO2 directly for electrochemical conversion. H2 is not required as a reactant in this electrochemical conversion process. The electrochemical reduction of CO2 is not only a practical way to utilize CO2, but also a promising future alternative for storing intermittent energy from renewable sources, since it allows electrical energy to be stored in the form of chemical bonds. Carbon monoxide (CO), formic acid (HCOOH), formaldehyde (CH2O), methanol (CH3OH), methane (CH4), ethanol (C2H6O), ethylene (C2H4), or n-propanol (C3H8O) are some of the important byproducts of CO2 electroreduction [1,8]. The hurdles of converting CO2 to CH3OH are particularly daunting, but the potential benefits are huge, as CH3OH has a very high energy density and is a crucial intermediary for various bulk chemicals used in everyday items such as silicone, paints, and plastics [9,10].
In addition, the majority of electrodes used in CO2 electroreduction are metal plates, metal granules, or electrodeposited metals on a substrate [1]. The mass transfer of CO2 from the bulk to the solid electrode surface, however, is limited by the comparatively low solubility of CO2 in water under ambient circumstances, thus limiting the reaction rates and current densities of CO2 electroreduction [11,12].
This review highlights the recent progress in the field CO2 electroreduction including the use of gas diffusion electrode configuration (GDE). We have reviewed the different electrode materials ranging from oxides, metallic and bimetallic, carbon-based materials, single-atom catalysts, and molecular catalysts (porphyrins, metal–organic frameworks, covalent organic frameworks, and phthalocyanines) for the CO2 reduction to C1 and C2 chemicals. The effect of several parameters was discussed.

2. Electrocatalytic CO2 Reduction

2.1. Oxide, Metallic, and Bimetallic Catalysts

The use of gas-diffusion electrodes (GDEs) reduces CO2 by pouring pure CO2 gas onto the catalytic layer of the GDE, delivering it onto the cathode without being dissolved in catholyte in gas-phase electrolysis of CO2. A porous composite electrode, or GDE, is typically made up of polymer-bonded catalyst particles and carbon support. Higher current densities (200–600 mA cm−2) may be achieved using GDEs. Furthermore, due to their high porosity and partial hydrophobicity, GDEs create a unique gas–solid–liquid three-phase interface, allowing for a uniform dispersion across the catalytic surface. Because of these characteristics, GDEs are particularly well suited to CO2 electroreduction in the gas phase [13,14,15,16]. Janaky’s group has reported an important study on the comparison of the operation of electrolyzer cells using different anode materials. The authors showed that while Ir is stable under process conditions, the degradation of Ni leads to a rapid cell failure [17]. The same group has also shed light on other anodic oxygen evolution catalysts that are also detrimental to good GDEs stability during a CO2RR reaction [18]. Electrocatalytic reduction is frequently plagued by high overpotential, poor kinetics, limited product selectivity, and catalyst stability [19,20,21]. Noble metal electrodes provide great selectivity and stability for CO2 reduction at low over-potential [22,23,24,25]. Furthermore, catalysts based on low-cost materials, such as Sn [26,27,28], Cu [29,30], Co [31,32,33], and carbon compounds [34,35,36], are being investigated. CO is the most common result of carbon dioxide reduction reactions (CO2RR), and it is produced by Au, Ag, Zn, and Pd [37]. CO is a significant chemical feedstock for a variety of chemical reactions [16]. The binding energy of *COOH is a critical characteristic for CO generation. The metals bind to *COOH in a sequential manner, generating *CO following dehydration [38,39,40]. The CO reaction pathway consumes two electrons and is quite simple [38]. When CO is the major product, there is no need to separate the gaseous CO from the liquid electrolyte because it will spontaneously separate. To this date, we can rank three distinct groups of monometallic catalysts: (1) CO selective metals such as (Au, Ag, Pd, Ga, and Zn) [41,42]; (2) metals that mainly produce HCOOH (e.g., Pb, Cd, Sn, In, and Ti) [43,44,45,46]; (3) metals that form hydrocarbons such as CH4 and C2H4 (e.g., Cu) [47].
Numerous investigations attempting to control the nanostructures of these metals have been known to have high CO production from CO2RR, such as concave rhombic dodecahedral Au nanoparticles with high-index facets [48], TiC-supported Au nanoparticles [49], hexagonal Zn particles [50], electrodeposited Zn dendrites [51], Au electrode with adsorbed CN or Cl ions [52], Ag nanoparticles with surface-bonded oxygen [53], monodispersed Au or Ag nanoparticles [54,55], ligand-free Au nanoparticles with < 2 nm [56], and inverse opal Au or Ag thin films [57,58]. Although it is difficult to evaluate their performance due to the differences in reaction circumstances, CO2 to CO conversion typically achieves 90 to 100 percent Faradaic efficiency at a modest overpotential of 0.4 to 0.7 V. Kanan’s group [59] has reported remarkable locally enhanced CO2 reduction on gold electrode by studying the influence of bulk defects. These latter appeared to affect the faradaic efficiency and selectivity during CO2 reduction. The same group has also reported the production of formate on SnOx with a Faradaic efficiency of 58% compared to tin foil only~19%. The recorded current density of 1.8 mA cm−2 was achieved at −0.7 V vs. RHE [26].
Vasileff et al. [37] discussed and reviewed the surface and interface of copper-based-bimetallic toward CO2 electroreduction. Au has been the most typical group 1 metal alloyed with Cu for the CO2RR because it is a d-block metal with poor hydrogen and oxygen adsorption. Increased Au concentration encouraged CO generation, and the route to CH4 was restricted, according to the Christophe study [60]. CO desorption on Cu sites was aided by the decreased activation energy for CO desorption generated by Au alloying on a mechanistic level. In another study, it was discovered that the composition and nanostructure of Cu–Au nanoparticles influenced catalytic performance, resulting in the selective production of CH3OH and C2H5OH [61].
The Faradaic efficiency (FE) for alcohols in the ideal Cu63.9Au36.1 mixture was 28% (including 15.9% for CH3OH), which is 19 times greater than that of pure Cu. This study stated that *CO is a key intermediary in the conversion of CO2 to hydrocarbons and alcohols and that the binding of *CO in this Cu–Au system was likely optimized [62]. Electrochemical results from a comprehensive examination into the effect of the Cu–Au stoichiometric ratio in bimetallic catalysts revealed that alloys with higher Cu content obtained various reduction products, whereas alloys with higher Au content improved CO formation while suppressing other pathways. Cu–Au alloys were shown to enhance CO generation due to their synergistic electrical and geometric effects. The d-band center drops downwards from pure Cu to pure Au, according to density functional theory (DFT) calculations (Figure 1a). As a result, as the Au content increases, the binding strength for *COOH and *CO should decrease, and the generation of CO in Cu–Au systems should follow a monotonic pattern (Figure 1b); however, because of a geometric effect that stabilized *COOH intermediates, *COOH binding was shown to be substantially unaffected. This justifies their experimental outcomes, which show that the Au3Cu alloy has the highest FE toward CO (Figure 1c), and it gives them a better understanding of the implications of electronic structure and geometric change in bimetallic materials. Furthermore, raising the degree of atomic ordering in Cu–Au alloys was discovered to control the selectivity of CO2 reduction toward CO with a high FE of 80%, which is attributed to the stability *COOH intermediates on compressively strained Au sites [63].
By depositing a single layer of Cu with varying coverages, Ross et al. created another form of Cu–Au alloy [64]. They discovered that lower Cu coverage enhanced CO generation, whereas higher Cu coverage promoted H2 evolution. They studied the impact of the Cu/Au ratio on the *CO adsorption strength using in situ Raman microscopy and the vibration of the C-O bond in *CO species as a descriptor. The red shift in vibration of C-O was shown to be linked with bond lengthening due to increased metal contact (Figure 1d). Figure 1e shows that on more Au-dominant surfaces, the projected density of states (DOS) went farther away from the Fermi level, favoring CO generation (DFT calculations). Cu enrichment, on the other hand, improved the adsorption of *H more than it did for *CO. As a result, the degree of Cu enrichment can modify the HER’s relative activity to the CO2RR, allowing for the generation of tunable syngas (Figure 1f). Experiments in a Au–Cu core-shell (Au@Cu) system revealed that seven to eight layers of Cu resulted in greater selectivity for C2H4, but CH4 generation rose somewhat for 14 or more Cu layers [65]. The computed DFT findings revealed that on terraces, *COH intermediates were preferred over *CHO; but, as *CO coverage rose, *CHO was somewhat favored [66]. As a result, structural and electrical factors that modify the binding of *CO on Au@Cu catalysts have a considerable impact on selectivity and product distribution. In another work, Cu–Au core-shell nanostructures (Cu@Au) had a higher FE toward CO and had a higher current density than polycrystalline Cu [67].
Contemporary research has found that oxide-derived metal electrodes outperform virgin metal electrodes in terms of catalytic performance [68]. The most typical method for making oxide-derived electrocatalysts is to oxidize the metal before reducing it to its original metallic form. At the same overpotential, oxide-derived Cu generated more C2 products of C2H4, C2H6, and ethanol than electropolished Cu [68,69,70]. Cl ion-adsorbed oxide-derived Cu [71] yielded C3 and C4 products of C3H7OH, C3H6, C3H8, and C4H10. For the synthesis of formic acid, oxide-derived Sn had a substantially greater current density and Faraday efficiency than a pure Sn electrode [72]. As shown in Figure 2a, oxygen-derived Au [73] or Ag [74] had a higher FE for CO generation, ranging from 90 to 100 percent at only 0.3 V overpotential.
The origin of the increase in oxide-derived metals for CO2RR has been a point of conflict. The source of the strengthening has been proposed to be nanostructures produced in the catalysts or residual subsurface oxygen. After oxidation-reduction cycling, nanostructured surfaces with rich grain boundaries were formed [75,76]. More defect sites with greater binding energy to *CO and higher local pH were found on the induced surface, which improved selectivity toward CO2RR while reducing HER [76,77,78]. Despite the CO2RR’s extremely decreased circumstances, it was also hypothesized that some oxygen persisted in the subsurface. As demonstrated in Figure 2b [79,80], ambient pressure XPS, in situ electron energy loss spectroscopy examinations, and DFT simulations revealed that oxygen assisted in the early activation of CO2 on the surface; however, a conflicting conclusion was also published, claiming that under the CO2RR situation, the remaining oxide was highly unstable and the amount of oxygen was insignificant [81].
Commercial Cu2O and Cu2O–ZnO mixes coated on carbon sheets have been used by Albo et al. [82] to make gas-diffusion electrodes, which are tested in a filter-press electrochemical cell for continuous CO2 gas-phase electroreduction (Figure 3). The operation mostly yielded methanol, with minor amounts of ethanol and n-propanol. The investigation uses a 0.5 M KHCO3 aqueous solution to measure critical variables affecting the electroreduction process: current density (j = 10–40 mA cm−2), electrolyte flow/area ratio (Qe/A = 1–3 mL min−1 cm−2), and CO2 gas flow/area ratio (Qg/A = 10–40 mL min−1 cm−2). At an applied potential of 1.39 and 1.16 V vs. Ag/AgCl, respectively, the greatest CO2 conversion efficiency to liquid-phase products was 54.8 percent and 31.4 percent for Cu2O and Cu2O/ZnO-based electrodes.

2.2. Single-Atom Catalysts

Single-atom catalysts (SAC) are metal catalysts that are atomically scattered on the surface of a support. They have unusual selectivity and have extremely different electronic structures and adsorption patterns of reactants and intermediates [83]. Electrochemical CO2RR [84] has been studied using SACs. As shown in Figure 4 [84], Ni single atoms on N-doped graphene can selectively catalyze CO2RR and produce CO. Various metal atoms with quite different d-band structures, such as Fe, Co, Mn, and Cu, have demonstrated varying selectivity. The electronic structure and binding energy of important carbon intermediates have been found to be affected by the coordination environment around the Ni single atom [85,86]. Cu Ion-O vacancy pairs formed when Cu was atomically doped into CeO2, and the oxygen defect sites of CeO2 governed copper’s oxidation state. CO2RR was catalyzed by a single atomic Cu, which produced CH4 with a 58 percent Faraday efficiency [87]. With the right metal atoms and supports, DFT calculations predict that the SAC structure can suppress HER while promoting CO2RR [88,89]. Computational methods have also suggested single-atom alloys, in which a single-atomic metal is located on another metal surface, as effective CO2RR catalysts [90].
Pan and coworkers have developed a Co-N5 single atom through pyrolysis and wt impregnation method for the electrocatalytic reduction of CO2 to Co, reaching a Faradaic efficiency of 99% at −0.73 V vs. RHE at a current density of 6.2 mA cm−2. The Co SAC was stable for 10 h of electrolysis [33]. Another Co single atom (Co-N2) has been reported by [91] from the pyrolysis of Co/Zn MOF; this electrocatalyst achieved a Faradaic efficiency for CO2 reduction of 94% at −0.63 V vs. RHE and a current density of 18.1 2 mA cm−2. This catalyst had a steady-state stability of 60 h. Iron single atoms have also been reported for CO2 electroreduction; for instance, Pan and coworkers [92] have recently reported Fe-N-C prepared from Fe salt, Zn salt, and 2-methylimidazole. The prepared material was evaluated for CO2-to-CO with a selectivity of 93% at −0.7 V vs. RHE and a current density of 2.8 mA cm−2. This Fe SAC showed a steady-state CO evolution for 20 h. Zhang et al. [93] have synthesized an Fe/NG SAC electrocatalyst using Lyophilization and reduction of the precursors (Graphene oxide and Iron salt). The Fe/NG SAC yielded 80% Faradaic efficiency for CO and stability of 10 h.
In a CO2-saturated 0.1 M KHCO3 solution, the electrocatalytic performance of Cu-CeO2 nanorod samples was evaluated [87]. CV curves of Cu-CeO2-4% nanorods, undoped CeO2 nanorods, and Cu nanoparticles vs. a reversible hydrogen electrode (RHE, Figure 5a) were measured in a potential window between −0.2 and −1.8 V. Because CeO2 has a lower electrical conductivity than Cu, the Cu-CeO2-4% nanorods (red curve) have a lower total current density (Jtol) than pure Cu (blue curve), although they are still much greater than CeO2 (black curve). Figure 5b–d show the electrocatalytic reduction products of these three catalysts as determined by in-line gas chromatography (GC) and 1H nuclear magnetic resonance (NMR). Cu-CeO2 nanorods had a much smaller quantity of H2 side products from water reduction (gray columns in Figure 5b–d) and a significantly higher number of electrocatalytic CO2 reduction products than Cu nanoparticles and undoped CeO2 nanorods, showing strong CO2 reduction activity on the Cu-doped CeO2 electrocatalysts. The current densities for all deep reduction products (jdrp) were computed and plotted by multiplying jtotal and the corresponding FEs for all deep reduction products (i.e., CO2 reduction products excluding CO and HCOO) (Figure 5b–d, red y-axis on the right). At −1.6, −1.8, and −2.0 V versus RHE, the jdrp of the Cu-CeO2-4% nanorods reaches 40, 70, and 90 mA cm−2 (based on geometric surface area), which was many times greater than the pure Cu and undoped CeO2 samples.

2.3. Carbon-Based Catalysts

Carbon-based materials are being investigated as potential electrocatalysts for electrochemical processes such as the oxygen reduction reaction (ORR), the oxygen evolution reaction (OER), and the hydrogen evolution reaction (HER) [94,95]. Carbon materials provide a number of benefits for electrochemical applications, including the capacity to be easily transformed into different sizes and forms [96]. Well-developed material science techniques may be used to create zero-dimensional carbon dots, graphene quantum dots, one-dimensional carbon nanotubes, two-dimensional graphene, and three-dimensional graphene aerogel [21]. Carbon materials have strong chemical and mechanical stability, as well as high conductivity and surface area.
CO2RR is essentially inert to pure carbon compounds. Electrocatalytic activity is considerably improved when heteroatoms such as N are doped in the carbon matrix. CO2RR considers negatively charged N sites to be active sites [97,98]. N-doping the catalyst creates a Lewis base site, which helps to stabilize CO2 [98]. N-doped carbon nanotubes [99,100], N-doped graphene [101], and N-doped graphene quantum dots [35] are among the carbon materials that have been reported for CO2RR through the two-electron route. Acetate and formate with N-sp3C active sites were synthesized by N-doped diamonds [102]. CO2RR has also been performed with other dopants, such as S or B [103,104].
Pan et al. [33] used an N-coordination technique to build a stable CO2 reduction reaction electrocatalyst with an atomically distributed Co–N5 site anchored to hollow N-doped porous carbon spheres made from polymers. The synthesis steps are depicted in Figure 6. The authors use a modified Stöber technique [105] to make core@shell SiO2@melamine-resorcinol-formaldehyde polymer spheres (MRFPSs). Then, by pyrolyzing SiO2@MRFPSs at 700 °C under Ar, SiO2@N-doped porous carbon spheres were produced. The HNPCSs were created after etching the silica core with HF. Finally, the CoN5/HNPCSs catalyst was developed by establishing a coordination connection between Co and N. The catalyst has a strong selectivity for CO2 reduction, with a CO Faradaic efficiency (FECO) of more than 90% throughout a wide potential range of −0.57 to −0.88 V (the FECO approached 99 percent at −0.73 and −0.79 V). After electrolyzing for 10 h, the CO current density and FECO remained practically constant, demonstrating excellent stability. Experiments and density functional theory simulations demonstrate that the single-atom Co–N5 site is the primary active center for simultaneous CO2 activation, fast production of the critical intermediate COOH*, and CO desorption.
Carbon compounds doped with nitrogen are effective CO2 electroreduction catalysts [21,106]. In ionic liquids, nitrogen-doped carbon nanofibers showed a modest overpotential for CO2 reduction [36]. Although the product selectivity of each was very poor, the N-doped graphene quantum dot generated multi-carbon compounds such as ethanol, acetate, and n-propanol [35]. In aqueous conditions, nitrogen-doped mesoporous carbon was recently employed to convert CO2 to ethanol with great efficiency and selectivity (77%) [34]. Other N-doped materials for CO2 reduction reactions have been reported, including N-doped graphene [107,108], and carbon [109,110].
Because of their unique electrical and geometric properties [111], N-doped carbon nanotubes have attracted a lot of interest in CO2 reduction and other electrocatalysis [112]. NCNTs modified with polyethylenimine may convert CO2 to formate in aqueous environments with good selectivity (87%) and current density [113]. NCNT arrays produced by chemical vapor deposition (CVD) demonstrated good selectivity for CO of 80% at −0.26 V overpotential [99]. The high density of pyridinic N sites (27 percent of all Ns) in this NCNT array [100] was attributable to its superior activity. When compared to a reversible hydrogen electrode (RHE) with a pyridinic N concentration of 32%, NCNTs catalysts produced by calcination of polymers may obtain a maximum current efficiency of 90% for CO production at a potential of 0.9 V [98]. In comparison to noble-metal catalysts, however, such NCNT catalysts have a low CO current density. For more effective catalysts, increasing the N concentration is crucial.
Pyridinic N is the most significant catalytic site for carbon dioxide reduction reactions (CO2RR) among nitrogen-doped carbon materials. Graphitic N defects have a lower ability to bind CO2, while pyrrolic N defects have little to no effect on CO2RR activity; however, the atomic abundance of pyridinic N in most catalysts was low, accounting for just around 30% of all N atoms, and only a few materials could achieve a pyridinic N content of over 60%. Increasing the number of pyridinic N defects is therefore crucial. Pyrolysis is an effective method for producing high-N-content NCNTs [101,108,109].
Pyrolysis of electrospun nanofiber mats of heteroatomic polyacrylonitrile (PAN) polymer yielded a low-cost, metal-free carbon nanofiber (CNF) catalyst for CO2 reduction [36]. This catalyst’s heteroatomic structure was intended to make use of nitrogen atoms already present in the precursor’s backbone (PAN). CNF catalysts include two electrochemically active species: pyridinic nitrogen and positively charged carbon atoms. To balance out the pyridinic N’s high negative charge density, the adjacent carbon atom has a higher positive charge density and is an oxidized carbon. If the fascinating CO2 conversion seen for CNFs is linked to nitrogen functional groups, the composition of nitrogen atoms should alter dramatically following the experiment. The authors [36] evaluated the change in the N atom configuration of the CNFs catalyst by recording high-resolution N1s spectra before and after the 9 h electrochemical reaction (Figure 7). In CNFs, Figure 7a shows the presence of three primary nitrogen species: pyridinic (B.E. ~398.5 eV), quaternary (B.E. ~401.1 eV), and nitrogen oxides (B.E. ~402.2 eV). The quantitative studies show that pyridinic nitrogen makes up 25.8%, quaternary nitrogen makes up 36.7 percent, and N-oxide makes up 37.5 percent of the total nitrogen. An extra prominent N peak (pyridonic nitrogen) was identified at B.E. (400.1 eV) in the N1s spectra (Figure 7b) collected for CNFs following the 9 h reaction. According to the authors, the size of the N-oxide peak reduces dramatically (37.5–10%), showing that N-oxides are transformed into pyridonic nitrogen (peak area varies from 0 to 37%). Though, the CNF catalysts’ electrochemical activity stays unaltered, indicating that N-oxides were not involved in the CO2 conversion process. Surprisingly, following the 9-h trials, the strength of the pyridinic (very active) and quaternary nitrogen (less active) peaks stays practically unchanged. Furthermore, the authors speculated that there might be two alternative processes if pyridinic nitrogen was directly involved in the reaction. First, pyridinic nitrogen may be permanently protonated, resulting in quaternary nitrogen [114], which would increase the peak area of quaternary nitrogen since the B.E. for protonated nitrogen is comparable to that of quaternary (401.3 eV) [115]. Instead of getting irreversibly protonated, pyridinic nitrogen might weakly attach to CO2 species in a way similar to pyridine reduction, resulting in pyridinic nitrogen conversion to pyridinic species [114]. In both situations, the peak area of the pyridinic nitrogen peak would have been reduced (after tests), but it remains the same (25.8%), demonstrating that such reactions do not occur in the system. As a result, N1s spectra studies force authors to consider that positively charged carbon atoms lead to the electrochemical reduction of CO2. This is further supported by the fact that nitrogen-free carbon atom catalysts (such as graphite) have a very low CO2 reduction current density.
Based on theoretical [116,117] and experimental [118,119,120] investigations, the oxidized carbon atoms can function as excellent catalysts for reduction reactions due to their high atomic charge and spin density. The naturally oxidized carbon atoms can be decreased at first by the redox cycling mechanism. The intermediate complex [EMIM–CO2] adsorbs on reduced carbon atoms and reoxidizes them to their original form, yielding CO as a product in the second step (Figure 7e).
Wu and coworkers [101] employed a CVD method to create microporous graphene foams, which were subsequently doped with nitrogen (N) using graphitic carbon nitride (g-C3N4). In terms of CO generation, the resulting N-graphene was both active and selective, with a nitrogen content of 6.5 percent. At −0.58 V vs. the reversible hydrogen electrode (RHE), which is an overpotential of −0.47 V. Formate production was also reported, although at a low FE of 3% (at −0.58 V), implying that the CO2RR on this catalyst material follows a 2e route.
To boost the concentration of pyridine N, phenathroline was utilized as a precursor [121]. The effects of N doping and atomic configurations on activity were studied, and catalytic active sites were discovered. The mechanism of CO2RR on NCNTs was also postulated. By pyrolysis of a phenathroline heterocycle precursor, nitrogen-doped carbon nanotubes (NCNTs) with a high concentration of pyridinic N sites (62.3 percent) were created, and they can convert CO2 to CO with great selectivity and stability. Between 0.6 and 0.9 V versus the reversible hydrogen electrode (RHE), the Faradaic efficiency of CO was maintained at >94.5 percent, and the CO current density was as high as −20.2 mA cm−2 (Figure 8). Furthermore, after 40 h of electrolysis at −0.8 V, the CO faradic efficiency remained stable at 95% (Figure 8). The remarkable performance was attributed to the large quantities of pyridine N sites in NCNTs, which serve as catalytic active sites. Furthermore, gas-phase CO2 electrolysis demonstrated approximately 100% Faradic efficiency for CO (Figure 8), implying that the NCNT can optimize CO2 reduction efficiency while entirely suppressing hydrogen evolution.
Researchers coupled a high inherent defect density acquired by adjusting the size and shape of carbon nanostructures at the nanometer scale with foreign N-doping to create an improved metal-free catalyst for the electroreduction of CO2 to value-added compounds (Figure 9) [35]. The end product, N-doped graphene quantum dots (NGQDs), has a much higher density of N-doping defects at edge locations. These NGQDs have high activity for electrochemical CO2 reduction, as evidenced by high reduction current densities at low overpotentials, and, more importantly, they preferentially produce multi-carbon hydrocarbons and oxygenates, particularly the C2 products ethylene (C2H4) and ethanol (C2H5OH), at FEs comparable to those obtained with Cu nanoparticle-based catalysts.

2.4. Porphyrins, Covalent, and Metal-Organic Framework Catalysts

Porphyrins and other organometallic compounds have long been explored for the CO2RR and were among the first materials to solve the problems associated with metal electrodes [1,122,123]. In our recent study, we have elucidated the working state of iron porphyrin for the CO2-to-CO in an aqueous medium [124]. Using operando UV-spectroscopy and X-ray absorption near-edge structure spectra, we have confirmed that during the cathodic reaction, the Fe(II) species acts as catalytic sites that accommodate CO as Fe(II)–CO adducts. DFT studies have confirmed and pointed out that the ligand [Fe(II)F20(TPP•)]−prevails in the catalytic cycle prior to the rate-controlling step.
Metal-functionalized porphyrin materials that are employed as CO2RR electrocatalysts are typically synthesized as homogeneous molecular catalysts. As a consequence, a variety of porphyrins may be functionalized with a variety of transition metal centers (Co, Fe, Zn, Cu, etc.) and the resulting electrocatalysts have well-defined active centers that can be carefully adjusted for high activity and selectivity towards the CO2RR [1,125,126,127,128,129].
The active centers of heterogeneous electrocatalysts are typically difficult to characterize, making performance optimization difficult. Heterogeneous electrocatalysts, on the other hand, provide stability in electrocatalytic function, particularly in aqueous conditions, which is critical for their practical use. In general, however, these molecular catalysts are unstable and degenerate after just a few catalytic cycles, in addition to catalyst–electrolyte separation difficulties [128]. In order to synergistically boost the stability and effectiveness of homogeneous porphyrin-based catalysts, such as weak Lewis and Brönsted acids, a co-catalyst is usually used in solution with them [130,131,132]. The production of Fe porphyrin dimers with carefully adjusted Fe center spacing is a new example that addresses some of these challenges [128]. Without the use of co-catalysts, the presence of two metal centers resulted in coordinated stabilization and binding of CO2 molecules, which boosted activity and stability.
Transition metal porphyrin and other organometallic materials have recently been synthesized and constructed as metal–organic frameworks (MOFs) and covalent organic frameworks (COFs) and functionalized on other nanostructured supports such as graphene and MWCNTs in an effort to combine the exemplary features of both homogeneous and heterogeneous electrocatalysts [125,126,127,133]. The porphyrin-based materials are typically prepared using solvothermal or hydrothermal methods, and the resulting materials are then placed on conductive substrates to generate CO2RR electrodes. The structure of the prophyrins and their well-defined active metal centers are preserved since the electrocatalysts are built without high-temperature stages. Deposition on conductive substrates enhances the stability and electron transport to these active sites, resulting in an improved electrocatalytic activity.
Weng et al. [129] describe copper (II)-5,10,15,20-tetrakis (2,6-dihydroxyphenyl) porphyrin (PorCu), a novel copper-porphyrin complex with unique catalytic characteristics for CO2 reduction in neutral aqueous conditions. For electrochemical CO2 reduction to hydrocarbons, the PorCu catalyst exhibits great activity and selectivity (methane and ethylene). The catalyst converted CO2 to hydrocarbons with a Faradaic efficiency of 44 percent at a mass loading of 0.25 mg/cm2 and an electrochemical potential of −0.976 V vs. the reversible hydrogen electrode (RHE), significantly inhibiting the other CO2 reduction routes. Under the same circumstances, an ultrahigh geometric current density of 21 mA/cm2 was reached for simultaneous methane and ethylene production, resulting in turnover frequencies (TOFs) of 4.3 methane and 1.8 ethylene molecules. site−1 s−1. The built-in hydroxyl groups on the porphyrin ligand, as well as the oxidation state of the Cu center, were both key elements leading to the higher catalytic activity, according to this research.
Iron porphyrin monomers have been reported to catalyze the electrochemical CO2 reduction to CO in DMF/tetraalkylammonium salts as a supporting electrolyte, with high selectivity at the electro-generated [FeI(por)]2− (conventionally described as [Fe0(por)]2− species [134] among the non-precious metal-based 2e/2H+ coupled CO2 electrochemical reduction catalysts. These catalysts, on the other hand, degrade after just a few catalytic cycles [135]. The presence of Lewis acids such as Mg2+ and Ca2+ [132,136], or weak Brönsted acids such as trifluoroethanol and 1-propanol [130], boosts their catalytic efficiency and stability via a push–pull process where the electro-generated electron-rich [Fe0(por)]2− increases their catalytic efficiency and stability. The electron-deficient synergist Lewis or Brönsted acid stimulates the breaking of one of the C–O bonds by pushing an electron pair to the CO2 molecule [131]. Due to the large local concentration of protons associated with the phenolic hydroxy substituents, modification of the iron tetraphenylporphyrin monomer, FeTPP, with phenolic hydroxy groups at all phenyl group ortho positions improves its activity and stability for CO2 electro-reduction to CO [137]. Carbon monoxide dehydrogenase (CODH) is a metalloenzyme with a Ni–Fe dinuclear complex at its active core that facilitates the selective conversion of CO2 to CO [138]. The electrochemical process supported by CODH produces catalytic CO2 reduction with a very low overpotential [139]. As a result, dinuclear catalysts are excellent candidates for CO2 reduction catalysis. Naruta groups [128] previously documented the utilization of multiple cofacial porphyrin dimers as ligands for retaining two manganese ions with an appropriate Mn–Mn separation distance (3.7–6.2 Å) to facilitate water oxidation to oxygen or H2O2 disproportionation [140]. The utilization of a dimeric combination of two iron ions as bio-inspired catalysts was described for the first time by Naruta team [128]. In a DMF/10 percent H2O solution, a cofacial iron tetraphenyl porphyrin dimer, o-Fe2DTPP (Figure 10), effectively and selectively catalyzes the electrochemical reduction of CO2 to CO. The activity of the 1,3-phenylene bridged iron porphyrin dimer (FeTPP) was compared to that of the comparable iron porphyrin monomer (FeTPP) (m-Fe2DTPP). The CVs of o-Fe2DTPP (0.5 mM) in a DMF/10% H2O solution containing TBAPF6 (TBAPF6 = tetra-n-butylammonium hexafluorophosphate, 0.1 M) saturated with Ar gas (blue line) or CO2 gas (red line) are shown in Figure 10b. The detection of a significant catalytic current in the presence of CO2 gas was the most intriguing discovery, showing electrocatalytic CO2 reduction enhanced by o-Fe2DTPP. The emergence of the catalytic peak over the Fe+–Fe+/Fe+–Fe0 redox couple under Ar at −1.48/−1.46 V vs. NHE (later, all potentials are given against NHE unless otherwise mentioned) shows the beginning of the catalytic process after the Fe+–Fe0 porphyrin species was electro-generated. Figure 10c depicts the temporal sequence of the products’ appearance. Without the catalyst, H2 is the only product produced with 99 percent Faradic efficiency and a low average current density of −0.1 mA cm−2. In the presence of o-Fe2DTPP, however, a considerable charge, Q = 41.4 C, was burned at an average current density of −1.15 mA cm−2 across a 10 h electrolysis process, with the concurrent generation of CO (88 percent Faradic efficiency) and H2 (12 percent Faradic efficiency). When the quantity of H2 created during the control experiment is subtracted, the dimer catalyzes the CO2 reduction to CO with 95% Faradic efficiency. The present density–time profile revealed no reduction over the previous ten hours.
A study describes the electrochemical reduction of CO2 to CO and methane, as well as trace quantities of HCOOH and methanol, using a simple Co protoporphyrin molecular catalyst immobilized on a pyrolytic graphite (PG) electrode in a completely aqueous electrolyte solution [127]. Previous research utilizing immobilized Co porphyrins or Co phthalocyanines demonstrated that Co-based catalysts might reach a high FE towards CO, which is very sensitive to pH and potential [141,142,143]. Immobilized Co-based porphyrins are excellent CO2 reduction electrocatalysts, according to Shen et al. [127], and can produce multi-electron products such as methane and methanol. More importantly, this research highlights the importance of pH in directing catalytic activity and selectivity towards CO and CH4, particularly in the absence of coordinating anions in the pH range of 1–3. This great sensitivity to pH is explained by a mechanism that emphasizes the critical significance of the first electron transfer in electrochemically activating CO2. The authors also show how such a CO2 reduction process occurs in the experiment and how this characteristic might be used to restrict concurrent hydrogen evolution. Furthermore, researchers demonstrate that the catalyst’s overpotential and associated turnover frequency (TOF) for CO2 reduction match favorably with the best molecular porphyrin-based catalyst in the literature [137]. The authors proposed the mechanism of their study in Figure 11a. As a result, the authors believe that these findings could have significant implications for the development of new and improved molecular catalyst electrodes, as well as the formulation of optimized process conditions for efficient electrochemical CO2 reduction to CO and the reduction of products to a greater degree. Cobalt porphyrins were investigated in order to take advantage of the frameworks’ distinctive features, such as charge carrier mobility due to π–π stacking and the stability afforded by covalent bonding and reticular geometries [140]. When deposited on porous carbon fabric for electrochemical testing, the COFs had a catalytic onset potential of −0.42 V vs. RHE in CO2 saturated carbonate electrolyte and a maximal activity of −0.67 V vs. RHE, generating CO predominantly at a FE of 90%. With hydrogen evolution being favored at increasingly negative potentials, this strong selectivity for the CO2RR begins to decrease.
COFs were synthesized with longer linkage molecules to increase the spacing between porphyrins for greater pore volume, as illustrated in Figure 1b, in order to improve their performance. As a result, more electrolyte access and CO2 adsorption were possible, resulting in a lower onset potential (−0.40 V) and a 2.2-fold increase in catalytic activity at −0.67 V. For graphene-enhanced CO2 diffusion restrictions, as well as Re-porphyrins, were discovered to have a considerable impact on activity [144]. In comparison to non-stirring circumstances, stirring to boost CO2 diffusion into the electrolyte increased the reaction rate by three times while maintaining selectivity. This is inextricably tied to the fact that, whereas active centers are clearly defined in these materials, active site density is often low, necessitating effective use of active sites.
Wang and coworkers [145] have used the synthesis of silver MOF-mediated as a simple and scalable method to prepare highly dispersed supported Ag catalysts with very low metal loadings for CO2ER in GDE configuration. The resulting Ag-coordination polymer was directly grown in carbon paper with a microporous layer. The remarkable activity of these catalysts reached a Faradaic efficiency of more than 96% for CO production at an outstanding current density of 300 mA cm−2. This technology of using MOF materials as mediators to prepare ordered metallic and doped structures have known considerable attention in the past decade [146,147,148,149,150].

2.5. Phthalocyanines-Based Catalysts

Lu and coworkers [151] have used cobalt phthalocyanines (CoPC) as an electrocatalyst for CO2 reduction to CO. The authors have used microflow cell configurations at low voltages using a KOH catholyte. The cell was operating at 0.26 overpotential, reaching nearly 94% Faradaic efficiency. The partial current density of CO2-TO-CO reached 31 mA/cm−2. This study outperforms the previously reported cobalt phthalocyanine in the H-Cell configuration, which yielded only −6 mA/cm−2 total current density and a Faradaic efficiency of 93% of CO [152]. Previously reported literature has suggested that incorporation of CoPc in a coordination polymer such as poly-4-vinylpyridine (P4VP) can lead to a selective CO2 reduction activity over hydrogen evolution reaction, which is a CO2RR competing reaction [142,153,154,155].
More recently, Liu et al. [156] have revealed the effect of using the P4VP coordination polymer encapsulation on CO2RR activity. Indeed, authors have shown that the rate-determining step in the CO2 mechanism is axial coordination from the pyridyl moieties in poly-4-vinylpyridine to CoPc while the HER was suppressed due to the sluggish and weak proton transport through the polymer. Whereas earlier, another team used a scanning tunnel microscope to unveil the CO2RR mechanism over CoPC catalysts, the authors have revealed that making the CoIPC-CO2 intermediate is the rate-limiting step [157]. X. Zhang [158] has elaborated on carbon materials supported by CoPC for CO2 reduction; the CoPC/CNT material had the best Faradaic efficiency of CO production (90%) at a current density of −10 mA/cm−2 at −0.63V vs. RHE. The carbon black/CoPc and reduced graphene oxide/CoPc showed less than a third of the current density at −0.59 V vs. RHE and a lower FE(CO) as well as low reusability. The authors have yet to improve their performance of the CoPC/CNTs by using the Cyano-substituted CoPc hybrid approach and the prepared catalyst was noted as CoPc-CN/CNT. This substituted catalyst had a current density of −15 mA/cm−2 and FE(CO) of 95%. The CNT hybridization acts as a conducting platform, allowing the easiness of electron transfer and enabling the high degree of catalytic site exposure that leads to high current densities. The cyano groups facilitate the electron withdrawal to form the CoI responsible for CO2-to-CO reduction.
Copper phthalocyanines (CuPC) have been studied by several groups for their interesting properties for CO2 reduction properties. Latiff and coworkers [159] have developed a long (10–30 μm) and thin (10–30 nm Ø) carbon nanotubes supported by CuPC structures that can efficiently reduce CO2 with better Faradaic efficiencies. The CuPC/CNTs yielded an overall Faradaic efficiency of 66.3% for C1 and C2 byproducts, with CO being the highest evolving product with a Faradaic efficiency of nearly 44% (Figure 12).
B. Mei et al. have used operando elucidation of the dynamic and structural transformation of CuPc during CO2RR electrolysis (Figure 13). Authors have applied operando high-energy resolution fluorescence-detected X-ray absorption spectroscopy to reveal the responsible phenomenon for their observed C2H4 formation. They have suggested that the main phenomenon taking place is the aggregation of Cu sites (making copper clusters) with applied potential, leading to the byproduct’s formation [160]. Whereas S. Kusama and coworkers reached high electrochemical CO2 reduction to C2H4 with a Faradaic efficiency of 25% by using bare crystalline CuPC supported by a conductive carbon black at −1.6 V vs. Ag/AgCl. The CO and CH4 were also produced but with low Faradaic efficiency when a limited electrolysis time was performed; however, when long-term 12 h electrolysis was performed, the CO evolution became more pronounceable, terminating the C2H4 evolution [161].
Other metal phthalocyanines have also been studied for CO2 reduction electrolysis, such as tin phthalocyanine [162], nickel phthalocyanines [163], iron phthalocyanines [164], and zinc phthalocyanines [165]. In the case of tin phthalocyanine dichloride, the resulting aggregation hybrid catalyst can catalyze the electroreduction of CO2 to HCOOH and CO at a total Faradaic efficiency of ca. 90%. The active site of tin phthalocyanine dichloride responsible for electrocatalytic CO2 reduction is confirmed to be metallic Sn, whose local structure is strongly affected by the adjacent macrocyclic ligands. The dispersed NiPc molecules unlocked remarkable electrocatalytic properties for the CO2RR, unlike the aggregated form. The molecular dispersed electrocatalyst NiPc–OMe exhibited FE(CO)s of >99.5% over a wide current density range of −10 to −300 mA cm−2 and stable performance at the practically relevant current density of −150 mA cm−2 for 40 h [163].
The iron phthalocyanine electrocatalytic performance of FePc-G, FePc-Gr, FePc-R, FePc-R/H2O2, FePc/G heterostructures, FePc nanorods, and graphene were investigated to elucidate the role of iron valence degree +II and +III. The optimal catalyst exhibited a high FECO of >90% at about −0.5 V vs. RHE and an onset potential of −190 mV, and syngas production is easy to obtain and depends mainly on the potential. Furthermore, the DFT simulation revealed that for CO2RR, the catalytic activity of Fe(II)Pc should be better than Fe(III)Pc, and that of Fe(II)Pc/Fe(III)Pc dimer higher than individual Fe(II)Pc or Fe(III)Pc [164]. Finally, ZnPc/carbon nitride nanosheet hybrid catalysts could be effectively excited by visible light for PEC-CO2RR. The major product was methanol, and the highest methanol generation efficiency was achieved at −1.0 V. The methanol yield was 13 µmol. L−1 after 8 h. The mechanisms for the three different CO2RR processes, including PC, EC, and PEC-CO2RR, are proposed. In PEC-CO2RR, ZnPc/-carbon nitride nanosheets exhibited a synergic effect and methanol production efficiency is much better PC- and EC-CO2RR [165].

2.6. CO2 Reduction Mechanisms

Depending on the three classes of electrocatalysts that were highlighted in the sub-Section 2.1. Different CO2 value-added products can be obtained. The target byproducts are controlled by tuning the binding energy of the adsorbed intermediate such as (CO*, COOH*, CHO*, COH*) (Figure 14). For example, when the interaction between the surface of the electrocatalysts and the reduction intermediates is not strong enough, CO and formate are the main reduction products (Type 1 and 2). Inversely, when the electrocatalysts bind strongly with CO*, this will be further reduced to other by-products (Type 3) [166]. This is where copper shows an incredible ability to transform CO2 into hydrocarbons, The basic explanation for its ability to generate products other than CO is that Cu binds *CO neither too weakly nor too strongly [37].

3. Conclusions and Prospects

The Electrochemical CO2 reduction technique is still in its early stages compared to other CO2 conversion technologies, although it is being actively researched. For electrochemical CO2 reduction, a range of materials have been investigated as catalysts, and the catalysts should be modified depending on the intended products. Nanostructured catalysts should be further adjusted in light of the cell design of gas-diffusion electrodes. To date, the majority of investigations have employed pure CO2 that has been concentrated; however, for practical applications, the conversion of dilute CO2, especially in the presence of possible catalyst poisons such as S compounds, should be researched more intensively. In addition, several technological hurdles remain in CO2 electrochemical reduction technology, including (i) inadequate catalyst activity, (ii) limited product selectivity, and (iii) insufficient stability. Our technology appears to be far from adequate when it comes to the actual application of CO2 reduction to creating useable low-carbon fuels. Low catalyst stability appears to be the current key barrier to industrial-scale deployment. As a result, the main emphasis of effort in this field remains the development of highly active, selective, and stable electrocatalysts for CO2 reduction.

Author Contributions

H.A.A.: Conceptualization; Writing the draft, Data curation; Formal analysis; Project administration. M.Z.: Writing the draft, review & editing; Data curation; Formal analysis. A.B.: Writing—review & editing. M.A.: Writing—review & editing. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Acknowledgments

This work was supported by the faculty of sciences and the Mohammed V University in Rabat.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Characterization and performance of Cu–Au catalysts for the CO2RR. (ac) Surface valence-band photoemission spectra of Au–Cu bimetallic nanoparticles (the white bars indicate the d-band centers) (a); proposed mechanism for the CO2RR on the surface of Au–Cu bimetallic nanoparticles (gray, red, and white atoms represent C, O, and H, respectively) (b); CO generation rate on various alloy electrocatalysts at a certain overpotential (inset shows relative CO generation rate as a function of the applied potential) (c). (Reprinted with permission from Ref. [51]. Copyright 2015 American Chemical Society). (df) Scheme depicting the relationship between the Cu-enriched Au surface, in situ characterization of CO* coordination, and syngas composition (d); calculated d-band electronic states for increasingly Cu-enriched Au surfaces (e); partial current densities (left axis) and production rates (right axis) for CO and H2 as a function of Cu monolayer deposition on Au (f). (Reprinted with permission from Ref. [64]. Copyright 2017 American Chemical Society).
Figure 1. Characterization and performance of Cu–Au catalysts for the CO2RR. (ac) Surface valence-band photoemission spectra of Au–Cu bimetallic nanoparticles (the white bars indicate the d-band centers) (a); proposed mechanism for the CO2RR on the surface of Au–Cu bimetallic nanoparticles (gray, red, and white atoms represent C, O, and H, respectively) (b); CO generation rate on various alloy electrocatalysts at a certain overpotential (inset shows relative CO generation rate as a function of the applied potential) (c). (Reprinted with permission from Ref. [51]. Copyright 2015 American Chemical Society). (df) Scheme depicting the relationship between the Cu-enriched Au surface, in situ characterization of CO* coordination, and syngas composition (d); calculated d-band electronic states for increasingly Cu-enriched Au surfaces (e); partial current densities (left axis) and production rates (right axis) for CO and H2 as a function of Cu monolayer deposition on Au (f). (Reprinted with permission from Ref. [64]. Copyright 2017 American Chemical Society).
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Figure 2. (a): FEs for CO and HCO2 production on oxide-derived Au and polycrystalline Au electrodes at various potentials between −0.2 and −0.5 V in 0.5 M NaHCO3, pH 7.2. Dashed line indicates the CO equilibrium potential. (b): suggested mechanisms for CO2 reduction to CO on polycrystalline Au and oxide-derived Au (Reprinted with permission from Ref. [74]. Copyright 2016 Wiley-VCH).
Figure 2. (a): FEs for CO and HCO2 production on oxide-derived Au and polycrystalline Au electrodes at various potentials between −0.2 and −0.5 V in 0.5 M NaHCO3, pH 7.2. Dashed line indicates the CO equilibrium potential. (b): suggested mechanisms for CO2 reduction to CO on polycrystalline Au and oxide-derived Au (Reprinted with permission from Ref. [74]. Copyright 2016 Wiley-VCH).
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Figure 3. Representation diagram of the electrolytic cell configuration for the electroreduction of CO2 supplied directly from the gas phase. In this study, the filter-press electrochemical system possesses three inputs (catholyte, anolyte, and CO2 separately) and two outputs (catholyte–CO2 and anolyte) for the electroreduction of CO2 in gas phase. (Reprinted with permission from Ref. [82]. Copyright 2016 Elsevier).
Figure 3. Representation diagram of the electrolytic cell configuration for the electroreduction of CO2 supplied directly from the gas phase. In this study, the filter-press electrochemical system possesses three inputs (catholyte, anolyte, and CO2 separately) and two outputs (catholyte–CO2 and anolyte) for the electroreduction of CO2 in gas phase. (Reprinted with permission from Ref. [82]. Copyright 2016 Elsevier).
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Figure 4. Structural evolution of Ni single-atom sites on graphene during CO2RR. ΔD in shows the displacement of Ni atom out of plane resulting from electron transfer from Ni atom to CO2. The upper-right schematic shows the activation processes for CO2 molecules on the Ni(i) site. A valence band structure, similar to metallic nickel, was used to simplify the schematic illustration. The red arrow represents the electron transfer from the Ni(i) to adsorbed CO2. E F 1 and E F 2 are Fermi levels of A-Ni-NG before and after formation of Ni-CO2, respectively. 1πg and 2πu are CO2 molecular orbitals. (Reprinted with permission from Ref. [84]. Copyright 2018 SpringerNature).
Figure 4. Structural evolution of Ni single-atom sites on graphene during CO2RR. ΔD in shows the displacement of Ni atom out of plane resulting from electron transfer from Ni atom to CO2. The upper-right schematic shows the activation processes for CO2 molecules on the Ni(i) site. A valence band structure, similar to metallic nickel, was used to simplify the schematic illustration. The red arrow represents the electron transfer from the Ni(i) to adsorbed CO2. E F 1 and E F 2 are Fermi levels of A-Ni-NG before and after formation of Ni-CO2, respectively. 1πg and 2πu are CO2 molecular orbitals. (Reprinted with permission from Ref. [84]. Copyright 2018 SpringerNature).
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Figure 5. Electrochemical CO2 reduction performance. (a) Cyclic voltammetry curves for Cu-CeO2, CeO2, and Cu. (bd) Faradaic efficiencies (bars on the left y−axis) and deep reduction product current density (jdrp, red curves on the right y−axis) of (b) Cu−CeO2−4%, (c) pure Cu, and (d) undoped CeO2 at various overpotentials. The deep reduction products were the first five products in the legends at the bottom, marked with a red line. (e) A comparison of the Faradaic efficiency of samples with varying levels of Cu doping. (f) Stability of FECH4 (blue squares) and FEH2 (black squares) on the left y−axis. Right y−axis: total current density (jtotal) of Cu−CeO2−4% at −1.8 V (red curves, right y−axis). (Reprinted with permission from Ref. [87]. Copyright 2018 American Chemical Society).
Figure 5. Electrochemical CO2 reduction performance. (a) Cyclic voltammetry curves for Cu-CeO2, CeO2, and Cu. (bd) Faradaic efficiencies (bars on the left y−axis) and deep reduction product current density (jdrp, red curves on the right y−axis) of (b) Cu−CeO2−4%, (c) pure Cu, and (d) undoped CeO2 at various overpotentials. The deep reduction products were the first five products in the legends at the bottom, marked with a red line. (e) A comparison of the Faradaic efficiency of samples with varying levels of Cu doping. (f) Stability of FECH4 (blue squares) and FEH2 (black squares) on the left y−axis. Right y−axis: total current density (jtotal) of Cu−CeO2−4% at −1.8 V (red curves, right y−axis). (Reprinted with permission from Ref. [87]. Copyright 2018 American Chemical Society).
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Figure 6. Schematic illustration of catalyst preparation. The core@shell SiO2@melamine-resorcinol-formaldehyde polymer spheres (MRFPSs) were first synthesized. Then, SiO2@N-doped porous carbon spheres were obtained by pyrolysis of SiO2@MRFPSs at 700 °C under Ar. After etching the silica core with HF, the HNPCSs were obtained. Finally, the Co−N5/HNPCSs catalyst was prepared through constructing coordination interaction between Co and N. (Reprinted with permission from Ref. [33]. Copyright 2018 American Chemical Society).
Figure 6. Schematic illustration of catalyst preparation. The core@shell SiO2@melamine-resorcinol-formaldehyde polymer spheres (MRFPSs) were first synthesized. Then, SiO2@N-doped porous carbon spheres were obtained by pyrolysis of SiO2@MRFPSs at 700 °C under Ar. After etching the silica core with HF, the HNPCSs were obtained. Finally, the Co−N5/HNPCSs catalyst was prepared through constructing coordination interaction between Co and N. (Reprinted with permission from Ref. [33]. Copyright 2018 American Chemical Society).
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Figure 7. (ad) Evolution of nitrogen atomic nature in CNFs by XPS. (a) Deconvoluted N1s spectra for CNFs before and (b) after electrochemical experiments. In used catalysts, CNFs N1s spectra, N-oxide type of nitrogen content reduced radically and new peak (green solid line) at 400.2 eV (pyridonic N) appears. (c,d) The corresponding atomic structure on the basis of XPS analysis. (e): CO2 reduction mechanism schematic diagram. The CO2 reduction reaction takes place in three steps: (1) an intermediate (EMIM–CO2 complex) formation, (2) adsorption of EMIM–CO2 complex on the reduced carbon atoms, and (3) CO formation. (Reprinted with permission from Ref. [36]. Copyright 2013 SpringerNature).
Figure 7. (ad) Evolution of nitrogen atomic nature in CNFs by XPS. (a) Deconvoluted N1s spectra for CNFs before and (b) after electrochemical experiments. In used catalysts, CNFs N1s spectra, N-oxide type of nitrogen content reduced radically and new peak (green solid line) at 400.2 eV (pyridonic N) appears. (c,d) The corresponding atomic structure on the basis of XPS analysis. (e): CO2 reduction mechanism schematic diagram. The CO2 reduction reaction takes place in three steps: (1) an intermediate (EMIM–CO2 complex) formation, (2) adsorption of EMIM–CO2 complex on the reduced carbon atoms, and (3) CO formation. (Reprinted with permission from Ref. [36]. Copyright 2013 SpringerNature).
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Figure 8. Gas−phase electrolysis in a flow cell and gas-phase CO2 electrolysis. FE of CO (blue) and H2 (red) vs. cell voltage (left axis) and partial current density of CO vs. cell voltage (right axis), values above the column are cathode potentials vs. normal hydrogen electrode (NHE) (Reprinted with permission from Ref. [121]. Copyright 2019 Elsevier).
Figure 8. Gas−phase electrolysis in a flow cell and gas-phase CO2 electrolysis. FE of CO (blue) and H2 (red) vs. cell voltage (left axis) and partial current density of CO vs. cell voltage (right axis), values above the column are cathode potentials vs. normal hydrogen electrode (NHE) (Reprinted with permission from Ref. [121]. Copyright 2019 Elsevier).
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Figure 9. Electrocatalytic activity of carbon nanostructures towards CO2 reduction. (a) FEs of carbon monoxide (CO), methane (CH4), ethylene (C2H4), formate (HCOO), ethanol (EtOH), acetate (AcO) and n-propanol (n-PrOH) at various applied cathodic potential for NGQDs. (b) FE of CO2 reduction products for pristine GQDs. (c) Selectivity to CO2 reduction products for NRGOs. (d) Tafel plots of partial current density of CO2 reduction versus applied cathodic potential for three nanostructured carbon catalysts. The error bar represents the s.d. of three separate measurements for an electrode. (Reprinted with permission from Ref. [35]. Copyright 2016 SpringerNature).
Figure 9. Electrocatalytic activity of carbon nanostructures towards CO2 reduction. (a) FEs of carbon monoxide (CO), methane (CH4), ethylene (C2H4), formate (HCOO), ethanol (EtOH), acetate (AcO) and n-propanol (n-PrOH) at various applied cathodic potential for NGQDs. (b) FE of CO2 reduction products for pristine GQDs. (c) Selectivity to CO2 reduction products for NRGOs. (d) Tafel plots of partial current density of CO2 reduction versus applied cathodic potential for three nanostructured carbon catalysts. The error bar represents the s.d. of three separate measurements for an electrode. (Reprinted with permission from Ref. [35]. Copyright 2016 SpringerNature).
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Figure 10. (a) Chemical structures of the iron porphyrin monomer, FeTPP, and iron porphyrin dimers, o−Fe2DTPP and m-Fe2DTPP. (b) CVs of o−Fe2DTPP at 100 mV scan rate in DMF/10% H2O containing 0.1 M TBAPF6 supporting electrolyte under Ar or CO2. Inset: magnified trace of CVs. (c) CO2 reduction products with time and the current density–time profile (inset) produced during the 10 h chronoamperometry experiment at −1.35 V vs. NHE in a DMF/10% H2O/0.1 M TBAPF6 solution saturated with CO2 without (black lines) and with 0.5 mM o−Fe2DTPP (red lines). (Reprinted with permission from Ref. [128]. Copyright 2015 Royal Society of Chemistry).
Figure 10. (a) Chemical structures of the iron porphyrin monomer, FeTPP, and iron porphyrin dimers, o−Fe2DTPP and m-Fe2DTPP. (b) CVs of o−Fe2DTPP at 100 mV scan rate in DMF/10% H2O containing 0.1 M TBAPF6 supporting electrolyte under Ar or CO2. Inset: magnified trace of CVs. (c) CO2 reduction products with time and the current density–time profile (inset) produced during the 10 h chronoamperometry experiment at −1.35 V vs. NHE in a DMF/10% H2O/0.1 M TBAPF6 solution saturated with CO2 without (black lines) and with 0.5 mM o−Fe2DTPP (red lines). (Reprinted with permission from Ref. [128]. Copyright 2015 Royal Society of Chemistry).
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Figure 11. (a) Proposed mechanistic scheme for the electrochemical reduction of CO2 on Co protoporphyrin. (Reprinted with permission from ref. [126]. 2015, American Association for the Advancement of Science). (b) Design and synthesis of metalloporphyrin-derived 2D covalent organic frameworks. Materials Studio 7.0 was used to generate space-filling structural models of COF-366-M and COF-367-M, which were then improved with experimental PXRD data. (Reprinted with permission from Ref. [126]. Copyright 2015 American Association for the Advancement of Science).
Figure 11. (a) Proposed mechanistic scheme for the electrochemical reduction of CO2 on Co protoporphyrin. (Reprinted with permission from ref. [126]. 2015, American Association for the Advancement of Science). (b) Design and synthesis of metalloporphyrin-derived 2D covalent organic frameworks. Materials Studio 7.0 was used to generate space-filling structural models of COF-366-M and COF-367-M, which were then improved with experimental PXRD data. (Reprinted with permission from Ref. [126]. Copyright 2015 American Association for the Advancement of Science).
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Figure 12. (A) CV measurements of various carbon-supported copper(II) phthalocyanines in CO2-saturated (marked in continuous lines) and N2-saturated (marked in dotted lines) 0.5 M KCl solution. (B) Chronoamperometry measurements of the materials over 1 h under an applied potential of −1.05 V vs. RHE. (C) Corresponding product analysis results from chronoamperometry runs. (D) EIS spectra for the materials under study are shown by their Nyquist plots, where CPE stands for constant phase element (Reprinted with permission from Ref. [159]. Copyright 2020 Elsevier).
Figure 12. (A) CV measurements of various carbon-supported copper(II) phthalocyanines in CO2-saturated (marked in continuous lines) and N2-saturated (marked in dotted lines) 0.5 M KCl solution. (B) Chronoamperometry measurements of the materials over 1 h under an applied potential of −1.05 V vs. RHE. (C) Corresponding product analysis results from chronoamperometry runs. (D) EIS spectra for the materials under study are shown by their Nyquist plots, where CPE stands for constant phase element (Reprinted with permission from Ref. [159]. Copyright 2020 Elsevier).
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Figure 13. (a) Energy scheme of Kα and Kβ emission lines. (b) Experimental setup; (c) Kα-RIXS plane of CuO around the Cu K-edge. The contour planes at the emission energy of ~8026 and 8046 eV are the Kα2 and Kα1-RIXS plane, respectively. The black-dashed line located at constant emission energy of 8046.3 eV. (d) HERFD-XANES (red) and conventional XANES (blue) spectra of CuO (Reprinted with permission from Ref. [160]. Copyright 2022 Elsevier).
Figure 13. (a) Energy scheme of Kα and Kβ emission lines. (b) Experimental setup; (c) Kα-RIXS plane of CuO around the Cu K-edge. The contour planes at the emission energy of ~8026 and 8046 eV are the Kα2 and Kα1-RIXS plane, respectively. The black-dashed line located at constant emission energy of 8046.3 eV. (d) HERFD-XANES (red) and conventional XANES (blue) spectra of CuO (Reprinted with permission from Ref. [160]. Copyright 2022 Elsevier).
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Figure 14. Schematic mechanism of different metal electrocatalysts for CO2 reduction reaction in aqueous solution. (Reprinted with permission from Ref. [165]. Copyright 2019 Elsevier).
Figure 14. Schematic mechanism of different metal electrocatalysts for CO2 reduction reaction in aqueous solution. (Reprinted with permission from Ref. [165]. Copyright 2019 Elsevier).
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Ait Ahsaine, H.; Zbair, M.; BaQais, A.; Arab, M. CO2 Electroreduction over Metallic Oxide, Carbon-Based, and Molecular Catalysts: A Mini-Review of the Current Advances. Catalysts 2022, 12, 450. https://doi.org/10.3390/catal12050450

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Ait Ahsaine H, Zbair M, BaQais A, Arab M. CO2 Electroreduction over Metallic Oxide, Carbon-Based, and Molecular Catalysts: A Mini-Review of the Current Advances. Catalysts. 2022; 12(5):450. https://doi.org/10.3390/catal12050450

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Ait Ahsaine, Hassan, Mohamed Zbair, Amal BaQais, and Madjid Arab. 2022. "CO2 Electroreduction over Metallic Oxide, Carbon-Based, and Molecular Catalysts: A Mini-Review of the Current Advances" Catalysts 12, no. 5: 450. https://doi.org/10.3390/catal12050450

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Ait Ahsaine, H., Zbair, M., BaQais, A., & Arab, M. (2022). CO2 Electroreduction over Metallic Oxide, Carbon-Based, and Molecular Catalysts: A Mini-Review of the Current Advances. Catalysts, 12(5), 450. https://doi.org/10.3390/catal12050450

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