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Review

Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction

by
Tong Wu
,
Lihua Zhang
,
Yinbo Zhan
,
Yilin Dong
,
Zheng Tan
,
Bowei Zhou
,
Fei Wei
,
Dongliang Zhang
and
Xia Long
*
Low Carbon College, Shanghai Jiaotong University, Shanghai 201306, China
*
Author to whom correspondence should be addressed.
Molecules 2023, 28(24), 8154; https://doi.org/10.3390/molecules28248154
Submission received: 28 November 2023 / Revised: 15 December 2023 / Accepted: 16 December 2023 / Published: 18 December 2023
(This article belongs to the Special Issue Exclusive Feature Papers in Inorganic Chemistry, 2nd Edition)
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Versions Notes

Abstract

:
An efficient carbon dioxide reduction reaction (CO2RR), which reduces CO2 to low-carbon fuels and high-value chemicals, is a promising approach for realizing the goal of carbon neutrality, for which effective but low-cost catalysts are critically important. Recently, many inorganic perovskite-based materials with tunable chemical compositions have been applied in the electrochemical CO2RR, which exhibited advanced catalytic performance. Therefore, a timely review of this progress, which has not been reported to date, is imperative. Herein, the physicochemical characteristics, fabrication methods and applications of inorganic perovskites and their derivatives in electrochemical CO2RR are systematically reviewed, with emphasis on the structural evolution and product selectivity of these electrocatalysts. What is more, the current challenges and future directions of perovskite-based materials regarding efficient CO2RR are proposed, to shed light on the further development of this prospective research area.

1. Introduction

The booming development of industry and the economic level of modern society lead to an exponential growth in demand for energy, while the massive consumption of fossil fuels has resulted in some terrible environmental problems [1,2]. According to a report by the International Energy Agency (IEA), the total global greenhouse gas emissions in 2021 reached an equivalent of 40.8 billion tons of carbon dioxide (CO2), in which fuel combustion and industrial production accounted for ~89% [3,4]. Several strategies and policies such as the Paris Agreement [5,6] and China’s “3060 two carbon goals” have been proposed to tackle carbon emission issues, which have stimulated extensive fundamental studies on developing efficient materials and technologies to convert CO2 into value-added chemicals.
The electrochemical reduction in CO2, activated by electricity from renewable energy sources such as wind, solar, etc., is one of the most promising methods for realizing the re-utilization of CO2 and dealing with the intermittency problem of renewable energy sources [7,8]. However, due to the stable chemical properties of CO2 molecules, the CO2 reduction process usually requires relatively harsh operation conditions, and the reaction pathways are greatly complicated, leading to varieties of products (e.g., CO, CH4, CH3OH, HCOOH, C2H4, C2H6, CH3CH2OH, CH3COOH, CH3CH2CH2OH, etc.) [9], despite the distinct equilibrium potentials of producing these chemicals (Table 1) [10]. Therefore, efficient catalysts with high activity, target product selectivity, and long-term stability are required to facilitate the CO2 reduction reaction (CO2RR) to meet the requirements of practical applications. Many significant achievements concerning noble-metal free electrocatalysts, especially inorganic perovskite oxides, which have some promising compositional and structural characters, have recently been obtained. Therefore, a timely review of this progress would surely attract a wide readership from both energy and material science search areas and contribute to the further advancement of CO2RR systems. Herein, as illustrated in Figure 1, we start with an introduction of the fundamental principles of CO2RR and the unique physicochemical properties of perovskites as electrocatalysts, followed by a detailed discussion on the applications of perovskite-based materials in the electrocatalysis of CO2RR, with emphasis on the investigation of structural evolution and product selectivity, using representative works published in the last few years. Finally, insights into the status, challenges and prospects for future research opportunities are provided. The search criteria used in this review included CO2RR/CO2ER and perovskite. Though most results were about solid oxide electrolyzers with high operation temperatures, our work mainly focuses on the low-temperature electrochemical studies of CO2RR catalyzed by perovskite-based materials. According to the search results, the works on utilizing perovskites as electrocatalysts for CO2RR are very limited, lacking a comprehensive review of the progress in this field. Herein, we provide such a review that systematically introduces the representative works published so far and discusses the key points deserving attention in future studies on electrochemical CO2RR processes catalyzed by perovskites-based materials, which would surely shed light on the design and modification of advanced perovskites-based electrocatalysts for efficient and sustainable CO2 conversion.

2. Fundamentals of CO2RR and Perovskite Oxides

2.1. Fundamentals of CO2RR

A CO2 reduction reaction (CO2RR) occurs at the interface of the tri-phase (CO2 gas, liquid electrolyte, and solid catalyst surface), involving multiple electron and proton transfer processes. Generally, three steps are required for CO2RR, as shown in Figure 2 [8,12,13]: (1) the CO2 molecules are adsorbed on the active sites on the catalyst surface; (2) the adsorbed CO2 molecules transform to a CO2•− intermediate, and this initial electron transfer step is usually deemed the rate-determining step (RDS) of CO2RR; and (3) the generated products are desorbed and depart from the catalyst surface, making the active sites ready for the subsequent catalytic cycle. Nonetheless, the detailed reaction mechanisms are far more complicated than the abovementioned three basic steps, and the reaction pathways are distinct for different catalyst materials, even for the same product [14].
Laboratory-scale CO2RR is usually conducted in a three-electrode system, which is also the most widely used configuration in studies that investigate the catalytic performance of perovskite-based electrocatalysts. The system consists of a cathode (working electrode, where CO2RR occurs), an anode (usually platinum or nickel materials), and a reference electrode (Hg/HgO in an alkaline electrolyte, Ag/AgCl in a neutral or acidic electrolyte). Under the negative working potentials, CO2RR and the oxygen evolution reaction (OER) occur over the cathode and anode, respectively. Studies of CO2RR generally focus on the cathode, including both the catalytic materials and electrode structure. Herein, we only focus on the development of electrocatalysts for CO2RR. Generally, compared with metal catalysts, metal oxides have flexible and tunable structures, as well as interesting p–d coupling effects, which provide more abundant opportunities for tuning the electronic configuration of transition metal-based active sites and hence lead to promising catalytic properties. Among all the CO2RR catalysts that have been explored to date, perovskite-based materials exhibit some interesting characteristics and great potential in various electrochemical reactions [15,16,17,18,19,20].

2.2. Fundamentals of Perovskite Oxides

Perovskite is a family of compounds that have a general chemical formula of ABX3, the A-site elements could be rare-earth, alkaline-earth, or alkaline metals (e.g., Sr, La, Pr, Nd, Li, Na, Mg, Ca, etc.), while the B-site elements are transition metals (e.g., Ti, V, Mn, Fe, Co, Ni, Cu, etc.) that usually work as the active components during various catalytic reactions due to the existence of abundant d electrons and unfilled d orbitals. The anion X is usually oxygen for most of the perovskite-based CO2RR catalysts that will be discussed in this review article. Arising from the distinct atomic features of different A and B elements, the crystal structure of perovskites could be tuned by modulating the chemical compositions, which range from cubic to orthorhombic, tetragonal, or trigonal. In 1926, Goldschmidt proposed a relationship between the bond length of both A-X and B-X bonds to predict if a combination of a pair of cations could form the perovskite structure [21]. Then, this theory was optimized to use ionic radii as a substitute for bond length in order to expand the application range. The equation of modified Goldschmidt’s rule is displayed as follows:
t = r A + r X 2 r B + r X
where t is called the tolerance factor, rA is the radius of the A-site cation, rB is the radius of the B-site cation, and rX is the radius of the anion. The compound could be in an ideal perovskite structure when the tolerance factor is equal to precisely 1. Generally, the perovskite structure is stable when the tolerance factor is in the range of 0.75 to 1.00 [22]. If t lies in the approximately range of 0.9 to 1.0, the perovskite tends to exist in the ideal cubic structure. When t is lower than 0.9 but higher than 0.71, the octahedral structure will distort to break the cuboctahedral coordination and form a structure with a lower symmetry than the cubic one.
In addition to the simple ABX3 type, the family of perovskite materials also contains many other derivatives that show different atomic ratios, such as the Ruddlesden–Popper perovskite (RP-type) [22], Dion-Jacobson perovskite [23], Aurivillius perovskite [24], etc. All these perovskite derivatives can be realized by adjusting the thickness of perovskite units or inter-layer species. Regular and repeated phases can be synthesized when the structures are ordered, while disordered modules are non-stoichiometric. Such perovskites can be regarded as “layered materials”, which leads to their special physical structures and chemical characterizations. What is more, the special crystal structure of perovskites allows some elements to exist in unusual or mixed valence states with non-stoichiometric ratios of oxygen, leading to tunable and unique chemical properties that would further benefit the catalytic reactions. Actually, the positive roles of oxygen vacancies in perovskites for catalysis have been extensively investigated. It has been found that the moderate concentration of oxygen vacancies on the catalyst surface could effectively suppress the competitive hydrogen evolution reaction (HER) and also facilitate charge transfer during the CO2RR process [25].
The electrical conductivity of perovskites is another significant property when applied as an electrocatalyst. The RP-type perovskite materials were found to have high electrical conductivity due to the BO6 octahedra structure [26], which benefits the charge transfer process during electrochemical reactions [27]. Compared with the simple ABO3 perovskite, the RP-type perovskite (A2BO4) shows better electrical conductivity; moreover, the capability can be improved with the increasing n number because of the higher three-dimensional layered structure. In addition, the RP-type perovskite materials are stable enough under different pH conditions and oxidative potentials [28], making them promising electrocatalysts for many energy conversion reactions. In summary, the unique physicochemical properties of perovskite materials endow them with a broad application in various fields, such as energy conversion, storage, and electrochemical sensors [29,30].

2.3. Fabrication Methods of Perovskite Materials

In addition to chemical composition and crystal structure, particle size and microstructure also affect the performance of catalysts. Consequently, many approaches have been developed to synthesize perovskites with controlled particle size and morphology, such as wet chemistry methods, deposition-based approaches, templated-assisted synthesis, electrospinning, infiltration, exsolution, etc. In wet chemical synthesis, sol-gel processes are widely used to prepare nanosized perovskites [31,32]. In this method, citric acid [33] and ethylenediamine tetra-acetic acid [34] are often applied as the complexing agents to coordinate with the metal ions. A subsequent high-temperature calcination process should be carried out to remove the organics and facilitate the growth of perovskite crystals. Although the sol-gel method can produce purer-phase perovskites with higher surface areas when compared with the conventional solid-state method, the high-temperature calcination would inevitably lead to large agglomerated particles with a size of tens to hundreds of nanometers [35]. Template-assisted approaches have also been developed to synthesize perovskites with a porous microstructure [36]. Generally, a porous soft or hard template will be introduced in the preparation procedures, and then removed via calcination or chemical etching. The soft templates usually are self-assembled amphiphilic molecules [37,38] such as surfactants, and the hard ones can be silica-based molecular sieves [39,40] and organic polymethyl methacrylate (PMMA) [41,42]. The choice of templates should be based on the requirements for the pore size of the targeted structure of perovskites. Until now, perovskites with micropores, mesopores, three-dimensional ordered macropores, and hierarchical pores have been successfully prepared [43,44]. The porous microstructure could not only increase the surface area and hence provide more active sites but also provide convenient mass transfer channels, contributing to the greatly improved catalytic performance of perovskite-based materials for CO2RR.

3. Perovskite and Perovskite-Derived Catalysts for CO2RR

In this section, we summarize various perovskites or perovskite-derived materials, which were applied in the electrochemical CO2RR. CO2 can be converted into different valuable chemicals in both gas and liquid states. Generally, the products with one carbon (C1) include carbon monoxide, methane, methanol, and formate/formic acid, while ethylene, ethane, acetic acid, propanol, and other chemicals, with at least two carbon atoms, are classified into C2+ products. Due to the completely distinct reaction processes, e.g., the formation of C2+ requires C-C coupling, the design principles of catalysts for C1 and C2+ production via CO2RR are greatly different. Therefore, we classified the developed perovskite-based catalysts according to their main products in this section.

3.1. Perovskite-Based Catalysts for CO2RR Favoring C1 Products

As one of the most common products of CO2RR, CO is a widely used industrial resource for the synthesis of methanol and ammonia [45], as well as the feedstock of syngas with different H2-to-CO ratios. The relative studies have focused on enhancing faradaic efficiency (FE), which almost reached 100% with negligible H2 production [46,47,48]. Based on previous studies, it is well-known that a series of noble metals, including Au, Ag and Pd, have been proven to show remarkable CO2RR activity toward CO, with high FE and low overpotential [49,50,51]. For instance, the ultra-thin silver nanowires synthesized by Luo et al. [52] could realize the maximum FE (CO) of 99.3% with a quite small onset overpotential of 350 mV. In addition, some other active metals such as Zn [53,54], Co [55], and Ni [48] also attracted attention from researchers because the high cost of noble metals considerably restricts their industrial applications on a larger scale. Therefore, the specific element combinations in perovskites also help us to explore some efficient but inexpensive catalysts for CO2RR. In the study of Federico A’s team [56], a perovskite material with A-site substitution (La0.5Ba0.5CoO3) was prepared via the microwave irradiation method by using polycarbonate as the template. In this work, perovskites in a cubic structure, along with some other phases, were synthesized. The electrochemical and CO2RR tests were conducted in the H-cell and rotating ring-disc electrode (RRDE), respectively. All the products of CO2RR were C1 (CO and formate), and formate disappeared with the increase in reaction potential at −1.1 V vs. SHE. The density functional theory (DFT) calculations revealed that the CO2 molecules were adsorbed on the (001) and (110) planes of La0.5Ba0.5CoO3, where the surface oxygen sites were in a bend configuration. The generation of formate can be realized on both facets under the potential of −0.7 V and −0.8 V vs. SHE, while CO can only be generated on the (001) facet under more negative potentials.
Formate (in an alkaline environment)/formic acid (in a neutral or acidic environment) is another important C1 product of CO2RR and is an essential raw material in medical and chemical industries [57,58]. According to previous research, p-block elements including In, Sn, Pb, and Bi [59,60,61,62,63,64] and some copper-based catalysts [65] are highly reactive in converting CO2RR into formate/formic acid. The low cost and environmental friendliness of these active elements attract particular attention and a wide range of investigations. It is also noticeable that formate is produced in most studies instead of formic acid because most CO2RRs are carried out in alkaline electrolytes.
As a post-transition metal, tin (Sn) often acts as a B-site element in perovskite. In 2019, Huang et al. synthesized a one-dimensional SrSnO3 nanowires (NWs) via a facile hydrolysis method [66], which exhibited a much-enhanced selectivity toward formate production (FE~80%) with a long-term durability of 10 h, when compared with the traditional bulk perovskites and SnO2 nanoparticles. Based on a series of electrochemical characterizations, it was found that the stabilization of the intermediate CO2•− promoted the kinetics for formate production, while the kinetics for HER can be inhibited over SrSnO3 NWs at the same time. However, the relationship between the NWs morphology and catalytic activity that is critically important remains unclear. The bulk SrSnO3 perovskite was also utilized as electrocatalysts for CO2RR in Zhang’s research [67]. The Cu2+ ions with different ratios were doped on the SrSnO3 (0.5 wt%-SS and 1 wt%-SS) to synthesize the final CO2RR catalysts as depicted in Figure 3d. Different from the studies over SS NWs that formate was the major product [66], the CO selectivity showed an obvious boost when the Cu2+ doping ratio reached to 1 wt%, with the highest FE (CO) of 49%. The product distribution indicated that the copper on the catalyst surface played the role of active species to generate CO, while the bulk SS could be active to generate formate, due to the different surface structure that changed the reaction pathway.
In the RP-type perovskite (A2BO4), the insertion of AO-interlayers into ABO3 can stabilize the crystal structure under negative potentials, avoiding the catalyst deactivation due to the surface amorphization and structural reconstruction [68,69,70]. Gong’s group prepared an RP-type Sr2SnO4 perovskite through a solid-state approach and managed to solve the instability problem of SrSnO3 during CO2RR [71]. Though the active elements in perovskites were found to be reduced into a metallic state under the negative working potential of CO2RR, they found that Sr2SnO4 could stably work at –1.08 V vs. RHE for more than 24 h, due to the much-improved structural durability of RP perovskite (Figure 3b) when compared with the normal SrSnO3 (Figure 3a). The insertion of the SrO layer led to the strong interaction between perovskite layers and inhibited the structural reconstruction during CO2RR.
It is also reported that tuning A-site cations in perovskite influences the coordination environment of B-site elements, modifying the physicochemical properties of the catalysts. Therefore, another Sn-based Ba1–xSrxSnO3 perovskite with different A-site element ratios was synthesized via a high-energy ball-milling process [72]. With the change of Ba:Sr ratios, the average cation radius decreased from 1.61 to 1.44 Å, leading to the shortening of the Sn-O bonds from 2.06 to 2.02 Å (Figure 3c). The precise regulation of Sn-O bonds strengthened the bond covalency and shifted the total band center closer to the Fermi level. The much-enhanced catalytic performance suggests that A-site modulation is indeed an efficient approach to idealizing the electronic structure, electron transfer property, adsorption of reaction intermediates, and other important features of perovskite-based catalysts.
Molecules 28 08154 g003
Figure 3. Crystal structures of (a) SrSnO3 and (b) Sr2SnO4, reprinted with permission from ref [66]. Copyright Royal Society of Chemistry, 2022; (c) structure–performance relationship of Ba1−xSrxSnO3, reprinted with permission from ref. [72]. Copyright Wiley VCH GmbH, 2023; (d) doping effect of Cu2+ on SrSnO3 perovskite oxides, reprinted with permission from ref. [67]. Copyright Wiley VCH GmbH, 2022.
Figure 3. Crystal structures of (a) SrSnO3 and (b) Sr2SnO4, reprinted with permission from ref [66]. Copyright Royal Society of Chemistry, 2022; (c) structure–performance relationship of Ba1−xSrxSnO3, reprinted with permission from ref. [72]. Copyright Wiley VCH GmbH, 2023; (d) doping effect of Cu2+ on SrSnO3 perovskite oxides, reprinted with permission from ref. [67]. Copyright Wiley VCH GmbH, 2022.
Molecules 28 08154 g003
The exsolution of B-site elements in perovskite oxides under a reductive environment (negative potential or reductive atmosphere) is an inevitable phenomenon, and such a structural evolution is pivotal for the identification of active sites and reaction mechanisms. Bedford et al. [73] applied a novel biomineralization approach for the synthesis of perovskite-type tin-zinc oxides (TZO), which exhibited a porous microstructure with abundant defects and amorphous phases, rather than normal perovskite oxides with specific crystal structures. The as-prepared SnxZnyOz exhibited good catalytic activity toward CO2RR with the major products of formate and CO. What is more, as exhibited in Figure 4a,b, the product selectivity was found to vary with Sn:Zn ratios due to the distinct capability of Sn and Zn in the formation of CO. The coordination numbers during CO2RR demonstrated that the electronic configurations and local structures of metal components depended on the applied cathodic potentials over different SnxZnyOz catalysts (Figure 4c–f), generating highly active sites of oxygen vacancies that determined the CO2RR performance. The DFT modeling results also proved that oxygen vacancy can facilitate the interaction between intermediates and undercoordinated Sn and Zn sites to tune the selectivity toward formate.
In addition to Sn, bismuth (Bi) is another active species for converting CO2 into C1 products. Previous research proved that Bi species are more favorable to generating formate in aqueous solutions [74]. The advantages of Bi include environmental friendliness, low cost, high biocompatibility, and being inert to hydrogen evolution [75]. In the study of Luo’s team [76], the electricity-driven reconstructions of a BaBiO3 (BBO) perovskite were emphasized. The experimental results showed that an irreversible structural and phase transformation can be observed during CO2RR, as displayed in Figure 5e. The B-site Bi in pristine BBO exsolved from the perovskite crystals under cathodic potentials. Then, the re-nucleation and growth of dissolved Bi particles led to the complete transformation of BBO from the monoclinic phase to Bi nanosheets with atomic-scale thickness, acting as the real active species during CO2RR. Notably, the authors compared the structural reconstruction of the BBO catalyst with another typical RP-type perovskite (La2CuO4) that was also active in the CO2RR [77]. La2O3, the reduction product of La2CuO4, is insoluble in aqueous electrolytes; however, due to the solubility of BaO, the cleavage of Ba-O and Bi-O bonds resulted in almost complete A-site element loss. The ionic form, Ba2+, can also enhance the adsorption of carbonate intermediates, thereby promoting formate production. This study revealed the real structure and active species of perovskites during CO2RR again, and the electrochemical reduction process can be regarded as a catalyst synthesis method using perovskite material as the precursor.
Consequently, a perovskite precursor with halide and alkali metal compositions was prepared by a hot-injection method and showed a hexagonal Cs3Bi2I9 nanocrystal [75]. The pre-catalyst was successfully converted into Bi crystals with halide and alkali metal dual modification (Figure 5f). The trace amounts of I– and Cs+ ions were found to be located on the Bi surface and outer Helmholtz layer, respectively, which affected the catalytic processes. There are also many works on the combination of halide perovskites with carbon materials to improve their stability. For example, Cs3Bi2Br9 was mixed with carbon black (Figure 5a,b) to form a composite efficient for CO2RR in an acidic electrolyte (HBr) [78]. The in-situ tests and characterizations of electrodes after CO2RR proved that the Cs3Bi2Br9/C composites exhibited remarkable structural durability due to the quick electron transport and fast CO2 reduction rate, which leads to a smaller degradation effect. This method also works well for stabilizing perovskite materials with lead (Pb) and indium (In) in their B-sites. For example, Wang et al. reported a metal halide perovskite (CsPbI3) that combined with reduced graphene oxide (rGO), which effectively tackled the poor phase stability of inorganic halide perovskite [79]. Generally, with the addition of rGO, the perovskite nanocrystals would be wrapped and stabilized by rGO (Figure 5c,d), avoiding the formation of inactive Pb defects or Pb nanoparticles usually observed after the CO2RR in pristine CsPbI3. What is more, the electron density near the perovskite/rGO interface was also regulated, contributing to the enhanced durability and selectivity of formate formation.
Additionally, it is noteworthy that halide perovskites demonstrate a broader range of applications in the field of CO2 conversion compared to perovskite oxides, particularly in terms of CO2RR via photoelectrochemical (PEC) processes. PEC reduction technology can transform CO2 directly into a variety of chemicals within integrated photo absorber-electrocatalyst systems, driven by both solar and electrical energy [80,81], thereby mitigating excessive reliance on external power sources. Among the semiconductor materials for PEC CO2 reduction, lead-based halide perovskites have garnered significant attention because of their appealing photoelectronic properties, including a defect-tolerant band structure, high photoluminescence efficiency, a wide absorption range, and a tunable band gap expanding the whole visible range [82,83,84]. Due to toxicity and long-term instability, lead-based halide perovskites are usually combined with other materials during PEC CO2 reduction. Huang et al. [85] modified the CsPbBr3 (CPB) perovskite with fluorine doping, Nafion solution, and Au coating. Such an interface-engineering approach can greatly facilitate light adsorption and charge transfer when compared with the pristine photocathode. In another study by Luo et al. [86], PbS nanoparticles were uniformly anchored on CPB nanocrystals with the assistance of an amino acid as a capping ligand. The introduction of PbS significantly boosted the charge transfer, leading to enhanced CO and CH4 production rates of 2.94 and 0.36 μmol cm−2 h−1, respectively. Besides this, a lead-free halide perovskite of CsAgBr2 was also successfully synthesized and exhibited superior CO2 reduction performance, with around 14 μmol g−1 h−1 of CO yield and 50% FE [87]. These studies underscored the practicability of directly using inorganic halide perovskites in PEC CO2 reduction.
Though there are still many uncertainties regarding the structure–performance relationship of perovskite derivatives for CO2 reduction, especially the underlying reasons for the stability, it could be concluded that perovskites could be good precursors for preparing the metallic catalysts that are active for CO2RR. The rational coupling of perovskites with other materials such as carbon and organic capping ligands could efficiently enhance their stability during the reaction process.
The CO2RR with methane as the main product is most likely to be realized on copper-based materials, and copper is one of most utilized B-site elements for forming the perovskite structure. In the study of Xia’ et al. [77], the RP-type La2CuO4 perovskite was applied in CO2RR to produce methane. The structural evolution during CO2RR was emphasized to play the key role in the methanation process. The surface layers of La2CuO4 were partially reduced under negative potentials to form metallic Cu0 and La2O3, generating the heterostructure of Cu/La2CuO4. Such a hetero-interface can optimize the surface adsorption of CO2 and charge transfer, leading to considerable methanation activity, with an FE (methane) of 56.3% at −1.4 V vs. RHE. A-site elements in perovskites are usually supposed to be inactive during catalytic reactions, and the candidates include lanthanide elements (La, Ce, Pr, etc.) and rare earth metals (Mg, Ca, Ba, etc.). A recent report [88] chose the alkaline-earth element of Ca as an A-site element to synthesize the perovskite oxides (Ca2CuO3). The calcium at the A-site caused Ca2CuO3 to feature a strong basic strength and a remarkable capability for CO2 chemisorption, compared with the non-basic Sr2CuO3 and La2CuO4. The leaching problem of Ca2+ ions also occurred over Ca2CuO3 perovskite. However, the leaching can help to form uncoordinated copper sites, which were beneficial for the hydrogenation of *CO and *CHO intermediates to generate *CH2O, leading to great methanation activity with extremely high current densities and relatively low overpotentials.
In addition to Cu-based materials, some other perovskite catalysts also exhibited good capability of producing methane. It was reported for the first time that lead halide perovskite (CsPbBr3) nanocrystals showed high activity in CO2RR for producing methane and CO [89]. The water-dispersible CsPbBr3 exhibited an ultrahigh catalytic stability of 350 h in H-cells, where the FE (CO) and FE (methane) were 40% and 32%, respectively. A diverse range of perovskite materials (LaCoO3, LaCrO3 LaMnO3, LaFeO3, etc.) were also prepared and examined for electrochemical methanation [90], and the LaCoO3 perovskite exhibited the highest methanation activity among all the samples. The O 2p-band center was proposed as an activity descriptor that can rationalize activity and selectivity for CO2RR, which influences the COads binding energy of the catalyst to enhance CH4 selectivity. The studies about electrochemical methanation using perovskite materials as catalysts are much fewer than the papers focused on producing CO and formate, and the catalytic performance is far below satisfactory. Consequently, there are still plenty of strategies and there is much development room for perovskite-based catalysts to improve methane selectivity by rationally designing both the chemical composition and microstructure of the perovskite-based catalytic materials.

3.2. Perovskite-Based Catalysts for C2+ Production

Common C2+ products of CO2RR include ethylene, ethanol, acetic acid, propanol, etc., which generally possess higher energy densities and economic value than C1 products [91]. Similar to methane production, copper-based perovskite materials are also widely used to facilitate *CO dimerization and hydrogenation, which are regarded as the key pathways for generating C2+ products [92].
In 1993, Schwartz [93] applied perovskites as electrocatalysts in CO2RR for the first time, and the main products were found to be various alcohols. The RP-type perovskite with different A and B elements was tested over gas diffusion electrodes. The results indicated all the non-copper-containing perovskite materials were inactive toward CO2RR, while the total FE for alcohols including methanol, ethanol, and n-propanol could reach around 40% over La1.8Sr0.2O4 at 180 mA/cm−2. Furthermore, the valence changes of copper ions in the perovskites were confirmed via X-ray diffraction (XRD) patterns before and after CO2RR tests, as shown in Figure 6a, demonstrating the structural evolution of perovskite crystals, and the active sites could be the mixture of Cu0 and Cun+. This ground-breaking work proved the potential activity of copper-based perovskite in CO2RR, and more importantly, it reminded subsequent researchers that the structural evolution during the reaction should be emphasized.
Decades after the first paper, the RP-type copper-based perovskite was investigated in CO2RR again by various research teams [94,95,96]. Mignard et al. [95] further investigated RP-type La2-xSrxCuO4 for CO2RR with modified testing conditions, including a much enlarged applied potential range, reaction temperatures from 2 to 40 °C, and CO2 pressures from 1 to 43 bar. The main products were unexpected to be the hydrocarbons of methane and ethylene, rather than alcohols, as in Schwartz’s work. The differences were further analyzed from several aspects such as electrolyte recirculation, impurities, and perovskite compositions. The different perovskite crystals could be the determinant. The synthesized La1.8Sr0.2O4 exhibited two crystal phases of (LaSr)CuO4 and (LaSr)CuO2.6 (Figure 6b), even though prepared with the same procedure. The ratios between these two perovskite phases could be vital to the product distribution of CO2RR; however, this was without the support of experimental data. Despite the distinctions in results, this study still displayed the essential influences of reaction conditions and devices on the CO2RR process. Further, the structural change of La2CuO4 under negative potentials was systematically investigated based on a series of in-situ and ex-situ experiments [94]. According to the electrochemical cyclic voltammetry curves, it was found that the RP-type La2CuO4 underwent a two-step electroreduction, which was attributed to Cu2+ to Cu2O and Cu2O to metallic Cu0, respectively. The in-situ formed Cu+ in the perovskite was considered as the active site for CO2RR to produce ethylene. In addition, the influence of A-site cation in La2CuO4 was also fully investigated [96]. Nonstoichiometric La2–xCuO4–δ (x = 0, 0.1, 0.2, and 0.3) with different La amounts was synthesized to introduce vacancies into the perovskite structure. As depicted in Figure 6c, when the La deficiency concentration was relatively low (x < 0.1), a certain quantity of oxygen vacancies could efficiently facilitate the C2+ formation and suppress the competing HER. Nonetheless, too much of an La deficiency (x > 0.1) would result in the phase separation of the perovskite and form CuO/perovskite hybrids, and the CuO was favorable for methane and H2 production. In short, by simply controlling the cation defects, researchers could realize the tunable catalytic selectivity of defected La2–xCuO4–δ hybrids toward CO2RR to generate C2+ products.
Molecules 28 08154 g006
Figure 6. (a) XRD patterns of La1.8Sr0.2O4 before and after CO2RR, reprinted with permission from ref. [93]. Copyright The Electrochemical Society Inc, 1993; (b) La2-xSrxCuO4 synthesized by Mignard et al., reprinted with permission from ref. [95]. Copyright Elsevier Ltd., 2014; (c) illustration of crystal structure properties of L2C, L1.9C, L1.8C, and L1.7C, reprinted with permission from ref. [96]. Copyright Wiley VCH GmbH, 2021.
Figure 6. (a) XRD patterns of La1.8Sr0.2O4 before and after CO2RR, reprinted with permission from ref. [93]. Copyright The Electrochemical Society Inc, 1993; (b) La2-xSrxCuO4 synthesized by Mignard et al., reprinted with permission from ref. [95]. Copyright Elsevier Ltd., 2014; (c) illustration of crystal structure properties of L2C, L1.9C, L1.8C, and L1.7C, reprinted with permission from ref. [96]. Copyright Wiley VCH GmbH, 2021.
Molecules 28 08154 g006
Grain boundaries and interface engineering are emerging techniques to optimize the adsorption of reaction intermediates on the catalysts, thereby enhancing the selectivity for particular products [97,98]. Such strategies also work well over perovskites to facilitate C2+ hydrocarbon production via CO2RR. The electrospinning approach (Figure 7a) was applied to synthesize La2CuO4 catalysts with different microscopic morphologies [69]. With the increase in heating rate during calcination, the perovskite morphology changed from nano bamboos (NBs) to nanorods (NRs), and finally to bulk perovskite. The optimized perovskite NBs exhibited symmetric twin boundaries of the (113) facet, as depicted in Figure 7b, which induced a strain effect that facilitated charge transfer and C-C coupling, leading to the high FE (ethylene) of 60% at −1.0 V vs. RHE. However, a high FE (CO) of 91% was observed over the bulk perovskite without regular grain boundaries. What is more, the introduction of twin boundaries seemed to be helpful for stabilizing the perovskite structure based on the characterization results of spent catalysts. The grain boundaries can also be generated by an in-situ electroreduction treatment [99]. The La2CuO4-derived copper catalyst presented multiple GBs composed of different nanocrystallites, including Cu (111) and Cu2O (111). With the assistance of CO2, the La oxides can form soluble La(CO3)3 and further lead to the complete phase evolution from a single-crystal perovskite to diverse grains of copper species, such as metallic Cu0 and copper oxides. The high-density grain boundaries generated more defective sites, which were beneficial for the strong binding of COads, therefore promoting C-C coupling to realize a high C2+ selectivity of 80.3%.
Similar to electroreduction, thermal reduction is another strategy to construct active copper species derived from perovskites (Figure 7c). The strong metal-support interactions (SMSIs) were introduced by in-situ generated copper nanoparticles that uniformly dispersed over La0.4Sr0.4Ti0.9O3−δ (LST) support, forming the LSTr-Cu catalyst with sub-3 nm copper nanoparticles on the surface [100]. Figure 7d illustrates that the SMSIs effect not only modulated the electronic properties but facilitated the adsorption of key reaction intermediates. More importantly, strong adhesion between the surface Cu atoms and LST backbones inhibited the migration of active copper clusters, enhancing the resistance to active site degradation. Although the stability test was conducted in H-cells with a low current density of 15 mA/cm2, the positive influence of SMSIs could definitely be demonstrated according to the stable FE (CO2RR). Moreover, the perovskite was found to be reactive in producing other C2+ products such as oxalate. The production of oxalate via CO2RR usually suffers from high energy barriers and slow kinetics [74]. Surprisingly, a recently published paper found that the lead-based perovskite material (PbSnO3/C) exhibited excellent activity with a low overpotential and high FE (oxalate) of 85.1% [101]. Though the underlying reasons are still obscure, this provides promising opportunities for modifying the physicochemical properties of perovskite materials to realize controlled CO2RR and target products such as oxalate.

4. Summary and Outlook

Perovskite materials with the general formula of ABX3 have abundant catalytically active transition-metal ions in B-sites, which have found extensive applications in diverse electrochemical reactions and energy conversion devices over an extended period. However, the utilization of perovskite-based catalysts for efficient CO2RR remains at the initial stage, and it needs a timely and comprehensive review to delve into the underlying problems and challenges according to the reported studies and hence promote the further development of this research area. In this review, we encapsulate the recent progress of perovskites and their derivatives as electrocatalysts for CO2RR, starting with the introduction of fundamentals of CO2RR and perovskite materials. Then, the pivotal and representative studies of perovskites as CO2RR catalysts are comprehensively discussed according to the major products of CO2RR (Table 2).
By analyzing and discussing these representative works, we found that the catalytic activity, selectivity and stability of perovskites and their derivatives for CO2RR are strongly related to their chemical composition, crystal structure, micro-morphology, etc. In general, the active B-site metals determine the product selectivity. For instance, Sn-, Pb-, Bi-, and In-based perovskites mainly generate C1 products such as formate and CO, while Cu-based perovskites could be good candidates for the formation of methane or C2+ products. As for the influence of crystal structure, an RP-type perovskite was found to possess better structural stability because the insertion of AO-interlayers could stabilize the ABO3 structure under negative working potentials of CO2RR. In addition, the crystal structure could also be tuned via A-site substitution. The mismatch between the ion radius of different A-site elements would result in the formation of lattice distortion and vacancies and even generate a second phase that contributes to the change of product selectivity.
What is more, most of the perovskite materials usually underwent structural evolution during CO2RR processes. Some preparation methods such as electrospinning were developed to fabricate perovskites with special micro-morphologies such as nanowires, nanorods, and nano bamboos, which demonstrated much enhanced structural stability. Further, the structural evolution phenomenon was utilized to synthesize high-active metallic catalysts by using a perovskite as a precursor. Both of these directions can realize the controlled preparation of perovskite-based materials with suitable microstructures. In addition, the real active sites could also evolve during the structural reconstruction. Therefore, the precise determination of active sites and their evolution pathways should be exploited in order to reveal the structure–performance relationship of the perovskite-based electrocatalysts toward CO2RR.
Last but not least, the advancements and possible research directions to address the existing limitations are summarized and proposed below:
  • The pivotal factor in assessing a catalyst material lies in its catalytic activity. As for the production of C1 products, the recently developed noble metal-based or even transition metal-based catalysts can reach an FE (CO) close to 100% [102,103,104,105], and other lead- and tin-based catalysts can also reach an FE (formate) higher than 90% [106,107]. However, the selectivity of perovskite-based catalysts toward CO2RR is far below these levels, particularly in C2+ production. Thus, there is large space for further improving the activity and selectivity of perovskite-based catalysts for producing high-value C2+ products, which would be realized by precisely modulating the physicochemical characteristics of active sites.
  • The active transition-metal ions in perovskites would be reduced under the negative potential condition during CO2RR. Though a few papers improved the stability of their perovskite-based materials during CO2RR, the reduction processes could be challenging to observe under the small current densities applied in their studies. Consequently, there is a pressing need for further investigations on the possible structure evolution of perovskites under high current densities.
  • Moreover, in-situ technologies are essential to provide real-time information on the evolution of active sites during the CO2RR process. For instance, in-situ XRD and X-ray photoelectron spectroscopy (XPS) could provide direct experimental results to observe the change in crystal structure and metal valences; in-situ Raman and Fourier transform infrared (FTIR) are also crucial for revealing the catalytic mechanism [108,109]. Additionally, theoretical simulation of the reaction mechanisms of CO2RR over perovskites also needs to take the structural change into consideration, because the selection of active facets during CO2RR profoundly impacts the accuracy of the calculations.
  • Until now, most studies have focused on applying perovskite oxides for CO2RR, while metal oxides have to face a series of issues such as instability under negative potentials and acidic electrolytes. Therefore, inorganic perovskites incorporate other anions such as halide elements (F−, Br−, I−, etc.) [110,111], which have been reported to possess the capability of regulating the electronic properties of copper and enhancing its selectivity toward C2+ products, so they deserve further exploration.

Author Contributions

Conceptualization, T.W. and X.L.; investigation, X.L.; writing, T.W.; review and editing, T.W., L.Z., Y.Z., Y.D., Z.T., B.Z., F.W., D.Z. and X.L. All authors have read and agreed to the published version of the manuscript.

Funding

The authors appreciate the financial support from Shanghai Jiao Tong University (No. WH220828001 and No. ZXDF280001).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

No new data were created.

Conflicts of Interest

The authors declare no conflict of interest.

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Molecules 28 08154 g001
Figure 1. Schematic representation of the main content of this review.
Figure 1. Schematic representation of the main content of this review.
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Molecules 28 08154 g002
Figure 2. Three main steps on the catalyst surface of CO2RR processes. Black spheres represent carbon atoms; red spheres represent oxygen atoms; white spheres represent hydrogen atoms; orange atoms represent the CO2RR catalyst.
Figure 2. Three main steps on the catalyst surface of CO2RR processes. Black spheres represent carbon atoms; red spheres represent oxygen atoms; white spheres represent hydrogen atoms; orange atoms represent the CO2RR catalyst.
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Figure 4. (a) FE (CO) and (b) FE (formate) over SnxZnyOz catalysts; Different coordination numbers (CN) calculated based on in-situ extended X-ray absorption fine structure (EXAFS) results for (c,d) Sn0.5Zn0.5Oy, (e) ZnOy, and (f) SnOy, measured under electrochemical CO2RR at potentials of open circuit voltage, 0.8, 0.9, 1.0, and 1.1 V. vs. RHE, reprinted with permission from ref. [73]. Copyright Elsevier Ltd., 2022.
Figure 4. (a) FE (CO) and (b) FE (formate) over SnxZnyOz catalysts; Different coordination numbers (CN) calculated based on in-situ extended X-ray absorption fine structure (EXAFS) results for (c,d) Sn0.5Zn0.5Oy, (e) ZnOy, and (f) SnOy, measured under electrochemical CO2RR at potentials of open circuit voltage, 0.8, 0.9, 1.0, and 1.1 V. vs. RHE, reprinted with permission from ref. [73]. Copyright Elsevier Ltd., 2022.
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Figure 5. The transmission electron microscope (TEM) images of (a) Cs3Bi2Br9 NCs and (b) Cs3Bi2Br9/Carbon black composite, reprinted with permission from ref. [78]. Copyright Wiley VCH GmbH, 2022; TEM images of (c) CsPbI3 NCs and (d) CsPbI3/rGO composite, reprinted with permission from ref [79]. Copyright Springer Ltd., 2023, red arrows and yellow arrows in (b,d) point to perovskite nanocubes and carbon materials, respectively; (e) the structural evolution of BaBiO3 perovskite during CO2RR, reprinted with permission from ref. [76]. Copyright Elsevier Ltd., 2022; (f) the conversion of Cs3Bi2I9 nanocrystals to bismuth with I− and Cs+ dual modification, reprinted with permission from ref [75]. Copyright Wiley VCH GmbH, 2023.
Figure 5. The transmission electron microscope (TEM) images of (a) Cs3Bi2Br9 NCs and (b) Cs3Bi2Br9/Carbon black composite, reprinted with permission from ref. [78]. Copyright Wiley VCH GmbH, 2022; TEM images of (c) CsPbI3 NCs and (d) CsPbI3/rGO composite, reprinted with permission from ref [79]. Copyright Springer Ltd., 2023, red arrows and yellow arrows in (b,d) point to perovskite nanocubes and carbon materials, respectively; (e) the structural evolution of BaBiO3 perovskite during CO2RR, reprinted with permission from ref. [76]. Copyright Elsevier Ltd., 2022; (f) the conversion of Cs3Bi2I9 nanocrystals to bismuth with I− and Cs+ dual modification, reprinted with permission from ref [75]. Copyright Wiley VCH GmbH, 2023.
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Figure 7. (a) Illustration of electrospinning approach to prepare La2CuO4 NBs, reprinted with permission from ref. [69]. Copyright ACS Publications, 2021; (b) the high-resolution transmission electron microscope (HRTEM) images of grain boundaries in La2CuO4 with different micro-morphologies, reprinted with permission from ref. [69]. Copyright ACS Publications, 2021; (c) schematic illustrations of microstructure evolutions during the LSTr-Cu formation, reprinted with permission from ref. [100]. Copyright Wiley VCH GmbH, 2022; (d) the SMSIs for the LSTr-Cu catalyst, reprinted with permission from ref. [100]. Copyright Wiley VCH GmbH, 2022.
Figure 7. (a) Illustration of electrospinning approach to prepare La2CuO4 NBs, reprinted with permission from ref. [69]. Copyright ACS Publications, 2021; (b) the high-resolution transmission electron microscope (HRTEM) images of grain boundaries in La2CuO4 with different micro-morphologies, reprinted with permission from ref. [69]. Copyright ACS Publications, 2021; (c) schematic illustrations of microstructure evolutions during the LSTr-Cu formation, reprinted with permission from ref. [100]. Copyright Wiley VCH GmbH, 2022; (d) the SMSIs for the LSTr-Cu catalyst, reprinted with permission from ref. [100]. Copyright Wiley VCH GmbH, 2022.
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Table 1. Electrochemical reactions in CO2RR under equilibrium potentials [11].
Table 1. Electrochemical reactions in CO2RR under equilibrium potentials [11].
Electrolyte ConditionsReactionsE0/(V vs. RHE)Products
/2H + + 2e− → H20hydrogen evolution reaction (HER)
/xCO2 + nH + + ne− → product + yH2O/CO2RR
Alkaline
(pH: 8~14)		CO2 + 2H + + 2e− → H + + HCOO–−0.12formate
CO2 + 2H + + 2e− → CO (g) + H2O−0.10carbon monoxide
CO2 + 6H + + 6e → CH3OH (aq) + H2O0.03methanol
CO2 + 4H + + 4e− → C (s) + 2H2O0.21carbon
CO2 + 8H + + 8e− → CH4 (g) + 2H2O0.17methane
2CO2 + 8H + + 8e− → H + + CH3COO– + 2H2O0.11acetate
2CO2 + 10H + + 10e− → CH3CHO (aq) + 3H2O0.06acetaldehyde
2CO2 + 12H + + 12e− → C2H5OH (aq) + 3H2O0.09ethanol
2CO2 + 2H + + 12e− → C2H4 (g) + 4H2O0.08ethylene
2CO2 + 14H + + 14e− → C2H6 (g) + 4H2O0.14ethane
3CO2 + 18H + + 18e− → C3H7OH (aq) + 5H2O0.10propanol
Acidic
(pH: 0~7)		CO2 + 2H + + 2e− → HCOOH (aq)−0.12formic acid
2CO2 + 8H + + 8e− → CH3COOH (aq) + 2H2O0.11acetic acid
Table 2. Summary of the representative studies discussed in this review.
Table 2. Summary of the representative studies discussed in this review.
Perovskite CatalystMajor ProductsFE of Main ProductsReference
Cs3Bi2Br9/carbon blackformic acid92%[78]
SrSnO3 nanowiresformate~80%[66]
Sr2SnO4formate83.7%[71]
SnaZnbOyformate~70%[73]
BaBiO3formate98.7%[76]
Ba1−xSrxSnO3formate90.9%[96]
CsPbI3/rGOformate>92%[79]
Cs3Bi2I9formate98.2%[75]
La2CuO4methane56.3%[77]
Ca2CuO3methane51.7%[88]
La1.8Sr0.2CuO4methane and ethyleneNot mentioned[95]
Cu-SrSnO3CO and formate89% (formate) over 0.5 wt% Cu-SrSnO3; 49% (CO) over 1 wt% Cu-SrSnO3[64]
CsPbBr3methane and CO32% for methane, 40% for CO[89]
La0.5Ba0.5CoO3CO85%[56]
A1.8A0.2CuO4 (A = La, Pr, and Gd; A’ = Sr and Th)alcohols~40%[93]
La2CuO4ethylene40.3%[94]
La2CuO4 nanobamboosethylene60%[69]
reduced La0.4Sr0.4Ti0.9O3−δ-CuC2+ products54.9%[100]
La2–xCuO4-δC2+ products41.5%[96]
La2CuO4 derived-CuC2+ products80.3%[99]
PbSnO3/Coxalate85.1%[101]
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Wu, T.; Zhang, L.; Zhan, Y.; Dong, Y.; Tan, Z.; Zhou, B.; Wei, F.; Zhang, D.; Long, X. Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction. Molecules 2023, 28, 8154. https://doi.org/10.3390/molecules28248154

AMA Style

Wu T, Zhang L, Zhan Y, Dong Y, Tan Z, Zhou B, Wei F, Zhang D, Long X. Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction. Molecules. 2023; 28(24):8154. https://doi.org/10.3390/molecules28248154

Chicago/Turabian Style

Wu, Tong, Lihua Zhang, Yinbo Zhan, Yilin Dong, Zheng Tan, Bowei Zhou, Fei Wei, Dongliang Zhang, and Xia Long. 2023. "Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction" Molecules 28, no. 24: 8154. https://doi.org/10.3390/molecules28248154

APA Style

Wu, T., Zhang, L., Zhan, Y., Dong, Y., Tan, Z., Zhou, B., Wei, F., Zhang, D., & Long, X. (2023). Recent Progress on Perovskite-Based Electrocatalysts for Efficient CO2 Reduction. Molecules, 28(24), 8154. https://doi.org/10.3390/molecules28248154

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