Wenyu
Luo
a,
Jiawei
Liu
ab,
Yue
Hu
c and
Qingyu
Yan
*ad
aSchool of Materials Science and Engineering, Nanyang Technological University, 639798, Singapore. E-mail: alexyan@ntu.edu.sg
bInstitute of Sustainability for Chemicals, Energy and Environment (ISCE2), Agency for Science, Technology and Research (A*STAR), 1 Pesek Road, Jurong Island, Singapore 627833, Republic of Singapore
cSchool of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China
dInstitute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis #08-03, Singapore 138634, Republic of Singapore
First published on 22nd October 2024
Ammonia and urea represent two important chemicals that have contributed to the rapid development of humanity. However, their industrial production requires harsh conditions, consuming excessive energy and resulting in significant greenhouse gas emission. Therefore, there is growing interest in the electrocatalytic synthesis of ammonia and urea as it can be carried out under ambient conditions. Recently, atomic catalysts (ACs) have gained increased attention for their superior catalytic properties, being able to outperform their micro and nano counterparts. This review examines the advantages and disadvantages of ACs and summarises the advancement of ACs in the electrocatalytic synthesis of ammonia and urea. The focus is on two types of AC – single-atom catalysts (SACs) and diatom catalysts (DACs). SACs offer various advantages, including the 100% atom utilization that allows for low material mass loading, suppression of competitive reactions such as hydrogen evolution reaction (HER), and alternative reaction pathways allowing for efficient synthesis of ammonia and urea. DACs inherit these advantages, possessing further benefits of synergistic effects between the two catalytic centers at close proximity, particularly matching the NN bond for N2 reduction and boosting C–N coupling for urea synthesis. DACs also possess the ability to break the linear scaling relation of adsorption energy of reactants and intermediates, allowing for tuning of intermediate adsorption energies. Finally, possible future research directions using ACs are proposed.
The current industrial production of ammonia and urea is by the H–B process and Bazarov process, respectively. In the H–B process, the main source of hydrogen comes from fossil fuel feedstocks, resulting in the H–B process emitting 1.2% of global anthropogenic CO2 emission.12 The energy consumption of H–B is significant as well, a hefty 11% of the total energy consumed by the chemical industry. This massive energy consumption is due to the conditions in which ammonia is synthesized: a temperature of 723–823 K and pressure of 250–350 atm.13 80% of the produced ammonia is then fed to the Bazarov process to synthesize urea,14,15 a process requiring a temperature of 150 °C and 2 MPa to combine CO2 and ammonia supercritical fluid.16,17 Both H–B and Bazarov processes require high temperature and high pressure, consuming more than 2% of the world's energy each.15,18,19 Electrocatalytic synthesis of ammonia and urea is therefore much desired, as it can be done under ambient conditions using energy from renewable sources.20,21 The absence of heat and pressure in the electrocatalytic method results in a significantly lower energy requirement compared with the H–B process or Bazarov process. Much research has been done on the utilisation of catalysts on the microscale and nanoscale involving transition metals such as Zn,21 Co,22,23 Ti,24 Fe,19 Cu,25 In15,26 and Ru.27 Main group metals such as Al28 and even metal-free catalysts were also reported.29,30
Going further down the scale of size, the atomic catalyst (AC) is a relatively new topic that has gained increased attention from the catalytic community.31 Single atomic catalyst (SAC) is the atomic dispersion of a single catalytic material onto a support material such that the active centers are isolated.32,33 One of the most prominent advantages of SACs is the small amount of materials required to achieve the same results as their nano or micro counterparts due to the 100% atom efficiency of AC from the atomically dispersed catalyst, maximising the use of catalytic surface area.34 This atomic dispersion of catalytic material, however, brings in the question of catalyst stability as isolated atoms have high surface energy, resulting in a tendency to aggregate.35,36 There are methods to circumvent this, for example, by tuning the catalyst mass loading37 or by varying the type of support material.38 Further advantages of SACs include the suppression of competitive reactions such as hydrogen evolution reaction (HER) from (1) the ensemble effect, where the lack of adjacent active centers allows for only top site adsorption, while the preferred adsorption of *H is bridge or hollow site which is only possible with more than one active center present in nanomaterials, and (2) the electronic effect, where the metal atom–support interaction induces charge transfer from the metal atom to the support, resulting in the metal active center being positively charged, forming an electrostatic repulsion against H+.39 There is also the possibility of new reaction pathways not possible for nano and micro counterparts, such as the direct oxidation of methane to methanol or ethane when comparing Rh SACs with Rh nanoparticles and a two-electron pathway in the oxygen reduction reaction (ORR) when using Pt SACs compared with the four-electron pathway when using Pt nanoparticles.40
On the other hand, the distance between catalytic centers in SACs is too wide for any cooperative effects. For example, in dinitrogen N2, the NN bond has a bond length of 0.1–0.2 nm.41 The interatomic distance of catalytic centers must be reduced to match that of N2 to have cooperative effects. Diatomic catalysts (DACs) are able to effectively bridge this problem by having two catalyst atoms side by side.42 While inheriting the unique traits of SACs, DACs further exhibit advantages that SACs do not possess, as having two catalytic atoms side by side also results in synergistic effects for the catalytic process. One of the atoms can regulate the spin state and electronic configuration of the other atom, enhancing the catalytic activity.43 Strong interactions between the two atoms can also stabilise each other, preventing agglomerations.44 The Sabatier principle states that an ideal catalyst must have an intermediate binding energy that is neither too strong to the extent that it inhibits desorption of products nor too weak to the extent the reactants cannot be activated.45–47 A linear scaling relation between the adsorption energy of reactants and adsorption energy of intermediate is therefore detrimental to catalytic activities, as while a stronger adsorption energy of reactants will strongly activate the reactants, a corresponding stronger adsorption energy of intermediates will inhibit the desorption of products, potentially resulting in the formation of unwanted side-products. DACs are able to break this scaling relationship, allowing for fine tuning of adsorption energy for intermediates, further improving the catalytic activity.48,49
ACs have been utilised in many various reactions, such as carbon dioxide reduction (CO2RR), the nitrogen reduction reaction (NRR), nitrate reduction reaction (NO3RR) and water splitting reaction. Many reviews were published regarding ACs,50–55 exploring various synthesis methods, introducing the recent advances of SACs in various electrochemical reactions and summarising the characterisation techniques used for ACs. Some reviews were published outlining advancements in using SACs for ammonia synthesis from nitrate56,57 and nitrogen gas.58–60 One review even focused on theoretical DACs.61 These reviews are specific to nitrate reduction or nitrogen reduction to ammonia only. In this review, we emphasize specifically the recent advancements in NH3 and urea electrosynthesis that utilise SACs and DACs (Scheme 1) and compare the various nitrogen sources that are used. Research into the electrochemical synthesis of urea has taken off with atomic catalysts as well. It is about time to step back and look at the various advancements utilizing these catalysts. We will look at the challenges of each reaction and how both SACs and DACs overcome them in their unique ways. We will also explore some theoretical papers that utilise density functional theory (DFT) to screen suitable catalysts for the respective application. Finally, we will give suggestions and outlooks for further research in the area of NH3 and urea synthesis using ACs.
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Fig. 1 (a) HAADF-STEM image of Au-NDPC. Single Au atoms are circled. (b) LSV curves of Au-NDPC in Ar- and N2-saturated electrolytes. (c) NH3 FEs and yield rates across various potentials. (d) Comparison of FEs for SAC, NP and blank support. Reproduced with permission.67 Copyright 2018, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (e) Illustration of SA-Mo/NPC. (f) LSV curves of SA-Mo/NPC in Ar- and N2-saturated electrolytes. (g) NH3 FEs and yield rates across different potentials. (h) NH3 FE comparison of various Mo wt% loading. (i) Stability test of SA-Mo/NPC across 50![]() |
Reaction | Classification | Catalysts | Mass loading | Yield rate | FE | Potential vs. RHE | Electrolyte | Ref. |
---|---|---|---|---|---|---|---|---|
a Not stated in paper, back calculated. | ||||||||
NRR | SAC | AuSAs-NDPC | 0.205 wt% | 2.32 μgNH3 h−1 cm−2/1886 μgNH3 h−1 mgAu−1 | 12.30% | −0.2 V | 0.1 M HCl | 67 |
Au1/C3N4 | 0.15 wt% | 1305 μgNH3 h−1 mgAu−1 | 11.10% | −0.1 V | 5 mM H2SO4 | 68 | ||
SA-Mo/NPC | 9.54 wt% | 34.0 ± 3.6 μgNH3 h−1 mgcat−1/356 μgNH3 h−1 mgMo−1![]() |
14.6 ± 1.6% | −0.3 V | 0.1 M KOH | 37 | ||
Ru–S–C | 0.55 wt%a | 13.17 μgNH3 h−1 mgcat−1/2.4 mgNH3 h−1 mgRu−1 | 6.16% | −0.15 V | 0.1 M H2SO4 | 70 | ||
BG | 6.2 wt% | 9.8 μgNH3 h−1 cm−2 | 10.80% | −0.5 V | 0.05 M H2SO4 | 71 | ||
DAC | CNT @C3N4-Fe&Cu | Fe: 7.51 wt%, Cu: 10.77 wt% | 9.86 μgNH3 h−1 mg−1 @ −1.2 V vs. Ag/AgCl | 34% @ −0.8 V vs. Ag/AgCl | — | Not stated | 42 | |
O–V2-NC | 1.32 wt% | 26 μgNH3 h−1 mg−1/1969 μgNH3 h−1 mgV−1![]() |
77.2% @ 0 V vs. RHE | — | 0.1 M HCl | 73 | ||
NO3RR | SAC | Fe-Ppy SAC | 2.38 wt% | 30 mmolNH3 h−1 mgFe−1 | 100% | −0.6 V | 0.1 M KOH + 0.1 M KNO3 | 86 |
Fe1/CN-900 | 0.44 wt% | 1.10 mmolNH3 h−1 mgcat−1/18.8 mgNH3 h−1 mgcat−1/4250 mgNH3 h−1 mgFe−1![]() |
86.7% @ −0.7 V vs. RHE | — | 0.1 M K2SO4 + 0.5 M KNO3 | 87 | ||
Fe SAC | 2.9 wt% | 46 mgNH3 h−1 mgcat−1 @ −0.88 V vs. RHE | 92% @ −0.68 V vs. RHE | — | 0.1 M K2SO4 + 0.5 M KNO3 | 88 | ||
Cu–N–C | 1.0 wt% | 4.5 mgNH3 h−1 cm−2/212.5 mgNH3 h−1 mgCu−1 | 84.70% | −1 V | 0.1 M KOH + 0.1 M KNO3 | 90 | ||
ZnSA-MNC | 1.33 wt% | 39 mgNH3 h−1 mgcat−1 @ −1.0 V vs. RHE | 94.8% @ −0.9 V vs. RHE | — | 0.1 M Na2SO4 + 0.5 mM NaNO3 | 91 | ||
NiO4-CCP | 18 wt% | 1.83 mmolNH3 h−1 mg−1/173 mgNH3 h−1 mgNi−1![]() |
94.70% | −0.7 V | 1 M Na2SO4 + 0.5 M NO3− | 92 | ||
VCu-Au1CuSAA | 0.41 wt% | 555 μgNH3 h−1 cm−2/169 mgNH3 h−1 mgAu−1![]() |
98.70% | −0.2 V | 0.1 M KOH + 7.14 mM KNO3 | 93 | ||
Ru1–TiOx/Ti | 0.03 wt% | 22.2 mgNH3 h−1 mg−1/74![]() ![]() |
87.60% | −0.3 V | 1 M KOH + 0.5 M NaNO3 | 94 | ||
DAC | Cu/Ni-NC | Not stated | 5480 μg h−1 mgcat−1 cm−2 | 97% | −0.7 V | 0.5 M Na2SO4 + 100 ppm NaNO3 | 97 | |
Fe/Cu-HNG | Fe: 3.3 wt%, Cu: 2.8 wt% | 1.08 mmolNH3 h−1 mg−1 @ −0.5 V vs. RHE | 92.51% @ −0.3 V vs. RHE | — | 1 M KOH + 0.1 M KNO3 | 98 | ||
NO2RR | SAC | Co1Ru | Co: 3.3 wt%a | 476.8 μmol h−1 cm−2 (H-cell)/2379.2 μmol h−1 cm−2 (flow cell) | 94.2%/92% | −0.7 V/−0.8 V | 0.5 M Na2SO4 + 0.1 M NaNO2 | 106 |
CuRh1 | Rh: 10.4 wt%a | 2191.6 μmol h−1 cm−2 | 98.9% | −0.6 V | 0.5 M Na2SO4 + 0.1 M NaNO2 | 107 | ||
Rh1/BN | Not stated | 2165.4 μmol h−1 cm−2 | 97.83% | −0.7 V | 0.5 M Na2SO4 + 0.1 M NaNO2 | 108 | ||
DAC | FeCu DAC | Not stated | 24![]() |
99.88% | −0.6 V | 0.1 M KOH + 0.1 M NaNO2 | 115 | |
NORR | SAC | W1/MoO3−x | W: 13.7 wt% | 308.6 μmol h−1 mg−1 @−0.5 V vs. RHE/38.4 mgNH3 h−1 mgW−1 | 91.2% @ −0.4 V vs. RHE | — | 0.5 M Na2SO4 | 109 |
Cu1/MoS2 | Cu: 1.58 wt% | 337.5 μmol h−1 cm−2 | 90.6% | −0.6 V | 0.5 M Na2SO4 | 111 | ||
Ir1/a-MoO3 | Ir: 7.6 wt% | 438.8 μmol h−1 cm−2 | 93.2% | −0.47 V | 0.5 M Na2SO4 | 110 | ||
Urea synthesis | SAC | Cu-GS-800 | 3.9 wt% | 1.8 mgurea h−1 mgcat−1/4.3 nmolurea s−1 cm−2/46.2 mgurea h−1 mgCu−1 | 28% | −0.9 V | 0.1 M KHCO3 + 0.1 M KNO3 + CO2 | 126 |
L-Cu1–CeO2 | 3.99 wt% | 52.84 mmolurea h−1 gcat−1/79.5 mgurea h−1 mgCu−1 | Not stated | −1.6 V | 0.1 M KHCO3 + 50 mM KNO3 + CO2 | 127 | ||
DAC | B-FeNi-DASC | Fe: 0.991 wt%, Ni: 0.896 wt% | 20.2 mmolurea h−1 gcat−1 | 17.80% | −1.5 V | 0.1 M KHCO3 + 50 mM KNO3 + CO | 119 | |
Pd1Cu1–TiO2 | Not stated | 166.67 molurea molPd−1 h−1/10 mmolurea h−1 gcat−1 | 22.54% | −0.5 V | 0.1 M KHCO3 + CO2 + N2 | 129 |
Non-metallic catalysts were reported as well. Yu et al. doped 6.2% concentration Boron onto graphene and managed to achieve a high NH3 FE of 10.8%.71 The electronegative difference between Boron (2.04) and Carbon (2.55) results in Boron having a positive charge of +0.59e. This small positive charge allowed Boron to adsorb N2 easily, acting as excellent catalytic centers for NRR. In addition, competitive HER was suppressed due to the unfavourable adsorption of H+ ions, thus further boosting NH3 FE.
Computational studies on SACs have been conducted as well. Various transition metal-porphyrins (TM-PPs) were studied by Xue et al.72 They found that Ti, V, Co, Zr, Ru and Hf should be excluded due to their high first hydrogenation energies. W-PP was found to exhibit the best performance. This could be attributed to the strong interaction between W and N atoms, which was due to the hybridisation of W-5d and Nc-2p orbitals, resulting in W having a charge of +0.51e and a magnetic moment of 2.23μB. This charge and magnetic moment led to good N2 adsorption and HER suppression.
Fe and Cu atoms were synthesized with a ratio of 1:
1 on graphitic carbon nitride (CNT@C3N4-Fe&Cu), simultaneously coordinating with each other and surrounding N atoms.42 A two-step synthesis process was developed: the precursor solution was first lyophilised followed by annealing under an inert atmosphere (Fig. 2a). These confined atoms formed a “sub-nano” reactor with three atoms (Fig. 2b–d), achieving a high NH3 yield rate of 9.86 μg h−1 mg−1 at −1.2 V vs. Ag/AgCl. A significantly higher FE of 34.0% vs. −0.8 V vs. Ag/AgCl was obtained as compared with single Fe catalyst (15.3%) and single Cu catalyst (22.0%). This excellent performance can be attributed to the triple metal atoms consisting of both Fe and Cu. An adsorbed N2 molecule is stabilised by all three atoms at once, resulting in a weaker N–metal bond and NH3 formed can be desorbed with lower energy. The sub-nano reactor consisting of both Fe and Cu atoms catalyst also changed the potential-determining step (PDS) to the first hydrogenation step with a low energy barrier of 0.58 eV (Fig. 2e), compared with Fe-only catalyst (0.71 eV) and Cu-only catalyst (0.86 eV). The metal–metal coordination between Fe and Cu facilitated electron transfer better compared with metal–N coordination in conventional SAC. In another paper by Wang et al., a DAC consisting of dual vanadium atoms with oxygen bridge on N-doped carbon (O–V2-NC) was synthesized by a template-assisted pyrolysis method.73 The catalyst exhibited an extremely high NH3 FE of 77.2% at 0 V vs. RHE and a yield rate of 26 μg h−1 mg−1 at −0.4 V vs. RHE. Extended X-ray absorption fine structure (EXAFS) showed the presence of V–V bond with an unusually long bond length of 2.70 Å. The authors attributed this anomaly to the O atom bridging the two V atoms. This was further proved by treatment of the catalyst in 5% H2 at 250 °C for 2 hours, where the V–O bond disappeared. The catalyst also exhibited good stability after 10 consecutive cycling tests, showing V leaching of only 5 parts per billion (ppb) after the cycling tests. Post-test characterisations also showed no changes to the catalyst structure. On the other hand, DFT study found that during the protonation process, V–O–V broke down to V–O and isolated V due to hindrance of *NNH, leaving vanadium connected to *NNH alone instead of V–O–V*NNH. This transformed structure remained until nitrogen species were released from vanadium and it was regenerated back to V–O–V.
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Fig. 2 (a) Schematic diagram for synthesis process and morphology of CNT@C3N4-Fe&Cu (b) TEM image of CNT@C3N4-Fe&Cu, (c and d) STEM image of CNT@C3N4-Fe&Cu. Reproduced with permission.42 Copyright 2020, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (f) Illustration of catalytic mechanism of SAC and DAC. Reproduced with permission.74 Copyright 2021 American Chemical Society. (g) Fe2 in-plane of g-C3N4 (h) Fe2 on the side of the g-C3N4 (i) and (j) effect of strain on overpotential and adsorption energy, respectively. Reproduced with permission.75 Copyright 2021 American Chemical Society. |
The local environment of the active centers for DACs can be easily tuned via various strategies, such as changing the substrate that the DACs are anchored on, utilisation of doping and even changing the DACs themselves. A theoretical study was done to test the feasibility of using boron and transition metals (TMs) (B-TM@g-CN) as DACs.74 As illustrated in Fig. 2f, both B and TMs can act as the catalytic active centers for NRR because d orbitals of TMs and sp3 hybrid orbitals of B are able to accept the lone-pair electrons of N2. The difference in charge transfer ability of the two centers can enhance the polarisation of adsorbed N2 and reduce the N–N bond strength. From this, a hypothesis was put forward: “The greater the difference in valence electron distribution between the two atoms in the DAC, the more favourable it is to achieve low potential nitrogen fixation”. It was found that electrons were more likely to enter the antibonding orbitals on B-TM@g-CN and the difference in electron supply caused N2 to polarise greatly, easily pulling N2 apart. 29 TMs were tested, and it was found that Ti and Ta showed the best results with low limiting potentials of 0.13 V and 0.11 V, respectively, for NRR and high potentials of 0.54 V and 0.82 V, respectively, for competitive HER. In another paper, investigation was done on iron dimer Fe2 on g-C3N4 monolayer.75 Two most stable geometries were found, with both geometries comprising the two iron atoms containing positive charges and located side by side – together in the same plane as g-C3N4 or on one side of the g-C3N4 matrix, as shown in Fig. 2g and h, respectively. It was postulated that during the electrocatalytic process, the two geometries may interchange. Further study on the strain effect was done, as it is known that strain can tune the catalytic properties of transition metals. When a tensile strain of 2% was applied, the rate-determining step changed with a decrease in overpotential (Fig. 2i). This was attributed to the change in geometry due to strain. One Fe–N bond was shortened due to the strain, weakening the binding between the two Fe atoms. This resulted in a much stronger interaction between the other Fe atom and adsorbates. Most importantly, the scaling relation was shown to be broken. Adsorption energies of *N2 and *HNN were expected to be monotonic and smooth with the magnitude of applied stress. However, for iron dimer DAC, the adsorption energy of *N2 exhibited a hysteresis instead (Fig. 2j). The effect of coordination on DAC was studied by Wu et al.76 They found that when B or O was doped, the adsorption free energy of N2 increased, enhancing the activation of reactants. Linear scaling of adsorption energy between intermediates was also found to be poor in both cases. In particular, Mn2ON5/G was found to be the most active DAC, with a limiting potential of −0.27 V, much lower than that of MnN6/G with a limiting potential of −0.48 V. Mn2ON5/G was found to adopt the enzymatic pathway instead of the distal pathway that Mn2N6/G adopted. Alkaline earth (AE) metals are typically not used as catalysts as they lack partially filled d-orbitals for the acceptance-donation reaction with reactants. However, a study by Wu et al. showed that AE metals can form partially filled d orbitals by the diffusion of electrons from the ns orbital to low-lying (n − 1)d orbitals.77 This was illustrated in Ca2 dimer, where the d-orbital gained 1.08 electrons when forming Ca2@WS2 DAC, allowing for adsorption and activation of reactants. AE metals were thought to have difficulty catalysing NRR as they lack partially occupied d-orbitals for the acceptance-donation reaction with N2. It was also found that the adsorption strengths of the intermediates have poor scaling relation, with R2 values of 0.80 for adsorption energies between *N2 and *NH2 and 0.79 for adsorption energies between *NH2 and *NH3, further improving NRR activity. Further testing found that CaBa@MoSe2 DAC has the lowest limiting potential of −0.6 V owing to the synergistic effect between Ca, which has a stronger adsorption for NxHy, and Ba which has a weaker adsorption for NxHy, facilitating N2 adsorption and activation while at the same time reducing the binding strength of *NH2, reducing the amount of energy required to convert it to *NH3.
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Fig. 3 (a) Schematic for the synthesis of Fe SAC from MOF precursor. (b) LSV curves of Fe SAC in electrolytes with and without KNO3. (c) NH3 FEs of Fe SAC across different potentials. (d) LSV curves of Fe SAC (2.0 wt%), Fe SAC (1.6 wt%), Fe nanoparticles and blank support. (e) Stability test of Fe SAC over 15 cycles. (f) Gibbs free energy diagram of NO3RR on FeN2O2 and FeN4. Reproduced with permission from ref. 88, copyright 2022 Elsevier B.V. (g) Operando first-order derivatives of XANES at various potentials. (h) LCF results of Cu K-edge XANES spectra at various potentials. (i) Mechanism of Cu SAC aggregation and dispersion. Reprinted with permission from ref. 90. Copyright 2022 American Chemical Society. |
While copper is cheap and abundant, there are various issues when using Cu in electrocatalysis: deactivation of catalyst after long operation due to passivation, leaching and corrosion, and accumulation of toxic secondary product of nitrite.89 Cu SACs can circumvent these issues. Zhu et al. synthesized Cu atoms supported on nitrogenated carbon nanosheets, demonstrating good activity and stability towards NO3RR.89 The catalyst synthesized at 800 °C showed the best (minimum) selectivity towards nitrite of only 5.0%, a stark contrast to Cu plate showing 60.6% selectivity. Furthermore, stability testing after 20 cycles showed an electrocatalytic activity drop of only 7.2%. The drop was due to the formation of Cu nanoparticles, but this aggregation was not significant based on the absence of additional peaks in the X-ray diffraction (XRD) pattern. Further DFT studies showed the established rate-determining step of adsorption was much lower for that of Cu SAC: 6.13 eV for Cu(111) in bulk copper vs. −4.06 eV for Cu–N2 and −2.05 eV for Cu–N4 in Cu SAC. In another instance, Cu SAC on N-doped carbon was synthesized and phase transformation was observed as the potential was changed from 0 to −1 V vs. RHE as evident in the operando X-ray absorption spectroscopy (XAS) measurements.90 The first-order derivatives X-ray absorption near edge structure (XANES) spectra and linear combination fitting (LCF) results of Cu K-edge XANES spectra in Fig. 3g and h revealed that the Cu–N4 structure transformed from Cu–N3 to near free Cu0 single atoms to eventually aggregated Cu0 nanoparticles. The NH3 FE and yield rate were enhanced throughout the transformation, reaching a maximum FE of 84.7% and yield rate of 0.264 mmolNH3 h−1 mgcat−1 at −1 V vs. RHE, indicating that these nanoparticles are active sites that contribute greatly to the NO3RR process. It was also found that the nanoparticles can be restored back to the SAC state of Cu–N4. However, the restoration is not as straightforward as the forward process by simply changing the potential from −1 V back to 0. It must be done so in an oxidative environment, via the formation of [Cu(OH)4]2− intermediate which is captured by the pyridinic nitrogen on the carbon support (Fig. 3i).
SACs composed of other cheap and abundant transition metals such as Ni and Zn have also been used for NO3RR to NH3. Zhao et al. synthesized Zn SACs with 1.33 wt% on microporous N-doped carbon (ZnSA-MNC).91 They managed to achieve an NH3 yield rate of 39000 μg h−1 mgcat−1 at −1.0 V vs. RHE, 4 times that of the corresponding nanoparticles. A high FE of 94.8% at −0.9 V vs. RHE was achieved as well. The selectivity of ammonia was also very high at 97.2% due to the lack of adjacent sites in the isolated active metal centers preventing N–N coupling and reducing N2 selectivity. Further DFT study showed Zn single atoms possessed a positive charge of +1.58e which was conducive for the adsorption of negatively charged NO3−. Zhang et al. synthesised Ni SAC with either NiO4 or NiN4 coordination on conjugated coordination polymers (CCP) using a one-step solvothermal method.92 CCP was selected due to the enhancement of electrical conductivity via interactions between the π system of aromatic domains in CCP and the d orbitals of transition metals. Both configurations exhibited a high metal loading of around 18 wt%. In contrast to NiN4-CCP, which exhibited an NH3 FE of 61.8% and a yield rate of 0.86 mmol h−1 mg−1, NiO4-CCP was able to deliver a superior NH3 FE of 94.7% and a yield rate of 1.83 mmol h−1 mg−1 at −0.7 V vs. RHE. Additionally, the catalyst demonstrated good stability over the course of three days of continuous chronoamperometry testing, exhibiting no structural alterations and no obvious decline in both current density and NH3 FE.
Precious metals have been used for their generally excellent catalytic activity. Au single atoms were anchored on two-dimensional (2D) Cu nanosheets with (111) single crystal surface and Cu vacancies (VCu-Au1Cu SAA) via a three-step process (Fig. 4a).93 Single-crystal Cu nanosheets were first prepared by chemical reduction, then single Au atoms were deposited via galvanic replacement. Finally, the resulting product was dispersed in acetic acid for etching to generate vacancies in the copper nanosheet. High-resolution TEM (HRTEM) and energy dispersive X-ray spectroscopy (EDS) (Fig. 4c and d) showed the structure and distribution of Au on Cu nanosheet with Au loading of 0.41 wt%. HAADF-STEM (Fig. 4b) revealed the presence of both Au single atoms and Cu vacancies. NH3 FE of 98.7% and yield rate of 555 μg h−1 cm−2 were achieved at −0.2 V vs. RHE, superior to those of pristine copper nanosheet, copper nanosheet with vacancies and Au NPs (Fig. 4e–g). Mechanism study showed that Au atoms and Cu vacancies can prevent HER by inhibiting the Heyrovsky step: *H + H2O + e− → H2 + HO−. Single Ru atoms anchored on an amorphous layer of monolithic Ti support was synthesized,94 exhibiting an NH3 FE of 87.6% and a yield rate of 22.2 mol g−1 h−1. The authors tested the scaling capability of their synthesized catalyst and found that Ru atoms were evenly dispersed with no aggregation even when the titanium-based monolithic single-atom electrode was increased from 2 × 2 cm to 25 × 15 cm. The synthesis method was found to be applicable to other single-atom electrodes, such as Sn, Bi, Pd, and Pt, demonstrating the versatility of the synthesis method.
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Fig. 4 (a) Scheme illustrating synthesis of VCu-Au1Cu SAA. (b) HAADF-STEM image. Single Au atoms indicated by red arrows while Cu vacancies are circled in white. (c) HRTEM image and fast Fourier transformation (FFT) pattern of VCu-Au1Cu SAA. (d) EDS mapping showing distribution of Cu and Au elements. (e) LSV curves comparison of various synthesized catalysts. (f) Selectivity of various samples. (g) NH3 FE and selectivity of SAC compared with NP. Reproduced with permission from ref. 93. Copyright 2022 Elsevier B.V. |
In a theoretical work by Wu et al., AE metals were screened for their feasibility to be used as SACs for NO3RR.95 Similar to NRR, it had been thought that the lack of partially filled d-orbitals renders AE metals catalytically inactive. However, it was proved experimentally that AE metals have catalytic properties, being able to catalyse ORR. Nitrate can adsorb onto AE metals with two O atoms binding to the AE active site, with an adsorption energy similar to that of transition metals. The change in Gibbs free energy from binding of nitrate was also found to be more negative than that of hydrogen, indicating a more favourable NO3RR instead of competitive HER. The limiting potential of SrN3C and BaN3C was found to be −0.05 V, even lower than those of TM SACs. Interestingly, AE metal was stabilised by ionic bond interactions with the N-doped support. Similarly, NO3− was mainly adsorbed via ionic bond interaction. The N-doped graphene support acted as an electron reservoir while the AE metal acted as a transmitter, allowing for the mimicking of TM's donation–back donation mechanism of activating nitrate.
In what might be the first synthesis of DACs for NO3RR to NH3, Wang and colleagues synthesized Cu–Ni DAC anchored in N-doped carbon (Cu/Ni-NC) by pyrolyzing ZIF-8 MOF precursor97 (Fig. 5a). The synthesized materials consisted of both Ni–Cu dual atoms as well as Cu and Ni single atoms, as evident in the atomic resolution HAADF-STEM image (Fig. 5b). They were able to achieve a stable NH3 FE of ∼97% and yield rate of 5480 μg h−1 mgcat−1 cm−2 at −0.70 V vs. RHE (Fig. 5d). LSV comparison with Cu SAC and Ni SAC in Fig. 5c showcased the superiority of the synthesized Cu/Ni-NC as it had the greatest increase in current density. DFT study showed that the optimal adsorption site of nitrate was N-coordinated Cu–Ni dual–single-atom rather than single Cu or Ni atom due to the much lower adsorption energy of 0.5 eV. The rate-determining step of the deoxidation process of HNO* to N* on Cu–Ni (−0.37 eV) was also much lower than those on Cu (1.03 eV) and Ni (1.30 eV) (Fig. 5e). Stronger hybridisation was also found between Cu–Ni and O of adsorbed nitrate, effectively forming chemical bonds of Cu–O–NO3−*–O–Ni and promoting electron transfer from the DAC to NO3−*. Zhang et al. synthesized Fe/Cu DACs anchored on holey edge sites of nitrogen-doped graphene (HNG).98 Holes were made in graphene to create a large number of edge sites which were then nitrified to bind Fe/Cu atoms, forming a “Y-type” ML3 structure (Fe/Cu-HNG). Compared with homogeneous diatomic catalysts (Fe/Fe-HNG and Cu/Cu-HNG) and SACs (Fe-HNG and Cu-HNG), Fe/Cu-HNG exhibited the best performance with an NH3 FE of 92.51% at −0.3 V vs. RHE and a yield rate of 1.08 mmol h−1 mg−1 at −0.5 V vs. RHE. DFT study showed that two oxygen atoms of NO3− were adsorbed to Fe/Cu dual sites, with a higher binding energy (−1.19 eV) compared with Fe SACs (−0.89 eV) and Cu SACs (−0.56 eV). This high binding energy led to a lower energy barrier of the first discharge step: * + NO3− → NO3* + e−. Subsequent adsorption energies of intermediate products were also shown to have medium binding energies compared with Fe and Cu SAC, with all steps showing a downhill trend (Fig. 2d).
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Fig. 5 (a) Schematic of the synthesis of Cu/Ni-NC. (b) Atomic resolution HAADF-STEM image of Cu/Ni-NC. Cu/Ni DACs are circled in red; Cu or Ni SACs are circled in yellow. (c) LSV curves of Ni SAC, Cu SAC and Cu/Ni DAC. (d) NH3 FEs and yield rates of Cu/Ni-NC at various potentials. (e) Free energy diagram of NO3RR. Reproduced with permission.97 Copyright 2023, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (f–h) Free energy diagrams for Cr2, V2 and Ti2, respectively. Reproduced with permission.99 Copyright 2022, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (i) Screening methods for filtering elements suitable for BSAC. (j and k) Illustrations of conventional BACs and proposed BSACs, respectively. Reproduced with permission.101 Copyright 2022, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. |
The effect of varying substrate on DACs was introduced in the following theoretical studies, followed by a novel DACs structure with an entirely different mechanism. Rehman et al. conducted a theoretical study on DACs for NO3RR to NH3 using metal catalysts in 2D expanded phthalocyanine (Pc) substrate.99 Pc was used as it has a strong ability to bind metal atoms, being able to accommodate both TMs and main group metals. It was found that Cr2-Pc, V2-Pc, Ti2-Pc and Mn2-Pc DAC showed the best potential for NO3RR, with incredibly complex mechanisms. As shown in the free energy diagrams (Fig. 5f–h), the limiting potentials were found to be −0.02, −0.25, −0.34 and −0.41 V, respectively, significantly lower than other metals. Nitrate ion binds strongly to the dual-atom site compared with proton, indicating better selectivity to NO3RR over competitive HER. In another paper, catalysts on N-doped graphene were theoretically studied.100 N-doped graphene (N6-G) was chosen due to its higher electrical conductivity compared with graphene and higher tunability to improve electrochemical activity in a coordinated environment. The paper found that Cr2/N6-G, Mn2/N6-G and Cu2/N6-G had the best potential due to their high stability, selectivity (FEs of 100, 61.26 and 99.99%, respectively) and relatively low limiting potentials of −0.46, −0.45 and −0.36 V, respectively. Cr, Mn and Cu were able to effectively adsorb NO3− ions and activate them by the ease of charge transfer from d-orbitals of TMs to the empty p* orbital of the *NO3 molecule. Free energy calculations also showed that hydrogen poisoning can be avoided. In a novel approach to the topic of DAC, Lv et al. proposed an entirely different DAC structure. Instead of the usual focus on “in-plane” DACs where the two catalytic atoms are located in the same plane and dispersed on one support material (Fig. 5j), they proposed a bilayer SAC (BSAC), shown in Fig. 5k.101 This structure has many advantages: prevention of metal aggregation, lack of neighbouring sites in BSAC reducing undesirable N–N coupling as it reduces NH3 selectivity, and preservation of the ability to tune reactivity. This tunability comes from BSAC composed of different catalytic atoms, or heterogeneous BSAC. Heterogeneous BSAC can induce polarisation perpendicular to the surface, resulting in an electric field that can accumulate a higher concentration of NOx, and adjust the binding strength between reactants and catalysts. With this, DFT calculations for homogeneous and heterogeneous BSAC were carried out on a support of N-doped graphene for its structural flexibility and thermal stability. After several rounds of screening and filtering (Fig. 5i), only V2-N4-GN was found to be a promising homogeneous BSAC. It was discovered that there are two ways polarisation can affect the mechanism of NO3RR: (1) Polarisation does not change the mechanism of NO3RR, instead altering the free energy change of each step. This can be seen in the case of NbV-N4-GN. (2) Polarisation completely changes the NO adsorption pattern and reaction pathway, which can be seen in the example of Hf and Zr. TiV-N4, NbV-N4 and GaV-N4-GN were found to be the best three systems to suppress HER, with a limiting potential of −0.32 V, −0.20 V and −0.25 V, respectively.
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Fig. 6 (a) Synthesis of single Rh atoms on defective BN nanosheet. (b) LSV curves of Rh1/BN in H cell and flow cell. (c) Stability test of Rh1/BN over 200 h. Reproduced with permission.108 Copyright 2024, Elsevier Inc. (d) The donation–backdonation mechanic of NORR. Reproduced with permission.113 Copyright 2023 American Chemical Society. (e) R-space curve fitting of FeCu DAC with the proposed structure of FeCuN7. Reproduced with permission.115 Copyright 2023 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (f) Bader charge number obtained by NO in various configurations. (g) Reaction pathway for FeCuN7. Reproduced with permission.116 Copyright 2024 Elsevier Ltd. (h) Gibbs free energy diagram for NORR on MoMo@g-CN. Reproduced with permission.117 Copyright 2023 American Chemical Society. |
Moving on to NORR, the following papers studied the usage of different elements and their different substrates. Chen et al. confined W single atoms in amorphous MoO3−x nanosheet (W1/MoO3−x) with W1–O5 motifs for NORR.109 They managed to achieve a NH3 FE of 91.2% at −0.4 V vs. RHE and yield rate of 308.6 μmol h−1 cm−2 at −0.5 V vs. RHE. Compared with pristine MoO3 on which NO adsorbed weakly, OV-induced coordinatively unsaturated Mo1–O5 and W1–O5 could effectively adsorb and dissociate the NO bond, with W1–O5 further promoting H2O dissociation and retarding *H dimerization to supply adequate protons. W1–O5 motifs also exhibited a dual function forming a self-tandem NORR mechanism, where some W1–O5 activated NO to form intermediates while others dissociated H2O and supplied *H for intermediate protonation. In two other studies done by the same group, Ir SACs110 and Cu SACs111 were synthesized for NORR. In both studies, NH3 FE exceeded 90% and showcased high NH3 yield rates of 337.5 μmol h−1 cm−2 for Cu SACs and 438.8 μmol h−1 cm−2 for Ir SACs. Similar to Rh SACs, the respective SACs showcased unique moieties (Cu1–S3 and Ir1–O5) which boosted the selectivity of NH3 and suppressed HER. In another study by Zhao et al., they demonstrated that the active metal center is pivotal in product selectivity.112 When Ni was anchored on a metalloporphyrin framework epitaxially grown on graphene, NH3 FE reached 81.2% and a yield rate of 1.6 mmol mg−1 h−1 was achieved at −0.51 V vs. RHE, whereas if Fe was used instead, NH2OH was selectively produced with a FE of 83.5% and a yield rate of 3.1 mmol mg−1 h−1 at −0.14 V vs. RHE.
In a theoretical paper published by Hu et al., TMs on 1,3,5-triethynnylbenzene (TM–TEB) were screened as candidates for NORR.113 The TM–TEB system was an assembly of TM atoms and TEB molecules through twofold TM–alkynyl coordination bonds (–CC–TM–C
C–), combining the superior properties of SACs and graphynes, such as unsaturated metal coordination, electrochemical stability, high electrical conductivity, easy synthesis and separation, fast mass transfer and effective charge transport. After extensive screening and selection, Cr, Pd and Pt were identified as potential candidates. Cr-TEB was found to be the best candidate, having high NH3 selectivity and low limiting potential. Cr-TEB interacted with *NO by a “donation–backdonation” mechanism (Fig. 6d). The empty d orbitals of TM accepted the electrons of NO-σ orbitals, forming the bonding states to strengthen the adsorption of NO molecules. The occupied d orbitals of TM then back-donated electrons to the empty π* orbitals of NO, leading to the activation of *NO. Protonation of *N2O2 was the potential-determining step with an energy barrier of 0.867 eV for NORR to N2. With such a high energy barrier, N2 selectivity was thus low, improving ammonia selectivity. In another DFT study, Li et al. looked at graphene-based Fe SACs for NORR. 26 systems were investigated, including PD-FeN4 (coordinated N atom replacing one C atom of the six-membered ring), PR-FeN4 (coordinated N atom replacing one C atom of the five-membered ring) and the C, N and O, N coordinated cases.114 Similar to the previous paper, Fe SACs could adsorb and activate NO via the same electron donation–backdonation mechanism. PD-FeN3O and PR-FeN4 were found to have excellent NORR properties with low limiting potentials of −0.33 and −0.26 V, respectively. They also exhibited good selectivity towards NH3, not only suppressing HER but also prohibiting the formation of N2O and N2. Finally, Qian et al. looked at the effect of pH and potential on the product selectivity of NORR. It was found that before −1.60 V, *NO adsorption dominated, whereas any potential more negative than −1.60 V became *H dominated. The branching reaction of *NO was deterministic of what N-containing products would form in the end: if *HNO intermediate was formed, single-N products tended to form (e.g. NH3 or NH2OH). If *ONNO intermediate was formed, N–N coupled products tended to form instead (e.g. N2O or N2). In a highly acidic solution, a lower NO concentration and a more negative applied potential selectively promoted the formation of *HNO, while in a highly alkaline solution, increased NO concentration and a moderately negative applied potential favourably benefited the formation of *ONNO.
Cu was introduced into Fe–N–C (iron–metal–carbon) to form FeCu DAC with a configuration of FeCuN7 (Fig. 6e) for NO2RR.115 An impressive NH3 FE of 99.88% and a yield rate of 24526 μg h−1 mgcat−1 at −0.6 V vs. RHE were achieved. DFT study showed that NO2 adsorption was enhanced by the introduction of Cu atom as the d-band center shifted upwards from −1.55 eV (FeN4) to −1.48 eV (FeCuN7). The energy barrier of PDS (*N → *NH) also decreased from 0.74 eV to 0.49 eV (Fig. 6g). The electronic property of the Fe atom was altered upon incorporation of the Cu atom, with a better electron redistribution promoting catalytic conversion of the intermediates, reducing the thermodynamic energy barriers of key steps for NO2RR.
While the experimental works regarding DACs for NORR are limited, several theoretical investigations have been conducted. The effects of substrate on DACs were investigated. Wu et al. published a study on SACs and DACs for NORR, looking at TMs doped on graphdiyne (GDY).118 SACs were found to be thermodynamic process controlled, i.e., NH3 and H2O molecule desorption, while DACs were found to be electrochemical process controlled i.e., hydrogenation steps. For SACs, Cu@GDY was found to have the lowest limiting potential of −0.1 V with a NH3 desorption energy of 2.81 eV. Cu2@GDY, on the other hand, was found to have a limiting potential of −1.04 V. However, Cu2@GDY showed a better selectivity towards ammonia compared with H2. In another paper, TMs on nitrogen-doped graphite was screened and Ti2–N6 was found to exhibit the best catalytic activity and selectivity towards NH3 for NORR, with a low limiting potential of −0.24 V and strongly repulsive against the HER process.116 This addresses the issue that while SACs exhibited good catalytic ability in catalysing NORR, they are not selective and are inclined to generate H2. The origin of the enhanced NH3 selectivity and activity comes from the introduction of adjacent metal atoms in active sites leading to enhanced charge communication. This allows for unique parallel-on structure adsorption of NO on DACs, which was found to be the most favourable and activated configuration of NO adsorption. Bader charge analysis also showed an impressive 0.9e charge donation from substrate to adsorbate, higher than all other configurations (Fig. 6f). Sun et al. conducted a similar study to screen candidates for heterogeneous DACs on graphitic carbon nitride (TM1TM2@g-CN) for NORR.117 TiCr, TiMo and MnMo@g-CN with limiting potentials of −0.37, −0.37 and −0.43 V, respectively, were screened as potential candidates. In particular, MoMo@g-CN was found to be able to reduce NO to NH3 spontaneously. Mo SAC has a 3d orbital that is localised and closer to Fermi level. A second Mo atom is able to modulate the orbital distribution and local electronic structure, making the d-band center in MoMo@g-CN more negative. This resulted in antibonding states between MoMo and NO having an electron occupancy greater than Mo and NO, weakening NO adsorption on MoMo@g-CN. This allowed for the thermodynamically spontaneous reduction of NO to NH3 as the PDS of Mo@g-CN stemmed from hydrogenation of *NO to *NOH (Fig. 6h).
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Fig. 7 (a) HAADF-STEM image of Cu SACs. Isolated Cu atoms are marked with red circles. (b–e) EDS mapping showing distribution of C, Cu and N elements. (f) FEs of various products across different potentials. (g) Yield rates of urea across potentials comparing the 3 different Cu SACs synthesized. (h) Illustration of various Cu SAC local environments. (i) Free energy diagrams of urea synthesis on the various Cu SACs. Reproduced with permission.126 Copyright 2022. Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. (j) Aberration-corrected TEM (AC-TEM) image. (k) AC-HAADF-STEM of Cu SAC on CeO2. (l–o) EDS mapping showing distribution of Cu, Ce and O, respectively. (p) Urea yield rates of various catalysts across a range of potentials. (q) Stability testing over 8 cycles comparing between Cu SAC and CuO on CeO2. (r) Cu K-edge XANES spectra and (s) Cu R space EXAFS of Cu SACs on CeO2 at various potentials. (t) Illustration of the reversible transformation between Cu SACs and Cu clusters. Reproduced with permission.127 Copyright 2023. Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. |
Boron has an empty sp2 orbital and an occupied p-orbital, allowing the acceptance of lone-pair electrons from N2 and back-donation to the antibonding orbital of N2. Therefore, Kong et al. theoretically studied single atoms anchored on porous boron nitride (p-BN) for urea synthesis.128 After a four-step strategy to screen and filter elements, Fe and Co were found to satisfy all four conditions. In both cases when N2 was adsorbed, the NN bond length increased from 1.12 Å to 1.35 Å, indicating the activation of N2. Both catalysts were also shown to have higher selectivity over HER. The PDS for both Fe and Cu was shown to be the hydrogenation step of NHCONH2* to NH2CONH2*, with limiting potentials of −0.63 V and −0.66 V, respectively.
Using a host–guest strategy, Zhang et al. synthesized Fe and Ni DACs (Fig. 8a–c).119 Experiments with individual Fe and Ni SACs found that NO3RR and CO2RR dominated, respectively, leading to low yield rates and FEs for urea. Isolated diatomic Fe–Ni pair (I-FeNi-DASC) showed improved results, showing much higher FEs of 82.5% for CO2RR and 7.9% for NO3RR, resulting in a yield rate of 10.7 mmol h−1 g−1 and FE of 3.8% for urea. On the other hand, bonded Fe–Ni (B-FiNi-DASC) showed far superior results, delivering a urea FE of 17.8% and a yield rate of 20.2 mmol h−1 g−1 at −1.5 V vs. RHE. DFT calculations were then done to identify the origin of activity. Electrons were mainly concentrated over Ni sites and electron-deficient Fe atoms served as the Lewis acidic sites to enhance the adsorption and activation of *NO, resulting in high urea FE and yield rate. Pan et al. compared single Pd1 and dual Pd1Cu1 atoms on TiO2 nanosheet for urea synthesis (Fig. 8f).129 As shown in Fig. 8g, DACs were shown to far outperform SACs, having a urea yield rate of 166.67 molurea molpd−1 h−1 with a FE of 22.54% at −0.5 V vs. RHE compared with that of SAC (urea yield rate of 29.36 molurea molpd−1 h−1, FE 3.79%). DFT study elucidated a synergistic effect of DAC on TiO2. Pd1Cu1 was electron-depleted, matching the electron-rich N atom in N2, while oxygen vacancies in TiO2 were electronegative, attracting CO2. The potential barrier to form *NCON was also much lower for DACs (−0.265 eV) compared with SACs (1.360 eV). Competitive NRR was also suppressed due to the barrier of *NCON formation being lower than that of *NNH (Fig. 8h).
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Fig. 8 (a) TEM image of FeNi DAC. (b) HAADF-STEM image with the FeNi DACs circled in red. (c) HAADF-STEM image profile intensity with atomic resolution EELS mapping of FeNi DAC. (d) FE comparisons of various catalysts in different reactions. (e) Free energy diagram of urea synthesis for FeNi DAC. Reproduced with permission.119 Copyright 2022, Springer Nature. (f) HAADF-STEM images of single Pd and dual PdCu catalysts on TiO2 with insets of their respective atomic structure. (g) Urea yield rate comparison of PdCu DAC and Pd SAC. (h) Free energy diagrams of NO3RR on Pd SAC and PdCu DAC. Reproduced with permission129 copyright 2023, Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim. |
Various starting precursor reactants were tested in theoretical studies and the best candidates were screened for each reaction. Zhang and Guo did a DFT study on the feasibility of using DACs to synthesize urea from CO2 and N2.130 Corrole was chosen as the base for its ability to modify catalytic activity by introducing different substituents at the median and β positions. The structure of V2N6C was found to have the best projected density of state with a d-band value of −0.40 eV, which showed the closest value to the Fermi level compared with other structures such as V2N4C. This improved interactions between catalyst and adsorbed molecules, enhancing catalyst activity. Competitive HER was also found to be inhibited, further increasing urea selectivity. In a continuation of this study, the authors published another paper studying heterogeneous DACs, with vanadium as one of the components (MVN6C).131 Nb was found to have the lowest d-band center closest to the Fermi level, making it the most catalytically active metal with a small limiting voltage of −0.37 V. Competitive HER on MVN6C catalyst was also found to have no effect on urea synthesis because the adsorption energy of hydrogen is weaker than that of CO2 and N2. Ren et al. explored the feasibility of urea formation from N2O and CO, both of which are toxic to human health and potent greenhouse gases.132 An entirely new mechanism for the reaction was proposed, where CO is directly inserted into *NN formed from the reduction of *N2O to form the key intermediate *NCON. TMs anchored on porous g-CN (TM2/g-CN) as DACs were screened. Cr2/g-CN, Fe2/g-CN and Co2/g-CN were identified to be the best TMs with high stability, activity and selectivity. Cr and Co presented low limiting potentials (−0.19 V and −0.15 V, respectively), while Fe presented the most efficient catalytic activity with no thermodynamic energy barriers. Competitive NRR and HER were found to be inhibited as well.
In a step away from the conventional use of transition metals as catalysts for urea synthesis, Roy et al. examined the usage of dual-Si-doped graphitic carbon nitride (g-C6N6) in urea synthesis from N2 and CO2.133 g-C6N6 is known to activate N2 easily. N2 is adsorbed onto dual Si via side-on configuration and then becomes activated. Subsequently CO2 is adsorbed onto the activated N2 and converted to CO via proton-coupled electron transfer. CO is then directly inserted into the activated N–N bond, essentially cleaving the N–N bond as charge is transferred from the nonbonding orbital of CO to antibonding N–N π* orbital. Competitive HER and NRR were found to be inhibited, as onset potentials for both reactions were higher than that of urea synthesis (−1.31 V, −0.92 V and −0.79 V, respectively).
In summary, SACs and DACs are able to improve the yield rate and FE of NRR, NO3RR, NO2RR, NORR and urea synthesis. For SAC:
(i) Synergistic effects between atomically dispersed catalyst and support lead to better activation of reactants – examples include Ru–S bond leading to a “push–push” effect where N2 is destabilised by two contributions and has better electrical conductivity.70
(ii) Easily tuneable local environment of atomic sites, leading to better optimisation of reaction. This can be observed in Fe SACs for NO3RR, where changing the temperature of pyrolysis results in different moieties – FeN3, Fe–N4–OH and FeN4, giving rise to different electrosynthesis performance.87
(iii) Better electronic properties that are more conducive for the various reactions. This is evident in the Fe-PPy SAC,86 where it has a more pronounced hybridisation between oxygen and Fe with overlapping electrons at antibonding orbitals.
(iv) Good stability over micro/nano materials, as seen in the case of Cu SAC on CeO2, where urea yield rate of CuO–CeO2 was found to rapidly decrease over a few cycles.127
(v) Lack of adjacent sites resulting in difficulty of N–N coupling, preventing N2 from forming and improving selectivity towards ammonia, as evident when Zn SAC was used in NO3RR91 and the novel BSAC proposed by Lv et al.101
For DAC:
(i) Reactants are better stabilised by multiple catalytic centers, resulting in better activation of reactants and lowering the desorption energy of products, which can be seen in the case of FeCu DACs for NRR42 and NO3RR.98
(ii) Synergistic effects between the two catalytic centers for urea synthesis: one site allows for efficient NO3RR while the other allows for CO2RR, enabling both reactions to occur simultaneously. Zhang et al. showcased this in their work with Fe–Ni DAC, where Fe dominated in NO3RR while Ni dominated in CO2RR and a bonded Fe–Ni DAC showed the most superior C–N coupling activity.119
(iii) The proximity at which the reactions take place makes it conducive for the intermediates to combine to form urea. This is apparent in the theoretical work done by Roy et al. in which *CO is inserted directly into the activated N2 to form urea.133
The FEs and yield rates of NH3 and urea synthesized via NRR, NO3RR, NO2RR, NORR and N–C coupling over various SACs and DACs are summarised in Table 1. The catalysts showed excellent FEs and high yield rates especially when normalised to the loading mass of catalytically active metals.
The topic of DAC for nitrate and nitrogen reduction can be further explored as it was already proved to be superior to SAC and nanoparticles in some cases due to its synergistic effects of having two atoms. For urea synthesis, theoretical works on it are lacking, let alone experimental. For theoretical works, more focus can be placed on exploring how the two atoms work synergistically to catalyse the reduction reaction more effectively. Investigation of the effects of homogeneous and heterogeneous DACs is another great direction to work on.
Catalyst mass loading can be further increased as well. Most works on SACs and DACs have a mass loading of <1%, with some as low as 0.15%.68 Only a few works have focused on increasing the mass loading to beyond 10%. A higher catalyst mass loading indicates a higher number of active sites, increasing product yield rate for the same amount of catalyst added.
The effects of various scaffolds for SACs and DACs upon which they are deposited on can be further investigated as well. Most SACs and DACs utilise N-doped carbon as scaffolding due to its great electrical conductivity and tunability. Other scaffolding such as chalcogenides, boron nitride, MXenes, MOFs and many others can be explored. Taking the example of chalcogenides, Zheng et al. showed that single transition metal atoms can achieve a high loading, with Fe reaching up to 10 wt% on transition metal chalcogenides (TMCs).134 Other substrates on which catalytic atoms are deposited may have other synergistic effects worth investigating as well. Li et al. conducted a study of Pt single atom on various supports, including Co3O4, CeO2, ZrO2 and graphene, and found that Pt on Co3O4 (Pt1/Co3O4) showed the best activity and stability in the dehydrogenation of ammonia borane.135
There could be attempts to increase the size of the atomic catalyst by synthesizing clusters of 3 or more atoms. When increasing the number of atoms, it also has the effect of increasing mass loading. A DFT study by Chen et al. postulated a possible 35.8 wt% of catalytic Fe3 on a stacked heterostructure of graphdiyne and graphene.136 In addition, considering the electrosynthesis of urea from CO2 and nitrogen oxides involves the coupling of two nitrogen and one carbon atoms, a triple-atom catalyst (TAC) may prove to have better adsorption than DACs.137 A TAC has been synthesized before for other functions: Ru3 synthesized for oxidation of alcohol, exhibiting 100% conversion and 100% efficiency.138 This proves the feasibility of the idea and the potential merit of synthesizing triple or larger atomic cluster catalysts.
Finally, there is a need for advancements on in operando/in situ techniques to observe the catalysts as the reaction occurs. It has already been proved that Cu SACs underwent structural changes from SAC to NP at a negative applied potential in NO3RR90 and urea synthesis.127 The real catalytic sites were therefore the clusters that formed under negative potentials, rather than the single-atom sites. Apart from operando XAS, other techniques such as operando TEM had been utilised to observe the structural changes of catalysts under reaction conditions.139
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