Tianxiang
Chen
ab,
Lin
Ye
*c and
Tsz Woon Benedict
Lo
*ab
aState Key Laboratory of Chemical Biology and Drug Discovery, Department of Applied Biology and Chemical Technology, The Hong Kong Polytechnic University, Hong Kong, China. E-mail: twblo@polyu.edu.hk
bThe Hong Kong Polytechnic University Shenzhen Research Institute, Shenzhen 519700, China
cDepartment of Chemistry and Shanghai Key Laboratory of Molecular Catalysis and Innovative Materials, Fudan University, Shanghai 200438, China. E-mail: yelin@fudan.edu.cn
First published on 7th June 2021
This article highlights some recent advances in the electronic and geometric structures of single-atom and nanocluster catalysts, which play an inevitably important role in modern catalysis. The combined use of modern characterisation techniques enables surface, solid-state and coordination chemists to develop more extensive, more cohesive and more appropriate frameworks to rationalise the structure–reactivity functions of these atomically dispersed entities, which further provides the necessary details for the identification of chemical trends and benchmark quantum sciences. We also offer an outlook on the challenges and opportunities of this research area.
The phenomenal cooperative actions between the electronic and geometric structures in many biological species shed light on the design of atomically precise metal-containing co-factors for catalysis. Due to the high surface-to-volume ratio, single-atoms (SAs) and multinuclear nanoclusters (NCs) are highly reactive and exhibit colloidal instability when compared to their bulk counterparts.4,5 Researchers have accordingly designed many SA and NC metal-containing inorganic compounds for highly chemo-, regio-, and enantio-selective catalytic processes.
The concept of supported SA and NC chemistry has been long discussed. The progress in the development of modern characterisation techniques, notably aberration-corrected scanning transmission electron microscopy (AC-STEM) and extended X-ray absorption fine structure (EXAFS) spectroscopy, has driven the recent blossom in the research of these materials, where these sub-nanometric species can be more reliably determined.
In 1999, Iwasawa et al. determined the structure of atomically dispersed Pt single-atoms on MgO by primarily employing EXAFS.6 In 2003, a simple cyanide leaching method was proposed by Stephanopoulos et al. for the synthesis of atomically dispersed single-atoms on metal oxide, where the single-atom Au,Pt/CeO2 catalysts exhibit much higher catalytic activity toward water-gas shift than Au and Pt nanoparticles.7 During the 1990s–2000s, the role of single-atoms in catalytic reactions was extensively discussed.8–13 Isolated Pd on Al2O3 and Ir on MgO have been observed by Lee14 and Gates15 by AC-STEM. Although Lee et al. proposed that ‘single-site catalysts’ can effectively promote the catalytic performance, the precise synthesis of well-defined ‘single-site catalysts’ is still a challenge to be extensively realised in a heterogeneous system. In 2011, Zhang et al. fabricated isolated Pt atoms on an FeOx support and further introduced the concept of ‘single-atom catalysis’ to describe the catalysis by SACs.16
As for NCs, Cotton first defined the term ‘metal atom cluster’ after investigating the chemistry of low-valent polynuclear rhenium halides of [Re3Cl12]3− in 1964.17,18 In the following decades, cluster chemistry has made substantial progress. Various transition metal clusters have emerged and exhibited remarkable catalytic potential.19–21 Among them, supported Cu NCs have received a lot of attention due to their potential in offering a practical solution for the utilisation of methane by selectively oxidising methane molecules to methanol.22–25 Microporous materials, such as zeolites and metal–organic frameworks, have been widely employed to encapsulate SAs and NCs thanks to the unique chemical functionality and framework confinement effect. However, to practically realise selective methane oxidation is extremely challenging primarily due to two reasons, (i) the high activation barrier to activate the non-polar C–H bond, and (ii) the difficulty in stabilising methanol at the intermediate step but not over-oxidising to yield CO2. Besides selective methane oxidation, Cu NCs have also been found useful in various catalytic applications. For example, Solomon et al. reported trinuclear Cu NCs in 1997 and revealed the role of trinuclear copper nanoclusters in the hydroperoxide reduction process.26 In 2003, Schoonheydt et al. reported bis(μ-oxo)dicopper species encapsulated in ZSM-5 zeolite for the decomposition of NO.27 Different zeolite topologies, such as Y and MOR, have also been used to host Cu NCs for catalytic applications.25,28,29
In general, there are two common and effective approaches for the fabrication of these atomically precise species, namely, (1) the conventional inorganic chemistry approach and (2) the solid-state chemistry approach.
Certainly, the inorganic chemistry approach (metal complexes) is well-established, where the electronic and geometric structures of the SAs and NCs can be finely tuned by elemental variation, nuclearity control and ligand design. Through the solid-state approach, SAs and NCs can also be prepared by immobilisation on the surface functionalities of various support materials.30,31 Recent advances in the design and fabrication of SAs and NCs have been focused on their stabilisation against sintering/leaching and achieving a high loading ratio. The successful immobilisation of these species over solid-state supports brings heterogeneous catalysis towards the molecular frontier and delivers substantial impact towards the catalysis and functional materials community. The surface free energy per metal atom increases significantly when the ensemble of nuclearity decreases from bulk to nanoparticles, to the NC and SA level. The high surface free energies from a lowered coordination make the supported SAs and NCs achieve higher chemical reactivity.32 In some cases, the assembly of surface metal atoms as NCs is essential to provide an optimal geometry for the activation of substrate molecules with the required surface bond formation.33
For these kinetically stable sub-nm species used in catalysis where their surface becomes more dominant, the properties of the chemical bonds on the surface can be altered because of various external microenvironmental factors.3,34 The bonding coordination, when compared to that in the bulk, is closely associated with local geometry that is affected by surface relaxation and reconstruction. The electronic properties at the surface can also differ substantially from that of the bulk. For example, the existence of a surface can induce additional electronic states or surface states.35 It should be noted that it is challenging to obtain precise atomic information about the local structure, leading to a general lack of understanding of the geometric properties and surface chemistry. Also, the asymmetric coordination to metal or ligand in a crystal can generate higher surface energetic facets that alter the local surface polarity in the structure.36,37
The support approach is a realistic alternative in offering extensive possibilities for the rational design and precise control of the electronic and geometric structures of SAs and NCs. The choice of support is critical; the support not only acts as physical carriers to immobilise SAs and NCs but also influences the electronic configurations and local geometric structures, as well as the molecular specificities through steric effects.32 Besides some open surface supports (e.g., TiO2 and MgO), micro/mesoporous supports (e.g., zeolites and metal–organic frameworks (MOFs)) can additionally provide a relatively inert framework to offer spatial properties.22,38–42
The advantages and disadvantages of using metal complexes (homogeneous) and solid-state materials (heterogeneous) for catalysis have long been discussed.35,43,44 However, a reliable characterisation of the atomically precise SAs and NCs over solid-state supports was difficult to achieve in the past due to technical limitations, in stark contrast to the more mature characterisation of inorganic metal complexes. The main limitation is that the local electronic and geometric environments of the metal sites (e.g., the coordination of the metal atom, the spatial structure of metal–ligand complexes, etc.) have not been well understood, which hinders the development of this class of highly promising solid-state materials. With the impetus in modern characterisation techniques, even single metal species can now be directly observed using suitable high-resolution electron microscopes.45,46 By combining with other advanced techniques, a more accurate and precise determination of the atomic and structural parameters can be achieved.16,47,48 Researchers can more confidently design sub-nm materials with highly precise atomicity based upon the crucial structural information.
With increasing attention to the atomically precise SAs and NCs with low nuclearity, this perspective article will primarily highlight some recent progress in the fundamental study of their electronic and geometric structures, and their corresponding influence on catalytic science.
The electronic structures are often elucidated and expressed in terms of density of states of specific metal sites, based upon simulations. Li et al. have compared the catalytic performance for CO oxidation with respect to the electronic structures of a series of d-metal SAs (Au, Rh, Pd, Co, Cu, Ru, and Ti) supported on iron oxide (FeOx) under the Langmuir–Hinshelwood mechanism.60 It has been found that the d-band centres of supported Pt, Rh, Pd and Ru SAs were shifted to higher energy when compared to the inactive supported Au SAs. Higher d-band metal centres render more empty d states and stronger adsorption interaction with the reaction substrates (CO and O2). Yang and co-workers have employed a similar approach to study the relationship between the electronic structures and catalytic activities of a series of SAs (Pd, Fe, Co, and Ni) supported on γ-Al2O3.61 Zheng et al. reported that the conversion of CO2 to CO is preferred over Au, Ag and Pd SA electrocatalysts as they can bind the COOH* intermediate strongly, but bind CO* weakly.62 Back et al. have predicted the electrochemical CO2 reduction reaction (eCO2RR) properties of a series of SAs on defective graphene based on theoretical calculations, where the electronic interactions between the d-orbital of the SAs and the p-orbital of graphene govern the density of states and hence the catalytic behaviours.63 Also, Li et al. have investigated the electronic structure–reactivity functions of a series of SA M–Nx moieties (M = Mn, Fe, Co, Ni, Cu) with respect to the eCO2RR.64 A volcano trend has been found between their catalytic activities toward CO formation and the nature of the transition metal in M–Nx sites, with Fe and Co at the top of the volcano. To correctly model the active sites under in operando conditions, operando X-ray absorption near edge structure spectroscopy was performed to study the changes in the metal oxidation state with electrochemical potential. The oxidation states of Co and Mn remained unchanged with potential, while Fe and Ni were partially reduced and Cu mostly reduced to Cu(0). M2+N4–H2O was identified as the most active centre in Fe–Nx and Co–Nx, while Ni1+N4 was predicted to be the most active one in Ni–Nx. The experimental activity and selectivity have been rationalised from the difference between the binding energies for CO2* and H* as a descriptor of selectivity toward CO.
The experimental measurements of the electronic structures of supported species have often relied on probing the oxidation states via a study of the metal binding energies. Wu et al. prepared a series of 3d-metal SAs supported on graphene oxide (Fe, Co, Ni and Cu).65 The electronic structures of these supported SAs were determined by X-ray absorption spectroscopy (XAS), where a charge transfer from the metal to oxygen (M–O bond formation) and the oxidation states of the isolated metal SAs Mδ+ within 0 < δ < 3 have been determined.
Besides oxidation states, the study of the electronic communication via redox hopping between neighbouring SAs can also offer critical information on the catalytic properties, where the extent of necessary electrons supplied can be probed. Xue et al. have employed voltammetric measurements to probe the redox hopping properties of a series of 3d-metal SAs (Fe, Co, Ni, Cu, and Zn) supported on UiO-66-NH2.66 It has been found that Cu2+ is the most active modifier that allows a rapid electron movement between neighbouring metal sites in the form of Cu2+/Cu+. It is consistent with their model eCO2RR reaction, which has been attributed to the enhanced redox hopping properties, in combination with optimum CO* binding, that facilitates multielectron (>2e−) products.
Bimetallic (or multimetallic) NCs particularly with well-defined alloy structures of noble metals, like Au–Ag, Au–Cd and Hg–Au, provide model examples for the influence of elemental composition and electronic structures on catalytic properties.67,68 The elemental variation effect has been commonly studied in colloidal species, such as Au25, where Zhu and co-workers utilised Au25(SR)18 (SR = SPhMe2) as a template to investigate this effect by employing the metal-exchange method.67 The doping effect has been investigated with a single foreign atom (Au, Pd, or Pt) in the core of an Ag25 NC on the catalytic properties, where the foreign atom is encapsulated by 24 Ag atoms (Au@Ag24, Pd@Ag24, Pt@Ag24) (see Fig. 2).69 It has been found that the catalytic performance in the carboxylation reaction of CO2 was influenced substantially due to the alternation in the electronic structures. Also, Kobayashi et al. systematically studied the electronic structures of three bimetallic Au–Ag NCs, namely Au12.2Ag2.8, Au14.4Ag3.6, and Au17.6Ag7.4.68 The optical spectroscopy results suggested that the electronic structures of Au NCs were modulated by the Ag heteroatoms.
Fig. 2 (a) ESI-MS and (b) UV/vis spectra of Ag@Ag24, Au@Ag24, Pd@Ag24, and Pt@Au24 clusters capped by thiolates. Inset: the structural framework of Au/Pd/Pt/Ag@Ag24. SR = SPhMe2; the SR moiety is omitted for clarity.67 Reprinted with permission from ref. 67. Copyright (2015) American Chemical Society. |
Yang and co-workers have employed first-principles calculations to probe the electronic structures of Con (n = 1–5) NCs supported on γ-Al2O3 (100) and (110) surfaces (see Fig. 3),74 and Pdn (n = 1–5) NCs supported on rutile TiO2 (100), (001) and (110) surfaces.75 It has been found that the stability of the NCs varies as a function of nuclearity and surface support, as the surface binding preferences and nucleation energies of the NCs are notably different. Based upon charge analysis, both metal clusters and support are critical in the charge state of the NCs. The charge of the NCs is highly dependent on the balance between the preferential binding to the surface atoms. The density of states of Pdn/TiO2 revealed that the 4d orbitals of Pd are close to the Fermi level in some cases (such as Pd4/TiO2 and Pd5/TiO2), which can be correlated with catalytic activity.
Fig. 3 Nucleation energies Enuc of Con clusters in the gas phase and on the dehydrated (100) and hydrated (110) surfaces.74 Reproduced from ref. 74 with permission from The Royal Society of Chemistry. |
Yao et al. have engineered the electronic structures of Ru SAs on a series of PtCu alloys via compressive strain to boost the electrocatalytic oxygen evolution reaction.79 A volcano relation has been reported between the catalytic activity and the lattice constant of the PtCu alloys. According to density functional theory calculations, the compressive strain of the outer Pt shell can influence the electronic structures of the Ru SAs, which optimises the binding strengths of oxygen species. As discussed, Yang and co-workers have shown that the electronic structures of Co3 on dehydrated γ-Al2O3 (100) and hydrated γ-Al2O3 (110) surfaces are notably different (see Fig. 4).74
Fig. 4 Electron density difference maps (isovalue = 0.04) for the Co3 cluster adsorbed on the (a) dehydrated γ-Al2O3 (100) surface and (b) hydrated γ-Al2O3 (110) surface. The charge depletion and accumulation regions are shown in blue and yellow, respectively.74 Reproduced from ref. 74 with permission from The Royal Society of Chemistry. |
The systematic study of the ligand effect of d-metal complexes is undeniably more mature than that of supported SAs and NCs. Desnoyer et al. systematically studied the electronic structures of a series of square planar d10 Ni diphosphine π-complexes that vary as a function of the degree of π-backbonding of alkene or carbonyl-containing π-ligand.80 The degree of π-backbonding has been quantitatively correlated between J-coupling (from nuclear magnetic resonance (NMR)) and the binding energy of Ni (from the 1s → 4pz pre-edge in Ni K-edge X-ray absorption spectroscopy (XAS)), which is determined by the energy of the π* ligand acceptor orbital (see Fig. 5). In addition, He et al. have also utilised the binding energy of Ni (Ni L-edge XAS) to quantify the degree of π-backbonding in a series of Ni diphosphine π-complexes.81
Fig. 5 Calculated Ni K-edge XAS time dependent-DFT results for the pre-edge region of the spectrum. Each complex is represented by a blue circle (Ni 4pz ← 1s) and a red circle (Ni 3dx2−y2 ← 1s). The area of each circle is proportional to the calculated oscillator strength (fosc) for each transition. All calculated time dependent-DFT energies at the Ni K-edge were shifted by −98.55 eV.80 Reproduced from ref. 80 with permission from Wiley, copyright 2019. |
The influence of ligands on the electronic structures of d-metal inorganic NC complexes has been shown to be similar to those of traditional d-metal complexes. In recent work by Cirri et al., the electronic structures of precise Au NCs with different ligands, namely Au9(P(p-X–Ph)3)83+ and Au8(P(p-X–Ph)3)72+, where X is –H, –CH3, or –OCH3, at the para position, have been elucidated.82 The electronic structures have been computed to generalise the unique observation from the mass-selective UV/visible absorption spectra. Using chemical derivatisation, the electronic structures of these complexes are related to the electron-donating or -withdrawing strength of the ligands. Wan et al. have also investigated the ligand effect in catalysis over Au38 NCs with different ligands.83
In brief, the ligands can affect the electronic structures of the NCs from two major perspectives, (1) by the manipulation of the energies of the ligand orbitals (which dominates the metal-to-ligand charge transfer transitions), and (2) by the redistribution of charge density in the NCs (which controls transitions local to the metal core). However, the surface coordination species (or ‘ligand’) in supported SAs and NCs are more difficult to probe accurately and precisely due to a lack of appropriate techniques from the atomic perspective.
There are also many multinuclear NC systems; for instance, Zhang et al. reported a series of related binuclear Cu2 complexes to mimic carboxylesterase.104 The Cu–Cu interatomic distance was determined to be ca. 3.0 Å, which agrees with the typical M–M interatomic distances in most multinuclear NC enzymes. Also, Jiang and co-workers have reported binuclear Cu2 complexes as carboxylesterase mimics which employed an alkoxo/acetato-bridged moiety as a model to promote the hydrolytic cleavage of p-nitrophenyl picolinate.105,106 Beloglazkina et al. synthesised a mixed-valence Cu complex with a tridentate N2S type organic ligand as an N2O reductase mimic, where it is often regarded as a mimic model for N2O reductase.107 Generally, the geometric structures about the metal-containing active sites can be readily elucidated by a combination of single-crystal XRD and spectroscopic techniques (NMR and electron paramagnetic resonance (EPR)).108,109 The prosperous development of this research area has benignly guided the design of the solid-state counterpart.
Here are many studies on the precise design of supported SAs and NCs in recent years. Notable zeolite-support examples include the trinuclear [Cu3(μ-O)3]2+ NC supported on MOR zeolite that exhibits a high reactivity towards C–H activation of methane (that mimics methane monooxygenase) by Lercher et al.22 The structure of the NC was determined by combined XAS analysis and density functional theory (DFT) calculation. The [Cu3(μ-O)3]2+ NC is stabilised by two anionic centres at the entrance of the MOR side pocket. It is proposed that the C–H activation can be facilitated by the unique atomic arrangement of the extra-framework O atoms directed towards the main MOR channel. Tsang et al. have also employed zeolite (MFI type) to host a nucleophilic ‘Zn–OH’ on the negatively charged framework (see Fig. 6), where the Zn/ZSM-5 catalyst was highly active for the catalytic conversion of γ-valerolactone to p-xylene.110 The atomic parameters were determined by combined XAS and synchrotron X-ray powder XRD (SXRD). The formation of the framework ‘Zn–OH’ site has been found to be responsible for the selective decarboxylation of the lactone group to butene through a new hydrolysis pathway, while the adjacent Brønsted acid sites can catalyse the subsequent dimerisation to yield aromatic products. The structure and basic pathway of nucleophilic attack at the terminal Zn–OH site are comparable to those of Zn-containing enzymes in biological systems.110
Fig. 6 The refined structures of the Zn/ZSM-5 catalyst derived from SXRD and refinements. (a) Zn/ZSM-5; (b) gamma-valerolactone (GVL) adsorbed on Zn/ZSM-5; (c) a close-up view of Zn-2-OH interacting with the carbonyl of GVL; (d) a published crystal structure showing a complex intermediate of Zn–OH of T199A-CA II enzyme with adsorbed CO2 for comparison (PDB: 1CAM) with permission for reproduction.110 Ball-and-stick model: O = red, Si = grey, Al = green, Zn = blue, and C = black. Reproduced from ref. 110 with permission from Wiley, copyright 2017. |
Recent MOF-supported examples include the binuclear Cu2 co-factor in a Ti-MOF (MIL-125, in the form of Ti8–Cu2; see Fig. 7) as an efficient artificial monooxygenase by Lin et al.111 It was found that the Cu2 site in Ti8–Cu2 exhibits much higher stability than the mononuclear Cu1 analogue (Ti8–Cu1), which has been attributed to the much promoted catalytic activities to a range of mono-oxidation reactions, such as epoxidation, hydroxylation, Baeyer–Villiger oxidation, and sulphoxidation. Zr-based MOF-808 was employed to post-synthetically install imidazole-based ligand units for subsequent Cu(I)-metalation. The Cu atoms were found coordinated to N atoms from imidazole and O2 to form N–Cu2O2–N species, and the interatomic distance between the Cu sites was found at a distance of 2.51 Å with a coordination number of 0.6 (assigned as bis(μ-oxo) dicopper species). Extra-framework binuclear Fe2 species have also been successfully incorporated into a Zr-based MOF by a post-synthetic exchange method by Ott et al.112 The catalyst has high structural similarities to the active site of [FeFe]-hydrogenase. From combined single-crystal XRD and XAS analysis, the Fe centres occupy a distorted octahedral geometry with three C atoms from carbonyl groups and two S atoms bridging the binuclear Fe2 centre at bond distances of 1.796–1.814 and 2.283–2.285 Å, respectively. A similar post-synthetic metalation approach has been reported by Bien et al. to generate Zn–OH within a Zn-based MOF, CFA-1.113 The Zn–OH site can promote trace CO2 capture due to the CO2/HCO3− chemisorption mechanism and cooperative intercluster H-bonding interactions, which is similar to the secondary coordination sphere interactions in α-carbonic anhydrases.
Fig. 7 Cu2 active sites with O2 bonding in (a) the natural enzyme tyrosinase (PDB code: 1WX2) and (b) the MOF-based artificial enzyme Ti8–Cu2.111 Reprinted with permission from ref. 111. Copyright (2021) American Chemical Society. |
Besides porous materials, the catalytic properties of SAs and NCs can also be modified by interactions with open-surface supports from the modulation of the geometric structures. The syntheses of SAs and NCs on g-C3N4 (ref. 114–116), porous SiO2 (ref. 117 and 118) and carbon-based materials119–122 have been shown to offer exciting catalytic performance in many reports. However, it has been challenging to systematically elucidate the geometric structures due to the lack of appropriate characterisation techniques, which hence hinders the establishment of structure–activity relationships.
Comprehensive elucidation of the electronic/geometric structures of SAs and NCs is key to studying their electronic/geometric structure–activity relationships. Various advanced techniques have been developed for the elucidation of the physical characteristics of SAs and NCs, such as high-resolution transmission electron microscopy (HRTEM), AC-STEM, CO-absorbed Fourier-transform infrared spectroscopy (CO-IR), XAS, X-ray photoelectron spectroscopy (XPS), ultraviolet-visible spectroscopy (UV-vis), and SXRD as well as DFT calculation, as summarised in Table 1.
Items | Characterisation contents | Examples | Ref. |
---|---|---|---|
HRTEM | Atomic dispersion | Pt clusters/γ-Al2O3, Pt/FeOx | 16 and 125 |
AC-STEM | Metal particle size distribution | Pt@MCM-22, 0.2 Pt/m-Al2O3 | 20 and 126 |
CO-IR | Surface properties | Pt/MFI, Pt/CeO2 | 127 and 128 |
XAS | Oxidation state, bond length, and average coordination numbers | Pt/θ-Al2O3, Pt1δ+/TiO2 | 47 and 129 |
XPS | Chemical and compositional properties of metal species | Pt1@Fe–N–C, Pt@PCM | 130 and 131 |
UV-vis | Geometric structure | Cu2(μ-O)2/MFI, [Cu3(μ-O)3]2+/MOR | 28 and 132 |
SXRD | Atomic and crystallographic information | Cu/UiO-66-NH2, Zn/MFI | 66 and 110 |
DFT | Binding nature to the supports, adsorption properties, and reaction energetics | pfSAC-Fe, PtSn/MFI | 133 and 134 |
From the extensive collection of studies, it can be seen that the catalytic properties are highly dependent on the electronic and geometric structures of the NCs. On the one hand, the electronic structures are highly related to four key parameters, namely elemental variation, nuclearity control, metal–support interaction, and ligand coordination. They all affect the electronic structures by influencing the HOMO–LUMO work functions that ultimately influence the thermodynamics when the NCs interact with incoming reaction substrates. On the other hand, the geometric structures, as extensively illustrated in multiple examples from metal complexes, enzymes, and over different supported materials, play pivotal roles in providing suitable adsorption configurations and stabilising particular reaction intermediates, as well as affecting the kinetics of catalytic reactions.
We anticipate that the precise synthesis of multi-metallic multinuclear NC active sites with tuneable electronic and geometric structures will be a key future research direction that shares significant coherence with the SA systems. By taking advantage of the synergistic effect between the neighbouring metal nuclei, many long-standing challenges that require the use of more than one catalytic centre can be tackled. For instance, multinuclear NCs can be highly effective catalysts in cross-coupling reactions, due to the presence of multiple neighbouring metal nuclei where reaction substrates can be co-adsorbed for the subsequent co-activation. However, it is important to first fill the critical knowledge gap of the difficulty in the atomic design of solid-state catalysts for the control of the structure sensitivity of catalytic reactions.
Although it is well known that the traditional inorganic chemistry approach can enable the precise synthesis of multinuclear complexes, as far as we are aware, directly preparing well-defined NCs on solid-state support materials is inevitably more challenging. This is due to various intrinsic limitations, such as direct metal aggregation and the combination of metal species and multi-basic species that often yield various reticular products.
On the other hand, the characterisation of the electronic and geometric structures will be essential where it is important for the understanding of the structure–reactivity functions. For the elucidation of the supported SAs and NCs, a combination of techniques will be required, depending on the nature of the materials. For instance, for SAs and NCs supported on amorphous materials (such as graphene oxide and amorphous carbon), electron microscopy and XAS have been the two primary techniques to reveal the microenvironment. The lack of long-range order hinders the use of whole-pattern analysis of XRD data to reveal the crystal structure due to the absence of a crystalline phase. In contrast, high-resolution powder XRD can be used to offer essential crystal information of SAs and NCs supported on crystalline support materials (such as zeolites and MOFs). Synchrotron-based XAS and powder XRD techniques, alongside other spectroscopic techniques such as solid-state NMR and EPR, can be combined to determine the coordination information and to elucidate the atomic parameters of supported SAs and NCs. Meanwhile, the Rietveld refinement of powder XRD data can be used to obtain the atomic parameters (to derive the bonding information around the metal sites hereafter), and XAS can provide direct coordination information. We hope that, in the near future, a combination of different in situ/operando synchrotron-based techniques will be applied to further elucidate the structure–reactivity functions, which will consequently make the preparation of more superior SA and NC catalysts more sophisticated and rational. Finally, we provide an outlook of several possible methods based upon our experience that could be effective in the preparation of atomically precise supported NCs where their electronic and geometric structures can be carefully engineered.
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