Heterogeneous Catalysts. Группа авторов

Heterogeneous Catalysts - Группа авторов


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important and often undervalued method for purification of chemical compounds because it works on the molecular recognition principle whereby only specific species, typical of the growing crystal, are incorporated into the growing lattice with impurities staying in solution. In some favorable cases, chemical synthesis of metal clusters can be scaled up to tens of grams of the product, which is a lot for the lab‐scale synthesis of such materials and hugely more than UHV techniques discussed earlier could produce [37, 38].

Structures of Au8 (left), Au9 (middle), and Au11 (right) in space‐filled (top) and ball‐and‐stick visualizations with isolated cluster cores shown in the bottom row.

      Source: Anderson et al. 2013 [39]. PCCP Owner Societies. CC BY 3.0

      . (See online version for color figure).

      It is worth highlighting how well the ligands can protect cluster metal cores, which are barely visible in the “space‐filled” (top row, Figure 5.4) structures – remember this for the discussion of catalyst activation later in the chapter.

      If a mixture of clusters is obtained during the synthesis, the individual components of the mixture can sometimes be separated using chromatography [40]. If sufficient quantities of each individual cluster can be separated and collected, attempts to crystallize each cluster can be made (in order to resolve their structures using X‐ray crystallography). However, if crystallization fails, high‐resolution mass spectrometry can also be used to confirm the identity of the atomically precise clusters in conjunction with modeling of the expected exact mass of each cluster, as well as the corresponding isotopic and fragmentation patterns [40].

Catalytic results of the partial oxidation of styrene using O2 alone for supported Au55 and comparison catalysts prepared by various techniques.

      Clusters are atomically precise species (definitely in the light of the original definition by Cotton), while colloids have particle size distributions (i.e. particles with different sizes are present in a mixture). Clusters have metal core sizes ranging from two to hundreds of atoms, with sizes of larger clusters typically sub‐3 nm. A famous example of the large cluster with solved crystallographic structure is Au102 [42]. While colloids can have sizes just below 3 nm, most of the time their particle sizes are greater and can be as large as hundreds of nanometers. Ultrasmall colloids with narrow particle size distribution are often called clusters in the literature [43]. The reason to bring up this similarity is that two prominent examples of colloids were assigned cluster‐like formulas – Au55 and Au101 [44, 45] – whereas direct imaging by high‐resolution transmission electron microscopy (TEM) confirmed the existence of a particle size distribution [46]. Such species proved impossible to crystallize or to confirm their identity by high‐resolution mass spectrometry, but, although they are not truly atomically precise, they constitute an important complementary example of cluster‐like colloids.

      The stability of classical organometallic complexes with one central atom is often explained based on the 18‐electron rule (think octet rule based on 2 + 6 electrons to fill s‐ and p‐orbitals, plus 10 electrons to fill d‐orbitals of the transition metal central atom). Similar electron‐counting rules such as effective atomic number rule (e.g. average of 18 electrons per metal atom in clusters) or Wade's rules (a better fit for delocalized bonding model) were successfully applied to relatively small metal carbonyl clusters [24]. The “magic‐number” concept was popular for rationalization of the high stability of some larger clusters. The idea behind such “magic numbers” is that closed‐shell, highly symmetric structures have a low free energy per atom. For example, Mackay icosahedra are uniquely defined by the number of closed shells around the initial central atom, with the total number of atoms per cluster with increase in number of shells being N = 13, 55, 147, 309, 561, 923, 1415, 2057, 2869, 3871, etc. The abovementioned assignment of the formula Au55 to a synthetically made gold cluster was inspired by this concept [44]. A very recent study demonstrated that, for larger (100+ atoms) cluster sizes, oscillation occurs with respect to the most stable structure between icosahedra, decahedra, and face‐centered cubic (typical for bulk gold) structures [47]. An important recent development was recently proposed – a unified view of ligand‐protected gold clusters as superatom complexes [48]. In this approach, exceptional stability is assigned to systems with electron counts corresponding to filling of shells (n = 2, 8, 18, 34, 58, 92, 138, etc.) and takes into account interactions of the cluster core and ligands. It was successfully applied to explain the stability of a wide range of clusters, including that of Au102 mentioned above [42, 48].

      However, care must be taken not to assign observed activity to intact clusters as the results of a recent study show that “very small gold clusters (3 to 10 atoms) formed from conventional gold salts and complexes can catalyze various organic reactions at room temperature, even when present at concentrations of parts per billion” and that such clusters formed, in situ, “give reaction turnover numbers of 107


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