Open Access Article
Yan-Li Gao
*,
Shiqing Bi,
Yufei Wang,
Jian Li,
Ting Su and
Xuchun Gao
School of Chemistry and Chemical Engineering, Yulin University, Yulin 719000, China. E-mail: gaoyanli8503@126.com
First published on 7th April 2022
We report the synthesis and crystal structure of novel co-ligand phosphine/alkynyl protected Au nanoclusters, with composition [Au11(PPh3)8(C
CPh–CF3)2](SbF6) (1). The gold atoms in the cluster as a capped crown structure subtend C3v symmetry with one deriving from a central icosahedron and 10 peripheral Au atoms, and all alkynides are exclusively σ coordination bonding. The mean core diameter is about 5.1 Å and the overall van der Waals diameter can be estimated to be 20.5 Å. The optical absorbance of 1 in solution reveals characteristic peaks at 384 and 426 nm and a shoulder between 450 and 550 nm.
The pioneering work of ([Au11(PPh3)7](SCN)3) can be traced back to Malatesta et al. in 1966, but the structure could not be accurately defined at that time.24,25 Subsequently, a series of smaller phosphine-capped gold clusters with nuclearity of 5–13 were synthesized and structurally characterized.26,27 Mingos et al. then predicted the complete icosahedral Au13 structure and later achieved it experimentally.28 Thereafter, major interests in ligand-coordinated gold clusters moved to heterometallic, higher-nuclearity, and thiolate-capped families.29–32 Schmid et al. reported the Au55 cluster, but its insufficient solubility precluded crystallization and mass spectrometry confirmation of the Au55(PPh3)12Cl6 formula, but no crystal structure has been attained to date.33
In addition to the habitual thiolate and phosphine ligands, alkynyl-protected nanoclusters often exhibit highly regular structures and typical coordination motifs forming fascinating assemblies exploiting this versatile coordination.34–39 Metallophilic interactions are often an important driving force for the formation of large clusters. Their structural features were exemplified in a series nanoclusters and intermetallic with interesting alkynyl-Au staple motifs,40–44 which resemble thiolate-protected Au nanoclusters.45–51 Gold complexes exhibit very simple coordination modes of the alkynyl ligands, dominated by two, the simple μ2-η1 end-on and the bridging μ2-η1η2 mode. That means the bonding of alkynyl ligands with golds can form σ coordination bond as well as π coordination bond, which is unlike thiol ligands, resulting the coordination mode very rich.
Recently, co-ligands have been used to endow metal nanomaterials with better performance than either of single ligand systems. However, in sharp contrast to the well-studied pure-ligand–metal interface, it remains an unsettled front for today's characterization techniques to fully identify the detailed binding structures in mixed-ligand metal nanomaterial systems, as they often lead to highly complicated surface structures or dynamic ligand arrangements.52–54
Herein, we report the preparation and structure determination of hybrid ligands protected gold nanocluster with the composition of [Au11(PPh3)8(C
CPh–CF3)2](SbF6) (1). The Au-skeleton have C3v symmetry of icosahedron that have one centered and 10 peripheral Au atoms. It is present in the conventional Au11(PAr3) clusters for various combinations of phosphine, sub-ligands and counter anion.55,56 And unlike in the other gold system for this undecagold cluster all alkynides are exclusively in their μ1-η1-end-on coordination mode.
CPh–CF3)2](SbF6) was synthesized by NaBH4 reduction of PPh3AuCl and RC
CAu with SbF6 anion in methanol. After reduction and centrifugation, the dark brown residue was dried up to afford brown solid. Further crystallization from dichloromethane/hexane led to the formation of black rod-shaped crystals.
The single-crystal X-ray analysis revealed that [Au11(PPh3)8(C
CPh-CF3)2](SbF6) crystallizes in the triclinic space group P-1 with two formula units (Table S1†). The unit cell parameters as follows: a = 16.0672 Å, b = 17.0707 Å, c = 32.9552 Å; α = 80.8164°, β = 82.7276°, γ = 63.1499°. The packing structure of 1 is shown in Fig. S1† with two molecules in one unit cell. The molecular structure of 1 is shown in Fig. 1 comprising eleven Au atoms, eight PPh3 and two RC
C ligands, and one SbF6− anion. The structure of the coordination polyhedron formed by the Au atoms possesses the local symmetry C3 (3) and approximately C3v (3m) derived from a centered icosahedron.57,58 This geometry can also be viewed as a capped crown,59 which is also found for Au10 clusters.60 The Au11 core has one central and ten peripheral Au atoms. The Au11 core units can be described as capped chairs (icosahedron derivatives). Eight surface Au atoms are coordinated by triphenylphosphine ligand and the other two Au atoms bind to alkynyl ligand. The alkynyl ligands coordinate with Au atoms are in the μ1-η1-end-on coordination mode, which is unlike in most undecagold species (μ2-η1η2 mode).
The gold cluster core geometry is similar to the one found in Au11(PAr3)7X3 (X = halide or pseudohalide). The structure is compared to [Au11(PPh3)7Cl3](2).58 The substitution pattern of the bulky alkynyl groups and the small halides is different, which has an influence on the Au–Au bond lengths and angles. As observed for most centered Au clusters, the radial Au–Au bond lengths of [2.6273(8)–2.7279(7) Å] in 1 but [2.6079(7)–2.7044(7) Å] in 2, are significantly shorter than the peripheral bond lengths [2.8062(8)–3.3125(9) Å] (Table S2†), which is [2.84504(7)–2.9677(7) Å] in 2. The center-to-peripheral radial bond distances are shorter than the peripheral bond distances, indicating the crucial contribution of radial bonding to the stability of cluster skeleton, as observed before. Its mean bond length of 2.7934 Å. The minimal length of 2.6273(8) Å is short for gold clusters while the maximal length of 3.3125(11) Å is quite large.
The mean core diameter is about 5.1 Å (minimal 4.7 Å, maximal 5.4 Å), which was measured between the centers of the Au atoms of opposite sides of the cluster. And the overall van der Waals diameter could be estimated to 20.5 Å which is deduced from measuring the distance between the hydrogen atoms at opposite sides of the cluster (center to center) and the addition of 2.5 Å for the van der Waals radii of the hydrogen atoms. They are all bigger than cluster 2, which respectively is 4.9 Å, 4.7 Å and 5.3 Å.
In addition, the length of the Au–P bond are from 2.271(3) to 2.305(3) Å in ungecaglod cluster and the mean bond length is 2.287 Å, while the Au–C bond lengths are 1.982(15) Å and 2.026(18) Å respectively. These are in good agreement with those gold clusters in general. The coordination geometries of Au(core)–Au–L (L = P, C) are almost linear, that the angles are from 170.7(1)° to 178.9(5)°. The angle of Au(4)–Au(1)–Au(7) is 125.02(3)° (The Au atom refers to the atom that connected to the alkynyl group, Table S2†).
The sample was further characterized by a ESI-MS spectrometer with an electrospray ionization source under positive mode in CH2Cl2 (Fig. 2). The spectrum is quite clean, with the molecular ion peak [Au11(PPh3)8(C
CPh–CF3)2]+ at m/z = 4602.4 being dominant. Perfect agreement was observed between the experimental spectrum and simulated isotopic distribution pattern. 8 of the 11 gold atoms should have a valence of zero in order to fulfill the requirement of charge balance. According to the superatom theory, 8 electrons available for cluster bonding a shell closing within the jellium model is plausible (1s and 2p state), leading to an electronically stable compound, which is corresponding to mass spectrum.
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| Fig. 2 ESI-MS spectrum of 1 crystals dissolved in CH2Cl2. Inset: the experimental (black trace) and simulated (red trace) isotopic patterns of molecular ion peak. | ||
The optical absorbance of the dilute solution is easily to obtain and provides first information on the quality of product. Specifically, the size dispersity of the nanoparticles plays a significant role, because the spectrum of molecular clusters shows obvious characteristics, which are sensitive to the number of metal atoms, charge and conformation of the core, whereas the spectrum of metallic colloids (>2 nm) possesses feature and broad inter band and plasmon bands. Fig. 3 presents the UV-vis absorption spectrum of 1 in CH2Cl2. The spectrum exhibits an intense absorption band at 426 nm which corresponds to water-soluble undecagold and characteristic of phosphine-stabilized undecagold. Apart from the 426 nm band, there are an intense absorption at 384 nm and a broad absorption of the peak between 450 and 550 nm. This absorption feature at 384 nm should arise from the [Au11(PPh3)8(C
CPh–CF3)2]+ cation, as revealed in the crystal structureFig. 3.
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| Fig. 3 UV/Vis absorbance spectra of 1 in CH2Cl2. Peaks at 384 and 426 nm and a shoulder between 450 and 550 nm confirm the molecular character. Inset: spectrum with a photon energy scale. | ||
The NMR spectrum recorded in CDCl3 revealed both only one singlet at δ = 63.29 ppm for 19F and 52.32 ppm for 31P{1H}Fig. 4, although discrimination between three chemically in equivalent positions of phosphorus atoms is possible in the solid structure of 1. The observation of only one singlet show that the cluster is dynamic in solution as frequently observed in cluster science, leading to a lower number of signals than expected from the solid-state structure.5
CPh–CF3)2](SbF6) (1)
CAu were dissolved in 3 mL toluene. To the solution 5 mg NaSbF6 in 0.5 mL ethanol was added. The solution was stirred for 10 min. After that, a freshly-prepared NaBH4 solution in methanol (1 mg mL−1) was dropwise added. The solution turns from pale brown to finally dark brown. The reaction continued for 24 h in the dark. It was centrifuged for 2 min at 14
000 rpm. The solution was then dried up to afford brown solid. The solid was thoroughly washed with hexane and ether. 2 mL of dichloromethane was finally used to dissolve the raw product. After filtering, the solution was subjected to the diffusion of hexane in the dark. Black rod crystals were obtained after 4 weeks in a yield of ∼36.2% (based on Au).
CPh–CF3)2](SbF6) using an Agilent Technologies SuperNova system. X-ray single-crystal diffractometer using Cu Kα (λ = 1.54184 Å) at 100 K. The data were processed using CrysAlisPro.61 The structure was solved and refined using Full-matrix least-squares based on F2 using ShelXT,62 ShelXL63 in Olex2 (ref. 64) and Shelxle.65 Almost all hydrogen atoms were located from difference Fourier maps and those not found were added at theoretical positions using the riding model. Further details can be obtained from the cif files deposited at the Cambridge Crystallographic Data Centre. The CCDC reference number is 2127378. The thermal elipsoids of the ORTEP diagram at 50% probability is shown in Fig. S2.† Detailed crystal data and structure refinements are summarized in Table S1.†
CPh–CF3)2](SbF6) that was obtained from the reduction of PPh3AuCl and CF3PhC
CAu with NaBH4 in methanol. The crystal structure crystallizes in triclinic P-1 space group with the same almost C3v symmetric constitution. In the molecular structure, the coordination polyhedron of the gold atoms derived from a centered icosahedron, and unlike in the other gold system two alkynides are exclusively in their μ1-η1 coordination mode for this undecagold cluster. The Au–Au distances with a mean value of 2.7934 Å are in good agreement with those gold clusters in general. The optical absorbance of a solution of 1 reveals several features that are characteristic of gold cluster molecules. In accordance with the literature, only one singlet in the 31P{1H} NMR spectrum is found.
Since the composition of 1 represents a missing link in undecagold cluster chemistry, these findings close this important gap and are considered to promote scientific progress in the understanding of molecular precision synthesis, functionalization of gold nanoparticles and their electronic structure.
Footnote |
| † Electronic supplementary information (ESI) available: The experimental section, structure information in detail and additional NMR data. CCDC 2127378. For ESI and crystallographic data in CIF or other electronic format see https://doi.org/10.1039/d2ra01080a |
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