Kirill
Monakhov
Leibniz Institute of Surface Engineering (IOM), Permoserstraße 15, Leipzig 04318, Germany. E-mail: kirill.monakhov@iom-leipzig.de
First published on 18th December 2024
Gold and atomically precise polyoxometalates (POMs) are widely used materials with electron reservoir redox properties. The combination of optically excited gold nanoparticles, gold surface/tip electrodes, or molecular gold(I) complexes with {VV6} Lindqvist-, {MnMoVI6} Anderson-Evans-, and {PWVI12} Keggin-type POM structures leads to interfacial multielectron transformations with far-reaching implications for electronics, photonics, biomedical diagnostics, and catalysis.
Gold in compounds has two main oxidation states (+I and +III), can be easily converted into gold(0) nanoparticles (AuNPs) of different sizes and morphologies (e.g., nanorods and nanoclusters) and, thus, exhibit different optical and electronic properties. AuNPs can be obtained by a conventional citrate reduction method or solid-state dewetting with Ar+ bombardment to control the oxidation state of gold.2 When AuNPs are capped with electron acceptor agents (or so-called electron sponges), these engineered gold–sample interfaces can lead to plasmon-induced charge transfer triggered by an external stimulus such as light irradiation.3
The latest study showed8 that attachment of H3PW12O40 to the surface of AuNPs under UV light leads to the transfer and storage of hot electrons in these Kegging-type POM structures (Fig. 1A). Such hybrid ensembles with donor–acceptor interactions hold great potential for the development of experimental prototype devices with the underlying charge separation, recombination dynamics, and redox switching mechanisms. Their wavelength-selective photon-electron control could be used for future practical applications in osmotic energy conversion, photocatalysis, optical multiplexed bioassays, and opto-electronic transducers.
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Fig. 1 (A) Optically activated AuNPs (35 nm) act as electron donors for POM acids H3PW12O40 ({PW12}), which behave as electron acceptors in POM-based plasmonic electron sponge membranes. (B) A single-POM junction [MnMo6O18{(OCH2)3CC5H4N}2]3− in the four-electrode configuration immersed in the ionic liquid BMIM-OTf. 1 is the POM junction. WE is a working electrode (Au substrate), CE is a counter electrode (Pt), and RE is a reference electrode (Pt). (C) Anderson-Evans-type POMs [MnMo6O18{(OCH2)3CNH2}2]3− ({MnMo6}) bis-functionalized with monovalent Au3(carbene)3, Au2(carbene)2, and Au(carbene) moieties. Color code: Au = yellow; Mo = green; Mn = brown; O = red; N = blue; C = gray and light blue. (D) STM image of a sample obtained by drop-casting of CH2Cl2 solution of a Lindqvist-type hexavanadate ({V6}) bis-functionalized with monovalent Au(phosphine) moieties and coordinative S-termini on the Au(111) surface. The heterometallic dianion was synthesized from a [V6O13{(OCH2)3CCH2N3}2]2− precursor ({V6}) via Cu(I)-catalyzed alkyne–azide cycloaddition. For (A)–(D) H atoms and counterions are omitted for clarity. Reproduced/adapted from ref. 8 (A, copyright Springer Nature), ref. 9 (B, copyright Wiley), ref. 10 (C, copyright Wiley), and ref. 14 (D, copyright RSC). |
Gold–POM interfaces with multielectron transformation processes were also observed9 under electrochemical control by incorporating a tris(tetrabutylammonium) salt of the pyridyl-terminated Anderson-Evans-type POM [MnMo6O18{(OCH2)3CC5H4N}2]3− as a single-molecule junction in a four-electrode cell configuration (Fig. 1B). Electrochemical scanning tunneling microscopy (EC-STM) measurements were performed in the ionic liquid 1-butyl-3-methylimidazolium trifluoromethanesulfonate (BMIM-OTf). The results showed that this redox-active POM exhibits the behavior of a three-state electrochemical transistor.
Chemical post-functionalization of the related amine-terminated POM [MnMo6O18{(OCH2)3CNH2}2]3− with N-heterocyclic carbene (NHC) gold(I) complexes resulted in the formation of molecular triads,10 in which the POM acceptor is covalently sandwiched by low-valent Au3(NHC)3, Au2(NHC)2, or Au(NHC) donor moieties (Fig. 1C). The synergistic effect between gold and POM also plays a key role here. The triads showed excellent performance in the catalytic conversion of H2O2. Moreover, these can be viewed as molecular models of the POM-based EC-STM break junction, albeit direct comparison is indeed difficult due to the different type of gold and the different binding situations in these gold–POM heterostructures (Au⋯NH4C5-POM in the single-molecule junctions vs. (NHC)3Au3–N-POM, (NHC)2Au2–NH-POM, and (NHC)Au–NH2-POM in the individual molecules).
It is known from the chemistry of low-valent metalates that their highly reduced nature can be of great importance for the activation of inert bonds and for catalytically relevant multielectron transformations.11 However, data on the covalent derivatization of POM-based inorganic–organic hybrids with organogold(I) moieties and their application on metal surfaces are still scarce. This contrasts with the extensive data on intermetallic compounds consisting of negatively charged POM structures counter-balanced with mono- or polynuclear gold(I) complexes acting as cations.12 Discrete POMs such as, e.g., [NaAu4Pd8O8(AsO4)8]11− with incorporated gold(III) centers were also reported.13 The combination of POM electron sponges and highly reduced organometallic compounds or even AuNPs may be critical for the development of memory devices with extremely high data capacity.
It has recently been demonstrated that organogold(I) substituents introduced at the periphery of the trisalkoxo ligands of the Lindqvist-type hexavanadate precursors such as, e.g., [V6O13{(OCH2)3CCH2N3}2]2− affect the electrical properties of these four-state {V6}POM switches in new {Au(I)–V6–Au(I)} POMs on the Au(111) surface (Fig. 1D).14 The enhanced multielectron transformations observed at the “gold//{Au(I)–V6–Au(I)}-POM//vacuum–Pt-tip” interface are due to the efficient Au(I)-mediated charge redistribution across molecular linkages. This resulted in more than four distinct charge states of the POM under the influence of applied bias voltages and electron tunneling through vacuum. The described stimulus-responsive behavior is significantly different from the situation when Lindqvist-type hexavanadate structures bear non-metallic ligand substituents. In that case, no effect on the resistance steps in the current–voltage profiles was observed.15
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