Fabrication of electrodes by deposition of lead clusters from the Matrix Assembly Cluster Source (MACS) into porous carbon paper for electrocatalysis

Nanoparticles are assemblies of atoms or molecules with sizes in the range 1–100 nm [1, 2]. The ability to tailor the unique chemical or physical properties of the nanoparticles has enabled them to be used in a wide spectrum of applications, such as catalysis [3, 4], medicine [5, 6] and photonics [7, 8]. Many approaches have been explored for the production of nanoparticles with well controlled size and composition, including chemical [9, 10], physical [11, 12] and biological [13, 14] methods. Cluster (nanoparticle) beam deposition is a physical technique recognised as a promising method for environmentally clean (“green”) nanoparticle production [2, 15].

The directional and ballistic nature of the cluster beam generated by a cluster source presents challenges for coating the desired cluster support in an even way. Scaled-up cluster beam sources are now available [16, 17], which are capable of depositing fractions of a gram of clusters per hour onto a support to create functional materials such as catalysts. To take full advantage of these new instruments, such as the Matrix Assembly Cluster Source [18, 19], we must learn to present to the directed beam large surface areas of the support material. A successful innovation has been to agitate or stir a powder while it is coated (from above) by the cluster beam. Several examples of heterogeneous catalysis with such cluster-decorated powder materials have been reported [20‐23]. A problem of cluster deposition into powders is that the impact parameters of the cluster-surface collision vary, because each powder particle presents a curved surface at uncontrolled angle to the incoming cluster. If the fate of the cluster—in terms of its final shape on, and diffusion across, the surface—depends on the precise landing site and angle, non-uniform cluster coverage and morphology may result. Presenting to the cluster beam a planar surface at normal incidence overcomes this problem, but obviously limits the area that can be decorated, if the preservation of individual clusters is required. Scanning of the planar support to be coated underneath the beam resolves these issues [24]. A third approach, as demonstrated herein, is to present to the beam a porous support material whose microscopic surface area, available for cluster binding, is enormously higher than the macroscopic projected surface area of the material. Porous carbon paper [25] is one of many such examples. Since nanocomposite layers—consisting of nanoparticles dispersed by chemical means within such porous supporting frameworks—already have important applications in, e.g. the chemicals and energy sectors [26, 27], the demonstration of cluster beam deposition into porous materials has obvious practical relevance as well as fundamental interest.

The deposition of lead (Pb) clusters into porous carbon paper was accomplished with the Matrix Assembly Cluster Source (MACS) technique. The carbon paper (Sigracet 29 AA, SGL Carbon) used in this work has a thickness of about 200 μm, with a mean pore size of about 50-μm diameter. The porosity of the carbon paper is 80% according to the specification sheet of the supplier. The details of this cluster beam technique have been described previously [21]. The Pb clusters were formed and deposited onto carbon paper in the MACS deposition chamber. An oxygen-free copper support was cooled to around 20 K by a closed-loop helium cryocooler, then a solid cryo-matrix of Pb and argon (Ar) atoms was produced on the surface of the copper support, by evaporating Pb atoms and dosing Ar gas at the same time. After the formation of the matrix, an Ar⁺ ion beam (1.1 kV, 15–20 mA) was employed to sputter the matrix, creating a beam of Pb clusters, which were directly deposited onto the carbon paper. The clusters are formed by collision cascades in the matrix. The carbon paper (circular shape) with diameter 10 cm was introduced into the deposition chamber from a load-lock chamber prior to Pb cluster deposition from the matrix; we refer to the result as “Pb-C” paper.

During the formation of the matrix, a quartz crystal microbalance was used to measure the metal evaporation rate in the matrix, 10 Å/s. The Ar dosing pressure was set (4.5 × 10⁻⁴ mbar) to achieve a metal loading in the matrix of ~ 4% by number of atoms. The production of Pb cluster beam was achieved by sputtering the matrix with Ar⁺ ion beam (1.1 kV, 15–20 mA). The carbon paper was rotated on a stage throughout entirety of the deposition to achieve uniform deposition. In order to achieve a decent metal loading on the support, a deposition time of 1 h was used. To measure the amount deposited, quartz crystal microbalances were used. We estimate that the total amount of Pb clusters deposited on the carbon papers was about 1.45 mg for the scanning transmission electron microscopy (STEM) study and 4.40 mg for the scanning electron microscopy (SEM) and electrochemical studies, i.e. 0.018mg/cm² and 0.056mg/cm², respectively.

The microscopic morphology of the C-paper before and after deposition with Pb clusters was characterised with SEM. Chemical information on the Pb-C paper was revealed with EDX analysis. SEM images of the bare carbon paper support and Pb-C paper are shown in Fig. 1A and B, respectively. The carbon substrate was characterised as interconnected carbon fibres with an average thickness of 7 μm as well as carbon particles and flakes with a diameter ranging from 10 to 30 μm, randomly scattered over the surface. Changes in the surface morphology of the carbon fibres as a result of Pb coating confirm that Pb was successfully deposited. Additionally, from magnified sections of the SEM images, the surface of the pristine C-paper appeared smooth whereas the surface of the Pb-C paper presented to the cluster beam became rougher.

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For cross-sectional analysis, the samples were cut with a surgical blade and mounted vertically on the SEM sample holder. The cross-sectional SEM and EDX analysis of the Pb-C paper, Fig. 1C, showed that the ~ 200-μm-thick carbon film was built of interconnected carbon fibres and particles as described, with pores evident throughout the material, providing tunnels for the directed Pb clusters to penetrate into. The upper cross-section (0–50-μm depth) shown in Fig. 1C showed Pb cluster deposition throughout the depth analysed, ~ 50 μm from the top surface of the C-paper, which is comparable with the pore size. The lower cross-section (50–200-μm depth), showing a reduced amount of Pb within the C-paper; this section had a depth ~ 150 μm. EDX analysis of the Pb-C paper shown in Fig. 1D indicates that the concentration of Pb decreases from top surface to cross-section. ~ 54.5% of the total amount of Pb infiltrated the paper and settled on the inner carbon fibres.

The stability of the Pb-C paper was also evaluated by EDX analysis. Samples of carbon paper with deposited Pb clusters were immersed in de-ionised water and also 0.5 M H₂SO₄ for 16 h. After this time, the amount of Pb in the carbon paper was reduced by 81% and 97% for DI water and the acid, respectively, suggesting rather weak adhesion of Pb to the carbon paper matrix.

A small section with a diameter of ~ 3 mm was cut from the Pb-carbon paper for scanning transmission electron microscopy (STEM) imaging. The STEM imaging was performed using a Thermo Scientific Talos F200X Transmission Electron Microscope operating at 200 kV in the high-angle annular dark-field (HAADF) mode. The images were taken from the ultrathin area located on the carbon flake of the carbon paper. It can be seen from Fig. 2a that the surface of the Pb-carbon paper is covered with sphere-like structures. Figure 2b shows that those sphere-like structures are decorated with small Pb clusters. The HAADF contrast indicates that the spheres themselves are carbon rather than Pb, as the small Pb clusters would not be visible if the spheres were Pb.

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In order to study the size of the structures assigned to carbon spheres and Pb clusters, their projected surface areas were measured and converted into diameters. One hundred forty-right and two hundred sixty carbon sphere and Pb nanoparticles were measured for the size distributions of Fig. 2c and d. The carbon structures have a mean diameter of 15.9 nm, while the Pb clusters have a mean diameter of 2.1 nm. The porous structure of the carbon paper can allow the cluster beam to penetrate into a certain depth, which is confirmed by the SEM-EDS mapping of the cross-section shown in Fig. 1. The uniform dispersion and the narrow size distribution of Pb clusters indicate there is no further diffusion and aggregation for Pb clusters after landing on the support.

The functionality of the nanocomposite material was demonstrated in a preliminary fashion by experiments in which the Pb-C paper was used as an electrode (anode) in an electrochemical flow cell reactor, to generate reactive oxidative species (ROS) in aqueous solution, as tested through the degradation of potassium indigo trisulphonate. With a constant voltage of 10 V applied for 60 min, the potassium indigo trisulphonate electrolyte was allowed to circulate in the cell at a constant rate of 2.5 L/h. The absorbance due to the blue indigo trisulphonate indicator (wavelength 600 nm) gradually decreased as a result of oxidation by ROS produced in the cell (e.g. hydroxy radicals and ozone) (Fig. 3). The colour change of the dye solution is indicative that such species were generated in the reaction cell [28, 29]. At the molecule level, the double bonds between carbon atoms (> C = C <) in the indigo molecule break when exposed to oxidative species and the carbon atoms are oxidised (two > C = O entities are created). The products are colourless. The reaction is below:

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Regarding the specifics of the UV/Vis spectra, the characteristic absorbance band for indigo is at 600 nm. The other three peaks observed in the UV region correspond to structural features of the dye: the peak at 300 nm is related to the amino group, that at 250 nm is attributed to the carbonyl group and the peak at 205 nm corresponds to the resonance of the aromatic ring. The peak which grows with time at approximately 700 nm could be due to interaction between the dye and metal ions (e.g. Pb(II) or Cu(II)) to form a metal-dye complex that absorbs at higher wavelength [30]. Pb(II) could be formed by dissolution of the Pb clusters into electrolyte and Cu(II) could be formed by dissolution of the conductor. In order to prevent the dissolution of Pb from support to solution, an oxide support can be used to anchor the Pb cluster in place.

In this work, Pb clusters with an average diameter of ~ 2 nm were fabricated with the MACS technique and deposited into porous C-paper. Both STEM and SEM studies together with EDX mapping confirm the successful deposition of Pb clusters to form the nanocomposite Pb-C paper system. The EDX analysis indicates that the Pb clusters are deposited to a depth into the carbon paper comparable with the pore size of the carbon paper, ~ 50 μm. The Pb-C paper was tested as an electrode for the electrochemical generation of highly reactive oxidative species in an electrochemical flow cell reactor. The Pb-C paper showed initial activity but deactivated on the timescale of 10 s, attributed to the dissolution of Pb clusters into electrolyte. Future work will need to address the adhesion/anchoring of the clusters to the fibres of the host material. Most significantly, this study has demonstrated a method of presenting a high surface area host material to an intense directed beam of sub-10-nm clusters. The method has few steps and may be competitive with chemical approaches.