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Here, we describe the surprising reactivity between surface-attached (a) 0.9, 1.6, and 4.1 nm diameter weakly stabilized Au nanoparticles (NPs) and aqueous 1.0 × 10–4 M Ag+ solution, and (b) 1.6 and 4.1 nm diameter weakly stabilized Au NPs and aqueous 1.0 × 10–5 M PtCl4 2–, which are considered to be antigalvanic replacement (AGR) reactions because they are not thermodynamically favorable for bulk-sized Au under these conditions. Anodic Stripping Voltammetry (ASV) and Scanning Transmission Electron Microscopy with Energy-Dispersive X-ray Spectroscopy (STEM-EDS) mapping provide quantitation of the extent of Ag and Pt replacement as a function of Au NP diameter. The extent of the reaction increases as the Au NP size decreases. The percentage of Ag in the AuAg alloy following AGR based on ASV is 17.8 ± 0.6% for 4.1 nm diameter Au NPs, 87.2 ± 2.9% for 1.6 nm Au NPs, and an unprecedented full 100% Ag for 0.9 nm diameter Au NPs. STEM-EDS mapping shows very close agreement with the ASV-determined compositions. In the case of PtCl4 2–, STEM-EDS mapping shows AuPt alloy NPs with 3.9 ± 1.3% and 41.1 ± 8.7% Pt following replacement with 4.1 and 1.6 nm diameter Au NPs, respectively, consistent with qualitative changes to the ASV. The size-dependent AGR correlates well with the negative shift in the standard potential (E0) for Au oxidation with decreasing NP size.

Understanding and improving charge transfer pathways between extracted Photosystem I (PSI) protein complexes and electrodes is necessary for the development of low‐cost PSI‐based devices for energy conversion. We incorporated PSI multilayers within porous indium tin oxide (ITO) electrodes and observed a greater mediated photocurrent in comparison to multilayers on planar ITO. First, the mediated electron transfer (MET) pathway in the presence of 2,6‐dichlorophenolindophenol (DCPIP) and ascorbate (AscH) was studied via photochronoamperometry on planar ITO. ITO nanoparticles were then used to fabricate two porous electrode morphologies; mesoporous (20–100 nm pores) and macroporous (5 μm pores). PSI multilayers within macroporous ITO cathodes produced 42±5 μA cm−2 of photocurrent, three times the photocurrent produced by mesoporous ITO. Additionally, macroporous cathodes are able to utilize twice as much active surface area, when compared to mesoporous cathodes. Our findings show that MET within PSI multilayers is greater in 5 μm macropores than mesoporous ITO due to both an increase in electrode surface area and the location of PSI complexes within the pores. Improving MET in PSI‐based bioelectrodes has applications including improving the total charge transfer achieved in PSI‐based photoelectrochemical cells or even incorporation in bio‐photocatalytic cells.

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