Sunlight‐powered reduction of CO₂ to fuels and chemicals is a promising strategy to close the carbon loop and facilitate the energy transition. In this research, we demonstrate that Au nanoparticles supported on TiO₂ are an efficient plasmonic catalyst for the sunlight‐powered reverse water‐gas shift (rWGS) reaction. A maximum CO production rate of 429 mmol ⋅ g_Au⁻¹ ⋅ h⁻¹ with a selectivity of 98 % and an apparent quantum efficiency of 4.7 % were achieved using mildly concentrated sunlight (1.44 W ⋅ cm⁻² equals 14.4 sun). The CO production rate showed an exponential increase with increasing light intensity, suggesting that the process is mainly promoted by a photothermal effect. Thermal reference experiments with the same catalysts promoted CH₄ formation, dropping the CO selectivity to 70 %. Thus, mildly concentrated sunlight can efficiently and selectively enhance the promotion of the rWGS reaction without using external heating.

Plasmon catalysis is an interesting technology concept for powering chemical processes with light. Here, we report the use of various Al₂O₃‐supported Ru spheroidal nanoparticles as catalyst for the low‐temperature conversion of CO₂ and H₂ to CH₄ (Sabatier reaction), using sunlight as energy source. At high loadings of Ru spheroidal nanoparticles (5.9 % w/w), we observe a sharp increase in the rate of the sunlight powered reaction when compared to the reaction in dark at the same catalyst bed temperature. Based on our results we exclude plasmon coupling as cause, and attribute the rate enhancement to collective photothermal heating of the Al₂O₃‐supported Ru nanoparticles.

Platelets can release extracellular vesicles (EVs) upon stimulation with various agonists. Interestingly, platelets from patients with Glanzmann thrombasthenia have reduced EV release. These platelets lack functional α_IIbβ₃ integrins, indicating that α_IIbβ₃ integrin is critical in vesicle release. Integrin activation is central in platelet function and is associated with e.g. adhesion, aggregation and cytoskeletal rearrangement. However, while platelet activation pathways are widely known, the mechanisms underlying EV release remain uncharacterized. We investigated the role of integrin α_IIbβ₃, phosphatidyl serine (PS) exposure, cytoskeletal rearrangement and their associated signalling pathways in EV release. EVs were isolated from activated platelets. Platelet activation status was measured by multicolour flow cytometry. A panel of pharmacologic inhibitors was used to interfere in specific signalling pathways. EV release was quantified enzymatically based on membrane PS content and nanoparticle tracking analysis. In addition, real-time visualization of EV shedding with confocal microscopy and EVs with Cryo-TEM imaging was performed. Platelet activation with convulxin resulted in higher EV release than with activation by thrombin. Kinetic measurements indicated that EV release followed the pattern of α_IIbβ₃ integrin activation and subsequent closure paralleled by PS exposure. Prevention of α_IIbβ₃ activation with the inhibitor tirofiban dramatically suppressed EV release. Similar results were obtained using α_IIbβ₃-deficient platelets from patients with Glanzmann thrombasthenia. Inhibition of actin cytoskeleton rearrangement decreased EV release, whereas inhibition of individual signalling targets upstream of cytoskeletal rearrangement showed no such effects. Platelet EV release requires three main events: integrin activation and closure, PS exposure, and cytoskeletal rearrangement.

Plasmonic CO₂ methanation using γ-Al₂O₃-supported Ru nanorods was carried out under continuous-flow conditions without conventional heating, using mildly concentrated sunlight as the sole and sustainable energy source (AM 1.5, irradiance 5.5–14.4 kW·m⁻² = 5.5–14.4 suns). Under 12.5 suns, a CO₂ conversion exceeding 97% was achieved with complete selectivity towards CH₄ and a stable production rate (261.9 $\mathrm{mmol}·{\mathrm{g}}_{\mathrm{Ru}}^{-1}·{\mathrm{h}}^{-1}$) for at least 12 h. The CH₄ production rate showed an exponential increase with increasing light intensity, suggesting that the process was mainly promoted by photothermal heating. This was confirmed by the apparent activation energy of 64.3 kJ·mol⁻¹, which is very similar to the activation energy obtained for reference experiments in dark (67.3 kJ·mol⁻¹). The flow rate influence was studied under 14.4 suns, achieving a CH₄ production plateau of 264 µmol min⁻¹ (792 $\mathrm{mmol}·{\mathrm{g}}_{\mathrm{Ru}}^{-1}·{\mathrm{h}}^{-1}$) with a constant catalyst bed temperature of approximately 204 °C.

To tailor the properties of nanoparticles and nanocomposites, precise control over particle size is of vital importance. Real-time monitoring of particle size during bottom-up synthesis in liquids would allow a detailed study of particle nucleation and growth, which provides valuable insights in the mechanism of formation of the nanoparticles. Furthermore, it facilitates a rational scale-up, and would enable adequate intervention in the production process of nanoparticle dispersions to minimize the number of off-spec batches. Since real-time monitoring requires particle size measurements on dispersions in flow, conventional dynamic light scattering (DLS) techniques are not suited: they rely on single scattering and measure the Brownian motion of particles dispersed in a liquid. Here, we present a set-up that allows accurate measurements in real-time on flowing dispersions using a DLS technique based on modulated 3D cross-correlation. This technique uses two simultaneous light scattering experiments performed at the same scattering vector on the same sample volume in order to extract only the single scattering information common to both. We connected the reactor to a flow-cell in the DLS equipment using a tailor-made analysis loop, and successfully demonstrated the complete set-up through monitoring of the size of spherical silica nanoparticles during Stöber synthesis in a water-alcohol mixture starting from the molecular precursor tetraethyl orthosilicate.