The interaction of materials with light is of fundamental importance in a variety of applications such as photovoltaics or photocatalysis. Among promising materials for efficient light interaction are metal nanoparticles (NPs) due to their localized surface plasmon resonances (LSPRs), which cause strong light absorption and scattering, a phenomenon that is exploited in many fields ranging from physics to biology and medicine. The wavelength and strength at which the interaction happens can be tuned by changing the shape, size and metal of the NPs. In particular, anisotropic shapes enhance the interaction and are thus intriguing systems to study. Next to NPs with only one material, NPs with two metals, i.e. bimetallic NPs, offer an additional way of tuning the functionality and LSPR resonance.
Because the parameter space is large, understanding the delicate interplay between particle morphology, composition and optical properties is of utmost importance in optimizing particle design for the desired applications. Optical properties can be measured by e.g. luminescence or scattering measurements using lasers or white light lamps as excitation sources but also by using high energetic electrons in electron energy loss spectroscopy. The connection to their structure is often done by scanning electron microscopy or transmission electron microscopy (TEM) performed on similar particles from the same sample batch. However, for a full understanding of how the morphology and composition of a metal NP is related to its optical properties, the characterization of optical and structural properties needs to happen on the same single NP. Moreover, electron microscopy generally yields 2D information but for complex anisotropic NPs, a 2D projection does not yield enough information on the morphology.
To overcome these challenges, the overall objective of this project is to perform optical and TEM measurements on the same single monometallic and bimetallic NPs to directly correlate the composition, size and morphology to their optical properties. As the focus lies on anisotropic NPs, electron tomography is used to obtain the full 3D structure of the NP, down to atomic resolution. With that methodology, three key questions in nanoscience are tackled: 1) In how far does the deviation from a perfect atomic crystal influence the optical properties of metal NPs? 2) How does the 3D morphology and composition of anisotropic bimetallic NPs dictate their optical properties? 3) What are the differences between exciting metal NPs by light or electrons?