TEM studies of stress relaxation in catalytic Au-Pd core-shell nanoparticles Abstract. Transmission electron microscopy and diffraction are used to measure the lattice strain in catalytic Au-Pd core-shell nanoparticles. In order to simplify analysis, single nanoparticles were oriented to achieve strong two-beam diffracting conditions from the nanoparticle centre, such that diffraction was sensitive to the strain parallel to the Au-Pd interface. Corresponding selected area diffraction patterns were used to measure the in-plane strain as a function of the Pd thickness, which is shown to follow the equilibrium (Matthews) theory. These results suggest that, contrary to expectation, strain is not an important factor accounting for the difference in catalytic activity between nanoparticles and thin films. The significance of these results is discussed.
Introduction.Bimetallic nanoparticles (NPs) have attracted great interest among the scientific and technological community since they lead to many interesting size-dependent electrical, chemical, and optical properties. Specifically they often exhibit enhanced catalytic properties which differ from that of their monometallic counterparts, and from thin films. This paper examines Au-Pd core-shell nanoparticles (CS-NPs). These have been widely studied by several research groups [1][2][3][4] in terms of fabrication, stabilization and catalytic behaviour, but the factors controlling catalytic behaviour, in particular the relative contribution of lattice strain and ligand (electronic) effects, remain unclear. Here, we examine the strain and morphology in Au-Pd CS-NPs as a function of the Pd thickness. Au-Pd CS-NPs were synthesized by colloidal methods for generating Pd shell thickness in a range of 1-10nm over an Au core. Strain in CS-NPs can easily be studied by selected area electron diffraction patterns (SADPs) from particle ensembles, but this method is difficult to interpret as the patterns contain contributions from an in-plane expansion of the Pd (which has the smaller lattice parameter and should be under tensile stress) and an out-of-plane Poisson contraction, This leads to a complex displacement field for the diffracting planes, which are oriented near edge-on to the incoming electron beam (Figure 1). To avoid this problem, we have examined two-beam SADPs from individual CSNPs, which are oriented by observing the bright field image contrast, to maximise diffraction from the particle centres, and which should, therefore, be sensitive to the strain parallel to the Au-Pd interface (in-plane strain). It is shown that the strain as a function of Pd thickness follows equilibrium theory.