Figure 1 allows us to confirm the crystal structure of intermetallic Cu3Sn, disordered Cu-Sn alloy and pure Cu NPs, respectively. The main diffraction peaks of Cu NPs and disordered Cu-Sn alloy can be observed which are assigned as FCC-type structure while the XRD pattern of intermetallic NPs shows a good fit with stoichiometric Cu3Sn structure based on Cu3Ti-type lattice (1). Figure 2 shows the Faradaic efficiency (FE) for gaseous products which was evaluated in CO2 reduction for intermetallic Cu3Sn under the potential varying from -0.8 V to -1.6 V vs.RHE. It is suggested that the FE of CO production reaches the highest value of 40 % at -1.4 V, while the FE of hydrogen production is suppressed under 17%.
[1] Y. Watanabe, et al., Acta Cryst., B39, 1983, 306-311.