I. Introduction
The conventional metals Ag, Au, and Cu are the metals of choice for visible range plasmonics [1]. Although these are high quality plasmonic materials, their tunability is limited due to the ohmic losses and their fixed optical response for a given wavelength. In this respect, alloying has been one of the traditional routes to tailor the properties of pure metals and can potentially result in novel functionalities [2]. However, this approach for increasing the materials available for visible plasmonics has only gained attention in the recent times. The plasmonic response of alloy thin films of Ag-Au, Ag-Cu, and Au-Cu was studied by Gong and Leite as a function of alloy composition [3]. They showed that the plasmon resonances supported by the alloy films change as a function of composition and lie within the resonance range of pure metal constituents. Furthermore, amongst these plasmonic alloys, Ag-Cu is a eutectic system that is cost-effective and forms compositionally inhomogeneous two-phase microstructures under appropriate fabrication conditions [4]. Depending on the composition of the alloy, the phase separation can happen either by spinodal decomposition or by nucleation and growth. This kind of two-phase microstructure is a unique and interesting system to investigate the behavior of surface plasmons. However, the effect of such complex microstructures on the plasmonic behavior has not yet been investigated.