Role of core-shell energetics on anti-Mackay, chiral stacking in Agcu nanoalloys and thermally induced transition to chiral stacking Manoj Settem & Anand K. Kanjarla in Agcu nanoalloys a size-dependent transition to the chiral stacking from the anti-Mackay stacking has been predicted previously. this trend is explained by considering the interplay between the core-shell energetics. Results indicate that the energy changes in the Ag shell alone is not sufficient to explain the stability of the chiral stacking and the energy changes in the cu core also need to be considered. in addition to this, thermally induced transition to chiral stacking was observed at sizes where anti-Mackay stacking is energetically favourable. on transition to the chiral stacking, the Ag-Ag, Ag-cu and Cu-Cu bond lengths change significantly. These observations are also applicable for AgCu nanoalloys with incomplete Ag shells. Bimetallic nanoalloy systems exhibit novel properties due to synergistic effects between the constituent metals. Bimetallic nanoclusters and nanoparticles have been extensively studied as they afford the opportunity to tune their chemical and physical properties through composition and chemical ordering 1-3. Along with the geometrical structure of a bimetallic nanocluster, due to the presence of two elements, different types of chemical ordering are possible: phase segregated and mixed. Depending on the bimetallic system, phase segregation can manifest as core-shell structure 4,5 where one of the constituent element covers the other completely or two phases joined at an interface, usually referred to as "Janus" type arrangemen 6-8. Similarly, mixed chemical ordering can be ordered (as is the case for bimetallic systems that form intermetallic phases) 9 or disordered 10. It is essential to know the optimal structures as a function of the size and the composition in order to understand the properties of bimetallic nanoclusters. Finding the optimal structures involves exploring the potential energy surface (PES) 11. Typically, methods based on genetic algorithm 12 or Monte Carlo combined with energy minimization commonly referred to as "basin hopping" Monte Carlo 13 are used to explore the PES and find the optimal structures using empirical atom-atom potentials such as the second moment approximation to tight binding (SMATB) 14-17 potential or the embedded atom method (EAM) 18 potential. Finally, the putative global minima and the lowest lying isomers belonging to the different structural motifs are singled out for relaxation using density functional theory (DFT). This provides a database of optimal structures which can be used to compare with the experimentally synthesized bimetallic nanoclusters. Depending on the constituent atoms in a bimetallic nanoalloy, specific structural motifs can become energetically favourable. The anti-Mackay icosahedron becomes stable in alloy systems which have a tendency to phase segregate and have atomic size mismatch combined with low surface energy for the larger atoms 19-21. AgCu, AgNi...