Study of the structure evolution and ground state energy of Co_n Cu_(55-n) (n=0—55)bimetallic clusters by using the Gupta potential combined with a genetic algorithm
En-Cai Xiao
Abstract
En-Cai Xiao
Abstract
The ground-state structures and energies of the bimetallic clusters ConCu55 - n(n = 0—55)were obtained by using the semi-empirical Gupta potential combined with a genetic algorithm. The ground-state geometries of those bimetallic clusters can be characterized by the basic Mackay icosahedron of the pure Co55 (Cu55 ) cluster. Beginning with n = 0 (Cu55 ),the Cu atom(s) is(are) replaced in order and continuously by the Co atom( s) from the center to the surface and from the edge to the vertex. The ground-state structure depends on the number of the Co—Co bonds which have the largest energy, the number of the Co-Cu bonds with large energy and the average bond length of those bonds. Co13 Cu42 is a magic cluster with an icosahedral core formed by 13 Co atoms,which plays a key role in the high stability of those bimetallic clusters.
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The ground-state structures and energies of the bimetallic clusters ConCu55 - n(n = 0—55)were obtained by using the semi-empirical Gupta potential combined with a genetic algorithm. The ground-state geometries of those bimetallic clusters can be characterized by the basic Mackay icosahedron of the pure Co55 (Cu55 ) cluster. Beginning with n = 0 (Cu55 ),the Cu atom(s) is(are) replaced in order and continuously by the Co atom( s) from the center to the surface and from the edge to the vertex. The ground-state structure depends on the number of the Co—Co bonds which have the largest energy, the number of the Co-Cu bonds with large energy and the average bond length of those bonds. Co13 Cu42 is a magic cluster with an icosahedral core formed by 13 Co atoms,which plays a key role in the high stability of those bimetallic clusters.
Key concepts: Bimetallic strip, Icosahedral symmetry, Ground state, Cluster (spacecraft), Crystallography, Atom (system on chip), Chemistry, Atomic physics