Abstract

The interactions between Pt n clusters ( n ⩽ 13 ) and a graphene sheet have been investigated by first-principles calculations based on density functional theory. For single Pt-atom and Pt 2 -dimer adsorptions, the stable adsorption sites are bridge sites between neighboring carbon atoms. When the number of Pt atoms in a cluster increases, the Pt–C interaction energy per contacting Pt atom becomes smaller. For smaller clusters ( 3 ⩽ n ⩽ 7 ) , the adsorption as a vertical planar cluster is more stable than that as parallel planar or three-dimensional (3D) clusters, due to the stability of a planar configuration itself and the stronger planar-edge/graphene interaction, while the adsorption as a parallel planer cluster becomes stable for larger cluster ( n ⩾ 7 ) via the deformation of the planar configuration so as to attain the planar-edge/graphene contact. For much larger clusters ( n ⩾ 10 ) , the adsorption as a 3D cluster becomes the most stable due to the stability of the 3D configuration itself as well as substantial Pt–C interactions of edge or corner Pt atoms. The interfacial interaction between a Pt cluster and graphene seriously depends on the shape and size of a cluster and the manner of contact on a graphene sheet.

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