The structures of [Pt(CNMe) 2 (CN) 2 ] n (n = 1-4) in the ground states (S 0 ) and lowest-energy triplet excited states (T 1 ) were calculated by using the second-order Møller-Plesset perturbation (MP2) and density functional theory (DFT) methods, respectively. The MP2 results show that the formation of the dimer causes a significant red shift in emission energy, and the frequency calculations reveal that a weak metal-metal interaction exists in the S 0 state, which is greatly enhanced in the 3 [d σ* p σ ] excited state. The aggregation of [Pt(CNMe) 2 -(CN) 2 ] n (n = 1-4) was explored by using the slate-type VWN functional in the DFT method. The 3 B u Ǟ 1 A g transition in the dimer at 509 nm corresponds to the experimental higher-