Abstract
Making use of molecular graphics software, we designed numerous models of BeC n − ( n = 1–8). Geometry optimization and calculation on vibration frequency were carried out by the B3LYP density functional method. After comparison of structure stability, we found that the ground-state isomers of BeC n − ( n = 1–8) are linear with the beryllium atom located at one end of the C n chain, except that the linear BeC 5 − isomer is slightly higher in energy than the planar cyclic BeC 5 − isomer. When n is even, the C n chain of BeC n − ( n = 1–8) is polyacetylene-like whereas when at odd n, the carbon chain is cumulene-like. The BeC n − ( n = 1–8) with even n are found to be more stable than those with odd n, and the result is in good accord with the relative intensities of BeC n − ( n = 1–8) observed in mass spectrometric studies. In this paper, we provide satisfactory explanation for such trend of even/odd alternation based on concepts of bonding nature, electronic configuration, electron affinity, incremental binding energy, and dissociation channels.
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