Abstract

AbstractThe protonated water dimer has a symmetric structure 1 in contrast to the asymmetric structure of protonated ammonia dimer 2. To make a general understanding of structural symmetry difference for these D–A–D systems, we carried out a systematic theoretical study with the B3LYP/6‐31+G** method. We considered the electron donors (D) of the lone pair on either side of BF, CO, and N2 molecules, as well as the electron acceptors (A) like Li+, CH3+, SiH3+, and PH2+ beside the proton. We found the magnitude of the first bonding energy between D and A [BE(1)] is decisive for the symmetry of the D–A–D system. A larger BE(1) leads to a smaller BE(2), the bonding energy of D–A with the second donor. This gives rise to a stronger tendency toward asymmetry. The magnitude of BE(1) correlates well with the difference in ionization potential (ΔIP) of the orbitals involved in the D–A interaction. © 2002 Wiley Periodicals, Inc. Int J Quantum Chem, 2002

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