Abstract
Abstract The equilibrium structures, binding energies, and vibrational spectra of the clusters CH3F⋯(HF)1 ⩽ n ⩽ 3 and CH2F2⋯(HF)1 ⩽ n ⩽ 3 have been investigated with the aid of large-scale ab initio calculations performed at the Moller–Plesset second-order level. In all complexes, a strong C–F⋯H–F halogen–hydrogen bond is formed. For the cases n = 2 and n = 3, blue-shifting C–H⋯F–H hydrogen bonds are formed additionally. Blue shifts are, however, encountered for all C–H stretching vibrations of the fluoromethanes in all complexes, whether they take part in a hydrogen bond or not, in particular also for n = 1. For the case n = 3, blue shifts of the ν(C–H) stretching vibrational modes larger than 50 cm−1 are predicted. As with the previously treated case of CHF3⋯(HF)1 ⩽ n ⩽ 3 complexes (A. Karpfen, E. S. Kryachko, J. Phys. Chem. A 107 (2003) 9724), the typical blue-shifting properties are to a large degree determined by the presence of a strong C–F⋯H–F halogen–hydrogen bond. Therefore, the term blue-shifted appears more appropriate for this class of complexes. Stretching the C–F bond of a fluoromethane by forming a halogen–hydrogen bond causes a shortening of all C–H bonds. The shortening of the C–H bonds is proportional to the stretching of the C–F bond.
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