Abstract

Several IR bands for two isotopic forms of the CH3CN–HCl complex have been measured in neon matrices at 6 K. Assigned bands for the primary isotopomer include the νCC band at 926 cm−1, νHCl the band at 2677 cm−1, and the νCN band, which occurs as a doublet at 2308/2279 cm−1. The observed frequencies are reasonably consistent with previous observations in solid argon and/or nitrogen, with the exception of νHCl bands, which differed, and were ultimately found to shift systematically across various condensed-phase media. A plot of medium-induced shifts for the νHCl band vs. polarizability of the host substances is essentially continuous; except for the N2-matrix frequency, for which the shift is considerably larger than that expected on this basis. In an effort to clarify the physical underpinnings of these shifts, and their structural implications, a computational study was undertaken, which examined CH3CN–HCl as well as H3N–HCl; a system for which analogous frequency shifts have been observed and characterized previously. Beyond equilibrium structure and frequency calculations, which predict that the ammonia complex is stronger and undergoes a greater degree of structural change in bulk, condensed-phase media, the N–Cl potentials of both complexes were mapped in the gas-phase and in bulk, dielectric media. The predicted medium effects on these potentials are consistent with observations. The CH3CN–HCl curves shift slightly in response to the medium, consistent with a subtle enhancement of the hydrogen bond, and relatively small frequency shifts. The effects of the dielectric media on H3N–HCl are more substantial, and indicate a significant degree of proton transfer, even for low-dielectric environments, which is consistent with the extreme spectral shifts noted previously for this system.

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