IR-Spectroscopic and X-ray-Structural Study of Vinyl-Type Carbocations in Their Carborane Salts

The butylene carbocation in its salts with anions CHB11F11- and CHB11Cl11- forms isomers CH2=C+-CH2-CH3 (I) and CH3-(C+)=CH-CH3 (II), which were characterized here by infrared (IR) spectroscopy and X-ray diffraction analysis. The strongest influence on the structure of the cations is exerted by geometric ordering of their anionic environment. In the crystalline phase, the cations uniformly interact with neighboring anions, and the C=C bond is located in the middle part of the cations forming a -CH=C+- moiety with the highest positive charge on it and the lowest nu C=C frequency, at 1490 cm(-1). In the amorphous phase with a disordered anionic environment of the cations, contact ion pairs Anion(-)center dot center dot center dot CH2=C+-CH2-CH3 form predominantly, with terminal localization of the C=C bond through which the contact occurs. The positive charge is slightly extinguished by the anion, and the C=C stretch frequency is higher by similar to 100 cm(-1). The replacement of the hydrogen atom in cations I/II by a Cl atom giving rise to cations CH2=C+-CHCl-CH3 and CH3-C+= CCl-CH3 means that the donation of electron density from the Cl atom quenches the positive charge on the C+=C bond more strongly, and the C=C stretch frequency increases so much that it even exceeds that of neutral alkene analogues by 35-65 cm(-1). An explanation is given for the finding that upon stabilization of the vinyl cations by polyatomic substituents such as silylium (SiMe3) and t-Bu groups, the stretching C=C frequency approaches the triple-bond frequency. Namely, the scattering of a positive charge on these substituents enhances their donor properties so much that the electron density on the C=C bond with a weakened charge becomes much higher than that of neutral alkenes.

Automated summary

The isomeric structures of butylene carbocation in its salts with anions CHB11F11- and CHB11Cl11- have been characterized, and it was found that the structure of the cations is influenced by the geometric ordering of their anionic environment. The structures and C=C bond vibrational frequencies of the isomers differ.