H-BONDED AND STACKED DIMERS OF PYRIMIDINE AND P-BENZOQUINONE - A COMBINED MATRIX-ISOLATION INFRARED AND THEORETICAL AB-INITIO STUDY

Citation
W. Mccarthy et al., H-BONDED AND STACKED DIMERS OF PYRIMIDINE AND P-BENZOQUINONE - A COMBINED MATRIX-ISOLATION INFRARED AND THEORETICAL AB-INITIO STUDY, The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory, 101(39), 1997, pp. 7208-7216
Citations number
22
Categorie Soggetti
Chemistry Physical
ISSN journal
10895639
Volume
101
Issue
39
Year of publication
1997
Pages
7208 - 7216
Database
ISI
SICI code
1089-5639(1997)101:39<7208:HASDOP>2.0.ZU;2-O
Abstract
Matrix isolation IR spectroscopy and high-level ab initio calculations were applied to investigate the structure and vibrational spectra of quinone-pyrimidine heterodimers formed in low-temperature Ar matrices. A specially developed experimental technique was used to separate ban ds of quinone-pyrimidine dimer from bands of quinone and pyrimidine mo nomers and homodimers in the IR spectra. As a result, nine bands assig ned to the quinone-pyrimidine heterodimer were identified. Ab initio c alculations at the MP2/6-31+G, MP2/6-31++G** and SCF/6-31++G** levels of theory have been carried out to determine the relative energies an d vibrational spectra of three stable configurations of the quinone-py rimidine dimer found theoretically. These configurations are two plana r complexes with two weak C-H ... O and C-H ... N hydrogen bonds and o ne stacked complex stabilized by dispersion forces. The effect of basi s set superposition error (BSSE) on the relative stabilities and the v ibrational spectra of the dimers was also investigated. The non-BSSE-c orrected calculations at the MP2/6-31+G and MP2/6-31++G** levels of t heory predict the stacked dimer to be the most stable conformer, but a ccounting for BSSE resulted in a reverse stability ordering of the sta cked and the planar dimers. The comparison of the observed frequency s hifts with the theoretically predicted shifts has shown that the plana r configuration is responsible for the experimentally observed bands. This is in agreement with the stability ordering derived from the BSSE -corrected relative energies. To account for the matrix effects on the stability of the planar and stacked dimers, additional calculations w ere carried out using the Onsager's reaction field model and the MP2/6 -31++G* level of theory. These calculations confirm that the planar H -bonded dimer is the most stable configuration.