PHENYL RADICAL, CATION, AND ANION - THE TRIPLET-SINGLET GAP AND HIGHER EXCITED-STATES OF THE PHENYL CATION

Citation
A. Nicolaides et al., PHENYL RADICAL, CATION, AND ANION - THE TRIPLET-SINGLET GAP AND HIGHER EXCITED-STATES OF THE PHENYL CATION, Journal of the American Chemical Society, 119(34), 1997, pp. 8083-8088
Citations number
61
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
119
Issue
34
Year of publication
1997
Pages
8083 - 8088
Database
ISI
SICI code
0002-7863(1997)119:34<8083:PRCAA->2.0.ZU;2-X
Abstract
High-level ab initio molecular orbital calculations have been carried out for the phenyl cation (1), the phenyl radical (2), and the phenyl anion (3). Our best estimate for the heat of formation (Delta H-f298) Of the phenyl radical is 340 kJ mol(-1), corresponding to 476 kJ mol(- 1) for the 298 K C-H bond dissociation energy in benzene. The calculat ed Delta H-f298 Of the phenyl anion is 224 kJ mol(-1), leading to an e lectron affinity for the phenyl radical of 116 kJ mol(-1), and a gas-p hase acidity for benzene of 1671 kJ mol(-1). The ground state of the p henyl cation is found to be a singlet (1-(1)A(1), Delta H-f298 = 1134 kJ mol(-1)), with the tripler (1-B-3(1), Delta H-f298 = 1237 kJ mol(-1 )) lying significantly higher in energy (by 103 kJ mol(-1)). The energ ies of the 1-(1)A(1) and 1-B-3(1) states of the phenyl cation at the p henyl radical geometry are much closer, but 1-(1)A(1) remains the ener getically lowest electronic state. The essentially isoenergetic 1-(3)A (2) and 1-(1)A(2) states lie about 25 kJ mol(-1) higher in energy than 1-B-3(1), while 1-B-1(1) is nearly 60 kJ mol(-1) higher in energy. Th e implications of these results with respect to recent spectroscopic s tudies of the phenyl radical and the role of the triplet phenyl cation in the dissociation of benzene cation are discussed.