Density-functional methods give accurate vibrational frequencies and spin densities for phenoxyl radical
- 22 January 1995
- journal article
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 102 (4) , 1689-1698
- https://doi.org/10.1063/1.468901
Abstract
The structure, electronic spin density ratios, harmonic vibrational frequencies, and deuterium isotopic vibrational frequency shifts for phenoxyl radical, C6H5Ȯ, were calculated by using spin unrestricted Hartree–Fock (UHF), second-order Mo/ller–Plesset perturbation (UMP2), and various density functional (DF) and hybrid Hartree–Fock/density functional (HF/DF) methods with a 6–31G(d) basis set. Computed results are compared with experiment and with recently published complete active space self-consistent field (CASSCF) and unrestricted natural orbital-complete active space (UNO-CAS) calculations to evaluate the accuracy of DF and HF/DF methods for the highly delocalized, strongly correlated phenoxyl radical. Bond lengths and angles calculated by using DF and HF/DF methods appear as accurate as those obtained by using the UMP2 method. The correlation functional of Vosko, Wilk, and Nusair combined with Slater’s exchange functional (SVWN) gives a structure closest to the best available CASSCF calculations, with the structures from three parameter hybrid HF/DF methods (B3P86 and B3LYP) nearly as good. Electronic spin density ratios computed by using DF methods are closest to experimentally derived spin density ratios, UHF spin densities are the worst, and the hybrid HF/DF methods give intermediate quality spin density ratios. Unscaled vibrational frequencies from the DF and HF/DF methods are closer to experimentally measured frequencies than uniformly scaled UHF or UMP2 frequencies. Unscaled frequencies calculated by using the B3LYP method, for example, differ from the nine experimentally observed frequencies by an average of only 22 cm−1. The vibrational mode of phenoxyl radical observed experimentally at 1552 cm−1 is confirmed to correspond to a C=C stretching vibration and the band observed at 1505 cm−1 is primarily a C–O stretch. Vibrational modes of phenoxyl radical shift to lower frequencies upon deuteration and the larger shift of the C=C stretch, compared to the C–O stretch, confirms their assignment. Thus density functional methods give electronic spin density ratios, vibrational frequencies, mode assignments, and isotopic frequency shifts in good agreement with experiment and with more expensive UNO-CAS//CASSCF calculations for phenoxyl radical.Keywords
This publication has 66 references indexed in Scilit:
- Resonance Raman studies of substituent effects on the electronic structure of phenoxyl radicalsThe Journal of Physical Chemistry, 1988
- Ab initio calculations of vibrational spectra and their use in the identification of unusual moleculesChemical Reviews, 1986
- Ultraviolet resonance Raman characterization of photochemical transients of phenol, tyrosine, and tryptophanJournal of the American Chemical Society, 1986
- The resonance Raman spectrum of phenoxyl radicalThe Journal of Chemical Physics, 1984
- The time-resolved resonance raman spectrum of pulse radiolytically produced phenoxyl radicalChemical Physics Letters, 1983
- The resonance Raman spectra of aqueous phenoxy and phenoxy-d5 radicalsThe Journal of Chemical Physics, 1982
- Determination of the acidity constants of some phenol radical cations by means of electron spin resonanceJournal of the Chemical Society, Faraday Transactions 2: Molecular and Chemical Physics, 1976
- Hydroxyl radical reactions with phenols and anilines as studied by electron spin resonanceThe Journal of Physical Chemistry, 1974
- 935. Electron spin resonance studies of oxidation. Part IV. Some benzenoid compoundsJournal of the Chemical Society, 1964
- 35. Aryloxy-radicals. Part I. Electron spin resonance spectra of radicals from some substituted monohydric phenolsJournal of the Chemical Society, 1964