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• W2081616504 abstract "The experimental techniques of H (Rydberg) atom photofragment translational spectroscopy and resonance-enhanced multiphoton ionisation time-of-flight spectroscopy have been used to investigate the dynamics of H atom loss processes from gas phase 4-fluorophenol (4-FPhOH), 4-chlorophenol (4-ClPhOH) and 4-bromophenol (4-BrPhOH) molecules, following excitation at many wavelengths, λphot, in the range between their respective S1–S0 origins (284.768 nm, 287.265 nm and 287.409 nm) and 216 nm. Many of the Total Kinetic Energy Release (TKER) spectra obtained from photolysis of 4-FPhOH show structure, the analysis of which reveals striking parallels with that reported previously for photolysis of bare phenol (M. G. D. Nix, A. L. Devine, B. Cronin, R. N. Dixon and M. N. R. Ashfold, J. Chem. Phys., 2006, 125, 133318). The data demonstrates the importance of O–H bond fission, and that the resulting 4-FPhO co-fragments are formed in a select fraction of their available vibrational state density. All spectra recorded at λphot ≥ 238 nm show a feature centred at TKER ∼5500 cm−1. These H atom fragments show no recoil anisotropy, and are rationalised in terms of initial S1 ← S0 (π* ← π) excitation and subsequent dissociation via two successive radiationless transitions: internal conversion to ground (S0) state levels carrying sufficient O–H stretch vibrational energy to allow efficient transfer to (and round) the Conical Intersection (CI) between the S0 and S2(1πσ*) Potential Energy Surfaces (PESs) at larger RO–H, en route to H atoms and ground state 4-FPhO products. The vibrational energy disposal in the 4-FPhO products indicates that parent mode ν16a promotes non-adiabatic coupling at the S0/S2 CI. Spectra recorded at λphot ≤ 238 nm reveal a faster (but still isotropic) distribution of recoiling H atoms, centred at TKER ∼12 000 cm−1, attributable to H + 4-FPhO products formed when the optically excited 1ππ* molecules couple directly with the 1πσ* PES. Parent mode ν16b is identified as the dominant coupling mode at the S1(1ππ*)/S2(1πσ*) CI, and the resulting 4-FPhO radical co-fragments display progressions in ν18b (the C–O in-plane wagging mode) and ν7a (an in-plane ring breathing mode involving significant C–O stretching motion). Analysis of all structured TKER spectra yields a C–F bond dissociation energy: D0(H–OC6H4F) = 29 370 ± 50 cm−1. The photodissociation of 4-ClPhOH shows many similarities, though the 4-ClPhO products formed together with faster H atoms at shorter wavelengths (λphot ≤ 238 nm, by coupling through the S1/S2 CI) show activity in an alternative ring breathing mode (ν19a rather than ν7a). Spectral analysis yields D0(H–OC6H4Cl) = 29 520 ± 50 cm−1. H atom formation via O–H bond fission is (at best) a very minor channel in the photolysis of 4-BrPhOH at all wavelengths investigated. Time-dependent density functional theory calculations suggest that this low H atom yield is because of competition from the alternative C–Br bond fission channel, and that the analogous C–Cl bond fission may be responsible for the weakness of the one photon-induced H atom signals observed when photolysing 4-ClPhOH at longer wavelengths." @default.
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• W2081616504 date "2007-01-01" @default.
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• W2081616504 title "Near-UV photolysis of substituted phenols, I: 4-fluoro-, 4-chloro- and 4-bromophenol" @default.
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• W2081616504 doi "https://doi.org/10.1039/b704146b" @default.
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