期刊
PHYSICAL CHEMISTRY CHEMICAL PHYSICS
卷 15, 期 18, 页码 6879-6892出版社
ROYAL SOC CHEMISTRY
DOI: 10.1039/c3cp51108a
关键词
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资金
- Leverhulme Trust
- EPSRC [EP/G041717/1, EP/J006602, EP/H003401, EP/J007153]
- University of Warwick
- European Research Council under the European Union [258990]
- Royal Society
- EPSRC [EP/H003401/1, EP/J006602/1, EP/J007153/1, EP/G041717/1] Funding Source: UKRI
- Engineering and Physical Sciences Research Council [EP/J006602/1, EP/G041717/1, EP/H003401/1, EP/J007153/1] Funding Source: researchfish
Ultrafast time-resolved velocity map ion imaging (TR-VMI) and time-resolved ion-yield (TR-IY) methods are utilised to reveal a comprehensive picture of the electronic state relaxation dynamics in photoexcited catechol (1,2-dihydroxybenzene). After excitation to the S-1 ((1)pi pi(star)) state between 280.5 (the S-1 origin band, S-1(v = 0)) to 243 nm, the population in this state is observed to decay through coupling onto the S-2 ((1)pi sigma(star)) state, which is dissociative with respect to the non-hydrogen bonded 'free' O-H bond (labelled O-1-H). This process occurs via tunnelling under an S-1/S-2 conical intersection (CI) on a timeframe of 5-11 ps, resulting in O-1-H bond fission along S-2. Concomitant formation of ground state catechoxyl radicals (C6H5O2(X)), in coincidence with translationally excited H-atoms, occurs over the same timescale as the S-1 state population decays. Between 254-237 nm, direct excitation to the S-2 state is also observed, manifesting in the ultrafast (similar to 100 fs) formation of H-atoms with high kinetic energy release. From these measurements we determine that the S-1/S-2 CI lies similar to 3700-5500 cm(-1) above the S-1(v = 0) level, indicating that the barrier height to tunnelling from S-1(v = 0) -> S-2 is comparable to that observed in the related 'benchmark' species phenol (hydroxybenzene). We discuss how a highly 'vibrationally-enhanced' tunnelling mechanism is responsible for the two orders of magnitude enhancement to the tunnelling rate in catechol, relative to that previously determined in phenol (>1.2 ns), despite similar barrier heights. This phenomenon is a direct consequence of the non-planar S-1 excited state minimum structure (C-1 symmetry) in catechol, which in turn yields relaxed symmetry constraints for vibronic coupling from S-1(v = 0) -> S-2 - a scenario which does not exist for phenol. These findings offer an elegant example of how even simple chemical modifications (ortho-hydroxy substitution) to a fundamental, biologically relevant, UV chromophore, such as phenol, can have profound effects on the ensuing excited state dynamics.
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