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Photochemistry of the Water Molecule: Adiabatic versus Nonadiabatic Dynamics
Water and light are two common constituents of both the earth’s atmosphere and interstellar space. Consequently, water photodissociation is a central component of the chemistry of these environments. Electronically excited molecules can dissociate adiabatically (on a single potential energy surface,...
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Published in: | Accounts of chemical research 2011-05, Vol.44 (5), p.369-378 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Water and light are two common constituents of both the earth’s atmosphere and interstellar space. Consequently, water photodissociation is a central component of the chemistry of these environments. Electronically excited molecules can dissociate adiabatically (on a single potential energy surface, or PES) or nonadiabatically (with transfer between PESs), and water serves as a prototype for understanding these two processes in unimolecular dissociation. In recent years, extensive experimental and theoretical studies have been focused on water photolysis, particularly on the primary product of the dissociation, the OH radical. The use of the high-resolution H-atom Rydberg tagging technique, in combination with various vacuum ultraviolet (VUV) sources, has spurred significant advances in water photochemistry. As the excitation energy increases, different excited electronic states of water can be reached, and the mutual interactions between these states increase significantly. In this Account, we present the most recent developments in water photodissociation that have been derived from the study of the four lowest electronic excited states. The à 1B1 state photodissociation of H2O has been studied at 157.6 nm and was found to be a fast and direct dissociation process on a single repulsive surface, with only vibrational excitation of the OH(X2Π) product. In contrast, the dissociation of the B̃ 1A1 state was found to proceed via two main routes: one adiabatic pathway leading to OH(A2Σ+) + H, and one nonadiabatic pathway to OH(X2Π) + H through conical intersections between the B̃ state and the ground state X̃ 1A1. An interesting quantum interference between two conical intersection pathways has also been observed. In addition, photodissociation of H2O between 128 and 133 nm has been studied with tunable VUV radiation. Experimental results illustrate that excitation to the different unstable resonances of the state has very different effects on the OH(X2Π) and OH(A2Σ+) product channels. The C̃ 1B1 state of H2O is a predissociative Rydberg state with fully resolved rotational structures. A striking variation in the OH product state distribution and its stereodynamics has been observed for different rotational states. There are two kinds of nonadiabatic dissociation routes on the C̃ state. The first involves Renner−Teller (electronic Coriolis) coupling to the B̃ state, leading to rotationally hot and vibrationally cold OH products. The second goes through a newl |
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ISSN: | 0001-4842 1520-4898 |
DOI: | 10.1021/ar100153g |