Nonadiabatic dissociation dynamics in H 2 O: Competition between rotationally and nonrotationally mediated pathways
Author(s) -
Kaijun Yuan,
Yuan Cheng,
Lina Cheng,
Qing Guo,
Dongxu Dai,
Xiuyan Wang,
Xueming Yang,
Richard N. Dixon
Publication year - 2008
Publication title -
proceedings of the national academy of sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.011
H-Index - 771
eISSN - 1091-6490
pISSN - 0027-8424
DOI - 10.1073/pnas.0807719105
Subject(s) - photodissociation , excited state , chemistry , dissociation (chemistry) , excitation , atomic physics , rydberg formula , rydberg state , ground state , molecular physics , photochemistry , ionization , physics , ion , quantum mechanics , organic chemistry
The photochemistry of H(2)O in the VUV region is important in interstellar chemistry. Whereas previous studies of the photodissociation used excitation via unbound states, we have used a tunable VUV photolysis source to excite individual levels of the rotationally structured C state near 124 nm. The ensuing OH product state distributions were recorded by using the H-atom Rydberg tagging technique. Experimental results indicate a dramatic variation in the OH product state distributions and its stereodynamics for different resonant states. Photodissociation of H(2)O(C) in rotational states with k'(a) = 0 occurs exclusively through a newly discovered homogeneous coupling to the A state, leading to OH products that are vibrationally hot (up to v = 13), but rotationally cold. In contrast, for H(2)O in rotationally excited states with k'(a) > 0, an additional pathway opens through Coriolis-type coupling to the B state surface. This yields extremely rotationally hot and vibrationally cold ground state OH(X) and electronically excited OH(A) products, through 2 different mechanisms. In the case of excitation via the 1(10) <-- 0(00) transition the H atoms for these 2 product channels are ejected in completely different directions. Quantum dynamical models for the C-state photodissociation clearly support this remarkable dynamical picture, providing a uniquely detailed illustration of nonadiabatic dynamics involving at least 4 electronic surfaces.
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