4.6 Article

State-to-state photodissociation dynamics of CO2 around 108 nm: the O(1S) atom channel

期刊

PHYSICAL CHEMISTRY CHEMICAL PHYSICS
卷 22, 期 11, 页码 6260-6265

出版社

ROYAL SOC CHEMISTRY
DOI: 10.1039/c9cp06919d

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资金

  1. National Natural Science Foundation of China [21873099, 21673232, 21922306, 21773213, 21403207, 21773236]
  2. Strategic Priority Research Program of the Chinese Academy of Sciences [XDB 17000000]
  3. Chemical Dynamics Research Center [21688102]
  4. International Partnership Program of Chinese Academy of Sciences [121421KYSB20170012]
  5. Natural Science Research Project of Education Department of Anhui Province [KJ2019A0521]
  6. Open Foundation of State Key Laboratory [SKLMRD-K202003, SKLMRD-K201906]

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State-to-state photodissociation of carbon dioxide (CO2) via the 3p(1)pi(u) Rydberg state was investigated by the time-sliced velocity map ion imaging technique (TSVMI) using a tunable vacuum ultraviolet free electron laser (VUV FEL) source. Raw images of the O(S-1) products resulting from the O(S-1) + CO(X-1 sigma(+)) channel were acquired at the photolysis wavelengths between 107.37 and 108.84 nm. From the vibrational resolved O(S-1) images, the product total kinetic energy releases and the vibrational state distributions of the CO(X-1 sigma(+)) co-products were obtained, respectively. It is found that vibrationally excited CO co-products populate at as high as v = 6 or 7 while peaking at v = 1 and v = 4, and most of the individual vibrational peaks present a bimodal rotational structure. Furthermore, the angular distributions at all studied photolysis wavelengths have also been determined. The associated vibrational-state specific anisotropy parameters (beta) exhibit a photolysis wavelength-dependent feature, in which the beta-values observed at 108.01 nm and 108.27 nm are more positive than those at 107.37 nm and 107.52 nm, while the beta-values have almost isotropic behaviour at 108.84 nm. These experimental results indicate that the initially prepared CO2 molecules around 108 nm should decay to the 4(1)A ' state via non-adiabatic coupling, and dissociate in the 4(1)A ' state to produce O(S-1) + CO(X-1 sigma(+)) products with different dissociation time scales.

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