4.4 Article

Product rotational Franck-Condon oscillations in HOD (Jka,kc) dissociation

Journal

MOLECULAR PHYSICS
Volume 108, Issue 7-9, Pages 905-914

Publisher

TAYLOR & FRANCIS LTD
DOI: 10.1080/00268970903563469

Keywords

photodissociation; HOD; Franck-Condon; Oscillations

Funding

  1. Chinese Academy of Sciences
  2. Ministry of Science and Technology
  3. National Science Foundation of China
  4. University of Bristol Senior Research Fellowship

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The technique of H(D) atom photofragment translation spectroscopy has been used to investigate the dissociation of jet-cooled HOD molecules following excitation to individual rovibrational levels of its (C) over tilde((1)B(1)) Rydberg state near 124 nm. Spectra have been recorded for both the D + OH and H + OD dissociation channels. The branching ratios between OH/OD(X (2)Pi, high nu, low N), OH/OD(X (2)Pi, low nu, high N), and OH/OD(A (2)Sigma(+)) channels vary between different parent rotational levels, and between the OH and OD products. The variation between the OH and OD channels can be attributed to an isotopic mass effect on the rotational axes which influences non-adiabatic coupling strengths. In addition, there is a population alternation with product rotational quantum number N for the OH/OD(X, high nu, low N) product, most striking for the OH case, the sense of which is correlated with the value of the parent pseudo-quantum number K(a)(1). It is shown that this is a consequence of recoil forces which lead to a closing of the HOD angle to near 90 degrees accompanying non-adiabatic transfer from the (C) over tilde state to the (A) over tilde((1)B(1)) state. The oscillation in population then derives from the symmetry properties around this angle of the product rotational wavefunctions. This suggests that the symmetry-induced population oscillation can only occur for a narrowly defined angular dissociation path. Model calculations also explain the different structure of the spin-orbit doubled low N band heads for each nu(OH/OD) which also alternates for even and odd K(a)(1). The necessary conditions to observe these phenomena are discussed.

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