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Molecular Physics: An International Journal at the Interface Between Chemistry and Physics

Volume 108, Issue 7-9, 2010

Special Issue: A Special Issue on Spectroscopy and Dynamics in Honour of Richard N. Zare

Angular momentum polarisation in the O(1D) products of O2 photolysis via the B   state

Angular momentum polarisation in the O(1D) products of O2 photolysis via the B state

DOI:
10.1080/00268971003665113
Shiou-Min Wua, Dmitri Chestakova, Gerrit C. Groenenbooma, Wim J. van der Zandea, David H. Parkera*, Guorong Wub, Xueming Yangb & Claire Vallancec

pages 1145-1157

Available online: 20 Apr 2010

Abstract

The first fully allowed spectroscopic transition in O2 is the transition comprising the well-known Schumann–Runge bands and continuum. We report a velocity-map imaging study in which the O(1 D) angular momentum polarisation and O(3 P) spin–orbit branching ratios arising from this process have been measured. We show that direct 157 nm excitation into the Schumann–Runge continuum leads to extremely strong angular momentum polarisation in the O(1D) product. Comparison with previous studies indicates that this is a general feature of dissociation via the B state. The fine structure branching ratios in the co-fragment O(3P J=2,1,0) were measured to be 88.5 ± 1.6 : 9.7 ± 1.4 : 1.9 ± 0.4. Based on a consideration of the Massey parameter for the system, the data were modelled using theoretical calculations based on adiabatic and diabatic models of the dissociation. While both models were able to describe some aspects of the dissociation accurately, neither was able to predict both the fine structure branching ratios of the O(3P) products and the O(1D2) alignment. We have also investigated O(1D2) alignment arising from 203.8 and 205.5 nm photodissociation via the state of O2 vibrationally excited to v=6–11. As in the 157 nm photodissciation of vibrationally ground state O2, strong polarisation of the O(1D2) photofragments is observed.

Keywords

 

Details

  • Available online: 20 Apr 2010

Author affiliations

  • a Radboud University Nijmegen, Institute for Molecules and Materials, Heyendaalsweg 135, 6525 AJ, Nijmegen, The Netherlands
  • b State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, Liaoning, 116023, People's Republic of China
  • c Department of Chemistry, University of Oxford, Chemistry Research Laboratory, 12 Mansfield Rd, Oxford, OX1 3TA, UK

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