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J. Chem. Phys. 127, 154306 (2007); http://dx.doi.org/10.1063/1.2795722 (7 pages)

Observation of three weakly bound valence states of I2

Trevor Ridley, Kenneth P. Lawley, and Robert J. Donovan

School of Chemistry, The University of Edinburgh, West Mains Road, Edinburgh EH9 3JJ, Scotland, United Kingdom

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(Received 28 July 2006; accepted 17 September 2007; published online 16 October 2007)

Structured emission in the gas phase to two weakly bound valence states that correlate with the third dissociation limit, I*(2P1/2)+I*(2P1/2), designated as (bb), from two third tier ion-pair states of I2 correlating with I(1S0)+I+(1D2), the 1g(1D2), and F′0u+(1D2) states, has been observed for the first time. The 1u(bb) state is shown to be bound by 377±2 cm−1 and molecular constants have been determined. Vibrational structure in the 0g+(bb) state could not be resolved but the spectrum is consistent with the state being bound by 435 cm−1. The relative integrated intensities of the emissions from both ion-pair states to various valence states have also been measured, and some aspects are rationalized in terms of the electronic configurations of the upper and lower states. Bound levels of a previously uncharacterized 1g(ab) valence state have also been observed in emission from the γ1u(3P2) ion-pair state. The lower state is shown to be bound by 270±2 cm−1 and molecular constants have been determined.

© 2007 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. EXPERIMENT
  3. RESULTS AND DISCUSSION
    1. Simulation of the fluorescence spectra
    2. Emission from the 1g(1D2) ion-pair state
    3. Emission from the F′0u+(1D2) ion-pair state
    4. Emission from the γ1u(3P2) ion-pair state
    5. Distribution of emission intensities
  4. CONCLUSIONS

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KEYWORDS and PACS

PACS

  • 33.15.Mt

    Rotation, vibration, and vibration-rotation constants

  • 33.15.Fm

    Bond strengths, dissociation energies

  • 33.70.Fd

    Absolute and relative line and band intensities

ARTICLE DATA

PUBLICATION DATA

ISSN

0021-9606 (print)  
1089-7690 (online)

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