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J. Chem. Phys. 131, 124307 (2009); http://dx.doi.org/10.1063/1.3123426 (14 pages)

Bound states of the OH(2Π)–HCl complex on ab initio diabatic potentials

Gerrit C. Groenenboom, Anna V. Fishchuk, and Ad van der Avoird

Theoretical Chemistry, IMM, Radboud University Nijmegen, Heyendaalseweg 135, 6525 AJ Nijmegen, The Netherlands

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(Received 3 February 2009; accepted 2 April 2009; published online 24 September 2009; publisher error corrected 12 October 2009)

The bound states of the open-shell OH(2Π)–HCl complex were calculated in four dimensions with a diabatic model using electronic states that correlate asymptotically with the ground and excited spin-orbit states of the OH(2Π) fragment and the ground state of the HCl fragment. The ab initio diabatic potentials and their analytic expansion applied in these calculations were obtained earlier by Wormer et al. [J. Chem. Phys. 122, 244325 (2005)] . In addition to the four-dimensional calculations, we considered a (3+1)-dimensional model in which the intermolecular distance coordinate R is adiabatically separated from the remaining coordinates. Both models include the important spin-orbit coupling in the OH fragment. Energy levels and parity splittings were computed for a total angular momentum of J = ½ and math; rotational constants and other spectroscopic parameters were extracted from these calculations. The vibrationally averaged geometry in the ground state of the complex is planar and this state is more or less localized near the minimum in the lowest adiabatic potential with binding energy De = 1123 cm−1; the dissociation energy D0 with respect to OH(2Π3/2) and HCl is found to be 685 cm−1. The splitting between the 2Π3/2 and 2Π1/2 spin-orbit states of free OH is largely reduced by the anisotropic interaction with HCl through the off-diagonal diabatic coupling potential and these states are strongly mixed. Low lying rovibronic states that correlate with the OH(2Π3/2) ground state were found at 14 cm−1 for total angular momentum projection quantum number |Ω| = math and 26 cm−1 for |Ω| = ½, relative to the ground state with |Ω| = ½. The OH–HCl stretch fundamental frequency equals to 93.6 cm−1, the lowest bend excited states (involving a coupled bend motion of both fragments) were found in the region of 150–160 cm−1 above the ground state. Especially in the excited states important nonadiabatic effects are observed that involve both of the asymptotically degenerate adiabatic electronic states. In some of these excited states the vibrationally averaged geometry is nonplanar.

© 2009 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. THEORY
  3. BOUND STATE CALCULATIONS
    1. 4D calculations
    2. (3+1)D calculations
  4. RESULTS AND DISCUSSION
    1. Assignment of bound states
    2. Interpretation and discussion
  5. SUMMARY AND CONCLUSIONS

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KEYWORDS and PACS

PACS

  • 33.20.Vq

    Vibration-rotation analysis

  • 33.20.Wr

    Vibronic, rovibronic, and rotation-electron-spin interactions

  • 31.15.aj

    Relativistic corrections, spin-orbit effects, fine structure; hyperfine structure

  • 33.15.Ry

    Ionization potentials, electron affinities, molecular core binding energy

  • 33.20.Sn

    Rotational analysis

ARTICLE DATA

PUBLICATION DATA

ISSN

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

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