Your browser doesn't support javascript.
loading
Full-dimensional quantum dynamics of CO in collision with H2.
Yang, Benhui; Balakrishnan, N; Zhang, P; Wang, X; Bowman, J M; Forrey, R C; Stancil, P C.
Afiliação
  • Yang B; Department of Physics and Astronomy and the Center for Simulational Physics, The University of Georgia, Athens, Georgia 30602, USA.
  • Balakrishnan N; Department of Chemistry, University of Nevada, Las Vegas, Nevada 89154, USA.
  • Zhang P; Department of Chemistry, Duke University, Durham, North Carolina 27708, USA.
  • Wang X; Department of Chemistry, Emory University, Atlanta, Georgia 30322, USA.
  • Bowman JM; Department of Chemistry, Emory University, Atlanta, Georgia 30322, USA.
  • Forrey RC; Department of Physics, Penn State University, Berks Campus, Reading, Pennsylvania 19610, USA.
  • Stancil PC; Department of Physics and Astronomy and the Center for Simulational Physics, The University of Georgia, Athens, Georgia 30602, USA.
J Chem Phys ; 145(3): 034308, 2016 Jul 21.
Article em En | MEDLINE | ID: mdl-27448888
ABSTRACT
Inelastic scattering computations are presented for collisions of vibrationally and rotationally excited CO with H2 in full dimension. The computations utilize a newly developed six-dimensional potential energy surface (PES) and the previously reported four-dimensional V12 PES [P. Jankowski et al., J. Chem. Phys. 138, 084307 (2013)] and incorporate full angular-momentum coupling. At low collision energies, pure rotational excitation cross sections of CO by para-, ortho-, and normal-H2 are calculated and convolved to compare with recent measurements. Good agreement with the measured data is shown except for j1 = 0 → 1 excitation of CO for very low-energy para-H2 collisions. Rovibrational quenching results are presented for initially excited CO(v1j1) levels with v1 = 1, j1 = 1-5 and v1 = 2, j1 = 0 for collisions with para-H2 (v2 = 0, j2 = 0) and ortho-H2 (v2 = 0, j2 = 1) over the kinetic energy range 0.1-1000 cm(-1). The total quenching cross sections are found to have similar magnitudes, but increase (decrease) with j1 for collision energies above ∼300 cm(-1) (below ∼10 cm(-1)). Only minor differences are found between para- and ortho-H2 colliders for rovibrational and pure rotational transitions, except at very low collision energies. Likewise, pure rotational deexcitation of CO yields similar cross sections for the v1 = 0 and v1 = 1 vibrational levels, while rovibrational quenching from v1 = 2, j1 = 0 is a factor of ∼5 larger than that from v1 = 1, j1 = 0. Details on the PES, computed at the CCSD(T)/aug-cc-pV5Z level, and fitted with an invariant polynomial method, are also presented.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article