An accurate analytic He-H2 potential energy surface from a greatly expanded set of ab initio energies

Details An accurate analytic He-H2 potential energy surface from a greatly expanded set of ab initio energies An accurate analytic He-H2 potential energy surface from a greatly expanded set of ab initio energies

2003-05-21

arxiv.org/abs/astro-ph/0305386v2

Journal of Chemical Physics, 119, 3187-3207 (2003)

Astronomy and Astrophysics

Astrophysics

(44 pages, including 13 figures) error in Eq. (9) has been corrected; Fortran PES, ab initio data available at http://www.ci

Scientific paper

10.1063/1.1589734

The interaction potential energy surface (PES) of He-H2 is of great importance for quantum chemistry, as the simplest test case for interactions between a molecule and a closed-shell atom. It is also required for a detailed understanding of certain astrophysical processes, namely collisional excitation and dissociation of H2 in molecular clouds, at densities too low to be accessible experimentally. A new set of 23703 ab initio energies was computed, for He-H2 geometries where the interaction energy was expected to be non-negligible. These have an estimated rms "random" error of about 0.2 millihartree and a systematic error of about 0.6 millihartree (0.4 kcal/mol). A new analytic He-H2 PES, with 112 parameters, was fitted to 20203 of these new ab initio energies (and to an additional 4862 points generated at large separations). This yielded an improvement by better than an order of magnitude in the fit to the interaction region, relative to the best previous surfaces (which were accurate only for near-equilibrium H2 molecule sizes). This new PES has an rms error of 0.95 millihartree (0.60 kcal/mole) relative to the the 14585 ab initio energies that lie below twice the H2 dissociation energy, and 2.97 millihartree (1.87 kcal/mole) relative to the full set of 20203 ab initio energies (the fitting procedure used a reduced weight for high energies, yielding a weighted rms error of 1.42 millihartree, i.e., 0.89 kcal/mole). These rms errors are comparable to the estimated error in the ab initio energies themselves; the conical intersection between the ground state and the first excited state is the largest source of error in the PES.

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