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Anharmonic Densities of States for Vibrationally Excited I - (H 2 O), (H 2 O) 2 , and I - (H 2 O) 2 .

Authors :
Ma X
Yang N
Johnson MA
Hase WL
Source :
Journal of chemical theory and computation [J Chem Theory Comput] 2018 Aug 14; Vol. 14 (8), pp. 3986-3997. Date of Electronic Publication: 2018 Jul 20.
Publication Year :
2018

Abstract

Monte Carlo sampling calculations were performed to determine the anharmonic sum of states, N <subscript>anh</subscript> ( E), for I <superscript>-</superscript> (H <subscript>2</subscript> O), (H <subscript>2</subscript> O) <subscript>2</subscript> , and I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> versus internal energy up to their dissociation energies. The anharmonic density of states, ρ <subscript>anh</subscript> ( E), is found from the energy derivative of N <subscript>anh</subscript> ( E). Analytic potential energy functions are used for the calculations, consisting of TIP4P for H <subscript>2</subscript> O···H <subscript>2</subscript> O interactions and an accurate two-body potential for the I <superscript>-</superscript> ···H <subscript>2</subscript> O fit to quantum chemical calculations. The extensive Monte Carlo samplings are computationally demanding, and the use of computationally efficient potentials was essential for the calculations. Particular emphasis is directed toward I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> , and distributions of its structures versus internal energy are consistent with experimental studies of the temperature-dependent vibrational spectra. At their dissociation thresholds, the anharmonic to harmonic density of states ratio, ρ <subscript>anh</subscript> ( E)/ρ <subscript>h</subscript> ( E), is ∼2, ∼ 3, and ∼260 for I <superscript>-</superscript> (H <subscript>2</subscript> O), (H <subscript>2</subscript> O) <subscript>2</subscript> , and I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> , respectively. The large ratio for I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> results from the I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> → I <superscript>-</superscript> (H <subscript>2</subscript> O) + H <subscript>2</subscript> O dissociation energy being more than 2 times larger than the (H <subscript>2</subscript> O) <subscript>2</subscript> → 2H <subscript>2</subscript> O dissociation energy, giving rise to highly mobile H <subscript>2</subscript> O molecules near the I <superscript>-</superscript> (H <subscript>2</subscript> O) <subscript>2</subscript> dissociation threshold. This work illustrates the importance of treating anharmonicity correctly in unimolecular rate constant calculations.

Details

Language :
English
ISSN :
1549-9626
Volume :
14
Issue :
8
Database :
MEDLINE
Journal :
Journal of chemical theory and computation
Publication Type :
Academic Journal
Accession number :
29944367
Full Text :
https://doi.org/10.1021/acs.jctc.8b00300