Intermolecular bending states and tunneling splittings of water trimer from rigorous 9D quantum calculations: II. Characterization of the states

03 June 2025, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

In a recent work we reported on the computation of intermolecular bending states in water trimer, a 9D problem when the monomers are treated as rigid and the intermonomer distances are fixed. In this paper we present the results of an effort to ascertain the vibrational character of those states. The large-amplitude, highly-coupled nature of these vibrations presents significant challenges in respect to their assignment. We introduce a new methodology, based on the use of symmetry coordinates for all nine of the torsional and librational degrees of freedom that constitute the intermolecular bending modes in the trimer, which addresses those challenges. The approach ultimately yields expressions for the bend eigenstates as expansions over small numbers of physically meaningful terms, from which the contributions of the torsional and librational excitations to a bending state can be identified and quantified. Results for approximately one hundred bending states with excitation energies below ∼ 560 cm−1 are presented.

Keywords

Quantum molecular calculation
Vibrational states
Hydrogen bond
Molecular trimer
Water trimer
Water
Intermolecular vibrations
Tunneling splitting
Assignment of states

Supplementary materials

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Description
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Title
Supplementary Material
Description
Tables containing the composition of the 9D bend eigenstates and the assignment of the components; Additional computational details (character table of the G6 MS group, details of the transformation of bend eigenstates from the coordinates employed for solving the Schrödinger equation to the coordinates used in the present analysis, details of isolating the G_6^† region, selection rules and transformation properties corresponding to the amplitude functions, calculation of the Fourier amplitudes, assignment of “upper” and “lower” to K = 3 and K = 6 pseudorotation excitations)
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