Abstract

A numerical application of linear-molecule symmetry properties, described by the D ∞ h point group, is formulated in terms of lower-order symmetry groups D n h with finite n. Character tables and irreducible representation transformation matrices are presented for D n h groups with arbitrary n-values. These groups can subsequently be used in the construction of symmetry-adapted ro-vibrational basis functions for solving the Schrödinger equations of linear molecules. Their implementation into the symmetrisation procedure based on a set of “reduced” vibrational eigenvalue problems with simplified Hamiltonians is used as a practical example. It is shown how the solutions of these eigenvalue problems can also be extended to include the classification of basis-set functions using ℓ, the eigenvalue (in units of ℏ) of the vibrational angular momentum operator L ^ z . This facilitates the symmetry adaptation of the basis set functions in terms of the irreducible representations of D n h . 12 C 2 H 2 is used as an example of a linear molecule of D ∞ h point group symmetry to illustrate the symmetrisation procedure of the variational nuclear motion program Theoretical ROVibrational Energies (TROVE).

Highlights

  • The geometrical symmetry of a centrosymmetric linear molecule in its equilibrium geometry is described by the D∞h point group

  • While the molecular vibrational states span the representations of this point group of infinite order, the symmetry properties of the combined rotation-vibration states must satisfy the nuclear-statistics requirements and transform according to the irreducible representations of the finite molecular symmetry group

  • As an illustration of the practical application of the finite Dnh group being used in place of D∞h, we show an example of the construction of the vibrational basis set in case of the linear molecule 12 C2 H2

Read more

Summary

Introduction

The geometrical symmetry of a centrosymmetric linear molecule in its equilibrium geometry is described by the D∞h point group (see Table 1). The particular problems associated with the symmetry description of linear molecules were described early on by Hougen [3], and by Bunker and Papoušek [4] The latter authors introduced the so-called Extended Molecular Symmetry (EMS) Group which, for a centrosymmetric linear molecule, is isomorphic to the D∞h point group. D∞h point group and thereby introduce the possibility of labelling these basis functions by the value of the vibrational angular momentum quantum number

Rotational and Vibrational Symmetry
General Structure
Irreducible Representations
Transformation Matrices
Symmetrization Using the TROVE Approach
Symmetrization
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.