The discrete variable representation of a triatomic Hamiltonian in bond length–bond angle coordinates

The discrete variable representation (DVR) is used to calculate vibrational energy levels of H2O and SO2. The Hamiltonian is written in terms of bond length–bond angle coordinates and their conjugate momenta. It is shown that although these coordinates are not orthogonal and the appropriate kinetic energy operator is complicated, the discrete variable representation is quite simple and facilitates the calculation of vibrational energy levels. The DVR enables one to use an internal coordinate Hamiltonian without expanding the coordinate dependence of the kinetic energy or evaluating matrix elements numerically. The accuracy of previous internal coordinate calculations is assessed.

[1]  Bruce R. Johnson,et al.  Adiabatic separations of stretching and bending vibrations: Application to H2O , 1986 .

[2]  J. Light,et al.  Generalized discrete variable approximation in quantum mechanics , 1985 .

[3]  J. Light,et al.  Highly excited vibrational levels of "floppy" triatomic molecules: A discrete variable representation - Distributed Gaussian basis approach , 1986 .

[4]  L. Halonen,et al.  A simple curvilinear internal coordinate model for vibrational energy levels of hydrogen sulfide and , 1992 .

[5]  N. Handy,et al.  The variational method for the calculation of RO-vibrational energy levels , 1986 .

[6]  W. Domcke,et al.  Nuclear dynamics in resonant electron-molecule scattering beyond the local approximation: model calculations on dissociative attachment and vibrational excitation , 1984 .

[7]  D. O. Harris,et al.  Calculation of Matrix Elements for One‐Dimensional Quantum‐Mechanical Problems and the Application to Anharmonic Oscillators , 1965 .

[8]  J. Light,et al.  Efficient pointwise representations for vibrational wave functions: Eigenfunctions of H+3 , 1989 .

[9]  K. Yamanouchi,et al.  Vibrational level structure of highly excited SO2 in the electronic ground state. II. Vibrational assignment by dispersed fluorescence and stimulated emission pumping spectroscopy , 1990 .

[10]  D. Papoušek,et al.  Molecular vibrational-rotational spectra , 1982 .

[11]  J. Tennyson,et al.  The ab initio calculation of the vibrational‐rotational spectrum of triatomic systems in the close‐coupling approach, with KCN and H2Ne as examples , 1982 .

[12]  E. Sibert Rotationally induced vibrational mixing in formaldehyde , 1989 .

[13]  John C. Light,et al.  Theoretical Methods for Rovibrational States of Floppy Molecules , 1989 .

[14]  N. Handy,et al.  A variational method for the calculation of vibrational levels of any triatomic molecule , 1982 .

[15]  P. Jensen,et al.  A new Morse-oscillator based Hamiltonian for H3+: Extension to H2D+ and D2H+ , 1986 .

[16]  C. Hamilton,et al.  Stimulated Emission Pumping: New Methods in Spectroscopy and Molecular Dynamics , 1986 .

[17]  P. Jensen The potential energy surface for the electronic ground state of the water molecule determined from experimental data using a variational approach , 1989 .

[18]  A. S. Dickinson,et al.  Calculation of Matrix Elements for One‐Dimensional Quantum‐Mechanical Problems , 1968 .

[19]  T. Carrington,et al.  Fermi resonances and local modes in water, hydrogen sulfide, and hydrogen selenide , 1988 .

[20]  Ian M. Mills,et al.  Anharmonic force constant calculations , 1972 .

[21]  Joel M. Bowman,et al.  The self-consistent-field approach to polyatomic vibrations , 1986 .

[22]  David C. Clary,et al.  Potential optimized discrete variable representation , 1992 .

[23]  N. Handy,et al.  On the calculation of vibration-rotation energy levels of quasi-linear molecules , 1982 .

[24]  R. Wallace,et al.  Analytic quantum mechanics of the morse oscillator , 1976 .

[25]  D. Watt,et al.  A variational localized representation calculation of the vibrational levels of the water molecule up to 27 000 cm−1 , 1988 .