Characterization of molecular orbitals by counting nodal regions

The number of nodal regions can be used as an index for characterizing molecular orbitals. A computer program has been developed to count the number of nodal regions, based on the labeling and contraction algorithms. This program is applied to the water molecule, the hydrogen sulfide molecule, the hydrogen atomic orbitals, the Rydberg excited states of ethylene, dissociation of carbon monoxide, and CASSCF calculations of formaldehyde. Because the number of nodal regions is independent of the coordinate system, the method is applicable even when the molecular structure changes drastically as in bond rotation or bond elongation. Changes of nodal regions with bond elongation are investigated for carbon monoxide. A prescription for problems arising with basis set expansion techniques is also given. © 2005 Wiley Periodicals, Inc. J Comput Chem 26: 325–333, 2005

[1]  Nicholas C. Handy,et al.  Exact solution (within a double-zeta basis set) of the schrodinger electronic equation for water , 1981 .

[2]  Mark S. Gordon,et al.  General atomic and molecular electronic structure system , 1993, J. Comput. Chem..

[3]  Henry F. Schaefer,et al.  The photodissociation of formaldehyde: A coupled cluster study including connected triple excitations of the transition state barrier height for H2CO→H2+CO , 1989 .

[4]  G. Choppin,et al.  The shapes of the f orbitals , 1964 .

[5]  D. Griffiths,et al.  Introduction to Quantum Mechanics , 1960 .

[6]  E. Dubois,et al.  Digital picture processing , 1985, Proceedings of the IEEE.

[7]  H. Korsch On the nodal behaviour of eigenfunctions , 1983 .

[8]  K. Hirao,et al.  Transition state barrier height for the reaction H2CO→H2+CO studied by multireference Mo/ller–Plesset perturbation theory , 1997 .

[9]  U. Nagashima,et al.  Development of a program for MCSCF calculations with large basis sets , 1988 .

[10]  Daniel C. Harris,et al.  Symmetry and spectroscopy , 1978 .

[11]  E. L. Short,et al.  Quantum Chemistry , 1969, Nature.

[12]  Kensaku Mori,et al.  Distance Transformation and Skeletonization of 3D Pictures and Their Applications to Medical Images , 2000, Digital and Image Geometry.

[13]  K. Hirao,et al.  Multireference Møller–Plesset method with a complete active space configuration interaction reference function , 2001 .

[14]  W. A. Lester,et al.  Formaldehyde: Abinitio MCSCF+CI transition state for H2CO → CO+H2 on the S0 surface , 1983 .

[15]  Random-walk approach to mapping nodal regions of N -body wave functions: Ground-state Hartree--Fock wave functions for Li--C , 1992 .

[16]  E. Bright Wilson,et al.  Symmetry, nodal surfaces, and energy ordering of molecular orbitals , 1975 .

[17]  Geerd H. F. Diercksen,et al.  Intelligent software: The OpenMol program , 1994 .

[18]  B. Roos,et al.  A complete active space SCF method (CASSCF) using a density matrix formulated super-CI approach , 1980 .

[19]  T. H. Dunning Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .

[20]  T. Dunning,et al.  Electron affinities of the first‐row atoms revisited. Systematic basis sets and wave functions , 1992 .

[21]  G. G. Hall,et al.  Single determinant wave functions , 1961, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[22]  H. Tatewaki,et al.  Excited states of ethylene interpreted in terms of perturbed Rydberg series , 2003 .

[23]  E. Villaseñor Introduction to Quantum Mechanics , 2008, Nature.