Comparison of the polarizabilities and hyperpolarizabilities obtained from finite basis set and finite difference Hartree–Fock calculations for diatomic molecules: III. The ground states of N2, CO and BF

A comparison is made of the accuracy by which the electric dipole polarizability αzz and hyperpolarizability βzzz can be calculated by using the finite basis set approach (the algebraic approximation) and finite difference method in calculations employing the Hartree-Fock model. The numerical and algebraic methods were tested on the ground states of H2, LiH, BH and FH molecules at their respective experimental equilibrium geometries. For the FH molecule at its experimental equilibrium geometry, a sequence of distributed universal even-tempered basis sets have been used to explore the convergence pattern of the total energy, dipole moment and polarizabilities. The comparison of finite difference and finite basis set methods is extended to geometries for which the nuclear separation, RFH, lies in the range 1.5-2.2 b. The methods give consistent results to within 1% or better. In the case of the FH molecule the dependence of truncation errors of the total energy, dipole moment and polarizabilities on the geometry have been studied and are shown to be negligible.

[1]  D. Moncrieff,et al.  A comparison of finite basis set and finite difference Hartree-Fock calculations for the InF and TlF molecules , 1998 .

[2]  Michael W. Schmidt,et al.  Effective convergence to complete orbital bases and to the atomic Hartree–Fock limit through systematic sequences of Gaussian primitives , 1979 .

[3]  Pekka Pyykkö,et al.  Fully numerical hartree-fock methods for molecules , 1986 .

[4]  W. Kołos,et al.  Accurate Electronic Wave Functions for the H 2 Molecule , 1960 .

[5]  D. Moncrieff,et al.  A comparison of finite basis set and finite difference methods for the ground state of the CS molecule , 1994 .

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

[7]  Finite basis set versus finite difference and finite element methods , 1993 .

[8]  A. Weiss,et al.  ANALYTICAL SELF-CONSISTENT FIELD FUNCTIONS FOR THE ATOMIC CONFIGURATIONS 1s$sup 2$, 1s$sup 2$2s, AND 1s$sup 2$2s$sup 2$ , 1960 .

[9]  T. Dunning,et al.  Ab initio characterization of the structure and energetics of the ArHF complex , 1997 .

[10]  A. D. Buckingham,et al.  Direct Method of Measuring Molecular Quadrupole Moments , 1959 .

[11]  J. Kobus Vectorizable algorithm for the (multicolour) successive overrelaxation method , 1994 .

[12]  D. Moncrieff,et al.  A universal basis set for high-precision molecular electronic structure studies: correlation effects in the ground states of , CO, BF and , 1998 .

[13]  Angela K. Wilson,et al.  The Effect of Basis Set Superposition Error (BSSE) on the Convergence of Molecular Properties Calculated with the Correlation Consistent Basis Sets , 1998 .

[14]  J. Kobus Diatomic Molecules: Exact Solutions of HF Equations , 1997 .

[15]  Anthony J. Stone,et al.  Distributed multipole analysis, or how to describe a molecular charge distribution , 1981 .

[16]  S. F. Boys,et al.  The calculation of small molecular interactions by the differences of separate total energies. Some procedures with reduced errors , 1970 .

[17]  A. Buckingham Molecular quadrupole moments , 1959 .

[18]  Leif Laaksonen,et al.  A Numerical Hartree-Fock Program for Diatomic Molecules , 1996 .

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

[20]  J. Applequist,et al.  Fundamental relationships in the theory of electric multipole moments and multipole polarizabilities in static fields , 1984 .

[21]  C. C. J. Roothaan,et al.  Self-Consistent Field Theory for Open Shells of Electronic Systems , 1960 .

[22]  G. Herzberg Molecular Spectra and Molecular Structure IV. Constants of Diatomic Molecules , 1939 .

[24]  D. Moncrieff,et al.  Comparison of the electric moments obtained from finite basis set and finite-difference Hartree-Fock calculations for diatomic molecules , 2000 .

[25]  J. Kobus Finite-difference versus finite-element methods , 1993 .

[26]  D. Moncrieff,et al.  A universal basis set for high precision electronic structure studies , 1995 .

[27]  H. B. Jansen,et al.  Non-empirical molecular orbital calculations on the protonation of carbon monoxide , 1969 .

[28]  David E. Woon,et al.  Gaussian basis sets for use in correlated molecular calculations. IV. Calculation of static electrical response properties , 1994 .

[29]  A. D. McLean,et al.  Theory of Molecular Polarizabilities , 1967 .

[30]  D. Moncrieff,et al.  Visualization of deficiencies in approximate molecular wave functions: the local orbital energy function for the matrix Hartree—Fock model , 2001 .

[31]  D. Moncrieff,et al.  A universal basis set for high-precision molecular electronic structure studies , 1994 .

[32]  George Maroulis,et al.  A systematic study of basis set, electron correlation, and geometry effects on the electric multipole moments, polarizability, and hyperpolarizability of HCl , 1998 .

[33]  D. Moncrieff,et al.  On the accuracy of the algebraic approximation in molecular electronic structure calculations. III. Comparison of matrix Hartree-Fock and numerical Hartree-Fock calculations for the ground state of the nitrogen molecule , 1993 .

[34]  D. Moncrieff,et al.  A comparison of finite difference and finite basis set Hartree-Fock calculations for the ground state potential energy curve of CO , 1994 .

[35]  Thom H. Dunning,et al.  Gaussian basis sets for use in correlated molecular calculations. V. Core-valence basis sets for boron through neon , 1995 .

[36]  Angela K. Wilson,et al.  Gaussian basis sets for use in correlated molecular calculations. VI. Sextuple zeta correlation consistent basis sets for boron through neon , 1996 .

[37]  P. Schleyer Encyclopedia of computational chemistry , 1998 .

[38]  Stephen Wilson,et al.  On the accuracy of the algebraic approximation in molecular electronic structure calculations: V. Electron correlation in the ground state of the nitrogen molecule , 1996 .