Roothaan-Hartree-Fock wave functions for cations and anions in Slater-type basis sets with doubly even tempered exponents

1995 ◽  
Vol 91 (1-2) ◽  
pp. 47-66 ◽  
Author(s):  
Toshikatsu Koga ◽  
Eri Shibata ◽  
Ajit J. Thakkar
1995 ◽  
Vol 91 (1) ◽  
pp. 47
Author(s):  
Toshikatsu Koga ◽  
Eri Shibata ◽  
Ajit J. Thakkar

1994 ◽  
Vol 88 (4) ◽  
pp. 273-283 ◽  
Author(s):  
Toshikatsu Koga ◽  
Hiroshi Tatewaki ◽  
Ajit J. Thakkar

1985 ◽  
Vol 63 (7) ◽  
pp. 1812-1828 ◽  
Author(s):  
S. Huzinaga ◽  
M. Klobukowski ◽  
H. Tatewaki

We have started to prepare a new family of high-quality Gaussian-type function basis sets capable of producing near Hartree–Fock atomic and molecular wave functions. A conspicuous feature of the family of basis sets is that many of the exponent parameters are shared among s-, p-, d-, and f-basis functions. In the present paper we report the first phase of the work covering atoms from Li to Ar, together with near Hartree–Fock calculations on N2, CO, Na2, and P2 as the applications. A modified form of Raffenetti's contraction scheme is used.


2001 ◽  
Vol 73 (4) ◽  
pp. 511-517 ◽  
Author(s):  
EUSTÁQUIO V. R. DE CASTRO ◽  
FRANCISCO E. JORGE

The generator coordinate Hartree-Fock method is used to generate adapted Gaussian basis sets for the atoms from Li (Z=3) through Xe (Z=54). In this method the Griffin-Hill-Wheeler-Hartree-Fock equations are integrated through the integral discretization technique. The wave functions generated in this work are compared with the widely used Roothaan-Hartree-Fock wave functions of Clementi and Roetti (1974), and with other basis sets reported in the literature. For all atoms studied, the errors in our total energy values relatively to the numerical Hartree-Fock limits are always less than 7.426 mhartree.


1987 ◽  
Vol 62 (1) ◽  
pp. 91-95 ◽  
Author(s):  
Herbert F.M. da Costa ◽  
Milan Trsic ◽  
J.R. Mohallem

1993 ◽  
Vol 48 (1-2) ◽  
pp. 325-333
Author(s):  
R. O. Horenian ◽  
W. Weyrich

Abstract High-purity powder samples of lithium and sodium azide (LiN3 , NaN3), cyanate (LiOCN, NaOCN) and hydrogen fluoride (LiFHF, NaFHF) were studied by means of 59.54 keV Compton spectroscopy. The measured isotropic Compton profiles were corrected for multiple scattering and transformed to spherically averaged reciprocal form factors Ba(s).The experimental results are compared with theoretical reciprocal form factors obtained from Hartree-Fock calculations with different types of basis sets (Gaussian-and Slater-type orbitals, with and without polarisation functions) both for the free ions and for several kinds of clusters. The importance of intraionic and interionic interaction for the description of chemical bonding in these compounds is pointed out and discussed.


2006 ◽  
Vol 05 (02) ◽  
pp. 223-233 ◽  
Author(s):  
F. E. JORGE ◽  
L. M. BERNARDO ◽  
E. P. MUNIZ

The performance of the previously proposed double zeta valence quality plus polarization functions (DZP) and augmented DZP (ADZP) basis sets is tested at the Hartree–Fock, second-order Møller–Plesset, and density functional levels of theory for the electronic ground state of the second-row diatomic hydrides. Total energy, second-order correlation energy, dissociation energy, bond length, vibrational frequency, and dipole moment are calculated and compared with results obtained with popular basis sets reported in the literature. It is shown that the DZP and ADZP basis sets in general provides better accuracy for a similar number of basis functions.


Author(s):  
Roberto Nada ◽  
John B. Nicholas ◽  
Maureen I. McCarthy ◽  
Anthony C. Hess
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