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Structure Coulomb integral computation

Most modern Hiickel programs will accept the molecular structure as the input. In older programs, the input requires the kind of atoms present in the molecule (characterized by their Coulomb integrals a) and the way in which they are connected (described by the resonance integrals. ). These are fed into the computer in the form of a secular determinant. Remember that the Coulomb and resonance integrals cannot be calculated (the mathematical expression of the Hiickel Hamiltonian being unknown) and must be treated as empirical parameters. [Pg.37]

It must be emphasized that the computation of at small k is very delicate, and must not be crudely pursued. There is a great deal of structure in the integrand of the multiple wavenumber integrals due to incipient singularities of the bare Coulomb potential and of the repeated energy denominators which are characteristic of perturbation expansions. In fact, the contributions of the individual Feynman graphs had already been calculated analytically in the... [Pg.49]

As presented, the Roothaan SCF process is carried out in a fully ab initio manner in that all one- and two-electron integrals are computed in terms of the specified basis set no experimental data or other input is employed. As described in Appendix F, it is possible to introduce approximations to the coulomb and exchange integrals entering into the Fock matrix elements that permit many of the requisite F, v elements to be evaluated in terms of experimental data or in terms of a small set of fundamental orbital-level coulomb interaction integrals that can be computed in an ab initio manner. This approach forms the basis of so-called semi-empirical methods. Appendix F provides the reader with a brief introduction to such approaches to the electronic structure problem and deals in some detail with the well known Htickel and CNDO- level approximations. [Pg.351]

This structure is computationally advantageous for the ERI calculation and the numerical integration of the auxiliary density. The Coulomb fitting coefficients Xjf are obtained by minimizing the following Conlomb energy error ... [Pg.205]


See other pages where Structure Coulomb integral computation is mentioned: [Pg.207]    [Pg.138]    [Pg.262]    [Pg.128]    [Pg.13]    [Pg.346]    [Pg.472]    [Pg.261]    [Pg.351]    [Pg.17]    [Pg.102]    [Pg.70]    [Pg.139]    [Pg.135]    [Pg.135]    [Pg.584]    [Pg.262]    [Pg.19]    [Pg.616]    [Pg.147]    [Pg.234]    [Pg.194]    [Pg.312]    [Pg.68]    [Pg.79]    [Pg.195]    [Pg.234]    [Pg.338]    [Pg.450]    [Pg.386]    [Pg.562]    [Pg.1652]    [Pg.169]    [Pg.258]    [Pg.251]    [Pg.223]    [Pg.349]   
See also in sourсe #XX -- [ Pg.207 ]




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