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Nuclear attraction integrals computational results

Some Computational Results on Nuclear Attraction Integrals... [Pg.205]

Now we will calculate one by one aU die integrals fliat appear in the Dirac matrix equation. The integral y ) = because die scalar product leads to the nuclear attraction integral with a hydrogen-like atomic orbital, and diis gives the result above (see Appendix H available at booksite.elsevier.com/978-0-444-59436-5, p. e91). The next integral can be computed as follows ... [Pg.138]

Therefore, in order to obtain Va (r) at point r, it is sufficient to calculate the distances of the point from any of the nuclei (trivial) as well as the one-electron integrals, which appear after inserting into Eq. (14.34) Pa(/) = 2 I a./C ) - Within the LCAO MO approximation, the electron density distribution pa represents the sum of products of two atomic orbitals (in general centered at two different points). As a result, the task reduces to calculating typical one-electron three-center integrals of the nuclear attraction type (cf.. Chapter 8 and Appendix P available at booksite.elsevier.com/978-0-444-59436-5), because the third center corresponds to the point r (Fig. 14.14). There is no computational problem with this for contemporary quantum chemistry. [Pg.923]


See other pages where Nuclear attraction integrals computational results is mentioned: [Pg.252]    [Pg.257]    [Pg.115]    [Pg.412]    [Pg.15]    [Pg.923]    [Pg.38]    [Pg.362]   
See also in sourсe #XX -- [ Pg.205 , Pg.206 ]




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