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Improvement of the LCAO MO

As we have seen the MO calculations of the last paragraph yielded a bond distance which was 25% too long and a dissociation energy which was 37% too low. How could the accuracy be improved  [Pg.108]

Comparison of the probability densities calculated for the approximate wavefunction P+ with those calculated from the exact wavefunction P shows that the probability density in the low-energy region near and in between the two nuclei is underestimated by some 40%. No wonder then that the calculations fail to reproduce the true strength of the bond  [Pg.108]

The simplest way to increase the probability density near the nuclei is to modify the Is orbitals  [Pg.108]

When the two nuclei are far apart, the best value for f is obviously equal to 1.0. In the other limiting situation, i.e. when the internuclear distance approaches zero, the Ht molecule is [Pg.108]

The calculations are carried out as outlined in the preceding section. Thus E is calculated from equation (7.10)  [Pg.109]


See other pages where Improvement of the LCAO MO is mentioned: [Pg.108]   


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