en:reactivity:radical_addition:pmo
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| - | where the summing is done over a set of spin orbitals and //γ// is the resonance integral on the atomic orbitals (//AOs//) of reactive centers //r// and //s//. | + | where the summing is done over a set of spin orbitals and //γ// is the resonance integral on the atomic orbitals (//AO//) of reactive centers //r// and //s//. |
| Using RHF π-orbitals of isolated reagents we calculated CT energies (// | Using RHF π-orbitals of isolated reagents we calculated CT energies (// | ||
| - | So, // | + | So, // |
| Although //FMO// cannot be approved as a true approximation (see [[# | Although //FMO// cannot be approved as a true approximation (see [[# | ||
| - | The use of //localized molecular orbitals// can serve as another approach. For example, using a projective procedure we managed to build a pair of //localized MOs// of a monomer that combined ≈95% of π-density both of occupied and unoccupied shells. It is a pity that even 5% is too great an error for such sums as **Eq. (1)**. So, a desire arises to " | + | The use of //localized molecular orbitals// can serve as another approach. For example, using a projective procedure we managed to build a pair of //localized MOs// of a monomer that combined ≈95% of π-density both of occupied and unoccupied shells. It is a pity that even 5% is too great an error for such sums as **Eq. (1)**. So, a desire arises to " |
| - | Now, we are going to propose an [[.: | + | Now, we are going to propose an [[.: |
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en/reactivity/radical_addition/pmo.1790144733.txt.gz · Last modified: by abc
