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Application to the Allyl System

The basis set size of three implies that we will need to solve a 3 x 3 secular equation. Hiickel conventions (b)-(e) tell us the value of each element in the secular equation, so that Eq. (4.21) is rendered as [Pg.117]

The use of the KrOnecker delta to define the overlap matrix ensures that E appears only in the diagonal elements of the determinant. Since this is a 3 x 3 determinant, it may be expanded using Cramer s rule as [Pg.117]

Since a and P are negative by definition, the lowest energy solution is a + /ip. To find the MO associated with this energy, we employ it in the set of linear Eqs. (4.20), together [Pg.117]

Some fairly trivial algebra reduces these equations to flz = J2ai [Pg.118]

While there are infinitely many values of ai, a, and aj. which satisfy Eq. (4.28), the requirement that the wave function be normalized provides a final constraint in the form of Eq. (4.11). The unique values satisfying both equations are [Pg.118]


See other pages where Application to the Allyl System is mentioned: [Pg.116]    [Pg.106]   


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Allyl system

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