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Administrator<br />

A variety of other basis sets, such as diffuse<br />

function basis sets and high angular momentum<br />

basis sets, are tailored to the properties of particular<br />

of models under investigation.<br />

The coefficients (C νi ) used for a given AO basis set<br />

(φ ν ) are derived from the solution of the Roothaan-<br />

Hall matrix equation with a diagonalized matrix of<br />

orbital energies, E.<br />

The Roothaan-Hall Matrix Equation<br />

This equation, shown below, includes the Fock<br />

matrix (F), the matrix of molecular orbital<br />

coefficients (C) from the LCAO approximation,<br />

the overlap matrix (S), and the diagonalized<br />

molecular orbital energies matrix (E).<br />

FC = SCE<br />

Since the Fock equations are a function of the<br />

molecular orbitals, they are not linearly<br />

independent. As such the equations must be solved<br />

using iterative, self-consistent field (SCF) methods.<br />

The initial elements in the Fock matrix are guessed.<br />

The molecular coefficients are calculated and the<br />

energy determined. Each subsequent iteration uses<br />

the results of the previous iteration until no further<br />

variation in the energy occurs (a self-consistent field<br />

is reached).<br />

Ab Initio vs. Semiempirical<br />

Ab initio (meaning literally “from first principles”)<br />

methods use the complete form of the Fock<br />

operator to construct the wave equation. The<br />

semiempirical methods use simplified Fock<br />

operators, in which 1-electron matrix elements and<br />

some of the two electron integral terms are replaced<br />

by empirically determined parameters.<br />

Both the SCF RHF and UHF methods<br />

underestimate the electron-electron repulsion and<br />

lead to electron correlation errors, which tend to<br />

overestimate the energy of a model. The use of<br />

configuration interaction (CI) is one method<br />

available to correct for this overestimation. For<br />

more information see “Configuration Interaction”<br />

on page 143.<br />

The Semi-empirical Methods<br />

Semiempirical methods can be divided into two<br />

categories: one-electron types and two-electron<br />

types. One-electron semiempirical methods use<br />

only a one-electron Hamiltonian, while twoelectron<br />

methods use a Hamiltonian which includes<br />

a two-electron repulsion term. Authors differ<br />

concerning the classification of methods with oneelectron<br />

Hamiltonians; some prefer to classify these<br />

as empirical.<br />

The method descriptions that follow represent a<br />

very simplified view of the semiempirical methods<br />

available in Chem3D and CS MOPAC. For more<br />

information see the online MOPAC manual.<br />

Extended Hückel Method<br />

Developed from the qualitative Hückel MO<br />

method, the Extended Hückel Method (EH)<br />

represents the earliest one-electron semiempirical<br />

method to incorporate both σ and p valence<br />

systems. It is still widely used, owing to its versatility<br />

and success in analyzing and interpreting groundstate<br />

properties of organic, organometallic, and<br />

inorganic compounds of biological interest. Built<br />

into Chem3D, EH is the default semiempirical<br />

method used to calculate data required for<br />

displaying molecular surfaces.<br />

The EH method uses a one-electron Hamiltonian<br />

with matrix elements defined as follows:<br />

H µµ = – I µ<br />

H µν = 0.5K( H µµ + H νν )S µν µ ≠ ν<br />

where I µ is the valence state ionization energy<br />

(VSIE) of orbital µ as deduced from spectroscopic<br />

data, and K is the Wolfsberg-Helmholtz constant<br />

142•<strong>Com</strong>putation Concepts<br />

<strong>CambridgeSoft</strong><br />

Quantum Mechanics Theory in Brief

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