‘Ab initio’ Molecular Orbital Calculations

The electronic energy of a molecule can be calculated by treating the overall electronic wavefunction as being a product of molecular orbitals (strictly as a Slater determinant of molecular orbitals to satisfy the Pauli principle; we should also include the electron spin). 

So we can write a molecular wavefunction as:

Y = y1y2y3y4yn                  (27)

Each molecular orbital, yi, is written as a linear combination of atomic orbitals (the familiar LCAO approximation):

                    (28)

The molecular orbitals can be found by the Hartree-Fock method.  The Hamiltonian operator contains terms for the potential and kinetic energy of the electrons.  It includes the interactions between the nuclei and the electrons, and the electron-electron repulsion.  The molecular orbitals are found by making an initial guess at the coefficients.  Then the determinant

½H–ES½= 0                            (29)

H contains the Hamiltonian matrix elements, and S the overlap matrix elements.  Solving this determinant gives the molecular orbital energies E, which are substituted into the secular equations to give new values of the coefficients ci.  This whole process is repeated until the coefficients do not change from one cycle to the next.  The orbitals are then described as self-consistent, and this process as a self-consistent field procedure. 

      Each molecular orbital is made up of a combination of atomic orbitals:

                    (28)

The set of atomic orbitals (fk) used is called a basis set.  When one function is used for each filled atomic orbital (e.g. using 1s, 2s and 2p orbitals for a carbon atom, this basis set is called a minimal basis.  Using more functions than this will improve the calculation – it will increase the flexibility and quality of the overall wavefunction.  From the variational principle we know that a better wavefunction will give a lower energy.  The bigger the basis set, the better the calculation.  If a very large number of functions – a very large basis set – is used to represent the atomic orbitals, we approach the Hartree-Fock limiting energy: the lowest energy (best molecular wavefunction) that can be achieved by the Hartree-Fock method. 

Correlation energy