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Convergence for Problems with Several Stationary Points<br />

no optimization method can make that a guarantee. Furthermore, it cannot be tested if the minimum<br />

found is a local or the global minimum without knowledge of the whole surface. Depending on the<br />

start guess and the optimization approach, an optimization can converge to different stationary<br />

points. Further, it is necessary to decide in which subspace of orbital rotations the desired solution<br />

should be found, since a solution representing a stable stationary point in one subspace is not<br />

necessarily stable in another.<br />

Orbital rotations can be divided in real and complex rotations and each of those can be further<br />

divided in singlet and triplet rotations. Each of those can then again be divided in rotations within<br />

the different point group symmetries. Generally, we do not consider the complex rotations, and we<br />

only optimize in the real space. Further, when optimizing a closed shell wave function, only the<br />

total-symmetric part of the singlet rotations is considered. A stationary point in the subspace of real,<br />

total-symmetric, singlet rotations can be shown through elementary arguments to be a stationary<br />

point for all types of rotations. However, a stationary point can both be a maximum, a saddle point<br />

or a minimum. A way to realize if the stationary point also is a minimum is to evaluate the Hessian<br />

eigenvalues. This is done within the subspace in which the solution should be stable. If a negative<br />

Hessian eigenvalue is found in the subspace of singlet rotations, the stationary point is said to have<br />

a singlet instability and if a negative Hessian eigenvalue is found in the subspace of triplet rotations,<br />

it is said to have a triplet instability 54,56 . Triplet instabilities are connected to breaking the symmetry<br />

between α and β orbitals. If a triplet instability is found, a minimum with a lower energy than the<br />

current stationary point can be found, if the α and β parts are allowed to differ, typically leading to<br />

2<br />

a solution which is not an eigenfunction of Ŝ . Hence, the lower minimum could be found by an<br />

unrestricted HF (UHF) optimization. A singlet instability found in the total-symmetric subspace<br />

indicates that the current stationary point is a saddle point and a minimum with lower energy exists<br />

within the subspace. If a singlet instability is found outside the total-symmetric subspace, orbitals of<br />

different symmetries should be mixed to decrease the energy further, changing the symmetry of the<br />

resulting wave function.<br />

The aufbau ordering rule assumes that occupying the orbitals of lowest energy also leads to the<br />

lowest Hartree-Fock energy. This cannot be proven to always apply for restricted HF as it can for<br />

UHF 57 . Thus it is a risk when the aufbau ordering is forced upon an optimization, that a lower<br />

energy with the aufbau ordering broken could exist. However in a study by Dardenne et. al. 58 , in<br />

which different ordering schemes were tested, they found in all cases that the minimum was an<br />

aufbau solution. The aufbau ordering was broken only for saddle points. In our schemes we always<br />

apply the aufbau ordering rule, but if the RH step is level shifted to the end of the optimization, it<br />

can force the convergence to a non-aufbau solution.<br />

45

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