MCD C-Term Signs, Saturation Behavior, and Determination of Band Polarizations in
Randomly Oriented Systems with Spin S ≥ 1/2. Applications to S = 1/2 and S = 5/2
posted on 1999-03-19, 00:00authored byFrank Neese, Edward I. Solomon
The magnetic circular dichroism (MCD) properties of a spin-allowed transition from an orbitally nondegenerate
ground state manifold A to an orbitally nondegenerate excited state manifold J in the presence of spin−orbit
coupling (SOC) are derived for any S ≥ 1/2. Three physically distinct mechanisms are identified that lead to
MCD intensity and depend on SOC between excited states which leads to a sum rule and SOC between the
ground state and other excited states that leads to deviations from the sum rule. The model is valid for any
symmetry of the magnetic coupling tensors and arbitrary transition polarizations. The S = 1/2 case is analytically
solved, and the determination of linear polarizations from MCD saturation magnetization data is discussed. For
all mechanisms the MCD intensity is proportional to the spin-expectation values of the ground state sublevels
which are conveniently generated from a spin-Hamiltonian (SH). For Kramers systems with large zero-field splittings
(ZFSs) this allows the contribution from each Kramers doublet to the total MCD intensity to be related through
their effective g-values, therefore significantly reducing the number of parameters required to analyze experimental
data. The behavior of high-spin systems is discussed in the limits of weak, intermediate, and strong ZFS relative
to the Zeeman energy. The model remains valid in the important case of intermediate ZFS where the ground state
sublevels may cross as a function of applied magnetic field and there are significant off-axis contributions to the
MCD intensity due to a change of the electron spin quantization axis. The model permits calculation of MCD
C-term signs from molecular wave functions, and explicit expressions are derived in terms of MOs for S = 1/2
and S = 5/2. Two examples from the literature are analyzed to demonstrate how the C-term signs can be evaluated
by a graphical method that gives insight into their physical origin.