Conspectus
Complexes
of lanthanide(III) ions are being actively studied because
of their unique ground and excited state properties and the associated
optical and magnetic behavior. In particular, they are used as emissive
probes in optical spectroscopy and microscopy and as contrast agents
in magnetic resonance imaging (MRI). However, the design of new complexes
with specific optical and magnetic properties requires a thorough
understanding of the correlation between molecular structure and electric
and magnetic susceptibilities, as well as their anisotropies. The
traditional Judd–Ofelt–Mason theory has failed to offer
useful guidelines for systematic design of emissive lanthanide optical
probes. Similarly, Bleaney’s theory of magnetic anisotropy
and its modifications fail to provide accurate detail that permits
new paramagnetic shift reagents to be designed rather than discovered.
A key determinant of optical and magnetic behavior in f-element
compounds is the ligand field, often considered as an electrostatic
field at the lanthanide created by the ligands. The resulting energy
level splitting is a sensitive function of several factors: the nature
and polarizability of the whole ligand and its donor atoms; the geometric
details of the coordination polyhedron; the presence and extent of
solvent interactions; specific hydrogen bonding effects on donor atoms
and the degree of supramolecular order in the system. The relative
importance of these factors can vary widely for different lanthanide
ions and ligands. For nuclear magnetic properties, it is both the
ligand field splitting and the magnetic susceptibility tensor, notably
its anisotropy, that determine paramagnetic shifts and nuclear relaxation
enhancement.
We review the factors that control the ligand field
in lanthanide
complexes and link these to aspects of their utility in magnetic resonance
and optical emission spectroscopy and imaging. We examine recent progress
in this area particularly in the theory of paramagnetic chemical shift
and relaxation enhancement, where some long-neglected effects of zero-field
splitting, magnetic susceptibility anisotropy, and spatial distribution
of lanthanide tags have been accommodated in an elegant way.