The magnetic structures of the actinides (i.e. those materials contain
ing 5 (f) under bar electrons) exhibit considerable complexity. The re
asons for this are a competition between exchange, often anisotropic i
n nature, crystal-held, and quadrupolar mteractions. Based on work on
compounds of the lanthanides (4 (f) under bar electrons), we have well
-developed mechanisms for understanding magnetic structures. The probl
em in the actinides is compounded by our inability to quantify the ind
ividual interactions. The reason for this difficulty is the hybridizat
ion that often occurs between the 5 (f) under bar electrons surroundin
g the actinide with both the conduction electrons and those of the sur
rounding atoms. To simplify this paper we shall discuss only one set o
f magnetic structures, those of the actinide monopnictides. These have
received perhaps the most attention of any series, and exemplify the
complexities and challenges of this held; one to which Jean Rossat-Mig
nod made seminal contributions.