  A resolution over the existence of magnetic charges has eluded the high
energy physics community for centuries, and their search has gained momentum as
recent models predict these may be observable at current colliders. They appear
in field theories in two forms: the widely studied but heavily suppressed
monopole with structure (soliton) and the not-so-well-covered point-like
monopole. The latter was first proposed by Dirac as the source of a singular
magnetic field and in effect symmetrises Maxwell's equations. Following this
line of research, work by S. Baines et al. analysed these sources as matter
fields that carry spins 0, $\frac{1}{2}$, or 1, in an effective field theory
that is perturbative for monopoles produced at threshold where the coupling
strength $g(\beta)$ is suppressed. All three cases are currently under
investigation by the MoEDAL collaboration at CERN, and the theoretical
expressions for kinematic distributions proposed in this work serve as guides
to these searches. The cross section distributions in each case are derived
from a \emph{U}(1) invariant gauge theory. It is not assumed that, like the
electron, the monopole's magnetic moment is generated through spin interactions
at minimal coupling, as it may be quite large. Instead, the analytical
expressions in the spin $\frac{1}{2}$ and $1$ cases are kept completely general
through the inclusion of a phenomenological parameter $\kappa$, related to the
gyromagnetic ratio $g_R=1+\kappa$. In fact, the inclusion of this parameter
gives the effective theory validity in the high energy limit if the magnetic
coupling scales with the particle's velocity $\beta=\frac{v}{c}$.
