  We discuss a geometric approach to confining a Dirac neutral particle with a
permanent magnetic dipole moment interacting with external fields to a
hard-wall confining potential in the Minkowski spacetime through noninertial
effects. We discuss the behaviour of external fields induced by noninertial
effects, and a case where relativistic bound states can be achieved in
analogous way to having a Dirac particle confined to a quantum dot. We show
that this confinement of a Dirac neutral particle analogous to a quantum dot
arises from noninertial effects that give rise to the geometry of the manifold
playing the role of a hard-wall confining potential. We also discuss the
possible use of this mathematical model in studies of noninertial effects on
condensed matter systems described by the Dirac equation.
