  Interactions are responsible for intriguing physics, e.g. emergence of exotic
ground states and excitations, in a wide range of systems. Here we
theoretically demonstrate that dipole-dipole interaction leads to bosonic
eigen-excitations with average spin ranging from zero to above $\hbar$ in
magnets with uniformly magnetized ground states. These exotic excitations can
be interpreted as quantum coherent conglomerates of spin $\hbar$ magnons, the
eigen-excitations when the dipolar interactions are disregarded. We further
find that the eigenmodes in an easy-axis antiferromagnet are spin-zero
quasiparticles instead of the widely believed spin $\pm \hbar$ magnons. The
latter re-emerge when the symmetry is broken by a sufficiently large applied
magnetic field. The average spin greater than $\hbar$ is accompanied by vacuum
fluctuations and may be considered to be a weak form of frustration.
