Theoretical studies have predicted that interactions
between magnetic
skyrmions and antiskyrmions give rise to various properties, such
as unique arrangements, pair annihilation, topological transformation,
and rectilinear and trochoidal motions that do not appear in only
skyrmions or antiskyrmions. Recently, experimental studies have discovered
that a Heusler material with the anisotropic Dzyaloshinskii–Moriya
interaction shows a coexisting phase at 268 K and in-plane magnetic
field-induced topological transformation of elliptical skyrmions and
square-shaped antiskyrmions. Therefore, experimentally observing the
coexisting phase and the topological transformation could be promising
for developing skyrmion–antiskyrmion-based spintronics. However,
such interactions and the detailed transformation mechanism remain
unrevealed and unclear, respectively. Using Lorentz transmission electron
microscopy experiments and micromagnetic simulations, we comprehensively
study the properties in a coexisting phase of skyrmions and antiskyrmions
in a Heusler material, Mn1.3Pt1.0Pd0.1Sn. Control of dipolar interaction (the sample thickness) allows
us to realize a room-temperature coexisting phase. We find that the
topological transformation occurs stochastically rather than deterministically,
which can be explained by considering the magnetic point group and
the direction of an in-plane magnetic field. We further observe isotropic
long-range repulsive interaction between skyrmions and antiskyrmions
in contrast to the conventional thought of the relative-position-
and helicity-dependent short-range pairwise interactions, and deformation
of skyrmions and antiskyrmions depending on the distance between them.
Our simulations show that the deformation exerts significant influence
on the magnetic energies and the energy landscape, contributing to
the interaction. Our results provide insight into coexisting phases
of skyrmions and antiskyrmions and a guide for developing skyrmion–antiskyrmion-based
spintronics.