  Exchange bias is a phenomenon critical to solid-state technologies that
require spin valves or non-volatile magnetic memory. The phenomenon is usually
studied in the context of magnetic interfaces between antiferromagnets and
ferromagnets, where the exchange field of the former acts as a means to pin the
polarization of the latter. In the present study, we report an unusual instance
of this phenomenon in the topological Weyl semimetal Co3Sn2S2, where the
magnetic interfaces associated with domain walls suffice to bias the entire
ferromagnetic bulk. Remarkably, our data suggests the presence of a hidden
order parameter whose behavior can be independently tuned by applied magnetic
fields. For micron-size samples, the domain walls are absent, and the exchange
bias vanishes, suggesting the boundaries are a source of pinned uncompensated
moment arising from the hidden order. The novelty of this mechanism suggests
exciting opportunities lie ahead for the application of topological materials
in spintronic technologies.
