  In classes of Weyl semimetals where the symmetry protects nodes with higher
than unit charge, the nematic Weyl liquid appears as interactions destroy this
underlying symmetry. In the symmetry-broken phase, the multiple-charge nodes
are split into objects of unit charge, the position of which in momentum space
is determined by the nematic order parameter. We examine the phenomenology of
this phase, focusing on topological edge states and Landau levels. We find that
the symmetry-broken phase itself, as well as the orientation of the nematic
order, are identifiable from the resulting edge states. We also find that the
nematic order couples to an in-plane magnetic field, indicating that it can be
controlled in situ via an external field. Finally, we provide an estimate for
the critical coupling where spontaneous symmetry-breaking occurs for contact
interaction.
