We show that topological phases should be realizable in readily available and well-studied heterostructures in spintronics: helical ferromagnet-superconducting junctions. The particular heterostructures we address exhibit finite-range proximity effects leading to nodal superconductors with Majorana modes localized well away from the interface between helical-ferromagnet and  superconductor. To show this, we implement a Bogoliubov–de Gennes proximity numerical scheme and illustrate in a concrete fashion the wave functions belong to zero energy flat bands. In the process we establish consistency with a simple analytical model.