  Over the past decade, it has been proposed theoretically and confirmed
experimentally that long-range spin triplet (LRT) superconductivity can be
generated in ferromagnet-superconductor hybrids either by the presence of spin
textures (ST-LRT) or thanks to spin-orbit coupling (SOC-LRT). Nevertheless,
there has been no theoretical or experimental investigation to date suggesting
that both contributions could simultaneously exist within an experimental
system. To disentangle these contributions, we present a comprehensive study of
superconducting quasiparticle interference effects taking place inside a
ferromagnetic layer interfacing a superconductor, through the investigation of
above-gap conductance anomalies (CAs) related to MacMillan-Rowell resonances.
The bias dependence of the CAs has been studied under a wide range of in-plane
(IP) and out-of-plane (OOP) magnetic fields in two types of epitaxial,
V/MgO/Fe-based ferromagnet-superconductor junctions with interfacial spin-orbit
coupling. We observe an anisotropy of the CAs amplitude under small IP and OOP
magnetic fields while remaining weakly affected by high fields, and implement
micromagnetic simulations to help us distinguish between the ST-LRT and SOC-LRT
contributions. Our findings suggest that further exploration of Fabry-P\'erot
type interference effects in electron transport could yield valuable insights
into the hybridization between superconductors and ferromagnets induced by
spin-orbit coupling and spin textures.
