“…In the last decades, the conceptual problem was just studying SW propagation, which is inherently a two-dimensional problem, since a signal travelling along a waveguide can be embedded in one- (1D) or two-dimensional (2D) space, depending on the curvature 5 – 9 . Hence, the research exploration has mainly involved structures displaying 1D/2D magnetization textures, either periodic 10 – 13 or aperiodic 14 – 17 , while structures with in-plane periodicity, but inhomogeneous along the perpendicular direction, have been poorly explored so far. However, exploring the third dimension is crucial indeed, because a 3D distribution of the magnetization offers a new degree of freedom, which in general allows, from one side, to fit more functionality into a smaller space, and hence to considerably increase the density of elements in magnonic devices 18 , 19 , and from the other, further possibilities for the SW dynamics and transport (e.g., vertical magnon transport, nonreciprocal coupling 20 – 22 ).…”