“…Located at the edges of 1D devices, they are responsible for the emergence of stretched nonlocal electron states 13,19 allowing for distance independent tunnelling, 20 crossed Andreev reflection, 21 teleportationlike coherent transfer of a fermion 22 and fractional Josephson effects. 23,24 Their effects emerge in a variety of platforms: quantum wires immersed in a p-wave superconductor, 13,19,20 cold atomic systems, 25 topological insulator-superconductor magnetic structures, 22,26,27 semiconductor heterostructures, [28][29][30][31] superconducting wires, 32 Josephson arrays 33 and spin systems 34 In addition, they may be relevant excitations also in conventional s-wave superconductors. 35 It is worth to stress here that, when a superconductor is coupled to a conducting wire in a SN-junction, the Majorana mode hybridizes with the conducting electrons at the normal side of the junction.…”