“…5,6 Metallic behavior can be induced, also as in graphene, by means of electric field effects or by doping, and the corresponding Fermi surface is typically made up of inequivalent Fermi pockets, [7][8][9][10][11][12] defining a valley degree of freedom which is strongly entangled with the spin degree of freedom, 13 and it can be further controlled and manipulated, opening promising perspectives for spintronics. At high carrier concentrations (n ∼ 10 14 cm −2 ), and in the presence of high-κ dielectrics, MoS 2 has also been shown to undergo a superconducting transition, with a doping-dependent critical temperature T c (n) which exhibits a maximum as a function of n and drops to zero at sufficiently large values of n. 14,15 A ferromagnetic behavior has also been reported in MoS 2 , [16][17][18][19] and it has been related to edges or to the existence of defects. 20,21 The magnetic properties of MoS 2 nanoribbons indicate that the electron-electron interactions are non-negligible.…”