Fig. 3: Magnetotransport data at CN.
From: Spin-orbit proximity in MoS2/bilayer graphene heterostructures
a Conductivity as a function of B⊥ and D at T = 30 mK. This plot represents the (D, B) phase diagram of SOC proximitized BLG. Phase (I) is a gapped phase with a layer-polarized wave function. Phase (II) is another gapped phase that has been attributed to the canted antiferromagnetic phase in pristine BLG41,62. The phase boundary between phases (I) and (II) (straight dotted lines) is described in Supplementary Note 10. Phase (III) is a weakly insulating phase that arises from the presence of spin-gaps in the single-particle spectrum. b σxx plotted against D for B⊥ = 0 and two values of in-plane magnetic field: B∥ = 0 (violet) and B∥ = 1.8 T (orange). c Linecuts of panel (a) at D = 0 (violet) and D = Dc (orange). The black dashed and dotted lines highlight the 1/B dependence of the conductivity. d Differential conductance Gd = dI/dVSD as a function of the voltage bias VSD and magnetic field B⊥ at D = 0. The dotted line highlights Eg ∝ B⊥ (see discussion in Supplementary Note 11).
