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Transport Signatures Of Quantum Phase Transitions And The Interplay Of Geometry And Topology In Nodal Materials

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Figure

Figure 3.1: Domain walls in bilayer graphene can be induced by applying a perpendicular electricfield and varying either the interlayer stacking (a) or the electric field direction (b)
Figure 3.4: The regions in interaction space for which tunneling processes become relevant (∆ <in Eqs
Figure 3.5: The eight angular variables in the full formulation of the S-matrix, seven of which arelinearly independent
Figure 3.7: RG flow of the variables Tto quadratic order in the interactions0/π, which control the pinching off of the junction, calculated ϵ+/− (Eq
+7

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