Trigonal warping, pseudodiffusive transport, and finite-system version of the Lifshitz transition in magnetoconductance of bilayer-graphene Corbino disks
arXiv:1511.04705 · doi:10.1103/PhysRevB.93.075419
Abstract
Using the transfer matrix in the angular-momentum space we investigate the impact of trigonal warping on magnetotransport and scaling properties of a ballistic bilayer graphene in the Corbino geometry. Although the conductivity at the charge-neutrality point and zero magnetic field exhibits a one-parameter scaling, the shot-noise characteristics, quantified by the Fano factor and the third charge-transfer cumulant , remain pseudodiffusive. This shows that the pseudodiffusive transport regime in bilayer graphene is not related to the universal value of the conductivity but can be identified by higher charge-transfer cumulants. For Corbino disks with larger radii ratios the conductivity is suppressed by the trigonal warping, mainly because the symmetry reduction amplifies backscattering for normal modes corresponding to angular-momentum eigenvalues . Weak magnetic fields enhance the conductivity, reaching the maximal value near the crossover field , where () is the nearest-neighbor intra- (inter-)layer hopping integral, is the skew-interlayer hopping integral, and () is the outer (inner) disk radius. For magnetic fields we observe quasiperiodic conductance oscillations characterized by the decreasing mean value , where . The conductivity, as well as higher charge-transfer cumulants, show beating patterns with an envelope period proportional to . This constitutes a qualitative difference between the high-field () magnetotransport in the case (earlier discussed in Ref. [1]) and in the case, providing a finite-system analog of the Lifshitz transition.
Minor revisions; new Ref. [41]. A version accepted for publication in Physical Review B
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