We report on magneto-transport measurements on low-density, large-area
monolayer epitaxial graphene devices grown on SiC. We observe temperature
(T)-independent crossing points in the longitudinal
resistivity ρxx, which are signatures of the
insulator-quantum Hall (I-QH) transition, in all three devices. Upon converting
the raw data into longitudinal and Hall conductivities σxx
and σxy, in the most disordered device, we observed
T-driven flow diagram approximated by the semi-circle law
as well as the T-independent point in
σxy near
e2/h. We discuss our
experimental results in the context of the evolution of the zero-energy Landau
level at low magnetic fields B. We also compare the observed
strongly insulating behaviour with metallic behaviour and the absence of the
I-QH transition in graphene on SiO2 prepared by mechanical
exfoliation.
We have performed magnetotransport measurements on multilayer epitaxial graphene. By increasing the driving current I through our graphene devices while keeping the bath temperature fixed, we are able to study Dirac fermion heating and current scaling in such devices. Using zero-field resistivity as a self thermometer, we are able to determine the effective Dirac fermion temperature (TDF) at various driving currents. At zero field, it is found that TDF ∝ I≈1/2. Such results are consistent with electron heating in conventional two-dimensional systems in the plateau-plateau transition regime. With increasing magnetic field B, we observe an I-independent point in the measured longitudinal resistivity ρxx which is equivalent to the direct insulator-quantum Hall (I-QH) transition characterized by a temperature-independent point in ρxx. Together with recent experimental evidence for direct I-QH transition, our new data suggest that such a transition is a universal effect in graphene, albeit further studies are required to obtain a thorough understanding of such an effect.
The development of graphene electronic devices produced by industry relies on efficient control of heat transfer from the graphene sheet to its environment. In nanoscale devices, heat is one of the major obstacles to the operation of such devices at high frequencies. Here we have studied the transport of hot carriers in epitaxial graphene sheets on 6H-SiC (0001) substrates with and without hydrogen intercalation by driving the device into the non-equilibrium regime. Interestingly, we have demonstrated that the energy relaxation time of the device without hydrogen intercalation is two orders of magnitude shorter than that with hydrogen intercalation, suggesting application of epitaxial graphene in high-frequency devices which require outstanding heat exchange with an outside cooling source.
By changing the measurement temperature (T), one can vary the effective sample size so as to study the renormalization group (RG) (or T-driven) flow of a semiconductor, a topological insulator, or a graphene device in the complex conductivity plane.
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