40 research outputs found
Multiband ballistic transport and anisotropic commensurability magnetoresistance in antidot lattices of AB-stacked trilayer graphene
Ballistic transport was studied in a multiple-band system consisting of an
antidot lattice of AB-stacked trilayer graphene. The low temperature
magnetoresistance showed commensurability peaks arising from matching of the
antidot lattice period and radius of cyclotron orbits for each mono- and
bilayer-like band in AB stacked trilayer graphene. The commensurability peak of
the monolayer-like band appeared at a lower magnetic field than that of the
bilayer-like band, which reflects the fact that the Fermi surface of the
bilayer-like band is larger than that of monolayer-like band. Rotation of the
antidot lattice relative to the crystallographic axes of graphene resulted in
anisotropic magnetoresistance, which reflects the trigonally warped Fermi
surface of the bilayer-like band. Numerical simulations of magnetoresistance
that assumed ballistic transport in the mono- and bilayer-like bands
approximately reproduced the observed magnetoresistance features. It was found
that the monolayer-like band significantly contributes to the conductivity even
though its carrier density is an order smaller than that of the bilayer-like
band. These results indicate that ballistic transport experiments could be used
for studying the anisotropic band structure of multiple-band systems
Multilayer graphene shows intrinsic resistance peaks in the carrier density dependence
Since the advent of graphene, a variety of studies have been performed to
elucidate its fundamental physics, or to explore its practical applications.
Gate-tunable resistance is one of the most important properties of graphene and
has been studied in 1-3 layer graphene in a number of efforts to control the
band gap to obtain a large on-off ratio. On the other hand, the transport
property of multilayer graphene with more than three layers is less well
understood. Here we show a new aspect of multilayer graphene. We found that
four-layer graphene shows intrinsic peak structures in the gate voltage
dependence of its resistance at zero magnetic field. Measurement of quantum
oscillations in magnetic field confirmed that the peaks originate from the
specific band structure of graphene and appear at the carrier density for the
bottoms of conduction bands and valence bands. The intrinsic peak structures
should generally be observed in AB-stacked multilayer graphene. The present
results would be significant for understanding the physics of graphene and
making graphene FET devices
Low-energy band structure and even-odd layer number effect in AB-stacked multilayer graphene
How atoms acquire three-dimensional bulk character is one of the fundamental questions in materials science. Before addressing this question, how atomic layers become a bulk crystal might give a hint to the answer. While atomically thin films have been studied in a limited range of materials, a recent discovery showing how to mechanically exfoliate bulk crystals has opened up the field to study the atomic layers of various materials. Here, we show systematic variation in the band structure of high mobility graphene with one to seven layers by measuring the quantum oscillation of magnetoresistance. The Landau fan diagram showed distinct structures that reflected differences in the band structure, as if they were finger prints of multilayer graphene. In particular, an even-odd layer number effect was clearly observed, with the number of bands increasing by one for every two layers and a Dirac cone observed only for an odd number of layers. The electronic structure is significantly influenced by the potential energy arising from carrier screening associated with a gate electric field.This work was supported by MEXT KAKENHI Grant Number JP25107003
Shubnikov-de-Haas oscillation and possible modification of effective mass in CeTe3 thin films
Magnetoresistance measurements have been performed in CeTe3 thin film devices in a temperature range from 2.1 to 20 K up to 8 T. A clear Shubnikov-de-Haas oscillation was observed in the whole temperature range. The temperature dependence of the oscillation amplitude was found to deviate from the Lifshitz-Kosevich formula below the magnetic transition temperature at T-N1 approximate to 3 K. This indicates a significant interplay between the magnetic ordering and the conduction electrons, which could lead to a modification of the effective cyclotron mass. By analyzing the temperature dependence of the oscillation amplitude, we have estimated the effective mass, quantum lifetime and quantum mobility of the material both in the paramagnetic and antiferromagnetic states