scholarly journals Upstream modes and antidots poison graphene quantum Hall effect

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
N. Moreau ◽  
B. Brun ◽  
S. Somanchi ◽  
K. Watanabe ◽  
T. Taniguchi ◽  
...  

AbstractThe quantum Hall effect is the seminal example of topological protection, as charge carriers are transmitted through one-dimensional edge channels where backscattering is prohibited. Graphene has made its marks as an exceptional platform to reveal new facets of this remarkable property. However, in conventional Hall bar geometries, topological protection of graphene edge channels is found regrettably less robust than in high mobility semi-conductors. Here, we explore graphene quantum Hall regime at the local scale, using a scanning gate microscope. We reveal the detrimental influence of antidots along the graphene edges, mediating backscattering towards upstream edge channels, hence triggering topological breakdown. Combined with simulations, our experimental results provide further insights into graphene quantum Hall channels vulnerability. In turn, this may ease future developments towards precise manipulation of topologically protected edge channels hosted in various types of two-dimensional crystals.

Science ◽  
2019 ◽  
Vol 363 (6422) ◽  
pp. 54-57 ◽  
Author(s):  
Fabien Lafont ◽  
Amir Rosenblatt ◽  
Moty Heiblum ◽  
Vladimir Umansky

The quantum Hall effect, observed in a two-dimensional (2D) electron gas subjected to a perpendicular magnetic field, imposes a 1D-like chiral, downstream, transport of charge carriers along the sample edges. Although this picture remains valid for electrons and Laughlin’s fractional quasiparticles, it no longer holds for quasiparticles in the so-called hole-conjugate states. These states are expected, when disorder and interactions are weak, to harbor upstream charge modes. However, so far, charge currents were observed to flow exclusively downstream in the quantum Hall regime. Studying the canonical spin-polarized and spin-unpolarized v = 2/3 hole-like states in GaAs-AlGaAs heterostructures, we observed a significant upstream charge current at short propagation distances in the spin unpolarized state.


2003 ◽  
Vol 17 (27) ◽  
pp. 4765-4818 ◽  
Author(s):  
K. ISHIKAWA ◽  
T. AOYAMA ◽  
Y. ISHIZUKA ◽  
N. MAEDA

The von Neumann lattice representation is a convenient representation for studying several intriguing physics of quantum Hall systems. In this formalism, electrons are mapped to lattice fermions. A topological invariant expression of the Hall conductance is derived and is used for the proof of the integer quantum Hall effect in the realistic situation. Anisotropic quantum Hall gas is investigated based on the Hartree–Fock approximation in the same formalism. Thermodynamic properties, transport properties, and unusual response under external modulations are found. Implications for the integer quantum Hall effect in the finite systems are also studied and a new quantum Hall regime with non-zero longitudinal resistance is shown to exist.


2009 ◽  
Vol 95 (22) ◽  
pp. 223108 ◽  
Author(s):  
Xiaosong Wu ◽  
Yike Hu ◽  
Ming Ruan ◽  
Nerasoa K Madiomanana ◽  
John Hankinson ◽  
...  

2016 ◽  
Vol 2 (1) ◽  
pp. e1501117 ◽  
Author(s):  
Hidetoshi Masuda ◽  
Hideaki Sakai ◽  
Masashi Tokunaga ◽  
Yuichi Yamasaki ◽  
Atsushi Miyake ◽  
...  

For the innovation of spintronic technologies, Dirac materials, in which low-energy excitation is described as relativistic Dirac fermions, are one of the most promising systems because of the fascinating magnetotransport associated with extremely high mobility. To incorporate Dirac fermions into spintronic applications, their quantum transport phenomena are desired to be manipulated to a large extent by magnetic order in a solid. We report a bulk half-integer quantum Hall effect in a layered antiferromagnet EuMnBi2, in which field-controllable Eu magnetic order significantly suppresses the interlayer coupling between the Bi layers with Dirac fermions. In addition to the high mobility of more than 10,000 cm2/V s, Landau level splittings presumably due to the lifting of spin and valley degeneracy are noticeable even in a bulk magnet. These results will pave a route to the engineering of magnetically functionalized Dirac materials.


2002 ◽  
Vol 16 (20n22) ◽  
pp. 3089-3089
Author(s):  
V. M. YAKOVENKO

Theoretical overview of the quantum Hall effect in quasi-one-dimensional (Q1D) organic conductors (TMTSF) 2 X will be presented.1 The emphasis will be on the recent developments, such as the temperature evolution of the Hall effect2,3 and the chiral edge states.4 Time permitting, a theory of the nonchiral electron edge states in a Q1D triplet superconductor5 and the holon edge states in the charge-gap regime6 will be presented too.


2007 ◽  
Vol 76 (8) ◽  
Author(s):  
A. Baumgartner ◽  
T. Ihn ◽  
K. Ensslin ◽  
K. Maranowski ◽  
A. C. Gossard

1992 ◽  
Vol 263 (1-3) ◽  
pp. 81-86 ◽  
Author(s):  
A.G. Davies ◽  
R. Newbury ◽  
M. Pepper ◽  
J.E.F. Frost ◽  
D.A. Ritchie ◽  
...  

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