scholarly journals Evidence for Topological Edge States in a Large Energy Gap near the Step Edges on the Surface ofZrTe5

2016 ◽  
Vol 6 (2) ◽  
Author(s):  
R. Wu ◽  
J.-Z. Ma ◽  
S.-M. Nie ◽  
L.-X. Zhao ◽  
X. Huang ◽  
...  
Nanomaterials ◽  
2020 ◽  
Vol 10 (11) ◽  
pp. 2098
Author(s):  
Paolo Marconcini ◽  
Massimo Macucci

We perform a numerical simulation of the effects of an orthogonal magnetic field on charge transport and shot noise in an armchair graphene ribbon with a lattice of antidots. This study relies on our envelope-function based code, in which the presence of antidots is simulated through a nonzero mass term and the magnetic field is introduced with a proper choice of gauge for the vector potential. We observe that by increasing the magnetic field, the energy gap present with no magnetic field progressively disappears, together with features related to commensurability and quantum effects. In particular, we focus on the behavior for high values of the magnetic field: we notice that when it is sufficiently large, the effect of the antidots vanishes and shot noise disappears, as a consequence of the formation of edge states crawling along the boundaries of the structure without experiencing any interaction with the antidots.


2002 ◽  
Vol 16 (32) ◽  
pp. 4897-4909 ◽  
Author(s):  
KATSUNORI WAKABAYASHI ◽  
TAKASHI AOKI

The electric conductance of the graphite ribbon with locally applied gate voltage has been studied in terms of the Landauer approach. In the low-energy region, nano-graphite ribbon with zigzag boundaries exhibits the single electronic transport channel due to the edge states. The chemical potential dependence of the electric conductance shows qualitatively different behavior, depending on whether the magnitude of the potential barrier (gate voltage bias) Vg is larger than the energy gap Δ of the single channel region of the zigzag ribbon. For positive Vg with Vg < Δ, the zero-conductance resonances appear for 0 ≤ E ≤ Vg, and average transmission probability is quite small in this region. However the transmission probability is almost one, i.e. perfect transmission, for E > Vg. This step-function-like behavior of the conductance shows that it is possible to fabricate a nano-graphite-based switching device by the application of weak gate voltage bias.


1989 ◽  
Vol 39 (14) ◽  
pp. 10174-10178 ◽  
Author(s):  
R. P. McCall ◽  
J. M. Ginder ◽  
M. G. Roe ◽  
G. E. Asturias ◽  
E. M. Scherr ◽  
...  
Keyword(s):  

1988 ◽  
Vol 153-155 ◽  
pp. 1020-1021 ◽  
Author(s):  
W. Loram ◽  
K.A. Mirza

2009 ◽  
Vol 80 (12) ◽  
Author(s):  
Kenta Esaki ◽  
Masatoshi Sato ◽  
Mahito Kohmoto ◽  
Bertrand I. Halperin

1996 ◽  
Vol 11 (17) ◽  
pp. 1417-1428 ◽  
Author(s):  
A.A. ANDRIANOV ◽  
M.V. IOFFE ◽  
F. CANNATA

Starting from a polynomial (higher-order derivative) quantum mechanical SUSY algebra we study its contraction to the standard SUSYQM in the limit of large energy shifts between the lowest states of the super-Hamiltonian (of Schrödinger type). By a quasi-linearization method we obtain the charges of the higher derivative SUSY algebra in the (singular) limit of infinite energy gap, and find the resulting Hamiltonian. The singular behavior of the potential generated by this construction reflects the existence of the very deep level. Our results can suggest constructions of toy models where large energy splittings between fermionic and bosonic partners do not affect SUSY for other states.


1990 ◽  
Vol 04 (02) ◽  
pp. 201-237 ◽  
Author(s):  
J. R. KIRTLEY

The current status of tunneling measurements of the superconducting density of states near the Fermi level of high-T c superconductors is reviewed. A number of the characteristics of the tunneling data that had previously been considered to be "non-ideal" follow quite naturally from conventional tunneling theory, if the effects of the unusually large energy gap, often unusually small tunneling barriers, and gap anisotropy and/or inhomogeneity are correctly accounted for. Despite formidable problems in making these measurements, due to both the very short coherence lengths and materials problems in these superconductors, a consistent body of data is emerging. A consistent picture can be drawn from this data with the aid of the new modelling presented here.


2009 ◽  
Vol 131 (21) ◽  
pp. 7220-7221 ◽  
Author(s):  
Manzhou Zhu ◽  
Huifeng Qian ◽  
Rongchao Jin
Keyword(s):  

Nano Letters ◽  
2014 ◽  
Vol 14 (5) ◽  
pp. 2443-2447 ◽  
Author(s):  
Chendong Zhang ◽  
Amber Johnson ◽  
Chang-Lung Hsu ◽  
Lain-Jong Li ◽  
Chih-Kang Shih

2020 ◽  
Author(s):  
Aristides Zdetsis ◽  
Eleftherios Economou

We show that very narrow armchair graphene nanoribbons (AGNRs) of length L and width of 2 zigzag-rings undergo a metal-insulator-like transition at a critical length of 10nm, where the energy gap drops rather abruptly, and the conductivity, estimated, through an invoked computational scheme, rises almost discontinuously to a value between that of a perfect quasi one-dimensional system, and the nominal minimum conductivity of graphene. At this length, the aromatic and non-aromatic rings are interchanged, and sharp peaks appear in the density of states around the Fermi level, suggesting metallic-like behaviour. Such peaks linked to edge states at the Dirac point(s) coincide with the charge-neutrality point(s), associated with the minimum conductivity of graphene. Thus, we have an uncommon combination of interrelated “short-long”, “core-edge,” topological-aromatic transition(s) due to strong quantum confinement, driven by inversion symmetry conflict. The bandgap decreases with the 2/3 power of length before the “transition” and logarithmically afterwards. These effects are practically non-existent for wider AGNRs


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