Coherent-scatterer enhancement and Klein-tunneling suppression by potential barriers in gapped graphene with chirality-time-reversal symmetry

被引:3
作者
Anwar, Farhana [1 ]
Iurov, Andrii [2 ]
Huang, Danhong [3 ]
Gumbs, Godfrey [4 ,5 ]
Sharma, Ashwani [3 ,6 ,7 ]
机构
[1] Lawrence Berkeley Natl Lab, 1 Cyclotron Rd, Berkeley, CA 94720 USA
[2] CUNY, Dept Phys & Comp Sci, Medgar Evers Coll, Brooklyn, NY 11225 USA
[3] Space Vehicles Directorate, Air Force Res Lab, Kirtland AFB, NM 87117 USA
[4] CUNY Hunter Coll, Dept Phys & Astron, 695 Pk Ave, New York, NY 10065 USA
[5] Donostia Int Phys Ctr DIPC, P de Manuel Lardizabal 4, San Sebastian 20018, Spain
[6] Univ New Mexico, Ctr High Technol Mat, 1313 Goddard SE, Albuquerque, NM 87106 USA
[7] Univ New Mexico, Dept Elect & Comp Engn, Albuquerque, NM 87106 USA
关键词
smooth barrier; coherent scatterer; Klein tunneling suppression; gapped graphene; ELECTRONIC-PROPERTIES; BAND-GAP; REFLECTION;
D O I
10.1088/1361-648X/ac2866
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
We have utilized the finite-difference approach to explore electron-tunneling properties in gapped graphene through various electrostatic-potential barriers ranging from Gaussian to a triangular envelope function in comparison with a square potential barrier. The transmission coefficient is calculated numerically for each case and applied to the corresponding tunneling conductance. It is well known that Klein tunneling in graphene will be greatly reduced in gapped graphene. Our results further demonstrate that such a decrease of transmission can be significantly enhanced for spatially-modulated potential barriers. Moreover, we investigate the effect from a bias field applied to those barrier profiles, from which we show that it enables the control of electron flow under normal incidence. Meanwhile, the suppression of Klein tunneling is found more severe for a non-square barrier and exhibits a strong dependence on bias-field polarity for all kinds of barriers. Finally, roles of a point impurity on electron transmission and conductance are analyzed with a sharp peak appearing in electron conductance as the impurity atom is placed in the middle of a square barrier. For narrow triangular and Gaussian barriers, however, the conductance peaks become significantly broadened, associated with an enhancement in tunneling conductance.
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页数:14
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