|
|
Enhanced robustness of zero-line modes in graphene via magnetic field |
Ke Wang1,2, Tao Hou1,2, Yafei Ren1,2, Zhenhua Qiao1,2( ) |
1. ICQD, Hefei National Laboratory for Physical Sciences at Microscale, and Synergetic Innovation Centre of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China 2. CAS Key Laboratory of Strongly-Coupled Quantum Matter Physics and Department of Physics, University of Science and Technology of China, Hefei 230026, China |
|
|
Abstract We systematically studied the influence of magnetic field on zero-line modes (ZLMs) in graphene and demonstrated the physical origin of their enhanced robustness by employing nonequilibrium Green’s functions and the Landauer–Büttiker formula. We found that a perpendicular magnetic field can separate the wavefunctions of the counter-propagating kink states into opposite directions. Specifically, the separation vanishes at the charge neutrality point and increases as the Fermi level deviates from the charge neutrality point and can reach a magnitude comparable to the wavefunction spread at a moderate field strength. Such spatial separation of oppositely propagating ZLMs effectively suppresses backscattering and is more significant under zigzag boundary condition than under armchair boundary condition. Moreover, the presence of magnetic field enlarges the bulk gap and suppresses the bound states, thereby further reducing the scattering. These mechanisms effectively increase the mean free paths of the ZLMs to approximately 1 μm in the presence of a disorder.
|
Keywords
graphene
topological state
zero-line state
electronic transport
|
Corresponding Author(s):
Zhenhua Qiao
|
Issue Date: 29 November 2018
|
|
1 |
M. Bttiker, Edge-state physics without magnetic fields, Science 325(5938), 278 (2009)
https://doi.org/10.1126/science.1177157
|
2 |
G. W. Semenoff, V. Semenoff, and F. Zhou, Domain walls in gapped graphene, Phys. Rev. Lett. 101(8), 087204 (2008)
https://doi.org/10.1103/PhysRevLett.101.087204
|
3 |
I. Martin, M. Blanter, and A. F. Morpurgo, Topological confinement in bilayer graphene, Phys. Rev. Lett. 100(3), 036804 (2008)
https://doi.org/10.1103/PhysRevLett.100.036804
|
4 |
W. Yao, S. A. Yang, and Q. Niu, Edge states in graphene: From gapped flat-band to gapless chiral modes, Phys. Rev. Lett. 102(9), 096801 (2009)
https://doi.org/10.1103/PhysRevLett.102.096801
|
5 |
M. Killi, S. Wu, and A. Paramekanti, Band structures of bilayer graphene superlattices, Phys. Rev. Lett. 107(8), 086801 (2011)
https://doi.org/10.1103/PhysRevLett.107.086801
|
6 |
Y. Ran, Y. Zhang, and A. Vishwanath, One-dimensional topologically protected modes in topological insulators with lattice dislocations, Nat. Phys. 5(4), 298 (2009)
|
7 |
Y. B. Zhang, Y. W. Tan, H. L. Stormer, and P. Kim, Experimental observation of quantum Hall effect and Berry’s phase in graphene, Nature 438, 201 (2005)
https://doi.org/10.1038/nature04235
|
8 |
K. S. Novoselov, Z. Jiang, Y. Zhang, S. V. Morozov, H. L. Stormer, U. Zeitler, J. C. Maan, G. S. Boebinger, P. Kim, and A. K. Geim, Room-temperature quantum Hall effect in graphene, Science 315(5817), 1379 (2007)
https://doi.org/10.1126/science.1137201
|
9 |
C. Z. Chang, J. S. Zhang, X. Feng, J. Shen, Z. C. Zhang, M. H. Guo, K. Li, Y. B. Ou, P. Wei, L. L. Wang, Z. Q. Ji, Y. Feng, S. K. Ji, X. Chen, J. F. Jia, X. Dai, Z. Fang, S. C. Zhang, K. He, Y. Y. Wang, L. Lu, X. C. Ma, and Q. K. Xue, Experimental observation of the quantum anomalous Hall effect in a magnetic topological insulator, Science 340(6129), 167 (2013)
https://doi.org/10.1126/science.1234414
|
10 |
Z. Qiao, S. A. Yang, W. Feng, W. K. Tse, J. Ding, Y. Yao, J. Wang, and Q. Niu, Quantum anomalous Hall effect in graphene from Rashba and exchange effects, Phys. Rev. B 82(16), 161414R (2010)
https://doi.org/10.1103/PhysRevB.82.161414
|
11 |
L. Sheng, D. N. Sheng, and C. S. Ting, Spin-Hall effect in two-dimensional electron systems with Rashba spin-orbit coupling and disorder, Phys. Rev. Lett. 94(1), 016602 (2005)
https://doi.org/10.1103/PhysRevLett.94.016602
|
12 |
Z. H. Qiao, J. Jung, Q. Niu, and A. H. MacDonald, Electronic highways in bilayer graphene, Nano Lett. 11(8), 3453 (2011)
https://doi.org/10.1021/nl201941f
|
13 |
T. Hou, G. H. Chen, W. K. Tse, C. G. Zeng, and Z. H. Qiao, Topological zero-line modes in folded bilayer graphene, arXiv: 1809.04036 (2018)
|
14 |
K. Wang, Y. F. Ren, X. Z. Deng, S. A. Yang, J. Jung, and Z. H. Qiao, Gate-tunable current partition in graphenebased topological zero lines, Phys. Rev. B 95(24), 245420 (2017)
https://doi.org/10.1103/PhysRevB.95.245420
|
15 |
Z. H. Qiao, J. Jung, C. Lin, Y. F. Ren, A. H. MacDonald, and Q. Niu, Current partition at topological channel intersections, Phys. Rev. Lett. 112(20), 206601 (2014)
https://doi.org/10.1103/PhysRevLett.112.206601
|
16 |
J. Li, K. Wang, K. J. McFaul, Z. Zern, Y. F. Ren, K. Watanabe, T. Taniguchi, Z. H. Qiao, and J. Zhu, Gate-controlled topological conducting channels in bilayer graphene, Nat. Nanotechnol. 11, 1060 (2016)
https://doi.org/10.1038/nnano.2016.158
|
17 |
M. Kim, J. H. Choi, S. H. Lee, K. Watanabe, T. Taniguchi, S. H. Jhi, and H. J. Lee, Valley-symmetrypreserved transport in ballistic graphene with gatedefined carrier guiding, Nat. Phys. 12(11), 1022 (2016)
|
18 |
L. Ju, Z. Shi, N. Nair, Y. Lv, C. Jin, H. A. Velasco, M. C. Bechtel, A. Martin, J. Zettl, Analytis, and F. Wang, Topological valley transport at bilayer graphene domain walls, Nature 520(7549), 650 (2015)
https://doi.org/10.1038/nature14364
|
19 |
S. Datta, Electronic Transport in Mesoscopic Systems, Cambridge University Press, 1997
|
20 |
M. P. L. Sancho, J. M. L. Sancho, and J. Rubio, Quick iterative scheme for the calculation of transfer matrices: Application to Mo(100), J. Phys. F Met. Phys. 14(5), 1205 (1984)
https://doi.org/10.1088/0305-4608/14/5/016
|
|
Viewed |
|
|
|
Full text
|
|
|
|
|
Abstract
|
|
|
|
|
Cited |
|
|
|
|
|
Shared |
|
|
|
|
|
Discussed |
|
|
|
|