Degeneracy enhancement of Landau Levels in graphene 1D superlattices
Alina Mrenca-Kolasinska1*, Ming-Hao Liu2
1Faculty of Physics and Applied Computer Science, AGH University of Krakow, Krakow, Poland
2Department of Physics and Center for Quantum Frontiers of Research and Technology (QFort), National Cheng Kung University, Tainan, Taiwan
* Presenter:Alina Mrenca-Kolasinska, email:alina.mrenca@fis.agh.edu.pl
The presence of a one-dimensional (1D) superlattice (SL) in graphene can lead to the modification of the band structure, anisotropic renormalization of velocity transverse to the SL modulation [1], and formation of 2N+1 multiple zero-energy Dirac cones, where their number (with N = 0, 1, 2, ...) is tunable by the SL modulation strength [2]. This leads to increase of the zero-energy Landau level degeneracy, resulting in the Hall conductivity step of 4(2N + 1)e^2/h [3], namely, skipping the lowest plateaus. 1D SLs can for example be introduced into graphene via periodically patterned electrostatic gates, which induce a modulated potential profile.
The main focus of this work is a theoretical study of the magnetotransport in 1D induced superlattices within the Landauer-Büttiker formalism, and investigation of the conditions necessary for the observation of degeneracy enhancement. We find that the higher order conductance plateaus (with N ≥ 1) are strongly affected by the modulation asymmetry, inherent of realistic gate-induced superlattices. In such scenarios we observe a modified sequence of conductance plateaus. We confront our findings with experimental transport measurements. Our results provide a tool for characterization of the electronic structure induced by the SL modulation.

References
[1] ] C.-H. Park, L. Yang, Y.-W. Son, M. L. Cohen, and S. G. Louie, Nat. Phys. 4, 213 (2008).
[2] L. Brey and H. A. Fertig, Phys. Rev. Lett. 103, 046809 (2009).
[3] C.-H. Park, Y.-W. Son, L. Yang, M. L. Cohen, and S. G. Louie, Phys. Rev. Lett. 103, 046808 (2009).


Keywords: electrostatic superlattices, quantum transport, Hall effect