Massless Dirac Fermions Trapping in a Quasi-one-dimensional npn Junction of a Continuous Graphene Monolayer
Ke-Ke Bai, Jia-Bin Qiao, Hua Jiang, Haiwen Liu, Lin He

TL;DR
This paper demonstrates that massless Dirac fermions in graphene can be trapped in a quasi-one-dimensional npn junction, forming quasi-bound states, challenging the traditional view of their unimpeded transmission due to Klein tunneling.
Contribution
The study provides experimental and theoretical evidence of trapping Dirac fermions in graphene using a quasi-1D npn junction, revealing new confinement phenomena.
Findings
Observation of quasi-bound states in graphene npn junctions
Visualization of quantum interference patterns via STM
Confirmation of Dirac fermion trapping contrary to Klein tunneling expectations
Abstract
Massless Dirac fermions in graphene provide unprecedented opportunities to realize the Klein paradox, which is one of the most exotic and striking properties of relativistic particles. In the seminal theoretical work [Katsnelson et al., Nat. Phys. 2 620 (2006)], it was predicted that the massless Dirac fermions can pass through one-dimensional (1D) potential barriers unimpededly at normal incidence. Such a result seems to preclude confinement of the massless Dirac fermions in graphene by using 1D potential barriers. Here, we demonstrate, both experimentally and theoretically, that massless Dirac fermions can be trapped in quasi-1D npn junction of a continuous graphene monolayer. Because of highly anisotropic transmission of the massless Dirac fermions at n-p junction boundaries (the so-called Klein tunneling in graphene), charge carries incident at large oblique angles will be reflected…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
