| Literature DB >> 29045153 |
Monica T Allen1, Oles Shtanko2, Ion C Fulga3,4, Joel I-J Wang2, Daniyar Nurgaliev1, Kenji Watanabe5, Takashi Taniguchi5, Anton R Akhmerov6, Pablo Jarillo-Herrero2, Leonid S Levitov2, Amir Yacoby1,7.
Abstract
Electron surface states in solids are typically confined to the outermost atomic layers and, due to surface disorder, have negligible impact on electronic transport. Here, we demonstrate a very different behavior for surface states in graphene. We probe the wavelike character of these states by Fabry-Perot (FP) interferometry and find that, in contrast to theoretical predictions, these states can propagate ballistically over micron-scale distances. This is achieved by embedding a graphene resonator formed by gate-defined p-n junctions within a graphene superconductor-normal-superconductor structure. By combining superconducting Aharanov-Bohm interferometry with Fourier methods, we visualize spatially resolved current flow and image FP resonances due to p-n-p cavity modes. The coherence of the standing-wave edge states is revealed by observing a new family of FP resonances, which coexist with the bulk resonances. The edge resonances have periodicity distinct from that of the bulk states manifest in a repeated spatial redistribution of current on and off the FP resonances. This behavior is accompanied by a modulation of the multiple Andreev reflection amplitude on-and-off resonance, indicating that electrons propagate ballistically in a fully coherent fashion. These results, which were not anticipated by theory, provide a practical route to developing electron analog of optical FP resonators at the graphene edge.Entities:
Keywords: Ballistic transport; Fabry−Perot interference; Josephson interferometry; electron optics; graphene edge states
Year: 2017 PMID: 29045153 DOI: 10.1021/acs.nanolett.7b03156
Source DB: PubMed Journal: Nano Lett ISSN: 1530-6984 Impact factor: 11.189