4.8 Article

Direct evidence of interaction-induced Dirac cones in a monolayer silicene/Ag(111) system

Publisher

NATL ACAD SCIENCES
DOI: 10.1073/pnas.1613434114

Keywords

photoemission; silicene; Dirac cone; interaction

Funding

  1. National Science Foundation of China [91021006, 11474336]
  2. Ministry of Science and Technology (MOST) of China (973 Program) [2012CB821402, 2013CB921700, 2013CB921904]
  3. Strategic Priority Research Program (B) of the Chinese Academy of Sciences [XDB07020300]
  4. US Department of Energy (DOE), Office of Science, Basic Energy Sciences [DE-FG02-07ER46352]
  5. DOE [DE-AC02-05CH11231]
  6. DOE Energy Frontier Research Centers: Center for the Computational Design of Functional Layered Materials [DE-SC0012575]
  7. Singapore National Research Foundation under National Research Foundation (NRF) Award [NRF-NRFF2013-03]
  8. National Center for Theoretical Sciences
  9. Taiwan Ministry of Science and Technology [MOST-101-2112-M-110-002-MY3, MOST-101-2218-E-110-003-MY3]

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Silicene, analogous to graphene, is a one-atom-thick 2D crystal of silicon, which is expected to share many of the remarkable properties of graphene. The buckled honeycomb structure of silicene, along with enhanced spin-orbit coupling, endows silicene with considerable advantages over graphene in that the spin-split states in silicene are tunable with external fields. Although the low-energy Dirac cone states lie at the heart of all novel quantum phenomena in a pristine sheet of silicene, a hotly debated question is whether these key states can survive when silicene is grown or supported on a substrate. Here we report our direct observation of Dirac cones in monolayer silicene grown on a Ag(111) substrate. By performing angle-resolved photoemission measurements on silicene(3 x 3)/Ag(111), we reveal the presence of six pairs of Dirac cones located on the edges of the first Brillouin zone of Ag(111), which is in sharp contrast to the expected six Dirac cones centered at the K points of the primary silicene(1 x 1) Brillouin zone. Our analysis shows clearly that the unusual Dirac cone structure we have observed is not tied to pristine silicene alone but originates from the combined effects of silicene(3 x 3) and the Ag(111) substrate. Our study thus identifies the case of a unique type of Dirac cone generated through the interaction of two different constituents. The observation of Dirac cones in silicene/Ag(111) opens a unique materials platform for investigating unusual quantum phenomena and for applications based on 2D silicon systems.

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