Experimental observation of Dirac cones in artificial graphene lattices
arXiv:2010.16152 · doi:10.1103/PhysRevB.102.201401
Abstract
Artificial lattices provide a tunable platform to realize exotic quantum devices. A well-known example is artificial graphene (AG), in which electrons are confined in honeycomb lattices and behave as massless Dirac fermions. Recently, AG systems have been constructed by manipulating molecules using scanning tunnelling microscope tips, but the nanoscale size typical for these constructed systems are impossible for practical device applications and insufficient for direct investigation of the electronic structures using angle-resolved photoemission spectroscopy (ARPES). Here, we demonstrate the synthesis of macroscopic AG by self-assembly of C molecules on metal surfaces. Our theoretical calculations and ARPES measurements directly confirm the existence of Dirac cones at the () points of the Brillouin zone (BZ), in analogy to natural graphene. These results will stimulate ongoing efforts to explore the exotic properties in artificial lattices and provide an important step forward in the realization of novel molecular quantum devices.
arXiv commentto appear in Physical Review B
References in corpus (13)
- The electronic properties of graphene
- Two-Dimensional Gas of Massless Dirac Fermions in Graphene
- Experimental Observation of Quantum Hall Effect and Berry's Phase in Graphene
- Chiral tunneling and the Klein paradox in graphene
- Optical nano-imaging of gate-tuneable graphene plasmons
- Quantum interference and Klein tunneling in graphene heterojunctions
- Creating, moving and merging Dirac points with a Fermi gas in a tunable honeycomb lattice
- Artificial graphene as a tunable Dirac material
- Design and characterization of electronic fractals
- Robust zero-energy modes in an electronic higher-order topological insulator: the dimerized Kagome lattice
- Two-dimensional Mott-Hubbard electrons in an artificial honeycomb lattice
- Engineering artificial graphene in a two-dimensional electron gas
- Coexistence of full-gap superconductivity and pseudogap in two-dimensional fullerides