Affiliation: | 1. Departamento Física de la Materia Condensada, Universidad Autónoma de Madrid, Madrid, E-28049 Spain;2. Université Grenoble Alpes, Grenoble, F-38400 France CNRS, Institut Néel, Grenoble, F-38042 France;3. Department of Applied Physics, Aalto University, Aalto, FI-00076 Finland;4. QuantaLab, International Iberian Nanotechnology Laboratory (INL), Avenida Mestre José Veiga, Braga, 4715-310 Portugal Departamento de Física Aplicada, Universidad de Alicante, San Vicente del Raspeig, Alicante, E-03690 Spain;5. Departamento Física de la Materia Condensada, Universidad Autónoma de Madrid, Madrid, E-28049 Spain Condensed Matter Physics Center (IFIMAC), Universidad Autónoma de Madrid, Madrid, E-28049 Spain Instituto Nicolás Cabrera, Universidad Autónoma de Madrid, Madrid, E-28049 Spain |
Abstract: | Quantum confinement of graphene Dirac-like electrons in artificially crafted nanometer structures is a long sought goal that would provide a strategy to selectively tune the electronic properties of graphene, including bandgap opening or quantization of energy levels. However, creating confining structures with nanometer precision in shape, size, and location remains an experimental challenge, both for top-down and bottom-up approaches. Moreover, Klein tunneling, offering an escape route to graphene electrons, limits the efficiency of electrostatic confinement. Here, a scanning tunneling microscope (STM) is used to create graphene nanopatterns, with sub-nanometer precision, by the collective manipulation of a large number of H atoms. Individual graphene nanostructures are built at selected locations, with predetermined orientations and shapes, and with dimensions going all the way from 2 nm up to 1 µm. The method permits the patterns to be erased and rebuilt at will, and it can be implemented on different graphene substrates. STM experiments demonstrate that such graphene nanostructures confine very efficiently graphene Dirac quasiparticles, both in 0D and 1D structures. In graphene quantum dots, perfectly defined energy bandgaps up to 0.8 eV are found that scale as the inverse of the dot’s linear dimension, as expected for massless Dirac fermions. |