6533b82dfe1ef96bd1291f8c

RESEARCH PRODUCT

Tuning the Pseudospin Polarization of Graphene by a Pseudomagnetic Field.

Yang CaoT. MashoffMartin SchneiderRamon Carrillo-bastosRamon Carrillo-bastosNancy SandlerA. GeorgiNils M. FreitagSilvia Viola KusminskiySilvia Viola KusminskiyDaiara FariaDaiara FariaMarcus LiebmannLudger WirtzMarkus MorgensternMarco PratzerPéter Nemes-inczeD. SubramaniamColin R. WoodsKostya S. NovoselovRoman V. GorbachevDawei Zhai

subject

STM: Physics [G04] [Physical chemical mathematical & earth Sciences]FOS: Physical sciencesBioengineering02 engineering and technology01 natural sciencespseudospin polarizationlaw.inventionstrainlaw0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)valley filterGeneral Materials ScienceSymmetry breaking010306 general physicsPhysicsLocal density of statesCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsGrapheneMechanical EngineeringgrapheneObservableGeneral ChemistryLandau quantization021001 nanoscience & nanotechnologyCondensed Matter PhysicsPolarization (waves)Magnetic field: Physique [G04] [Physique chimie mathématiques & sciences de la terre]pseudomagnetic fieldScanning tunneling microscope0210 nano-technology

description

One of the intriguing characteristics of honeycomb lattices is the appearance of a pseudo-magnetic field as a result of mechanical deformation. In the case of graphene, the Landau quantization resulting from this pseudo-magnetic field has been measured using scanning tunneling microscopy. Here we show that a signature of the pseudo-magnetic field is a local sublattice symmetry breaking observable as a redistribution of the local density of states. This can be interpreted as a polarization of graphene's pseudospin due to a strain induced pseudo-magnetic field, in analogy to the alignment of a real spin in a magnetic field. We reveal this sublattice symmetry breaking by tunably straining graphene using the tip of a scanning tunneling microscope. The tip locally lifts the graphene membrane from a SiO$_2$ support, as visible by an increased slope of the $I(z)$ curves. The amount of lifting is consistent with molecular dynamics calculations, which reveal a deformed graphene area under the tip in the shape of a Gaussian. The pseudo-magnetic field induced by the deformation becomes visible as a sublattice symmetry breaking which scales with the lifting height of the strained deformation and therefore with the pseudo-magnetic field strength. Its magnitude is quantitatively reproduced by analytic and tight-binding models, revealing fields of 1000 T. These results might be the starting point for an effective THz valley filter, as a basic element of valleytronics.

10.1021/acs.nanolett.6b04870https://pubmed.ncbi.nlm.nih.gov/30264572