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. 2017 Apr 12;17(4):2240-2245.
doi: 10.1021/acs.nanolett.6b04870. Epub 2017 Mar 2.

Tuning the Pseudospin Polarization of Graphene by a Pseudomagnetic Field

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Tuning the Pseudospin Polarization of Graphene by a Pseudomagnetic Field

Alexander Georgi et al. Nano Lett. .

Erratum in

  • Correction to Tuning the Pseudospin Polarization of Graphene by a Pseudomagnetic Field.
    Georgi A, Nemes-Incze P, Carrillo-Bastos R, Faria D, Kusminskiy SV, Zhai D, Schneider M, Subramaniam D, Mashoff T, Freitag NM, Liebmann M, Pratzer M, Wirtz L, Woods CR, Gorbachev RV, Cao Y, Novoselov KS, Sandler N, Morgenstern M. Georgi A, et al. Nano Lett. 2018 Oct 10;18(10):6654. doi: 10.1021/acs.nanolett.8b03872. Epub 2018 Sep 28. Nano Lett. 2018. PMID: 30264572 No abstract available.

Abstract

One of the intriguing characteristics of honeycomb lattices is the appearance of a pseudomagnetic field as a result of mechanical deformation. In the case of graphene, the Landau quantization resulting from this pseudomagnetic field has been measured using scanning tunneling microscopy. Here we show that a signature of the pseudomagnetic 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 pseudomagnetic 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 SiO2 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 pseudomagnetic 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 pseudomagnetic 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.

Keywords: Graphene; STM; pseudomagnetic field; pseudospin polarization; strain; valley filter.

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