Abstract

We analyze theoretically 4-terminal electronic devices composed of two crossed graphene nanoribbons (GNRs) and show that they can function as beam splitters or mirrors. These features are identified for electrons in the low-energy region where a single valence or conduction band is present. Our modeling is based on $p_z$ orbital tight-binding with Slater--Koster type matrix elements fitted to accurately reproduce the low-energy bands from density functional theory calculations. We analyze systematically all devices that can be constructed with either zigzag or armchair GNRs in AA and AB stackings. From Green's function theory the elastic electron transport properties are quantified as a function of the ribbon width. We find that devices composed of relatively narrow zigzag GNRs and AA-stacked armchair GNRs are the most interesting candidates to realize electron beam splitters with a close to 50-50 ratio in the two outgoing terminals. Structures with wider ribbons instead provide electron mirrors, where the electron wave is mostly transferred into the outgoing terminal of the other ribbon, or electron filters where the scattering depends sensitively on the wavelength of the propagating electron. We also test the robustness of these transport properties against variations in intersection angle, stacking pattern, lattice deformation (uniaxial strain), inter-GNR separation, and electrostatic potential differences between the layers. These generic features show that GNRs are interesting basic components to construct electronic quantum optical setups.

Highlights

  • The similarities between the wave nature of electrons propagating coherently in ballistic conductors with photon propagation in optical waveguides has spawned the field of electron quantum optics [1,2]

  • The symmetry of the honeycomb lattice yields a perfect matching between the bottom and top graphene nanoribbons (GNRs) lattices for θ = 60◦

  • The inter-GNR transmission is enhanced for angles within [50◦, 70◦], which highlights the tunability of our devices

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Summary

Introduction

The similarities between the wave nature of electrons propagating coherently in ballistic conductors with photon propagation in optical waveguides has spawned the field of electron quantum optics [1,2] In this way several electronic analogs of optical setups—such as the Mach-Zehnder [3,4] and Fabry-Pérot [5,6,7] interferometers, as well as the Hanbury Brown–Twiss [8,9,10,11] geometry to study the Fermion antibunching and the two-particle Aharonov-Bohm [12] effects— have been implemented. With two BSs and two oriented Ms the Mach-Zehnder interferometer can be fully implemented, which has been demonstrated to work as a quantum logic processor [18]

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