Ballistic Electron Source with Magnetically Controlled Valley Polarization in Bilayer Graphene

Journal Article (2024)
Author(s)

J. Ingla AynΓ©s (TU Delft - QN/van der Zant Lab, Kavli institute of nanoscience Delft)

A.L. Rigotti Manesco (TU Delft - QN/Akhmerov Group, Kavli institute of nanoscience Delft)

T.S. Ghiasi (TU Delft - QN/van der Zant Lab, Kavli institute of nanoscience Delft)

Kenji Watanabe (National Institute for Materials Science)

Takashi Taniguchi (National Institute for Materials Science)

Herre S.J. van der Zant (Kavli institute of nanoscience Delft, TU Delft - QN/van der Zant Lab)

Research Group
QN/van der Zant Lab
DOI related publication
https://doi.org/10.1103/PhysRevLett.133.156301
More Info
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Publication Year
2024
Language
English
Research Group
QN/van der Zant Lab
Issue number
15
Volume number
133
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Abstract

The achievement of valley-polarized electron currents is a cornerstone for the realization of valleytronic devices. Here, we report on ballistic coherent transport experiments where two opposite quantum point contacts (QPCs) are defined by electrostatic gating in a bilayer graphene (BLG) channel. By steering the ballistic currents with an out-of-plane magnetic field we observe two current jets, a consequence of valley-dependent trigonal warping. Tuning the BLG carrier density and number of QPC modes (π‘š) with a gate voltage we find that the two jets are present for π‘š=1 and up to π‘š=6, indicating the robustness of the effect. Semiclassical simulations confirm the origin of the signals by quantitatively reproducing the jet separations without fitting parameters. In addition, our model shows that the ballistic current jets have opposite valley polarization. As a consequence, by steering each jet toward the detector using a magnetic field, we achieve full control over the valley polarization of the collected currents, envisioning such devices as ballistic current sources with tunable valley polarization. We also show that collimation experiments are a sensitive probe to the trigonal warping of the Fermi surface.

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