Research paperTheoreticalComputational MultiscaleAsymmetric-gate Mach–Zehnder interferometry in graphene: Multi-path conductance oscillations and visibility characteristicsTaegeun Song, Nojoon MyoungCurrent Applied Physics·2025·10.1016/j.cap.2025.09.016·arXiv:2508.07380AbstractGraphene provides an excellent platform for investigating electron quantum interference due to its outstanding coherent properties. In the quantum Hall regime, Mach–Zehnder (MZ) electronic interferometers are realized using p–n junctions in graphene, where electron interference is highly protected against decoherence. In this work, we present a phenomenological framework for graphene-based MZ interferometry with asymmetric p–n junction configurations. We show that the enclosed interferometer area can be tuned by asymmetric gate potentials, and additional MZ pathways emerge in higher-filling-factor scenarios, e.g. (νn, νp) = (−3, +3). The resulting complicated beat oscillations in asymmetric-gate MZ interference are efficiently analyzed using a machine-learning–based Fourier transform, which yields improved peak-to-background ratios compared to conventional signal-processing techniques. Furthermore, we examine the impact of the asymmetric gate on the interference visibility, finding that interference visibility is enhanced under symmetric gate conditions.Read more
Graphene Hall bar with an electrostatically defined p–n junction used as a model Mach–Zehnder interferometer in the quantum Hall regime.No measurements recordedSimulatedCStudied MaterialExpand
Research paperTheoreticalComputational MultiscaleAsymmetric-gate Mach–Zehnder interferometry in graphene: Multi-path conductance oscillations and visibility characteristicsTaegeun Song, Nojoon MyoungCurrent Applied Physics·2025·10.1016/j.cap.2025.09.016·arXiv:2508.07380AbstractGraphene provides an excellent platform for investigating electron quantum interference due to its outstanding coherent properties. In the quantum Hall regime, Mach–Zehnder (MZ) electronic interferometers are realized using p–n junctions in graphene, where electron interference is highly protected against decoherence. In this work, we present a phenomenological framework for graphene-based MZ interferometry with asymmetric p–n junction configurations. We show that the enclosed interferometer area can be tuned by asymmetric gate potentials, and additional MZ pathways emerge in higher-filling-factor scenarios, e.g. (νn, νp) = (−3, +3). The resulting complicated beat oscillations in asymmetric-gate MZ interference are efficiently analyzed using a machine-learning–based Fourier transform, which yields improved peak-to-background ratios compared to conventional signal-processing techniques. Furthermore, we examine the impact of the asymmetric gate on the interference visibility, finding that interference visibility is enhanced under symmetric gate conditions.Read more
Graphene Hall bar with an electrostatically defined p–n junction used as a model Mach–Zehnder interferometer in the quantum Hall regime.No measurements recordedSimulatedCStudied MaterialExpand
Research paperTheoreticalComputational MultiscaleAsymmetric-gate Mach–Zehnder interferometry in graphene: Multi-path conductance oscillations and visibility characteristicsTaegeun Song, Nojoon MyoungCurrent Applied Physics·2025·10.1016/j.cap.2025.09.016·arXiv:2508.07380AbstractGraphene provides an excellent platform for investigating electron quantum interference due to its outstanding coherent properties. In the quantum Hall regime, Mach–Zehnder (MZ) electronic interferometers are realized using p–n junctions in graphene, where electron interference is highly protected against decoherence. In this work, we present a phenomenological framework for graphene-based MZ interferometry with asymmetric p–n junction configurations. We show that the enclosed interferometer area can be tuned by asymmetric gate potentials, and additional MZ pathways emerge in higher-filling-factor scenarios, e.g. (νn, νp) = (−3, +3). The resulting complicated beat oscillations in asymmetric-gate MZ interference are efficiently analyzed using a machine-learning–based Fourier transform, which yields improved peak-to-background ratios compared to conventional signal-processing techniques. Furthermore, we examine the impact of the asymmetric gate on the interference visibility, finding that interference visibility is enhanced under symmetric gate conditions.Read more
Graphene Hall bar with an electrostatically defined p–n junction used as a model Mach–Zehnder interferometer in the quantum Hall regime.No measurements recordedSimulatedCStudied MaterialExpand
Research paperTheoreticalComputational MultiscaleAsymmetric-gate Mach–Zehnder interferometry in graphene: Multi-path conductance oscillations and visibility characteristicsTaegeun Song, Nojoon MyoungCurrent Applied Physics·2025·10.1016/j.cap.2025.09.016·arXiv:2508.07380AbstractGraphene provides an excellent platform for investigating electron quantum interference due to its outstanding coherent properties. In the quantum Hall regime, Mach–Zehnder (MZ) electronic interferometers are realized using p–n junctions in graphene, where electron interference is highly protected against decoherence. In this work, we present a phenomenological framework for graphene-based MZ interferometry with asymmetric p–n junction configurations. We show that the enclosed interferometer area can be tuned by asymmetric gate potentials, and additional MZ pathways emerge in higher-filling-factor scenarios, e.g. (νn, νp) = (−3, +3). The resulting complicated beat oscillations in asymmetric-gate MZ interference are efficiently analyzed using a machine-learning–based Fourier transform, which yields improved peak-to-background ratios compared to conventional signal-processing techniques. Furthermore, we examine the impact of the asymmetric gate on the interference visibility, finding that interference visibility is enhanced under symmetric gate conditions.Read more
Graphene Hall bar with an electrostatically defined p–n junction used as a model Mach–Zehnder interferometer in the quantum Hall regime.No measurements recordedSimulatedCStudied MaterialExpand