Quantum Interference in SnTe nanowires
ORAL
Abstract
SnTe is a topological crystalline insulator (TCI) [1] and is predicted to undergo a phase transition to a higher-order topological state [2] by breaking crystal symmetry. These higher-order topological insulators (HOTI) have not been experimentally realized; they host hinge states on the boundary of two gapped surfaces, leading to conducting hinges. When combined with a superconductor, this system could host parafermions on a pair of hinge states due to the one-dimensional character of these states. Detecting the 2D surface and 1D hinge states in this material is therefore a key objective.
To this end, we perform transport measurements on SnTe nanowires. However, probing the topological surface states of SnTe is challenging due to a high bulk carrier density (~1021 cm-3) and electrostatic gating therefore has a negligible effect. Nevertheless, conductance oscillations are observed as function of source-drain and backgate voltage which we attribute to Fabry-Pérot oscillations, a coherent transport behaviour indicating a (quasi-) ballistic transport channel [3]. The period of the oscillation corresponds to a characteristic length closely resembling the physical length of the device. Furthermore, the conductance variation on top of the background signal has a magnitude corresponding to one ballistic transport channel, hinting towards transport through a SnTe surface state.
[1] Nature Phys 8, 800–803 (2012).
[2] Nat Rev Phys 3, 283–297 (2021).
[3] Nano Letters 10 (9), 3439-3445 (2010).
To this end, we perform transport measurements on SnTe nanowires. However, probing the topological surface states of SnTe is challenging due to a high bulk carrier density (~1021 cm-3) and electrostatic gating therefore has a negligible effect. Nevertheless, conductance oscillations are observed as function of source-drain and backgate voltage which we attribute to Fabry-Pérot oscillations, a coherent transport behaviour indicating a (quasi-) ballistic transport channel [3]. The period of the oscillation corresponds to a characteristic length closely resembling the physical length of the device. Furthermore, the conductance variation on top of the background signal has a magnitude corresponding to one ballistic transport channel, hinting towards transport through a SnTe surface state.
[1] Nature Phys 8, 800–803 (2012).
[2] Nat Rev Phys 3, 283–297 (2021).
[3] Nano Letters 10 (9), 3439-3445 (2010).
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Presenters
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Femke Witmans
University of Twente
Authors
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Femke Witmans
University of Twente
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Maarten Kamphuis
University of Twente
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Joost Ridderbos
University of Twente
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Job Noordkamp
University of Twente
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Mathijs Mientjes
Eindhoven University of Technology
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Max Hoskam
Eindhoven University of Technology
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Xin Guan
Eindhoven University of Technology
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Chuan Li
University of Twente
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Erik P. A. M. Bakkers
Eindhoven University of Technology
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Floris Zwanenburg
Univ of Twente
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Alexander Brinkman
University of Twente, U Twente