Publications
7 results found
Burke D, Heffels D, Moors K, et al., 2024, Robust Majorana bound states in magnetic topological insulator nanoribbons with fragile chiral edge channels, Physical Review B, Vol: 109, ISSN: 2469-9950
Heffels D, Burke D, Connolly MRR, et al., 2023, Robust and fragile Majorana bound states in proximitized topological insulator nanoribbons, Nanomaterials, Vol: 13, ISSN: 2079-4991
Topological insulator (TI) nanoribbons with proximity-induced superconductivity are a promising platform for Majorana bound states (MBSs). In this work, we consider a detailed modeling approach for a TI nanoribbon in contact with a superconductor via its top surface, which induces a superconducting gap in its surface-state spectrum. The system displays a rich phase diagram with different numbers of end-localized MBSs as a function of chemical potential and magnetic flux piercing the cross section of the ribbon. These MBSs can be robust or fragile upon consideration of electrostatic disorder. We simulate a tunneling spectroscopy setup to probe the different topological phases of top-proximitized TI nanoribbons. Our simulation results indicate that a top-proximitized TI nanoribbon is ideally suited for realizing fully gapped topological superconductivity, in particular when the Fermi level is pinned near the Dirac point. In this regime, the setup yields a single pair of MBSs, well separated at opposite ends of the proximitized ribbon, which gives rise to a robust quantized zero-bias conductance peak.
Connolly M, 2022, Microwave sensing of Andreev bound states in a gate-defined superconducting quantum point contact, Physical Review Research, Vol: 4, Pages: 1-9, ISSN: 2643-1564
We use a superconducting microresonator as a cavity to sense absorption of microwaves by asuperconducting quantum point contact defined by surface gates over a proximitized two-dimensionalelectron gas. Renormalization of the cavity frequency with phase difference across the point contact isconsistent with coupling to Andreev bound states. Near π phase difference, we observe randomfluctuations in absorption with gate voltage, related to quantum interference-induced modulations in theelectron transmission. Close to pinch-off, we identify features consistent with the presence of a singleAndreev bound state and describe the Andreev-cavity interaction using a dispersive Jaynes-Cummingsmodel. By fitting the weak Andreev-cavity coupling, we extract ~GHz decoherence consistent with chargenoise and the transmission dispersion associated with a localized state.
Schmitt TW, Connolly MR, Schleenvoigt M, et al., 2022, Integration of topological insulator josephson junctions in superconducting qubit circuits., Nano Letters: a journal dedicated to nanoscience and nanotechnology, Vol: 22, ISSN: 1530-6984
The integration of semiconductor Josephson junctions (JJs) in superconducting quantum circuits provides a versatile platform for hybrid qubits and offers a powerful way to probe exotic quasiparticle excitations. Recent proposals for using circuit quantum electrodynamics (cQED) to detect topological superconductivity motivate the integration of novel topological materials in such circuits. Here, we report on the realization of superconducting transmon qubits implemented with (Bi0.06Sb0.94)2Te3 topological insulator (TI) JJs using ultrahigh vacuum fabrication techniques. Microwave losses on our substrates, which host monolithically integrated hardmasks used for the selective area growth of TI nanostructures, imply microsecond limits to relaxation times and, thus, their compatibility with strong-coupling cQED. We use the cavity-qubit interaction to show that the Josephson energy of TI-based transmons scales with their JJ dimensions and demonstrate qubit control as well as temporal quantum coherence. Our results pave the way for advanced investigations of topological materials in both novel Josephson and topological qubits.
Wang S-W, Ziao D, Dou Z, et al., 2020, Demonstration of dissipative quasihelical edge transport in quantum anomalous hall insulators, Physical Review Letters, Vol: 125, Pages: 126801 – 1-126801 – 6, ISSN: 0031-9007
Doping a topological insulator (TI) film with transition metal ions can break its time-reversal symmetry and lead to the realization of the quantum anomalous Hall (QAH) effect. Prior studies have shown that the longitudinal resistance of the QAH samples usually does not vanish when the Hall resistance shows a good quantization. This has been interpreted as a result of the presence of possible dissipative conducting channels in magnetic TI samples. By studying the temperature- and magnetic field-dependence of the magnetoresistance of a magnetic TI sandwich heterostructure device, we demonstrate that the predominant dissipation mechanism in thick QAH insulators can switch between non-chiral edge states and residual bulk states in different magnetic field regimes. The interactions between bulk states, chiral edge states, and non-chiral edge states are also investigated. Our study provides a way to distinguish between the dissipation arising from the residual bulk states and non-chiral edge states, which is crucial for achieving true dissipationless transport in QAH insulators and for providing deeper insights into QAH-related phenomena.
Casparis L, Connolly MR, Kjaergaard M, et al., 2018, Superconducting gatemon qubit based on a proximitized two-dimensional electron gas, Nature Nanotechnology, Vol: 13, Pages: 915-919, ISSN: 1748-3387
The coherent tunnelling of Cooper pairs across Josephson junctions (JJs) generates a nonlinear inductance that is used extensively in quantum information processors based on superconducting circuits, from setting qubit transition frequencies1 and interqubit coupling strengths2 to the gain of parametric amplifiers3 for quantum-limited readout. The inductance is either set by tailoring the metal oxide dimensions of single JJs, or magnetically tuned by parallelizing multiple JJs in superconducting quantum interference devices with local current-biased flux lines. JJs based on superconductor–semiconductor hybrids represent a tantalizing all-electric alternative. The gatemon is a recently developed transmon variant that employs locally gated nanowire superconductor–semiconductor JJs for qubit control4,5. Here we go beyond proof-of-concept and demonstrate that semiconducting channels etched from a wafer-scale two-dimensional electron gas (2DEG) are a suitable platform for building a scalable gatemon-based quantum computer. We show that 2DEG gatemons meet the requirements6 by performing voltage-controlled single qubit rotations and two-qubit swap operations. We measure qubit coherence times up to ~2 μs, limited by dielectric loss in the 2DEG substrate.
Dou Z, Morikawa S, Cresti A, et al., 2018, Imaging bulk and edge transport near the dirac point in graphene moiré superlattices, Nano Letters, Vol: 18, Pages: 2530-2537, ISSN: 1530-6984
Van der Waals structures formed by aligning monolayer graphene with insulating layers of hexagonal boron nitride exhibit a moiré superlattice that is expected to break sublattice symmetry. Despite an energy gap of several tens of millielectronvolts opening in the Dirac spectrum, electrical resistivity remains lower than expected at low temperature and varies between devices. While subgap states are likely to play a role in this behavior, their precise nature is unclear. We present a scanning gate microscopy study of moiré superlattice devices with comparable activation energy but with different charge disorder levels. In the device with higher charge impurity (∼1010 cm–2) and lower resistivity (∼10 kΩ) at the Dirac point we observe current flow along the graphene edges. Combined with simulations, our measurements suggest that enhanced edge doping is responsible for this effect. In addition, a device with low charge impurity (∼109 cm–2) and higher resistivity (∼100 kΩ) shows subgap states in the bulk, consistent with the absence of shunting by edge currents.
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