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Large, Tunable Valley Splitting and Single-Spin Relaxation Mechanisms in a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:mi>Si</mml:mi></mml:math>/<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:msub><mml:mi>Si</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:msub><mml:mi>Ge</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math> Quantum Dot

Arne Hollmann, Tom Struck, Veit Langrock, Andreas Schmidbauer, Floyd Schauer, Tim Leonhardt, Kentarou Sawano, Helge Riemann, Nikolay V. Abrosimov, Dominique Bougeard, Lars R. Schreiber

2020Physical Review Applied85 citationsDOIOpen Access PDF

Abstract

Valley splitting is a key feature of silicon-based spin qubits. Quantum dots in $\mathrm{Si}$/${\mathrm{Si}}_{x}{\mathrm{Ge}}_{1\ensuremath{-}x}$ heterostructures reportedly suffer from a relatively low valley splitting, limiting the operation temperature and the scalability of such qubit devices. Here, we demonstrate a robust and large valley splitting exceeding 200 $\ensuremath{\mu}\mathrm{eV}$ in a gate-defined single quantum dot, hosted in molecular-beam-epitaxy-grown $^{28}\mathrm{Si}/{\mathrm{Si}}_{x}{\mathrm{Ge}}_{1\ensuremath{-}x}$. The valley splitting is monotonically and reproducibly tunable up to 15% by gate voltages, originating from a 6-nm lateral displacement of the quantum dot. We observe static spin relaxation times ${T}_{1}&gt;1$ s at low magnetic fields in our device containing an integrated nanomagnet. At higher magnetic fields, ${T}_{1}$ is limited by the valley hotspot and by phonon noise coupling to intrinsic and artificial spin-orbit coupling, including phonon bottlenecking.

Topics & Concepts

Condensed matter physicsQuantum dotPhysicsPhononQubitLimitingMagnetic fieldRelaxation (psychology)QuantumCoupling (piping)Displacement (psychology)HeterojunctionSpin (aerodynamics)Materials scienceQuantum wellHotspot (geology)Zero field splittingSpintronicsQuantum gateDisplacement fieldQuantum and electron transport phenomenaSemiconductor Quantum Structures and DevicesAdvancements in Semiconductor Devices and Circuit Design
Large, Tunable Valley Splitting and Single-Spin Relaxation Mechanisms in a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:mi>Si</mml:mi></mml:math>/<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:msub><mml:mi>Si</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:msub><mml:mi>Ge</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math> Quantum Dot | Litcius