Abstract
Electrons confined in silicon quantum dots exhibit orbital, spin, and valley degrees of freedom. The valley degree of freedom originates from the bulk bandstructure of silicon, which has six degenerate electronic minima. The degeneracy can be lifted in silicon quantum wells due to strain and electronic confinement, but the "valley splitting" of the two lowest lying valleys is known to be sensitive to atomic-scale disorder. Large valley splittings are desirable to have a well-defined spin qubit. In addition, an understanding of the inter-valley tunnel coupling that couples different valleys in adjacent quantum dots is extremely important, as the resulting gaps in the energy level diagram may affect the fidelity of charge and spin transfer protocols in silicon quantum dot arrays. Here we use microwave spectroscopy to probe spatial variations in the valley splitting, and the intra- and inter-valley tunnel couplings ($t_{ij}$ and $t'_{ij}$) that couple dots $i$ and $j$ in a triple quantum dot (TQD). We uncover large spatial variations in the ratio of inter-valley to intra-valley tunnel couplings $t_{12}'/t_{12}=0.90$ and $t_{23}'/t_{23}=0.56$. By tuning the interdot tunnel barrier we also show that $t'_{ij}$ scales linearly with $t_{ij}$, as expected from theory. The results indicate strong interactions between different valley states on neighboring dots, which we attribute to local inhomogeneities in the silicon quantum well.
Highlights
Continuous research on electron spin qubits defined in silicon quantum dots has led to increasingly impressive levels of quantum control, with recent demonstrations of high single-qubit fidelities [1,2,3] and > 90% two-qubit gate fidelities [4,5]
Through timedomain control of the quantum-dot confinement potential, it is feasible to shuttle a single charge down an array of nine silicon quantum dots in approximately 50 ns [12]
Microwave spectroscopy of a triple quantum dot (TQD) in the circuit quantum electrodynamics device architecture (cQED) architecture provides an opportunity to sensitively probe the spatial variation of valley states in a silicon quantum device
Summary
Continuous research on electron spin qubits defined in silicon quantum dots has led to increasingly impressive levels of quantum control, with recent demonstrations of high single-qubit fidelities [1,2,3] and > 90% two-qubit gate fidelities [4,5]. Valley splittings range from 38–63 μeV and the intervalley tunnel coupling t12 between dots 1 and 2 is nearly 2 times larger than t23 These results have important implications on future experiments aimed at demonstrating coherent spin shuttling in quantum-dot arrays and reinforce the need for additional improvements in the growth of Si/Si0.7Ge0.3 heterostructures, especially interface abruptness. High-fidelity gate operations have been demonstrated with electrically tunable RX spin qubits, which can operate at zero magnetic field This increases compatibility with superconducting cavities [3] and allows for scalable control of the qubit frequency. Due to isotopic enrichment, silicon spin qubits offer much longer spin coherence times and may enable operation deep in the strong coupling regime, once the complications stemming from the presence of valley states are overcome
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