Abstract

High-fidelity control of quantum bits is paramount for the reliable execution of quantum algorithms and for achieving fault tolerance—the ability to correct errors faster than they occur1. The central requirement for fault tolerance is expressed in terms of an error threshold. Whereas the actual threshold depends on many details, a common target is the approximately 1% error threshold of the well-known surface code2,3. Reaching two-qubit gate fidelities above 99% has been a long-standing major goal for semiconductor spin qubits. These qubits are promising for scaling, as they can leverage advanced semiconductor technology4. Here we report a spin-based quantum processor in silicon with single-qubit and two-qubit gate fidelities, all of which are above 99.5%, extracted from gate-set tomography. The average single-qubit gate fidelities remain above 99% when including crosstalk and idling errors on the neighbouring qubit. Using this high-fidelity gate set, we execute the demanding task of calculating molecular ground-state energies using a variational quantum eigensolver algorithm5. Having surpassed the 99% barrier for the two-qubit gate fidelity, semiconductor qubits are well positioned on the path to fault tolerance and to possible applications in the era of noisy intermediate-scale quantum devices.

Highlights

  • Among all the candidate platforms, electron spins in semiconductor quantum dots have advantages, such as their long coherence times[8], small footprint[9], the potential for scaling up[10] and the compatibility with advanced semiconductor manufacturing technology[4]

  • We use a gate-defined double quantum dot in an isotopically enriched 28Si/SiGe heterostructure[17] (Fig. 1a), with each dot occupied by a single electron

  • The spin states of the electrons serve as qubits

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Summary

XY XZ YI YX YY YZ ZI Input

Errors from the microwave drive, such as through heating effects, will be a crucial step to improve the quality of the single-qubit operations further. For a high-fidelity adiabatic CZ gate, precise control of the exchange coupling, J, between the two qubits is required. We observe a minimum energy at around 0.72 Å and an error of approximately 20 mHa at the theoretical bond length 0.7414 Å, mainly attributed to slow drift in the readout parameters This accuracy matches the results obtained using superconducting and trapped ion qubits with comparable gate fidelities[36,39]. J. et al A quantum-dot spin qubit with coherence limited by charge noise and fidelity higher than 99.9%. K. et al Quantum tomography of an entangled three-qubit state in silicon. Efficient controlled-phase gate for single-spin qubits in quantum dots. P. et al Optimization of a solid-state electron spin qubit using gate set tomography. S. et al Fast gate-based readout of silicon quantum dots using Josephson parametric amplification. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/

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