Abstract

The implementation of high fidelity two-qubit gates is a bottleneck in the progress toward universal quantum computation in semiconductor quantum dot qubits. We study capacitive coupling between two triple quantum dot spin qubits encoded in the S = 1/2, Sz = −1/2 decoherence-free subspace—the exchange-only (EO) spin qubits. We report exact gate sequences for CPHASE and CNOT gates, and demonstrate theoretically, the existence of multiple two-qubit sweet spots (2QSS) in the parameter space of capacitively coupled EO qubits. Gate operations have the advantage of being all-electrical, but charge noise that couple to electrical parameters of the qubits cause decoherence. Assuming noise with a 1/f spectrum, two-qubit gate fidelities and times are calculated, which provide useful information on the noise threshold necessary for fault-tolerance. We study two-qubit gates at single and multiple parameter 2QSS. In particular, for two existing EO implementations—the resonant exchange (RX) and the always-on exchange-only (AEON) qubits—we compare two-qubit gate fidelities and times at positions in parameter space where the 2QSS are simultaneously single-qubit sweet spots (1QSS) for the RX and AEON. These results provide a potential route to the realization of high fidelity quantum computation.

Highlights

  • Semiconductor quantum dots are one of the leading platforms for building a quantum computer

  • High fidelity gate operations have been demonstrated in single quantum dot (QD)3,4, double QD5–10, and triple quantum dot (TQD)11–13 architectures

  • We study two capacitively coupled EO qubits, and report exact gate sequences for CPHASE and CNOT gates

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Summary

Introduction

Semiconductor quantum dots are one of the leading platforms for building a quantum computer. They present promises of scalability, coherence, and integration with existing microelectronics technologies. Qubits encoded in the decoherence-free subspace of three electron spins have the advantage of fast, all-electrical control. Singlequbit gates are based on the exchange interaction, its namesake, the exchange-only (EO) qubit. The total spin of three electrons comprise a S = 3/2 quadruplet and two S = 1/2 degenerate doublets, whose degeneracy can be lifted by an external magnetic field. Logical qubit states are encoded in the total spin S = 1/2, Sz = −1/2 doublet, which provides immunity against collective decoherence

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