Unseld Florian K, Undseth Brennan, Raymenants Eline, Matsumoto Yuta, de Snoo Sander L, Karwal Saurabh, Pietx-Casas Oriol, Ivlev Alexander S, Meyer Marcel, Sammak Amir, Veldhorst Menno, Scappucci Giordano, Vandersypen Lieven M K
QuTech and Kavli Institute of Nanoscience, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, Delft, The Netherlands.
QuTech and Netherlands Organization for Applied Scientific Research (TNO), Stieltjesweg 1, 2628 CK Delft, Delft, Netherlands.
Nat Commun. 2025 Jul 1;16(1):5605. doi: 10.1038/s41467-025-60351-x.
Micromagnet-enabled electric-dipole spin resonance (EDSR) is an established method for high-fidelity single-spin control in silicon, although so far experiments have been restricted to one-dimensional arrays. In contrast, qubit control based on hopping spins has recently emerged as a compelling alternative, with high-fidelity baseband control realized in sparse two-dimensional hole arrays in germanium. In this work, we commission a Si/SiGe 2 × 2 quantum dot array both as a four-qubit device using EDSR and as a two-qubit device using baseband hopping control. We establish a lower bound on the fidelity of the hopping gate of 99.50(6)%, which is similar to the average fidelity of the resonant gate. The hopping gate also circumvents the transient pulse-induced resonance shift from heating observed during EDSR operation. To motivate hopping spins as an attractive means of scaling silicon spin-qubit arrays, we propose an extensible nanomagnet design that enables engineered baseband control of large spin arrays.
基于微磁体的电偶极子自旋共振(EDSR)是一种用于在硅中实现高保真单自旋控制的成熟方法,尽管迄今为止实验仅限于一维阵列。相比之下,基于跳跃自旋的量子比特控制最近已成为一种引人注目的替代方案,在锗中的稀疏二维空穴阵列中实现了高保真基带控制。在这项工作中,我们调试了一个Si/SiGe 2×2量子点阵列,既将其用作使用EDSR的四量子比特器件,也用作使用基带跳跃控制的双量子比特器件。我们确定了跳跃门保真度的下限为99.50(6)%,这与谐振门的平均保真度相似。跳跃门还避免了在EDSR操作期间观察到的由加热引起的瞬态脉冲诱导的共振偏移。为了激发跳跃自旋作为扩展硅自旋量子比特阵列的一种有吸引力的手段,我们提出了一种可扩展的纳米磁体设计,该设计能够对大型自旋阵列进行工程化基带控制。