Pino J M, Dreiling J M, Figgatt C, Gaebler J P, Moses S A, Allman M S, Baldwin C H, Foss-Feig M, Hayes D, Mayer K, Ryan-Anderson C, Neyenhuis B
Honeywell Quantum Solutions, Broomfield, CO, USA.
Nature. 2021 Apr;592(7853):209-213. doi: 10.1038/s41586-021-03318-4. Epub 2021 Apr 7.
The trapped-ion quantum charge-coupled device (QCCD) proposal lays out a blueprint for a universal quantum computer that uses mobile ions as qubits. Analogous to a charge-coupled device (CCD) camera, which stores and processes imaging information as movable electrical charges in coupled pixels, a QCCD computer stores quantum information in the internal state of electrically charged ions that are transported between different processing zones using dynamic electric fields. The promise of the QCCD architecture is to maintain the low error rates demonstrated in small trapped-ion experiments by limiting the quantum interactions to multiple small ion crystals, then physically splitting and rearranging the constituent ions of these crystals into new crystals, where further interactions occur. This approach leverages transport timescales that are fast relative to the coherence times of the qubits, the insensitivity of the qubit states of the ion to the electric fields used for transport, and the low crosstalk afforded by spatially separated crystals. However, engineering a machine capable of executing these operations across multiple interaction zones with low error introduces many difficulties, which have slowed progress in scaling this architecture to larger qubit numbers. Here we use a cryogenic surface trap to integrate all necessary elements of the QCCD architecture-a scalable trap design, parallel interaction zones and fast ion transport-into a programmable trapped-ion quantum computer that has a system performance consistent with the low error rates achieved in the individual ion crystals. We apply this approach to realize a teleported CNOT gate using mid-circuit measurement, negligible crosstalk error and a quantum volume of 2 = 64. These results demonstrate that the QCCD architecture provides a viable path towards high-performance quantum computers.
囚禁离子量子电荷耦合器件(QCCD)方案为一种以移动离子作为量子比特的通用量子计算机勾勒了蓝图。类似于电荷耦合器件(CCD)相机,它将成像信息存储并处理为耦合像素中可移动的电荷,QCCD计算机将量子信息存储在带电离子的内部状态中,这些离子利用动态电场在不同的处理区域之间传输。QCCD架构的前景在于,通过将量子相互作用限制在多个小的囚禁离子晶体中,然后将这些晶体的组成离子物理拆分并重新排列成新的晶体,在新晶体中进一步发生相互作用,从而保持在小型囚禁离子实验中所展示的低错误率。这种方法利用了相对于量子比特相干时间而言较快的传输时间尺度、离子的量子比特状态对用于传输的电场的不敏感性以及空间分离的晶体所提供的低串扰。然而,设计一台能够在多个相互作用区域以低错误率执行这些操作的机器会带来许多困难,这减缓了将该架构扩展到更大量子比特数的进展。在这里,我们使用低温表面阱将QCCD架构的所有必要元素——可扩展的阱设计、并行相互作用区域和快速离子传输——集成到一台可编程的囚禁离子量子计算机中,该计算机的系统性能与在单个离子晶体中实现的低错误率一致。我们应用这种方法,通过电路中测量实现了一个隐形传态的CNOT门,串扰误差可忽略不计,量子体积达到2 = 64。这些结果表明,QCCD架构为高性能量子计算机提供了一条可行的途径。