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48自旋单重态流形的交换控制基准测试

Benchmarking exchange-only control of a 48-spin singlet manifold

HRL Quantum Team, Microsoft Collaborators, :, Stephen Carr, Matt Abbitt, Michael Abraham, Edwin Acuna, I. Alverado, Carter Andrews, Hussein Anton, Katherine M. Beech, Aaron J. Bluestone, Jacob Z. Blumoff, Matthew G. Borselli, Brydon Boyd, Jacob T. Boyer, Peter Brewer, Steven L. Brown, Joseph D. Broz, Tyler A. Cain, John B. Carpenter, Faustin W. Carter, Brittany Carter, Matthew D. Chambers, James M. Chappell, Kevin C. Chen, Edward H. Chen, Maxwell D. Choi, Matthew N. H. Chow, Justin E. Christensen, Aaron M. Chronister, Andrew M. Clapper, Michael D. Cornelius, Gregory M. Crosswhite, Stanislav Culaclii, Erik S. Daniel, Dominic Daprano, John K. David, Charles R. Elliott, Kevin Eng, Colin P. Feeney, David J. Fialkow, Dylan H. Finestone, Bryan H. Fong, Richie Fu, Zachary A. Geiger, Bradley W. Greene, Rafael Guerra-Fuentes, Hrayr K. Gurgenian, Alex Hamill, Brooke M. Hardesty, Jim W. Harrington, Alex Hirman, Donald A. Hitko, Silas Hoffman, Dominic Holloman, Daniel R. Hulbert, Jake Hundley, Clayton A. C. Jackson, Paul C. Jerger, B. Johnson, Aaron M. Jones, Michael P. Jura, Adour V. Kabakian, Tyler Keating, Joseph Kerckhoff, Andrey A. Kiselev, Patrick W. Krantz, Thaddeus D. Ladd, Sanaaya Lakdawala, Elias Lawson-Fox, Alwina R. Liu, Dwight Luhman, Manny Macias, Theodore K. Macioce, Ryan M. Martin, Daniel S. Matic, Gavin C. Mazur, Ryan McGeehan, Olivia Means, Austin Meyer, Samuel Mumford, Tina Niknejad, Riley P. O'Neil, Andrew Pan, Winston Pouse, Eric M. Prophet, Matthew D. Reed, Marcus Rentie, Alec Roberson, Zechariah Rogers, Golam Sabbir, Spencer Sager, Christopher D. Sanborn, Jonathan Sanchez, Rachel H. Sarmiento, Christian J. Schnaible, Cole Scott, Aaron Smith, Daniel E. Smith, James Soash, Kevin C. Staley, Andrea Su, Bo Sun, Christopher M. Swank, Noah Swimmer, Charles Tahan, Bryan J. Thomas, Yessica Torres, Alan Tran, Ivan Tran, James R. van Meter, Franklin Vartanian, John Samuel Venker, Daniel Volya, Annette L. Wagner, Daniel R. Ward, Aaron J. Weinstein, Abigail L. Wessels, Thomas V. Westrick, Evan T. White, Randall M. White, Parker Williams, Catrina E. Wilson, Courtney P. Wilt, Matthew Wingert, Clifford S. YoungSciortino, Andrew Ziegler

arXiv 2610.07393首次发表:更新:

发表机构

HRL Quantum Team; Microsoft Collaborators(HRL量子团队; 微软合作者)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

该研究提出一种利用全部希尔伯特空间的交换型性能度量方法,在多达48个电子自旋阵列上通过OTOC和广义随机基准测试,测得每个交换的有效系统级误差为3×10⁻⁴,较其他平台低一个数量级。

AI 中文摘要

交换型量子计算得益于交换相互作用提供的高保真度和直接控制。然而,可独立控制的量子比特必须编码在至少三个电子自旋的子系统中,这限制了计算只能利用可用自旋希尔伯特空间的一部分。其余状态被视为泄漏态,仅在门序列中临时使用。相比之下,一种定量的、系统范围的交换型性能度量可以利用全部可用的希尔伯特空间,包括传统上被视为泄漏态的状态。在这里,我们将此方法应用于多达48个电子自旋的阵列,访问总自旋为零的希尔伯特空间,其维度超过$2^{40}$。超出时间顺序相关器(OTOC)的测量揭示了丰富的加扰动力学,并展示了访问与量子计算优势相关的机制。利用交叉熵和镜像随机基准测试的广义形式,我们还评估了完整交换型系统在每个基本两体相互作用(即两自旋交换)上的总体性能。我们获得了每个交换的有效系统级误差为$3 \ imes 10^{-4}$,其中包含了完整的实验控制序列和所有相关噪声源。该值比撰写本文时其他平台上类似基准测试报告的值低至多一个数量级。

英文摘要

Exchange-only quantum computing benefits from high fidelity and straightforward control afforded by the exchange interaction. However, independently controllable qubits must be encoded into subsystems of at least three electron spins, restricting computation to only a fraction of the available spin Hilbert space. The remaining states are treated as leakage and used only transiently in gate sequences. By contrast, a quantitative, system-wide measure of exchange-only performance can exploit the full available Hilbert space, including states conventionally treated as leakage. Here, we apply this approach to arrays of up to 48 electron spins, accessing a total-spin-zero Hilbert space with dimension exceeding $2^{40}$. Measurements of out-of-time-order correlators (OTOCs) reveal rich scrambling dynamics and demonstrate access to regimes relevant to quantum computational advantage. Using generalized forms of cross-entropy and mirror randomized benchmarking, we also assess the aggregate performance of the full exchange-only system per fundamental two-body interaction: the two-spin exchange. We obtain an effective system-level error of $3 \times 10^{-4}$ per exchange, incorporating the complete experimental control sequence and all associated noise sources. This value is up to an order of magnitude lower than those reported from comparable benchmarks on other platforms at the time of writing.

论文原文

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