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    Direct Implementation of High-Fidelity Three-Qubit Gates for Superconducting Processor with Tunable Couplers

    Hao-Tian Liu1,2,*, Bing-Jie Chen1,2,*, Jia-Chi Zhang1,2, Yong-Xi Xiao1,2, Tian-Ming Li1,2, Kaixuan Huang3, Ziting Wang3, Hao Li3, Kui Zhao3 et al.

    Yueshan Xu3, Cheng-Lin Deng1,2, Gui-Han Liang1,2, Zheng-He Liu1,2, Si-Yun Zhou1,2, Cai-Ping Fang1,2, Xiaohui Song1,2,4, Zhongcheng Xiang1,2,4, Dongning Zheng1,2,4, Yun-Hao Shi1,4,†, Kai Xu1,2,3,4,5,‡, and Heng Fan1,2,3,4,5,§

    • *These authors contributed equally to this work.
    • †Contact author: yhshi@iphy.ac.cn
    • ‡Contact author: kaixu@iphy.ac.cn
    • §Contact author: hfan@iphy.ac.cn

    Phys. Rev. Lett. 135, 050602 – Published 29 July, 2025

    DOI: https://doi.org/10.1103/lvb9-pfr3

    Abstract

    Three-qubit gates can be constructed using combinations of single-qubit and two-qubit gates, making their independent realization unnecessary. However, direct implementation of three-qubit gates reduces the depth of quantum circuits, streamlines quantum programming, and facilitates efficient circuit optimization, thereby enhancing overall performance in quantum computation. In this work, we propose and experimentally demonstrate a high-fidelity scheme for implementing a three-qubit controlled-controlled-z (ccz) gate in a flip-chip superconducting quantum processor with tunable couplers. This direct ccz gate is implemented by simultaneously leveraging two tunable couplers interspersed between three qubits to enable three-qubit interactions, achieving an average final state fidelity of 97.94% and a process fidelity of 93.54%. This high fidelity cannot be achieved through a simple combination of single- and two-qubit gate sequences from processors with similar performance levels. Our experiments also verify that multilayer direct implementation of the ccz gate exhibits lower leakage compared to decomposed gate approaches. As a showcase, we utilize the ccz gate as an oracle to implement the Grover search algorithm on three qubits, demonstrating high performance with the target probability amplitude significantly enhanced after two iterations. These results highlight the advantage of our approach, and facilitate the implementation of complex quantum circuits.

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