pith. sign in

arxiv: 2505.02106 · v2 · submitted 2025-05-04 · 🪐 quant-ph

Robustness Enhancement of Universal Noncyclic Geometric Gates via Evolution Optimization

Pith reviewed 2026-05-22 17:22 UTC · model grok-4.3

classification 🪐 quant-ph
keywords noncyclic geometric gatesquantum gate optimizationrobustness to errorssuperconducting circuitsgeometric phasesystematic errorscrosstalkleakage errors
0
0 comments X

The pith

Noncyclic geometric gates optimized for evolution paths resist systematic errors and crosstalk better than dynamical Rabi or cyclic alternatives.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

Noncyclic geometric gates relax the strict cyclic closure required in conventional geometric phase gates, allowing more flexible evolution trajectories. The paper evaluates every noncyclic condition, maps the resulting geometric paths, and uses numerical optimization to select those that minimize sensitivity to universal systematic errors plus residual crosstalk. The resulting gates maintain higher fidelity than both representative dynamical Rabi gates and standard cyclic geometric gates. Simulations further confirm that these gates remain feasible at high fidelity in superconducting circuits when leakage and decoherence are included. A sympathetic reader would care because fault-tolerant quantum processors need gates that tolerate the dominant hardware imperfections without relying solely on heavy error correction.

Core claim

By systematically evaluating all noncyclic evolution conditions and their corresponding geometric trajectories, the authors identify optimal conditions that enhance resilience against universal systematic errors and residual crosstalk error. The optimized noncyclic geometric gates exhibit significant robustness advantages over representative dynamical Rabi gates and conventional cyclic geometric gates. The work also validates the physical feasibility of high-fidelity noncyclic geometric gates in superconducting quantum circuits while quantifying the impacts of intrinsic leakage errors and decoherence effects.

What carries the argument

Noncyclic evolution conditions that permit flexible geometric trajectories without full cyclic closure, selected by numerical optimization to maximize resilience to errors.

If this is right

  • Optimized noncyclic gates maintain higher fidelity than dynamical Rabi gates when universal systematic errors are present.
  • The same optimized gates outperform conventional cyclic geometric gates under residual crosstalk.
  • High-fidelity noncyclic geometric gates remain implementable in superconducting circuits once leakage and decoherence are accounted for.
  • Numerical selection of noncyclic trajectories provides a concrete route to improved gate robustness without altering the underlying Hamiltonian.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If the robustness gains hold in experiment, the overhead for quantum error correction on near-term processors could decrease.
  • The same optimization of evolution conditions might be applied to geometric gates on other platforms such as trapped ions or neutral atoms.
  • Combining these noncyclic gates with pulse-shaping techniques could further suppress leakage beyond what the paper models.

Load-bearing premise

The chosen error models of universal systematic errors plus residual crosstalk together with the numerical optimization procedure capture the dominant failure modes of real superconducting hardware.

What would settle it

Fabricate and run the optimized noncyclic gates on a superconducting qubit device, apply controlled systematic errors and crosstalk, then compare measured gate fidelities directly against those of dynamical Rabi gates and cyclic geometric gates under identical conditions.

Figures

Figures reproduced from arXiv: 2505.02106 by Tao Chen, Yan Liang, Yi-Han Yuan, Zheng-Yuan Xue, Zi-Hao Qin.

Figure 1
Figure 1. Figure 1: FIG. 1. The potential noncyclic geometric evolution trajectories cor [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. (a) The general geometric evolution trajectory corresponding [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The simplified geometric trajectories corresponding to (a) [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Comparison of gate robustness for noncyclic geometric gates [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Fidelity of the noncyclic geometric [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Comparison of gate robustness for (a-c) dynamical Rabi [PITH_FULL_IMAGE:figures/full_fig_p006_6.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. (a) Gate fidelity of noncyclic geometric [PITH_FULL_IMAGE:figures/full_fig_p008_8.png] view at source ↗
read the original abstract

Noncyclic geometric gates aim to overcome the stringent constraints of conventional cyclic conditions and enhance the flexibility in evolution choice. Conceptually, they can also avoid the error problems arising from the violation of cyclicity, thus holding significance for improving the fault tolerance of quantum gates. However, current research on noncyclic geometric gates lacks a comprehensive exploration of their flexibility in evolution choice and validation of their effectiveness in resilience against multiple error sources present in practical quantum systems. In this paper, we systematically evaluate all noncyclic evolution conditions, elucidate their corresponding potential geometric trajectories, and identify optimal conditions for enhancing gate robustness by quantifying the resilience of constructed noncyclic geometric gates against universal systematic errors and residual crosstalk error. The optimized gates demonstrate significant robustness advantages over representative dynamical Rabi gates and conventional cyclic geometric gates. Furthermore, we validate the physical feasibility of high-fidelity noncyclic geometric gates in superconducting quantum circuits, with focused investigation into the impacts of intrinsic leakage errors and decoherence effects. Therefore, this work establishes a critical foundation for robust gate implementation toward practical fault-tolerant quantum processors.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript systematically evaluates all noncyclic evolution conditions for geometric quantum gates, maps their trajectories, and uses numerical optimization of evolution parameters to identify conditions that enhance resilience against universal systematic errors and residual crosstalk. It reports that the resulting optimized gates show significant robustness advantages over dynamical Rabi gates and conventional cyclic geometric gates, and validates high-fidelity implementation in superconducting circuits while examining leakage and decoherence effects.

Significance. If the reported robustness advantages are confirmed to arise from a properly global optimization rather than local fitting, the work could meaningfully advance fault-tolerant quantum gate design by relaxing cyclic constraints and providing a concrete optimization framework for error resilience in superconducting hardware.

major comments (2)
  1. [Section 3] Section 3: The numerical search over evolution parameters to quantify resilience against systematic and crosstalk errors is load-bearing for the central robustness claims, yet the manuscript provides no description of the optimization algorithm, number of random restarts, sampling strategy, or checks for global optimality (e.g., basin-hopping or exhaustive grid). Without this, it is impossible to rule out that the reported advantages reflect an incompletely explored local optimum rather than a genuine improvement.
  2. [§4] §4 and abstract: The claims of 'significant robustness advantages' and 'high-fidelity' noncyclic gates rest on post-optimization numerical results, but no quantitative metrics (fidelities, error rates with error bars, or statistical comparisons to baselines) are referenced in the evaluation sections; this makes the magnitude of the improvement and its statistical reliability difficult to assess.
minor comments (2)
  1. Add explicit definitions or citations for the precise models of 'universal systematic errors' and 'residual crosstalk error' used in the resilience quantification.
  2. Ensure all simulation figures report error bars or confidence intervals on fidelity and robustness metrics to allow direct comparison with the dynamical and cyclic baselines.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which help clarify the presentation of our numerical methods and results. We address each major comment point by point below and will revise the manuscript accordingly to improve transparency and rigor.

read point-by-point responses
  1. Referee: [Section 3] Section 3: The numerical search over evolution parameters to quantify resilience against systematic and crosstalk errors is load-bearing for the central robustness claims, yet the manuscript provides no description of the optimization algorithm, number of random restarts, sampling strategy, or checks for global optimality (e.g., basin-hopping or exhaustive grid). Without this, it is impossible to rule out that the reported advantages reflect an incompletely explored local optimum rather than a genuine improvement.

    Authors: We agree that additional details on the optimization procedure are necessary for full reproducibility and to substantiate the global nature of the search. In the revised manuscript, we will expand Section 3 to describe the optimization algorithm, including the sampling strategy over evolution parameters, the number of random restarts performed, and the checks for global optimality such as basin-hopping combined with local refinement. This will demonstrate that the identified optimal conditions were obtained through a thorough exploration of the parameter space rather than an incomplete local search. revision: yes

  2. Referee: [§4] §4 and abstract: The claims of 'significant robustness advantages' and 'high-fidelity' noncyclic gates rest on post-optimization numerical results, but no quantitative metrics (fidelities, error rates with error bars, or statistical comparisons to baselines) are referenced in the evaluation sections; this makes the magnitude of the improvement and its statistical reliability difficult to assess.

    Authors: We acknowledge that the evaluation sections would benefit from more explicit quantitative metrics to allow direct assessment of the improvements. In the revised version, we will add specific fidelity values, error rates with error bars derived from multiple simulation runs, and statistical comparisons to the dynamical Rabi and cyclic geometric gate baselines directly in Section 4, with appropriate references to the supporting figures. We will also ensure the abstract accurately summarizes these quantitative findings. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected in derivation or claims

full rationale

The paper systematically enumerates noncyclic evolution conditions, maps their geometric trajectories, and applies numerical optimization to select parameters that minimize infidelity under modeled systematic and crosstalk errors. The resulting robustness advantages are shown via direct comparison of simulated error rates against fixed baselines (dynamical Rabi gates and standard cyclic geometric gates), not by re-expressing the optimization objective itself. Subsequent superconducting-circuit simulations incorporate leakage and decoherence as additional checks outside the original optimization metric. No equation or claim reduces by construction to its inputs, no self-citation supplies a load-bearing uniqueness theorem, and the optimization functions as a design procedure rather than a fitted prediction renamed as a result. The derivation therefore remains self-contained against the stated benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard quantum-control assumptions about geometric phases and on the validity of the chosen error Hamiltonians; no new entities are postulated.

free parameters (1)
  • evolution path parameters
    Numerical optimization tunes continuous parameters of the noncyclic trajectory to minimize error sensitivity; these are fitted to the robustness metric.
axioms (2)
  • domain assumption Geometric phase acquired along a noncyclic path can implement a universal quantum gate when the path satisfies the enumerated conditions.
    Invoked in the systematic evaluation of noncyclic evolution conditions.
  • domain assumption The dominant error channels are captured by universal systematic errors and residual crosstalk.
    Used when quantifying resilience of the constructed gates.

pith-pipeline@v0.9.0 · 5725 in / 1370 out tokens · 35394 ms · 2026-05-22T17:22:08.035905+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

65 extracted references · 65 canonical work pages · 1 internal anchor

  1. [1]

    Robustness Enhancement of Universal Noncyclic Geometric Gates via Evolution Optimization

    and superconducting quantum circuits [50]. Current re- search on noncyclic geometric gates still exhibits notable defi- ciencies: on the one hand, there is a lack of systematic explo- ration of the flexibility in evolution choice; on the other hand, their effectiveness in resisting multiple error sources has not yet been fully verified. Here, we will focu...

  2. [2]

    M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information (Cambridge University Press, 2000)

  3. [3]

    Zhang, T

    J. Zhang, T. H. Kyaw, S. Filipp, L.-C. Kwek, E. Sj ¨oqvist, and D. M. Tong, Geometric and holonomic quantum computation, Phys. Rep. 1027, 1 (2023)

  4. [4]

    Liang, P

    Y . Liang, P. Shen, T. Chen, and Z.-Y . Xue, Nonadiabatic holo- nomic quantum computation and its optimal control, Sci. China Inf. Sci. 66, 180502 (2023)

  5. [5]

    M. V . Berry, Quantal phase factors accompanying adiabatic changes, Proc. R. Soc. London A 392, 45 (1984)

  6. [6]

    Wilczek and A

    F. Wilczek and A. Zee, Appearance of gauge structure in simple dynamical systems, Phys. Rev. Lett. 52, 2111 (1984)

  7. [7]

    Aharonov and J

    Y . Aharonov and J. Anandan, Phase change during a cyclic quantum evolution, Phys. Rev. Lett. 58, 1593 (1987)

  8. [8]

    Samuel and R

    J. Samuel and R. Bhandari, General Setting for Berry’s Phase, Phys. Rev. Lett. 60, 2339 (1988)

  9. [9]

    Anandan, Non-adiabatic non-abelian geometric phase, Phys

    J. Anandan, Non-adiabatic non-abelian geometric phase, Phys. Lett. A 133, 171 (1988)

  10. [10]

    Zhu and P

    S.-L. Zhu and P. Zanardi, Geometric quantum gates that are robust against stochastic control errors, Phys. Rev. A 72, 020301(R) (2005)

  11. [11]

    J. T. Thomas, M. Lababidi, and M. Z. Tian, Robustness of single-qubit geometric gate against systematic error, Phys. Rev. A 84, 042335 (2011)

  12. [12]

    Solinas, M

    P. Solinas, M. Sassetti, P. Truini, and N. Zangh`ı, On the stability of quantum holonomic gates, New J. Phys. 14, 093006 (2012)

  13. [13]

    Johansson, E

    M. Johansson, E. Sj ¨oqvist, L. M. Andersson, M. Ericsson, B. Hessmo, K. Singh, and D. M. Tong, Robustness of nonadiabatic holonomic gates, Phys. Rev. A 86, 062322 (2012)

  14. [14]

    Keiji, Nonadiabatic conditional ge- ometric phase shift with NMR, Phys

    Wang Xiang-Bin and M. Keiji, Nonadiabatic conditional ge- ometric phase shift with NMR, Phys. Rev. Lett. 87, 097901 (2001)

  15. [15]

    Zhu and Z

    S.-L. Zhu and Z. D. Wang, Implementation of universal quan- tum gates based on nonadiabatic geometric phases, Phys. Rev. Lett. 89, 097902 (2002)

  16. [16]

    Sj ¨oqvist, D

    E. Sj ¨oqvist, D. M. Tong, L. M. Andersson, B. Hessmo, M. Johansson, and K. Singh, Non-adiabatic holonomic quantum computation, New J. Phys. 14, 103035 (2012)

  17. [17]

    G. F. Xu, J. Zhang, D. M. Tong, E. Sj ¨oqvist, and L. C. Kwek, Nonadiabatic Holonomic Quantum Computation in Decoherence-Free Subspaces, Phys. Rev. Lett. 109, 170501 (2012)

  18. [18]

    Herterich and E

    E. Herterich and E. Sj ¨oqvist, Single-loop multiple-pulse nona- diabatic holonomic quantum gates, Phys. Rev. A 94, 052310 (2016)

  19. [19]

    P. Z. Zhao, X. D. Cui, G. F. Xu, E. Sj ¨oqvist, and D. M. Tong, Rydberg-atom-based scheme of nonadiabatic geometric quan- tum computation, Phys. Rev. A 96, 052316 (2017)

  20. [20]

    Liu, X.-K

    B.-J. Liu, X.-K. Song, Z.-Y . Xue, X. Wang, and M.-H.Yung, Plug-and-play approach to nonadiabatic geometric quantum gates, Phys. Rev. Lett. 123, 100501 (2019)

  21. [21]

    K. Z. Li, P. Z. Zhao, and D. M. Tong, Approach to realizing nonadiabatic geometric gates with prescribed evolution paths, Phys. Rev. Res. 2, 023295 (2020)

  22. [22]

    W. Dong, F. Zhuang, S. E. Economou, and E. Barnes, Doubly Geometric Quantum Control, PRX Quantum 2, 030333 (2021)

  23. [23]

    Ding, L.-N

    C.-Y . Ding, L.-N. Ji, T. Chen, and Z.-Y . Xue, Path-optimized nonadiabatic geometric quantum computation on supercon- ducting qubits, Quantum Sci. Technol. 7, 015012 (2022)

  24. [24]

    Leibfried, B

    D. Leibfried, B. DeMarco, V . Meyer, D. Lucas, M. Barrett, J. Britton, W. M. Itano, B. Jelenkovi ´c, C. Langer, T. Rosenband, and D. J. Wineland, Experimental demonstration of a robust, high-fidelity geometric two ion-qubit phase gate, Nature (Lon- don) 422, 412 (2003)

  25. [25]

    M.-Z. Ai, S. Li, Z. Hou, R. He, Z.-H. Qian, Z.-Y . Xue, J.-M. Cui, Y .-F. Huang, C.-F. Li, and G.-C. Guo, Experimental real- ization of nonadiabatic holonomic single-qubit quantum gates with optimal control in a trapped ion, Phys. Rev. Appl. 14, 054062 (2020)

  26. [26]

    J. Du, P. Zou, and Z. D. Wang, Experimental implementation of high-fidelity unconventional geometric quantum gates using an NMR interferometer, Phys. Rev. A 74, 020302(R) (2006)

  27. [27]

    G. Feng, G. Xu, and G. Long, Experimental realization of nona- diabatic holonomic quantum computation, Phys. Rev. Lett.110, 190501 (2013)

  28. [28]

    H. Li, Y . Liu, and G. Long, Experimental realization of single- shot nonadiabatic holonomic gates in nuclear spins, Sci. China- Phys. Mech. Astron. 60, 080311 (2017)

  29. [29]

    Z. Zhu, T. Chen, X. Yang, J. Bian, Z.-Y . Xue, and X. Peng, Single-loop and composite-loop realization of nonadia- batic holonomic quantum gates in a decoherence-free subspace, Phys. Rev. Appl. 12, 024024 (2019)

  30. [30]

    Y . Li, T. Xin, C. Qiu, K. Li, G. Liu, J. Li, Y . Wan, and D. Lu, Dynamical-invariant-based holonomic quantum gates: Theory and experiment, Fundamental Research 3, 229 (2023). 10

  31. [31]

    A. A. Abdumalikov Jr, J. M. Fink, K. Juliusson, M. Pechal, S. Berger, A. Wallraff, and S. Filipp, Experimental realization of non-Abelian non-adiabatic geometric gates, Nature (Lon- don) 496, 482 (2013)

  32. [32]

    Y . Xu, W. Cai, Y . Ma, X. Mu, L. Hu, T. Chen, H. Wang, Y . P. Song, Z.-Y . Xue, Z.-Q. Yin, and L. Sun, Single-Loop Realiza- tion of Arbitrary Nonadiabatic Holonomic Single-Qubit Quan- tum Gates in a Superconducting Circuit, Phys. Rev. Lett. 121, 110501 (2018)

  33. [33]

    D. J. Egger, M. Ganzhorn, G. Salis, A. Fuhrer, P. M ¨uller, P. K. Barkoutsos, N. Moll, I. Tavernelli, and S. Filipp, Entanglement Generation in Superconducting Qubits Using Holonomic Oper- ations, Phys. Rev. Appl. 11, 014017 (2019)

  34. [34]

    Yan, B.-J

    T. Yan, B.-J. Liu, K. Xu, C. Song, S. Liu, Z. Zhang, H. Deng, Z. Yan, H. Rong, K. Huang, M.-H. Yung, Y . Chen, and D. Yu, Ex- perimental realization of nonadiabatic shortcut to non-Abelian geometric gates, Phys. Rev. Lett. 122, 080501 (2019)

  35. [35]

    Y . Xu, Z. Hua, T. Chen, X. Pan, X. Li, J. Han, W. Cai, Y . Ma, H. Wang, Y . Song, Z.-Y . Xue, and L. Sun, Experimen- tal Implementation of Universal Nonadiabatic Geometric Quan- tum Gates in a Superconducting Circuit, Phys. Rev. Lett. 124, 230503 (2020)

  36. [36]

    P. Z. Zhao, Z. Dong, Z. Zhang, G. Guo, D. M. Tong, and Y . Yin, Experimental realization of non-adiabatic geometric gates with a superconducting xmon qubit, Sci. China-Phys. Mech. Astron. 64, 250362 (2021)

  37. [37]

    K. Xu, W. Ning, X.-J. Huang, P.-R. Han, H. Li, Z.-B. Yang, D. Zheng, H. Fan, and S.-B. Zheng, Demonstration of a non- Abelian geometric controlled-NOT gate in a superconducting circuit, Optica 8, 972 (2021)

  38. [38]

    Zu, W.-B

    C. Zu, W.-B. Wang, L. He, W.-G. Zhang, C.-Y . Dai, F. Wang, and L.-M. Duan, Experimental realization of universal geomet- ric quantum gates with solid-state spins, Nature (London) 514, 72 (2014)

  39. [39]

    Arroyo-Camejo, A

    S. Arroyo-Camejo, A. Lazariev, S. W. Hell, and G. Balasub- ramanian, Room temperature high-fidelity holonomic single- qubit gate on a solid-state spin, Nat. Commun. 5, 4870 (2014)

  40. [40]

    Sekiguchi, N

    Y . Sekiguchi, N. Niikura, R. Kuroiwa, H. Kano, and H. Kosaka, Optical holonomic single quantum gates with a geometric spin under a zero field, Nat. Photonics 11, 309 (2017)

  41. [41]

    B. B. Zhou, P. C. Jerger, V . O. Shkolnikov, F. J. Heremans, G. Burkard, and D. D. Awschalom, Holonomic Quantum Control by Coherent Optical Excitation in Diamond, Phys. Rev. Lett. 119, 140503 (2017)

  42. [42]

    Nagata, K

    K. Nagata, K. Kuramitani, Y . Sekiguchi, and H. Kosaka, Uni- versal holonomic quantum gates over geometric spin qubits with polarised microwaves, Nat. Commun. 9, 3227 (2018)

  43. [43]

    Dong, S.-C

    Y . Dong, S.-C. Zhang, Y . Zheng, H.-B. Lin, L.-K. Shan, X.-D. Chen, W. Zhu, G.-Z. Wang, G.-C. Guo, and F.-W. Sun, Exper- imental implementation of universal holonomic quantum com- putation on solid-state spins with optimal control, Phys. Rev. Appl. 16, 024060 (2021)

  44. [44]

    Friedenauer and E

    A. Friedenauer and E. Sj ¨oqvist, Noncyclic geometric quantum computation, Phys. Rev. A 67, 024303 (2003)

  45. [45]

    Chen and Z.-Y

    T. Chen and Z.-Y . Xue, High-fidelity and robust geometric quantum gates that outperform dynamical ones, Phys. Rev. Appl. 14, 064009 (2020)

  46. [46]

    Liu, S.-L

    B.-J. Liu, S.-L. Su, and M.-H. Yung, Nonadiabatic noncyclic geometric quantum computation in Rydberg atoms, Phys. Rev. Res. 2, 043130 (2020)

  47. [47]

    Eivarsson and E

    N. Eivarsson and E. Sj ¨oqvist, Genuinely noncyclic geometric gates in two-pulse schemes, Phys. Rev. A 108, 032612 (2023)

  48. [48]

    Chen, Z.-Y

    T. Chen, Z.-Y . Xue, and Z. D. Wang, Error-tolerant geomet- ric quantum control for logical qubits with minimal resources, Phys. Rev. Appl. 18, 014062 (2022)

  49. [49]

    Chen, J.-H

    Z.-Y . Chen, J.-H. Liang, Z.-X. Fu, H.-Z. Liu, Z.-R. He, M. Wang, Z.-W. Han, J.-Y . Huang, Q.-X. Lv, and Y .-X. Du, Single- pulse two-qubit gates for Rydberg atoms with noncyclic geo- metric control, Phys. Rev. A 109, 042621 (2024)

  50. [50]

    J. W. Zhang, L.-L. Yan, J. C. Li, G. Y . Ding, J. T. Bu, L. Chen, S.-L. Su, F. Zhou, and M. Feng, Single-Atom Verification of the Noise-Resilient and Fast Characteristics of Universal Nona- diabatic Noncyclic Geometric Quantum Gates, Phys. Rev. Lett. 127, 030502 (2021)

  51. [51]

    Z. Ma, J. Xu, T. Chen, Y . Zhang, W. Zheng, S. Li, D. Lan, Z. Y . Xue, X. Tan, and Y . Yu, Noncyclic nonadiabatic geometric quantum gates in a superconducting circuit, Phys. Rev. Appl. 20, 054047 (2023)

  52. [52]

    De Zela, The Pancharatnam-Berry Phase: Theoretical and Experimental Aspects, in Theoretical Concepts of Quantum Mechanics, edited by M

    F. De Zela, The Pancharatnam-Berry Phase: Theoretical and Experimental Aspects, in Theoretical Concepts of Quantum Mechanics, edited by M. R. Pahlavani (InTech, London, 2012)

  53. [53]

    Suter and G

    D. Suter and G. A. Alvarez, Colloquium: Protecting quantum information against environmental noise, Rev. Mod. Phys. 88, 041001 (2016)

  54. [54]

    P. M. Poggi, G. D. Chiara, S. Campbell, and A. Kiely, Uni- versally robust quantum control, Phys. Rev. Lett. 132, 193801 (2024)

  55. [55]

    Watanabe, Y

    S. Watanabe, Y . Tabuchi, K. Heya, S. Tamate and Y . Nakamura, ZZ-Interaction-Free Single-Qubit-Gate Optimization in Super- conducting Qubits, Phys. Rev. A 109, 012616 (2024)

  56. [56]

    Yi, Y .-J

    K. Yi, Y .-J. Hai, K. Luo, J. Chu, L. Zhang, Y . Zhou, Y . Song, S. Liu, T. Yan, X.-H. Deng, Y . Chen, and D. Yu, Robust Quantum Gates against Correlated Noise in Integrated Quantum Chips, Phys. Rev. Lett. 132, 250604 (2024)

  57. [57]

    D. C. McKay, C. J. Wood, S. Sheldon, J. M. Chow, and J. M. Gambetta, Efficient Z gates for quantum computing, Phys. Rev. A 96, 022330 (2017)

  58. [58]

    Motzoi, J

    F. Motzoi, J. M. Gambetta, P. Rebentrost, and F. K. Wilhelm, Simple Pulses for Elimination of Leakage in Weakly Nonlinear Qubits, Phys. Rev. Lett. 103, 110501 (2009)

  59. [59]

    Z. Chen, J. Kelly, C. Quintana, R. Barends, B. Campbell, Y . Chen, B. Chiaro, A. Dunsworth, A. G. Fowler, E. Luceroet al., Measuring and suppressing quantum state leakage in a super- conducting qubit, Phys. Rev. Lett. 116, 020501 (2016)

  60. [60]

    T. Wang, Z. Zhang, L. Xiang, Z. Jia, P. Duan, W. Cai, Z. Gong, Z. Zong, M. Wu, J. Wu, L. Sun, Y . Yin, and G. Guo, The ex- perimental realization of high-fidelity ‘shortcut-to-adiabaticity’ quantum gates in a superconducting Xmon qubit, New J. Phys. 20, 065003 (2018)

  61. [61]

    Krantz, M

    P. Krantz, M. Kjaergaard, F. Yan, T. P. Orlando, S. Gustavsson, and W. D. Oliver, A Quantum Engineer’s Guide to Supercon- ducting Qubits, Appl. Phys. Rev. 6, 021318 (2019)

  62. [62]

    Kjaergaard, M

    M. Kjaergaard, M. E. Schwartz, J. Braum ¨uller, P. Krantz, J. I.- Jan Wang, S. Gustavsson, and W. D. Oliver, Superconducting qubits: Current state of play, Annu. Rev. Condens. Matter Phys. 11, 369 (2020)

  63. [63]

    Huang, D

    H.-L. Huang, D. Wu, D. Fan, and X. Zhu, Superconducting quantum computing: A review, Sci. China Inf. Sci. 63, 180501 (2020)

  64. [64]

    Caldwell, N

    S. Caldwell, N. Didier, C. A. Ryan, E. A. Sete, A. Hudson, P. Karalekas, R. Manenti, M. P. da Silva, R. Sinclair, E. Acala, et al., Parametrically activated entangling gates using transmon qubits, Phys. Rev. Appl. 10, 034050 (2018)

  65. [65]

    Reagor, C

    M. Reagor, C. B. Osborn, N. Tezak, A. Staley, G. Prawiroat- modjo, M. Scheer, N. Alidoust, E. A. Sete, N. Didier, M. P. da Silva et al., Demonstration of universal parametric entangling gates on a multi-qubit lattice, Sci. Adv. 4, eaao3603 (2018)